| # |
| # This file is the units database for use with GNU units, a units conversion |
| # program by Adrian Mariano adrianm@gnu.org |
| # |
| # Febuary 2024 Version 3.19 |
| # last updated 16 February 2024 |
| # |
| # Copyright (C) 1996-2002, 2004-2020, 2022, 2024 |
| # Free Software Foundation, Inc |
| # |
| # This program is free software; you can redistribute it and/or modify |
| # it under the terms of the GNU General Public License as published by |
| # the Free Software Foundation; either version 3 of the License, or |
| # (at your option) any later version. |
| # |
| # This program is distributed in the hope that it will be useful, |
| # but WITHOUT ANY WARRANTY; without even the implied warranty of |
| # MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the |
| # GNU General Public License for more details. |
| # |
| # You should have received a copy of the GNU General Public License |
| # along with this program; if not, write to the Free Software |
| # Foundation, Inc., 51 Franklin Street, Fifth Floor, |
| # Boston, MA 02110-1301 USA |
| # |
| ############################################################################ |
| # |
| # Improvements and corrections are welcome. |
| # |
| # See the end of this file for a list of items we have chosen to exclude |
| # or have decided are out of scope for GNU units. |
| # |
| # Fundamental constants in this file are the 2018 CODATA recommended values. |
| # |
| # Most units data was drawn from |
| # 1. NIST Special Publication 811, Guide for the |
| # Use of the International System of Units (SI). |
| # Barry N. Taylor. 2008 |
| # https://www.nist.gov/pml/special-publication-811 |
| # 2. CRC Handbook of Chemistry and Physics 70th edition |
| # 3. Oxford English Dictionary |
| # 4. Webster's New Universal Unabridged Dictionary |
| # 5. Units of Measure by Stephen Dresner |
| # 6. A Dictionary of English Weights and Measures by Ronald Zupko |
| # 7. British Weights and Measures by Ronald Zupko |
| # 8. Realm of Measure by Isaac Asimov |
| # 9. United States standards of weights and measures, their |
| # creation and creators by Arthur H. Frazier. |
| # 10. French weights and measures before the Revolution: a |
| # dictionary of provincial and local units by Ronald Zupko |
| # 11. Weights and Measures: their ancient origins and their |
| # development in Great Britain up to AD 1855 by FG Skinner |
| # 12. The World of Measurements by H. Arthur Klein |
| # 13. For Good Measure by William Johnstone |
| # 14. NTC's Encyclopedia of International Weights and Measures |
| # by William Johnstone |
| # 15. Sizes by John Lord |
| # 16. Sizesaurus by Stephen Strauss |
| # 17. CODATA Recommended Values of Physical Constants available at |
| # http://physics.nist.gov/cuu/Constants/index.html |
| # 18. How Many? A Dictionary of Units of Measurement. Available at |
| # http://www.ibiblio.org/units/ |
| # 19. Numericana. http://www.numericana.com |
| # 20. UK history of measurement |
| # https://metrication.uk/more/timeline/ |
| # 21. NIST Handbook 44, Specifications, Tolerances, and |
| # Other Technical Requirements for Weighing and Measuring |
| # Devices. 2011 |
| # 22. NIST Special Publication 447, Weights and Measures Standards |
| # of the United States: a brief history. Lewis V. Judson. |
| # 1963; rev. 1976 |
| # 23. CRC Handbook of Chemistry and Physics, 96th edition |
| # 24. Dictionary of Scientific Units, 6th ed. H.G. Jerrard and D.B. |
| # McNeill. 1992 |
| # 25. NIST Special Publication 330, The International System of |
| # Units (SI). ed. Barry N. Taylor and Ambler Thompson. 2008 |
| # https://www.nist.gov/pml/special-publication-330 |
| # 26. BIPM Brochure, The International System of Units (SI). |
| # 9th ed., 2019 |
| # https://www.bipm.org/en/publications/si-brochure/ |
| # |
| ########################################################################### |
| # |
| # If units you use are missing or defined incorrectly, please contact me. |
| # If your country's local units are missing and you are willing to supply |
| # them, please send me a list. |
| # |
| ########################################################################### |
| |
| ########################################################################### |
| # |
| # Brief Philosophy of this file |
| # |
| # Most unit definitions are made in terms of integers or simple fractions of |
| # other definitions. The typical exceptions are when converting between two |
| # different unit systems, or the values of measured physical constants. In |
| # this file definitions are given in the most natural and revealing way in |
| # terms of integer factors. |
| # |
| # If you make changes be sure to run 'units --check' to check your work. |
| # |
| # The file is USA-centric, but there is some modest effort to support other |
| # countries. This file is now coded in UTF-8. To support environments where |
| # UTF-8 is not available, definitions that require this character set are |
| # wrapped in !utf8 directives. |
| # |
| # When a unit name is used in different countries with the different meanings |
| # the system should be as follows: |
| # |
| # Suppose countries ABC and XYZ both use the "foo". Then globally define |
| # |
| # ABCfoo <some value> |
| # XYZfoo <different value> |
| # |
| # Then, using the !locale directive, define the "foo" appropriately for each of |
| # the two countries with a definition like |
| # |
| # !locale ABC |
| # foo ABCfoo |
| # !endlocale |
| # |
| ########################################################################### |
| |
| !locale en_US |
| ! set UNITS_ENGLISH US |
| !endlocale |
| |
| !locale en_GB |
| ! set UNITS_ENGLISH GB |
| !endlocale |
| |
| !set UNITS_ENGLISH US # Default setting for English units |
| |
| !set UNITS_SYSTEM default # Set a default value |
| |
| !varnot UNITS_SYSTEM si emu esu gaussian gauss hlu natural natural-gauss hartree planck planck-red default |
| !message Unknown unit system given with -u or UNITS_SYSTEM environment variable |
| !message Valid systems: si, emu, esu, gauss[ian], hlu, natural, natural-gauss |
| !message planck, planck-red, hartree |
| !message Using SI |
| !prompt (SI) |
| !endvar |
| |
| !var UNITS_SYSTEM si |
| !message SI units selected |
| !prompt (SI) |
| !endvar |
| |
| ########################################################################### |
| # # |
| # Primitive units. Any unit defined to contain a '!' character is a # |
| # primitive unit which will not be reduced any further. All units should # |
| # reduce to primitive units. # |
| # # |
| ########################################################################### |
| |
| # |
| # SI units |
| # |
| # On 20 May 2019, the SI was revised to define the units by fixing the |
| # values of physical constants that depend on those units. |
| # |
| # https://www.nist.gov/si-redefinition/ |
| # |
| # The BIPM--the International Bureau of Weights and Measures--provides a |
| # succinct description of the new SI in its Concise Summary: |
| # |
| # https://www.bipm.org/utils/common/pdf/si-brochure/SI-Brochure-9-concise-EN.pdf |
| # |
| # The SI is the system of units in which: |
| # |
| # * the unperturbed ground state hyperfine transition frequency of the |
| # caesium 133 atom is delta nu_Cs = 9 192 631 770 Hz, |
| # * the speed of light in vacuum, c, is 299 792 458 m/s, |
| # * the Planck constant, h, is 6.626 070 15 * 10^-34 J s, |
| # * the elementary charge, e, is 1.602 176 634 * 10^-19 C, |
| # * the Boltzmann constant, k, is 1.380 649 * 10^-23 J/K, |
| # * the Avogadro constant, N_A, is 6.022 140 76 * 10^23 mol^-1, |
| # * the luminous efficacy of monochromatic radiation of frequency |
| # 540 * 10^12 Hz, K_cd, is 683 lm/W, |
| # |
| # where the hertz, joule, coulomb, lumen, and watt, with unit symbols Hz, |
| # J, C, lm, and W, respectively, are related to the units second, metre, |
| # kilogram, ampere, kelvin, mole, and candela, with unit symbols s, m, kg, |
| # A, K, mol, and cd, respectively, according to Hz = s^-1, J = kg m^2 s^-2, |
| # C = A s, lm = cd m^2 m^-2 = cd sr, and W = kg m^2 s^-3. |
| # |
| # These definitions specify the exact numerical value of each constant when |
| # its value is expressed in the corresponding SI unit. By fixing the exact |
| # numerical value the unit becomes defined, since the product of the |
| # numerical value and the unit has to equal the value of the constant, |
| # which is invariant. |
| # |
| # The defining constants have been chosen such that, when taken together, |
| # their units cover all of the units of the SI. In general, there is no |
| # one-to-one correspondence between the defining constants and the SI base |
| # units. Any SI unit is a product of powers of these seven constants and a |
| # dimensionless factor. |
| # |
| # Until 2018, the SI was defined in terms of base units and derived units. |
| # These categories are no longer essential in the SI, but they are maintained |
| # in view of their convenience and widespread use. They are arguably more |
| # intuitive than the new definitions. (They are also essential to the |
| # operation of GNU units.) The definitions of the base units, which follow |
| # from the definition of the SI in terms of the seven defining constants, are |
| # given below. |
| # |
| |
| s ! # The second, symbol s, is the SI unit of time. It is defined |
| second s # by taking the fixed numerical value of the unperturbed |
| # ground-state hyperfine transition frequency of the |
| # cesium-133 atom to be 9 192 631 770 when expressed in the |
| # unit Hz, which is equal to 1/s. |
| # |
| # This definition is a restatement of the previous one, the |
| # duration of 9192631770 periods of the radiation corresponding |
| # to the cesium-133 transition. |
| |
| nu_133Cs 9192631770 Hz # Cesium-133 transition frequency (exact) |
| |
| c_SI 299792458 |
| c 299792458 m/s # speed of light in vacuum (exact) |
| |
| m ! # The metre, symbol m, is the SI unit of length. It is |
| meter m # defined by taking the fixed numerical value of the speed |
| metre m # of light in vacuum, c, to be 299 792 458 when expressed in |
| # units of m/s. |
| # |
| # This definition is a rewording of the previous one and is |
| # equivalent to defining the meter as the distance light |
| # travels in 1|299792458 seconds. The meter was originally |
| # intended to be 1e-7 of the length along a meridian from the |
| # equator to a pole. |
| |
| h_SI 6.62607015e-34 |
| h 6.62607015e-34 J s # Planck constant (exact) |
| |
| kg ! # The kilogram, symbol kg, is the SI unit of mass. It is |
| kilogram kg # defined by taking the fixed numerical value of the Planck |
| # constant, h, to be 6.626 070 15 * 10^-34 when expressed in |
| # the unit J s which is equal to kg m^2 / s. |
| # |
| # One advantage of fixing h to define the kilogram is that this |
| # affects constants used to define the ampere. If the kg were |
| # defined by directly fixing the mass of something, then h |
| # would be subject to error. |
| # |
| # The previous definition of the kilogram was the mass of the |
| # international prototype kilogram. The kilogram was the last |
| # unit whose definition relied on reference to an artifact. |
| # |
| # It is not obvious what this new definition means, or |
| # intuitively how fixing Planck's constant defines the |
| # kilogram. To define the kilogram we need to give the mass |
| # of some reference in kilograms. Previously the prototype in |
| # France served as this reference, and it weighed exactly 1 |
| # kg. But the reference can have any weight as long as you |
| # know the weight of the reference. The new definition uses |
| # the "mass" of a photon, or more accurately, the mass |
| # equivalent of the energy of a photon. The energy of a |
| # photon depends on its frequency. If you pick a frequency, |
| # f, then the energy of the photon is hf, and hence the mass |
| # equivalent is hf/c^2. If we reduce this expression using |
| # the constant defined values for h and c the result is a |
| # value in kilograms for the mass-equivalent of a photon of |
| # frequency f, which can therefore define the size of the |
| # kilogram. |
| # |
| # For more on the relationship between mass an Planck's |
| # constant: |
| # |
| # https://www.nist.gov/si-redefinition/kilogram-mass-and-plancks-constant |
| # This definition may still seem rather abstract: you can't |
| # place a "kilogram of radiation" on one side of a balance. |
| # Metrologists realize the kilogram using a Kibble Balance, a |
| # device which relates mechanical energy to electrical energy |
| # and can measure mass with extreme accuracy if h is known. |
| # |
| # For more on the Kibble Balance see |
| # |
| # https://www.nist.gov/si-redefinition/kilogram-kibble-balance |
| # https://en.wikipedia.org/wiki/Kibble_balance |
| |
| k_SI 1.380649e-23 |
| boltzmann 1.380649e-23 J/K # Boltzmann constant (exact) |
| k boltzmann |
| |
| K ! # The kelvin, symbol K, is the SI unit of thermodynamic |
| kelvin K # temperature. It is defined by taking the fixed numerical |
| # value of the Boltzmann constant, k, to be 1.380 649 * 10^-23 |
| # when expressed in the unit J/K, which is equal to |
| # kg m^2/s^2 K. |
| # |
| # The boltzmann constant establishes the relationship between |
| # energy and temperature. The average thermal energy carried |
| # by each degree of freedom is kT/2. A monatomic ideal gas |
| # has three degrees of freedom corresponding to the three |
| # spatial directions, which means its thermal energy is |
| # (3/2) k T. |
| # |
| # The previous definition of the kelvin was based on the |
| # triple point of water. The change in the definition of the |
| # kelvin will not have much effect on measurement practice. |
| # Practical temperature calibration makes use of two scales, |
| # the International Temperature Scale of 1990 (ITS-90), which |
| # covers the range of 0.65 K to 1357.77K and the Provisional |
| # Low Temperature Scale of 2000 (PLTS-2000), which covers the |
| # range of 0.9 mK to 1 K. |
| # https://www.bipm.org/en/committees/cc/cct/publications-cc.html |
| # |
| # The ITS-90 contains 17 reference points including things |
| # like the triple point of hydrogen (13.8033 K) or the |
| # freezing point of gold (1337.33 K), and of course the triple |
| # point of water. The PLTS-2000 specifies four reference |
| # points, all based on properties of helium-3. |
| # |
| # The redefinition of the kelvin will not affect the values of |
| # these reference points, which have been determined by |
| # primary thermometry, using thermometers that rely only on |
| # relationships that allow temperature to be calculated |
| # directly without using any unknown quantities. Examples |
| # include acoustic thermometers, which measure the speed of |
| # sound in a gas, or electronic thermometers, which measure |
| # tiny voltage fluctuations in resistors. Both variables |
| # depend directly on temperature. |
| |
| e_SI 1.602176634e-19 |
| e 1.602176634e-19 C # electron charge (exact) |
| |
| A ! # The ampere, symbol A, is the SI unit of electric current. |
| ampere A # It is defined by taking the fixed numerical value of the |
| amp ampere # elementary charge, e, to be 1.602 176 634 * 10^-19 when |
| # expressed in the unit C, which is equal to A*s. |
| # |
| # The previous definition was the current which produces a |
| # force of 2e-7 N/m between two infinitely long wires a meter |
| # apart. This definition was difficult to realize accurately. |
| # |
| # The ampere is actually realized by establishing the volt and |
| # the ohm, since A = V / ohm. These measurements can be done |
| # using the Josephson effect and the quantum Hall effect, |
| # which accurately measure voltage and resistance, respectively, |
| # with reference to two fixed constants, the Josephson |
| # constant, K_J=2e/h and the von Klitzing constant, R_K=h/e^2. |
| # Under the previous SI system, these constants had official |
| # fixed values, defined in 1990. This created a situation |
| # where the standard values for the volt and ohm were in some |
| # sense outside of SI because they depended primarily on |
| # constants different from the ones used to define SI. After |
| # the revision, since e and h have exact definitions, the |
| # Josephson and von Klitzing constants will also have exact |
| # definitions that derive from SI instead of the conventional |
| # 1990 values. |
| # |
| # In fact we know that there is a small offset between the |
| # conventional values of the electrical units based on the |
| # conventional 1990 values and the SI values. The new |
| # definition, which brings the practical electrical units back |
| # into SI, will lead to a one time change of +0.1ppm for |
| # voltage values and +0.02ppm for resistance values. |
| # |
| # The previous definition resulted in fixed exact values for |
| # the vacuum permeability (mu0), the impedance of free space |
| # (Z0), the vacuum permittivity (epsilon0), and the Coulomb |
| # constant. With the new definition, these four values are |
| # subject to experimental error. |
| |
| avogadro 6.02214076e23 / mol # Size of a mole (exact) |
| N_A avogadro |
| |
| mol ! # The mole, symbol mol, is the SI unit of amount of |
| mole mol # substance. One mole contains exactly 6.022 140 76 * 10^23 |
| # elementary entities. This number is the fixed numerical |
| # value of the Avogadro constant, N_A, when expressed in the |
| # unit 1/mol and is called the Avogadro number. The amount of |
| # substance, symbol n, of a system is a measure of the number |
| # of specified elementary entities. An elementary entity may |
| # be an atom, a molecule, an ion, an electron, any other |
| # particle or specified group of particles. |
| # |
| # The atomic mass unit (u) is defined as 1/12 the mass of |
| # carbon-12. Previously the mole was defined so that a mole |
| # of carbon-12 weighed exactly 12g, or N_A u = 1 g/mol |
| # exactly. This relationship is now an experimental, |
| # approximate relationship. |
| # |
| # To determine the size of the mole, researchers used spheres |
| # of very pure silicon-28 that weighed a kilogram. They |
| # measured the molar mass of Si-28 using mass spectrometry and |
| # used X-ray diffraction interferometry to determine the |
| # spacing of the silicon atoms in the sphere. Using the |
| # sphere's volume it was then possible to determine the number |
| # of silicon atoms in the sphere, and hence determine the |
| # Avogadro constant. The results of this experiment were used |
| # to define N_A, which is henceforth a fixed, unchanging |
| # quantity. |
| |
| cd ! # The candela, symbol cd, is the SI unit of luminous intensity |
| candela cd # in a given direction. It is defined by taking the fixed |
| # numerical value of the luminous efficacy of monochromatic |
| # radiation of the frequency 540e12 Hz to be 683 when |
| # expressed in the unit lumen/watt, which is equal to |
| # cd sr/W, or cd sr s^3/kg m^2 |
| # |
| # This definition is a rewording of the previous definition. |
| # Luminous intensity differs from radiant intensity (W/sr) in |
| # that it is adjusted for human perceptual dependence on |
| # wavelength. The frequency of 540e12 Hz (yellow; |
| # wavelength approximately 555 nm in vacuum) is where human |
| # perception is most efficient. |
| |
| K_cd 683 lumen/W # Luminous efficiency at 540e12 Hz (exact) |
| |
| # Angular Measure |
| # |
| # The radian and steradian are defined as dimensionless primitive units. |
| # The radian is equal to m/m and the steradian to m^2/m^2 so these units are |
| # dimensionless. Retaining them as named units is useful because it allows |
| # clarity in expressions and makes the meaning of unit definitions more clear. |
| # These units will reduce to 1 in conversions but not for sums of units or for |
| # arguments to functions. |
| # |
| |
| radian !dimensionless # Plane angle subtended at the center of a circle by |
| # an arc equal in length to the radius of the |
| # circle. |
| # Dimension: LENGTH (of arc) / DISTANCE (radius) |
| |
| sr !dimensionless # Solid angle which cuts off an area of the surface |
| steradian sr # of the sphere equal to that of a square with |
| # sides of length equal to the radius of the |
| # sphere. |
| # Dimension: AREA (of surface) / DISTANCE^2 |
| # (radius^2) |
| # |
| # A primitive non-SI unit |
| # |
| |
| bit ! # Basic unit of information (entropy). The entropy in bits |
| # of a random variable over a finite alphabet is defined |
| # to be the sum of -p(i)*log2(p(i)) over the alphabet where |
| # p(i) is the probability that the random variable takes |
| # on the value i. |
| |
| # |
| # Currency: the primitive unit of currency is defined in currency.units. |
| # It is usually the US$ or the euro, but it is user selectable. |
| # |
| |
| # |
| # Absolute value |
| # |
| |
| abs(x) noerror sqrt(x^2) |
| |
| ########################################################################### |
| # # |
| # Prefixes (longer names must come first) # |
| # # |
| ########################################################################### |
| |
| quetta- 1e30 # Allegedly from "q" plus Greek "deka" (ten) |
| ronna- 1e27 # Allegedly from "r" plus Greek "ennea" (nine) |
| yotta- 1e24 # Greek or Latin "octo" (eight) |
| zetta- 1e21 # Latin "septem" (seven) |
| exa- 1e18 # Greek "hex" (six) |
| peta- 1e15 # Greek "pente" (five) |
| tera- 1e12 # Greek "teras" (monster) |
| giga- 1e9 # Greek "gigas" (giant) |
| mega- 1e6 # Greek "megas" (large) |
| myria- 1e4 # Not an official SI prefix |
| kilo- 1e3 # Greek "chilioi" (thousand) |
| hecto- 1e2 # Greek "hekaton" (hundred) |
| deca- 1e1 # Greek "deka" (ten) |
| deka- deca |
| deci- 1e-1 # Latin "decimus" (tenth) |
| centi- 1e-2 # Latin "centum" (hundred) |
| milli- 1e-3 # Latin "mille" (thousand) |
| micro- 1e-6 # Latin "micro" or Greek "mikros" (small) |
| nano- 1e-9 # Latin "nanus" or Greek "nanos" (dwarf) |
| pico- 1e-12 # Spanish "pico" (a bit) |
| femto- 1e-15 # Danish-Norwegian "femten" (fifteen) |
| atto- 1e-18 # Danish-Norwegian "atten" (eighteen) |
| zepto- 1e-21 # Latin "septem" (seven) |
| yocto- 1e-24 # Greek or Latin "octo" (eight) |
| ronto- 1e-27 # Allegedly "r" plus Latin "novum" (nine) |
| quecto- 1e-30 # Allegedly "q" plus Latin "decim" (ten) |
| |
| quarter- 1|4 |
| semi- 0.5 |
| demi- 0.5 |
| hemi- 0.5 |
| half- 0.5 |
| double- 2 |
| triple- 3 |
| treble- 3 |
| |
| kibi- 2^10 # In response to the improper and confusing |
| mebi- 2^20 # use of SI prefixes for powers of two, |
| gibi- 2^30 # the International Electrotechnical |
| tebi- 2^40 # Commission aproved these binary prefixes |
| pebi- 2^50 # in IEC 60027-2 Amendment 2 (1999). |
| exbi- 2^60 |
| zebi- 2^70 # Zebi- and yobi- were added in the 2005 ed., |
| yobi- 2^80 # later superseded by ISO/IEC 80000-13:2008. |
| robi- 2^90 |
| quebi- 2^100 |
| Ki- kibi |
| Mi- mebi |
| Gi- gibi |
| Ti- tebi |
| Pi- pebi |
| Ei- exbi |
| Zi- zebi |
| Yi- yobi |
| Ri- robi |
| Qi- quebi |
| |
| Q- quetta |
| R- ronna |
| Y- yotta |
| Z- zetta |
| E- exa |
| P- peta |
| T- tera |
| G- giga |
| M- mega |
| k- kilo |
| h- hecto |
| da- deka |
| d- deci |
| c- centi |
| m- milli |
| u- micro # it should be a mu but u is easy to type |
| n- nano |
| p- pico |
| f- femto |
| a- atto |
| z- zepto |
| y- yocto |
| r- ronto |
| q- quecto |
| |
| # |
| # Names of some numbers |
| # |
| |
| one 1 |
| two 2 |
| double 2 |
| couple 2 |
| three 3 |
| triple 3 |
| four 4 |
| quadruple 4 |
| five 5 |
| quintuple 5 |
| six 6 |
| seven 7 |
| eight 8 |
| nine 9 |
| ten 10 |
| eleven 11 |
| twelve 12 |
| thirteen 13 |
| fourteen 14 |
| fifteen 15 |
| sixteen 16 |
| seventeen 17 |
| eighteen 18 |
| nineteen 19 |
| twenty 20 |
| thirty 30 |
| forty 40 |
| fifty 50 |
| sixty 60 |
| seventy 70 |
| eighty 80 |
| ninety 90 |
| hundred 100 |
| thousand 1000 |
| million 1e6 |
| |
| twoscore two score |
| threescore three score |
| fourscore four score |
| fivescore five score |
| sixscore six score |
| sevenscore seven score |
| eightscore eight score |
| ninescore nine score |
| tenscore ten score |
| twelvescore twelve score |
| |
| # These number terms were described by N. Chuquet and De la Roche in the 16th |
| # century as being successive powers of a million. These definitions are still |
| # used in most European countries. The current US definitions for these |
| # numbers arose in the 17th century and don't make nearly as much sense. These |
| # numbers are listed in the CRC Concise Encyclopedia of Mathematics by Eric |
| # W. Weisstein. |
| |
| shortbillion 1e9 |
| shorttrillion 1e12 |
| shortquadrillion 1e15 |
| shortquintillion 1e18 |
| shortsextillion 1e21 |
| shortseptillion 1e24 |
| shortoctillion 1e27 |
| shortnonillion 1e30 |
| shortnoventillion shortnonillion |
| shortdecillion 1e33 |
| shortundecillion 1e36 |
| shortduodecillion 1e39 |
| shorttredecillion 1e42 |
| shortquattuordecillion 1e45 |
| shortquindecillion 1e48 |
| shortsexdecillion 1e51 |
| shortseptendecillion 1e54 |
| shortoctodecillion 1e57 |
| shortnovemdecillion 1e60 |
| shortvigintillion 1e63 |
| |
| centillion 1e303 |
| googol 1e100 |
| |
| longbillion million^2 |
| longtrillion million^3 |
| longquadrillion million^4 |
| longquintillion million^5 |
| longsextillion million^6 |
| longseptillion million^7 |
| longoctillion million^8 |
| longnonillion million^9 |
| longnoventillion longnonillion |
| longdecillion million^10 |
| longundecillion million^11 |
| longduodecillion million^12 |
| longtredecillion million^13 |
| longquattuordecillion million^14 |
| longquindecillion million^15 |
| longsexdecillion million^16 |
| longseptdecillion million^17 |
| longoctodecillion million^18 |
| longnovemdecillion million^19 |
| longvigintillion million^20 |
| |
| # These numbers fill the gaps left by the long system above. |
| |
| milliard 1000 million |
| billiard 1000 million^2 |
| trilliard 1000 million^3 |
| quadrilliard 1000 million^4 |
| quintilliard 1000 million^5 |
| sextilliard 1000 million^6 |
| septilliard 1000 million^7 |
| octilliard 1000 million^8 |
| nonilliard 1000 million^9 |
| noventilliard nonilliard |
| decilliard 1000 million^10 |
| |
| # For consistency |
| |
| longmilliard milliard |
| longbilliard billiard |
| longtrilliard trilliard |
| longquadrilliard quadrilliard |
| longquintilliard quintilliard |
| longsextilliard sextilliard |
| longseptilliard septilliard |
| longoctilliard octilliard |
| longnonilliard nonilliard |
| longnoventilliard noventilliard |
| longdecilliard decilliard |
| |
| # The long centillion would be 1e600. The googolplex is another |
| # familiar large number equal to 10^googol. These numbers give overflows. |
| |
| # |
| # The short system prevails in English speaking countries |
| # |
| |
| billion shortbillion |
| trillion shorttrillion |
| quadrillion shortquadrillion |
| quintillion shortquintillion |
| sextillion shortsextillion |
| septillion shortseptillion |
| octillion shortoctillion |
| nonillion shortnonillion |
| noventillion shortnoventillion |
| decillion shortdecillion |
| undecillion shortundecillion |
| duodecillion shortduodecillion |
| tredecillion shorttredecillion |
| quattuordecillion shortquattuordecillion |
| quindecillion shortquindecillion |
| sexdecillion shortsexdecillion |
| septendecillion shortseptendecillion |
| octodecillion shortoctodecillion |
| novemdecillion shortnovemdecillion |
| vigintillion shortvigintillion |
| |
| # |
| # Numbers used in India |
| # |
| |
| lakh 1e5 |
| crore 1e7 |
| arab 1e9 |
| kharab 1e11 |
| neel 1e13 |
| padm 1e15 |
| shankh 1e17 |
| |
| ############################################################################# |
| # # |
| # Derived units which can be reduced to the primitive units # |
| # # |
| ############################################################################# |
| |
| |
| |
| # |
| # Named SI derived units (officially accepted) |
| # |
| |
| newton kg m / s^2 # force |
| N newton |
| pascal N/m^2 # pressure or stress |
| Pa pascal |
| joule N m # energy |
| J joule |
| watt J/s # power |
| W watt |
| coulomb A s # charge |
| C coulomb |
| volt W/A # potential difference |
| V volt |
| ohm V/A # electrical resistance |
| siemens A/V # electrical conductance |
| S siemens |
| farad C/V # capacitance |
| F farad |
| weber V s # magnetic flux |
| Wb weber |
| henry V s / A # inductance, also Wb/A, but needs to be |
| H henry # defined this way for CGS units |
| tesla Wb/m^2 # magnetic flux density |
| T tesla |
| hertz /s # frequency |
| Hz hertz |
| |
| # |
| # Dimensions. These are here to help with dimensional analysis and |
| # because they will appear in the list produced by hitting '?' at the |
| # "You want:" prompt to tell the user the dimension of the unit. |
| # |
| |
| LENGTH meter |
| AREA LENGTH^2 |
| VOLUME LENGTH^3 |
| MASS kilogram |
| AMOUNT mole |
| ANGLE radian |
| SOLID_ANGLE steradian |
| MONEY US$ |
| FORCE newton |
| PRESSURE FORCE / AREA |
| STRESS FORCE / AREA |
| FREQUENCY hertz |
| WAVELENGTH LENGTH |
| WAVENUMBER 1/WAVELENGTH # number of waves per distance |
| VELOCITY DISPLACEMENT / TIME # a vector (includes direction) |
| SPEED DISTANCE / TIME # a scalar |
| ACCELERATION VELOCITY / TIME |
| MOMENTUM MASS VELOCITY # Also ENERGY / VELOCITY or IMPULSE |
| IMPULSE FORCE TIME |
| DISPLACEMENT LENGTH |
| DISTANCE LENGTH |
| ELONGATION LENGTH |
| STRAIN ELONGATION / LENGTH |
| ENERGY joule |
| POWER watt |
| WORK FORCE DISTANCE |
| DENSITY MASS / VOLUME |
| LINEAR_DENSITY MASS / LENGTH |
| SPECIFIC_ENERGY ENERGY / MASS |
| VISCOSITY FORCE TIME / AREA |
| KINEMATIC_VISCOSITY VISCOSITY / DENSITY |
| CURRENT ampere |
| CHARGE coulomb |
| CAPACITANCE farad |
| RESISTANCE ohm |
| CONDUCTANCE siemens |
| # It may be easier to understand the relationship by considering |
| # an object with specified dimensions and resistivity, whose |
| # resistance is given by the resistivity * length / area. |
| RESISTIVITY RESISTANCE AREA / LENGTH |
| CONDUCTIVITY CONDUCTANCE LENGTH / AREA |
| INDUCTANCE henry |
| E_FIELD ELECTRIC_POTENTIAL / LENGTH |
| B_FIELD tesla |
| # The D and H fields are related to the E and B fields by factors of |
| # epsilon and mu respectively, so their units can be found by |
| # multiplying/dividing by the epsilon0 and mu0. The more complex |
| # definitions below make it possible to use D_FIELD and E_FIELD to |
| # convert between SI and CGS units for these dimensions. |
| D_FIELD E_FIELD epsilon0 / epsilon0_SI # mu0_SI c^2 F / m |
| H_FIELD B_FIELD / (mu0/mu0_SI) |
| ELECTRIC_DIPOLE_MOMENT C m |
| MAGNETIC_DIPOLE_MOMENT J / T |
| POLARIZATION ELECTRIC_DIPOLE_MOMENT / VOLUME |
| MAGNETIZATION MAGNETIC_DIPOLE_MOMENT / VOLUME |
| ELECTRIC_POTENTIAL ENERGY / CHARGE #volt |
| VOLTAGE ELECTRIC_POTENTIAL |
| E_FLUX E_FIELD AREA |
| D_FLUX D_FIELD AREA |
| B_FLUX B_FIELD AREA |
| H_FLUX H_FIELD AREA |
| |
| # |
| # units derived easily from SI units |
| # |
| |
| gram millikg |
| gm gram |
| g gram |
| tonne 1000 kg |
| t tonne |
| metricton tonne |
| sthene tonne m / s^2 |
| funal sthene |
| pieze sthene / m^2 |
| quintal 100 kg |
| bar 1e5 Pa # About 1 atm |
| b bar |
| vac millibar |
| micron micrometer # One millionth of a meter |
| bicron picometer # One brbillionth of a meter |
| cc cm^3 |
| are 100 m^2 |
| a are |
| liter 1000 cc # The liter was defined in 1901 as the |
| oldliter 1.000028 dm^3 # space occupied by 1 kg of pure water at |
| L liter # the temperature of its maximum density |
| l liter # under a pressure of 1 atm. This was |
| # supposed to be 1000 cubic cm, but it |
| # was discovered that the original |
| # measurement was off. In 1964, the |
| # liter was redefined to be exactly 1000 |
| # cubic centimeters. |
| Ah amp hour # Unit of charge |
| mho siemens # Inverse of ohm, hence ohm spelled backward |
| galvat ampere # Named after Luigi Galvani |
| angstrom 1e-10 m # Convenient for describing molecular sizes |
| xunit xunit_cu # Used for measuring x-ray wavelengths. |
| siegbahn xunit # Originally defined to be 1|3029.45 of |
| xunit_cu 1.00207697e-13 m # the spacing of calcite planes at 18 |
| xunit_mo 1.00209952e-13 m # degC. It was intended to be exactly |
| # 1e-13 m, but was later found to be |
| # slightly off. Current usage is with |
| # reference to common x-ray lines, either |
| # the K-alpha 1 line of copper or the |
| # same line of molybdenum. |
| angstromstar 1.00001495 angstrom # Defined by JA Bearden in 1965 to replace |
| # the X unit. The wavelength of the |
| # tungsten K alpha1 line was defined as |
| # exactly 0.20901 angstrom star, with the |
| # value chosen to try to make the new |
| # unit close to the angstrom. |
| silicon_d220 1.920155716e-10 m # Silicon lattice spacing |
| siliconlattice sqrt(8) silicon_d220# Silicon lattice parameter, (a), the side |
| # length of the unit cell for the diamond |
| # centered cubic structure of silicon. |
| fermi 1e-15 m # Convenient for describing nuclear sizes |
| # Nuclear radius is from 1 to 10 fermis |
| barn 1e-28 m^2 # Used to measure cross section for |
| # particle physics collision, said to |
| # have originated in the phrase "big as |
| # a barn". |
| shed 1e-24 barn # Defined to be a smaller companion to the |
| # barn, but it's too small to be of |
| # much use. |
| brewster micron^2/N # measures stress-optical coef |
| diopter /m # measures reciprocal of lens focal length |
| fresnel 1e12 Hz # occasionally used in spectroscopy |
| shake 1e-8 sec |
| svedberg 1e-13 s # Used for measuring the sedimentation |
| # coefficient for centrifuging. |
| gamma microgram # Also used for 1e-9 tesla |
| lambda microliter |
| spat 1e12 m # Rarely used for astronomical measurements |
| preece 1e13 ohm m # resistivity |
| planck J s # action of one joule over one second |
| sturgeon /henry # magnetic reluctance |
| daraf 1/farad # elastance (farad spelled backwards) |
| leo 10 m/s^2 |
| poiseuille N s / m^2 # viscosity |
| mayer J/g K # specific heat |
| mired / microK # reciprocal color temperature. The name |
| # abbreviates micro reciprocal degree. |
| crocodile megavolt # used informally in UK physics labs |
| metricounce 25 g |
| mounce metricounce |
| finsenunit 1e5 W/m^2 # Measures intensity of ultraviolet light |
| # with wavelength 296.7 nm. |
| fluxunit 1e-26 W/m^2 Hz # Used in radio astronomy to measure |
| # the energy incident on the receiving |
| # body across a specified frequency |
| # bandwidth. [12] |
| jansky fluxunit # K. G. Jansky identified radio waves coming |
| Jy jansky # from outer space in 1931. |
| flick W / cm^2 sr micrometer # Spectral radiance or irradiance |
| pfu / cm^2 sr s # particle flux unit -- Used to measure |
| # rate at which particles are received by |
| # a spacecraft as particles per solid |
| # angle per detector area per second. [18] |
| pyron cal_IT / cm^2 min # Measures heat flow from solar radiation, |
| # from Greek work "pyr" for fire. |
| katal mol/sec # Measure of the amount of a catalyst. One |
| kat katal # katal of catalyst enables the reaction |
| # to consume or produce one mol/sec. |
| solarluminosity 382.8e24 W # A common yardstick for comparing the |
| # output of different stars. |
| # http://nssdc.gsfc.nasa.gov/planetary/factsheet/sunfact.html |
| # at mean Earth-Sun distance |
| solarirradiance solarluminosity / (4 pi sundist^2) |
| solarconstant solarirradiance |
| TSI solarirradiance # total solar irradiance |
| |
| # |
| # time |
| # |
| |
| sec s |
| minute 60 s |
| min minute |
| hour 60 min |
| hr hour |
| day 24 hr |
| d day |
| da day |
| week 7 day |
| wk week |
| sennight 7 day |
| fortnight 14 day |
| blink 1e-5 day # Actual human blink takes 1|3 second |
| ce 1e-2 day |
| cron 1e6 years |
| watch 4 hours # time a sentry stands watch or a ship's |
| # crew is on duty. |
| bell 1|8 watch # Bell would be sounded every 30 minutes. |
| |
| # French Revolutionary Time or Decimal Time. It was Proposed during |
| # the French Revolution. A few clocks were made, but it never caught |
| # on. In 1998 Swatch defined a time measurement called ".beat" and |
| # sold some watches that displayed time in this unit. |
| |
| decimalhour 1|10 day |
| decimalminute 1|100 decimalhour |
| decimalsecond 1|100 decimalminute |
| beat decimalminute # Swatch Internet Time |
| |
| # |
| # angular measure |
| # |
| |
| circle 2 pi radian |
| degree 1|360 circle |
| deg degree |
| arcdeg degree |
| arcmin 1|60 degree |
| arcminute arcmin |
| ' arcmin |
| arcsec 1|60 arcmin |
| arcsecond arcsec |
| " arcsec |
| '' " |
| rightangle 90 degrees |
| quadrant 1|4 circle |
| quintant 1|5 circle |
| sextant 1|6 circle |
| |
| sign 1|12 circle # Angular extent of one sign of the zodiac |
| turn circle |
| revolution turn |
| rev turn |
| pulsatance radian / sec |
| gon 1|100 rightangle # measure of grade |
| grade gon |
| centesimalminute 1|100 grade |
| centesimalsecond 1|100 centesimalminute |
| milangle 1|6400 circle # Official NIST definition. |
| # Another choice is 1e-3 radian. |
| pointangle 1|32 circle # Used for reporting compass readings |
| centrad 0.01 radian # Used for angular deviation of light |
| # through a prism. |
| mas milli arcsec # Used by astronomers |
| seclongitude circle (seconds/day) # Astronomers measure longitude |
| # (which they call right ascension) in |
| # time units by dividing the equator into |
| # 24 hours instead of 360 degrees. |
| # |
| # Some geometric formulas |
| # |
| |
| circlearea(r) units=[m;m^2] range=[0,) pi r^2 ; sqrt(circlearea/pi) |
| spherevolume(r) units=[m;m^3] range=[0,) 4|3 pi r^3 ; \ |
| cuberoot(spherevolume/4|3 pi) |
| spherevol() spherevolume |
| square(x) range=[0,) x^2 ; sqrt(square) |
| |
| # |
| # Solid angle measure |
| # |
| |
| sphere 4 pi sr |
| squaredegree 1|180^2 pi^2 sr |
| squareminute 1|60^2 squaredegree |
| squaresecond 1|60^2 squareminute |
| squarearcmin squareminute |
| squarearcsec squaresecond |
| sphericalrightangle 1|8 sphere |
| octant 1|8 sphere |
| |
| # |
| # Concentration measures |
| # |
| |
| percent 0.01 |
| % percent |
| mill 0.001 # Originally established by Congress in 1791 |
| # as a unit of money equal to 0.001 dollars, |
| # it has come to refer to 0.001 in general. |
| # Used by some towns to set their property |
| # tax rate, and written with a symbol similar |
| # to the % symbol but with two 0's in the |
| # denominator. [18] |
| proof 1|200 # Alcohol content measured by volume at |
| # 60 degrees Fahrenheit. This is a USA |
| # measure. In Europe proof=percent. |
| ppm 1e-6 |
| partspermillion ppm |
| ppb 1e-9 |
| partsperbillion ppb # USA billion |
| ppt 1e-12 |
| partspertrillion ppt # USA trillion |
| karat 1|24 # measure of gold purity |
| caratgold karat |
| gammil mg/l |
| basispoint 0.01 % # Used in finance |
| fine 1|1000 # Measure of gold purity |
| |
| # The pH scale is used to measure the concentration of hydronium (H3O+) ions in |
| # a solution. A neutral solution has a pH of 7 as a result of dissociated |
| # water molecules. |
| |
| pH(x) units=[1;mol/liter] range=(0,) 10^(-x) mol/liter ; (-log(pH liters/mol)) |
| |
| |
| # |
| # Temperature |
| # |
| # Two types of units are defined: units for converting temperature differences |
| # and functions for converting absolute temperatures. Conversions for |
| # differences start with "deg" and conversions for absolute temperature start |
| # with "temp". |
| # |
| # If the temperature inside is 72 degrees Fahrenheit and you want to |
| # convert this to degrees Celsius then you need absolute temperature: |
| # |
| # You have: tempF(72) |
| # You want: tempC |
| # 22.222222 |
| # |
| # If the temperature rose 72 degrees Fahrenheit during the chemical reaction |
| # then this is a temperature difference: |
| # |
| # You have: 72 degF |
| # You want: degC |
| # * 40 |
| # / 0.025 |
| # |
| |
| TEMPERATURE kelvin |
| TEMPERATURE_DIFFERENCE kelvin |
| |
| # In 1741 Anders Celsius introduced a temperature scale with water boiling at |
| # 0 degrees and freezing at 100 degrees at standard pressure. After his death |
| # the fixed points were reversed and the scale was called the centigrade |
| # scale. Due to the difficulty of accurately measuring the temperature of |
| # melting ice at standard pressure, the centigrade scale was replaced in 1954 |
| # by the Celsius scale which is defined by subtracting 273.15 from the |
| # temperature in Kelvins. This definition differed slightly from the old |
| # centigrade definition, but the Kelvin scale depends on the triple point of |
| # water rather than a melting point, so it can be measured accurately. |
| |
| tempC(x) units=[1;K] domain=[-273.15,) range=[0,) \ |
| x K + stdtemp ; (tempC +(-stdtemp))/K |
| tempcelsius() tempC |
| degcelsius K |
| degC K |
| |
| # Fahrenheit defined his temperature scale by setting 0 to the coldest |
| # temperature he could produce in his lab with a salt water solution and by |
| # setting 96 degrees to body heat. In Fahrenheit's words: |
| # |
| # Placing the thermometer in a mixture of sal ammoniac or sea |
| # salt, ice, and water a point on the scale will be found which |
| # is denoted as zero. A second point is obtained if the same |
| # mixture is used without salt. Denote this position as 30. A |
| # third point, designated as 96, is obtained if the thermometer |
| # is placed in the mouth so as to acquire the heat of a healthy |
| # man." (D. G. Fahrenheit, Phil. Trans. (London) 33, 78, 1724) |
| |
| tempF(x) units=[1;K] domain=[-459.67,) range=[0,) \ |
| (x+(-32)) degF + stdtemp ; (tempF+(-stdtemp))/degF + 32 |
| tempfahrenheit() tempF |
| degfahrenheit 5|9 degC |
| degF 5|9 degC |
| |
| |
| degreesrankine degF # The Rankine scale has the |
| degrankine degreesrankine # Fahrenheit degree, but its zero |
| degreerankine degF # is at absolute zero. |
| degR degrankine |
| tempR degrankine |
| temprankine degrankine |
| |
| tempreaumur(x) units=[1;K] domain=[-218.52,) range=[0,) \ |
| x degreaumur+stdtemp ; (tempreaumur+(-stdtemp))/degreaumur |
| degreaumur 10|8 degC # The Reaumur scale was used in Europe and |
| # particularly in France. It is defined |
| # to be 0 at the freezing point of water |
| # and 80 at the boiling point. Reaumur |
| # apparently selected 80 because it is |
| # divisible by many numbers. |
| |
| degK K # "Degrees Kelvin" is forbidden usage. |
| tempK K # For consistency |
| |
| # Gas mark is implemented below but in a terribly ugly way. There is |
| # a simple formula, but it requires a conditional which is not |
| # presently supported. |
| # |
| # The formula to convert to degrees Fahrenheit is: |
| # |
| # 25 log2(gasmark) + k_f gasmark<=1 |
| # 25 (gasmark-1) + k_f gasmark>=1 |
| # |
| # k_f = 275 |
| # |
| gasmark[degR] \ |
| .0625 634.67 \ |
| .125 659.67 \ |
| .25 684.67 \ |
| .5 709.67 \ |
| 1 734.67 \ |
| 2 759.67 \ |
| 3 784.67 \ |
| 4 809.67 \ |
| 5 834.67 \ |
| 6 859.67 \ |
| 7 884.67 \ |
| 8 909.67 \ |
| 9 934.67 \ |
| 10 959.67 |
| |
| |
| # The Beaufort wind force scale was developed from 1805-1807 by Sir Francis |
| # Beaufort to categorize wind conditions at sea. It is normally defined from |
| # Beaufort 0, also called "Force 0," through Beaufort 12. Beaufort numbers |
| # 13-17 were later defined for tropical cyclones but are rarely used. The |
| # original Beaufort scale was qualitative and did not relate directly to wind |
| # speed. In 1906, George Simpson of the British Met Office fit wind-speed |
| # measurements to visual Beaufort estimates made from five coastal and inland |
| # stations in Britain. Simpson's formula was adopted by the World Meterological |
| # Organization in 1946 to produce a table, known as WMO Code 1100, giving mean |
| # (and min/max) wind speed equivalents at a height of 10 meters for each |
| # Beaufort number. This is the "operational" Beaufort scale that mariners |
| # use. Meterological and climatic researchers typically use a "scientific" |
| # Beaufort scale based on more recent and comprehensive fits. See Wallbrink and |
| # Cook, Historical Wind Speed Equivalents Of The Beaufort Scale, 1850-1950, at |
| # https://icoads.noaa.gov/reclaim/pdf/Hisklim13.pdf |
| # |
| beaufort_WMO1100(B) units=[1;m/s] domain=[0,17] range=[0,) \ |
| 0.836 B^3|2 m/s; (beaufort_WMO1100 s / 0.836 m)^2|3 |
| |
| beaufort(B) units=[1;m/s] domain=[0,17] range=[0,) \ |
| beaufort_WMO1100(B); ~beaufort_WMO1100(beaufort) |
| |
| # Units cannot handle wind chill or heat index because they are two-variable |
| # functions, but they are included here for your edification. Clearly these |
| # equations are the result of a model fitting operation. |
| # |
| # wind chill index (WCI) a measurement of the combined cooling effect of low |
| # air temperature and wind on the human body. The index was first defined |
| # by the American Antarctic explorer Paul Siple in 1939. As currently used |
| # by U.S. meteorologists, the wind chill index is computed from the |
| # temperature T (in deg F) and wind speed V (in mi/hr) using the formula: |
| # WCI = 0.0817(3.71 sqrt(V) + 5.81 - 0.25V)(T - 91.4) + 91.4. |
| # For very low wind speeds, below 4 mi/hr, the WCI is actually higher than |
| # the air temperature, but for higher wind speeds it is lower than the air |
| # temperature. |
| # |
| # heat index (HI or HX) a measure of the combined effect of heat and |
| # humidity on the human body. U.S. meteorologists compute the index |
| # from the temperature T (in deg F) and the relative humidity H (as a |
| # value from 0 to 1). |
| # HI = -42.379 + 2.04901523 T + 1014.333127 H - 22.475541 TH |
| # - .00683783 T^2 - 548.1717 H^2 + 0.122874 T^2 H + 8.5282 T H^2 |
| # - 0.0199 T^2 H^2. |
| |
| # |
| # Physical constants |
| # |
| |
| # Basic constants |
| |
| pi 3.14159265358979323846 |
| tau 2 pi |
| phi (sqrt(5)+1)/2 |
| light c |
| coulombconst alpha hbar c / e^2 # Coulomb constant |
| k_C coulombconst # Gets overridden in CGS modes |
| k_C_SI alpha hbar_SI c_SI / e_SI^2 |
| epsilon0_SI 1 / 4 pi k_C_SI # Vacuum electric permittivity |
| epsilon0 1 / 4 pi k_C # Also overridden in CGS modes |
| mu0_SI 1 / epsilon0_SI c_SI^2 # Vacuum magnetic permeability |
| mu0 1 / epsilon0 c^2 # Also overridden in CGS modes |
| Z0 4 pi k_C / c # Free space impedance |
| energy c^2 # Convert mass to energy |
| hbar h / 2 pi |
| hbar_SI h_SI / 2 pi |
| spin hbar |
| G_SI 6.67430e-11 |
| G 6.67430e-11 N m^2 / kg^2 # Newtonian gravitational constant |
| |
| # Physico-chemical constants |
| |
| atomicmassunit_SI 1.66053906660e-27 # Unified atomic mass unit, defined as |
| atomicmassunit 1.66053906660e-27 kg # Unified atomic mass unit, defined as |
| u atomicmassunit # 1|12 of the mass of carbon 12. |
| amu atomicmassunit # The relationship N_A u = 1 g/mol |
| dalton u # is approximately, but not exactly |
| Da dalton # true (with the 2019 SI). |
| # Previously the mole was defined to |
| # make this relationship exact. |
| amu_chem 1.66026e-27 kg # 1|16 of the weighted average mass of |
| # the 3 naturally occuring neutral |
| # isotopes of oxygen |
| amu_phys 1.65981e-27 kg # 1|16 of the mass of a neutral |
| # oxygen 16 atom |
| gasconstant k N_A # Molar gas constant (exact) |
| R gasconstant |
| kboltzmann boltzmann |
| molarvolume R stdtemp / atm # Volume occupied by one mole of an |
| V_m molarvolume # ideal gas at STP. (exact) |
| loschmidt avogadro / molarvolume # Molecules per cubic meter of an |
| n0 loschmidt # ideal gas at STP. Loschmidt did |
| # work similar to Avogadro. |
| molarvolume_si N_A siliconlattice^3 / 8 # Volume of a mole of crystalline |
| # silicon. The unit cell contains 8 |
| # silicon atoms and has a side |
| # length of siliconlattice. |
| stefanboltzmann pi^2 k^4 / 60 hbar^3 c^2 # The power per area radiated by a |
| sigma stefanboltzmann # blackbody at temperature T is |
| # given by sigma T^4. (exact) |
| wiendisplacement (h c/k)/4.9651142317442763 # Wien's Displacement Law gives |
| # the frequency at which the |
| # Planck spectrum has maximum |
| # intensity. The relation is lambda |
| # T = b where lambda is wavelength, |
| # T is temperature and b is the Wien |
| # displacement. This relation is |
| # used to determine the temperature |
| # of stars. The constant is the |
| # solution to x=5(1-exp(-x)). |
| # This expression has no experimental |
| # error, and x is defined exactly |
| # by the equation above, so it is |
| # an exact definition. |
| K_J90 483597.9 GHz/V # Direct measurement of the volt is difficult. Until |
| K_J 2e/h # recently, laboratories kept Weston cadmium cells as |
| # a reference, but they could drift. In 1987 the |
| # CGPM officially recommended the use of the |
| # Josephson effect as a laboratory representation of |
| # the volt. The Josephson effect occurs when two |
| # superconductors are separated by a thin insulating |
| # layer. A "supercurrent" flows across the insulator |
| # with a frequency that depends on the potential |
| # applied across the superconductors. This frequency |
| # can be very accurately measured. The Josephson |
| # constant K_J relates the measured frequency to the |
| # potential. Two values given, the conventional |
| # (exact) value from 1990, which was used until the |
| # 2019 SI revision, and the current exact value. |
| R_K90 25812.807 ohm # Measurement of the ohm also presents difficulties. |
| R_K h/e^2 # The old approach involved maintaining resistances |
| # that were subject to drift. The new standard is |
| # based on the Hall effect. When a current carrying |
| # ribbon is placed in a magnetic field, a potential |
| # difference develops across the ribbon. The ratio |
| # of the potential difference to the current is |
| # called the Hall resistance. Klaus von Klitzing |
| # discovered in 1980 that the Hall resistance varies |
| # in discrete jumps when the magnetic field is very |
| # large and the temperature very low. This enables |
| # accurate realization of the resistance h/e^2 in the |
| # lab. The 1990 value was an exact conventional |
| # value used until the SI revision in 2019. This value |
| # did not agree with measurements. The new value |
| # is exact. |
| |
| # The 2019 update to SI gives exact definitions for R_K and K_J. Previously |
| # the electromagnetic units were realized using the 1990 conventional values |
| # for these constants, and as a result, the standard definitions were in some |
| # sense outside of SI. The revision corrects this problem. The definitions |
| # below give the 1990 conventional values for the electromagnetic units in |
| # terms of 2019 SI. |
| |
| ampere90 (K_J90 R_K90 / K_J R_K) A |
| coulomb90 (K_J90 R_K90 / K_J R_K) C |
| farad90 (R_K90/R_K) F |
| henry90 (R_K/R_K90) H |
| ohm90 (R_K/R_K90) ohm |
| volt90 (K_J90/K_J) V |
| watt90 (K_J90^2 R_K90 / K_J^2 R_K) W |
| |
| # Various conventional values |
| |
| gravity 9.80665 m/s^2 # std acceleration of gravity (exact) |
| # Established by the 3rd CGPM in |
| # 1901. This is a nominal midrange |
| # value, originally based on the |
| # acceleration of a body at sea |
| # level at 45 degrees latitude. |
| # The value was actually determined |
| # by measuring at the International |
| # Bureau and correcting the |
| # measurement by a theoretical |
| # cofficient to get the 45 deg |
| # latitude sea level value. |
| # (Wikipedia: Standard gravity) |
| force gravity # use to turn masses into forces |
| atm 101325 Pa # Standard atmospheric pressure |
| atmosphere atm |
| Hg 13.5951 gram force / cm^3 # Standard weight of mercury (exact) |
| water gram force/cm^3 # Standard weight of water (exact) |
| waterdensity gram / cm^3 # Density of water |
| H2O water |
| wc water # water column |
| mach 331.46 m/s # speed of sound in dry air at STP |
| standardtemp 273.15 K # standard temperature |
| stdtemp standardtemp |
| normaltemp tempF(70) # for gas density, from NIST |
| normtemp normaltemp # Handbook 44 |
| |
| # Weight of mercury and water at different temperatures using the standard |
| # force of gravity. |
| |
| Hg10C 13.5708 force gram / cm^3 # These units, when used to form |
| Hg20C 13.5462 force gram / cm^3 # pressure measures, are not accurate |
| Hg23C 13.5386 force gram / cm^3 # because of considerations of the |
| Hg30C 13.5217 force gram / cm^3 # revised practical temperature scale. |
| Hg40C 13.4973 force gram / cm^3 |
| Hg60F 13.5574 force gram / cm^3 |
| H2O0C 0.99987 force gram / cm^3 |
| H2O5C 0.99999 force gram / cm^3 |
| H2O10C 0.99973 force gram / cm^3 |
| H2O15C 0.99913 force gram / cm^3 |
| H2O18C 0.99862 force gram / cm^3 |
| H2O20C 0.99823 force gram / cm^3 |
| H2O25C 0.99707 force gram / cm^3 |
| H2O50C 0.98807 force gram / cm^3 |
| H2O100C 0.95838 force gram / cm^3 |
| |
| # Atomic constants |
| |
| hartree 4.3597447222071e-18 J # Approximate electric potential energy |
| E_h hartree # of the hydrogen atom in its ground |
| # state, and approximately twice its |
| # ionization energy. The hartree |
| # energy is traditionally defined as |
| # coulombconst^2 m_e e^4 / hbar^2, |
| # but it can be measured to greater |
| # precision using the relationship |
| # hartree = 2 h c Rinfinity |
| # because Rinfinity is one of the |
| # most accurately measured physical |
| # constants. Because h and c are |
| # exact we can choose either hartree |
| # or Rinfinity from CODATA to use as |
| # the primary value without |
| # affecting the precision. |
| Rinfinity hartree / 2 h c # The wavelengths of a spectral series |
| R_H Rinfinity m_p / (m_e + m_p) # can be expressed as |
| # 1/lambda = R (1/m^2 - 1/n^2). |
| # where R is a number that various |
| # slightly from element to element. |
| # For hydrogen, R_H is the value, |
| # and for heavy elements, the value |
| # approaches Rinfinity, which can be |
| # computed from |
| # Rinfinity = m_e c alpha^2 / 2 h |
| # with loss of precision. Rinfinity |
| # is one of the most accurately |
| # measured physical constants and is |
| # known to higher precision than m_e |
| # or alpha. |
| alpha 7.2973525693e-3 # The fine structure constant was |
| # introduced to explain fine |
| # structure visible in spectral |
| # lines. |
| bohrradius hbar / alpha m_e c |
| a0 bohrradius |
| prout 185.5 keV # nuclear binding energy equal to 1|12 |
| # binding energy of the deuteron |
| conductancequantum e^2 / pi hbar |
| G0 conductancequantum |
| magneticfluxquantum pi hbar / e |
| Phi0 magneticfluxquantum |
| |
| # Particle radius |
| |
| electronradius coulombconst e^2 / electronmass c^2 # Classical |
| deuteronchargeradius 2.12799e-15 m |
| protonchargeradius 0.8751e-15 m |
| |
| # Masses of elementary particles |
| |
| electronmass_SI electronmass_u atomicmassunit_SI |
| electronmass_u 5.48579909065e-4 |
| electronmass 5.48579909065e-4 u |
| m_e electronmass |
| muonmass 0.1134289259 u |
| m_mu muonmass |
| taumass 1.90754 u |
| m_tau taumass |
| protonmass 1.007276466621 u |
| m_p protonmass |
| neutronmass 1.00866491595 u |
| m_n neutronmass |
| deuteronmass 2.013553212745 u # Nucleus of deuterium, one |
| m_d deuteronmass # proton and one neutron |
| alphaparticlemass 4.001506179127 u # Nucleus of He, two protons |
| m_alpha alphaparticlemass # and two neutrons |
| tritonmass 3.01550071621 u # Nucleus of H3, one proton |
| m_t tritonmass # and two neutrons |
| helionmass 3.014932247175 u # Nucleus of He3, two protons |
| m_h helionmass # and one neutron |
| |
| # particle wavelengths: the compton wavelength of a particle is |
| # defined as h / m c where m is the mass of the particle. |
| |
| electronwavelength h / m_e c |
| lambda_C electronwavelength |
| protonwavelength h / m_p c |
| lambda_C,p protonwavelength |
| neutronwavelength h / m_n c |
| lambda_C,n neutronwavelength |
| muonwavelength h / m_mu c |
| lambda_C,mu muonwavelength |
| |
| # The g-factor or dimensionless magnetic moment is a quantity that |
| # characterizes the magnetic moment of a particle. The electron g-factor is |
| # one of the most precisely measured values in physics, with a relative |
| # uncertainty of 1.7e-13. |
| |
| g_d 0.8574382338 # Deuteron g-factor |
| g_e -2.00231930436256 # Electron g-factor |
| g_h -4.255250615 # Helion g-factor |
| g_mu -2.0023318418 # Muon g-factor |
| g_n -3.82608545 # Neutron g-factor |
| g_p 5.5856946893 # Proton g-factor |
| g_t 5.957924931 # Triton g-factor |
| |
| fermicoupling 1.1663787e-5 / GeV^2 |
| |
| # Magnetic moments (derived from the more accurate g-factors) |
| # |
| # The magnetic moment is g * mu_ref * spin where in most cases |
| # the reference is the nuclear magneton, and all of the particles |
| # except the deuteron have spin 1/2. |
| |
| bohrmagneton e hbar / 2 electronmass # Reference magnetic moment for |
| mu_B bohrmagneton # the electron |
| mu_e g_e mu_B / 2 # Electron spin magnet moment |
| mu_mu g_mu mu_B m_e / 2 muonmass # Muon spin magnetic moment |
| nuclearmagneton mu_B m_e / protonmass # Convenient reference magnetic |
| mu_N nuclearmagneton # moment for heavy particles |
| mu_p g_p mu_N / 2 # Proton magnetic moment |
| mu_n g_n mu_N / 2 # Neutron magnetic moment |
| mu_d g_d mu_N # Deuteron magnetic moment, spin 1 |
| mu_t g_t mu_N / 2 # Triton magnetic moment |
| mu_h g_h mu_N / 2 # Helion magnetic moment |
| |
| # |
| # Units derived from physical constants |
| # |
| |
| kgf kg force |
| technicalatmosphere kgf / cm^2 |
| at technicalatmosphere |
| hyl kgf s^2 / m # Also gram-force s^2/m according to [15] |
| mmHg mm Hg |
| torr atm / 760 # The torr, named after Evangelista |
| # Torricelli, and is very close to the mm Hg |
| tor Pa # Suggested in 1913 but seldom used [24]. |
| # Eventually renamed the Pascal. Don't |
| # confuse the tor with the torr. |
| inHg inch Hg |
| inH2O inch water |
| mmH2O mm water |
| eV e V # Energy acquired by a particle with charge e |
| electronvolt eV # when it is accelerated through 1 V |
| lightyear c julianyear # The 365.25 day year is specified in |
| ly lightyear # NIST publication 811 |
| lightsecond c s |
| lightminute c min |
| parsec au / tan(arcsec) # Unit of length equal to distance |
| pc parsec # from the Sun to a point having |
| # heliocentric parallax of 1 |
| # arcsec (derived from parallax |
| # second). A distant object with |
| # parallax theta will be about |
| # (arcsec/theta) parsecs from the |
| # Sun (using the approximation |
| # that tan(theta) = theta). |
| rydberg 1|2 hartree # Rydberg energy |
| crith 0.089885 gram # The crith is the mass of one |
| # liter of hydrogen at standard |
| # temperature and pressure. |
| amagat N_A / molarvolume # Used to measure gas as a number |
| amagatvolume mol molarvolume # density |
| lorentz bohrmagneton / h c # Used to measure the extent |
| # that the frequency of light |
| # is shifted by a magnetic field. |
| cminv h c / cm # Unit of energy used in infrared |
| invcm cminv # spectroscopy. |
| wavenumber 1/cm # |
| kcal_mol kcal_th / mol N_A # kcal/mol is used as a unit of |
| # energy by physical chemists. |
| # |
| # CGS system based on centimeter, gram and second |
| # |
| |
| dyne cm gram / s^2 # force |
| dyn dyne |
| erg cm dyne # energy |
| poise gram / cm s # viscosity, honors Jean Poiseuille |
| P poise |
| rhe /poise # reciprocal viscosity |
| stokes cm^2 / s # kinematic viscosity |
| St stokes |
| stoke stokes |
| lentor stokes # old name |
| Gal cm / s^2 # acceleration, used in geophysics |
| galileo Gal # for Earth's gravitational field |
| # (note that "gal" is for gallon |
| # but "Gal" is the standard symbol |
| # for the gal which is evidently a |
| # shortened form of "galileo".) |
| barye dyne/cm^2 # pressure |
| barad barye # old name |
| kayser 1/cm # Proposed as a unit for wavenumber |
| balmer kayser # Even less common name than "kayser" |
| kine cm/s # velocity |
| bole g cm / s # momentum |
| pond gram force |
| glug gram force s^2 / cm # Mass which is accelerated at |
| # 1 cm/s^2 by 1 gram force |
| darcy centipoise cm^2 / s atm # Measures permeability to fluid flow. |
| # One darcy is the permeability of a |
| # medium that allows a flow of cc/s |
| # of a liquid of centipoise viscosity |
| # under a pressure gradient of |
| # atm/cm. Named for H. Darcy. |
| mobileohm cm / dyn s # mobile ohm, measure of mechanical |
| # mobility |
| mechanicalohm dyn s / cm # mechanical resistance |
| acousticalohm dyn s / cm^5 # ratio of the sound pressure of |
| # 1 dyn/cm^2 to a source of strength |
| # 1 cm^3/s |
| ray acousticalohm |
| rayl dyn s / cm^3 # Specific acoustical resistance |
| eotvos 1e-9 Gal/cm # Change in gravitational acceleration |
| # over horizontal distance |
| # |
| # Electromagnetic CGS Units |
| # |
| # For measuring electromagnetic quantities in SI, we introduce the new base |
| # dimension of current, define the ampere to measure current, and derive the |
| # other electromagnetic units from the ampere. With the CGS units one approach |
| # is to use the basic equations of electromagnetism to define units that |
| # eliminate constants from those equations. Coulomb's law has the form |
| # |
| # F = k_C q1 q2 / r^2 |
| # |
| # where k_C is the Coulomb constant equal to 1|4 pi epsilon0 in SI units. |
| # Ampere's force law takes the form |
| # |
| # dF/dl = 2 k_A I1 I2 / r |
| # |
| # where k_A is the ampere constant. In the CGS system we force either k_C or |
| # k_A to 1 which then defines either a unit for charge or a unit for current. |
| # The other unit then becomes a derived unit. When k_C is 1 the ESU system |
| # results. When k_A is 1 the EMU system results. Note that these parameters |
| # are not independent of each other: Maxwell's equations indicate that |
| # |
| # k_C / k_A = c^2 |
| # |
| # where c is the speed of light. |
| # |
| # One more choice is needed to define a complete system. Using Coulomb's law |
| # we define the electric field as the force per unit charge |
| # |
| # E = k_C 1 / r^2. |
| # |
| # But what about the magnetic field? It is derived from Ampere's law but we |
| # have the option of adding a proportionality constant, k_B, that may have |
| # dimensions: |
| # |
| # B = 2 k_A k_B I / r |
| # |
| # We can choose k_B = 1, which is done in the SI, ESU and EMU systems. But if |
| # instead we give k_B units of length/time then the magnetic field has |
| # the same units as the electric field. This choice leads to the Gaussian |
| # and Heaviside-Lorentz systems. |
| # |
| # The relations above are used to determine the dimensions, but the units are |
| # derived from the base units of CGS, not directly from those formulas. We |
| # will use the notation [unit] to refer to the dimension of the unit in |
| # brackets. This same process gives rise to the SI units such as the tesla, |
| # which is defined by |
| # |
| # [tesla] = [2 (1/4 pi c^2 epsilon0) amp / m] = [(mu0 / 2) amp / m] |
| # |
| # which gives kg / A s^2 as expected. |
| # |
| # References: |
| # |
| # Classical Electrodynamics by John David Jackson, 3rd edition. |
| # Cardarelli, Francois. 1999. Scientific Unit Conversion. 2nd ed. Trans. |
| # M.J. Shields. London: Springer-Verlag. ISBN 1-85233-043-0 |
| # |
| # |
| # All of the CGS systems result in electromagnetic units that involve the square |
| # roots of the centimeter and gram. This requires a change in the primitive |
| # units. |
| # |
| |
| !var UNITS_SYSTEM esu emu gaussian gauss hlu |
| sqrt_cm ! |
| sqrt_centimeter sqrt_cm |
| +m 100 sqrt_cm^2 |
| sqrt_g ! |
| sqrt_gram sqrt_g |
| +kg kilo sqrt_g^2 |
| !endvar |
| |
| # Electrostatic CGS (ESU) |
| # |
| # This system uses the statcoulomb as the fundamental unit of charge, with |
| # derived units that parallel the conventional terminology but use the stat- |
| # prefix. The statcoulomb is derived from Coulomb's law based on the dyne |
| # |
| # dyne = statcoulomb^2 / k_C cm^2. |
| # |
| # and in the EUS system, k_C=1. The statcoulomb is also called the |
| # franklin or esu. |
| # |
| # The ESU system was specified by a committee report in 1873 and rarely used. |
| |
| statcoulomb sqrt(dyne cm^2/k_C) # Charge such that two charges |
| esu statcoulomb # of 1 statC separated by 1 cm |
| statcoul statcoulomb # exert a force of 1 dyne |
| statC statcoulomb |
| stC statcoulomb |
| franklin statcoulomb |
| Fr franklin |
| |
| !var UNITS_SYSTEM esu |
| !message CGS-ESU units selected |
| !prompt (ESU) |
| +coulombconst 1 |
| +epsilon0 1 / k_C # SI relation: 1 / 4 pi k_C |
| +A 10 c_SI statamp |
| !endvar |
| |
| statampere statcoulomb / s |
| statamp statampere |
| statA statampere |
| stA statampere |
| statvolt dyne cm / statamp sec |
| statV statvolt |
| stV statvolt |
| statfarad statamp sec / statvolt |
| statF statfarad |
| stF statfarad |
| cmcapacitance statfarad |
| stathenry statvolt sec / statamp |
| statH stathenry |
| stH stathenry |
| statohm statvolt / statamp |
| stohm statohm |
| statmho /statohm |
| stmho statmho |
| statweber statvolt sec |
| statWb statweber |
| stWb statweber |
| stattesla statWb/cm^2 # Defined by analogy with SI; rarely |
| statT stattesla # if ever used |
| stT stattesla |
| debye 1e-10 statC angstrom # unit of electrical dipole moment |
| helmholtz debye/angstrom^2 # Dipole moment per area |
| jar 1000 statfarad # approx capacitance of Leyden jar |
| |
| # Electromagnetic CGS (EMU) |
| # |
| # The abampere is the fundamental unit of this system, with the derived units |
| # using the ab- prefix. The dimensions of the abampere are defined by assuming |
| # that k_A=1, which |
| # |
| # [dyne / cm] = [2 abampere^2 / cm] |
| # |
| # where the brackets indicate taking the dimension of the unit in base units |
| # and discarding any constant factors. This results in the definition from |
| # base CGS units of: |
| # |
| # abampere = sqrt(dyne). |
| # |
| # The abampere is also called the biot. The magnetic field unit (the gauss) |
| # follows from the assumption that k_B=1, which means |
| # |
| # B = 2 I / r, |
| # |
| # and hence the dimensions of the gauss are given by |
| # |
| # [gauss] = [2 abampere / cm] |
| # |
| # or rewriting in terms of the base units |
| # |
| # gauss = abampere / cm. |
| # |
| # The definition given below is different because it is in a form that |
| # gives a valid reduction for SI and ESU and still gives the correct |
| # result in EMU. (It can be derived from Faraday's law.) |
| # |
| # The EMU system was developed by Gauss and Weber and formalized as a system in |
| # a committee report by the British Association for the Advancement of Science |
| # in 1873. |
| |
| abampere 10 A # Current which produces a force of |
| abamp abampere # 2 dyne/cm between two infinitely |
| aA abampere # long wires that are 1 cm apart |
| abA abampere |
| biot abampere |
| Bi biot |
| |
| !var UNITS_SYSTEM emu |
| !message CGS-EMU units selected |
| !prompt (EMU) |
| +coulombconst c^2 |
| +epsilon0 1 / k_C # SI relation: 1 / 4 pi k_C |
| +abampere sqrt(dyne) |
| +A 0.1 abamp |
| !endvar |
| |
| abcoulomb abamp sec |
| abcoul abcoulomb |
| abC abcoulomb |
| abfarad abampere sec / abvolt |
| abF abfarad |
| abhenry abvolt sec / abamp |
| abH abhenry |
| abvolt dyne cm / abamp sec |
| abV abvolt |
| abohm abvolt / abamp |
| abmho /abohm |
| maxwell erg / abamp # Also called the "line" |
| Mx maxwell |
| gauss maxwell / cm^2 # The magnetic field 2 cm from a wire |
| Gs gauss # carrying a current of 1 abampere |
| oersted gauss / mu0 # From the relation H = B / mu |
| Oe oersted |
| gilbert gauss cm / mu0 |
| Gb gilbert |
| Gi gilbert |
| unitpole 4 pi maxwell # unit magnetic pole |
| emu erg/gauss # "electro-magnetic unit", a measure of |
| # magnetic moment, often used as emu/cm^3 |
| # to specify magnetic moment density. |
| |
| # Electromagnetic CGS (Gaussian) |
| # |
| # The Gaussian system uses the statcoulomb and statamp from the ESU system |
| # derived by setting k_C=1, but it defines the magnetic field unit differently |
| # by taking k_B=c instead of k_B=1. As noted above, k_C and k_A are not |
| # independent. With k_C=1 we must have k_A=c^-2. This results in the magnetic |
| # field unit, the gauss, having dimensions give by: |
| # |
| # [gauss] = [2 (c^-2) c statamp / cm] = [statamp / c cm] |
| # |
| # We then define the gauss using base CGS units to obtain |
| # |
| # gauss = statamp / ((cm/s) cm) = statcoulomb / cm^2. |
| # |
| # Note that this definition happens to give the same result as the definition |
| # for the EMU system, so the definitions of the gauss are consistent. |
| # |
| # This definition gives the same dimensions for the E and B fields and was also |
| # known as the "symmetric system". This system was proposed by Hertz in 1888. |
| |
| !var UNITS_SYSTEM gaussian gauss |
| !message CGS-Gaussian units selected |
| !prompt (Gaussian) |
| !endvar |
| !var UNITS_SYSTEM gaussian gauss natural-gauss |
| +coulombconst 1 |
| +A 10 c_SI statamp |
| # Some SI-based definitions need re-scaling |
| # by factors of "c" and/or "4 pi": |
| +epsilon0 1 / k_C # SI relation: 1 / 4 pi k_C |
| +mu0 1 / epsilon0 # SI relation: 1 / epsilon0 c^2 |
| +bohrmagneton (e hbar / 2 electronmass) / c |
| +magneticfluxquantum c (pi hbar / e) |
| +maxwell c (erg / abamp) |
| +weber c (J / A) |
| !endvar |
| |
| # Electromagnetic CGS (Heaviside-Lorentz) |
| |
| # The Heaviside-Lorentz system is similar to the Gaussian system, but it is |
| # "rationalized" so that factors of 4 pi do not appear in Maxwell's equations. |
| # The SI system is similarly rationalized, but the other CGS systems are not. |
| # |
| # The factor of 4 pi appears instead in Coulomb's law, so in this system |
| # k_C = 1 / 4 pi, which means the charge unit is defined by |
| # |
| # dyne = (1 / 4 pi) hlu_charge^2 / cm^2. |
| # |
| # Since we have the leading constant of (1 / 4pi) the numerical value of the |
| # charge number is larger by sqrt(4pi), which in turns means that the HLU |
| # charge unit is smaller by this multiple. But note that the dimensions of the |
| # charge unit are the same as the Gaussian system, so both systems measure |
| # charge with cm^(3/2) g^(1/2) / s, but the amount of charge for this dimension |
| # differs by a factor of sqrt(4pi) between the two systems. |
| # |
| # Ampere's law for the Heaviside-Lorentz system has the form |
| # |
| # B = 1/(2 pi c) * I/r |
| |
| # The Heaviside-Lorentz system does not appear to have any named units, so we |
| # use "hlu" for "Heaviside-Lorentz unit" so we can define values for the basic |
| # units in this system. |
| |
| hlu_charge statcoulomb / sqrt(4 pi) |
| hlu_current hlu_charge / sec |
| hlu_volt erg / hlu_charge |
| hlu_efield hlu_volt / cm |
| hlu_bfield sqrt(4 pi) gauss |
| |
| !var UNITS_SYSTEM hlu |
| !message CGS-Heaviside-Lorentz Units selected |
| !prompt (HLU) |
| !endvar |
| !var UNITS_SYSTEM hlu natural planck planck-red |
| +coulombconst 1 / 4 pi |
| +A 10 c_SI statamp |
| # Some SI-based magnetism definitions |
| # need re-scaling by factors of "c": |
| +mu0 1 / epsilon0 # SI relation: 1 / epsilon0 c^2 |
| +bohrmagneton (e hbar / 2 electronmass) / c |
| +magneticfluxquantum c (pi hbar / e) |
| +weber c (J / A) |
| +maxwell c (erg / abamp) |
| !endvar |
| |
| # "Natural units" (high energy physics and cosmology) |
| # |
| # In particle physics "natural units" (which don't seem to have a more specific |
| # name) are defined by setting hbar = c = boltzmann = 1. In this system the |
| # electron volt is the only base unit. The electromagnetic units can be |
| # derived from the rationalized Heaviside-Lorentz units or from Gaussian units. |
| # The default form is the rationalized HLU derived version. |
| # |
| # The basic mechanical and thermodynamic definitions for the natural |
| # units are identical in both systems. These appear below. The |
| # natural-gauss system has additional electromagnetic redefinitions |
| # that appear above in the "Electromagnetic CGS (Gaussian)" Section. |
| |
| # These are the Heaviside-Lorentz natural units |
| |
| natural_energy eV |
| natural_charge e / sqrt(4 pi alpha) |
| natural_time hbar / natural_energy |
| natural_length natural_time c |
| natural_mass natural_energy / c^2 |
| natural_temp natural_energy / boltzmann |
| natural_force natural_energy / natural_length |
| natural_power natural_energy / natural_time |
| natural_volt natural_energy / natural_charge |
| natural_Efield natural_volt / natural_length |
| natural_Bfield natural_Efield / c |
| natural_current natural_charge / natural_time |
| |
| !var UNITS_SYSTEM natural |
| !message Natural units selected (Heavyside-Lorentz based) |
| !prompt (natural) |
| !endvar |
| |
| !var UNITS_SYSTEM natural-gauss |
| !message Natural units selected (Gaussian based) |
| !prompt (natgauss) |
| !endvar |
| |
| # These definitions are the same in both natural unit systems |
| |
| !var UNITS_SYSTEM natural natural-gauss |
| +eV ! |
| +h 2 pi |
| +c 1 |
| +boltzmann 1 |
| +m e_SI / hbar_SI c_SI eV |
| +kg (c_SI^2 / e_SI) eV |
| +s e_SI / hbar_SI eV |
| +K (k_SI / e_SI) eV |
| !endvar |
| |
| # |
| # Planck units |
| # |
| # Planck units are a set of "natural" units based on physical constants c, G, |
| # hbar, boltzmann's constant, and epsilon0, often used when working with |
| # gravitational theory. In planck units, all quantities are dimensionless. |
| # Some variations are possible for exactly how the units are defined. We |
| # provide two variations, the rationalized planck units and the |
| # rationalized-reduced planck units. |
| # |
| # In both forms the units are defined by c = hbar = boltzmann = 1. |
| # But the choice of rationalized and reduced affects how epsilon0 and G |
| # are treated. |
| # |
| # In the "rationalized" units, factors of 4 pi do not appear in Maxwell's |
| # equation, and Coulomb's law bears a factor of 1/4 pi. See the section on |
| # the Heaviside-Lorentz units for more about this. The choice of rationalized |
| # units means that epsilon0 = 1. (In the unrationalized case, which is not |
| # supported, 1/(4 pi epsilon0) = 1.) |
| # |
| # The "reduced" units similarly are defined to eliminate factors of 8 pi |
| # from the Einstein field equations for gravitation. With reduced units |
| # we set 8 pi G = 1 and with the unreduced units, simply G = 1. |
| |
| # Rationalized, unreduced planck units |
| |
| planckmass sqrt(hbar c / G) |
| m_P planckmass |
| planckenergy planckmass c^2 |
| E_P planckenergy |
| plancktime hbar / planckenergy |
| t_P plancktime |
| plancklength plancktime c |
| l_P plancklength |
| plancktemperature planckenergy / k |
| T_P plancktemperature |
| planckforce planckenergy / plancklength |
| planckcharge sqrt(epsilon0 hbar c) |
| planckcurrent planckcharge / plancktime |
| planckvolt planckenergy / planckcharge |
| planckEfield planckvolt / plancklength |
| planckBfield planckEfield / c |
| |
| # Rationalized, reduced planck units |
| |
| planckmass_red sqrt(hbar c / 8 pi G) |
| planckenergy_red planckmass_red c^2 |
| plancktime_red hbar / planckenergy_red |
| plancklength_red plancktime_red c |
| plancktemperature_red planckenergy_red / k |
| planckforce_red planckenergy_red / plancklength_red |
| planckcharge_red sqrt(epsilon0 hbar c) |
| planckcurrent_red planckcharge_red / plancktime_red |
| planckvolt_red planckenergy_red / planckcharge_red |
| planckEfield_red planckvolt_red / plancklength_red |
| planckBfield_red planckEfield_red /c |
| |
| |
| !var UNITS_SYSTEM planck |
| !message Planck units selected |
| !prompt (planck) |
| +c 1 |
| +h 2 pi |
| +G 1 |
| +boltzmann 1 |
| +kg sqrt(G_SI / hbar_SI c_SI) |
| +s c_SI^2 / hbar_SI kg |
| +m s / c_SI |
| +K k_SI / hbar_SI s |
| !endvar |
| |
| |
| !var UNITS_SYSTEM planck-red |
| !message Reduced planck units selected |
| !prompt (planck reduced) |
| +c 1 |
| +h 2 pi |
| +G 1/8 pi |
| +boltzmann 1 |
| +kg sqrt(8 pi G_SI / hbar_SI c_SI) |
| +s c_SI^2 / hbar_SI kg |
| +m s / c_SI |
| +K k_SI / hbar_SI s |
| !endvar |
| |
| # |
| # Some historical electromagnetic units |
| # |
| |
| intampere 0.999835 A # Defined as the current which in one |
| intamp intampere # second deposits .001118 gram of |
| # silver from an aqueous solution of |
| # silver nitrate. |
| intfarad 0.999505 F |
| intvolt 1.00033 V |
| intohm 1.000495 ohm # Defined as the resistance of a |
| # uniform column of mercury containing |
| # 14.4521 gram in a column 1.063 m |
| # long and maintained at 0 degC. |
| daniell 1.042 V # Meant to be electromotive force of a |
| # Daniell cell, but in error by .04 V |
| faraday N_A e mol # Charge that must flow to deposit or |
| faraday_phys 96521.9 C # liberate one gram equivalent of any |
| faraday_chem 96495.7 C # element. (The chemical and physical |
| faradayconst N_A e # values are off slightly from what is |
| # obtained by multiplying by amu_chem |
| # or amu_phys. These values are from |
| # a 1991 NIST publication.) Note that |
| # there is also a Faraday constant, |
| # which has units of C/mol. |
| kappline 6000 maxwell # Named by and for Gisbert Kapp |
| siemensunit 0.9534 ohm # Resistance of a meter long column of |
| # mercury with a 1 mm cross section. |
| # |
| # Printed circuit board units. |
| # |
| # Iowa State University Center for Nondestructive Evaluation |
| # Electrical Conductivity and Resistivity |
| # https://www.nde-ed.org/Physics/Materials/Physical_Chemical/Electrical.xhtml |
| # |
| # Conductivity is often expressed as a percentage of IACS. A copper wire a |
| # meter long with a 1 mm^2 cross section has a resistance of 1|58 ohm at |
| # 20 deg C. Copper density also has a standard IACS value at that temperature. |
| # |
| |
| copperconductivity 58 siemens m / mm^2 # A wire a meter long with |
| IACS copperconductivity # a 1 mm^2 cross section |
| copperdensity 8.89 g/cm^3 # The "ounce" measures the |
| ouncecopper oz / ft^2 copperdensity # thickness of copper used |
| ozcu ouncecopper # in circuitboard fabrication |
| |
| # |
| # Photometric units |
| # |
| |
| LUMINOUS_INTENSITY candela |
| LUMINOUS_FLUX lumen |
| LUMINOUS_ENERGY talbot |
| ILLUMINANCE lux |
| EXITANCE lux |
| |
| candle 1.02 candela # Standard unit for luminous intensity |
| hefnerunit 0.9 candle # in use before candela |
| hefnercandle hefnerunit # |
| violle 20.17 cd # luminous intensity of 1 cm^2 of |
| # platinum at its temperature of |
| # solidification (2045 K) |
| |
| lumen cd sr # Luminous flux (luminous energy per |
| lm lumen # time unit) |
| |
| talbot lumen s # Luminous energy |
| lumberg talbot # References give these values for |
| lumerg talbot # lumerg and lumberg both. Note that |
| # a paper from 1948 suggests that |
| # lumerg should be 1e-7 talbots so |
| # that lumergs/erg = talbots/joule. |
| # lumerg = luminous erg |
| lux lm/m^2 # Illuminance or exitance (luminous |
| lx lux # flux incident on or coming from |
| phot lumen / cm^2 # a surface) |
| ph phot # |
| footcandle lumen/ft^2 # Illuminance from a 1 candela source |
| # at a distance of one foot |
| metercandle lumen/m^2 # Illuminance from a 1 candela source |
| # at a distance of one meter |
| |
| mcs metercandle s # luminous energy per area, used to |
| # measure photographic exposure |
| |
| nox 1e-3 lux # These two units were proposed for |
| skot 1e-3 apostilb # measurements relating to dark adapted |
| # eyes. |
| # Luminance measures |
| |
| LUMINANCE nit |
| |
| nit cd/m^2 # Luminance: the intensity per projected |
| stilb cd / cm^2 # area of an extended luminous source. |
| sb stilb # (nit is from latin nitere = to shine.) |
| |
| apostilb cd/pi m^2 |
| asb apostilb |
| blondel apostilb # Named after a French scientist. |
| |
| # Equivalent luminance measures. These units are units which measure |
| # the luminance of a surface with a specified exitance which obeys |
| # Lambert's law. (Lambert's law specifies that luminous intensity of |
| # a perfectly diffuse luminous surface is proportional to the cosine |
| # of the angle at which you view the luminous surface.) |
| |
| equivalentlux cd / pi m^2 # luminance of a 1 lux surface |
| equivalentphot cd / pi cm^2 # luminance of a 1 phot surface |
| lambert cd / pi cm^2 |
| footlambert cd / pi ft^2 |
| |
| # The bril is used to express "brilliance" of a source of light on a |
| # logarithmic scale to correspond to subjective perception. An increase of 1 |
| # bril means doubling the luminance. A luminance of 1 lambert is defined to |
| # have a brilliance of 1 bril. |
| |
| bril(x) units=[1;lambert] 2^(x+-100) lamberts ;log2(bril/lambert)+100 |
| |
| # Some luminance data from the IES Lighting Handbook, 8th ed, 1993 |
| |
| sunlum 1.6e9 cd/m^2 # at zenith |
| sunillum 100e3 lux # clear sky |
| sunillum_o 10e3 lux # overcast sky |
| sunlum_h 6e6 cd/m^2 # value at horizon |
| skylum 8000 cd/m^2 # average, clear sky |
| skylum_o 2000 cd/m^2 # average, overcast sky |
| moonlum 2500 cd/m^2 |
| |
| # |
| # Photographic Exposure Value |
| # This section by Jeff Conrad (jeff_conrad@msn.com) |
| # |
| # The Additive system of Photographic EXposure (APEX) proposed in ASA |
| # PH2.5-1960 was an attempt to simplify exposure determination for people who |
| # relied on exposure tables rather than exposure meters. Shortly thereafter, |
| # nearly all cameras incorporated exposure meters, so the APEX system never |
| # caught on, but the concept of exposure value remains in use. Though given as |
| # 'Ev' in ASA PH2.5-1960, it is now more commonly indicated by 'EV'. EV is |
| # related to exposure parameters by |
| # |
| # A^2 LS ES |
| # 2^EV = --- = -- = -- |
| # t K C |
| # |
| # Where |
| # A = Relative aperture (f-number) |
| # t = Exposure time in seconds |
| # L = Scene luminance in cd/m2 |
| # E = Scene illuminance in lux |
| # S = Arithmetic ISO speed |
| # K = Reflected-light meter calibration constant |
| # C = Incident-light meter calibration constant |
| # |
| # Strictly, an exposure value is a combination of aperture and exposure time, |
| # but it's also commonly used to indicate luminance (or illuminance). |
| # Conversion to luminance or illuminance units depends on the ISO speed and the |
| # meter calibration constant. Common practice is to use an ISO speed of 100. |
| # Calibration constants vary among camera and meter manufacturers: Canon, |
| # Nikon, and Sekonic use a value of 12.5 for reflected-light meters, while |
| # Kenko (formerly Minolta) and Pentax use a value of 14. Kenko and Sekonic use |
| # a value of 250 for incident-light meters with flat receptors. |
| # |
| # The values for in-camera meters apply only averaging, weighted-averaging, or |
| # spot metering--the multi-segment metering incorporated in most current |
| # cameras uses proprietary algorithms that evaluate many factors related to the |
| # luminance distribution of what is being metered; they are not amenable to |
| # simple conversions, and are usually not disclosed by the manufacturers. |
| |
| s100 100 / lx s # ISO 100 speed |
| iso100 s100 |
| |
| # Reflected-light meter calibration constant with ISO 100 speed |
| |
| k1250 12.5 (cd/m2) / lx s # For Canon, Nikon, and Sekonic |
| k1400 14 (cd/m2) / lx s # For Kenko (Minolta) and Pentax |
| |
| # Incident-light meter calibration constant with ISO 100 film |
| |
| c250 250 lx / lx s # flat-disc receptor |
| |
| # Exposure value to scene luminance with ISO 100 imaging media |
| |
| # For Kenko (Minolta) or Pentax |
| #ev100(x) units=[;cd/m^2] range=(0,) 2^x k1400 / s100; log2(ev100 s100/k1400) |
| # For Canon, Nikon, or Sekonic |
| ev100(x) units=[1;cd/m^2] range=(0,) 2^x k1250 / s100; log2(ev100 s100/k1250) |
| EV100() ev100 |
| |
| # Exposure value to scene illuminance with ISO 100 imaging media |
| |
| iv100(x) units=[1;lx] range=(0,) 2^x c250 / s100; log2(iv100 s100 / c250) |
| |
| # Other Photographic Exposure Conversions |
| # |
| # As part of APEX, ASA PH2.5-1960 proposed several logarithmic quantities |
| # related by |
| # |
| # Ev = Av + Tv = Bv + Sv |
| # |
| # where |
| # Av = log2(A^2) Aperture value |
| # Tv = log2(1/t) Time value |
| # Sv = log2(N Sx) Speed value |
| # Bv = log2(B S / K) Luminance ("brightness") value |
| # Iv = log2(I S / C) Illuminance value |
| # |
| # and |
| # A = Relative aperture (f-number) |
| # t = Exposure time in seconds |
| # Sx = Arithmetic ISO speed in 1/lux s |
| # B = luminance in cd/m2 |
| # I = luminance in lux |
| |
| # The constant N derives from the arcane relationship between arithmetic |
| # and logarithmic speed given in ASA PH2.5-1960. That relationship |
| # apparently was not obvious--so much so that it was thought necessary |
| # to explain it in PH2.12-1961. The constant has had several values |
| # over the years, usually without explanation for the changes. Although |
| # APEX had little impact on consumer cameras, it has seen a partial |
| # resurrection in the Exif standards published by the Camera & Imaging |
| # Products Association of Japan. |
| |
| #N_apex 2^-1.75 lx s # precise value implied in ASA PH2.12-1961, |
| # derived from ASA PH2.5-1960. |
| #N_apex 0.30 lx s # rounded value in ASA PH2.5-1960, |
| # ASA PH2.12-1961, and ANSI PH2.7-1986 |
| #N_apex 0.3162 lx s # value in ANSI PH2.7-1973 |
| N_exif 1|3.125 lx s # value in Exif 2.3 (2010), making Sv(5) = 100 |
| K_apex1961 11.4 (cd/m2) / lx s # value in ASA PH2.12-1961 |
| K_apex1971 12.5 (cd/m2) / lx s # value in ANSI PH3.49-1971; more common |
| C_apex1961 224 lx / lx s # value in PH2.12-1961 (20.83 for I in |
| # footcandles; flat sensor?) |
| C_apex1971 322 lx / lx s # mean value in PH3.49-1971 (30 +/- 5 for I in |
| # footcandles; hemispherical sensor?) |
| N_speed N_exif |
| K_lum K_apex1971 |
| C_illum C_apex1961 |
| |
| # Units for Photographic Exposure Variables |
| # |
| # Practical photography sometimes pays scant attention to units for exposure |
| # variables. In particular, the "speed" of the imaging medium is treated as if |
| # it were dimensionless when it should have units of reciprocal lux seconds; |
| # this practice works only because "speed" is almost invariably given in |
| # accordance with international standards (or similar ones used by camera |
| # manufacturers)--so the assumed units are invariant. In calculating |
| # logarithmic quantities--especially the time value Tv and the exposure value |
| # EV--the units for exposure time ("shutter speed") are often ignored; this |
| # practice works only because the units of exposure time are assumed to be in |
| # seconds, and the missing units that make the argument to the logarithmic |
| # function dimensionless are silently provided. |
| # |
| # In keeping with common practice, the definitions that follow treat "speeds" |
| # as dimensionless, so ISO 100 speed is given simply as '100'. When |
| # calculating the logarithmic APEX quantities Av and Tv, the definitions |
| # provide the missing units, so the times can be given with any appropriate |
| # units. For example, giving an exposure time of 1 minute as either '1 min' or |
| # '60 s' will result in Tv of -5.9068906. |
| # |
| # Exposure Value from f-number and Exposure Time |
| # |
| # Because nonlinear unit conversions only accept a single quantity, |
| # there is no direct conversion from f-number and exposure time to |
| # exposure value EV. But the EV can be obtained from a combination of |
| # Av and Tv. For example, the "sunny 16" rule states that correct |
| # exposure for a sunlit scene can achieved by using f/16 and an exposure |
| # time equal to the reciprocal of the ISO speed in seconds; this can be |
| # calculated as |
| # |
| # ~Av(16) + ~Tv(1|100 s), |
| # |
| # which gives 14.643856. These conversions may be combined with the |
| # ev100 conversion: |
| # |
| # ev100(~Av(16) + ~Tv(1|100 s)) |
| # |
| # to yield the assumed average scene luminance of 3200 cd/m^2. |
| |
| # convert relative aperture (f-number) to aperture value |
| Av(A) units=[1;1] domain=[-2,) range=[0.5,) 2^(A/2); 2 log2(Av) |
| # convert exposure time to time value |
| Tv(t) units=[1;s] range=(0,) 2^(-t) s; log2(s / Tv) |
| # convert logarithmic speed Sv in ASA PH2.5-1960 to ASA/ISO arithmetic speed; |
| # make arithmetic speed dimensionless |
| # 'Sv' conflicts with the symbol for sievert; you can uncomment this function |
| # definition if you don't need that symbol |
| #Sv(S) units=[1;1] range=(0,) 2^S / (N_speed/lx s); log2((N_speed/lx s) Sv) |
| Sval(S) units=[1;1] range=(0,) 2^S / (N_speed/lx s); log2((N_speed/lx s) Sval) |
| |
| # convert luminance value Bv in ASA PH2.12-1961 to luminance |
| Bv(x) units=[1;cd/m^2] range=(0,) \ |
| 2^x K_lum N_speed ; log2(Bv / (K_lum N_speed)) |
| |
| # convert illuminance value Iv in ASA PH2.12-1961 to illuminance |
| Iv(x) units=[1;lx] range=(0,) \ |
| 2^x C_illum N_speed ; log2(Iv / (C_illum N_speed)) |
| |
| # convert ASA/ISO arithmetic speed Sx to ASA logarithmic speed in |
| # ASA PH2.5-1960; make arithmetic speed dimensionless |
| Sx(S) units=[1;1] domain=(0,) \ |
| log2((N_speed/lx s) S); 2^Sx / (N_speed/lx s) |
| |
| # convert DIN speed/ISO logarithmic speed in ISO 6:1993 to arithmetic speed |
| # for convenience, speed is treated here as if it were dimensionless |
| Sdeg(S) units=[1;1] range=(0,) 10^((S - 1) / 10) ; (1 + 10 log(Sdeg)) |
| Sdin() Sdeg |
| |
| # Numerical Aperture and f-Number of a Lens |
| # |
| # The numerical aperture (NA) is given by |
| # |
| # NA = n sin(theta) |
| # |
| # where n is the index of refraction of the medium and theta is half |
| # of the angle subtended by the aperture stop from a point in the image |
| # or object plane. For a lens in air, n = 1, and |
| # |
| # NA = 0.5 / f-number |
| # |
| # convert NA to f-number |
| numericalaperture(x) units=[1;1] domain=(0,1] range=[0.5,) \ |
| 0.5 / x ; 0.5 / numericalaperture |
| NA() numericalaperture |
| # |
| # convert f-number to itself; restrict values to those possible |
| fnumber(x) units=[1;1] domain=[0.5,) range=[0.5,) x ; fnumber |
| |
| # Referenced Photographic Standards |
| # |
| # ASA PH-2.5-1960. USA Standard, Method for Determining (Monochrome, |
| # Continuous-Tone) Speed of Photographic Negative Materials. |
| # ASA PH2.12-1961. American Standard, General-Purpose Photographic |
| # Exposure Meters (photoelectric type). |
| # ANSI PH3.49-1971. American National Standard for general-purpose |
| # photographic exposure meters (photoelectric type). |
| # ANSI PH2.7-1973. American National Standard Photographic Exposure Guide. |
| # ANSI PH2.7-1986. American National Standard for Photography -- |
| # Photographic Exposure Guide. |
| # CIPA DC-008-2010. Exchangeable image file format for digital still |
| # cameras: Exif Version 2.3 |
| # ISO 6:1993. International Standard, Photography -- Black-and-white |
| # pictorial still camera negative film/process systems -- |
| # Determination of ISO Speed. |
| |
| |
| # |
| # Astronomical time measurements |
| # |
| # Astronomical time measurement is a complicated matter. The length of the |
| # true day at a given place can be 21 seconds less than 24 hours or 30 seconds |
| # over 24 hours. The two main reasons for this are the varying speed of |
| # Earth in its elliptical orbit and the fact that the Sun moves on the ecliptic |
| # instead of along the celestial equator. To devise a workable system for time |
| # measurement, Simon Newcomb (1835-1909) used a fictitious "mean Sun". |
| # Consider a first fictitious Sun traveling along the ecliptic at a constant |
| # speed and coinciding with the true Sun at perigee and apogee. Then |
| # considering a second fictitious Sun traveling along the celestial equator at |
| # a constant speed and coinciding with the first fictitious Sun at the |
| # equinoxes. The second fictitious Sun is the "mean Sun". From this equations |
| # can be written out to determine the length of the mean day, and the tropical |
| # year. The length of the second was determined based on the tropical year |
| # from such a calculation and was officially used from 1960-1967 until atomic |
| # clocks replaced astronomical measurements for a standard of time. All of the |
| # values below give the mean time for the specified interval. |
| # |
| # See "Mathematical Astronomy Morsels" by Jean Meeus for more details |
| # and a description of how to compute the correction to mean time. |
| # |
| |
| TIME second |
| |
| anomalisticyear 365.2596 days # The time between successive |
| # perihelion passages of |
| # Earth. |
| siderealyear 365.256360417 day # The time for Earth to make |
| # one revolution around the Sun |
| # relative to the stars. |
| tropicalyear 365.242198781 day # The time needed for the mean Sun |
| # as defined above to increase |
| # its longitude by 360 degrees. |
| # Most references defined the |
| # tropical year as the interval |
| # between vernal equinoxes, but |
| # this is misleading. The length |
| # of the season changes over time |
| # because of the eccentricity of |
| # Earth's orbit. The time |
| # between vernal equinoxes is |
| # approximately 365.24237 days |
| # around the year 2000. See |
| # "Mathematical Astronomy |
| # Morsels" for more details. |
| eclipseyear 346.62 days # The line of nodes is the |
| # intersection of the plane of |
| # Earth's orbit around the Sun |
| # with the plane of the Moon's |
| # orbit around Earth. Eclipses |
| # can only occur when the Moon |
| # and Sun are close to this |
| # line. The line rotates and |
| # appearances of the Sun on the |
| # line of nodes occur every |
| # eclipse year. |
| saros 223 synodicmonth # The Earth, Moon and Sun appear in |
| # the same arrangement every |
| # saros, so if an eclipse occurs, |
| # then one saros later, a similar |
| # eclipse will occur. (The saros |
| # is close to 19 eclipse years.) |
| # The eclipse will occur about |
| # 120 degrees west of the |
| # preceding one because the |
| # saros is not an even number of |
| # days. After 3 saros, an |
| # eclipse will occur at |
| # approximately the same place. |
| solarday day # Time from noon to noon |
| siderealday 86164.09054 s # The sidereal day is the interval |
| siderealhour 1|24 siderealday # between two successive transits |
| siderealminute 1|60 siderealhour # of a star over the meridian, |
| siderealsecond 1|60 siderealminute # or the time required for |
| # Earth to make one rotation |
| # relative to the stars. Another |
| # way to think about it is to |
| # imagine looking down at the |
| # solar system and noting when |
| # Earth has made a rotation. |
| # The more usual solar day is the |
| # time required to make a |
| # rotation relative to the Sun, |
| # which means the same point on |
| # Earth faces the Sun again. |
| # Because Earth moves in its |
| # orbit, it has to rotate a bit |
| # more to face the Sun again, |
| # hence the solar day is slightly |
| # longer than the sidereal day. |
| # The value given here is the |
| # mean day length taken from |
| # ssd.jpl.nasa.gov/astro_par.html |
| # which in turn cites the |
| # "Explanatory Supplement to the |
| # Astronomical Almanac", 1992. |
| anomalisticmonth 27.55454977 day # Time for the Moon to travel from |
| # perigee to perigee |
| nodicalmonth 27.2122199 day # The nodes are the points where |
| draconicmonth nodicalmonth # an orbit crosses the ecliptic. |
| draconiticmonth nodicalmonth # This is the time required to |
| # travel from the ascending node |
| # to the next ascending node. |
| siderealmonth 27.321661 day # Time required for the Moon to |
| # orbit the Earth |
| lunarmonth 29 days + 12 hours + 44 minutes + 2.8 seconds |
| # Mean time between full moons. |
| synodicmonth lunarmonth # Full moons occur when the Sun |
| lunation synodicmonth # and Moon are on opposite sides |
| lune 1|30 lunation # of the Earth. Since the Earth |
| lunour 1|24 lune # moves around the Sun, the Moon |
| # has to move a bit further in its |
| # orbit to return to the full moon |
| # configuration. |
| year tropicalyear |
| yr year |
| month 1|12 year |
| mo month |
| lustrum 5 years # The Lustrum was a Roman |
| # purification ceremony that took |
| # place every five years. |
| # Classically educated Englishmen |
| # used this term. |
| decade 10 years |
| century 100 years |
| millennium 1000 years |
| millennia millennium |
| solaryear year |
| lunaryear 12 lunarmonth |
| calendaryear 365 day |
| commonyear 365 day |
| leapyear 366 day |
| |
| # The Julian year is The length of an average year over a 4-year cycle in the |
| # Julian calendar. The calendar was proposed by Julius Caesar in 46 BCE and |
| # took effect the following year. It has a normal year of 365 days and a leap |
| # year of 366 days every four years. Though this calendar was used in |
| # Europe for more than 1600 years, it drifts from the topical year by |
| # about 1 day every 128 years, which became noticeable over its period |
| # of use. |
| |
| # This growing discrepancy between the seasons and the calendar was perhaps |
| # confusing but was also of concern to the Catholic Church because it led to a |
| # shift in the date of Easter. To correct this discrepancy, Pope Gregory XIII |
| # introduced the more accurate Gregorian calendar in 1582. The Gregorian year |
| # is the length of an average year over a 400-year cycle in the Gregorian |
| # calendar. Every year that is exactly divisible by four is a |
| # leap year, except for years that are exactly divisible by 100, unless these |
| # centurial years are exactly divisible by 400. This calendar was adopted by |
| # many Catholic countries when it was proclaimed, but was not adopted by many |
| # other countries until much later; Britain and the British Empire, including |
| # what is now the eastern part of the United States, adopted it in 1752. See |
| # https://en.wikipedia.org/wiki/List_of_adoption_dates_of_the_Gregorian_calendar_by_country |
| # for additional details. |
| |
| julianyear 365.25 days |
| gregorianyear 365.2425 days |
| |
| islamicyear 354 day # A year of 12 lunar months. They |
| islamicleapyear 355 day # began counting on July 16, AD 622 |
| # when Muhammad emigrated to Medina |
| # (the year of the Hegira). They need |
| # 11 leap days in 30 years to stay in |
| # sync with the lunar year which is a |
| # bit longer than the 29.5 days of the |
| # average month. The months do not |
| # keep to the same seasons, but |
| # regress through the seasons every |
| # 32.5 years. |
| islamicmonth 1|12 islamicyear # They have 29 day and 30 day months. |
| |
| # The Hebrew year is also based on lunar months, but synchronized to the solar |
| # calendar. The months vary irregularly between 29 and 30 days in length, and |
| # the years likewise vary. The regular year is 353, 354, or 355 days long. To |
| # keep up with the solar calendar, a leap month of 30 days is inserted every |
| # 3rd, 6th, 8th, 11th, 14th, 17th, and 19th years of a 19 year cycle. This |
| # gives leap years that last 383, 384, or 385 days. |
| |
| # |
| # Planetary data from JPL's planet fact sheets. Each planet has its |
| # own sheet at https://nssdc.gsfc.nasa.gov/planetary/factsheet/<name>fact.html |
| # The source for data on the fact sheets is described at |
| # https://nssdc.gsfc.nasa.gov/planetary/factsheet/fact_notes.html |
| # and they also indicate that the values listed are not "official" values: |
| # there is no single set of agreed upon values. |
| |
| # Sidereal days. The sidereal day is the time required for a planet to make a |
| # revolution relative to the stars. This is the default day value. |
| |
| mercuryday mercuryday_sidereal |
| venusday venusday_sidereal |
| earthday earthday_sidereal |
| marsday marsday_sidereal |
| jupiterday jupiterday_sidereal |
| saturnday saturnday_sidereal |
| uranusday uranusday_sidereal |
| neptuneday neptuneday_sidereal |
| plutoday plutoday_sidereal |
| |
| mercuryday_sidereal 1407.6 hr # Mercury is in a 3:2 resonance lock |
| # where it makes 3 rotations per 2 orbits |
| # so 3 sidereal days = 2 years |
| venusday_sidereal 5832.6 hr # Retrograde |
| earthday_sidereal siderealday |
| marsday_sidereal 24.6229 hr |
| jupiterday_sidereal 9.9250 hr |
| saturnday_sidereal 10.656 hr |
| uranusday_sidereal 17.24 hr # Retrograde |
| neptuneday_sidereal 16.11 hr |
| plutoday_sidereal 153.2928 hr # Retrograde |
| |
| # In astronomy, an object's rotation is "prograde" if it rotates in |
| # the same direction as the primary object it orbits. Prograde |
| # rotation is the more common case: in Earth's solar system, Mercury, |
| # Earth, Mars, Jupiter, Saturn, and Neptune have prograde rotation. |
| # When an object rotates opposite the direction of its primary object, |
| # the object's rotation is "retrograde". Venus, Uranus, and Pluto have |
| # retrograde rotation. |
| # |
| # The solar (or synodic) day is the time from noon to noon on a planet. This |
| # is different from the sidereal day because the planet has moved in its orbit, |
| # so (if its rotation is prograde) it needs additional rotation to return to |
| # the same orientation relative to the Sun. In one orbital period (a year), |
| # this amounts to one additional complete rotation, so the number of sidereal |
| # days in a year is one greater than the number of solar days. |
| # |
| # If the planet's rotation is retrograde, less rotation is needed to return to |
| # the same orientation relative to the Sun, and the number of sidereal days in |
| # a year is one fewer than the number of solar days. |
| # |
| # The solar day can be computed from the sidereal day in the typical prograde |
| # case by: |
| # solar_day = sidereal_day year / (year - sidereal_day) |
| # If the planet's rotation is retrograde like Venus then the formula is |
| # solar_day = sidereal_day year / (year + sidereal_day) |
| # If the sidereal day and year are the same length then the same face of the |
| # planet faces the Sun and there is no solar day. |
| |
| mercuryday_solar 4222.6 hr |
| venusday_solar 2802.0 hr |
| earthday_solar 24 hr |
| marsday_solar 24.6597 hr |
| jupiterday_solar 9.9259 hr |
| saturnday_solar 10.656 hr |
| uranusday_solar 17.24 hr |
| neptuneday_solar 16.11 hr |
| plutoday_solar 153.2820 hr |
| |
| # Sidereal years |
| |
| mercuryyear 87.969 day |
| venusyear 224.701 day |
| earthyear siderealyear |
| marsyear 686.980 day |
| jupiteryear 4332.589 day |
| saturnyear 10759.22 day |
| uranusyear 30685.4 day |
| neptuneyear 60189 day |
| plutoyear 90560 day |
| |
| # Equatorial radii for the planets from JPL fact sheets |
| |
| mercuryradius 2440.5 km |
| venusradius 6051.8 km |
| earthradius 6378.137 km |
| marsradius 3396.2 km |
| jupiterradius 71492 km # 1 bar level |
| saturnradius 60268 km # 1 bar level |
| uranusradius 25559 km # 1 bar level |
| neptuneradius 24764 km # 1 bar level |
| plutoradius 1188 km |
| |
| # Volumetric mean radii |
| |
| mercuryradius_mean 2440.5 km |
| venusradius_mean 6051.8 km |
| earthradius_mean 6371 km |
| marsradius_mean 3389.5 km |
| jupiterradius_mean 69911 km |
| saturnradius_mean 58232 km |
| uranusradius_mean 25362 km |
| neptuneradius_mean 24622 km |
| plutoradius_mean 1188 km |
| |
| # Polar radii |
| |
| mercuryradius_polar 2438.3 km |
| venusradius_polar 6051.8 km |
| marsradius_polar 3376.2 km |
| jupiterradius_polar 66854 km |
| saturnradius_polar 54364 km |
| uranusradius_polar 24973 km |
| neptuneradius_polar 24341 km |
| plutoradius_polar 1188 km |
| |
| mercurysundist_min 46.000 Gm |
| mercurysundist_max 69.818 Gm |
| venussundist_min 107.480 Gm |
| venussundist_max 108.941 Gm |
| earthsundist_min sundist_min |
| earthsundist_max sundist_max |
| marssundist_min 206.650 Gm |
| marssundist_max 249.261 Gm |
| jupitersundist_min 740.595 Gm |
| jupitersundist_max 816.363 Gm |
| saturnsundist_min 1357.554 Gm |
| saturnsundist_max 1506.527 Gm |
| uranussundist_min 2732.696 Gm |
| uranussundist_max 3001.390 Gm |
| neptunesundist_min 4471.050 Gm |
| neptunesundist_max 4558.857 Gm |
| plutosundist_min 4434.987 Gm |
| plutosundist_max 7304.326 Gm |
| |
| sundist 1.0000010178 au # mean Earth-Sun distance |
| moondist 384400 km # mean Earth-Moon distance |
| sundist_near 147.095 Gm # Earth-Sun distance at perihelion |
| sundist_min sundist_near |
| sundist_far 152.100 Gm # Earth-Sun distance at aphelion |
| sundist_max sundist_far |
| |
| # The Earth-Moon distances at perigee and apogee are different for every |
| # lunation. The values here are the extremes for 1500-2500 according to |
| # Jean Meeus's Astronomical Algorithms (1991, 332). |
| |
| moondist_min 356371 km # minimum distance at perigee 1500-2500 |
| moondist_max 406720 km # maximum distance at apogee 1500-2500 |
| |
| # Objects on Earth are charted relative to a perfect ellipsoid whose |
| # dimensions are specified by different organizations. The ellipsoid is |
| # specified by an equatorial radius and a flattening value which defines the |
| # polar radius. |
| |
| earthflattening IERS_earthflattening |
| earthradius_equatorial IERS_earthradius_equatorial |
| earthradius_polar (1-earthflattening) earthradius_equatorial |
| |
| # The World Geodetic System maintains a standard, WGS84, which is used by the |
| # the GPS system. This system uses a conventional ellipsoid that was fixed in |
| # 1984 and has remained constant so that data collected at different times is |
| # referenced to the same ellipsoid. https://epsg.io/4326 |
| |
| WGS84_earthflattening 1|298.257223563 |
| WGS84_earthradius_equatorial 6378137 m |
| WGS84_earthradius_polar (1-WGS84_earthflattening) WGS84_earthradius_equatorial |
| |
| # The International Earth Rotation Service (IERS) attempts to |
| # maintain an accurate model of Earth, with updates to maintain the highest |
| # possible accuracy, even though this makes it more difficult to relate geodetic |
| # measurements made at different times. |
| # IERS Conventions, Chapter 1, General definitions and numerical standards (16 November 2017) |
| # https://iers-conventions.obspm.fr/content/chapter1/icc1.pdf |
| |
| IERS_earthflattening 1|298.25642 |
| IERS_earthradius_equatorial 6378136.6 m |
| IERS_earthradius_polar (1-IERS_earthflattening) IERS_earthradius_equatorial |
| |
| |
| landarea 148.847e6 km^2 |
| oceanarea 361.254e6 km^2 |
| |
| moonradius 1738 km # mean value |
| sunradius 6.96e8 m |
| |
| # Many astronomical values can be measured most accurately in a system of units |
| # using the astronomical unit and the mass of the Sun as base units. The |
| # uncertainty in the gravitational constant makes conversion to SI units |
| # significantly less accurate. |
| |
| # The astronomical unit was defined to be the length of the of the semimajor |
| # axis of a massless object with the same year as Earth. With such a |
| # definition in force, and with the mass of the Sun set equal to one, Kepler's |
| # third law can be used to solve for the value of the gravitational constant. |
| |
| # Kepler's third law says that (2 pi / T)^2 a^3 = G M where T is the orbital |
| # period, a is the size of the semimajor axis, G is the gravitational constant |
| # and M is the mass. With M = 1 and T and a chosen for Earth's orbit, we |
| # find sqrt(G) = (2 pi / T) sqrt(AU^3). This constant is called the Gaussian |
| # gravitational constant, apparently because Gauss originally did the |
| # calculations. However, when the original calculation was done, the value |
| # for the length of Earth's year was inaccurate. The value used is called |
| # the Gaussian year. Changing the astronomical unit to bring it into |
| # agreement with more accurate values for the year would have invalidated a |
| # lot of previous work, so instead the astronomical unit has been kept equal |
| # to this original value. This is accomplished by using a standard value for |
| # the Gaussian gravitational constant. This constant is called k. |
| |
| gauss_k 0.01720209895 # This beast has dimensions of |
| # au^(3|2) / day and is exact. |
| gaussianyear (2 pi / gauss_k) days # Year that corresponds to the Gaussian |
| # gravitational constant. This is a |
| # fictional year, and doesn't |
| # correspond to any celestial event. |
| astronomicalunit 149597870700 m # IAU definition from 2012, exact |
| au astronomicalunit # ephemeris for the above described |
| # astronomical unit. (See the NASA |
| # site listed above.) |
| GMsun 132712440041.279419 km^3 / s^2 # heliocentric gravitational constant |
| solarmass GMsun/G # is known more accurately than G. |
| sunmass solarmass # Estimated from DE440 |
| |
| |
| # The following are masses for planetary systems, not just the planet itself, |
| # except for the case of Earth, where the Moon is excluded. Masses are |
| # relative to G because they are known much more accurately than G. |
| # |
| # See https://ssd.jpl.nasa.gov/astro_par.html. Values are from |
| # the DE440 Ephemeris: https://ssd.jpl.nasa.gov/doc/Park.2021.AJ.DE440.pdf |
| |
| mercurymass 22031.868551 km^3 / s^2 G |
| venusmass 324858.592000 km^3 / s^2 G |
| marsmass 42828.375816 km^3 / s^2 G |
| jupitermass 126712764.100000 km^3 / s^2 G |
| saturnmass 37940584.841800 km^3 / s^2 G |
| uranusmass 5794556.400000 km^3 / s^2 G |
| neptunemass 6836527.100580 km^3 / s^2 G |
| plutomass 975.500000 km^3 / s^2 G |
| ceresmass 62.62890 km^3 / s^2 G |
| vestamass 17.288245 km^3 / s^2 G |
| |
| earthmass 398600.435507 km^3 / s^2 G # Earth alone |
| moonmass 4902.800118 km^3 / s^2 G |
| moonearthmassratio moonmass/earthmass |
| earthmoonmass earthmass+moonmass |
| |
| moongravity 1.62 m/s^2 |
| |
| # Earth gravity values at the equator and poles. These values are |
| # obtained from the WGS84 model. |
| |
| gravity_equatorial 9.7803263359 m / s^2 |
| gravity_polar 9.8321849378 m / s^2 |
| |
| # The Hubble constant gives the speed at which distance galaxies are moving |
| # away from Earth according to v = H0*d, where H0 is the hubble constant |
| # and d is the distance to the galaxy. |
| |
| hubble 70 km/s/Mpc # approximate |
| H0 hubble |
| |
| # Parallax is the angular difference between the topocentric (on Earth's |
| # surface) and geocentric (at Earth's center) direction toward a celestial body |
| # when the body is at a given altitude. When the body is on the horizon, the |
| # parallax is the horizontal parallax; when the body is on the horizon and the |
| # observer is on the equator, the parallax is the equatorial horizontal |
| # parallax. When the body is at zenith, the parallax is zero. |
| |
| lunarparallax asin(earthradius_equatorial / moondist) # Moon equatorial |
| moonhp lunarparallax # horizontal parallax |
| # at mean distance |
| |
| # Light from celestial objects is attenuated by passage through Earth's |
| # atmosphere. A body near the horizon passes through much more air than an |
| # object at zenith, and is consequently less bright. Air mass is the ratio of |
| # the length of the optical path at a given altitude (angle above the horizon) |
| # to the length at zenith. Air mass at zenith is by definition unity; at the |
| # horizon, air mass is approximately 38, though the latter value can vary |
| # considerably with atmospheric conditions. The general formula is # E = E0 |
| # exp(-c X), where E0 is the value outside Earth's atmosphere, E is the value |
| # seen by an observer, X is the air mass and c is the extinction coefficient. |
| # A common value for c in reasonably clear air is 0.21, but values can be |
| # considerably greater in urban areas. Apparent altitude is that perceived by |
| # an observer; it includes the effect of atmospheric refraction. There is no |
| # shortage of formulas for air mass |
| # (https://en.wikipedia.org/wiki/Air_mass_(astronomy)); all are subject to |
| # variations in local atmospheric conditions. The formula used here is simple |
| # and is in good agreement with rigorously calculated values under standard |
| # conditions. |
| # |
| # Extraterrestrial illuminance or luminance of an object at a given altitude |
| # determined with vmag() or SB_xxx() below can be multiplied by |
| # atm_transmission() or atm_transmissionz() to estimate the terrestrial value. |
| # |
| # Kasten and Young (1989) air mass formula. alt is apparent altitude |
| # Reference: |
| # Kasten, F., and A.T. Young. 1989. "Revised Optical Air Mass Tables |
| # and Approximation Formula." Applied Optics. Vol. 28, 4735-4738. |
| # Bibcode:1989ApOpt..28.4735K. doi:10.1364/AO.28.004735. |
| |
| airmass(alt) units=[degree;1] domain=[0,90] noerror \ |
| 1 / (sin(alt) + 0.50572 (alt / degree + 6.07995)^-1.6364) |
| |
| # zenith is apparent zenith angle (zenith = 90 deg - alt) |
| airmassz(zenith) units=[degree;1] domain=[0,90] noerror \ |
| 1 / (cos(zenith) + 0.50572 (96.07995 - zenith / degree)^-1.6364) |
| |
| # For reasonably clear air at sea level; values may need adjustment for |
| # elevation and local atmospheric conditions |
| # for scotopic vision (510 nm), appropriate for the dark-adapted eye |
| # extinction_coeff 0.26 |
| # for photopic vision, appropriate for observing brighter objects such |
| # as the full moon |
| extinction_coeff 0.21 |
| |
| atm_transmission(alt) units=[degree;1] domain=[0,90] noerror \ |
| exp(-extinction_coeff airmass(alt)) |
| |
| # in terms of zenith angle (zenith = 90 deg - alt) |
| atm_transmissionz(zenith) units=[degree;1] domain=[0,90] noerror \ |
| exp(-extinction_coeff airmassz(zenith)) |
| |
| # Moon and Sun data at mean distances |
| moonvmag -12.74 # Moon apparent visual magnitude at mean distance |
| sunvmag -26.74 # Sun apparent visual magnitude at mean distance |
| moonsd asin(moonradius / moondist) # Moon angular semidiameter at mean distance |
| sunsd asin(sunradius / sundist) # Sun angular semidiameter at mean distance |
| |
| # Visual magnitude of star or other celestial object. The system of stellar |
| # magnitudes, developed in ancient Greece, assigned magnitudes from 1 |
| # (brightest) to 6 (faintest visible to the naked eye). In 1856, British |
| # astronomer Norman Pogson made the system precise, with a magnitude 1 object |
| # 100 times as bright as a magnitude 6 object, and each magnitude differing |
| # from the next by a constant ratio; the ratio, sometimes known as Pogson's |
| # ratio, is thus 100^0.2, or approximately 2.5119. The logarithm of 100^0.2 is |
| # 0.4, hence the common use of powers of 10 and base-10 logarithms. |
| # |
| # Reference: |
| # Allen, C.W. 1976. Astrophysical Quantities, 3rd ed. 1973, reprinted |
| # with corrections, 1976. London: Athlone. |
| # |
| # The function argument is the (dimensionless) visual magnitude; reference |
| # illuminance of 2.54e-6 lx is from Allen (2000, 21), and is for outside |
| # Earth's atmosphere. Illuminance values can be adjusted to terrestrial values |
| # by multiplying by one of the atm_transmission functions above. |
| |
| # Illuminance from apparent visual magnitude |
| vmag(mag) units=[1;lx] domain=[,] range=(0,] \ |
| 2.54e-6 lx 10^(-0.4 mag); -2.5 log(vmag / (2.54e-6 lx)) |
| |
| # Surface brightness of a celestial object of a given visual magnitude |
| # is a logarithmic measure of the luminance the object would have if its |
| # light were emitted by an object of specified solid angle; it is |
| # expressed in magnitudes per solid angle. Surface brightness can be |
| # obtained from the visual magnitude by |
| # S = m + 2.5 log(pi pi k a b), |
| # where k is the phase (fraction illuminated), a is the equatorial |
| # radius, and b is the polar radius. For 100% illumination (e.g., full |
| # moon), this is often simplified to |
| # S = m + 2.5 log(pi k s^2), |
| # where s is the object's angular semidiameter; the units of s determine |
| # the units of solid angle. The visual magnitude and semidiameter must |
| # be appropriate for the object's distance; for other than 100% |
| # illumination, the visual magnitude must be appropriate for the phase. |
| # Luminance values are for outside Earth's atmosphere; they can be |
| # adjusted to terrestrial values by multiplying by one of the atm_transmission |
| # functions above. |
| |
| # luminance from surface brightness in magnitudes per square degree |
| SB_degree(sb) units=[1;cd/m^2] domain=[,] range=(0,] \ |
| vmag(sb) / squaredegree ; \ |
| ~vmag(SB_degree squaredegree) |
| |
| # luminance from surface brightness in magnitudes per square minute |
| SB_minute(sb) units=[1;cd/m^2] domain=[,] range=(0,] \ |
| vmag(sb) / squareminute ; \ |
| ~vmag(SB_minute squareminute) |
| |
| # luminance from surface brightness in magnitudes per square second |
| SB_second(sb) units=[1;cd/m^2] domain=[,] range=(0,] \ |
| vmag(sb) / squaresecond ; \ |
| ~vmag(SB_second squaresecond) |
| |
| # luminance from surface brightness in magnitudes per steradian |
| SB_sr(sb) units=[1;cd/m^2] domain=[,] range=(0,] \ |
| vmag(sb) / sr ; \ |
| ~vmag(SB_sr sr) |
| |
| SB() SB_second |
| SB_sec() SB_second |
| SB_min() SB_minute |
| SB_deg() SB_degree |
| |
| # The brightness of one tenth-magnitude star per square degree outside |
| # Earth's atmosphere; often used for night sky brightness. |
| S10 SB_degree(10) |
| |
| # Examples for magnitude and surface brightness functions |
| # Sun illuminance from visual magnitude |
| # You have: sunvmag |
| # You want: |
| # Definition: -26.74 = -26.74 |
| # You have: vmag(sunvmag) |
| # You want: lx |
| # * 126134.45 |
| # / 7.9280482e-06 |
| # |
| # Moon surface brightness from visual magnitude and semidiameter at 100% |
| # illumination (full moon): |
| # You have: moonvmag |
| # You want: |
| # Definition: -12.74 = -12.74 |
| # You have: moonsd |
| # You want: arcsec |
| # * 932.59484 |
| # / 0.001072277 |
| # You have: moonvmag + 2.5 log(pi 932.59484^2) |
| # You want: |
| # Definition: 3.3513397 |
| # |
| # Similar example with specific data obtained from another source (JPL |
| # Horizons, https://ssd.jpl.nasa.gov/horizons.cgi); semidiameter is in |
| # arcseconds |
| # |
| # You have: -12.9 + 2.5 log(pi 2023.201|2^2) |
| # You want: |
| # Definition: 3.3679199 |
| # You have: SB_second(-12.9 + 2.5 log(pi 2023.201|2^2)) |
| # You want: |
| # Definition: 4858.6547 cd / m^2 |
| # |
| # If surface brightness is provided by another source (e.g., Horizons), |
| # it can simply be used directly: |
| # You have: SB_second(3.3679199) |
| # You want: cd/m^2 |
| # * 4858.6546 |
| # / 0.0002058183 |
| # The illuminance and luminance values are extraterrestrial (outside |
| # Earth's atmosphere). The values at Earth's surface are less than these |
| # because of atmospheric extinction. For example, in the last example |
| # above, if the Moon were at an altitude of 55 degrees, the terrestrial |
| # luminance could be calculated with |
| # You have: SB_second(3.3679199) |
| # You want: cd/m^2 |
| # * 4858.6546 |
| # / 0.0002058183 |
| # You have: _ atm_transmission(55 deg) |
| # You want: cd/m^2 |
| # * 3760.6356 |
| # / 0.0002659125 |
| # If desired, photographic exposure can be determined with EV100(), |
| # leading to acceptable combinations of aperture and exposure time. |
| # For the example above, but with the Moon at 10 degrees, |
| # You have: SB_second(3.3679199) atm_transmission(10 deg) |
| # You want: EV100 |
| # 13.553962 |
| |
| # |
| # The Hartree system of atomic units, derived from fundamental units |
| # of mass (of the electron), action (Planck's constant), charge, and |
| # the Coulomb constant. This system is used in the fields of physical |
| # chemistry and condensed matter physics. |
| # |
| |
| # Fundamental units |
| |
| atomicmass electronmass |
| atomiccharge e |
| atomicaction hbar |
| atomicenergy hartree |
| |
| # Derived units |
| |
| atomicvelocity sqrt(atomicenergy / atomicmass) |
| atomictime atomicaction / atomicenergy |
| atomiclength atomicvelocity atomictime |
| atomicforce atomicenergy / atomiclength |
| atomicmomentum atomicenergy / atomicvelocity |
| atomiccurrent atomiccharge / atomictime |
| atomicpotential atomicenergy / atomiccharge # electrical potential |
| atomicvolt atomicpotential |
| atomicEfield atomicpotential / atomiclength |
| atomicBfield atomicEfield / atomicvelocity |
| atomictemperature atomicenergy / boltzmann |
| |
| # |
| # In Hartree units, m_e = hbar = e = coulombconst = bohrradius = alpha*c = 1 |
| # |
| |
| !var UNITS_SYSTEM hartree |
| !message Hartree units selected |
| !prompt (hartree) |
| +hartree 1 |
| +kg 1/electronmass_SI |
| +K k_SI / hbar_SI s |
| +m alpha c_SI electronmass_SI / hbar_SI |
| +s alpha c_SI m |
| +A 1 / s e_SI |
| !endvar |
| |
| # |
| # These thermal units treat entropy as charge, from [5] |
| # |
| |
| thermalcoulomb J/K # entropy |
| thermalampere W/K # entropy flow |
| thermalfarad J/K^2 |
| thermalohm K^2/W # thermal resistance |
| fourier thermalohm |
| thermalhenry J K^2/W^2 # thermal inductance |
| thermalvolt K # thermal potential difference |
| |
| |
| # |
| # United States units |
| # |
| |
| # linear measure |
| |
| # The US Metric Law of 1866 legalized the metric system in the USA and |
| # defined the meter in terms of the British system with the exact |
| # 1 meter = 39.37 inches. On April 5, 1893 Thomas Corwin Mendenhall, |
| # Superintendent of Weights and Measures, decided, in what has become |
| # known as the "Mendenhall Order" that the meter and kilogram would be the |
| # fundamental standards in the USA. The definition from 1866 was turned |
| # around to give an exact definition of the yard as 3600|3937 meters This |
| # definition was used until July of 1959 when the definition was changed |
| # to bring the US and other English-speaking countries into agreement; the |
| # Canadian value of 1 yard = 0.9144 meter (exactly) was chosen because it |
| # was approximately halfway between the British and US values; it had the |
| # added advantage of making 1 inch = 25.4 mm (exactly). Since 1959, the |
| # "international" foot has been exactly 0.3048 meters. At the same time, |
| # it was decided that any data expressed in feet derived from geodetic |
| # surveys within the US would continue to use the old definition and call |
| # the old unit the "survey foot." |
| # |
| # Until 1 January 2023, the US continued to define the statute |
| # mile, furlong, chain, rod, link, and fathom in terms of the US survey |
| # foot. Since then, use of the US survey foot has been officially |
| # deprecated, with its use limited to historical and legacy applications. |
| # These units are now defined in terms of the international foot. |
| # |
| # Sources: |
| # NIST Special Publication 447, Sects. 5, 7, and 8. |
| # NIST Handbook 44, 2024 ed., Appendix C. |
| # Canadian Journal of Physics, 1959, 37:(1) 84, 10.1139/p59-014. |
| |
| inch 2.54 cm # Exact, international inch (1959) |
| in inch |
| foot 12 inch |
| feet foot |
| ft foot |
| yard 3 ft |
| yd yard |
| mile 5280 ft # The mile was enlarged from 5000 ft |
| # to this number in order to make |
| # it an even number of furlongs. |
| # (The Roman mile is 5000 romanfeet.) |
| line 1|12 inch # Also defined as '.1 in' or as '1e-8 Wb' |
| rod 16.5 ft |
| pole rod |
| perch rod |
| furlong 40 rod # From "furrow long" |
| statutemile mile |
| league 3 mile # Intended to be an hour's walk |
| |
| # surveyor's measure |
| # The US survey foot is officially deprecated as of 1 January 2023 |
| US 1200|3937 m/ft # These four values will convert |
| US- US # international measures to |
| survey- US # US Survey measures |
| geodetic- US |
| int 3937|1200 ft/m # Convert US Survey measures to |
| int- int # international measures |
| |
| # values based on the US survey foot are deprecated as of 1 January 2023 |
| surveyorschain 66 surveyft |
| surveychain surveyorschain |
| surveyorspole 1|4 surveyorschain |
| surveyorslink 1|100 surveyorschain |
| USacre 10 surveychain^2 |
| USacrefoot USacre surveyfoot |
| |
| chain 66 ft |
| link 1|100 chain |
| ch chain |
| intacre 10 chain^2 # Acre based on international ft |
| intacrefoot acre foot |
| acrefoot intacrefoot |
| acre intacre |
| ac acre |
| section mile^2 |
| township 36 section |
| homestead 160 acre # Area of land granted by the 1862 Homestead |
| # Act of the United States Congress |
| gunterschain surveyorschain |
| |
| engineerschain 100 ft |
| engineerslink 1|100 engineerschain |
| ramsdenschain engineerschain |
| ramsdenslink engineerslink |
| |
| gurleychain 33 feet # Andrew Ellicott chain is the |
| gurleylink 1|50 gurleychain # same length |
| |
| wingchain 66 feet # Chain from 1664, introduced by |
| winglink 1|80 wingchain # Vincent Wing, also found in a |
| # 33 foot length with 40 links. |
| # early US length standards |
| |
| # The US has had four standards for the yard: one by Troughton of London |
| # (1815); bronze yard #11 (1856); the Mendhall yard (1893), consistent |
| # with the definition of the meter in the metric joint resolution of |
| # Congress in 1866, but defining the yard in terms of the meter; and the |
| # international yard (1959), which standardized definitions for Australia, |
| # Canada, New Zealand, South Africa, the UK, and the US. |
| # Sources: Pat Naughtin (2009), Which Inch?: |
| # https://metricationmatters.org/docs/WhichInch.pdf, |
| # Lewis E. Barbrow and Lewis V. Judson (1976). NBS Special |
| # Publication 447, Weights and Measures Standards of the United States: A |
| # Brief History. |
| |
| troughtonyard 914.42190 mm |
| bronzeyard11 914.39980 mm |
| mendenhallyard surveyyard |
| internationalyard yard |
| |
| # nautical measure |
| |
| fathom 6 ft # Originally defined as the distance from |
| # fingertip to fingertip with arms fully |
| # extended. |
| nauticalmile 1852 m # Supposed to be one minute of latitude at |
| # the equator. That value is about 1855 m. |
| # Early estimates of Earth's circumference |
| # were a bit off. The value of 1852 m was |
| # made the international standard in 1929. |
| # The US did not accept this value until |
| # 1954. The UK switched in 1970. |
| |
| # The cable is used for depth in water and has a wide range of definitions |
| |
| intcable 1|10 nauticalmile # international cable |
| uscable 120 fathom # value after 1 January 2023 |
| surveycable 120 USfathom # value before 1 January 2023 |
| UScable surveycable |
| cableslength cable |
| cablelength cable |
| navycablelength cable |
| brcable 1|10 brnauticalmile |
| admiraltycable brcable |
| |
| marineleague 3 nauticalmile |
| geographicalmile brnauticalmile |
| knot nauticalmile / hr |
| click km # US military slang |
| klick click |
| |
| # Avoirdupois weight |
| |
| pound 0.45359237 kg # Exact, International Pound (1959) |
| lb pound # From the Latin libra |
| grain 1|7000 pound # The grain is the same in all three |
| # weight systems. It was originally |
| # defined as the weight of a barley |
| # corn taken from the middle of the |
| # ear. |
| ounce 1|16 pound |
| oz ounce |
| dram 1|16 ounce |
| dr dram |
| ushundredweight 100 pounds |
| cwt hundredweight |
| shorthundredweight ushundredweight |
| uston shortton |
| shortton 2000 lb |
| quarterweight 1|4 uston |
| shortquarterweight 1|4 shortton |
| shortquarter shortquarterweight |
| |
| # Troy Weight. In 1828 the troy pound was made the first United States |
| # standard weight. It was to be used to regulate coinage. |
| |
| troypound 5760 grain |
| troyounce 1|12 troypound |
| ozt troyounce |
| pennyweight 1|20 troyounce # Abbreviated "d" in reference to a |
| dwt pennyweight # Frankish coin called the "denier" |
| # minted in the late 700's. There |
| # were 240 deniers to the pound. |
| assayton mg ton / troyounce # mg / assayton = troyounce / ton |
| usassayton mg uston / troyounce |
| brassayton mg brton / troyounce |
| fineounce troyounce # A troy ounce of 99.5% pure gold |
| |
| # Some other jewelers units |
| |
| metriccarat 0.2 gram # Defined in 1907 |
| metricgrain 50 mg |
| carat metriccarat |
| ct carat |
| jewelerspoint 1|100 carat |
| silversmithpoint 1|4000 inch |
| momme 3.75 grams # Traditional Japanese unit based |
| # on the chinese mace. It is used for |
| # pearls in modern times and also for |
| # silk density. The definition here |
| # was adopted in 1891. |
| # Apothecaries' weight |
| |
| appound troypound |
| apounce troyounce |
| apdram 1|8 apounce |
| apscruple 1|3 apdram |
| |
| # Liquid measure |
| |
| usgallon 231 in^3 # US liquid measure is derived from |
| gal gallon # the British wine gallon of 1707. |
| quart 1|4 gallon # See the "winegallon" entry below |
| pint 1|2 quart # more historical information. |
| gill 1|4 pint |
| usquart 1|4 usgallon |
| uspint 1|2 usquart |
| usgill 1|4 uspint |
| usfluidounce 1|16 uspint |
| fluiddram 1|8 usfloz |
| minimvolume 1|60 fluiddram |
| qt quart |
| pt pint |
| floz fluidounce |
| usfloz usfluidounce |
| fldr fluiddram |
| liquidbarrel 31.5 usgallon |
| usbeerbarrel 2 beerkegs |
| beerkeg 15.5 usgallon # Various among brewers |
| ponykeg 1|2 beerkeg |
| winekeg 12 usgallon |
| petroleumbarrel 42 usgallon # Originated in Pennsylvania oil |
| barrel petroleumbarrel # fields, from the winetierce |
| bbl barrel |
| ushogshead 2 liquidbarrel |
| usfirkin 9 usgallon |
| |
| # Dry measures: The Winchester Bushel was defined by William III in 1702 and |
| # legally adopted in the US in 1836. |
| |
| usbushel 2150.42 in^3 # Volume of 8 inch cylinder with 18.5 |
| bu bushel # inch diameter (rounded) |
| peck 1|4 bushel |
| uspeck 1|4 usbushel |
| brpeck 1|4 brbushel |
| pk peck |
| drygallon 1|2 uspeck |
| dryquart 1|4 drygallon |
| drypint 1|2 dryquart |
| drybarrel 7056 in^3 # Used in US for fruits, vegetables, |
| # and other dry commodities except for |
| # cranberries. |
| cranberrybarrel 5826 in^3 # US cranberry barrel |
| heapedbushel 1.278 usbushel# The following explanation for this |
| # value was provided by Wendy Krieger |
| # <os2fan2@yahoo.com> based on |
| # guesswork. The cylindrical vessel is |
| # 18.5 inches in diameter and 1|2 inch |
| # thick. A heaped bushel includes the |
| # contents of this cylinder plus a heap |
| # on top. The heap is a cone 19.5 |
| # inches in diameter and 6 inches |
| # high. With these values, the volume |
| # of the bushel is 684.5 pi in^3 and |
| # the heap occupies 190.125 pi in^3. |
| # Therefore, the heaped bushel is |
| # 874.625|684.5 bushels. This value is |
| # approximately 1.2777575 and it rounds |
| # to the value listed for the size of |
| # the heaped bushel. Sometimes the |
| # heaped bushel is reported as 1.25 |
| # bushels. This same explanation gives |
| # that value if the heap is taken to |
| # have an 18.5 inch diameter. |
| |
| # Grain measures. The bushel as it is used by farmers in the USA is actually |
| # a measure of mass which varies for different commodities. Canada uses the |
| # same bushel masses for most commodities, but not for oats. |
| |
| wheatbushel 60 lb |
| soybeanbushel 60 lb |
| cornbushel 56 lb |
| ryebushel 56 lb |
| barleybushel 48 lb |
| oatbushel 32 lb |
| ricebushel 45 lb |
| canada_oatbushel 34 lb |
| |
| # Wine and Spirits measure |
| |
| ponyvolume 1 usfloz |
| jigger 1.5 usfloz # Can vary between 1 and 2 usfloz |
| shot jigger # Sometimes 1 usfloz |
| eushot 25 ml # EU standard spirits measure |
| fifth 1|5 usgallon |
| winebottle 750 ml # US industry standard, 1979 |
| winesplit 1|4 winebottle |
| magnum 1.5 liter # Standardized in 1979, but given |
| # as 2 qt in some references |
| metrictenth 375 ml |
| metricfifth 750 ml |
| metricquart 1 liter |
| |
| # Old British bottle size |
| |
| reputedquart 1|6 brgallon |
| reputedpint 1|2 reputedquart |
| brwinebottle reputedquart # Very close to 1|5 winegallon |
| |
| # French champagne bottle sizes |
| |
| split 200 ml |
| jeroboam 2 magnum |
| rehoboam 3 magnum |
| methuselah 4 magnum |
| imperialbottle 4 magnum |
| salmanazar 6 magnum |
| balthazar 8 magnum |
| nebuchadnezzar 10 magnum |
| solomon 12 magnum |
| melchior 12 magnum |
| sovereign 17.5 magnum |
| primat 18 magnum |
| goliath 18 magnum |
| melchizedek 20 magnum |
| midas 20 magnum |
| |
| # The wine glass doesn't seem to have an official standard, but the same value |
| # is suggested by several sources in the US. |
| |
| wineglass 150 mL |
| |
| # In the UK, serving size offerings legally mandated by The Weights and |
| # Measures (Specified Quantities) (Unwrapped Bread and Intoxicating |
| # Liquor) Order 2011, effective 1st October 2011. The quantities--not |
| # the names--are mandated. Lawful size offerings are these or multiples |
| # thereof, but other sizes can be provided at the express request of a |
| # buyer. |
| |
| smallwineglass 125 mL |
| mediumwineglass 175 mL |
| |
| # Values vary considerably among countries and even more so in practice. The |
| # "standard" US value gives 5 glasses per standard 750 ml bottle. Old practice |
| # in the UK was 125 ml per glass, or 6 glasses per bottle. Some sources suggest |
| # a more recent common value of 250 ml per glass, or 3 glasses per |
| # bottle; as a multiple of 125 ml, this would be a lawful serving size offering. |
| # |
| # The value refers to the size of the serving, not the total volume of the |
| # glass, which is typically not filled above the height of its greatest |
| # diameter. |
| # |
| # A unit of alcohol is a specified amount of pure ethyl alcohol, expressed as a |
| # mass or volumetric equivalent. Many countries use the same concept but use |
| # different terms. "Alcohol unit" is used officially in the UK; the US, Canada, |
| # and Australia use "standard drink." Values vary considerably among |
| # countries. The UK value of 8 g is nominally the amount of alcohol that a |
| # typical adult can metabolize in one hour. |
| |
| alcoholunitus 14 g / ethanoldensity |
| alcoholunitca 13.6 g / ethanoldensity |
| alcoholunituk 8 g / ethanoldensity |
| alcoholunitau 10 g / ethanoldensity |
| |
| # Common serving sizes have roughly equivalent amounts of alcohol, as |
| # illustrated by US examples for wine (12% Alcohol By Volume), beer (5% ABV), |
| # and spirits (80 proof). |
| # |
| # alcoholunitus / 12% = 147.8 mL, close to the "standard" serving of 150 mL. |
| # alcoholunitus / 5% = 11.995346 floz, close to a standard 12 floz bottle or can |
| # alcoholunitus / 80 proof = 1.4994182 floz, close to a standard "shot" or jigger |
| |
| # https://www.rethinkingdrinking.niaaa.nih.gov/ |
| # https://www.cdc.gov/alcohol/faqs.htm |
| # https://www.canada.ca/en/health-canada/services/substance-use/alcohol/low-risk-alcohol-drinking-guidelines |
| # https://www.drinkaware.co.uk/ |
| # https://www.drinkaware.co.uk/facts/alcoholic-drinks-and-units |
| # https://www.gov.uk/government/uploads/system/uploads/attachment_data/file/545937/UK_CMOs__report.pdf |
| # https://adf.org.au/reducing-risk/alcohol/alcohol-guidelines/ |
| # https://www.health.gov.au/topics/alcohol/about-alcohol/standard-drinks-guide |
| # https://en.wikipedia.org/wiki/Unit_of_alcohol |
| # https://en.wikipedia.org/wiki/Standard_drink |
| |
| # Coffee |
| # |
| # The recommended ratio of coffee to water. Values vary considerably; |
| # one is from the Specialty Coffee Association of America: Brewing Best Practices |
| # https://sca.coffee/research/protocols-best-practices |
| |
| coffeeratio 55 g/L # +/- 10% |
| |
| # other recommendations are more loose, e.g., |
| # http://www.ncausa.org/About-Coffee/How-to-Brew-Coffee |
| |
| |
| # |
| # Water is "hard" if it contains various minerals, especially calcium |
| # carbonate. |
| # |
| |
| clarkdegree grains/brgallon # Content by weigh of calcium carbonate |
| gpg grains/usgallon # Divide by water's density to convert to |
| # a dimensionless concentration measure |
| # |
| # Shoe measures |
| # |
| |
| shoeiron 1|48 inch # Used to measure leather in soles |
| shoeounce 1|64 inch # Used to measure non-sole shoe leather |
| |
| # USA shoe sizes. These express the length of the shoe or the length |
| # of the "last", the form that the shoe is made on. But note that |
| # this only captures the length. It appears that widths change 1/4 |
| # inch for each letter within the same size, and if you change the |
| # length by half a size then the width changes between 1/8 inch and |
| # 1/4 inch. But this may not be standard. If you know better, please |
| # contact me. |
| |
| shoesize_delta 1|3 inch # USA shoe sizes differ by this amount |
| shoe_men0 8.25 inch |
| shoe_women0 (7+11|12) inch |
| shoe_boys0 (3+11|12) inch |
| shoe_girls0 (3+7|12) inch |
| |
| shoesize_men(n) units=[1;inch] shoe_men0 + n shoesize_delta ; \ |
| (shoesize_men+(-shoe_men0))/shoesize_delta |
| shoesize_women(n) units=[1;inch] shoe_women0 + n shoesize_delta ; \ |
| (shoesize_women+(-shoe_women0))/shoesize_delta |
| shoesize_boys(n) units=[1;inch] shoe_boys0 + n shoesize_delta ; \ |
| (shoesize_boys+(-shoe_boys0))/shoesize_delta |
| shoesize_girls(n) units=[1;inch] shoe_girls0 + n shoesize_delta ; \ |
| (shoesize_girls+(-shoe_girls0))/shoesize_delta |
| |
| # European shoe size. According to |
| # http://www.shoeline.com/footnotes/shoeterm.shtml |
| # shoe sizes in Europe are measured with Paris points which simply measure |
| # the length of the shoe. |
| |
| europeshoesize 2|3 cm |
| |
| # |
| # USA slang units |
| # |
| |
| buck US$ |
| fin 5 US$ |
| sawbuck 10 US$ |
| usgrand 1000 US$ |
| greenback US$ |
| key kg # usually of marijuana, 60's |
| lid 1 oz # Another 60's weed unit |
| footballfield usfootballfield |
| usfootballfield 100 yards |
| canadafootballfield 110 yards # And 65 yards wide |
| marathon 26 miles + 385 yards |
| |
| # |
| # British |
| # |
| |
| # The length measure in the UK was defined by a bronze bar manufactured in |
| # 1844. Various conversions were sanctioned for convenience at different |
| # times, which makes conversions before 1963 a confusing matter. Apparently |
| # previous conversions were never explicitly revoked. Four different |
| # conversion factors appear below. Multiply them times an imperial length |
| # units as desired. The Weights and Measures Act of 1963 switched the UK away |
| # from their bronze standard and onto a definition of the yard in terms of the |
| # meter. This happened after an international agreement in 1959 to align the |
| # world's measurement systems. |
| |
| UK UKlength_SJJ |
| UK- UK |
| british- UK |
| |
| UKlength_B 0.9143992 meter / yard # Benoit found the yard to be |
| # 0.9143992 m at a weights and |
| # measures conference around |
| # 1896. Legally sanctioned |
| # in 1898. |
| UKlength_SJJ 0.91439841 meter / yard # In 1922, Seers, Jolly and |
| # Johnson found the yard to be |
| # 0.91439841 meters. |
| # Used starting in the 1930's. |
| UKlength_K meter / 39.37079 inch # In 1816 Kater found this ratio |
| # for the meter and inch. This |
| # value was used as the legal |
| # conversion ratio when the |
| # metric system was legalized |
| # for contract in 1864. |
| UKlength_C meter / 1.09362311 yard # In 1866 Clarke found the meter |
| # to be 1.09362311 yards. This |
| # conversion was legalized |
| # around 1878. |
| brnauticalmile 6080 ft # Used until 1970 when the UK |
| brknot brnauticalmile / hr # switched to the international |
| admiraltymile brnauticalmile # nautical mile. |
| admiraltyknot brknot |
| seamile 6000 ft |
| shackle 15 fathoms # Adopted 1949 by British navy |
| |
| # British Imperial weight is mostly the same as US weight. A few extra |
| # units are added here. |
| |
| clove 7 lb |
| stone 14 lb |
| tod 28 lb |
| brquarterweight 1|4 brhundredweight |
| brhundredweight 8 stone |
| longhundredweight brhundredweight |
| longton 20 brhundredweight |
| brton longton |
| |
| # British Imperial volume measures |
| |
| brminim 1|60 brdram |
| brscruple 1|3 brdram |
| fluidscruple brscruple |
| brdram 1|8 brfloz |
| brfluidounce 1|20 brpint |
| brfloz brfluidounce |
| brgill 1|4 brpint |
| brpint 1|2 brquart |
| brquart 1|4 brgallon |
| brgallon 4.54609 l # The British Imperial gallon was |
| # defined in 1824 to be the volume of |
| # water which weighed 10 pounds at 62 |
| # deg F with a pressure of 30 inHg. |
| # It was also defined as 277.274 in^3, |
| # Which is slightly in error. In |
| # 1963 it was defined to be the volume |
| # occupied by 10 pounds of distilled |
| # water of density 0.998859 g/ml weighed |
| # in air of density 0.001217 g/ml |
| # against weights of density 8.136 g/ml. |
| # This gives a value of approximately |
| # 4.5459645 liters, but the old liter |
| # was in force at this time. In 1976 |
| # the definition was changed to exactly |
| # 4.54609 liters using the new |
| # definition of the liter (1 dm^3). |
| brbarrel 36 brgallon # Used for beer |
| brbushel 8 brgallon |
| brheapedbushel 1.278 brbushel |
| brquarter 8 brbushel |
| brchaldron 36 brbushel |
| |
| # Obscure British volume measures. These units are generally traditional |
| # measures whose definitions have fluctuated over the years. Often they |
| # depended on the quantity being measured. They are given here in terms of |
| # British Imperial measures. For example, the puncheon may have historically |
| # been defined relative to the wine gallon or beer gallon or ale gallon |
| # rather than the British Imperial gallon. |
| |
| bag 4 brbushel |
| bucket 4 brgallon |
| kilderkin 2 brfirkin |
| last 40 brbushel |
| noggin brgill |
| pottle 0.5 brgallon |
| pin 4.5 brgallon |
| puncheon 72 brgallon |
| seam 8 brbushel |
| coomb 4 brbushel |
| boll 6 brbushel |
| firlot 1|4 boll |
| brfirkin 9 brgallon # Used for ale and beer |
| cran 37.5 brgallon # measures herring, about 750 fish |
| brwinehogshead 52.5 brgallon # This value is approximately equal |
| brhogshead brwinehogshead # to the old wine hogshead of 63 |
| # wine gallons. This adjustment |
| # is listed in the OED and in |
| # "The Weights and Measures of |
| # England" by R. D. Connor |
| brbeerhogshead 54 brgallon |
| brbeerbutt 2 brbeerhogshead |
| registerton 100 ft^3 # Used for internal capacity of ships |
| shippington 40 ft^3 # Used for ship's cargo freight or timber |
| brshippington 42 ft^3 # |
| freightton shippington # Both register ton and shipping ton derive |
| # from the "tun cask" of wine. |
| displacementton 35 ft^3 # Approximate volume of a longton weight of |
| # sea water. Measures water displaced by |
| # ships. |
| waterton 224 brgallon |
| strike 70.5 l # 16th century unit, sometimes |
| # defined as .5, 2, or 4 bushels |
| # depending on the location. It |
| # probably doesn't make a lot of |
| # sense to define in terms of imperial |
| # bushels. Zupko gives a value of |
| # 2 Winchester grain bushels or about |
| # 70.5 liters. |
| amber 4 brbushel# Used for dry and liquid capacity [18] |
| |
| # British volume measures with "imperial" |
| |
| imperialminim brminim |
| imperialscruple brscruple |
| imperialdram brdram |
| imperialfluidounce brfluidounce |
| imperialfloz brfloz |
| imperialgill brgill |
| imperialpint brpint |
| imperialquart brquart |
| imperialgallon brgallon |
| imperialbarrel brbarrel |
| imperialbushel brbushel |
| imperialheapedbushel brheapedbushel |
| imperialquarter brquarter |
| imperialchaldron brchaldron |
| imperialwinehogshead brwinehogshead |
| imperialhogshead brhogshead |
| imperialbeerhogshead brbeerhogshead |
| imperialbeerbutt brbeerbutt |
| imperialfirkin brfirkin |
| |
| # obscure British lengths |
| |
| barleycorn 1|3 UKinch # Given in Realm of Measure as the |
| # difference between successive shoe sizes |
| nail 1|16 UKyard # Originally the width of the thumbnail, |
| # or 1|16 ft. This took on the general |
| # meaning of 1|16 and settled on the |
| # nail of a yard or 1|16 yards as its |
| # final value. [12] |
| UKpole 16.5 UKft # This was 15 Saxon feet, the Saxon |
| rope 20 UKft # foot (aka northern foot) being longer |
| englishell 45 UKinch |
| flemishell 27 UKinch |
| ell englishell # supposed to be measure from elbow to |
| # fingertips |
| span 9 UKinch # supposed to be distance from thumb |
| # to pinky with full hand extension |
| goad 4.5 UKft # used for cloth, possibly named after the |
| # stick used for prodding animals. |
| |
| # misc obscure British units |
| |
| hide 120 acre # English unit of land area dating to the 7th |
| # century, originally the amount of land |
| # that a single plowman could cultivate, |
| # which varied from 60-180 acres regionally. |
| # Standardized at Normon conquest. |
| virgate 1|4 hide |
| nook 1|2 virgate |
| rood furlong rod # Area of a strip a rod by a furlong |
| englishcarat troyounce/151.5 # Originally intended to be 4 grain |
| # but this value ended up being |
| # used in the London diamond market |
| mancus 2 oz |
| mast 2.5 lb |
| nailkeg 100 lbs |
| basebox 31360 in^2 # Used in metal plating |
| |
| # alternate spellings |
| |
| gramme gram |
| litre liter |
| dioptre diopter |
| sulphur sulfur |
| |
| # |
| # Units derived the human body (may not be very accurate) |
| # |
| |
| geometricpace 5 ft # distance between points where the same |
| # foot hits the ground |
| pace 2.5 ft # distance between points where alternate |
| # feet touch the ground |
| USmilitarypace 30 in # United States official military pace |
| USdoubletimepace 36 in # United States official doubletime pace |
| fingerbreadth 7|8 in # The finger is defined as either the width |
| fingerlength 4.5 in # or length of the finger |
| finger fingerbreadth |
| palmwidth hand # The palm is a unit defined as either the width |
| palmlength 8 in # or the length of the hand |
| hand 4 inch # width of hand |
| shaftment 6 inch # Distance from tip of outstretched thumb to the |
| # opposite side of the palm of the hand. The |
| # ending -ment is from the old English word |
| # for hand. [18] |
| smoot 5 ft + 7 in # Created as part of an MIT fraternity prank. |
| # In 1958 Oliver Smoot was used to measure |
| # the length of the Harvard Bridge, which was |
| # marked off in Smoot lengths. These |
| # markings have been maintained on the bridge |
| # since then and repainted by subsequent |
| # incoming fraternity members. During a |
| # bridge renovation the new sidewalk was |
| # scored every Smoot rather than at the |
| # customary 6 ft spacing. |
| tomcruise 5 ft + 7.75 in # Height of Tom Cruise |
| |
| # |
| # Cooking measures |
| # |
| |
| # Common abbreviations |
| |
| tbl tablespoon |
| tbsp tablespoon |
| tblsp tablespoon |
| Tb tablespoon |
| tsp teaspoon |
| saltspoon 1|4 tsp |
| |
| # US measures |
| |
| uscup 8 usfloz |
| ustablespoon 1|16 uscup |
| usteaspoon 1|3 ustablespoon |
| ustbl ustablespoon |
| ustbsp ustablespoon |
| ustblsp ustablespoon |
| ustsp usteaspoon |
| metriccup 250 ml |
| stickbutter 1|4 lb # Butter in the USA is sold in one |
| # pound packages that contain four |
| # individually wrapped pieces. The |
| # pieces are marked into tablespoons, |
| # making it possible to measure out |
| # butter by volume by slicing the |
| # butter. |
| |
| legalcup 240 ml # The cup used on nutrition labeling |
| legaltablespoon 1|16 legalcup |
| legaltbsp legaltablespoon |
| |
| # Scoop size. Ice cream scoops in the US are marked with numbers |
| # indicating the number of scoops required to fill a US quart. |
| |
| scoop(n) units=[1;cup] domain=[4,100] range=[0.04,1] \ |
| 32 usfloz / n ; 32 usfloz / scoop |
| |
| |
| # US can sizes. |
| |
| number1can 10 usfloz |
| number2can 19 usfloz |
| number2.5can 3.5 uscups |
| number3can 4 uscups |
| number5can 7 uscups |
| number10can 105 usfloz |
| |
| # British measures |
| |
| brcup 1|2 brpint |
| brteacup 1|3 brpint |
| brtablespoon 15 ml # Also 5|8 brfloz, approx 17.7 ml |
| brteaspoon 1|3 brtablespoon # Also 1|4 brtablespoon |
| brdessertspoon 2 brteaspoon |
| dessertspoon brdessertspoon |
| dsp dessertspoon |
| brtsp brteaspoon |
| brtbl brtablespoon |
| brtbsp brtablespoon |
| brtblsp brtablespoon |
| |
| # Australian |
| |
| australiatablespoon 20 ml |
| austbl australiatablespoon |
| austbsp australiatablespoon |
| austblsp australiatablespoon |
| australiateaspoon 1|4 australiatablespoon |
| austsp australiateaspoon |
| |
| # Italian |
| |
| etto 100 g # Used for buying items like meat and |
| etti etto # cheese. |
| |
| # Chinese |
| |
| catty 0.5 kg |
| oldcatty 4|3 lbs # Before metric conversion. |
| tael 1|16 oldcatty # Should the tael be defined both ways? |
| mace 0.1 tael |
| oldpicul 100 oldcatty |
| picul 100 catty # Chinese usage |
| |
| # Indian |
| |
| seer 14400 grain # British Colonial standard |
| ser seer |
| maund 40 seer |
| pakistanseer 1 kg |
| pakistanmaund 40 pakistanseer |
| chittak 1|16 seer |
| tola 1|5 chittak |
| ollock 1|4 liter # Is this right? |
| |
| # Japanese |
| |
| japancup 200 ml |
| |
| # densities of cooking ingredients from The Cake Bible by Rose Levy Beranbaum |
| # so you can convert '2 cups sugar' to grams, for example, or in the other |
| # direction grams could be converted to 'cup flour_scooped'. |
| |
| butter 8 oz/uscup |
| butter_clarified 6.8 oz/uscup |
| cocoa_butter 9 oz/uscup |
| shortening 6.75 oz/uscup # vegetable shortening |
| oil 7.5 oz/uscup |
| cakeflour_sifted 3.5 oz/uscup # The density of flour depends on the |
| cakeflour_spooned 4 oz/uscup # measuring method. "Scooped", or |
| cakeflour_scooped 4.5 oz/uscup # "dip and sweep" refers to dipping a |
| flour_sifted 4 oz/uscup # measure into a bin, and then sweeping |
| flour_spooned 4.25 oz/uscup # the excess off the top. "Spooned" |
| flour_scooped 5 oz/uscup # means to lightly spoon into a measure |
| breadflour_sifted 4.25 oz/uscup # and then sweep the top. Sifted means |
| breadflour_spooned 4.5 oz/uscup # sifting the flour directly into a |
| breadflour_scooped 5.5 oz/uscup # measure and then sweeping the top. |
| cornstarch 120 grams/uscup |
| dutchcocoa_sifted 75 g/uscup # These are for Dutch processed cocoa |
| dutchcocoa_spooned 92 g/uscup |
| dutchcocoa_scooped 95 g/uscup |
| cocoa_sifted 75 g/uscup # These are for nonalkalized cocoa |
| cocoa_spooned 82 g/uscup |
| cocoa_scooped 95 g/uscup |
| heavycream 232 g/uscup |
| milk 242 g/uscup |
| sourcream 242 g/uscup |
| molasses 11.25 oz/uscup |
| cornsyrup 11.5 oz/uscup |
| honey 11.75 oz/uscup |
| sugar 200 g/uscup |
| powdered_sugar 4 oz/uscup |
| brownsugar_light 217 g/uscup # packed |
| brownsugar_dark 239 g/uscup |
| |
| baking_powder 4.6 grams / ustsp |
| salt 6 g / ustsp |
| koshersalt 2.8 g / ustsp # Diamond Crystal kosher salt |
| koshersalt_morton 4.8 g / ustsp # Morton kosher salt |
| # Values are from the nutrition info |
| # on the packages |
| |
| |
| # Egg weights and volumes for a USA large egg |
| |
| egg 50 grams # without shell |
| eggwhite 30 grams |
| eggyolk 18.6 grams |
| eggvolume 3 ustablespoons + 1|2 ustsp |
| eggwhitevolume 2 ustablespoons |
| eggyolkvolume 3.5 ustsp |
| |
| # Alcohol density |
| |
| ethanoldensity 0.7893 g/cm^3 # From CRC Handbook, 91st Edition |
| alcoholdensity ethanoldensity |
| |
| # |
| # Density measures. Density has traditionally been measured on a variety of |
| # bizarre nonlinear scales. |
| # |
| |
| # Density of a sugar syrup is frequently measured in candy making procedures. |
| # In the USA the boiling point of the syrup is measured. Some recipes instead |
| # specify the density using degrees Baume. Conversion between degrees Baume |
| # and the boiling point measure has proved elusive. This table appeared in one |
| # text, and provides a fragmentary relationship to the concentration. |
| # |
| # temp(C) conc (%) |
| # 100 30 |
| # 101 40 |
| # 102 50 |
| # 103 60 |
| # 106 70 |
| # 112 80 |
| # 123 90 |
| # 140 95 |
| # 151 97 |
| # 160 98.2 |
| # 166 99.5 |
| # 171 99.6 |
| # |
| # The best source identified to date came from "Boiling point elevation of |
| # technical sugarcane solutions and its use in automatic pan boiling" by |
| # Michael Saska. International Sugar Journal, 2002, 104, 1247, pp 500-507. |
| # |
| # But I'm using equation (3) which is credited to Starzak and Peacock, |
| # "Water activity coefficient in aqueous solutions of sucrose--A comprehensive |
| # data analysis. Zuckerindustrie, 122, 380-387. (I couldn't find this |
| # document.) |
| # |
| # Note that the range of validity is uncertain, but answers are in agreement |
| # with the above table all the way to 99.6. |
| # |
| # The original equation has a parameter for the boiling point of water, which |
| # of course varies with altitude. It also includes various other model |
| # parameters. The input is the molar concentration of sucrose in the solution, |
| # (moles sucrose) / (total moles). |
| # |
| # Bsp 3797.06 degC |
| # Csp 226.28 degC |
| # QQ -17638 J/mol |
| # asp -1.0038 |
| # bsp -0.24653 |
| # tbw 100 degC # boiling point of water |
| # sugar_bpe_orig(x) ((1-QQ/R Bsp * x^2 (1+asp x + bsp x^2) (tbw + Csp) \ |
| # /(tbw+stdtemp)) / (1+(tbw + Csp)/Bsp *ln(1-x))-1) * (tbw + Csp) |
| # |
| # To convert mass concentration (brix) to molar concentration |
| # |
| # sc(x) (x / 342.3) / (( x/342.3) + (100-x)/18.02); \ |
| # 100 sc 342.3|18.02 / (sc (342.3|18.02-1)+1) |
| # |
| # Here is a simplified version of this equation where the temperature of boiling |
| # water has been fixed at 100 degrees Celsius and the argument is now the |
| # concentration (brix). |
| # |
| # sugar_bpe(x) ((1+ 0.48851085 * sc(x)^2 (1+ -1.0038 sc(x) + -0.24653 sc(x)^2)) \ |
| # / (1+0.08592964 ln(1-sc(x)))-1) 326.28 K |
| # |
| # |
| # The formula is not invertible, so to implement it in units we unfortunately |
| # must turn it into a table. |
| |
| # This table gives the boiling point elevation as a function of the sugar syrup |
| # concentration expressed as a percentage. |
| |
| sugar_conc_bpe[K] \ |
| 0 0.0000 5 0.0788 10 0.1690 15 0.2729 20 0.3936 25 0.5351 \ |
| 30 0.7027 35 0.9036 40 1.1475 42 1.2599 44 1.3825 46 1.5165 \ |
| 48 1.6634 50 1.8249 52 2.0031 54 2.2005 56 2.4200 58 2.6651 \ |
| 60 2.9400 61 3.0902 62 3.2499 63 3.4198 64 3.6010 65 3.7944 \ |
| 66 4.0012 67 4.2227 68 4.4603 69 4.7156 70 4.9905 71 5.2870 \ |
| 72 5.6075 73 5.9546 74 6.3316 75 6.7417 76 7.1892 77 7.6786 \ |
| 78.0 8.2155 79.0 8.8061 80.0 9.4578 80.5 9.8092 81.0 10.1793 \ |
| 81.5 10.5693 82.0 10.9807 82.5 11.4152 83.0 11.8743 83.5 12.3601 \ |
| 84.0 12.8744 84.5 13.4197 85.0 13.9982 85.5 14.6128 86.0 15.2663 \ |
| 86.5 15.9620 87.0 16.7033 87.5 17.4943 88.0 18.3391 88.5 19.2424 \ |
| 89.0 20.2092 89.5 21.2452 90.0 22.3564 90.5 23.5493 91.0 24.8309 \ |
| 91.5 26.2086 92.0 27.6903 92.5 29.2839 93.0 30.9972 93.5 32.8374 \ |
| 94.0 34.8104 94.5 36.9195 95.0 39.1636 95.5 41.5348 96.0 44.0142 \ |
| 96.5 46.5668 97.0 49.1350 97.5 51.6347 98.0 53.9681 98.1 54.4091 \ |
| 98.2 54.8423 98.3 55.2692 98.4 55.6928 98.5 56.1174 98.6 56.5497 \ |
| 98.7 56.9999 98.8 57.4828 98.9 58.0206 99.0 58.6455 99.1 59.4062 \ |
| 99.2 60.3763 99.3 61.6706 99.4 63.4751 99.5 66.1062 99.6 70.1448 \ |
| 99.7 76.7867 |
| |
| # Using the brix table we can use this to produce a mapping from boiling point |
| # to density which makes all of the units interconvertible. Because the brix |
| # table stops at 95 this approach works up to a boiling point elevation of 39 K |
| # or a boiling point of 139 C / 282 F, which is the "soft crack" stage in candy |
| # making. The "hard crack" stage continues up to 310 F. |
| |
| # Boiling point elevation |
| sugar_bpe(T) units=[K;g/cm^3] domain=[0,39.1636] range=[0.99717,1.5144619] \ |
| brix(~sugar_conc_bpe(T)); sugar_conc_bpe(~brix(sugar_bpe)) |
| # Absolute boiling point (produces an absolute temperature) |
| sugar_bp(T) units=[K;g/cm^3] domain=[373.15,412.3136] \ |
| range=[0.99717,1.5144619] \ |
| brix(~sugar_conc_bpe(T-tempC(100))) ;\ |
| sugar_conc_bpe(~brix(sugar_bp))+tempC(100) |
| |
| # In practice dealing with the absolute temperature is annoying because it is |
| # not possible to convert to a nested function, so you're stuck retyping the |
| # absolute temperature in Kelvins to convert to celsius or Fahrenheit. To |
| # prevent this we supply definitions that build in the temperature conversion |
| # and produce results in the Fahrenheit and Celsius scales. So using these |
| # measures, to convert 46 degrees Baume to a Fahrenheit boiling point: |
| # |
| # You have: baume(45) |
| # You want: sugar_bpF |
| # 239.05647 |
| # |
| sugar_bpF(T) units=[1;g/cm^3] domain=[212,282.49448] range=[0.99717,1.5144619]\ |
| brix(~sugar_conc_bpe(tempF(T)+-tempC(100))) ;\ |
| ~tempF(sugar_conc_bpe(~brix(sugar_bpF))+tempC(100)) |
| sugar_bpC(T) units=[1;g/cm^3] domain=[100,139.1636] range=[0.99717,1.5144619]\ |
| brix(~sugar_conc_bpe(tempC(T)+-tempC(100))) ;\ |
| ~tempC(sugar_conc_bpe(~brix(sugar_bpC))+tempC(100)) |
| |
| # Degrees Baume is used in European recipes to specify the density of a sugar |
| # syrup. An entirely different definition is used for densities below |
| # 1 g/cm^3. An arbitrary constant appears in the definition. This value is |
| # equal to 145 in the US, but was according to [], the old scale used in |
| # Holland had a value of 144, and the new scale or Gerlach scale used 146.78. |
| |
| baumeconst 145 # US value |
| baume(d) units=[1;g/cm^3] domain=[0,145) range=[1,) \ |
| (baumeconst/(baumeconst+-d)) g/cm^3 ; \ |
| (baume+((-g)/cm^3)) baumeconst / baume |
| |
| # It's not clear if this value was ever used with negative degrees. |
| twaddell(x) units=[1;g/cm^3] domain=[-200,) range=[0,) \ |
| (1 + 0.005 x) g / cm^3 ; \ |
| 200 (twaddell / (g/cm^3) +- 1) |
| |
| # The degree quevenne is a unit for measuring the density of milk. |
| # Similarly it's unclear if negative values were allowed here. |
| quevenne(x) units=[1;g/cm^3] domain=[-1000,) range=[0,) \ |
| (1 + 0.001 x) g / cm^3 ; \ |
| 1000 (quevenne / (g/cm^3) +- 1) |
| |
| # Degrees brix measures sugar concentration by weigh as a percentage, so a |
| # solution that is 3 degrees brix is 3% sugar by weight. This unit was named |
| # after Adolf Brix who invented a hydrometer that read this percentage |
| # directly. This data is from Table 114 of NIST Circular 440, "Polarimetry, |
| # Saccharimetry and the Sugars". It gives apparent specific gravity at 20 |
| # degrees Celsius of various sugar concentrations. As rendered below this |
| # data is converted to apparent density at 20 degrees Celsius using the |
| # density figure for water given in the same NIST reference. They use the |
| # word "apparent" to refer to measurements being made in air with brass |
| # weights rather than vacuum. |
| |
| brix[0.99717g/cm^3]\ |
| 0 1.00000 1 1.00390 2 1.00780 3 1.01173 4 1.01569 5 1.01968 \ |
| 6 1.02369 7 1.02773 8 1.03180 9 1.03590 10 1.04003 11 1.04418 \ |
| 12 1.04837 13 1.05259 14 1.05683 15 1.06111 16 1.06542 17 1.06976 \ |
| 18 1.07413 19 1.07853 20 1.08297 21 1.08744 22 1.09194 23 1.09647 \ |
| 24 1.10104 25 1.10564 26 1.11027 27 1.11493 28 1.11963 29 1.12436 \ |
| 30 1.12913 31 1.13394 32 1.13877 33 1.14364 34 1.14855 35 1.15350 \ |
| 36 1.15847 37 1.16349 38 1.16853 39 1.17362 40 1.17874 41 1.18390 \ |
| 42 1.18910 43 1.19434 44 1.19961 45 1.20491 46 1.21026 47 1.21564 \ |
| 48 1.22106 49 1.22652 50 1.23202 51 1.23756 52 1.24313 53 1.24874 \ |
| 54 1.25439 55 1.26007 56 1.26580 57 1.27156 58 1.27736 59 1.28320 \ |
| 60 1.28909 61 1.29498 62 1.30093 63 1.30694 64 1.31297 65 1.31905 \ |
| 66 1.32516 67 1.33129 68 1.33748 69 1.34371 70 1.34997 71 1.35627 \ |
| 72 1.36261 73 1.36900 74 1.37541 75 1.38187 76 1.38835 77 1.39489 \ |
| 78 1.40146 79 1.40806 80 1.41471 81 1.42138 82 1.42810 83 1.43486 \ |
| 84 1.44165 85 1.44848 86 1.45535 87 1.46225 88 1.46919 89 1.47616 \ |
| 90 1.48317 91 1.49022 92 1.49730 93 1.50442 94 1.51157 95 1.51876 |
| |
| # Density measure invented by the American Petroleum Institute. Lighter |
| # petroleum products are more valuable, and they get a higher API degree. |
| # |
| # The intervals of range and domain should be open rather than closed. |
| # |
| apidegree(x) units=[1;g/cm^3] domain=[-131.5,) range=[0,) \ |
| 141.5 g/cm^3 / (x+131.5) ; \ |
| 141.5 (g/cm^3) / apidegree + (-131.5) |
| # |
| # Average densities of various woods (dried) |
| # Data from The Wood Database https://www.wood-database.com |
| # |
| |
| # North American Hardwoods |
| |
| wood_cherry 35 lb/ft^3 |
| wood_redoak 44 lb/ft^3 |
| wood_whiteoak 47 lb/ft^3 |
| wood_blackwalnut 38 lb/ft^3 |
| wood_walnut wood_blackwalnut |
| wood_birch 43 lb/ft^3 |
| wood_hardmaple 44 lb/ft^3 |
| |
| wood_bigleafmaple 34 lb/ft^3 |
| wood_boxeldermaple 30 lb/ft^3 |
| wood_redmaple 38 lb/ft^3 |
| wood_silvermaple 33 lb/ft^3 |
| wood_stripedmaple 32 lb/ft^3 |
| wood_softmaple (wood_bigleafmaple \ |
| + wood_boxeldermaple \ |
| + wood_redmaple \ |
| + wood_silvermaple \ |
| + wood_stripedmaple) / 5 |
| wood_poplar 29 lb/ft^3 |
| wood_beech 45 lb/ft^3 |
| |
| # North American Softwoods |
| |
| wood_jeffreypine 28 lb/ft^3 |
| wood_ocotepine 44 lb/ft^3 |
| wood_ponderosapine 28 lb/ft^3 |
| |
| wood_loblollypine 35 lb/ft^3 |
| wood_longleafpine 41 lb/ft^3 |
| wood_shortleafpine 35 lb/ft^3 |
| wood_slashpine 41 lb/ft^3 |
| wood_yellowpine (wood_loblollypine \ |
| + wood_longleafpine \ |
| + wood_shortleafpine \ |
| + wood_slashpine) / 4 |
| wood_redpine 34 lb/ft^3 |
| |
| wood_easternwhitepine 25 lb/ft^3 |
| wood_westernwhitepine 27 lb/ft^3 |
| wood_whitepine (wood_easternwhitepine + wood_westernwhitepine) / 2 |
| |
| wood_douglasfir 32 lb/ft^3 |
| |
| wood_blackspruce 28 lb/ft^3 |
| wood_engelmannspruce 24 lb/ft^3 |
| wood_redspruce 27 lb/ft^3 |
| wood_sitkaspruce 27 lb/ft^3 |
| wood_whitespruce 27 lb/ft^3 |
| wood_spruce (wood_blackspruce \ |
| + wood_engelmannspruce \ |
| + wood_redspruce \ |
| + wood_sitkaspruce \ |
| + wood_whitespruce) / 5 |
| |
| # Other woods |
| |
| wood_basswood 26 lb/ft^3 |
| wood_balsa 9 lb/ft^3 |
| wood_ebony_gaboon 60 lb/ft^3 |
| wood_ebony_macassar 70 lb/ft^3 |
| wood_mahogany 37 lb/ft^3 # True (Honduran) mahogany, |
| # Swietenia macrophylla |
| wood_teak 41 lb/ft^3 |
| wood_rosewood_brazilian 52 lb/ft^3 |
| wood_rosewood_honduran 64 lb/ft^3 |
| wood_rosewood_indian 52 lb/ft^3 |
| wood_cocobolo 69 lb/ft^3 |
| wood_bubinga 56 lb/ft^3 |
| wood_zebrawood 50 lb/ft^3 |
| wood_koa 38 lb/ft^3 |
| wood_snakewood 75.7 lb/ft^3 |
| wood_lignumvitae 78.5 lb/ft^3 |
| wood_blackwood 79.3 lb/ft^3 |
| wood_blackironwood 84.5 lb/ft^3 # Krugiodendron ferreum, listed |
| # in database as the heaviest wood |
| |
| # |
| # Modulus of elasticity of selected woods. |
| # Data from The Wood Database https://www.wood-database.com |
| # |
| |
| # North American Hardwoods |
| |
| wood_mod_beech 1.720e6 lbf/in^2 |
| wood_mod_birchyellow 2.010e6 lbf/in^2 |
| wood_mod_birch wood_mod_birchyellow |
| wood_mod_cherry 1.490e6 lbf/in^2 |
| wood_mod_hardmaple 1.830e6 lbf/in^2 |
| |
| wood_mod_bigleafmaple 1.450e6 lbf/in^2 |
| wood_mod_boxeldermaple 1.050e6 lbf/in^2 |
| wood_mod_redmaple 1.640e6 lbf/in^2 |
| wood_mod_silvermaple 1.140e6 lbf/in^2 |
| wood_mod_softmaple (wood_mod_bigleafmaple \ |
| + wood_mod_boxeldermaple \ |
| + wood_mod_redmaple \ |
| + wood_mod_silvermaple) / 4 |
| |
| wood_mod_redoak 1.761e6 lbf/in^2 |
| wood_mod_whiteoak 1.762e6 lbf/in^2 |
| wood_mod_poplar 1.580e6 lbf/in^2 |
| wood_mod_blackwalnut 1.680e6 lbf/in^2 |
| wood_mod_walnut wood_mod_blackwalnut |
| |
| # North American Softwoods |
| |
| wood_mod_jeffreypine 1.240e6 lbf/in^2 |
| wood_mod_ocotepine 2.209e6 lbf/in^2 |
| wood_mod_ponderosapine 1.290e6 lbf/in^2 |
| |
| wood_mod_loblollypine 1.790e6 lbf/in^2 |
| wood_mod_longleafpine 1.980e6 lbf/in^2 |
| wood_mod_shortleafpine 1.750e6 lbf/in^2 |
| wood_mod_slashpine 1.980e6 lbf/in^2 |
| wood_mod_yellowpine (wood_mod_loblollypine \ |
| + wood_mod_longleafpine \ |
| + wood_mod_shortleafpine \ |
| + wood_mod_slashpine) / 4 |
| |
| wood_mod_redpine 1.630e6 lbf/in^2 |
| |
| wood_mod_easternwhitepine 1.240e6 lbf/in^2 |
| wood_mod_westernwhitepine 1.460e6 lbf/in^2 |
| wood_mod_whitepine (wood_mod_easternwhitepine + \ |
| wood_mod_westernwhitepine) / 2 |
| |
| wood_mod_douglasfir 1.765e6 lbf/in^2 |
| |
| wood_mod_blackspruce 1.523e6 lbf/in^2 |
| wood_mod_englemannspruce 1.369e6 lbf/in^2 |
| wood_mod_redspruce 1.560e6 lbf/in^2 |
| wood_mod_sitkaspruce 1.600e6 lbf/in^2 |
| wood_mod_whitespruce 1.315e6 lbf/in^2 |
| wood_mod_spruce (wood_mod_blackspruce \ |
| + wood_mod_englemannspruce \ |
| + wood_mod_redspruce + wood_mod_sitkaspruce \ |
| + wood_mod_whitespruce) / 5 |
| |
| # Other woods |
| |
| wood_mod_balsa 0.538e6 lbf/in^2 |
| wood_mod_basswood 1.460e6 lbf/in^2 |
| wood_mod_blackwood 2.603e6 lbf/in^2 # African, Dalbergia melanoxylon |
| wood_mod_bubinga 2.670e6 lbf/in^2 |
| wood_mod_cocobolo 2.712e6 lbf/in^2 |
| wood_mod_ebony_gaboon 2.449e6 lbf/in^2 |
| wood_mod_ebony_macassar 2.515e6 lbf/in^2 |
| wood_mod_blackironwood 2.966e6 lbf/in^2 # Krugiodendron ferreum |
| wood_mod_koa 1.503e6 lbf/in^2 |
| wood_mod_lignumvitae 2.043e6 lbf/in^2 |
| wood_mod_mahogany 1.458e6 lbf/in^2 # True (Honduran) mahogany, |
| # Swietenia macrophylla |
| wood_mod_rosewood_brazilian 2.020e6 lbf/in^2 |
| wood_mod_rosewood_honduran 3.190e6 lbf/in^2 |
| wood_mod_rosewood_indian 1.668e6 lbf/in^2 |
| wood_mod_snakewood 3.364e6 lbf/in^2 |
| wood_mod_teak 1.781e6 lbf/in^2 |
| wood_mod_zebrawood 2.374e6 lbf/in^2 |
| |
| # |
| # Area of countries and other regions. This is the "total area" which |
| # includes land and water areas within international boundaries and |
| # coastlines. Data from January, 2019. |
| # |
| # except as noted, sources are |
| # https://en.wikipedia.org/wiki/List_of_countries_and_dependencies_by_area |
| # US Central Intelligence Agency: The World Factbook |
| # https://www.cia.gov/the-world-factbook/ |
| |
| area_russia 17098246 km^2 |
| area_antarctica 14000000 km^2 |
| # area_canada is covered below as sum of province and territory areas |
| area_china 9596961 km^2 |
| # area_unitedstates is covered below as sum of state areas |
| # includes only the 50 states and District of Columbia |
| area_us area_unitedstates |
| area_brazil 8515767 km^2 |
| area_australia 7692024 km^2 |
| # area_europeanunion is covered below as sum of member areas |
| area_india 3287263 km^2 |
| area_argentina 2780400 km^2 |
| area_kazakhstan 2724900 km^2 |
| area_algeria 2381741 km^2 |
| area_drcongo 2344858 km^2 |
| area_greenland 2166086 km^2 |
| area_saudiarabia 2149690 km^2 |
| area_mexico 1964375 km^2 |
| area_indonesia 1910931 km^2 |
| area_sudan 1861484 km^2 |
| area_libya 1759540 km^2 |
| area_iran 1648195 km^2 |
| area_mongolia 1564110 km^2 |
| area_peru 1285216 km^2 |
| area_chad 1284000 km^2 |
| area_niger 1267000 km^2 |
| area_angola 1246700 km^2 |
| area_mali 1240192 km^2 |
| area_southafrica 1221037 km^2 |
| area_colombia 1141748 km^2 |
| area_ethiopia 1104300 km^2 |
| area_bolivia 1098581 km^2 |
| area_mauritania 1030700 km^2 |
| area_egypt 1002450 km^2 |
| area_tanzania 945087 km^2 |
| area_nigeria 923768 km^2 |
| area_venezuela 916445 km^2 |
| area_pakistan 881912 km^2 |
| area_namibia 825615 km^2 |
| area_mozambique 801590 km^2 |
| area_turkey 783562 km^2 |
| area_chile 756102 km^2 |
| area_zambia 752612 km^2 |
| area_myanmar 676578 km^2 |
| area_burma area_myanmar |
| area_afghanistan 652230 km^2 |
| area_southsudan 644329 km^2 |
| area_france 640679 km^2 |
| area_somalia 637657 km^2 |
| area_centralafrica 622984 km^2 |
| area_ukraine 603500 km^2 |
| area_crimea 27000 km^2 # occupied by Russia; included in |
| # (Encyclopedia Britannica) |
| area_madagascar 587041 km^2 |
| area_botswana 581730 km^2 |
| area_kenya 580367 km^2 |
| area_yemen 527968 km^2 |
| area_thailand 513120 km^2 |
| area_spain 505992 km^2 |
| area_turkmenistan 488100 km^2 |
| area_cameroon 475422 km^2 |
| area_papuanewguinea 462840 km^2 |
| area_sweden 450295 km^2 |
| area_uzbekistan 447400 km^2 |
| area_morocco 446550 km^2 |
| area_iraq 438317 km^2 |
| area_paraguay 406752 km^2 |
| area_zimbabwe 390757 km^2 |
| area_japan 377973 km^2 |
| area_germany 357114 km^2 |
| area_congorepublic 342000 km^2 |
| area_finland 338424 km^2 |
| area_vietnam 331212 km^2 |
| area_malaysia 330803 km^2 |
| area_norway 323802 km^2 |
| area_ivorycoast 322463 km^2 |
| area_poland 312696 km^2 |
| area_oman 309500 km^2 |
| area_italy 301339 km^2 |
| area_philippines 300000 km^2 |
| area_ecuador 276841 km^2 |
| area_burkinafaso 274222 km^2 |
| area_newzealand 270467 km^2 |
| area_gabon 267668 km^2 |
| area_westernsahara 266000 km^2 |
| area_guinea 245857 km^2 |
| # area_unitedkingdom is covered below |
| area_uganda 241550 km^2 |
| area_ghana 238533 km^2 |
| area_romania 238397 km^2 |
| area_laos 236800 km^2 |
| area_guyana 214969 km^2 |
| area_belarus 207600 km^2 |
| area_kyrgyzstan 199951 km^2 |
| area_senegal 196722 km^2 |
| area_syria 185180 km^2 |
| area_golanheights 1150 km^2 # occupied by Israel; included in |
| # Syria (Encyclopedia Britannica) |
| area_cambodia 181035 km^2 |
| area_uruguay 176215 km^2 |
| area_somaliland 176120 km^2 |
| area_suriname 163820 km^2 |
| area_tunisia 163610 km^2 |
| area_bangladesh 147570 km^2 |
| area_nepal 147181 km^2 |
| area_tajikistan 143100 km^2 |
| area_greece 131990 km^2 |
| area_nicaragua 130373 km^2 |
| area_northkorea 120540 km^2 |
| area_malawi 118484 km^2 |
| area_eritrea 117600 km^2 |
| area_benin 114763 km^2 |
| area_honduras 112492 km^2 |
| area_liberia 111369 km^2 |
| area_bulgaria 110879 km^2 |
| area_cuba 109884 km^2 |
| area_guatemala 108889 km^2 |
| area_iceland 103000 km^2 |
| area_southkorea 100210 km^2 |
| area_hungary 93028 km^2 |
| area_portugal 92090 km^2 |
| area_jordan 89342 km^2 |
| area_serbia 88361 km^2 |
| area_azerbaijan 86600 km^2 |
| area_austria 83871 km^2 |
| area_uae 83600 km^2 |
| area_czechia 78865 km^2 |
| area_czechrepublic area_czechia |
| area_panama 75417 km^2 |
| area_sierraleone 71740 km^2 |
| area_ireland 70273 km^2 |
| area_georgia 69700 km^2 |
| area_srilanka 65610 km^2 |
| area_lithuania 65300 km^2 |
| area_latvia 64559 km^2 |
| area_togo 56785 km^2 |
| area_croatia 56594 km^2 |
| area_bosnia 51209 km^2 |
| area_costarica 51100 km^2 |
| area_slovakia 49037 km^2 |
| area_dominicanrepublic 48671 km^2 |
| area_estonia 45227 km^2 |
| area_denmark 43094 km^2 |
| area_netherlands 41850 km^2 |
| area_switzerland 41284 km^2 |
| area_bhutan 38394 km^2 |
| area_taiwan 36193 km^2 |
| area_guineabissau 36125 km^2 |
| area_moldova 33846 km^2 |
| area_belgium 30528 km^2 |
| area_lesotho 30355 km^2 |
| area_armenia 29743 km^2 |
| area_solomonislands 28896 km^2 |
| area_albania 28748 km^2 |
| area_equitorialguinea 28051 km^2 |
| area_burundi 27834 km^2 |
| area_haiti 27750 km^2 |
| area_rwanda 26338 km^2 |
| area_northmacedonia 25713 km^2 |
| area_djibouti 23200 km^2 |
| area_belize 22966 km^2 |
| area_elsalvador 21041 km^2 |
| area_israel 20770 km^2 |
| area_slovenia 20273 km^2 |
| area_fiji 18272 km^2 |
| area_kuwait 17818 km^2 |
| area_eswatini 17364 km^2 |
| area_easttimor 14919 km^2 |
| area_bahamas 13943 km^2 |
| area_montenegro 13812 km^2 |
| area_vanatu 12189 km^2 |
| area_qatar 11586 km^2 |
| area_gambia 11295 km^2 |
| area_jamaica 10991 km^2 |
| area_kosovo 10887 km^2 |
| area_lebanon 10452 km^2 |
| area_cyprus 9251 km^2 |
| area_puertorico 9104 km^2 # United States territory; not included |
| # in United States area |
| area_westbank 5860 km^2 # (CIA World Factbook) |
| area_hongkong 2755 km^2 |
| area_luxembourg 2586 km^2 |
| area_singapore 716 km^2 |
| area_gazastrip 360 km^2 # (CIA World Factbook) |
| area_malta 316 km^2 # smallest EU country |
| area_liechtenstein 160 km^2 |
| area_monaco 2.02 km^2 |
| area_vaticancity 0.44 km^2 |
| |
| # Members as of 1 Feb 2020 |
| area_europeanunion area_austria + area_belgium + area_bulgaria \ |
| + area_croatia + area_cyprus + area_czechia + area_denmark \ |
| + area_estonia + area_finland + area_france + area_germany \ |
| + area_greece + area_hungary + area_ireland + area_italy \ |
| + area_latvia + area_lithuania + area_luxembourg \ |
| + area_malta + area_netherlands + area_poland \ |
| + area_portugal + area_romania + area_slovakia \ |
| + area_slovenia + area_spain + area_sweden |
| area_eu area_europeanunion |
| |
| # |
| # Areas of the individual US states |
| # |
| # https://en.wikipedia.org/wiki/List_of_U.S._states_and_territories_by_area |
| # |
| # United States Summary: 2010, Population and Housing Unit Counts, Table 18, p. 41 |
| # Issued September 2012 |
| |
| area_alaska 1723336.8 km^2 |
| area_texas 695661.6 km^2 |
| area_california 423967.4 km^2 |
| area_montana 380831.1 km^2 |
| area_newmexico 314917.4 km^2 |
| area_arizona 295233.5 km^2 |
| area_nevada 286379.7 km^2 |
| area_colorado 269601.4 km^2 |
| area_oregon 254799.2 km^2 |
| area_wyoming 253334.5 km^2 |
| area_michigan 250486.8 km^2 |
| area_minnesota 225162.8 km^2 |
| area_utah 219881.9 km^2 |
| area_idaho 216442.6 km^2 |
| area_kansas 213100.0 km^2 |
| area_nebraska 200329.9 km^2 |
| area_southdakota 199728.7 km^2 |
| area_washington 184660.8 km^2 |
| area_northdakota 183107.8 km^2 |
| area_oklahoma 181037.2 km^2 |
| area_missouri 180540.3 km^2 |
| area_florida 170311.7 km^2 |
| area_wisconsin 169634.8 km^2 |
| area_georgia_us 153910.4 km^2 |
| area_illinois 149995.4 km^2 |
| area_iowa 145745.9 km^2 |
| area_newyork 141296.7 km^2 |
| area_northcarolina 139391.0 km^2 |
| area_arkansas 137731.8 km^2 |
| area_alabama 135767.4 km^2 |
| area_louisiana 135658.7 km^2 |
| area_mississippi 125437.7 km^2 |
| area_pennsylvania 119280.2 km^2 |
| area_ohio 116097.7 km^2 |
| area_virginia 110786.6 km^2 |
| area_tennessee 109153.1 km^2 |
| area_kentucky 104655.7 km^2 |
| area_indiana 94326.2 km^2 |
| area_maine 91633.1 km^2 |
| area_southcarolina 82932.7 km^2 |
| area_westvirginia 62755.5 km^2 |
| area_maryland 32131.2 km^2 |
| area_hawaii 28313.0 km^2 |
| area_massachusetts 27335.7 km^2 |
| area_vermont 24906.3 km^2 |
| area_newhampshire 24214.2 km^2 |
| area_newjersey 22591.4 km^2 |
| area_connecticut 14357.4 km^2 |
| area_delaware 6445.8 km^2 |
| area_rhodeisland 4001.2 km^2 |
| area_districtofcolumbia 177.0 km^2 |
| |
| area_unitedstates area_alabama + area_alaska + area_arizona \ |
| + area_arkansas + area_california + area_colorado \ |
| + area_connecticut + area_delaware \ |
| + area_districtofcolumbia + area_florida \ |
| + area_georgia_us + area_hawaii + area_idaho \ |
| + area_illinois + area_indiana + area_iowa \ |
| + area_kansas + area_kentucky + area_louisiana \ |
| + area_maine + area_maryland + area_massachusetts \ |
| + area_michigan + area_minnesota + area_mississippi \ |
| + area_missouri + area_montana + area_nebraska \ |
| + area_nevada + area_newhampshire + area_newjersey \ |
| + area_newmexico + area_newyork + area_northcarolina \ |
| + area_northdakota + area_ohio + area_oklahoma \ |
| + area_oregon + area_pennsylvania + area_rhodeisland \ |
| + area_southcarolina + area_southdakota \ |
| + area_tennessee + area_texas + area_utah \ |
| + area_vermont + area_virginia + area_washington \ |
| + area_westvirginia + area_wisconsin + area_wyoming |
| |
| # Total area of Canadian province and territories |
| # |
| # Statistics Canada, "Land and freshwater area, by province and territory", |
| # 2016-10-07: |
| # |
| # https://www150.statcan.gc.ca/n1/pub/11-402-x/2012000/chap/geo/tbl/tbl06-eng.htm |
| |
| area_ontario 1076395 km^2 # confederated 1867-Jul-01 |
| area_quebec 1542056 km^2 # confederated 1867-Jul-01 |
| area_novascotia 55284 km^2 # confederated 1867-Jul-01 |
| area_newbrunswick 72908 km^2 # confederated 1867-Jul-01 |
| area_canada_original area_ontario + area_quebec + area_novascotia \ |
| + area_newbrunswick |
| area_manitoba 647797 km^2 # confederated 1870-Jul-15 |
| area_britishcolumbia 944735 km^2 # confederated 1871-Jul-20 |
| area_princeedwardisland 5660 km^2 # confederated 1873-Jul-01 |
| area_canada_additional area_manitoba + area_britishcolumbia \ |
| + area_princeedwardisland |
| area_alberta 661848 km^2 # confederated 1905-Sep-01 |
| area_saskatchewan 651036 km^2 # confederated 1905-Sep-01 |
| area_newfoundlandandlabrador 405212 km^2 # confederated 1949-Mar-31 |
| area_canada_recent area_alberta + area_saskatchewan \ |
| + area_newfoundlandandlabrador |
| area_canada_provinces area_canada_original + area_canada_additional \ |
| + area_canada_recent |
| area_northwestterritories 1346106 km^2 # NT confederated 1870-Jul-15 |
| area_yukon 482443 km^2 # YT confederated 1898-Jun-13 |
| area_nunavut 2093190 km^2 # NU confederated 1999-Apr-01 |
| area_canada_territories area_northwestterritories + area_yukon \ |
| + area_nunavut |
| area_canada area_canada_provinces + area_canada_territories |
| |
| # area-uk-countries.units - UK country (/province) total areas |
| # https://en.wikipedia.org/wiki/Countries_of_the_United_Kingdom#Statistics |
| # GB is official UK country code for some purposes but internally is a Kingdom |
| # |
| # areas from A Beginners Guide to UK Geography 2019 v1.0, Office for National Statistics |
| # England: country; 0927-Jul-12 united; 1603-Mar-24 union of crowns |
| area_england 132947.76 km^2 |
| # |
| # Wales: 1282 conquered; 1535 union; principality until 2011 |
| area_wales 21224.48 km^2 |
| # |
| # England and Wales: nation; 1535 union |
| area_englandwales area_england + area_wales |
| # |
| # Scotland: country; ~900 united; 1603-Mar-24 union of crowns |
| area_scotland 80226.36 km^2 |
| # |
| # Great Britain: kingdom; excludes NI; |
| # 1707 Treaty and Acts of Union: union of parliaments |
| area_greatbritain area_england + area_wales + area_scotland |
| area_gb area_greatbritain |
| # |
| # Northern Ireland: province; Ireland: 1177 Henry II lordship; |
| # 1542 Henry VIII kingdom; 1652 Cromwell commonwealth; |
| # 1691 William III kingdom; 1800 Acts of Union: UK of GB & Ireland; |
| # 1921 Irish Free State independent of UK |
| area_northernireland 14133.38 km^2 |
| # |
| # United Kingdom of GB & NI: 1800 Acts of Union: UK of GB & Ireland; |
| # 1921 Irish Free State independent of UK |
| area_unitedkingdom area_greatbritain + area_northernireland |
| area_uk area_unitedkingdom |
| |
| # |
| # Units derived from imperial system |
| # |
| |
| ouncedal oz ft / s^2 # force which accelerates an ounce |
| # at 1 ft/s^2 |
| poundal lb ft / s^2 # same thing for a pound |
| tondal longton ft / s^2 # and for a ton |
| pdl poundal |
| osi ounce force / inch^2 # used in aviation |
| psi pound force / inch^2 |
| psia psi # absolute pressure |
| # Note that gauge pressure can be given |
| # using the gaugepressure() and |
| # psig() nonlinear unit definitions |
| tsi ton force / inch^2 |
| reyn psi sec |
| slug lbf s^2 / ft |
| slugf slug force |
| slinch lbf s^2 / inch # Mass unit derived from inch second |
| slinchf slinch force # pound-force system. Used in space |
| # applications where in/sec^2 was a |
| # natural acceleration measure. |
| geepound slug |
| lbf lb force |
| tonf ton force |
| lbm lb |
| kip 1000 lbf # from kilopound |
| ksi kip / in^2 |
| mil 0.001 inch |
| thou 0.001 inch |
| tenth 0.0001 inch # one tenth of one thousandth of an inch |
| millionth 1e-6 inch # one millionth of an inch |
| circularinch 1|4 pi in^2 # area of a one-inch diameter circle |
| circleinch circularinch # A circle with diameter d inches has |
| # an area of d^2 circularinches |
| cylinderinch circleinch inch # Cylinder h inch tall, d inches diameter |
| # has volume d^2 h cylinder inches |
| circularmil 1|4 pi mil^2 # area of one-mil diameter circle |
| cmil circularmil |
| cental 100 pound |
| centner cental |
| |
| # Shotgun gauge measures the inside diameter of the barrel by counting |
| # the number of spherical lead balls you can make to fit that barrel |
| # using a pound of lead. Equivalently, this means that an n gauge gun |
| # has a bore diameter that fits a ball of lead that weighs 1|n pounds |
| |
| shotgungauge(ga) units=[1;m] domain=(0,] range=(0,] \ |
| 2 ~spherevol(1 pound / ga leaddensity) ; \ |
| 1 pound / leaddensity spherevol(shotgungauge/2) |
| shotgunga() shotgungauge |
| caliber 0.01 inch # for measuring bullets |
| |
| duty ft lbf |
| celo ft / s^2 |
| jerk ft / s^3 |
| australiapoint 0.01 inch # The "point" is used to measure rainfall |
| # in Australia |
| sabin ft^2 # Measure of sound absorption equal to the |
| # absorbing power of one square foot of |
| # a perfectly absorbing material. The |
| # sound absorptivity of an object is the |
| # area times a dimensionless |
| # absorptivity coefficient. |
| standardgauge 4 ft + 8.5 in # Standard width between railroad track |
| flag 5 ft^2 # Construction term referring to sidewalk. |
| rollwallpaper 30 ft^2 # Area of roll of wall paper |
| fillpower in^3 / ounce # Density of down at standard pressure. |
| # The best down has 750-800 fillpower. |
| pinlength 1|16 inch # A #17 pin is 17/16 in long in the USA. |
| buttonline 1|40 inch # The line was used in 19th century USA |
| # to measure width of buttons. |
| beespace 1|4 inch # Bees will fill any space that is smaller |
| # than the bee space and leave open |
| # spaces that are larger. The size of |
| # the space varies with species. |
| diamond 8|5 ft # Marking on US tape measures that is |
| # useful to carpenters who wish to place |
| # five studs in an 8 ft distance. Note |
| # that the numbers appear in red every |
| # 16 inches as well, giving six |
| # divisions in 8 feet. |
| retmaunit 1.75 in # Height of rack mountable equipment. |
| U retmaunit # Equipment should be 1|32 inch narrower |
| RU U # than its U measurement indicates to |
| # allow for clearance, so 4U=(6+31|32)in |
| # RETMA stands for the former name of |
| # the standardizing organization, Radio |
| # Electronics Television Manufacturers |
| # Association. This organization is now |
| # called the Electronic Industries |
| # Alliance (EIA) and the rack standard |
| # is specified in EIA RS-310-D. |
| count per pound # For measuring the size of shrimp |
| flightlevel 100 ft # Flight levels are used to ensure safe |
| FL flightlevel # vertical separation between aircraft |
| # despite variations in local air |
| # pressure. Flight levels define |
| # altitudes based on a standard air |
| # pressure so that altimeter calibration |
| # is not needed. This means that |
| # aircraft at separated flight levels |
| # are guaranteed to be separated. |
| # Hence the definition of 100 feet is |
| # a nominal, not true, measure. |
| # Customarily written with no space in |
| # the form FL290, which will not work in |
| # units. But note "FL 290" will work. |
| |
| # |
| # Other units of work, energy, power, etc |
| # |
| |
| # Calorie: approximate energy to raise a gram of water one degree celsius |
| |
| calorie cal_th # Default is the thermochemical calorie |
| cal calorie |
| calorie_th 4.184 J # Thermochemical calorie, defined in 1930 |
| thermcalorie calorie_th # by Frederick Rossini as 4.1833 J to |
| cal_th calorie_th # avoid difficulties associated with the |
| # uncertainty in the heat capacity of |
| # water. In 1948 the value of the joule |
| # was changed, so the thermochemical |
| # calorie was redefined to 4.184 J. |
| # This kept the energy measured by this |
| # unit the same. |
| calorie_IT 4.1868 J # International (Steam) Table calorie, |
| cal_IT calorie_IT # defined in 1929 as watt-hour/860 or |
| # equivalently 180|43 joules. At this |
| # time the international joule had a |
| # different value than the modern joule, |
| # and the values were different in the |
| # USA and in Europe. In 1956 at the |
| # Fifth International Conference on |
| # Properties of Steam the exact |
| # definition given here was adopted. |
| calorie_15 4.18580 J # Energy to go from 14.5 to 15.5 degC |
| cal_15 calorie_15 |
| calorie_fifteen cal_15 |
| calorie_20 4.18190 J # Energy to go from 19.5 to 20.5 degC |
| cal_20 calorie_20 |
| calorie_twenty calorie_20 |
| calorie_4 4.204 J # Energy to go from 3.5 to 4.5 degC |
| cal_4 calorie_4 |
| calorie_four calorie_4 |
| cal_mean 4.19002 J # 1|100 energy to go from 0 to 100 degC |
| Calorie kilocalorie # the food Calorie |
| thermie 1e6 cal_15 # Heat required to raise the |
| # temperature of a tonne of |
| # water from 14.5 to 15.5 degC. |
| |
| # btu definitions: energy to raise a pound of water 1 degF |
| |
| btu btu_IT # International Table BTU is the default |
| britishthermalunit btu |
| btu_IT cal_IT lb degF / gram K |
| btu_th cal_th lb degF / gram K |
| btu_mean cal_mean lb degF / gram K |
| btu_15 cal_15 lb degF / gram K |
| btu_ISO 1055.06 J # Exact, rounded ISO definition based |
| # on the IT calorie |
| quad quadrillion btu |
| |
| ECtherm 1e5 btu_ISO # Exact definition |
| UStherm 1.054804e8 J # Exact definition |
| therm UStherm |
| |
| # Water latent heat from [23] |
| |
| water_fusion_heat 6.01 kJ/mol / (18.015 g/mol) # At 0 deg C |
| water_vaporization_heat 2256.4 J/g # At saturation, 100 deg C, 101.42 kPa |
| |
| # Specific heat capacities of various substances |
| # |
| # SPECFIC_HEAT ENERGY / MASS / TEMPERATURE_DIFFERENCE |
| # SPECFIC_HEAT_CAPACITY ENERGY / MASS / TEMPERATURE_DIFFERENCE |
| |
| specificheat_water calorie / g K |
| water_specificheat specificheat_water |
| # Values from www.engineeringtoolbox.com/specific-heat-metals-d_152.html |
| specificheat_aluminum 0.91 J/g K |
| specificheat_antimony 0.21 J/g K |
| specificheat_barium 0.20 J/g K |
| specificheat_beryllium 1.83 J/g K |
| specificheat_bismuth 0.13 J/g K |
| specificheat_cadmium 0.23 J/g K |
| specificheat_cesium 0.24 J/g K |
| specificheat_chromium 0.46 J/g K |
| specificheat_cobalt 0.42 J/g K |
| specificheat_copper 0.39 J/g K |
| specificheat_gallium 0.37 J/g K |
| specificheat_germanium 0.32 J/g K |
| specificheat_gold 0.13 J/g K |
| specificheat_hafnium 0.14 J/g K |
| specificheat_indium 0.24 J/g K |
| specificheat_iridium 0.13 J/g K |
| specificheat_iron 0.45 J/g K |
| specificheat_lanthanum 0.195 J/g K |
| specificheat_lead 0.13 J/g K |
| specificheat_lithium 3.57 J/g K |
| specificheat_lutetium 0.15 J/g K |
| specificheat_magnesium 1.05 J/g K |
| specificheat_manganese 0.48 J/g K |
| specificheat_mercury 0.14 J/g K |
| specificheat_molybdenum 0.25 J/g K |
| specificheat_nickel 0.44 J/g K |
| specificheat_osmium 0.13 J/g K |
| specificheat_palladium 0.24 J/g K |
| specificheat_platinum 0.13 J/g K |
| specificheat_plutonum 0.13 J/g K |
| specificheat_potassium 0.75 J/g K |
| specificheat_rhenium 0.14 J/g K |
| specificheat_rhodium 0.24 J/g K |
| specificheat_rubidium 0.36 J/g K |
| specificheat_ruthenium 0.24 J/g K |
| specificheat_scandium 0.57 J/g K |
| specificheat_selenium 0.32 J/g K |
| specificheat_silicon 0.71 J/g K |
| specificheat_silver 0.23 J/g K |
| specificheat_sodium 1.21 J/g K |
| specificheat_strontium 0.30 J/g K |
| specificheat_tantalum 0.14 J/g K |
| specificheat_thallium 0.13 J/g K |
| specificheat_thorium 0.13 J/g K |
| specificheat_tin 0.21 J/g K |
| specificheat_titanium 0.54 J/g K |
| specificheat_tungsten 0.13 J/g K |
| specificheat_uranium 0.12 J/g K |
| specificheat_vanadium 0.39 J/g K |
| specificheat_yttrium 0.30 J/g K |
| specificheat_zinc 0.39 J/g K |
| specificheat_zirconium 0.27 J/g K |
| specificheat_ethanol 2.3 J/g K |
| specificheat_ammonia 4.6 J/g K |
| specificheat_freon 0.91 J/g K # R-12 at 0 degrees Fahrenheit |
| specificheat_gasoline 2.22 J/g K |
| specificheat_iodine 2.15 J/g K |
| specificheat_oliveoil 1.97 J/g K |
| |
| # en.wikipedia.org/wiki/Heat_capacity#Table_of_specific_heat_capacities |
| specificheat_hydrogen 14.3 J/g K |
| specificheat_helium 5.1932 J/g K |
| specificheat_argon 0.5203 J/g K |
| specificheat_tissue 3.5 J/g K |
| specificheat_diamond 0.5091 J/g K |
| specificheat_granite 0.79 J/g K |
| specificheat_graphite 0.71 J/g K |
| specificheat_ice 2.11 J/g K |
| specificheat_asphalt 0.92 J/g K |
| specificheat_brick 0.84 J/g K |
| specificheat_concrete 0.88 J/g K |
| specificheat_glass_silica 0.84 J/g K |
| specificheat_glass_flint 0.503 J/g K |
| specificheat_glass_pyrex 0.753 J/g K |
| specificheat_gypsum 1.09 J/g K |
| specificheat_marble 0.88 J/g K |
| specificheat_sand 0.835 J/g K |
| specificheat_soil 0.835 J/g K |
| specificheat_wood 1.7 J/g K |
| |
| specificheat_sucrose 1.244 J/g K #www.sugartech.co.za/heatcapacity/index.php |
| |
| |
| # Energy densities of various fuels |
| # |
| # Most of these fuels have varying compositions or qualities and hence their |
| # actual energy densities vary. These numbers are hence only approximate. |
| # |
| # E1. http://www.aps.org/policy/reports/popa-reports/energy/units.cfm |
| # E2. https://web.archive.org/web/20100825042309/http://www.ior.com.au/ecflist.html |
| |
| tonoil 1e10 cal_IT # Ton oil equivalent. A conventional |
| # value for the energy released by |
| toe tonoil # burning one metric ton of oil. [18,E1] |
| # Note that energy per mass of petroleum |
| # products is fairly constant. |
| # Variations in volumetric energy |
| # density result from variations in the |
| # density (kg/m^3) of different fuels. |
| # This definition is given by the |
| # IEA/OECD. |
| toncoal 7e9 cal_IT # Energy in metric ton coal from [18]. |
| # This is a nominal value which |
| # is close to the heat content |
| # of coal used in the 1950's |
| barreloil 5.8 Mbtu # Conventional value for barrel of crude |
| # oil [E1]. Actual range is 5.6 - 6.3. |
| naturalgas_HHV 1027 btu/ft3 # Energy content of natural gas. HHV |
| naturalgas_LHV 930 btu/ft3 # is for Higher Heating Value and |
| naturalgas naturalgas_HHV # includes energy from condensation |
| # combustion products. LHV is for Lower |
| # Heating Value and excludes these. |
| # American publications typically report |
| # HHV whereas European ones report LHV. |
| charcoal 30 GJ/tonne |
| woodenergy_dry 20 GJ/tonne # HHV, a cord weights about a tonne |
| woodenergy_airdry 15 GJ/tonne # 20% moisture content |
| coal_bituminous 27 GJ / tonne |
| coal_lignite 15 GJ / tonne |
| coal_US 22 GJ / uston # Average for US coal (short ton), 1995 |
| ethanol_HHV 84000 btu/usgallon |
| ethanol_LHV 75700 btu/usgallon |
| diesel 130500 btu/usgallon |
| gasoline_LHV 115000 btu/usgallon |
| gasoline_HHV 125000 btu/usgallon |
| gasoline gasoline_HHV |
| heating 37.3 MJ/liter |
| fueloil 39.7 MJ/liter # low sulphur |
| propane 93.3 MJ/m^3 |
| butane 124 MJ/m^3 |
| |
| # The US EPA defines a "miles per gallon equivalent" for alternative |
| # energy vehicles: |
| |
| mpg_e miles / gallon gasoline_LHV |
| MPGe mpg_e |
| |
| # These values give total energy from uranium fission. Actual efficiency |
| # of nuclear power plants is around 30%-40%. Note also that some reactors |
| # use enriched uranium around 3% U-235. Uranium during processing or use |
| # may be in a compound of uranium oxide or uranium hexafluoride, in which |
| # case the energy density would be lower depending on how much uranium is |
| # in the compound. |
| |
| uranium_pure 200 MeV avogadro / (235.0439299 g/mol) # Pure U-235 |
| uranium_natural 0.7% uranium_pure # Natural uranium: 0.7% U-235 |
| |
| # Celsius heat unit: energy to raise a pound of water 1 degC |
| |
| celsiusheatunit cal lb degC / gram K |
| chu celsiusheatunit |
| |
| # "Apparent" average power in an AC circuit, the product of rms voltage |
| # and rms current, equal to the true power in watts when voltage and |
| # current are in phase. In a DC circuit, always equal to the true power. |
| |
| VA volt ampere |
| |
| kWh kilowatt hour |
| |
| # The horsepower is supposedly the power of one horse pulling. Obviously |
| # different people had different horses. |
| |
| horsepower 550 foot pound force / sec # Invented by James Watt |
| mechanicalhorsepower horsepower |
| hp horsepower |
| metrichorsepower 75 kilogram force meter / sec # PS=Pferdestaerke in |
| electrichorsepower 746 W # Germany |
| boilerhorsepower 9809.50 W |
| waterhorsepower 746.043 W |
| brhorsepower horsepower # Value corrected Dec, 2019. Was 745.7 W. |
| donkeypower 250 W |
| chevalvapeur metrichorsepower |
| |
| # |
| # Heat Transfer |
| # |
| # Thermal conductivity, K, measures the rate of heat transfer across |
| # a material. The heat transferred is |
| # Q = K dT A t / L |
| # where dT is the temperature difference across the material, A is the |
| # cross sectional area, t is the time, and L is the length (thickness). |
| # Thermal conductivity is a material property. |
| |
| THERMAL_CONDUCTIVITY POWER / AREA (TEMPERATURE_DIFFERENCE/LENGTH) |
| THERMAL_RESISTIVITY 1/THERMAL_CONDUCTIVITY |
| |
| # Thermal conductance is the rate at which heat flows across a given |
| # object, so the area and thickness have been fixed. It depends on |
| # the size of the object and is hence not a material property. |
| |
| THERMAL_CONDUCTANCE POWER / TEMPERATURE_DIFFERENCE |
| THERMAL_RESISTANCE 1/THERMAL_CONDUCTANCE |
| |
| # Thermal admittance is the rate of heat flow per area across an |
| # object whose thickness has been fixed. Its reciprocal, thermal |
| # insulation, is used to for measuring the heat transfer per area |
| # of sheets of insulation or cloth that are of specified thickness. |
| |
| THERMAL_ADMITTANCE THERMAL_CONDUCTIVITY / LENGTH |
| THERMAL_INSULANCE THERMAL_RESISTIVITY LENGTH |
| THERMAL_INSULATION THERMAL_RESISTIVITY LENGTH |
| |
| Rvalue degF ft^2 hr / btu |
| Uvalue 1/Rvalue |
| europeanUvalue watt / m^2 K |
| RSI degC m^2 / W |
| clo 0.155 degC m^2 / W # Supposed to be the insulance |
| # required to keep a resting person |
| # comfortable indoors. The value |
| # given is from NIST and the CRC, |
| # but [5] gives a slightly different |
| # value of 0.875 ft^2 degF hr / btu. |
| tog 0.1 degC m^2 / W # Also used for clothing. |
| |
| |
| # Thermal Conductivity of a few materials |
| |
| diamond_natural_thermal_conductivity 2200 W / m K |
| diamond_synthetic_thermal_conductivity 3320 W / m K # 99% pure C12 |
| silver_thermal_conductivity 406 W / m K |
| aluminum_thermal_conductivity 205 W / m K |
| copper_thermal_conductivity 385 W / m K |
| gold_thermal_conductivity 314 W / m K |
| iron_thermal_conductivity 79.5 W / m K |
| stainless_304_thermal_conductivity 15.5 W / m K # average value |
| |
| # The bel was defined by engineers of Bell Laboratories to describe the |
| # reduction in audio level over a length of one mile. It was originally |
| # called the transmission unit (TU) but was renamed around 1923 to honor |
| # Alexander Graham Bell. The bel proved inconveniently large so the decibel |
| # has become more common. The decibel is dimensionless since it reports a |
| # ratio, but it is used in various contexts to report a signal's power |
| # relative to some reference level. |
| |
| bel(x) units=[1;1] range=(0,) 10^(x); log(bel) # Basic bel definition |
| decibel(x) units=[1;1] range=(0,) 10^(x/10); 10 log(decibel) # Basic decibel |
| dB() decibel # Abbreviation |
| dBW(x) units=[1;W] range=(0,) dB(x) W ; ~dB(dBW/W) # Reference = 1 W |
| dBk(x) units=[1;W] range=(0,) dB(x) kW ; ~dB(dBk/kW) # Reference = 1 kW |
| dBf(x) units=[1;W] range=(0,) dB(x) fW ; ~dB(dBf/fW) # Reference = 1 fW |
| dBm(x) units=[1;W] range=(0,) dB(x) mW ; ~dB(dBm/mW) # Reference = 1 mW |
| dBmW(x) units=[1;W] range=(0,) dBm(x) ; ~dBm(dBmW) # Reference = 1 mW |
| dBJ(x) units=[1;J] range=(0,) dB(x) J; ~dB(dBJ/J) # Energy relative |
| # to 1 joule. Used for power spectral |
| # density since W/Hz = J |
| |
| |
| # When used to measure amplitude, voltage, or current the signal is squared |
| # because power is proportional to the square of these measures. The root |
| # mean square (RMS) voltage is typically used with these units. |
| |
| dB_amplitude(x) units=[1;1] dB(0.5 x) ; ~dB(dB_amplitude^2) |
| dBV(x) units=[1;V] range=(0,) dB(0.5 x) V;~dB(dBV^2 / V^2) # Reference = 1 V |
| dBmV(x) units=[1;V] range=(0,) dB(0.5 x) mV;~dB(dBmV^2/mV^2)# Reference = 1 mV |
| dBuV(x) units=[1;V] range=(0,) dB(0.5 x) microV ; ~dB(dBuV^2 / microV^2) |
| # Reference = 1 microvolt |
| |
| # Here are dB measurements for current. Be aware that dbA is also |
| # a unit for frequency weighted sound pressure. |
| dBA(x) units=[1;A] range=(0,) dB(0.5 x) A;~dB(dBA^2 / A^2) # Reference = 1 A |
| dBmA(x) units=[1;A] range=(0,) dB(0.5 x) mA;~dB(dBmA^2/mA^2)# Reference = 1 mA |
| dBuA(x) units=[1;A] range=(0,) dB(0.5 x) microA ; ~dB(dBuA^2 / microA^2) |
| # Reference = 1 microamp |
| |
| # Referenced to the voltage that causes 1 mW dissipation in a 600 ohm load. |
| # Originally defined as dBv but changed to prevent confusion with dBV. |
| # The "u" is for unloaded. |
| dBu(x) units=[1;V] range=(0,) dB(0.5 x) sqrt(mW 600 ohm) ; \ |
| ~dB(dBu^2 / mW 600 ohm) |
| dBv(x) units=[1;V] range=(0,) dBu(x) ; ~dBu(dBv) # Synonym for dBu |
| |
| # Measurements for sound in air, referenced to the threshold of human hearing |
| # Note that sound in other media typically uses 1 micropascal as a reference |
| # for sound pressure. Units dBA, dBB, dBC, refer to different frequency |
| # weightings meant to approximate the human ear's response. |
| |
| # sound pressure level |
| dBSPL(x) units=[1;Pa] range=(0,) dB(0.5 x) 20 microPa ; \ |
| ~dB(dBSPL^2 / (20 microPa)^2) |
| # sound intensity level |
| dBSIL(x) units=[1;W/m^2] range=(0,) dB(x) 1e-12 W/m^2; \ |
| ~dB(dBSIL / (1e-12 W/m^2)) |
| # sound power level (The W in SWL is for the reference power, 1 W.) |
| dBSWL(x) units=[1;W] range=(0,) dB(x) 1e-12 W; ~dB(dBSWL/1e-12 W) |
| |
| # The neper is another similar logarithmic unit. Note that the neper |
| # is defined based on the ratio of amplitudes rather than the power |
| # ratio like the decibel. This means that if the data is power, and |
| # you convert to nepers you should take the square root of the data |
| # to convert to amplitude. If you want to convert nepers to a power |
| # measurement you need to square the resulting output. |
| |
| neper(x) units=[1;1] range=(0,) exp(x); ln(neper) |
| centineper(x) units=[1;1] range=(0,) exp(x/100); 100 ln(centineper) |
| Np() neper |
| cNp() centineper |
| Np_power(x) units=[1;1] Np(2 x) ; ~Np(Np_power)/2 |
| |
| # Misc other measures |
| |
| ENTROPY ENERGY / TEMPERATURE |
| clausius 1e3 cal/K # A unit of physical entropy |
| langley thermcalorie/cm^2 # Used in radiation theory |
| poncelet 100 kg force m / s |
| tonrefrigeration uston 144 btu / lb day # One ton refrigeration is |
| # the rate of heat extraction required |
| # turn one ton of water to ice in |
| # a day. Ice is defined to have a |
| # latent heat of 144 btu/lb. |
| tonref tonrefrigeration |
| refrigeration tonref / ton |
| frigorie 1000 cal_15 # Used in refrigeration engineering. |
| airwatt 8.5 (ft^3/min) inH2O # Measure of vacuum power as |
| # pressure times air flow. |
| |
| # The unit "tnt" is defined so that you can write "tons tnt". The |
| # question of which ton, exactly, is intended. The answer is that |
| # nobody knows: |
| # |
| # Quoting the footnote from page 13 of |
| # The Effects of Nuclear Weapons, 3rd ed. |
| # https://www.fourmilab.ch/etexts/www/effects/eonw_1.pdf |
| # |
| # The majority of the experimental and theoretical values of the |
| # explosive energy released by TNT range from 900 to 1,100 calories per |
| # gram. At one time, there was some uncertainty as to whether the term |
| # "kiloton" of TNT referred to a short kiloton (2*10^6 pounds), a metric |
| # kiloton (2.205*10^6 pounds), or a long kiloton (2.24*10^6 pounds). In |
| # order to avoid ambiguity, it was agreed that the term "kiloton" would |
| # refer to the release of 10^12 calories of explosive energy. This is |
| # equivalent to 1 short kiloton of TNT if the energy release is 1,102 |
| # calories per gram or to 1 long kiloton if the energy is 984 calories |
| # per gram of TNT. |
| # |
| # It is therefore not well-defined how much energy a "gram of tnt" is, |
| # though this term does appear in some references. |
| |
| tnt 1e9 cal_th / ton # Defined exact value |
| |
| # Nuclear weapon yields |
| |
| davycrocket 10 ton tnt # lightest US tactical nuclear weapon |
| hiroshima 15.5 kiloton tnt # Uranium-235 fission bomb |
| nagasaki 21 kiloton tnt # Plutonium-239 fission bomb |
| fatman nagasaki |
| littleboy hiroshima |
| ivyking 500 kiloton tnt # most powerful fission bomb |
| castlebravo 15 megaton tnt # most powerful US test |
| tsarbomba 50 megaton tnt # most powerful test ever: USSR, |
| # 30 October 1961 |
| b53bomb 9 megaton tnt |
| # http://rarehistoricalphotos.com/gadget-first-atomic-bomb/ |
| trinity 18 kiloton tnt # July 16, 1945 |
| gadget trinity |
| |
| # |
| # Permeability: The permeability or permeance, n, of a substance determines |
| # how fast vapor flows through the substance. The formula W = n A dP |
| # holds where W is the rate of flow (in mass/time), n is the permeability, |
| # A is the area of the flow path, and dP is the vapor pressure difference. |
| # |
| |
| perm_0C grain / hr ft^2 inHg |
| perm_zero perm_0C |
| perm_0 perm_0C |
| perm perm_0C |
| perm_23C grain / hr ft^2 in Hg23C |
| perm_twentythree perm_23C |
| |
| # |
| # Counting measures |
| # |
| |
| pair 2 |
| brace 2 |
| nest 3 # often used for items like bowls that |
| # nest together |
| hattrick 3 # Used in sports, especially cricket and ice |
| # hockey to report the number of goals. |
| dicker 10 |
| dozen 12 |
| bakersdozen 13 |
| score 20 |
| flock 40 |
| timer 40 |
| shock 60 |
| toncount 100 # Used in sports in the UK |
| longhundred 120 # From a germanic counting system |
| gross 144 |
| greatgross 12 gross |
| tithe 1|10 # From Anglo-Saxon word for tenth |
| |
| # Paper counting measure |
| |
| shortquire 24 |
| quire 25 |
| shortream 480 |
| ream 500 |
| perfectream 516 |
| bundle 2 reams |
| bale 5 bundles |
| |
| # |
| # Paper measures |
| # |
| |
| # USA paper sizes |
| |
| lettersize 8.5 inch 11 inch |
| legalsize 8.5 inch 14 inch |
| ledgersize 11 inch 17 inch |
| executivesize 7.25 inch 10.5 inch |
| Apaper 8.5 inch 11 inch |
| Bpaper 11 inch 17 inch |
| Cpaper 17 inch 22 inch |
| Dpaper 22 inch 34 inch |
| Epaper 34 inch 44 inch |
| |
| # Correspondence envelope sizes. #10 is the standard business |
| # envelope in the USA. |
| |
| envelope6_25size 3.5 inch 6 inch |
| envelope6_75size 3.625 inch 6.5 inch |
| envelope7size 3.75 inch 6.75 inch |
| envelope7_75size 3.875 inch 7.5 inch |
| envelope8_625size 3.625 inch 8.625 inch |
| envelope9size 3.875 inch 8.875 inch |
| envelope10size 4.125 inch 9.5 inch |
| envelope11size 4.5 inch 10.375 inch |
| envelope12size 4.75 inch 11 inch |
| envelope14size 5 inch 11.5 inch |
| envelope16size 6 inch 12 inch |
| |
| # Announcement envelope sizes (no relation to metric paper sizes like A4) |
| |
| envelopeA1size 3.625 inch 5.125 inch # same as 4bar |
| envelopeA2size 4.375 inch 5.75 inch |
| envelopeA6size 4.75 inch 6.5 inch |
| envelopeA7size 5.25 inch 7.25 inch |
| envelopeA8size 5.5 inch 8.125 inch |
| envelopeA9size 5.75 inch 8.75 inch |
| envelopeA10size 6 inch 9.5 inch |
| |
| # Baronial envelopes |
| |
| envelope4bar 3.625 inch 5.125 inch # same as A1 |
| envelope5_5bar 4.375 inch 5.75 inch |
| envelope6bar 4.75 inch 6.5 inch |
| |
| # Coin envelopes |
| |
| envelope1baby 2.25 inch 3.5 inch # same as #1 coin |
| envelope00coin 1.6875 inch 2.75 inch |
| envelope1coin 2.25 inch 3.5 inch |
| envelope3coin 2.5 inch 4.25 inch |
| envelope4coin 3 inch 4.5 inch |
| envelope4_5coin 3 inch 4.875 inch |
| envelope5coin 2.875 inch 5.25 inch |
| envelope5_5coin 3.125 inch 5.5 inch |
| envelope6coin 3.375 inch 6 inch |
| envelope7coin 3.5 inch 6.5 inch |
| |
| # The metric paper sizes are defined so that if a sheet is cut in half |
| # along the short direction, the result is two sheets which are |
| # similar to the original sheet. This means that for any metric size, |
| # the long side is close to sqrt(2) times the length of the short |
| # side. Each series of sizes is generated by repeated cuts in half, |
| # with the values rounded down to the nearest millimeter. |
| |
| A0paper 841 mm 1189 mm # The basic size in the A series |
| A1paper 594 mm 841 mm # is defined to have an area of |
| A2paper 420 mm 594 mm # one square meter. |
| A3paper 297 mm 420 mm |
| A4paper 210 mm 297 mm |
| A5paper 148 mm 210 mm |
| A6paper 105 mm 148 mm |
| A7paper 74 mm 105 mm |
| A8paper 52 mm 74 mm |
| A9paper 37 mm 52 mm |
| A10paper 26 mm 37 mm |
| |
| B0paper 1000 mm 1414 mm # The basic B size has an area |
| B1paper 707 mm 1000 mm # of sqrt(2) square meters. |
| B2paper 500 mm 707 mm |
| B3paper 353 mm 500 mm |
| B4paper 250 mm 353 mm |
| B5paper 176 mm 250 mm |
| B6paper 125 mm 176 mm |
| B7paper 88 mm 125 mm |
| B8paper 62 mm 88 mm |
| B9paper 44 mm 62 mm |
| B10paper 31 mm 44 mm |
| |
| C0paper 917 mm 1297 mm # The basic C size has an area |
| C1paper 648 mm 917 mm # of sqrt(sqrt(2)) square meters. |
| C2paper 458 mm 648 mm |
| C3paper 324 mm 458 mm # Intended for envelope sizes |
| C4paper 229 mm 324 mm |
| C5paper 162 mm 229 mm |
| C6paper 114 mm 162 mm |
| C7paper 81 mm 114 mm |
| C8paper 57 mm 81 mm |
| C9paper 40 mm 57 mm |
| C10paper 28 mm 40 mm |
| |
| # gsm (Grams per Square Meter), a sane, metric paper weight measure |
| |
| gsm grams / meter^2 |
| |
| # In the USA, a collection of crazy historical paper measures are used. Paper |
| # is measured as a weight of a ream of that particular type of paper. This is |
| # sometimes called the "substance" or "basis" (as in "substance 20" paper). |
| # The standard sheet size or "basis size" varies depending on the type of |
| # paper. As a result, 20 pound bond paper and 50 pound text paper are actually |
| # about the same weight. The different sheet sizes were historically the most |
| # convenient for printing or folding in the different applications. These |
| # different basis weights are standards maintained by American Society for |
| # Testing Materials (ASTM) and the American Forest and Paper Association |
| # (AF&PA). |
| |
| poundbookpaper lb / 25 inch 38 inch ream |
| lbbook poundbookpaper |
| poundtextpaper poundbookpaper |
| lbtext poundtextpaper |
| poundoffsetpaper poundbookpaper # For offset printing |
| lboffset poundoffsetpaper |
| poundbiblepaper poundbookpaper # Designed to be lightweight, thin, |
| lbbible poundbiblepaper # strong and opaque. |
| poundtagpaper lb / 24 inch 36 inch ream |
| lbtag poundtagpaper |
| poundbagpaper poundtagpaper |
| lbbag poundbagpaper |
| poundnewsprintpaper poundtagpaper |
| lbnewsprint poundnewsprintpaper |
| poundposterpaper poundtagpaper |
| lbposter poundposterpaper |
| poundtissuepaper poundtagpaper |
| lbtissue poundtissuepaper |
| poundwrappingpaper poundtagpaper |
| lbwrapping poundwrappingpaper |
| poundwaxingpaper poundtagpaper |
| lbwaxing poundwaxingpaper |
| poundglassinepaper poundtagpaper |
| lbglassine poundglassinepaper |
| poundcoverpaper lb / 20 inch 26 inch ream |
| lbcover poundcoverpaper |
| poundindexpaper lb / 25.5 inch 30.5 inch ream |
| lbindex poundindexpaper |
| poundindexbristolpaper poundindexpaper |
| lbindexbristol poundindexpaper |
| poundbondpaper lb / 17 inch 22 inch ream # Bond paper is stiff and |
| lbbond poundbondpaper # durable for repeated |
| poundwritingpaper poundbondpaper # filing, and it resists |
| lbwriting poundwritingpaper # ink penetration. |
| poundledgerpaper poundbondpaper |
| lbledger poundledgerpaper |
| poundcopypaper poundbondpaper |
| lbcopy poundcopypaper |
| poundblottingpaper lb / 19 inch 24 inch ream |
| lbblotting poundblottingpaper |
| poundblankspaper lb / 22 inch 28 inch ream |
| lbblanks poundblankspaper |
| poundpostcardpaper lb / 22.5 inch 28.5 inch ream |
| lbpostcard poundpostcardpaper |
| poundweddingbristol poundpostcardpaper |
| lbweddingbristol poundweddingbristol |
| poundbristolpaper poundweddingbristol |
| lbbristol poundbristolpaper |
| poundboxboard lb / 1000 ft^2 |
| lbboxboard poundboxboard |
| poundpaperboard poundboxboard |
| lbpaperboard poundpaperboard |
| |
| # When paper is marked in units of M, it means the weight of 1000 sheets of the |
| # given size of paper. To convert this to paper weight, divide by the size of |
| # the paper in question. |
| |
| paperM lb / 1000 |
| |
| # In addition paper weight is reported in "caliper" which is simply the |
| # thickness of one sheet, typically in inches. Thickness is also reported in |
| # "points" where a point is 1|1000 inch. These conversions are supplied to |
| # convert these units roughly (using an approximate density) into the standard |
| # paper weight values. |
| |
| pointthickness 0.001 in |
| paperdensity 0.8 g/cm^3 # approximate--paper densities vary! |
| papercaliper in paperdensity |
| paperpoint pointthickness paperdensity |
| |
| # |
| # Printing |
| # |
| |
| fournierpoint 0.1648 inch / 12 # First definition of the printers |
| # point made by Pierre Fournier who |
| # defined it in 1737 as 1|12 of a |
| # cicero which was 0.1648 inches. |
| olddidotpoint 1|72 frenchinch # Francois Ambroise Didot, one of |
| # a family of printers, changed |
| # Fournier's definition around 1770 |
| # to fit to the French units then in |
| # use. |
| bertholdpoint 1|2660 m # H. Berthold tried to create a |
| # metric version of the didot point |
| # in 1878. |
| INpoint 0.4 mm # This point was created by a |
| # group directed by Fermin Didot in |
| # 1881 and is associated with the |
| # imprimerie nationale. It doesn't |
| # seem to have been used much. |
| germandidotpoint 0.376065 mm # Exact definition appears in DIN |
| # 16507, a German standards document |
| # of 1954. Adopted more broadly in |
| # 1966 by ??? |
| metricpoint 3|8 mm # Proposed in 1977 by Eurograf |
| oldpoint 1|72.27 inch # The American point was invented |
| printerspoint oldpoint # by Nelson Hawks in 1879 and |
| texpoint oldpoint # dominates USA publishing. |
| # It was standardized by the American |
| # Typefounders Association at the |
| # value of 0.013837 inches exactly. |
| # Knuth uses the approximation given |
| # here (which is very close). The |
| # comp.fonts FAQ claims that this |
| # value is supposed to be 1|12 of a |
| # pica where 83 picas is equal to 35 |
| # cm. But this value differs from |
| # the standard. |
| texscaledpoint 1|65536 texpoint # The TeX typesetting system uses |
| texsp texscaledpoint # this for all computations. |
| computerpoint 1|72 inch # The American point was rounded |
| point computerpoint |
| computerpica 12 computerpoint # to an even 1|72 inch by computer |
| postscriptpoint computerpoint # people at some point. |
| pspoint postscriptpoint |
| twip 1|20 point # TWentieth of an Imperial Point |
| Q 1|4 mm # Used in Japanese phototypesetting |
| # Q is for quarter |
| frenchprinterspoint olddidotpoint |
| didotpoint germandidotpoint # This seems to be the dominant value |
| europeanpoint didotpoint # for the point used in Europe |
| cicero 12 didotpoint |
| |
| stick 2 inches |
| |
| # Type sizes |
| |
| excelsior 3 oldpoint |
| brilliant 3.5 oldpoint |
| diamondtype 4 oldpoint |
| pearl 5 oldpoint |
| agate 5.5 oldpoint # Originally agate type was 14 lines per |
| # inch, giving a value of 1|14 in. |
| ruby agate # British |
| nonpareil 6 oldpoint |
| mignonette 6.5 oldpoint |
| emerald mignonette # British |
| minion 7 oldpoint |
| brevier 8 oldpoint |
| bourgeois 9 oldpoint |
| longprimer 10 oldpoint |
| smallpica 11 oldpoint |
| pica 12 oldpoint |
| english 14 oldpoint |
| columbian 16 oldpoint |
| greatprimer 18 oldpoint |
| paragon 20 oldpoint |
| meridian 44 oldpoint |
| canon 48 oldpoint |
| |
| # German type sizes |
| |
| nonplusultra 2 didotpoint |
| brillant 3 didotpoint |
| diamant 4 didotpoint |
| perl 5 didotpoint |
| nonpareille 6 didotpoint |
| kolonel 7 didotpoint |
| petit 8 didotpoint |
| borgis 9 didotpoint |
| korpus 10 didotpoint |
| corpus korpus |
| garamond korpus |
| mittel 14 didotpoint |
| tertia 16 didotpoint |
| text 18 didotpoint |
| kleine_kanon 32 didotpoint |
| kanon 36 didotpoint |
| grobe_kanon 42 didotpoint |
| missal 48 didotpoint |
| kleine_sabon 72 didotpoint |
| grobe_sabon 84 didotpoint |
| |
| # |
| # Information theory units. Note that the name "entropy" is used both |
| # to measure information and as a physical quantity. |
| # |
| |
| INFORMATION bit |
| |
| nat (1/ln(2)) bits # Entropy measured base e |
| hartley log2(10) bits # Entropy of a uniformly |
| ban hartley # distributed random variable |
| # over 10 symbols. |
| dit hartley # from Decimal digIT |
| |
| # |
| # Computer |
| # |
| |
| bps bit/sec # Sometimes the term "baud" is |
| # incorrectly used to refer to |
| # bits per second. Baud refers |
| # to symbols per second. Modern |
| # modems transmit several bits |
| # per symbol. |
| byte 8 bit # Not all machines had 8 bit |
| B byte # bytes, but these days most of |
| # them do. But beware: for |
| # transmission over modems, a |
| # few extra bits are used so |
| # there are actually 10 bits per |
| # byte. |
| octet 8 bits # The octet is always 8 bits |
| nybble 4 bits # Half of a byte. Sometimes |
| # equal to different lengths |
| # such as 3 bits. |
| nibble nybble |
| nyp 2 bits # Donald Knuth asks in an exercise |
| # for a name for a 2 bit |
| # quantity and gives the "nyp" |
| # as a solution due to Gregor |
| # Purdy. Not in common use. |
| meg megabyte # Some people consider these |
| # units along with the kilobyte |
| gig gigabyte # to be defined according to |
| # powers of 2 with the kilobyte |
| # equal to 2^10 bytes, the |
| # megabyte equal to 2^20 bytes and |
| # the gigabyte equal to 2^30 bytes |
| # but these usages are forbidden |
| # by SI. Binary prefixes have |
| # been defined by IEC to replace |
| # the SI prefixes. Use them to |
| # get the binary units KiB, MiB, |
| # GiB, etc. |
| jiffy 0.01 sec # This is defined in the Jargon File |
| jiffies jiffy # (http://www.jargon.org) as being the |
| # duration of a clock tick for measuring |
| # wall-clock time. Supposedly the value |
| # used to be 1|60 sec or 1|50 sec |
| # depending on the frequency of AC power, |
| # but then 1|100 sec became more common. |
| # On linux systems, this term is used and |
| # for the Intel based chips, it does have |
| # the value of .01 sec. The Jargon File |
| # also lists two other definitions: |
| # millisecond, and the time taken for |
| # light to travel one foot. |
| cdaudiospeed 44.1 kHz 2*16 bits # CD audio data rate at 44.1 kHz with 2 |
| # samples of sixteen bits each. |
| cdromspeed 75 2048 bytes / sec # For data CDs (mode1) 75 sectors are read |
| # each second with 2048 bytes per sector. |
| # Audio CDs do not have sectors, but |
| # people sometimes divide the bit rate by |
| # 75 and claim a sector length of 2352. |
| # Data CDs have a lower rate due to |
| # increased error correction overhead. |
| # There is a rarely used mode (mode2) with |
| # 2336 bytes per sector that has fewer |
| # error correction bits than mode1. |
| dvdspeed 1385 kB/s # This is the "1x" speed of a DVD using |
| # constant linear velocity (CLV) mode. |
| # Modern DVDs may vary the linear velocity |
| # as they go from the inside to the |
| # outside of the disc. |
| # See http://www.osta.org/technology/dvdqa/dvdqa4.htm |
| |
| FIT / 1e9 hour # Failures In Time, number of failures per billion hours |
| |
| # |
| # The IP address space is divided into subnets. The number of hosts |
| # in a subnet depends on the length of the subnet prefix. This is |
| # often written as /N where N is the number of bits in the prefix. |
| # |
| # https://en.wikipedia.org/wiki/Subnetwork |
| # |
| # These definitions gives the number of hosts for a subnet whose |
| # prefix has the specified length in bits. |
| # |
| |
| ipv4subnetsize(prefix_len) units=[1;1] domain=[0,32] range=[1,4294967296] \ |
| 2^(32-prefix_len) ; 32-log2(ipv4subnetsize) |
| ipv4classA ipv4subnetsize(8) |
| ipv4classB ipv4subnetsize(16) |
| ipv4classC ipv4subnetsize(24) |
| |
| ipv6subnetsize(prefix_len) units=[1;1] domain=[0,128] \ |
| range=[1,340282366920938463463374607431768211456] \ |
| 2^(128-prefix_len) ; 128-log2(ipv6subnetsize) |
| |
| # |
| # Musical measures. Musical intervals expressed as ratios. Multiply |
| # two intervals together to get the sum of the interval. The function |
| # musicalcent can be used to convert ratios to cents. |
| # |
| |
| # Perfect intervals |
| |
| octave 2 |
| majorsecond musicalfifth^2 / octave |
| majorthird 5|4 |
| minorthird 6|5 |
| musicalfourth 4|3 |
| musicalfifth 3|2 |
| majorsixth musicalfourth majorthird |
| minorsixth musicalfourth minorthird |
| majorseventh musicalfifth majorthird |
| minorseventh musicalfifth minorthird |
| |
| pythagoreanthird majorsecond musicalfifth^2 / octave |
| syntoniccomma pythagoreanthird / majorthird |
| pythagoreancomma musicalfifth^12 / octave^7 |
| |
| # Equal tempered definitions |
| |
| semitone octave^(1|12) |
| musicalcent(x) units=[1;1] range=(0,) semitone^(x/100) ; \ |
| 100 log(musicalcent)/log(semitone) |
| |
| # |
| # Musical note lengths. |
| # |
| |
| wholenote ! |
| MUSICAL_NOTE_LENGTH wholenote |
| halfnote 1|2 wholenote |
| quarternote 1|4 wholenote |
| eighthnote 1|8 wholenote |
| sixteenthnote 1|16 wholenote |
| thirtysecondnote 1|32 wholenote |
| sixtyfourthnote 1|64 wholenote |
| dotted 3|2 |
| doubledotted 7|4 |
| breve doublewholenote |
| semibreve wholenote |
| minimnote halfnote |
| crotchet quarternote |
| quaver eighthnote |
| semiquaver sixteenthnote |
| demisemiquaver thirtysecondnote |
| hemidemisemiquaver sixtyfourthnote |
| semidemisemiquaver hemidemisemiquaver |
| |
| # |
| # yarn and cloth measures |
| # |
| |
| # yarn linear density |
| |
| woolyarnrun 1600 yard/pound # 1600 yds of "number 1 yarn" weighs |
| # a pound. |
| yarncut 300 yard/pound # Less common system used in |
| # Pennsylvania for wool yarn |
| cottonyarncount 840 yard/pound |
| linenyarncount 300 yard/pound # Also used for hemp and ramie |
| worstedyarncount 1680 ft/pound |
| metricyarncount meter/gram |
| denier 1|9 tex # used for silk and rayon |
| manchesteryarnnumber drams/1000 yards # old system used for silk |
| pli lb/in |
| typp 1000 yd/lb # abbreviation for Thousand Yard Per Pound |
| asbestoscut 100 yd/lb # used for glass and asbestos yarn |
| |
| tex gram / km # rational metric yarn measure, meant |
| drex 0.1 tex # to be used for any kind of yarn |
| poumar lb / 1e6 yard |
| |
| # yarn and cloth length |
| |
| skeincotton 80*54 inch # 80 turns of thread on a reel with a |
| # 54 in circumference (varies for other |
| # kinds of thread) |
| cottonbolt 120 ft # cloth measurement |
| woolbolt 210 ft |
| bolt cottonbolt |
| heer 600 yards |
| cut 300 yards # used for wet-spun linen yarn |
| lea 300 yards |
| |
| sailmakersyard 28.5 in |
| sailmakersounce oz / sailmakersyard 36 inch |
| |
| silkmomme momme / 25 yards 1.49 inch # Traditional silk weight |
| silkmm silkmomme # But it is also defined as |
| # lb/100 yd 45 inch. The two |
| # definitions are slightly different |
| # and neither one seems likely to be |
| # the true source definition. |
| |
| # |
| # drug dosage |
| # |
| |
| mcg microgram # Frequently used for vitamins |
| iudiptheria 62.8 microgram # IU is for international unit |
| iupenicillin 0.6 microgram |
| iuinsulin 41.67 microgram |
| drop 1|20 ml # The drop was an old "unit" that was |
| # replaced by the minim. But I was |
| # told by a pharmacist that in his |
| # profession, the conversion of 20 |
| # drops per ml is actually used. |
| bloodunit 450 ml # For whole blood. For blood |
| # components, a blood unit is the |
| # quantity of the component found in a |
| # blood unit of whole blood. The |
| # human body contains about 12 blood |
| # units of whole blood. |
| |
| # |
| # misc medical measure |
| # |
| |
| frenchcathetersize 1|3 mm # measure used for the outer diameter |
| # of a catheter |
| charriere frenchcathetersize |
| |
| |
| # |
| # fixup units for times when prefix handling doesn't do the job |
| # |
| |
| hectare hectoare |
| megohm megaohm |
| kilohm kiloohm |
| microhm microohm |
| megalerg megaerg # 'L' added to make it pronounceable [18]. |
| |
| # |
| # Money |
| # |
| # Note that US$ is the primitive unit so other currencies are |
| # generally given in US$. |
| # |
| |
| unitedstatesdollar US$ |
| usdollar US$ |
| $ dollar |
| mark germanymark |
| #bolivar venezuelabolivar # Not all databases are |
| #venezuelabolivarfuerte 1e-5 bolivar # supplying these |
| #bolivarfuerte 1e-5 bolivar # The currency was revalued |
| #oldbolivar 1|1000 bolivarfuerte # twice |
| peseta spainpeseta |
| rand southafricarand |
| escudo portugalescudo |
| guilder netherlandsguilder |
| hollandguilder netherlandsguilder |
| peso mexicopeso |
| yen japanyen |
| lira turkeylira |
| rupee indiarupee |
| drachma greecedrachma |
| franc francefranc |
| markka finlandmarkka |
| britainpound unitedkingdompound |
| greatbritainpound unitedkingdompound |
| unitedkingdompound ukpound |
| poundsterling britainpound |
| yuan chinayuan |
| |
| # Unicode Currency Names |
| |
| !utf8 |
| icelandkróna icelandkrona |
| polandzłoty polandzloty |
| tongapa’anga tongapa'anga |
| #venezuelabolívar venezuelabolivar |
| vietnamđồng vietnamdong |
| mongoliatögrög mongoliatugrik |
| sãotomé&príncipedobra saotome&principedobra |
| !endutf8 |
| |
| UKP GBP # Not an ISO code, but looks like one, and |
| # sometimes used on usenet. |
| |
| !include currency.units |
| |
| # Money on the gold standard, used in the late 19th century and early |
| # 20th century. |
| |
| olddollargold 23.22 grains goldprice # Used until 1934 |
| newdollargold 96|7 grains goldprice # After Jan 31, 1934 |
| dollargold newdollargold |
| poundgold 113 grains goldprice # British pound |
| |
| # Precious metals |
| |
| goldounce goldprice troyounce |
| silverounce silverprice troyounce |
| platinumounce platinumprice troyounce |
| XAU goldounce |
| XPT platinumounce |
| XAG silverounce |
| |
| # Nominal masses of US coins. Note that dimes, quarters and half dollars |
| # have weight proportional to value. Before 1965 it was $40 / kg. |
| |
| USpennyweight 2.5 grams # Since 1982, 48 grains before |
| USnickelweight 5 grams |
| USdimeweight US$ 0.10 / (20 US$ / lb) # Since 1965 |
| USquarterweight US$ 0.25 / (20 US$ / lb) # Since 1965 |
| UShalfdollarweight US$ 0.50 / (20 US$ / lb) # Since 1971 |
| USdollarweight 8.1 grams # Weight of Susan B. Anthony and |
| # Sacagawea dollar coins |
| |
| # British currency |
| |
| quid britainpound # Slang names |
| fiver 5 quid |
| tenner 10 quid |
| monkey 500 quid |
| brgrand 1000 quid |
| bob shilling |
| |
| shilling 1|20 britainpound # Before decimalisation, there |
| oldpence 1|12 shilling # were 20 shillings to a pound, |
| farthing 1|4 oldpence # each of twelve old pence |
| guinea 21 shilling # Still used in horse racing |
| crown 5 shilling |
| florin 2 shilling |
| groat 4 oldpence |
| tanner 6 oldpence |
| brpenny 0.01 britainpound |
| pence brpenny |
| tuppence 2 pence |
| tuppenny tuppence |
| ha'penny halfbrpenny |
| hapenny ha'penny |
| oldpenny oldpence |
| oldtuppence 2 oldpence |
| oldtuppenny oldtuppence |
| threepence 3 oldpence # threepence never refers to new money |
| threepenny threepence |
| oldthreepence threepence |
| oldthreepenny threepence |
| oldhalfpenny halfoldpenny |
| oldha'penny oldhalfpenny |
| oldhapenny oldha'penny |
| brpony 25 britainpound |
| |
| # Canadian currency |
| |
| loony 1 canadadollar # This coin depicts a loon |
| toony 2 canadadollar |
| |
| # Cryptocurrency |
| |
| satoshi 1e-8 bitcoin |
| XBT bitcoin # nonstandard code |
| |
| # Inflation. |
| # |
| # Currently US inflation as reported by the BLS CPI index is available. |
| # The UScpi() table reports the USA consumer price index. Note that |
| # if you specify a year like 2015, that refers to the CPI reported |
| # for December of 2014 (which is released in mid January 2015), |
| # so it refers to the point right at the start of the given year. |
| # Months are increments of 1|12 on the year, so the January 2015 |
| # release will be 2015+1|12 = 2015.08333. |
| |
| !include cpi.units |
| |
| USCPI() UScpi |
| USCPI_now UScpi_now |
| USCPI_lastdate UScpi_lastdate |
| cpi() UScpi |
| CPI() UScpi |
| cpi_now UScpi_now |
| CPI_now UScpi_now |
| cpi_lastdate UScpi_lastdate |
| CPI_lastdate UScpi_lastdate |
| |
| # These definitions hide the CPI index and directly convert US dollars |
| # from a specified date to current dollars. You can use this to convert |
| # historical dollars to present value or to convert money in the past |
| # between two dates. |
| |
| dollars_in() USdollars_in |
| US$in() USdollars_in |
| $in() USdollars_in |
| |
| # This definition gives the dimensionless US inflation factor since the |
| # specified date. |
| |
| inflation_since() USinflation_since |
| |
| |
| # |
| # Units used for measuring volume of wood |
| # |
| |
| cord 4*4*8 ft^3 # 4 ft by 4 ft by 8 ft bundle of wood |
| facecord 1|2 cord |
| cordfoot 1|8 cord # One foot long section of a cord |
| cordfeet cordfoot |
| housecord 1|3 cord # Used to sell firewood for residences, |
| # often confusingly called a "cord" |
| boardfoot ft^2 inch # Usually 1 inch thick wood |
| boardfeet boardfoot |
| fbm boardfoot # feet board measure |
| stack 4 yard^3 # British, used for firewood and coal [18] |
| rick 4 ft 8 ft 16 inches # Stack of firewood, supposedly |
| # sometimes called a face cord, but this |
| # value is equal to 1|3 cord. Name |
| # comes from an old Norse word for a |
| # stack of wood. |
| stere m^3 |
| timberfoot ft^3 # Used for measuring solid blocks of wood |
| standard 120 12 ft 11 in 1.5 in # This is the St Petersburg or |
| # Pittsburg standard. Apparently the |
| # term is short for "standard hundred" |
| # which was meant to refer to 100 pieces |
| # of wood (deals). However, this |
| # particular standard is equal to 120 |
| # deals which are 12 ft by 11 in by 1.5 |
| # inches (not the standard deal). |
| hoppusfoot (4/pi) ft^3 # Volume calculation suggested in 1736 |
| hoppusboardfoot 1|12 hoppusfoot # forestry manual by Edward Hoppus, for |
| hoppuston 50 hoppusfoot # estimating the usable volume of a log. |
| # It results from computing the volume |
| # of a cylindrical log of length, L, and |
| # girth (circumference), G, by V=L(G/4)^2. |
| # The hoppus ton is apparently still in |
| # use for shipments from Southeast Asia. |
| |
| # In Britain, the deal is apparently any piece of wood over 6 feet long, over |
| # 7 wide and 2.5 inches thick. The OED doesn't give a standard size. A piece |
| # of wood less than 7 inches wide is called a "batten". This unit is now used |
| # exclusively for fir and pine. |
| |
| deal 12 ft 11 in 2.5 in # The standard North American deal [OED] |
| wholedeal 12 ft 11 in 1.25 in # If it's half as thick as the standard |
| # deal it's called a "whole deal"! |
| splitdeal 12 ft 11 in 5|8 in # And half again as thick is a split deal. |
| |
| |
| # Used for shellac mixing rate |
| |
| poundcut pound / gallon |
| lbcut poundcut |
| |
| # |
| # Gas and Liquid flow units |
| # |
| |
| FLUID_FLOW VOLUME / TIME |
| |
| # Some obvious volumetric gas flow units (cu is short for cubic) |
| |
| cumec m^3/s |
| cusec ft^3/s |
| |
| # Conventional abbreviations for fluid flow units |
| |
| gph gal/hr |
| gpm gal/min |
| mgd megagal/day |
| brgph brgallon/hr |
| brgpm brgallon/min |
| brmgd mega brgallon/day |
| usgph usgallon/hr |
| usgpm usgallon/min |
| usmgd mega usgallon/day |
| cfs ft^3/s |
| cfh ft^3/hour |
| cfm ft^3/min |
| lpm liter/min |
| lfm ft/min # Used to report air flow produced by fans. |
| # Multiply by cross sectional area to get a |
| # flow in cfm. |
| |
| pru mmHg / (ml/min) # peripheral resistance unit, used in |
| # medicine to assess blood flow in |
| # the capillaries. |
| |
| # Miner's inch: This is an old historic unit used in the Western United |
| # States. It is generally defined as the rate of flow through a one square |
| # inch hole at a specified depth such as 4 inches. In the late 19th century, |
| # volume of water was sometimes measured in the "24 hour inch". Values for the |
| # miner's inch were fixed by state statues. (This information is from a web |
| # site operated by the Nevada Division of Water Planning: The Water Words |
| # Dictionary at http://water.nv.gov/WaterPlanDictionary.aspx, specifically |
| # http://water.nv.gov/programs/planning/dictionary/wwords-M.pdf. All |
| # but minersinchNV are s.v. Miner's Inch [Western United States]) |
| |
| minersinchAZ 1.5 ft^3/min |
| minersinchCA 1.5 ft^3/min |
| minersinchMT 1.5 ft^3/min |
| minersinchNV 1.5 ft^3/min |
| minersinchOR 1.5 ft^3/min |
| minersinchID 1.2 ft^3/min |
| minersinchKS 1.2 ft^3/min |
| minersinchNE 1.2 ft^3/min |
| minersinchNM 1.2 ft^3/min |
| minersinchND 1.2 ft^3/min |
| minersinchSD 1.2 ft^3/min |
| minersinchUT 1.2 ft^3/min |
| minersinchCO 1 ft^3/sec / 38.4 # 38.4 miner's inches = 1 ft^3/sec |
| minersinchBC 1.68 ft^3/min # British Columbia |
| |
| # Oceanographic flow |
| |
| sverdrup 1e6 m^3 / sec # Used to express flow of ocean |
| # currents. Named after Norwegian |
| # oceanographer H. Sverdrup. |
| |
| # In vacuum science and some other applications, gas flow is measured |
| # as the product of volumetric flow and pressure. This is useful |
| # because it makes it easy to compare with the flow at standard |
| # pressure (one atmosphere). It also directly relates to the number |
| # of gas molecules per unit time, and hence to the mass flow if the |
| # molecular mass is known. |
| |
| GAS_FLOW PRESSURE FLUID_FLOW |
| |
| sccm atm cc/min # 's' is for "standard" to indicate |
| sccs atm cc/sec # flow at standard pressure |
| scfh atm ft^3/hour # |
| scfm atm ft^3/min |
| slpm atm liter/min |
| slph atm liter/hour |
| lusec liter micron Hg / s # Used in vacuum science |
| |
| # US Standard Atmosphere (1976) |
| # Atmospheric temperature and pressure vs. geometric height above sea level |
| # This definition covers only the troposphere (the lowest atmospheric |
| # layer, up to 11 km), and assumes the layer is polytropic. |
| # A polytropic process is one for which PV^k = const, where P is the |
| # pressure, V is the volume, and k is the polytropic exponent. The |
| # polytropic index is n = 1 / (k - 1). As noted in the Wikipedia article |
| # https://en.wikipedia.org/wiki/Polytropic_process, some authors reverse |
| # the definitions of "exponent" and "index." The functions below assume |
| # the following parameters: |
| |
| # temperature lapse rate, -dT/dz, in troposphere |
| |
| lapserate 6.5 K/km # US Std Atm (1976) |
| |
| # air molecular weight, including constituent mol wt, given |
| # in Table 3, p. 3; CH4 (16.04303) and N2O (44.0128) from |
| # Table 15, p. 33. Values for molecular weights are slightly |
| # different from current values, so the original numerical |
| # values are retained. |
| |
| air_1976 78.084 % 28.0134 \ |
| + 20.9476 % 31.9988 \ |
| + 9340 ppm 39.948 \ |
| + 314 ppm 44.00995 \ |
| + 18.18 ppm 20.183 \ |
| + 5.24 ppm 4.0026 \ |
| + 1.5 ppm 16.04303 \ |
| + 1.14 ppm 83.80 \ |
| + 0.5 ppm 2.01594 \ |
| + 0.27 ppm 44.0128 \ |
| + 0.087 ppm 131.30 |
| |
| # from US Standard Atmosphere, 1962, Table I.2.7, p. 9 |
| |
| air_1962 78.084 % 28.0134 \ |
| + 20.9476 % 31.9988 \ |
| + 9340 ppm 39.948 \ |
| + 314 ppm 44.00995 \ |
| + 18.18 ppm 20.183 \ |
| + 5.24 ppm 4.0026 \ |
| + 2 ppm 16.04303 \ |
| + 1.14 ppm 83.80 \ |
| + 0.5 ppm 2.01594 \ |
| + 0.5 ppm 44.0128 \ |
| + 0.087 ppm 131.30 |
| |
| # Average molecular weight of air |
| # |
| # Concentration of greenhouse gases CO2, CH4, and N20 are from |
| # https://gml.noaa.gov/ccgg/trends/global.html (accessed 2023-04-10); |
| # others are from NASA Earth Fact Sheet |
| # https://nssdc.gsfc.nasa.gov/planetary/factsheet/earthfact.html (accessed 2023-04-10) |
| # Numbers do not add up to exactly 100% due to roundoff and uncertainty. Water |
| # is highly variable, typically makes up about 1% |
| |
| air_2023 78.08% nitrogen 2 \ |
| + 20.95% oxygen 2 \ |
| + 9340 ppm argon \ |
| + 419 ppm (carbon + oxygen 2) \ |
| + 18.18 ppm neon \ |
| + 5.24 ppm helium \ |
| + 1.92 ppm (carbon + 4 hydrogen) \ |
| + 1.14 ppm krypton \ |
| + 0.55 ppm hydrogen 2 \ |
| + 0.34 ppm (nitrogen 2 + oxygen) |
| |
| # from NASA Earth Fact Sheet (accessed 28 August 2015) |
| # http://nssdc.gsfc.nasa.gov/planetary/factsheet/earthfact.html |
| |
| air_2015 78.08% nitrogen 2 \ |
| + 20.95% oxygen 2 \ |
| + 9340 ppm argon \ |
| + 400 ppm (carbon + oxygen 2) \ |
| + 18.18 ppm neon \ |
| + 5.24 ppm helium \ |
| + 1.7 ppm (carbon + 4 hydrogen) \ |
| + 1.14 ppm krypton \ |
| + 0.55 ppm hydrogen 2 |
| |
| air air_2023 |
| |
| # universal gas constant |
| R_1976 8.31432e3 N m/(kmol K) |
| |
| # polytropic index n |
| polyndx_1976 air_1976 (kg/kmol) gravity/(R_1976 lapserate) - 1 |
| |
| # If desired, redefine using current values for air mol wt and R |
| |
| polyndx polyndx_1976 |
| # polyndx air (kg/kmol) gravity/(R lapserate) - 1 |
| |
| # for comparison with various references |
| |
| polyexpnt (polyndx + 1) / polyndx |
| |
| # The model assumes the following reference values: |
| # sea-level temperature and pressure |
| |
| stdatmT0 288.15 K |
| stdatmP0 atm |
| |
| # "effective radius" for relation of geometric to geopotential height, |
| # at a latitude at which g = 9.80665 m/s (approximately 45.543 deg); no |
| # relation to actual radius |
| |
| earthradUSAtm 6356766 m |
| |
| # Temperature vs. geopotential height h |
| # Assumes 15 degC at sea level |
| # Based on approx 45 deg latitude |
| # Lower limits of domain and upper limits of range are those of the |
| # tables in US Standard Atmosphere (NASA 1976) |
| |
| stdatmTH(h) units=[m;K] domain=[-5000,11e3] range=[217,321] \ |
| stdatmT0+(-lapserate h) ; (stdatmT0+(-stdatmTH))/lapserate |
| |
| # Temperature vs. geometric height z; based on approx 45 deg latitude |
| stdatmT(z) units=[m;K] domain=[-5000,11e3] range=[217,321] \ |
| stdatmTH(geop_ht(z)) ; ~geop_ht(~stdatmTH(stdatmT)) |
| |
| # Pressure vs. geopotential height h |
| # Assumes 15 degC and 101325 Pa at sea level |
| # Based on approx 45 deg latitude |
| # Lower limits of domain and upper limits of range are those of the |
| # tables in US Standard Atmosphere (NASA 1976) |
| |
| stdatmPH(h) units=[m;Pa] domain=[-5000,11e3] range=[22877,177764] \ |
| atm (1 - (lapserate/stdatmT0) h)^(polyndx + 1) ; \ |
| (stdatmT0/lapserate) (1+(-(stdatmPH/stdatmP0)^(1/(polyndx + 1)))) |
| |
| # Pressure vs. geometric height z; based on approx 45 deg latitude |
| stdatmP(z) units=[m;Pa] domain=[-5000,11e3] range=[22877,177764] \ |
| stdatmPH(geop_ht(z)); ~geop_ht(~stdatmPH(stdatmP)) |
| |
| # Geopotential height from geometric height |
| # Based on approx 45 deg latitude |
| # Lower limits of domain and range are somewhat arbitrary; they |
| # correspond to the limits in the US Std Atm tables |
| |
| geop_ht(z) units=[m;m] domain=[-5000,) range=[-5004,) \ |
| (earthradUSAtm z) / (earthradUSAtm + z) ; \ |
| (earthradUSAtm geop_ht) / (earthradUSAtm + (-geop_ht)) |
| |
| # The standard value for the sea-level acceleration due to gravity is |
| # 9.80665 m/s^2, but the actual value varies with latitude (Harrison 1949) |
| # R_eff = 2 g_phi / denom |
| # g_phi = 978.0356e-2 (1+0.0052885 sin(lat)^2+(-0.0000059) sin(2 lat)^2) |
| # or |
| # g_phi = 980.6160e-2 (1+(-0.0026373) cos(2 lat)+0.0000059 cos(2 lat)^2) |
| # denom = 3.085462e-6+2.27e-9 cos(2 lat)+(-2e-12) cos(4 lat) (minutes?) |
| # There is no inverse function; the standard value applies at a latitude |
| # of about 45.543 deg |
| |
| g_phi(lat) units=[deg;m/s2] domain=[0,90] noerror \ |
| 980.6160e-2 (1+(-0.0026373) cos(2 lat)+0.0000059 cos(2 lat)^2) m/s2 |
| |
| # effective Earth radius for relation of geometric height to |
| # geopotential height, as function of latitude (Harrison 1949) |
| |
| earthradius_eff(lat) units=[deg;m] domain=[0,90] noerror \ |
| m 2 9.780356 (1+0.0052885 sin(lat)^2+(-0.0000059) sin(2 lat)^2) / \ |
| (3.085462e-6 + 2.27e-9 cos(2 lat) + (-2e-12) cos(4 lat)) |
| |
| # References |
| # Harrison, L.P. 1949. Relation Between Geopotential and Geometric |
| # Height. In Smithsonian Meteorological Tables. List, Robert J., ed. |
| # 6th ed., 4th reprint, 1968. Washington, DC: Smithsonian Institution. |
| # NASA. US National Aeronautics and Space Administration. 1976. |
| # US Standard Atmosphere 1976. Washington, DC: US Government Printing Office. |
| |
| # Gauge pressure functions |
| # |
| # Gauge pressure is measured relative to atmospheric pressure. In the English |
| # system, where pressure is often given in pounds per square inch, gauge |
| # pressure is often indicated by 'psig' to distinguish it from absolute |
| # pressure, often indicated by 'psia'. At the standard atmospheric pressure |
| # of 14.696 psia, a gauge pressure of 0 psig is an absolute pressure of 14.696 |
| # psia; an automobile tire inflated to 31 psig has an absolute pressure of |
| # 45.696 psia. |
| # |
| # With gaugepressure(), the units must be specified (e.g., gaugepressure(1.5 |
| # bar)); with psig(), the units are taken as psi, so the example above of tire |
| # pressure could be given as psig(31). |
| # |
| # If the normal elevation is significantly different from sea level, change |
| # Patm appropriately, and adjust the lower domain limit on the gaugepressure |
| # definition. |
| |
| Patm atm |
| |
| gaugepressure(x) units=[Pa;Pa] domain=[-101325,) range=[0,) \ |
| x + Patm ; gaugepressure+(-Patm) |
| |
| psig(x) units=[1;Pa] domain=[-14.6959487755135,) range=[0,) \ |
| gaugepressure(x psi) ; ~gaugepressure(psig) / psi |
| |
| |
| # Pressure for underwater diving |
| |
| seawater 0.1 bar / meter |
| msw meter seawater |
| fsw foot seawater |
| |
| # |
| # Wire Gauge |
| # |
| # This area is a nightmare with huge charts of wire gauge diameters |
| # that usually have no clear origin. There are at least 5 competing wire gauge |
| # systems to add to the confusion. The use of wire gauge is related to the |
| # manufacturing method: a metal rod is heated and drawn through a hole. The |
| # size change can't be too big. To get smaller wires, the process is repeated |
| # with a series of smaller holes. Generally larger gauges mean smaller wires. |
| # The gauges often have values such as "00" and "000" which are larger sizes |
| # than simply "0" gauge. In the tables that appear below, these gauges must be |
| # specified as negative numbers (e.g. "00" is -1, "000" is -2, etc). |
| # Alternatively, you can use the following units: |
| # |
| |
| g00 (-1) |
| g000 (-2) |
| g0000 (-3) |
| g00000 (-4) |
| g000000 (-5) |
| g0000000 (-6) |
| |
| # American Wire Gauge (AWG) or Brown & Sharpe Gauge appears to be the most |
| # important gauge. ASTM B-258 specifies that this gauge is based on geometric |
| # interpolation between gauge 0000, which is 0.46 inches exactly, and gauge 36 |
| # which is 0.005 inches exactly. Therefore, the diameter in inches of a wire |
| # is given by the formula 1|200 92^((36-g)/39). Note that 92^(1/39) is close |
| # to 2^(1/6), so diameter is approximately halved for every 6 gauges. For the |
| # repeated zero values, use negative numbers in the formula. The same document |
| # also specifies rounding rules which seem to be ignored by makers of tables. |
| # Gauges up to 44 are to be specified with up to 4 significant figures, but no |
| # closer than 0.0001 inch. Gauges from 44 to 56 are to be rounded to the |
| # nearest 0.00001 inch. |
| # |
| # In addition to being used to measure wire thickness, this gauge is used to |
| # measure the thickness of sheets of aluminum, copper, and most metals other |
| # than steel, iron and zinc. |
| |
| wiregauge(g) units=[1;m] range=(0,) \ |
| 1|200 92^((36+(-g))/39) in; 36+(-39)ln(200 wiregauge/in)/ln(92) |
| awg() wiregauge |
| |
| # Next we have the SWG, the Imperial or British Standard Wire Gauge. This one |
| # is piecewise linear. It was used for aluminum sheets but also shows up for |
| # wire used in jewelry. |
| |
| brwiregauge[in] \ |
| -6 0.5 \ |
| -5 0.464 \ |
| -3 0.4 \ |
| -2 0.372 \ |
| 3 0.252 \ |
| 6 0.192 \ |
| 10 0.128 \ |
| 14 0.08 \ |
| 19 0.04 \ |
| 23 0.024 \ |
| 26 0.018 \ |
| 28 0.0148 \ |
| 30 0.0124 \ |
| 39 0.0052 \ |
| 49 0.0012 \ |
| 50 0.001 |
| |
| swg() brwiregauge |
| |
| # The following is from the Appendix to ASTM B 258 |
| # |
| # For example, in U.S. gage, the standard for sheet metal is based on the |
| # weight of the metal, not on the thickness. 16-gage is listed as |
| # approximately .0625 inch thick and 40 ounces per square foot (the original |
| # standard was based on wrought iron at .2778 pounds per cubic inch; steel |
| # has almost entirely superseded wrought iron for sheet use, at .2833 pounds |
| # per cubic inch). Smaller numbers refer to greater thickness. There is no |
| # formula for converting gage to thickness or weight. |
| # |
| # It's rather unclear from the passage above whether the plate gauge values are |
| # therefore wrong if steel is being used. Reference [15] states that steel is |
| # in fact measured using this gauge (under the name Manufacturers' Standard |
| # Gauge) with a density of 501.84 lb/ft3 = 0.2904 lb/in3 used for steel. |
| # But this doesn't seem to be the correct density of steel (.2833 lb/in3 is |
| # closer). |
| # |
| # This gauge was established in 1893 for purposes of taxation. |
| |
| # Old plate gauge for iron |
| |
| plategauge[(oz/ft^2)/(480*lb/ft^3)] \ |
| -5 300 \ |
| 1 180 \ |
| 14 50 \ |
| 16 40 \ |
| 17 36 \ |
| 20 24 \ |
| 26 12 \ |
| 31 7 \ |
| 36 4.5 \ |
| 38 4 |
| |
| # Manufacturers Standard Gage |
| |
| stdgauge[(oz/ft^2)/(501.84*lb/ft^3)] \ |
| -5 300 \ |
| 1 180 \ |
| 14 50 \ |
| 16 40 \ |
| 17 36 \ |
| 20 24 \ |
| 26 12 \ |
| 31 7 \ |
| 36 4.5 \ |
| 38 4 |
| |
| # A special gauge is used for zinc sheet metal. Notice that larger gauges |
| # indicate thicker sheets. |
| |
| zincgauge[in] \ |
| 1 0.002 \ |
| 10 0.02 \ |
| 15 0.04 \ |
| 19 0.06 \ |
| 23 0.1 \ |
| 24 0.125 \ |
| 27 0.5 \ |
| 28 1 |
| |
| # |
| # Imperial drill bit sizes are reported in inches or in a numerical or |
| # letter gauge. |
| # |
| |
| drillgauge[in] \ |
| 1 0.2280 \ |
| 2 0.2210 \ |
| 3 0.2130 \ |
| 4 0.2090 \ |
| 5 0.2055 \ |
| 6 0.2040 \ |
| 7 0.2010 \ |
| 8 0.1990 \ |
| 9 0.1960 \ |
| 10 0.1935 \ |
| 11 0.1910 \ |
| 12 0.1890 \ |
| 13 0.1850 \ |
| 14 0.1820 \ |
| 15 0.1800 \ |
| 16 0.1770 \ |
| 17 0.1730 \ |
| 18 0.1695 \ |
| 19 0.1660 \ |
| 20 0.1610 \ |
| 22 0.1570 \ |
| 23 0.1540 \ |
| 24 0.1520 \ |
| 25 0.1495 \ |
| 26 0.1470 \ |
| 27 0.1440 \ |
| 28 0.1405 \ |
| 29 0.1360 \ |
| 30 0.1285 \ |
| 31 0.1200 \ |
| 32 0.1160 \ |
| 33 0.1130 \ |
| 34 0.1110 \ |
| 35 0.1100 \ |
| 36 0.1065 \ |
| 38 0.1015 \ |
| 39 0.0995 \ |
| 40 0.0980 \ |
| 41 0.0960 \ |
| 42 0.0935 \ |
| 43 0.0890 \ |
| 44 0.0860 \ |
| 45 0.0820 \ |
| 46 0.0810 \ |
| 48 0.0760 \ |
| 51 0.0670 \ |
| 52 0.0635 \ |
| 53 0.0595 \ |
| 54 0.0550 \ |
| 55 0.0520 \ |
| 56 0.0465 \ |
| 57 0.0430 \ |
| 65 0.0350 \ |
| 66 0.0330 \ |
| 68 0.0310 \ |
| 69 0.0292 \ |
| 70 0.0280 \ |
| 71 0.0260 \ |
| 73 0.0240 \ |
| 74 0.0225 \ |
| 75 0.0210 \ |
| 76 0.0200 \ |
| 78 0.0160 \ |
| 79 0.0145 \ |
| 80 0.0135 \ |
| 88 0.0095 \ |
| 104 0.0031 |
| |
| drillA 0.234 in |
| drillB 0.238 in |
| drillC 0.242 in |
| drillD 0.246 in |
| drillE 0.250 in |
| drillF 0.257 in |
| drillG 0.261 in |
| drillH 0.266 in |
| drillI 0.272 in |
| drillJ 0.277 in |
| drillK 0.281 in |
| drillL 0.290 in |
| drillM 0.295 in |
| drillN 0.302 in |
| drillO 0.316 in |
| drillP 0.323 in |
| drillQ 0.332 in |
| drillR 0.339 in |
| drillS 0.348 in |
| drillT 0.358 in |
| drillU 0.368 in |
| drillV 0.377 in |
| drillW 0.386 in |
| drillX 0.397 in |
| drillY 0.404 in |
| drillZ 0.413 in |
| |
| # |
| # Screw sizes |
| # |
| # In the USA, screw diameters for both wood screws and machine screws |
| # are reported using a gauge number. Metric machine screws are |
| # reported as Mxx where xx is the diameter in mm. |
| # |
| |
| screwgauge(g) units=[1;m] range=[0,) \ |
| (.06 + .013 g) in ; (screwgauge/in + (-.06)) / .013 |
| |
| # |
| # Abrasive grit size |
| # |
| # Standards governing abrasive grit sizes are complicated, specifying |
| # fractions of particles that are passed or retained by different mesh |
| # sizes. As a result, it is not possible to make precise comparisons |
| # of different grit standards. The tables below allow the |
| # determination of rough equivlants by using median particle size. |
| # |
| # Standards in the USA are determined by the Unified Abrasives |
| # Manufacturers' Association (UAMA), which resulted from the merger of |
| # several previous organizations. One of the old organizations was |
| # CAMI (Coated Abrasives Manufacturers' Institute). |
| # |
| # UAMA has a web page with plots showing abrasive particle ranges for |
| # various different grits and comparisons between standards. |
| # |
| # https://uama.org/abrasives-101/ |
| # |
| # Abrasives are grouped into "bonded" abrasives for use with grinding |
| # wheels and "coated" abrasives for sandpapers and abrasive films. |
| # The industry uses different grit standards for these two |
| # categories. |
| # |
| # Another division is between "macrogrits", grits below 240 and |
| # "microgrits", which are above 240. Standards differ, as do methods |
| # for determining particle size. In the USA, ANSI B74.12 is the |
| # standard governing macrogrits. ANSI B74.10 covers bonded microgrit |
| # abrasives, and ANSI B74.18 covers coated microgrit abrasives. It |
| # appears that the coated standard is identical to the bonded standard |
| # for grits up through 600 but then diverges significantly. |
| # |
| # European grit sizes are determined by the Federation of European |
| # Producers of Abrasives. http://www.fepa-abrasives.org |
| # |
| # They give two standards, the "F" grit for bonded abrasives and the |
| # "P" grit for coated abrasives. This data is taken directly from |
| # their web page. |
| |
| # FEPA P grit for coated abrasives is commonly seen on sandpaper in |
| # the USA where the paper will be marked P600, for example. FEPA P |
| # grits are said to be more tightly constrained than comparable ANSI |
| # grits so that the particles are more uniform in size and hence give |
| # a better finish. |
| |
| grit_P[micron] \ |
| 12 1815 \ |
| 16 1324 \ |
| 20 1000 \ |
| 24 764 \ |
| 30 642 \ |
| 36 538 \ |
| 40 425 \ |
| 50 336 \ |
| 60 269 \ |
| 80 201 \ |
| 100 162 \ |
| 120 125 \ |
| 150 100 \ |
| 180 82 \ |
| 220 68 \ |
| 240 58.5 \ |
| 280 52.2 \ |
| 320 46.2 \ |
| 360 40.5 \ |
| 400 35 \ |
| 500 30.2 \ |
| 600 25.8 \ |
| 800 21.8 \ |
| 1000 18.3 \ |
| 1200 15.3 \ |
| 1500 12.6 \ |
| 2000 10.3 \ |
| 2500 8.4 |
| |
| # The F grit is the European standard for bonded abrasives such as |
| # grinding wheels |
| |
| grit_F[micron] \ |
| 4 4890 \ |
| 5 4125 \ |
| 6 3460 \ |
| 7 2900 \ |
| 8 2460 \ |
| 10 2085 \ |
| 12 1765 \ |
| 14 1470 \ |
| 16 1230 \ |
| 20 1040 \ |
| 22 885 \ |
| 24 745 \ |
| 30 625 \ |
| 36 525 \ |
| 40 438 \ |
| 46 370 \ |
| 54 310 \ |
| 60 260 \ |
| 70 218 \ |
| 80 185 \ |
| 90 154 \ |
| 100 129 \ |
| 120 109 \ |
| 150 82 \ |
| 180 69 \ |
| 220 58 \ |
| 230 53 \ |
| 240 44.5 \ |
| 280 36.5 \ |
| 320 29.2 \ |
| 360 22.8 \ |
| 400 17.3 \ |
| 500 12.8 \ |
| 600 9.3 \ |
| 800 6.5 \ |
| 1000 4.5 \ |
| 1200 3 \ |
| 1500 2.0 \ |
| 2000 1.2 |
| |
| # According to the UAMA web page, the ANSI bonded and ANSI coated standards |
| # are identical to FEPA F in the macrogrit range (under 240 grit), so these |
| # values are taken from the FEPA F table. The values for 240 and above are |
| # from the UAMA web site and represent the average of the "d50" range |
| # endpoints listed there. |
| |
| ansibonded[micron] \ |
| 4 4890 \ |
| 5 4125 \ |
| 6 3460 \ |
| 7 2900 \ |
| 8 2460 \ |
| 10 2085 \ |
| 12 1765 \ |
| 14 1470 \ |
| 16 1230 \ |
| 20 1040 \ |
| 22 885 \ |
| 24 745 \ |
| 30 625 \ |
| 36 525 \ |
| 40 438 \ |
| 46 370 \ |
| 54 310 \ |
| 60 260 \ |
| 70 218 \ |
| 80 185 \ |
| 90 154 \ |
| 100 129 \ |
| 120 109 \ |
| 150 82 \ |
| 180 69 \ |
| 220 58 \ |
| 240 50 \ |
| 280 39.5 \ |
| 320 29.5 \ |
| 360 23 \ |
| 400 18.25 \ |
| 500 13.9 \ |
| 600 10.55 \ |
| 800 7.65 \ |
| 1000 5.8 \ |
| 1200 3.8 |
| |
| grit_ansibonded() ansibonded |
| |
| # Like the bonded grit, the coated macrogrits below 240 are taken from the |
| # FEPA F table. Data above this is from the UAMA site. Note that the coated |
| # and bonded standards are evidently the same from 240 up to 600 grit, but |
| # starting at 800 grit, the coated standard diverges. The data from UAMA show |
| # that 800 grit coated has an average size slightly larger than the average |
| # size of 600 grit coated/bonded. However, the 800 grit has a significantly |
| # smaller particle size variation. |
| # |
| # Because of this non-monotonicity from 600 grit to 800 grit this definition |
| # produces a warning about the lack of a unique inverse. |
| |
| ansicoated[micron] noerror \ |
| 4 4890 \ |
| 5 4125 \ |
| 6 3460 \ |
| 7 2900 \ |
| 8 2460 \ |
| 10 2085 \ |
| 12 1765 \ |
| 14 1470 \ |
| 16 1230 \ |
| 20 1040 \ |
| 22 885 \ |
| 24 745 \ |
| 30 625 \ |
| 36 525 \ |
| 40 438 \ |
| 46 370 \ |
| 54 310 \ |
| 60 260 \ |
| 70 218 \ |
| 80 185 \ |
| 90 154 \ |
| 100 129 \ |
| 120 109 \ |
| 150 82 \ |
| 180 69 \ |
| 220 58 \ |
| 240 50 \ |
| 280 39.5 \ |
| 320 29.5 \ |
| 360 23 \ |
| 400 18.25 \ |
| 500 13.9 \ |
| 600 10.55 \ |
| 800 11.5 \ |
| 1000 9.5 \ |
| 2000 7.2 \ |
| 2500 5.5 \ |
| 3000 4 \ |
| 4000 3 \ |
| 6000 2 \ |
| 8000 1.2 |
| |
| grit_ansicoated() ansicoated |
| |
| |
| # |
| # Is this correct? This is the JIS Japanese standard used on waterstones |
| # |
| jisgrit[micron] \ |
| 150 75 \ |
| 180 63 \ |
| 220 53 \ |
| 280 48 \ |
| 320 40 \ |
| 360 35 \ |
| 400 30 \ |
| 600 20 \ |
| 700 17 \ |
| 800 14 \ |
| 1000 11.5 \ |
| 1200 9.5 \ |
| 1500 8 \ |
| 2000 6.7 \ |
| 2500 5.5 \ |
| 3000 4 \ |
| 4000 3 \ |
| 6000 2 \ |
| 8000 1.2 |
| |
| # The "Finishing Scale" marked with an A (e.g. A75). This information |
| # is from the web page of the sand paper manufacturer Klingspor |
| # https://www.klingspor.com/ctemplate1.aspx?page=default/html/gritGradingSystems_en-US.html |
| # |
| # I have no information about what this scale is used for. |
| |
| grit_A[micron]\ |
| 16 15.3 \ |
| 25 21.8 \ |
| 30 23.6 \ |
| 35 25.75 \ |
| 45 35 \ |
| 60 46.2 \ |
| 65 53.5 \ |
| 75 58.5 \ |
| 90 65 \ |
| 110 78 \ |
| 130 93 \ |
| 160 127 \ |
| 200 156 |
| # |
| # Grits for DMT brand diamond sharpening stones from |
| # https://www.dmtsharp.com/resources/dmt-catalog-product-information.html |
| # "DMT Diamond Grits" PDF download |
| |
| dmtxxcoarse 120 micron # 120 mesh |
| dmtsilver dmtxxcoarse |
| dmtxx dmtxxcoarse |
| dmtxcoarse 60 micron # 220 mesh |
| dmtx dmtxcoarse |
| dmtblack dmtxcoarse |
| dmtcoarse 45 micron # 325 mesh |
| dmtc dmtcoarse |
| dmtblue dmtcoarse |
| dmtfine 25 micron # 600 mesh |
| dmtred dmtfine |
| dmtf dmtfine |
| dmtefine 9 micron # 1200 mesh |
| dmte dmtefine |
| dmtgreen dmtefine |
| dmtceramic 7 micron # 2200 mesh |
| dmtcer dmtceramic |
| dmtwhite dmtceramic |
| dmteefine 3 micron # 8000 mesh |
| dmttan dmteefine |
| dmtee dmteefine |
| |
| # |
| # The following values come from a page in the Norton Stones catalog, |
| # available at their web page, http://www.nortonstones.com. |
| # |
| |
| hardtranslucentarkansas 6 micron # Natural novaculite (silicon quartz) |
| softarkansas 22 micron # stones |
| |
| extrafineindia 22 micron # India stones are Norton's manufactured |
| fineindia 35 micron # aluminum oxide product |
| mediumindia 53.5 micron |
| coarseindia 97 micron |
| |
| finecrystolon 45 micron # Crystolon stones are Norton's |
| mediumcrystalon 78 micron # manufactured silicon carbide product |
| coarsecrystalon 127 micron |
| |
| # The following are not from the Norton catalog |
| hardblackarkansas 6 micron |
| hardwhitearkansas 11 micron |
| washita 35 micron |
| |
| # |
| # Mesh systems for measuring particle sizes by sifting through a wire |
| # mesh or sieve |
| # |
| |
| # The Tyler system and US Sieve system are based on four steps for |
| # each factor of 2 change in the size, so each size is 2^1|4 different |
| # from the adjacent sizes. Unfortunately, the mesh numbers are |
| # arbitrary, so the sizes cannot be expressed with a functional form. |
| # Various references round the values differently. The mesh numbers |
| # are supposed to correspond to the number of holes per inch, but this |
| # correspondence is only approximate because it doesn't include the |
| # wire size of the mesh. |
| |
| # The Tyler Mesh system was apparently introduced by the WS Tyler |
| # company, but it appears that they no longer use it. They follow the |
| # ASTM E11 standard. |
| |
| meshtyler[micron] \ |
| 2.5 8000 \ |
| 3 6727 \ |
| 3.5 5657 \ |
| 4 4757 \ |
| 5 4000 \ |
| 6 3364 \ |
| 7 2828 \ |
| 8 2378 \ |
| 9 2000 \ |
| 10 1682 \ |
| 12 1414 \ |
| 14 1189 \ |
| 16 1000 \ |
| 20 841 \ |
| 24 707 \ |
| 28 595 \ |
| 32 500 \ |
| 35 420 \ |
| 42 354 \ |
| 48 297 \ |
| 60 250 \ |
| 65 210 \ |
| 80 177 \ |
| 100 149 \ |
| 115 125 \ |
| 150 105 \ |
| 170 88 \ |
| 200 74 \ |
| 250 63 \ |
| 270 53 \ |
| 325 44 \ |
| 400 37 |
| |
| # US Sieve size, ASTM E11 |
| # |
| # The WS Tyler company prints the list from ASTM E11 in |
| # A Calculator for ASTM E11 Standard Sieve Designations |
| # https://blog.wstyler.com/particle-analysis/astm-e11-standard-designations |
| |
| sieve[micron] \ |
| 3.5 5600 \ |
| 4 4750 \ |
| 5 4000 \ |
| 6 3350 \ |
| 7 2800 \ |
| 8 2360 \ |
| 10 2000 \ |
| 12 1700 \ |
| 14 1400 \ |
| 16 1180 \ |
| 18 1000 \ |
| 20 850 \ |
| 25 710 \ |
| 30 600 \ |
| 35 500 \ |
| 40 425 \ |
| 45 355 \ |
| 50 300 \ |
| 60 250 \ |
| 70 212 \ |
| 80 180 \ |
| 100 150 \ |
| 120 125 \ |
| 140 106 \ |
| 170 90 \ |
| 200 75 \ |
| 230 63 \ |
| 270 53 \ |
| 325 45 \ |
| 400 38 \ |
| 450 32 \ |
| 500 25 \ |
| 625 20 # These last two values are not in the standard series |
| # but were included in the ASTM standard because they |
| meshUS() sieve # were in common usage. |
| |
| # British Mesh size, BS 410: 1986 |
| # This system appears to correspond to the Tyler and US system, but |
| # with different mesh numbers. |
| # |
| # http://www.panadyne.com/technical/panadyne_international_sieve_chart.pdf |
| # |
| |
| meshbritish[micron] \ |
| 3 5657 \ |
| 3.5 4757 \ |
| 4 4000 \ |
| 5 3364 \ |
| 6 2828 \ |
| 7 2378 \ |
| 8 2000 \ |
| 10 1682 \ |
| 12 1414 \ |
| 14 1189 \ |
| 16 1000 \ |
| 18 841 \ |
| 22 707 \ |
| 25 595 \ |
| 30 500 \ |
| 36 420 \ |
| 44 354 \ |
| 52 297 \ |
| 60 250 \ |
| 72 210 \ |
| 85 177 \ |
| 100 149 \ |
| 120 125 \ |
| 150 105 \ |
| 170 88 \ |
| 200 74 \ |
| 240 63 \ |
| 300 53 \ |
| 350 44 \ |
| 400 37 |
| |
| # French system, AFNOR NFX11-501: 1970 |
| # The system appears to be based on size doubling every 3 mesh |
| # numbers, though the values have been aggressively rounded. |
| # It's not clear if the unrounded values would be considered |
| # incorrect, so this is given as a table rather than a function. |
| # Functional form: |
| # meshtamis(mesh) units=[1;m] 5000 2^(1|3 (mesh-38)) micron |
| # |
| # http://www.panadyne.com/technical/panadyne_international_sieve_chart.pdf |
| |
| meshtamis[micron] \ |
| 17 40 \ |
| 18 50 \ |
| 19 63 \ |
| 20 80 \ |
| 21 100 \ |
| 22 125 \ |
| 23 160 \ |
| 24 200 \ |
| 25 250 \ |
| 26 315 \ |
| 27 400 \ |
| 28 500 \ |
| 29 630 \ |
| 30 800 \ |
| 31 1000 \ |
| 32 1250 \ |
| 33 1600 \ |
| 34 2000 \ |
| 35 2500 \ |
| 36 3150 \ |
| 37 4000 \ |
| 38 5000 |
| |
| # |
| # Ring size. All ring sizes are given as the circumference of the ring. |
| # |
| |
| # USA ring sizes. Several slightly different definitions seem to be in |
| # circulation. According to [15], the interior diameter of size n ring in |
| # inches is 0.32 n + 0.458 for n ranging from 3 to 13.5 by steps of 0.5. The |
| # size 2 ring is inconsistently 0.538in and no 2.5 size is listed. |
| # |
| # However, other sources list 0.455 + 0.0326 n and 0.4525 + 0.0324 n as the |
| # diameter and list no special case for size 2. (Or alternatively they are |
| # 1.43 + .102 n and 1.4216+.1018 n for measuring circumference in inches.) One |
| # reference claimed that the original system was that each size was 1|10 inch |
| # circumference, but that source doesn't have an explanation for the modern |
| # system which is somewhat different. |
| |
| ringsize(n) units=[1;in] domain=[2,) range=[1.6252,) \ |
| (1.4216+.1018 n) in ; (ringsize/in + (-1.4216))/.1018 |
| |
| # Old practice in the UK measured rings using the "Wheatsheaf gauge" with sizes |
| # specified alphabetically and based on the ring inside diameter in steps of |
| # 1|64 inch. This system was replaced in 1987 by British Standard 6820 which |
| # specifies sizes based on circumference. Each size is 1.25 mm different from |
| # the preceding size. The baseline is size C which is 40 mm circumference. |
| # The new sizes are close to the old ones. Sometimes it's necessary to go |
| # beyond size Z to Z+1, Z+2, etc. |
| |
| sizeAring 37.50 mm |
| sizeBring 38.75 mm |
| sizeCring 40.00 mm |
| sizeDring 41.25 mm |
| sizeEring 42.50 mm |
| sizeFring 43.75 mm |
| sizeGring 45.00 mm |
| sizeHring 46.25 mm |
| sizeIring 47.50 mm |
| sizeJring 48.75 mm |
| sizeKring 50.00 mm |
| sizeLring 51.25 mm |
| sizeMring 52.50 mm |
| sizeNring 53.75 mm |
| sizeOring 55.00 mm |
| sizePring 56.25 mm |
| sizeQring 57.50 mm |
| sizeRring 58.75 mm |
| sizeSring 60.00 mm |
| sizeTring 61.25 mm |
| sizeUring 62.50 mm |
| sizeVring 63.75 mm |
| sizeWring 65.00 mm |
| sizeXring 66.25 mm |
| sizeYring 67.50 mm |
| sizeZring 68.75 mm |
| |
| # Japanese sizes start with size 1 at a 13mm inside diameter and each size is |
| # 1|3 mm larger in diameter than the previous one. They are multiplied by pi |
| # to give circumference. |
| |
| jpringsize(n) units=[1;mm] domain=[1,) range=[0.040840704,) \ |
| (38|3 + n/3) pi mm ; 3 jpringsize/ pi mm + (-38) |
| |
| # The European ring sizes are the length of the circumference in mm minus 40. |
| |
| euringsize(n) units=[1;mm] (n+40) mm ; euringsize/mm + (-40) |
| |
| # |
| # Abbreviations |
| # |
| |
| mph mile/hr |
| brmpg mile/brgallon |
| usmpg mile/usgallon |
| mpg mile/gal |
| kph km/hr |
| fL footlambert |
| fpm ft/min |
| fps ft/s |
| rpm rev/min |
| rps rev/sec |
| mi mile |
| smi mile |
| nmi nauticalmile |
| mbh 1e3 btu/hour |
| mcm 1e3 circularmil |
| ipy inch/year # used for corrosion rates |
| ccf 100 ft^3 # used for selling water [18] |
| Mcf 1000 ft^3 # not million cubic feet [18] |
| kp kilopond |
| kpm kp meter |
| Wh W hour |
| hph hp hour |
| plf lb / foot # pounds per linear foot |
| |
| # |
| # Compatibility units with Unix version |
| # |
| |
| pa Pa |
| ev eV |
| hg Hg |
| oe Oe |
| mh mH |
| rd rod |
| pf pF |
| gr grain |
| nt N |
| hz Hz |
| hd hogshead |
| dry drygallon/gallon |
| nmile nauticalmile |
| beV GeV |
| bev beV |
| coul C |
| |
| # |
| # Radioactivity units |
| # |
| event !dimensionless |
| becquerel event /s # Activity of radioactive source |
| Bq becquerel # |
| curie 3.7e10 Bq # Defined in 1910 as the radioactivity |
| Ci curie # emitted by the amount of radon that is |
| # in equilibrium with 1 gram of radium. |
| rutherford 1e6 Bq # |
| |
| RADIATION_DOSE gray |
| gray J/kg # Absorbed dose of radiation |
| Gy gray # |
| rad 1e-2 Gy # From Radiation Absorbed Dose |
| rep 8.38 mGy # Roentgen Equivalent Physical, the amount |
| # of radiation which , absorbed in the |
| # body, would liberate the same amount |
| # of energy as 1 roentgen of X rays |
| # would, or 97 ergs. |
| |
| sievert J/kg # Dose equivalent: dosage that has the |
| Sv sievert # same effect on human tissues as 200 |
| rem 1e-2 Sv # keV X-rays. Different types of |
| # radiation are weighted by the |
| # Relative Biological Effectiveness |
| # (RBE). |
| # |
| # Radiation type RBE |
| # X-ray, gamma ray 1 |
| # beta rays, > 1 MeV 1 |
| # beta rays, < 1 MeV 1.08 |
| # neutrons, < 1 MeV 4-5 |
| # neutrons, 1-10 MeV 10 |
| # protons, 1 MeV 8.5 |
| # protons, .1 MeV 10 |
| # alpha, 5 MeV 15 |
| # alpha, 1 MeV 20 |
| # |
| # The energies are the kinetic energy |
| # of the particles. Slower particles |
| # interact more, so they are more |
| # effective ionizers, and hence have |
| # higher RBE values. |
| # |
| # rem stands for Roentgen Equivalent |
| # Mammal |
| banana_dose 0.1e-6 sievert # Informal measure of the dose due to |
| # eating one average sized banana |
| roentgen 2.58e-4 C / kg # Ionizing radiation that produces |
| # 1 statcoulomb of charge in 1 cc of |
| # dry air at stp. |
| rontgen roentgen # Sometimes it appears spelled this way |
| sievertunit 8.38 rontgen # Unit of gamma ray dose delivered in one |
| # hour at a distance of 1 cm from a |
| # point source of 1 mg of radium |
| # enclosed in platinum .5 mm thick. |
| |
| eman 1e-7 Ci/m^3 # radioactive concentration |
| mache 3.7e-7 Ci/m^3 |
| |
| # |
| # Atomic weights. The atomic weight of an element is the ratio of the mass of |
| # a mole of the element to 1|12 of a mole of Carbon 12. For each element, we |
| # list the atomic weights of all of the isotopes. The Standard Atomic Weights |
| # apply to the elements in the isotopic composition that occurs naturally on |
| # Earth. These are computed values based on the isotopic distribution, and |
| # may vary for specific samples. Elements which do not occur naturally do |
| # not have Standard Atomic Weights. For these elements, if data on the most |
| # stable isotope is available, is given. Otherwise, the user must specify the |
| # desired isotope. |
| |
| !include elements.units |
| |
| # Density of the elements |
| # |
| # Note some elements occur in multiple forms (allotropes) with different |
| # densities, and they are accordingly listed multiple times. |
| |
| # Density of gas phase elements at STP |
| |
| hydrogendensity 0.08988 g/l |
| heliumdensity 0.1786 g/l |
| neondensity 0.9002 g/l |
| nitrogendensity 1.2506 g/l |
| oxygendensity 1.429 g/l |
| fluorinedensity 1.696 g/l |
| argondensity 1.784 g/l |
| chlorinedensity 3.2 g/l |
| kryptondensity 3.749 g/l |
| xenondensity 5.894 g/l |
| radondensity 9.73 g/l |
| |
| # Density of liquid phase elements near room temperature |
| |
| brominedensity 3.1028 g/cm^3 |
| mercurydensity 13.534 g/cm^3 |
| |
| # Density of solid elements near room temperature |
| |
| lithiumdensity 0.534 g/cm^3 |
| potassiumdensity 0.862 g/cm^3 |
| sodiumdensity 0.968 g/cm^3 |
| rubidiumdensity 1.532 g/cm^3 |
| calciumdensity 1.55 g/cm^3 |
| magnesiumdensity 1.738 g/cm^3 |
| phosphorus_white_density 1.823 g/cm^3 |
| berylliumdensity 1.85 g/cm^3 |
| sulfur_gamma_density 1.92 g/cm^3 |
| cesiumdensity 1.93 g/cm^3 |
| carbon_amorphous_density 1.95 g/cm^3 # average value |
| sulfur_betadensity 1.96 g/cm^3 |
| sulfur_alpha_density 2.07 g/cm^3 |
| carbon_graphite_density 2.267 g/cm^3 |
| phosphorus_red_density 2.27 g/cm^3 # average value |
| silicondensity 2.3290 g/cm^3 |
| phosphorus_violet_density 2.36 g/cm^3 |
| borondensity 2.37 g/cm^3 |
| strontiumdensity 2.64 g/cm^3 |
| phosphorus_black_density 2.69 g/cm^3 |
| aluminumdensity 2.7 g/cm^3 |
| bariumdensity 3.51 g/cm^3 |
| carbon_diamond_density 3.515 g/cm^3 |
| scandiumdensity 3.985 g/cm^3 |
| selenium_vitreous_density 4.28 g/cm^3 |
| selenium_alpha_density 4.39 g/cm^3 |
| titaniumdensity 4.406 g/cm^3 |
| yttriumdensity 4.472 g/cm^3 |
| selenium_gray_density 4.81 g/cm^3 |
| iodinedensity 4.933 g/cm^3 |
| europiumdensity 5.264 g/cm^3 |
| germaniumdensity 5.323 g/cm^3 |
| radiumdensity 5.5 g/cm^3 |
| arsenicdensity 5.727 g/cm^3 |
| tin_alpha_density 5.769 g/cm^3 |
| galliumdensity 5.91 g/cm^3 |
| vanadiumdensity 6.11 g/cm^3 |
| lanthanumdensity 6.162 g/cm^3 |
| telluriumdensity 6.24 g/cm^3 |
| zirconiumdensity 6.52 g/cm^3 |
| antimonydensity 6.697 g/cm^3 |
| ceriumdensity 6.77 g/cm^3 |
| praseodymiumdensity 6.77 g/cm^3 |
| ytterbiumdensity 6.9 g/cm^3 |
| neodymiumdensity 7.01 g/cm^3 |
| zincdensity 7.14 g/cm^3 |
| chromiumdensity 7.19 g/cm^3 |
| manganesedensity 7.21 g/cm^3 |
| promethiumdensity 7.26 g/cm^3 |
| tin_beta_density 7.265 g/cm^3 |
| indiumdensity 7.31 g/cm^3 |
| samariumdensity 7.52 g/cm^3 |
| irondensity 7.874 g/cm^3 |
| gadoliniumdensity 7.9 g/cm^3 |
| terbiumdensity 8.23 g/cm^3 |
| dysprosiumdensity 8.54 g/cm^3 |
| niobiumdensity 8.57 g/cm^3 |
| cadmiumdensity 8.65 g/cm^3 |
| holmiumdensity 8.79 g/cm^3 |
| cobaltdensity 8.9 g/cm^3 |
| nickeldensity 8.908 g/cm^3 |
| erbiumdensity 9.066 g/cm^3 |
| polonium_alpha_density 9.196 g/cm^3 |
| thuliumdensity 9.32 g/cm^3 |
| polonium_beta_density 9.398 g/cm^3 |
| bismuthdensity 9.78 g/cm^3 |
| lutetiumdensity 9.841 g/cm^3 |
| actiniumdensity 10 g/cm^3 |
| molybdenumdensity 10.28 g/cm^3 |
| silverdensity 10.49 g/cm^3 |
| technetiumdensity 11 g/cm^3 |
| leaddensity 11.34 g/cm^3 |
| thoriumdensity 11.7 g/cm^3 |
| thalliumdensity 11.85 g/cm^3 |
| americiumdensity 12 g/cm^3 |
| palladiumdensity 12.023 g/cm^3 |
| rhodiumdensity 12.41 g/cm^3 |
| rutheniumdensity 12.45 g/cm^3 |
| berkelium_beta_density 13.25 g/cm^3 |
| hafniumdensity 13.31 g/cm^3 |
| curiumdensity 13.51 g/cm^3 |
| berkelium_alphadensity 14.78 g/cm^3 |
| californiumdensity 15.1 g/cm^3 |
| protactiniumdensity 15.37 g/cm^3 |
| tantalumdensity 16.69 g/cm^3 |
| uraniumdensity 19.1 g/cm^3 |
| tungstendensity 19.3 g/cm^3 |
| golddensity 19.30 g/cm^3 |
| plutoniumdensity 19.816 g/cm^3 |
| neptuniumdensity 20.45 g/cm^3 # alpha form, only one at room temp |
| rheniumdensity 21.02 g/cm^3 |
| platinumdensity 21.45 g/cm^3 |
| iridiumdensity 22.56 g/cm^3 |
| osmiumdensity 22.59 g/cm^3 |
| |
| # A few alternate names |
| |
| tin_gray tin_alpha_density |
| tin_white tin_beta_density |
| graphitedensity carbon_graphite_density |
| diamonddensity carbon_diamond_density |
| |
| # Predicted density of elements that have not been made in sufficient |
| # quantities for measurement. |
| |
| franciumdensity 2.48 g/cm^3 # liquid, predicted melting point 8 degC |
| astatinedensity 6.35 g/cm^3 |
| einsteiniumdensity 8.84 g/cm^3 |
| fermiumdensity 9.7 g/cm^3 |
| nobeliumdensity 9.9 g/cm^3 |
| mendeleviumdensity 10.3 g/cm^3 |
| lawrenciumdensity 16 g/cm^3 |
| rutherfordiumdensity 23.2 g/cm^3 |
| roentgeniumdensity 28.7 g/cm^3 |
| dubniumdensity 29.3 g/cm^3 |
| darmstadtiumdensity 34.8 g/cm^3 |
| seaborgiumdensity 35 g/cm^3 |
| bohriumdensity 37.1 g/cm^3 |
| meitneriumdensity 37.4 g/cm^3 |
| hassiumdensity 41 g/cm^3 |
| |
| # |
| # population units |
| # |
| |
| people 1 |
| person people |
| death people |
| capita people |
| percapita per capita |
| |
| # TGM dozen based unit system listed on the "dozenal" forum |
| # http://www.dozenalsociety.org.uk/apps/tgm.htm. These units are |
| # proposed as an allegedly more rational alternative to the SI system. |
| |
| Tim 12^-4 hour # Time |
| Grafut gravity Tim^2 # Length based on gravity |
| Surf Grafut^2 # area |
| Volm Grafut^3 # volume |
| Vlos Grafut/Tim # speed |
| Denz Maz/Volm # density |
| Mag Maz gravity # force |
| Maz Volm kg / oldliter # mass based on water |
| |
| # Abbreviations |
| |
| # Tm Tim # Conflicts with Tm = Terameter |
| Gf Grafut |
| Sf Surf |
| Vm Volm |
| Vl Vlos |
| Mz Maz |
| Dz Denz |
| |
| # Dozen based unit prefixes |
| |
| Zena- 12 |
| Duna- 12^2 |
| Trina- 12^3 |
| Quedra- 12^4 |
| Quena- 12^5 |
| Hesa- 12^6 |
| Seva- 12^7 |
| Aka- 12^8 |
| Neena- 12^9 |
| Dexa- 12^10 |
| Lefa- 12^11 |
| Zennila- 12^12 |
| |
| Zeni- 12^-1 |
| Duni- 12^-2 |
| Trini- 12^-3 |
| Quedri- 12^-4 |
| Queni- 12^-5 |
| Hesi- 12^-6 |
| Sevi- 12^-7 |
| Aki- 12^-8 |
| Neeni- 12^-9 |
| Dexi- 12^-10 |
| Lefi- 12^-11 |
| Zennili- 12^-12 |
| |
| # |
| # Traditional Japanese units (shakkanhou) |
| # |
| # The traditional system of weights and measures is called shakkanhou from the |
| # shaku and the ken. Japan accepted SI units in 1891 and legalized conversions |
| # to the traditional system. In 1909 the inch-pound system was also legalized, |
| # so Japan had three legally approved systems. A change to the metric system |
| # started in 1921 but there was a lot of resistance. The Measurement Law of |
| # October 1999 prohibits sales in anything but SI units. However, the old |
| # units still live on in construction and as the basis for paper sizes of books |
| # and tools used for handicrafts. |
| # |
| # Note that units below use the Hepburn romanization system. Some other |
| # systems would render "mou", "jou", and "chou" as "mo", "jo" and "cho". |
| # |
| # |
| # http://hiramatu-hifuka.com/onyak/onyindx.html |
| |
| # Japanese Proportions. These are still in everyday use. They also |
| # get used as units to represent the proportion of the standard unit. |
| |
| wari_proportion 1|10 |
| wari wari_proportion |
| bu_proportion 1|100 # The character bu can also be read fun or bun |
| # but usually "bu" is used for units. |
| rin_proportion 1|1000 |
| mou_proportion 1|10000 |
| |
| |
| # Japanese Length Measures |
| # |
| # The length system is called kanejaku or |
| # square and originated in China. It was |
| # adopted as Japan's official measure in 701 |
| # by the Taiho Code. This system is still in |
| # common use in architecture and clothing. |
| |
| shaku 1|3.3 m |
| mou 1|10000 shaku |
| rin 1|1000 shaku |
| bu_distance 1|100 shaku |
| sun 1|10 shaku |
| jou_distance 10 shaku |
| jou jou_distance |
| |
| kanejakusun sun # Alias to emphasize architectural name |
| kanejaku shaku |
| kanejakujou jou |
| |
| # http://en.wikipedia.org/wiki/Taiwanese_units_of_measurement |
| taichi shaku # http://zh.wikipedia.org/wiki/台尺 |
| taicun sun # http://zh.wikipedia.org/wiki/台制 |
| !utf8 |
| 台尺 taichi # via Hanyu Pinyin romanizations |
| 台寸 taicun |
| !endutf8 |
| |
| # In context of clothing, shaku is different from architecture |
| |
| kujirajaku 10|8 shaku |
| kujirajakusun 1|10 kujirajaku |
| kujirajakubu 1|100 kujirajaku |
| kujirajakujou 10 kujirajaku |
| tan_distance 3 kujirajakujou |
| |
| ken 6 shaku # Also sometimes 6.3, 6.5, or 6.6 |
| # http://www.homarewood.co.jp/syakusun.htm |
| |
| # mostly unused |
| chou_distance 60 ken |
| chou chou_distance |
| ri 36 chou |
| |
| # Japanese Area Measures |
| |
| # Tsubo is still used for land size, though the others are more |
| # recognized by their homonyms in the other measurements. |
| |
| gou_area 1|10 tsubo |
| tsubo 36 shaku^2 # Size of two tatami = ken^2 ?? |
| se 30 tsubo |
| tan_area 10 se |
| chou_area 10 tan_area |
| |
| # http://en.wikipedia.org/wiki/Taiwanese_units_of_measurement |
| ping tsubo # http://zh.wikipedia.org/wiki/坪 |
| jia 2934 ping # http://zh.wikipedia.org/wiki/甲_(单位) |
| fen 1|10 jia # http://zh.wikipedia.org/wiki/分 |
| fen_area 1|10 jia # Protection against future collisions |
| !utf8 |
| 坪 ping # via Hanyu Pinyin romanizations |
| 甲 jia |
| 分 fen |
| 分地 fen_area # Protection against future collisions |
| !endutf8 |
| |
| # Japanese architecture is based on a "standard" size of tatami mat. |
| # Room sizes today are given in number of tatami, and this number |
| # determines the spacing between colums and hence sizes of sliding |
| # doors and paper screens. However, every region has its own slightly |
| # different tatami size. Edoma, used in and around Tokyo and |
| # Hokkaido, is becoming a nationwide standard. Kyouma is used around |
| # Kyoto, Osaka and Kyuushu, and Chuukyouma is used around Nagoya. |
| # Note that the tatami all have the aspect ratio 2:1 so that the mats |
| # can tile the room with some of them turned 90 degrees. |
| # |
| # http://www.moon2.net/tatami/infotatami/structure.html |
| |
| edoma (5.8*2.9) shaku^2 |
| kyouma (6.3*3.15) shaku^2 |
| chuukyouma (6*3) shaku^2 |
| jou_area edoma |
| tatami jou_area |
| |
| # Japanese Volume Measures |
| |
| # The "shou" is still used for such things as alcohol and seasonings. |
| # Large quantities of paint are still purchased in terms of "to". |
| |
| shaku_volume 1|10 gou_volume |
| gou_volume 1|10 shou |
| gou gou_volume |
| shou (4.9*4.9*2.7) sun^3 # The character shou which is |
| # the same as masu refers to a |
| # rectangular wooden cup used to |
| # measure liquids and cereal. |
| # Sake is sometimes served in a masu |
| # Note that it happens to be |
| # EXACTLY 7^4/11^3 liters. |
| to 10 shou |
| koku 10 to # No longer used; historically a measure of rice |
| |
| # Japanese Weight Measures |
| # |
| # https://web.archive.org/web/20040927115452/http://wyoming.hp.infoseek.co.jp/zatugaku/zamoney.html |
| # https://en.wikipedia.org/wiki/Japanese_units_of_measurement |
| |
| # Not really used anymore. |
| |
| rin_weight 1|10 bu_weight |
| bu_weight 1|10 monme |
| fun 1|10 monme |
| monme momme |
| kin 160 monme |
| kan 1000 monme |
| kwan kan # This was the old pronunciation of the unit. |
| # The old spelling persisted a few centuries |
| # longer and was not changed until around |
| # 1950. |
| |
| # http://en.wikipedia.org/wiki/Taiwanese_units_of_measurement |
| # says: "Volume measure in Taiwan is largely metric". |
| taijin kin # http://zh.wikipedia.org/wiki/台斤 |
| tailiang 10 monme # http://zh.wikipedia.org/wiki/台斤 |
| taiqian monme # http://zh.wikipedia.org/wiki/台制 |
| !utf8 |
| 台斤 taijin # via Hanyu Pinyin romanizations |
| 台兩 tailiang |
| 台錢 taiqian |
| !endutf8 |
| |
| # |
| # Australian unit |
| # |
| |
| australiasquare (10 ft)^2 # Used for house area |
| |
| |
| # |
| # A few German units as currently in use. |
| # |
| |
| zentner 50 kg |
| doppelzentner 2 zentner |
| pfund 500 g |
| |
| # The klafter, which was used in central Europe, was derived from the span of |
| # outstretched arms. |
| # |
| # https://en.wikipedia.org/wiki/Obsolete_Austrian_units_of_measurement |
| # https://www.llv.li/files/abi/klafter-m2-en.pdf |
| |
| austriaklafter 1.89648384 m # Exact definition, 23 July 1871 |
| austriafoot 1|6 austriaklafter |
| prussiaklafter 1.88 m |
| prussiafoot 1|6 prussiaklafter |
| bavariaklafter 1.751155 m |
| bavariafoot 1|6 bavariaklafter |
| hesseklafter 2.5 m |
| hessefoot 1|6 hesseklafter |
| switzerlandklafter metricklafter |
| switzerlandfoot 1|6 switzerlandklafter |
| swissklafter switzerlandklafter |
| swissfoot 1|6 swissklafter |
| metricklafter 1.8 m |
| |
| austriayoke 8 austriaklafter * 200 austriaklafter |
| |
| liechtensteinsquareklafter 3.596652 m^2 # Used until 2017 to measure land area |
| liechtensteinklafter sqrt(liechtensteinsquareklafter) |
| |
| # The klafter was also used to measure volume of wood, generally being a stack |
| # of wood one klafter wide, one klafter long, with logs 3 feet (half a klafter) |
| # in length |
| |
| prussiawoodklafter 0.5 prussiaklafter^3 |
| austriawoodklafter 0.5 austriaklafter^3 |
| festmeter m^3 # modern measure of wood, solid cube |
| raummeter 0.7 festmeter # Air space between the logs, stacked |
| schuettraummeter 0.65 raummeter # A cubic meter volume of split and cut |
| # firewood in a loose, unordered |
| # pile, not stacked. This is called |
| # "tipped". |
| !utf8 |
| schüttraummeter schuettraummeter |
| !endutf8 |
| |
| |
| # |
| # Swedish (Sweden) pre-metric units of 1739. |
| # The metric system was adopted in 1878. |
| # https://sv.wikipedia.org/wiki/Verkm%C3%A5tt |
| # |
| |
| verklinje 2.0618125 mm |
| verktum 12 verklinje |
| kvarter 6 verktum |
| fot 2 kvarter |
| aln 2 fot |
| famn 3 aln |
| |
| # |
| # Some traditional Russian measures |
| # |
| # If you would like to help expand this section and understand |
| # cyrillic transliteration, let me know. These measures are meant to |
| # reflect common usage, e.g. in translated literature. |
| # |
| |
| dessiatine 2400 sazhen^2 # Land measure |
| dessjatine dessiatine |
| |
| funt 409.51718 grams # similar to pound |
| zolotnik 1|96 funt # used for precious metal measure |
| pood 40 funt # common in agricultural measure |
| |
| arshin (2 + 1|3) feet |
| sazhen 3 arshin # analogous to fathom |
| verst 500 sazhen # of similar use to mile |
| versta verst |
| borderverst 1000 sazhen |
| russianmile 7 verst |
| |
| |
| |
| |
| # |
| # Old French distance measures, from French Weights and Measures |
| # Before the Revolution by Zupko |
| # |
| |
| frenchfoot 144|443.296 m # pied de roi, the standard of Paris. |
| pied frenchfoot # Half of the hashimicubit, |
| frenchfeet frenchfoot # instituted by Charlemagne. |
| frenchinch 1|12 frenchfoot # This exact definition comes from |
| frenchthumb frenchinch # a law passed on 10 Dec 1799 which |
| pouce frenchthumb # fixed the meter at |
| # 3 frenchfeet + 11.296 lignes. |
| frenchline 1|12 frenchinch # This is supposed to be the size |
| ligne frenchline # of the average barleycorn |
| frenchpoint 1|12 frenchline |
| toise 6 frenchfeet |
| arpent 180^2 pied^2 # The arpent is 100 square perches, |
| # but the perche seems to vary a lot |
| # and can be 18 feet, 20 feet, or 22 |
| # feet. This measure was described |
| # as being in common use in Canada in |
| # 1934 (Websters 2nd). The value |
| # given here is the Paris standard |
| # arpent. |
| frenchgrain 1|18827.15 kg # Weight of a wheat grain, hence |
| # smaller than the British grain. |
| frenchpound 9216 frenchgrain |
| |
| # |
| # Before the Imperial Weights and Measures Act of 1824, various different |
| # weights and measures were in use in different places. |
| # |
| |
| # Scots linear measure |
| |
| scotsinch 1.00540054 UKinch |
| scotslink 1|100 scotschain |
| scotsfoot 12 scotsinch |
| scotsfeet scotsfoot |
| scotsell 37 scotsinch |
| scotsfall 6 scotsell |
| scotschain 4 scotsfall |
| scotsfurlong 10 scotschain |
| scotsmile 8 scotsfurlong |
| |
| # Scots area measure |
| |
| scotsrood 40 scotsfall^2 |
| scotsacre 4 scotsrood |
| |
| # Irish linear measure |
| |
| irishinch UKinch |
| irishpalm 3 irishinch |
| irishspan 3 irishpalm |
| irishfoot 12 irishinch |
| irishfeet irishfoot |
| irishcubit 18 irishinch |
| irishyard 3 irishfeet |
| irishpace 5 irishfeet |
| irishfathom 6 irishfeet |
| irishpole 7 irishyard # Only these values |
| irishperch irishpole # are different from |
| irishchain 4 irishperch # the British Imperial |
| irishlink 1|100 irishchain # or English values for |
| irishfurlong 10 irishchain # these lengths. |
| irishmile 8 irishfurlong # |
| |
| # Irish area measure |
| |
| irishrood 40 irishpole^2 |
| irishacre 4 irishrood |
| |
| # English wine capacity measures (Winchester measures) |
| |
| winepint 1|2 winequart |
| winequart 1|4 winegallon |
| winegallon 231 UKinch^3 # Sometimes called the Winchester Wine Gallon, |
| # it was legalized in 1707 by Queen Anne, and |
| # given the definition of 231 cubic inches. It |
| # had been in use for a while as 8 pounds of wine |
| # using a merchant's pound, but the definition of |
| # the merchant's pound had become uncertain. A |
| # pound of 15 tower ounces (6750 grains) had been |
| # common, but then a pound of 15 troy ounces |
| # (7200 grains) gained popularity. Because of |
| # the switch in the value of the merchants pound, |
| # the size of the wine gallon was uncertain in |
| # the market, hence the official act in 1707. |
| # The act allowed that a six inch tall cylinder |
| # with a 7 inch diameter was a lawful wine |
| # gallon. (This comes out to 230.9 in^3.) |
| # Note also that in Britain a legal conversion |
| # was established to the 1824 Imperial gallon |
| # then taken as 277.274 in^3 so that the wine |
| # gallon was 0.8331 imperial gallons. This is |
| # 231.1 cubic inches (using the international |
| # inch). |
| winerundlet 18 winegallon |
| winebarrel 31.5 winegallon |
| winetierce 42 winegallon |
| winehogshead 2 winebarrel |
| winepuncheon 2 winetierce |
| winebutt 2 winehogshead |
| winepipe winebutt |
| winetun 2 winebutt |
| |
| # English beer and ale measures used 1803-1824 and used for beer before 1688 |
| |
| beerpint 1|2 beerquart |
| beerquart 1|4 beergallon |
| beergallon 282 UKinch^3 |
| beerbarrel 36 beergallon |
| beerhogshead 1.5 beerbarrel |
| |
| # English ale measures used from 1688-1803 for both ale and beer |
| |
| alepint 1|2 alequart |
| alequart 1|4 alegallon |
| alegallon beergallon |
| alebarrel 34 alegallon |
| alehogshead 1.5 alebarrel |
| |
| # Scots capacity measure |
| |
| scotsgill 1|4 mutchkin |
| mutchkin 1|2 choppin |
| choppin 1|2 scotspint |
| scotspint 1|2 scotsquart |
| scotsquart 1|4 scotsgallon |
| scotsgallon 827.232 UKinch^3 |
| scotsbarrel 8 scotsgallon |
| jug scotspint |
| |
| # Scots dry capacity measure |
| |
| scotswheatlippy 137.333 UKinch^3 # Also used for peas, beans, rye, salt |
| scotswheatlippies scotswheatlippy |
| scotswheatpeck 4 scotswheatlippy |
| scotswheatfirlot 4 scotswheatpeck |
| scotswheatboll 4 scotswheatfirlot |
| scotswheatchalder 16 scotswheatboll |
| |
| scotsoatlippy 200.345 UKinch^3 # Also used for barley and malt |
| scotsoatlippies scotsoatlippy |
| scotsoatpeck 4 scotsoatlippy |
| scotsoatfirlot 4 scotsoatpeck |
| scotsoatboll 4 scotsoatfirlot |
| scotsoatchalder 16 scotsoatboll |
| |
| # Scots Tron weight |
| |
| trondrop 1|16 tronounce |
| tronounce 1|20 tronpound |
| tronpound 9520 grain |
| tronstone 16 tronpound |
| |
| # Irish liquid capacity measure |
| |
| irishnoggin 1|4 irishpint |
| irishpint 1|2 irishquart |
| irishquart 1|2 irishpottle |
| irishpottle 1|2 irishgallon |
| irishgallon 217.6 UKinch^3 |
| irishrundlet 18 irishgallon |
| irishbarrel 31.5 irishgallon |
| irishtierce 42 irishgallon |
| irishhogshead 2 irishbarrel |
| irishpuncheon 2 irishtierce |
| irishpipe 2 irishhogshead |
| irishtun 2 irishpipe |
| |
| # Irish dry capacity measure |
| |
| irishpeck 2 irishgallon |
| irishbushel 4 irishpeck |
| irishstrike 2 irishbushel |
| irishdrybarrel 2 irishstrike |
| irishquarter 2 irishbarrel |
| |
| # English Tower weights, abolished in 1528 |
| |
| towerpound 5400 grain |
| towerounce 1|12 towerpound |
| towerpennyweight 1|20 towerounce |
| towergrain 1|32 towerpennyweight |
| |
| # English Mercantile weights, used since the late 12th century |
| |
| mercpound 6750 grain |
| mercounce 1|15 mercpound |
| mercpennyweight 1|20 mercounce |
| |
| # English weights for lead |
| |
| leadstone 12.5 lb |
| fotmal 70 lb |
| leadwey 14 leadstone |
| fothers 12 leadwey |
| |
| # English Hay measure |
| |
| newhaytruss 60 lb # New and old here seem to refer to "new" |
| newhayload 36 newhaytruss # hay and "old" hay rather than a new unit |
| oldhaytruss 56 lb # and an old unit. |
| oldhayload 36 oldhaytruss |
| |
| # English wool measure |
| |
| woolclove 7 lb |
| woolstone 2 woolclove |
| wooltod 2 woolstone |
| woolwey 13 woolstone |
| woolsack 2 woolwey |
| woolsarpler 2 woolsack |
| woollast 6 woolsarpler |
| |
| # |
| # Ancient history units: There tends to be uncertainty in the definitions |
| # of the units in this section |
| # These units are from [11] |
| |
| # Roman measure. The Romans had a well defined distance measure, but their |
| # measures of weight were poor. They adopted local weights in different |
| # regions without distinguishing among them so that there are half a dozen |
| # different Roman "standard" weight systems. |
| |
| romanfoot 296 mm # There is some uncertainty in this definition |
| romanfeet romanfoot # from which all the other units are derived. |
| pes romanfoot # This value appears in numerous sources. In "The |
| pedes romanfoot # Roman Land Surveyors", Dilke gives 295.7 mm. |
| romaninch 1|12 romanfoot # The subdivisions of the Roman foot have the |
| romandigit 1|16 romanfoot # same names as the subdivisions of the pound, |
| romanpalm 1|4 romanfoot # but we can't have the names for different |
| romancubit 18 romaninch # units. |
| romanpace 5 romanfeet # Roman double pace (basic military unit) |
| passus romanpace |
| romanperch 10 romanfeet |
| stade 125 romanpaces |
| stadia stade |
| stadium stade |
| romanmile 8 stadia # 1000 paces |
| romanleague 1.5 romanmile |
| schoenus 4 romanmile |
| |
| # Other values for the Roman foot (from Dilke) |
| |
| earlyromanfoot 29.73 cm |
| pesdrusianus 33.3 cm # or 33.35 cm, used in Gaul & Germany in 1st c BC |
| lateromanfoot 29.42 cm |
| |
| # Roman areas |
| |
| actuslength 120 romanfeet # length of a Roman furrow |
| actus 120*4 romanfeet^2 # area of the furrow |
| squareactus 120^2 romanfeet^2 # actus quadratus |
| acnua squareactus |
| iugerum 2 squareactus |
| iugera iugerum |
| jugerum iugerum |
| jugera iugerum |
| heredium 2 iugera # heritable plot |
| heredia heredium |
| centuria 100 heredia |
| centurium centuria |
| |
| # Roman volumes |
| |
| sextarius 35.4 in^3 # Basic unit of Roman volume. As always, |
| sextarii sextarius # there is uncertainty. Six large Roman |
| # measures survive with volumes ranging from |
| # 34.4 in^3 to 39.55 in^3. Three of them |
| # cluster around the size given here. |
| # |
| # But the values for this unit vary wildly |
| # in other sources. One reference gives 0.547 |
| # liters, but then says the amphora is a |
| # cubic Roman foot. This gives a value for the |
| # sextarius of 0.540 liters. And the |
| # encyclopedia Britannica lists 0.53 liters for |
| # this unit. Both [7] and [11], which were |
| # written by scholars of weights and measures, |
| # give the value of 35.4 cubic inches. |
| cochlearia 1|48 sextarius |
| cyathi 1|12 sextarius |
| acetabula 1|8 sextarius |
| quartaria 1|4 sextarius |
| quartarius quartaria |
| heminae 1|2 sextarius |
| hemina heminae |
| cheonix 1.5 sextarii |
| |
| # Dry volume measures (usually) |
| |
| semodius 8 sextarius |
| semodii semodius |
| modius 16 sextarius |
| modii modius |
| |
| # Liquid volume measures (usually) |
| |
| congius 12 heminae |
| congii congius |
| amphora 8 congii |
| amphorae amphora # Also a dry volume measure |
| culleus 20 amphorae |
| quadrantal amphora |
| |
| # Roman weights |
| |
| libra 5052 grain # The Roman pound varied significantly |
| librae libra # from 4210 grains to 5232 grains. Most of |
| romanpound libra # the standards were obtained from the weight |
| uncia 1|12 libra # of particular coins. The one given here is |
| unciae uncia # based on the Gold Aureus of Augustus which |
| romanounce uncia # was in use from BC 27 to AD 296. |
| deunx 11 uncia |
| dextans 10 uncia |
| dodrans 9 uncia |
| bes 8 uncia |
| seprunx 7 uncia |
| semis 6 uncia |
| quincunx 5 uncia |
| triens 4 uncia |
| quadrans 3 uncia |
| sextans 2 uncia |
| sescuncia 1.5 uncia |
| semuncia 1|2 uncia |
| siscilius 1|4 uncia |
| sextula 1|6 uncia |
| semisextula 1|12 uncia |
| scriptulum 1|24 uncia |
| scrupula scriptulum |
| romanobol 1|2 scrupula |
| |
| romanaspound 4210 grain # Old pound based on bronze coinage, the |
| # earliest money of Rome BC 338 to BC 268. |
| |
| # Egyptian length measure |
| |
| egyptianroyalcubit 20.63 in # plus or minus .2 in |
| egyptianpalm 1|7 egyptianroyalcubit |
| egyptiandigit 1|4 egyptianpalm |
| egyptianshortcubit 6 egyptianpalm |
| |
| doubleremen 29.16 in # Length of the diagonal of a square with |
| remendigit 1|40 doubleremen # side length of 1 royal egyptian cubit. |
| # This is divided into 40 digits which are |
| # not the same size as the digits based on |
| # the royal cubit. |
| |
| # Greek length measures |
| |
| greekfoot 12.45 in # Listed as being derived from the |
| greekfeet greekfoot # Egyptian Royal cubit in [11]. It is |
| greekcubit 1.5 greekfoot # said to be 3|5 of a 20.75 in cubit. |
| pous greekfoot |
| podes greekfoot |
| orguia 6 greekfoot |
| greekfathom orguia |
| stadion 100 orguia |
| akaina 10 greekfeet |
| plethron 10 akaina |
| greekfinger 1|16 greekfoot |
| homericcubit 20 greekfingers # Elbow to end of knuckles. |
| shortgreekcubit 18 greekfingers # Elbow to start of fingers. |
| |
| ionicfoot 296 mm |
| doricfoot 326 mm |
| |
| olympiccubit 25 remendigit # These olympic measures were not as |
| olympicfoot 2|3 olympiccubit # common as the other greek measures. |
| olympicfinger 1|16 olympicfoot # They were used in agriculture. |
| olympicfeet olympicfoot |
| olympicdakylos olympicfinger |
| olympicpalm 1|4 olympicfoot |
| olympicpalestra olympicpalm |
| olympicspithame 3|4 foot |
| olympicspan olympicspithame |
| olympicbema 2.5 olympicfeet |
| olympicpace olympicbema |
| olympicorguia 6 olympicfeet |
| olympicfathom olympicorguia |
| olympiccord 60 olympicfeet |
| olympicamma olympiccord |
| olympicplethron 100 olympicfeet |
| olympicstadion 600 olympicfeet |
| |
| # Greek capacity measure |
| |
| greekkotyle 270 ml # This approximate value is obtained |
| xestes 2 greekkotyle # from two earthenware vessels that |
| khous 12 greekkotyle # were reconstructed from fragments. |
| metretes 12 khous # The kotyle is a day's corn ration |
| choinix 4 greekkotyle # for one man. |
| hekteos 8 choinix |
| medimnos 6 hekteos |
| |
| # Greek weight. Two weight standards were used, an Aegina standard based |
| # on the Beqa shekel and an Athens (attic) standard. |
| |
| aeginastater 192 grain # Varies up to 199 grain |
| aeginadrachmae 1|2 aeginastater |
| aeginaobol 1|6 aeginadrachmae |
| aeginamina 50 aeginastaters |
| aeginatalent 60 aeginamina # Supposedly the mass of a cubic foot |
| # of water (whichever foot was in use) |
| |
| atticstater 135 grain # Varies 134-138 grain |
| atticdrachmae 1|2 atticstater |
| atticobol 1|6 atticdrachmae |
| atticmina 50 atticstaters |
| attictalent 60 atticmina # Supposedly the mass of a cubic foot |
| # of water (whichever foot was in use) |
| |
| # "Northern" cubit and foot. This was used by the pre-Aryan civilization in |
| # the Indus valley. It was used in Mesopotamia, Egypt, North Africa, China, |
| # central and Western Europe until modern times when it was displaced by |
| # the metric system. |
| |
| northerncubit 26.6 in # plus/minus .2 in |
| northernfoot 1|2 northerncubit |
| |
| sumeriancubit 495 mm |
| kus sumeriancubit |
| sumerianfoot 2|3 sumeriancubit |
| |
| assyriancubit 21.6 in |
| assyrianfoot 1|2 assyriancubit |
| assyrianpalm 1|3 assyrianfoot |
| assyriansusi 1|20 assyrianpalm |
| susi assyriansusi |
| persianroyalcubit 7 assyrianpalm |
| |
| |
| # Arabic measures. The arabic standards were meticulously kept. Glass weights |
| # accurate to .2 grains were made during AD 714-900. |
| |
| hashimicubit 25.56 in # Standard of linear measure used |
| # in Persian dominions of the Arabic |
| # empire 7-8th cent. Is equal to two |
| # French feet. |
| |
| blackcubit 21.28 in |
| arabicfeet 1|2 blackcubit |
| arabicfoot arabicfeet |
| arabicinch 1|12 arabicfoot |
| arabicmile 4000 blackcubit |
| |
| silverdirhem 45 grain # The weights were derived from these two |
| tradedirhem 48 grain # units with two identically named systems |
| # used for silver and used for trade purposes |
| |
| silverkirat 1|16 silverdirhem |
| silverwukiyeh 10 silverdirhem |
| silverrotl 12 silverwukiyeh |
| arabicsilverpound silverrotl |
| |
| tradekirat 1|16 tradedirhem |
| tradewukiyeh 10 tradedirhem |
| traderotl 12 tradewukiyeh |
| arabictradepound traderotl |
| |
| # Miscellaneous ancient units |
| |
| parasang 3.5 mile # Persian unit of length usually thought |
| # to be between 3 and 3.5 miles |
| biblicalcubit 21.8 in |
| hebrewcubit 17.58 in |
| li 10|27.8 mile # Chinese unit of length |
| # 100 li is considered a day's march |
| liang 11|3 oz # Chinese weight unit |
| |
| |
| # Medieval time units. According to the OED, these appear in Du Cange |
| # by Papias. |
| |
| timepoint 1|5 hour # also given as 1|4 |
| timeminute 1|10 hour |
| timeostent 1|60 hour |
| timeounce 1|8 timeostent |
| timeatom 1|47 timeounce |
| |
| # Given in [15], these subdivisions of the grain were supposedly used |
| # by jewelers. The mite may have been used but the blanc could not |
| # have been accurately measured. |
| |
| mite 1|20 grain |
| droit 1|24 mite |
| periot 1|20 droit |
| blanc 1|24 periot |
| |
| # |
| # Localization |
| # |
| |
| !var UNITS_ENGLISH US |
| hundredweight ushundredweight |
| ton uston |
| scruple apscruple |
| fluidounce usfluidounce |
| gallon usgallon |
| bushel usbushel |
| quarter quarterweight |
| cup uscup |
| tablespoon ustablespoon |
| teaspoon usteaspoon |
| dollar US$ |
| cent $ 0.01 |
| penny cent |
| minim minimvolume |
| pony ponyvolume |
| grand usgrand |
| firkin usfirkin |
| hogshead ushogshead |
| cable uscable |
| !endvar |
| |
| !var UNITS_ENGLISH GB |
| hundredweight brhundredweight |
| ton brton |
| scruple brscruple |
| fluidounce brfluidounce |
| gallon brgallon |
| bushel brbushel |
| quarter brquarter |
| chaldron brchaldron |
| cup brcup |
| teacup brteacup |
| tablespoon brtablespoon |
| teaspoon brteaspoon |
| dollar US$ |
| cent $ 0.01 |
| penny brpenny |
| minim minimnote |
| pony brpony |
| grand brgrand |
| firkin brfirkin |
| hogshead brhogshead |
| cable brcable |
| !endvar |
| |
| !varnot UNITS_ENGLISH GB US |
| !message Unknown value for environment variable UNITS_ENGLISH. Should be GB or US. |
| !endvar |
| |
| |
| !utf8 |
| ⅛- 1|8 |
| ¼- 1|4 |
| ⅜- 3|8 |
| ½- 1|2 |
| ⅝- 5|8 |
| ¾- 3|4 |
| ⅞- 7|8 |
| ⅙- 1|6 |
| ⅓- 1|3 |
| ⅔- 2|3 |
| ⅚- 5|6 |
| ⅕- 1|5 |
| ⅖- 2|5 |
| ⅗- 3|5 |
| ⅘- 4|5 |
| # U+2150- 1|7 For some reason these characters are getting |
| # U+2151- 1|9 flagged as invalid UTF8. |
| # U+2152- 1|10 |
| #⅐- 1|7 # fails under MacOS |
| #⅑- 1|9 # fails under MacOS |
| #⅒- 1|10 # fails under MacOS |
| ℯ exp(1) # U+212F, base of natural log |
| µ- micro # micro sign U+00B5 |
| μ- micro # small mu U+03BC |
| ångström angstrom |
| Å angstrom # angstrom symbol U+212B |
| Å angstrom # A with ring U+00C5 |
| röntgen roentgen |
| °C degC |
| °F degF |
| °K K # °K is incorrect notation |
| °R degR |
| ° degree |
| ℃ degC |
| ℉ degF |
| K K # Kelvin symbol, U+212A |
| ℓ liter # unofficial abbreviation used in some places |
| Ω ohm # Ohm symbol U+2126 |
| Ω ohm # Greek capital omega U+03A9 |
| ℧ mho |
| G₀ G0 |
| H₀ H0 |
| Z₀ Z0 |
| a₀ a0 |
| n₀ n0 |
| ε₀ epsilon0 |
| μ₀ mu0 |
| Φ₀ Phi0 |
| R∞ Rinfinity |
| R_∞ Rinfinity |
| λ_C lambda_C |
| μ_B mu_B |
| ν_133Cs nu_133Cs |
| ʒ dram # U+0292 |
| ℈ scruple |
| ℥ ounce |
| ℔ lb |
| ℎ h |
| ℏ hbar |
| τ tau |
| π pi # Greek letter pi |
| 𝜋 pi # mathematical italic small pi |
| α alpha |
| σ sigma |
| ‰ 1|1000 |
| ‱ 1|10000 |
| ′ ' # U+2032 |
| ″ " # U+2033 |
| |
| # |
| # Unicode currency symbols |
| # |
| |
| ¢ cent |
| £ britainpound |
| ¥ japanyen |
| € euro |
| ₩ southkoreawon |
| ₪ israelnewshekel |
| ₤ lira |
| # ₺ turkeylira # fails under MacOS |
| ₨ rupee # unofficial legacy rupee sign |
| # ₹ indiarupee # official rupee sign # MacOS fail |
| #؋ afghanafghani # fails under MacOS |
| ฿ thailandbaht |
| ₡ costaricacolon |
| ₣ francefranc |
| ₦ nigerianaira |
| ₧ spainpeseta |
| ₫ vietnamdong |
| ₭ laokip |
| ₮ mongoliatugrik |
| ₯ greecedrachma |
| ₱ philippinepeso |
| # ₲ paraguayguarani # fails under MacOS |
| #₴ ukrainehryvnia # fails under MacOS |
| #₵ ghanacedi # fails under MacOS |
| #₸ kazakhstantenge # fails under MacOS |
| #₼ azerbaijanmanat # fails under MacOS |
| #₽ russiaruble # fails under MacOS |
| #₾ georgialari # fails under MacOS |
| ﷼ iranrial |
| ﹩ $ |
| ¢ ¢ |
| £ £ |
| ¥ ¥ |
| ₩ ₩ |
| |
| # |
| # Square Unicode symbols starting at U+3371 |
| # |
| |
| ㍱ hPa |
| ㍲ da |
| ㍳ au |
| ㍴ bar |
| # ㍵ oV??? |
| ㍶ pc |
| #㍷ dm invalid on Mac |
| #㍸ dm^2 invalid on Mac |
| #㍹ dm^3 invalid on Mac |
| ㎀ pA |
| ㎁ nA |
| ㎂ µA |
| ㎃ mA |
| ㎄ kA |
| ㎅ kB |
| ㎆ MB |
| ㎇ GB |
| ㎈ cal |
| ㎉ kcal |
| ㎊ pF |
| ㎋ nF |
| ㎌ µF |
| ㎍ µg |
| ㎎ mg |
| ㎏ kg |
| ㎐ Hz |
| ㎑ kHz |
| ㎒ MHz |
| ㎓ GHz |
| ㎔ THz |
| ㎕ µL |
| ㎖ mL |
| ㎗ dL |
| ㎘ kL |
| ㎙ fm |
| ㎚ nm |
| ㎛ µm |
| ㎜ mm |
| ㎝ cm |
| ㎞ km |
| ㎟ mm^2 |
| ㎠ cm^2 |
| ㎡ m^2 |
| ㎢ km^2 |
| ㎣ mm^3 |
| ㎤ cm^3 |
| ㎥ m^3 |
| ㎦ km^3 |
| ㎧ m/s |
| ㎨ m/s^2 |
| ㎩ Pa |
| ㎪ kPa |
| ㎫ MPa |
| ㎬ GPa |
| ㎭ rad |
| ㎮ rad/s |
| ㎯ rad/s^2 |
| ㎰ ps |
| ㎱ ns |
| ㎲ µs |
| ㎳ ms |
| ㎴ pV |
| ㎵ nV |
| ㎶ µV |
| ㎷ mV |
| ㎸ kV |
| ㎹ MV |
| ㎺ pW |
| ㎻ nW |
| ㎼ µW |
| ㎽ mW |
| ㎾ kW |
| ㎿ MW |
| ㏀ kΩ |
| ㏁ MΩ |
| ㏃ Bq |
| ㏄ cc |
| ㏅ cd |
| ㏆ C/kg |
| ㏈() dB |
| ㏉ Gy |
| ㏊ ha |
| # ㏋ HP?? |
| ㏌ in |
| # ㏍ KK?? |
| # ㏎ KM??? |
| ㏏ kt |
| ㏐ lm |
| # ㏑ ln |
| # ㏒ log |
| ㏓ lx |
| ㏔ mb |
| ㏕ mil |
| ㏖ mol |
| ㏗() pH |
| ㏙ ppm |
| # ㏚ PR??? |
| ㏛ sr |
| ㏜ Sv |
| ㏝ Wb |
| #㏞ V/m Invalid on Mac |
| #㏟ A/m Invalid on Mac |
| #㏿ gal Invalid on Mac |
| |
| !endutf8 |
| |
| ############################################################################ |
| # |
| # Unit list aliases |
| # |
| # These provide a shorthand for conversions to unit lists. |
| # |
| ############################################################################ |
| |
| !unitlist uswt lb;oz |
| !unitlist hms hr;min;sec |
| !unitlist time year;day;hr;min;sec |
| !unitlist dms deg;arcmin;arcsec |
| !unitlist ftin ft;in;1|8 in |
| !unitlist inchfine in;1|8 in;1|16 in;1|32 in;1|64 in |
| !unitlist usvol cup;3|4 cup;2|3 cup;1|2 cup;1|3 cup;1|4 cup;\ |
| tbsp;tsp;1|2 tsp;1|4 tsp;1|8 tsp |
| |
| ############################################################################ |
| # |
| # The following units were in the Unix units database but do not appear in |
| # this file: |
| # |
| # wey used for cheese, salt and other goods. Measured mass or |
| # waymass volume depending on what was measured and where the measuring |
| # took place. A wey of cheese ranged from 200 to 324 pounds. |
| # |
| # sack No precise definition |
| # |
| # spindle The length depends on the type of yarn |
| # |
| # block Defined variously on different computer systems |
| # |
| # erlang A unit of telephone traffic defined variously. |
| # Omitted because there are no other units for this |
| # dimension. Is this true? What about CCS = 1/36 erlang? |
| # Erlang is supposed to be dimensionless. One erlang means |
| # a single channel occupied for one hour. |
| # |
| ############################################################################ |
| # |
| # The following have been suggested or considered and deemed out of scope. |
| # They will not be added to GNU units. |
| # |
| # Conversions between different calendar systems used in different countries or |
| # different historical periods are out of scope for units and will not be added. |
| # |
| # Wind chill and heat index cannot be handled because they are bivarite, |
| # with dependence on both the temperature and wind speed or humidity. |
| # |
| # Plain english text output like "one hectare is equivalent to one hundred |
| # million square centimeters" is out of scope. |
| # |