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# | |
# This file is the units database for use with GNU units, a units conversion | |
# program by Adrian Mariano [email protected] | |
# | |
# August 2015 Version 2.13 | |
# | |
# Copyright (C) 1996, 1997, 1998, 1999, 2000, 2001, 2002, 2004, 2005, 2006 | |
# 2007, 2008, 2009, 2010, 2011, 2012, 2013, 2014, 2015 | |
# 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. | |
# | |
# Fundamental constants in this file are the 2014 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. 1995 | |
# 2. CRC Handbook of Chemistry and Physics 70th edition | |
# 3. Oxford English Dictionary | |
# 4. Websters 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.unc.edu/~rowlett/units/index.html | |
# 19. Numericana. http://www.numericana.com | |
# 20. UK history of measurement | |
# http://www.ukmetrication.com/history.htm | |
# 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 the United States: a brief history. Lewis V. Judson. | |
# 1963; rev. 1976 | |
# | |
# Thanks to Jeff Conrad for assistance in ferreting out unit definitions. | |
# | |
########################################################################### | |
# | |
# 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. | |
# | |
# I added shoe size information but I'm not convinced that it's correct. | |
# If you know anything about shoe sizes please contact me. | |
# | |
########################################################################### | |
########################################################################### | |
# | |
# 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 | |
########################################################################### | |
# # | |
# 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 | |
# | |
kg ! # Mass of the international prototype | |
kilogram kg | |
s ! # Duration of 9192631770 periods of the radiation | |
second s # corresponding to the transition between the two hyperfine | |
# levels of the ground state of the cesium-133 atom | |
m ! # Length of the path traveled by light in a vacuum | |
meter m # during 1|299792458 seconds. Originally meant to be | |
# 1e-7 of the length along a meridian from the equator | |
# to a pole. | |
A ! # The current which produces a force of 2e-7 N/m between two | |
ampere A # infinitely long wires that are 1 meter apart | |
amp ampere | |
cd ! # Luminous intensity in a given direction of a source which | |
candela cd # emits monochromatic radiation at 540e12 Hz with radiant | |
# intensity 1|683 W/steradian. (This differs from radiant | |
# intensity (W/sr) in that it is adjusted for human | |
# perceptual dependence on wavelength. The frequency of | |
# 540e12 Hz (yellow) is where human perception is most | |
# efficient.) | |
mol ! # The amount of substance of a system which contains as many | |
mole mol # elementary entities as there are atoms in 0.012 kg of | |
# carbon 12. The elementary entities must be specified and | |
# may be atoms, molecules, ions, electrons, or other | |
# particles or groups of particles. It is understood that | |
# unbound atoms of carbon 12, at rest and in the ground | |
# state, are referred to. | |
K ! # 1|273.16 of the thermodynamic temperature of the triple | |
kelvin K # point of water | |
# | |
# 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 # The angle subtended at the center of a circle by | |
# an arc equal in length to the radius of the | |
# circle | |
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 | |
# | |
# Some primitive non-SI units | |
# | |
US$ ! # The US dollar is chosen arbitrarily to be the primitive | |
# unit of money. | |
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. | |
########################################################################### | |
# # | |
# Prefixes (longer names must come first) # | |
# # | |
########################################################################### | |
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" | |
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 convention of illegally | |
mebi- 2^20 # and confusingly using metric prefixes for | |
gibi- 2^30 # powers of two, the International | |
tebi- 2^40 # Electrotechnical Commission aproved these | |
pebi- 2^50 # binary prefixes for use in 1998. If you | |
exbi- 2^60 # want to refer to "megabytes" using the | |
Ki- kibi # binary definition, use these prefixes. | |
Mi- mebi | |
Gi- gibi | |
Ti- tebi | |
Pi- pebi | |
Ei- exbi | |
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 | |
# | |
# 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 | |
# 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 Wb/A # inductance | |
H henry | |
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 | |
CURRENT ampere | |
AMOUNT mole | |
ANGLE radian | |
SOLID_ANGLE steradian | |
MONEY US$ | |
FORCE newton | |
PRESSURE FORCE / AREA | |
STRESS FORCE / AREA | |
CHARGE coulomb | |
CAPACITANCE farad | |
RESISTANCE ohm | |
CONDUCTANCE siemens | |
INDUCTANCE henry | |
FREQUENCY hertz | |
VELOCITY LENGTH / TIME | |
ACCELERATION VELOCITY / TIME | |
DENSITY MASS / VOLUME | |
LINEAR_DENSITY MASS / LENGTH | |
VISCOSITY FORCE TIME / AREA | |
KINEMATIC_VISCOSITY VISCOSITY / DENSITY | |
# | |
# 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. | |
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 | |
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 on mol/sec. | |
solarluminosity 384.6e24 W # A common yardstick for comparing the | |
# output of different stars. | |
# http://nssdc.gsfc.nasa.gov/planetary/factsheet/sunfact.html | |
# | |
# 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 0.5 pi sr | |
octant 0.5 pi sr | |
# | |
# 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". | |
# | |
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 | |
# 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 °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 °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 | |
c 2.99792458e8 m/s # speed of light in vacuum (exact) | |
light c | |
mu0 4 pi 1e-7 H/m # permeability of vacuum (exact) | |
epsilon0 1/mu0 c^2 # permittivity of vacuum (exact) | |
energy c^2 # convert mass to energy | |
e 1.6021766208e-19 C # electron charge | |
h 4.135667662e-15 eV s # Planck constant | |
hbar h / 2 pi | |
spin hbar | |
G 6.67408e-11 N m^2 / kg^2 # Newtonian gravitational constant | |
# This is the NIST 2006 value. | |
# The relative uncertainty on this | |
# is 1e-4. | |
coulombconst 1/4 pi epsilon0 # listed as "k" sometimes | |
# Physico-chemical constants | |
atomicmassunit 1.660539040e-27 kg # atomic mass unit (defined to be | |
u atomicmassunit # 1|12 of the mass of carbon 12) | |
amu atomicmassunit | |
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 | |
dalton u # Maybe this should be amu_chem? | |
avogadro grams/amu mol # size of a mole | |
N_A avogadro | |
gasconstant k N_A # molar gas constant | |
R gasconstant | |
boltzmann 1.38064852e-23 J/K # Boltzmann constant | |
k boltzmann | |
kboltzmann boltzmann | |
molarvolume mol R stdtemp / atm # Volume occupied by one mole of an | |
# ideal gas at STP. | |
loschmidt avogadro mol / molarvolume # Molecules per cubic meter of an | |
# ideal gas at STP. Loschmidt did | |
# work similar to Avogadro. | |
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. | |
wiendisplacement 2.8977729e-3 m K # Wien's Displacement Law gives the | |
# frequency at which the 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. | |
K_J90 483597.9 GHz/V # Direct measurement of the volt is difficult. Until | |
K_J 483597.8525 GHz/V # 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, which is equal to 2e/h, relates the | |
# measured frequency to the potential. Two values | |
# given, the conventional (exact) value from 1990 and | |
# the current CODATA measured value. | |
R_K90 25812.807 ohm # Measurement of the ohm also presents difficulties. | |
R_K 25812.8074555 ohm # 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. Two values given, the conventional (exact) | |
# value from 1990 and the current CODATA measured | |
# value. | |
# Various conventional values | |
gravity 9.80665 m/s^2 # std acceleration of gravity (exact) | |
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 | |
Rinfinity 10973731.568539 /m # The wavelengths of a spectral series | |
R_H 10967760 /m # 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 | |
# m_e c alpha^2 / 2 h | |
# with a loss of 4 digits | |
# of precision. | |
alpha 7.2973525664e-3 # The fine structure constant was | |
# introduced to explain fine | |
# structure visible in spectral | |
# lines. It can be computed from | |
# mu0 c e^2 / 2 h | |
# with a loss of 3 digits precision | |
# and loss of precision in derived | |
# values which use alpha. | |
bohrradius alpha / 4 pi Rinfinity | |
prout 185.5 keV # nuclear binding energy equal to 1|12 | |
# binding energy of the deuteron | |
# Planck constants | |
planckmass 2.17651e-8 kg # sqrt(hbar c / G) | |
m_P planckmass | |
plancktime hbar / planckmass c^2 | |
t_P plancktime | |
plancklength plancktime c | |
l_P plancklength | |
# Particle radius | |
electronradius (1/4 pi epsilon0) e^2 / electronmass c^2 # Classical | |
deuteronchargeradius 2.1413e-15 m | |
protonchargeradius 0.8751e-15 m | |
# Masses of elementary particles | |
electronmass 5.48579909070e-4 u | |
m_e electronmass | |
protonmass 1.007276466879 u | |
m_p protonmass | |
neutronmass 1.00866491588 u | |
m_n neutronmass | |
muonmass 0.1134289257 u | |
m_mu muonmass | |
deuteronmass 2.013553212745 u | |
m_d deuteronmass | |
alphaparticlemass 4.001506179127 u | |
m_alpha alphaparticlemass | |
taumass 1.90749 u | |
m_tau taumass | |
tritonmass 3.01550071632 u | |
m_t tritonmass | |
helionmass 3.01493224673 u | |
m_h helionmass | |
# 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 | |
# Magnetic moments | |
bohrmagneton e hbar / 2 electronmass | |
mu_B bohrmagneton | |
nuclearmagneton e hbar / 2 protonmass | |
mu_N nuclearmagneton | |
mu_mu -4.49044826e-26 J/T # Muon magnetic moment | |
mu_p 1.4106067873e-26 J/T # Proton magnetic moment | |
mu_e -928.4764620e-26 J/T # Electron magnetic moment | |
mu_n -0.96623650e-26 J/T # Neutron magnetic moment | |
mu_d 0.4330735040e-26 J/T # Deuteron magnetic moment | |
mu_t 1.504609503e-26 J/T # Triton magnetic moment | |
mu_h -1.074617522e-26 J/T # 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 # These units, both named after Evangelista | |
tor Pa # Torricelli, should not be confused. The | |
inHg inch Hg # torr is very close to the mm 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 | |
# paralax theta will be about | |
# (arcsec/theta) parsecs from the | |
# sun (using the approximation | |
# that tan(theta) = theta). | |
rydberg h c Rinfinity # Rydberg energy | |
crith 0.089885 gram # The crith is the mass of one | |
# liter of hydrogen at standard | |
# temperature and pressure. | |
amagatvolume molarvolume | |
amagat mol/amagatvolume # Used to measure gas densities | |
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 cminv | |
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 units derived from the abampere | |
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 | |
biot aA # alternative name for abamp | |
Bi biot | |
abcoulomb abamp sec | |
abcoul abcoulomb | |
abfarad abampere sec / abvolt | |
abhenry abvolt sec / abamp | |
abvolt dyne cm / abamp sec | |
abohm abvolt / abamp | |
abmho /abohm | |
gauss abvolt sec / cm^2 | |
Gs gauss | |
maxwell abvolt sec # Also called the "line" | |
Mx maxwell | |
oersted gauss / mu0 | |
Oe oersted | |
gilbert gauss cm / mu0 | |
Gb gilbert | |
Gi gilbert | |
unitpole 4 pi maxwell | |
emu erg/gauss # "electro-magnetic unit", a measure of | |
# magnetic moment, often used as emu/cm^3 | |
# to specify magnetic moment density. | |
# Gaussian system: electromagnetic units derived from statampere. | |
# | |
# Note that the Gaussian units are often used in such a way that Coulomb's law | |
# has the form F= q1 * q2 / r^2. The constant 1|4*pi*epsilon0 is incorporated | |
# into the units. From this, we can get the relation force=charge^2/dist^2. | |
# This means that the simplification esu^2 = dyne cm^2 can be used to simplify | |
# units in the Gaussian system, with the curious result that capacitance can be | |
# measured in cm, resistance in sec/cm, and inductance in sec^2/cm. These | |
# units are given the names statfarad, statohm and stathenry below. | |
statampere 10 A cm / s c | |
statamp statampere | |
statvolt dyne cm / statamp sec | |
statcoulomb statamp s | |
esu statcoulomb | |
statcoul statcoulomb | |
statfarad statamp sec / statvolt | |
cmcapacitance statfarad | |
stathenry statvolt sec / statamp | |
statohm statvolt / statamp | |
statmho /statohm | |
statmaxwell statvolt sec | |
franklin statcoulomb | |
debye 1e-18 statcoul cm # unit of electrical dipole moment | |
helmholtz debye/angstrom^2 # Dipole moment per area | |
jar 1000 statfarad # approx capacitance of Leyden jar | |
# | |
# 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 | |
# 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 a Faraday constant which is | |
# equal to N_A e and hence 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. | |
# | |
# http://www.ndt-ed.org/GeneralResources/IACS/IACS.htm. | |
# | |
# 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 is also standarized 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 ([email protected]) | |
# | |
# 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 the | |
# 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 the | |
# earth. | |
siderealyear 365.256360417 day # The time for the 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 | |
# the 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 | |
# preceeding one because the | |
# saros is not an even number of | |
# days. After 3 saros, an | |
# eclipse will occur at | |
# approximately the same place. | |
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 the | |
# earth to make one rotation | |
# relative to the stars. The | |
# more usual solar day is the | |
# time required to make a | |
# rotation relative to the sun. | |
# Because the earth moves in its | |
# orbit, it has to turn a bit | |
# extra to face the sun again, | |
# hence the solar day is slightly | |
# longer. | |
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 revolve a bit extra to | |
# get into 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 | |
julianyear 365.25 day | |
gregorianyear 365.2425 day | |
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 Hewbrew 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. | |
# Sidereal days | |
mercuryday 58.6462 day | |
venusday 243.01 day # retrograde | |
earthday siderealday | |
marsday 1.02595675 day | |
jupiterday 0.41354 day | |
saturnday 0.4375 day | |
uranusday 0.65 day # retrograde | |
neptuneday 0.768 day | |
plutoday 6.3867 day | |
# Sidereal years from http://ssd.jpl.nasa.gov/phys_props_planets.html. Data | |
# was updated in May 2001 based on the 1992 Explanatory Supplement to the | |
# Astronomical Almanac and the mean longitude rates. Apparently the table of | |
# years in that reference is incorrect. | |
mercuryyear 0.2408467 julianyear | |
venusyear 0.61519726 julianyear | |
earthyear siderealyear | |
marsyear 1.8808476 julianyear | |
jupiteryear 11.862615 julianyear | |
saturnyear 29.447498 julianyear | |
uranusyear 84.016846 julianyear | |
neptuneyear 164.79132 julianyear | |
plutoyear 247.92065 julianyear | |
# Objects on the 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. These values are the 1996 values given by the International | |
# Earth Rotation Service (IERS) whose reference documents can be found at | |
# http://maia.usno.navy.mil/ | |
earthflattening 1|298.25642 | |
earthradius_equatorial 6378136.49 m | |
earthradius_polar (-earthflattening+1) 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 the 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 the 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 the 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. | |
# Many values below are from http://ssd.jpl.nasa.gov/?constants | |
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.) | |
solarmass 1.9891e30 kg | |
sunmass solarmass | |
sundist 1.0000010178 au # mean earth-sun distance | |
moondist 3.844e8 m # mean earth-moon distance | |
sundist_near 1.471e11 m # earth-sun distance at perihelion | |
sundist_far 1.521e11 m # earth-sun distance at aphelion | |
# The following are masses for planetary systems, not just the planet itself. | |
# The comments give the uncertainty in the denominators. As noted above, | |
# masses are given relative to the solarmass because this is more accurate. | |
# The conversion to SI is uncertain because of uncertainty in G, the | |
# gravitational constant. | |
# | |
# Values are from http://ssd.jpl.nasa.gov/astro_constants.html | |
mercurymass solarmass / 6023600 # 250 | |
venusmass solarmass / 408523.71 # 0.06 | |
earthmoonmass solarmass / 328900.56 # 0.02 | |
marsmass solarmass / 3098708 # 9 | |
jupitermass solarmass / 1047.3486 # 0.0008 | |
saturnmass solarmass / 3497.898 # 0.018 | |
uranusmass solarmass / 22902.98 # 0.03 | |
neptunemass solarmass / 19412.24 # 0.04 | |
plutomass solarmass / 1.35e8 # 0.07e8 | |
moonearthmassratio 0.012300034 # uncertainty 3 x 10-9 | |
earthmass earthmoonmass / ( 1 + moonearthmassratio) | |
moonmass moonearthmassratio earthmass | |
# These are the old values for the planetary masses. They may give | |
# the masses of the planets alone. | |
oldmercurymass 0.33022e24 kg | |
oldvenusmass 4.8690e24 kg | |
oldmarsmass 0.64191e24 kg | |
oldjupitermass 1898.8e24 kg | |
oldsaturnmass 568.5e24 kg | |
olduranusmass 86.625e24 kg | |
oldneptunemass 102.78e24 kg | |
oldplutomass 0.015e24 kg | |
# Mean radius from http://ssd.jpl.nsaa.gov/phys_props_planets.html which in | |
# turn cites Global Earth Physics by CF Yoder, 1995. | |
mercuryradius 2440 km | |
venusradius 6051.84 km | |
earthradius 6371.01 km | |
marsradius 3389.92 km | |
jupiterradius 69911 km | |
saturnradius 58232 km | |
uranusradius 25362 km | |
neptuneradius 24624 km | |
plutoradius 1151 km | |
moongravity 1.62 m/s^2 | |
# | |
# The Hartree system of atomic units, derived from fundamental units | |
# of mass (of electron), action (planck's constant), charge, and | |
# the coulomb constant. | |
# Fundamental units | |
atomicmass electronmass | |
atomiccharge e | |
atomicaction hbar | |
# derived units (Warning: accuracy is lost from deriving them this way) | |
atomiclength bohrradius | |
atomictime hbar^3/coulombconst^2 atomicmass e^4 # Period of first | |
# bohr orbit | |
atomicvelocity atomiclength / atomictime | |
atomicenergy hbar / atomictime | |
hartree atomicenergy | |
# | |
# 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." The US continues to define the statute | |
# mile, furlong, chain, rod, link, and fathom in terms of the US survey | |
# foot. | |
# Sources: | |
# NIST Special Publication 447, Sects. 5, 7, and 8. | |
# NIST Handbook 44, 2011 ed., Appendix C. | |
# Canadian Journal of Physics, 1959, 37:(1) 84, 10.1139/p59-014. | |
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 | |
inch 2.54 cm | |
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 5.5 yard | |
perch rod | |
furlong 40 rod # From "furrow long" | |
statutemile mile | |
league 3 mile # Intended to be an an hour's walk | |
# surveyor's measure | |
surveyorschain 66 surveyft | |
surveychain surveyorschain | |
surveyorspole 1|4 surveyorschain | |
surveyorslink 1|100 surveyorschain | |
chain 66 ft | |
link 1|100 chain | |
ch chain | |
USacre 10 surveychain^2 | |
intacre 10 chain^2 # Acre based on international ft | |
intacrefoot acre foot | |
USacrefoot USacre surveyfoot | |
acrefoot intacrefoot | |
acre intacre | |
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?, www.metricationmatters.com; | |
# 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 the 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. | |
cable 1|10 nauticalmile | |
intcable cable # international cable | |
cablelength cable | |
UScable 100 USfathom | |
navycablelength 720 USft # used for depth in water | |
marineleague 3 nauticalmile | |
geographicalmile brnauticalmile | |
knot nauticalmile / hr | |
click km # US military slang | |
klick click | |
# Avoirdupois weight | |
pound 0.45359237 kg # The one normally used | |
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 | |
# <[email protected]> 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 | |
wineglass 4 usfloz | |
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 | |
salmanazar 6 magnum | |
balthazar 8 magnum | |
nebuchadnezzar 10 magnum | |
# | |
# Water is "hard" if it contains various minerals, expecially 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 | |
brcable 1|10 brnauticalmile # nautical mile. | |
admiraltymile brnauticalmile | |
admiraltyknot brknot | |
admiraltycable brcable | |
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] | |
pole 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 | |
metre meter | |
gramme gram | |
litre liter | |
dioptre diopter | |
aluminium aluminum | |
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 smooth lengths. These | |
# markings have been maintained on the bridge | |
# since then and repainted by subsequent | |
# incoming fraternity members. During a | |
# bridge rennovation the new sidewalk was | |
# scored every smooth rather than at the | |
# customary 6 ft spacing. | |
# | |
# 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 requird 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 | |
# | |
# 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 analyzis. 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 simplfied version of this equation where the temperature of boiling | |
# water has been fixed at 100 degrees Celcius 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 Celcius 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) | |
# | |
# 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 | |
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 | |
# | |
# Other units of work, energy, power, etc | |
# | |
ENERGY joule | |
WORK joule | |
# Calories: energy to raise a gram of water one degree celsius | |
cal_IT 4.1868 J # International Table calorie | |
cal_th 4.184 J # Thermochemical calorie | |
cal_fifteen 4.18580 J # Energy to go from 14.5 to 15.5 degC | |
cal_twenty 4.18190 J # Energy to go from 19.5 to 20.5 degC | |
cal_mean 4.19002 J # 1|100 energy to go from 0 to 100 degC | |
calorie cal_IT | |
cal calorie | |
calorie_IT cal_IT | |
thermcalorie cal_th | |
calorie_th thermcalorie | |
Calorie kilocalorie # the food Calorie | |
thermie 1e6 cal_fifteen # 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 cal lb degF / gram K # international table BTU | |
britishthermalunit btu | |
btu_IT btu | |
btu_th cal_th lb degF / gram K | |
btu_mean cal_mean lb degF / gram K | |
quad quadrillion btu | |
ECtherm 1.05506e8 J # Exact definition, close to 1e5 btu | |
UStherm 1.054804e8 J # Exact definition | |
therm UStherm | |
# Water latent heat (from Wikipedia) | |
water_fusion_heat 79.8 calorie/g | |
water_vaporization_heat 1160 J/g | |
# Specific heat capacities of various substances | |
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://bioenergy.ornl.gov/papers/misc/energy_conv.html | |
# E2. http://www.aps.org/policy/reports/popa-reports/energy/units.cfm | |
# E3. 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,E2] | |
# 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 [E2]. 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 | |
# 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 | |
POWER watt | |
# "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 745.70 W | |
donkeypower 250 W | |
chevalvapeur metrichorsepower | |
# | |
# Heat Transfer | |
# | |
# Thermal conductivity, K, measures the rate of heat transfer across | |
# a material. The heat transfered 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. | |
# 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. | |
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 | |
# 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. | |
dBSPL(x) units=[1;Pa] range=(0,) dB(0.5 x) 20 microPa ; \ | |
~dB(dBSPL^2 / (20 microPa)^2) # pressure | |
dBSIL(x) units=[1;W/m^2] range=(0,) dB(x) 1e-12 W/m^2; \ | |
~dB(dBSIL / (1e-12 W/m^2)) # intensity | |
dBSWL(x) units=[1;W] range=(0,) dB(x) 1e-12 W; ~dB(dBSWL/1e-12 W) | |
# 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_fifteen# Used in refrigeration engineering. | |
tnt 1e9 cal_th / ton# So you can write tons tnt. This | |
# is a defined, not measured, value. | |
airwatt 8.5 (ft^3/min) inH2O # Measure of vacuum power as | |
# pressure times air flow. | |
# | |
# 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 # François 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 values: KiB, MiB, | |
# and GiB. | |
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 | |
# | |
# 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 | |
# quanity 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 | |
venezuelanbolivarfuerte venezuelabolivar | |
bolivarfuerte bolivar # The currency was revalued by | |
oldbolivar 1|1000 bolivar # a factor of 1000. | |
peseta spainpeseta | |
rand southafricarand | |
escudo portugalescudo | |
guilder netherlandsguilder | |
hollandguilder netherlandsguilder | |
peso mexicopeso | |
yen japanyen | |
lira italylira | |
rupee indiarupee | |
drachma greecedrachma | |
franc francefranc | |
markka finlandmarkka | |
britainpound unitedkingdompound | |
greatbritainpound unitedkingdompound | |
unitedkingdompound ukpound | |
poundsterling britainpound | |
yuan chinayuan | |
# Some European currencies have permanent fixed exchange rates with | |
# the Euro. These rates were taken from the EC's web site: | |
# http://ec.europa.eu/economy_finance/euro/adoption/conversion/index_en.htm | |
austriaschilling 1|13.7603 euro | |
belgiumfranc 1|40.3399 euro | |
estoniakroon 1|15.6466 euro # Equal to 1|8 germanymark | |
finlandmarkka 1|5.94573 euro | |
francefranc 1|6.55957 euro | |
germanymark 1|1.95583 euro | |
greecedrachma 1|340.75 euro | |
irelandpunt 1|0.787564 euro | |
italylira 1|1936.27 euro | |
luxembourgfranc 1|40.3399 euro | |
netherlandsguilder 1|2.20371 euro | |
portugalescudo 1|200.482 euro | |
spainpeseta 1|166.386 euro | |
cypruspound 1|0.585274 euro | |
maltalira 1|0.429300 euro | |
sloveniatolar 1|239.640 euro | |
slovakiakoruna 1|30.1260 euro | |
UKP GBP # Not an ISO code, but looks like one, and | |
# sometimes used on usenet. | |
VEB 1|1000 VEF # old venezuelan bolivar | |
!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 | |
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 | |
USdollarmass 8.1 grams | |
# 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 | |
# | |
# 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 | |
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://www.state.nv.us/cnr/ndwp/dict-1/waterwds.htm.) | |
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 | |
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 \ | |
+ 2 ppm 16.04303 \ | |
+ 1.14 ppm 83.80 \ | |
+ 0.55 ppm 2.01594 \ | |
+ 0.087 ppm 131.30 | |
# 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 | |
# | |
# 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. | |
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 | |
# 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 | |
# | |
# Screw sizes | |
# | |
# In the USA, screw diameters are reported using a gauge number. | |
# Metric 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. | |
# | |
# http://www.uama.org/Abrasives101/101Standards.html | |
# | |
# 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 | |
# http://www.klingspor.com/gritgradingsystems.htm | |
# | |
# 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 | |
# http://dmtsharp.com/products/colorcode.htm | |
# | |
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 | |
# | |
# 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 | |
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 | |
# | |
becquerel /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 | |
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. The Standard Atomic | |
# Weights apply to the elements as they occur naturally on earth. Elements | |
# which do not occur naturally or which occur with wide isotopic variability do | |
# not have Standard Atomic Weights. For these elements, the atomic weight is | |
# based on the longest lived isotope, as marked in the comments. In some | |
# cases, the comment for these entries also gives a number which is an atomic | |
# weight for a different isotope that may be of more interest than the longest | |
# lived isotope. | |
# | |
actinium 227.0278 | |
aluminum 26.981539 | |
americium 243.0614 # Longest lived. 241.06 | |
antimony 121.760 | |
argon 39.948 | |
arsenic 74.92159 | |
astatine 209.9871 # Longest lived | |
barium 137.327 | |
berkelium 247.0703 # Longest lived. 249.08 | |
beryllium 9.012182 | |
bismuth 208.98037 | |
boron 10.811 | |
bromine 79.904 | |
cadmium 112.411 | |
calcium 40.078 | |
californium 251.0796 # Longest lived. 252.08 | |
carbon 12.011 | |
cerium 140.115 | |
cesium 132.90543 | |
chlorine 35.4527 | |
chromium 51.9961 | |
cobalt 58.93320 | |
copper 63.546 | |
curium 247.0703 | |
deuterium 2.0141017778 | |
dysprosium 162.50 | |
einsteinium 252.083 # Longest lived | |
erbium 167.26 | |
europium 151.965 | |
fermium 257.0951 # Longest lived | |
fluorine 18.9984032 | |
francium 223.0197 # Longest lived | |
gadolinium 157.25 | |
gallium 69.723 | |
germanium 72.61 | |
gold 196.96654 | |
hafnium 178.49 | |
helium 4.002602 | |
holmium 164.93032 | |
hydrogen 1.00794 | |
indium 114.818 | |
iodine 126.90447 | |
iridium 192.217 | |
iron 55.845 | |
krypton 83.80 | |
lanthanum 138.9055 | |
lawrencium 262.11 # Longest lived | |
lead 207.2 | |
lithium 6.941 | |
lutetium 174.967 | |
magnesium 24.3050 | |
manganese 54.93805 | |
mendelevium 258.10 # Longest lived | |
mercury 200.59 | |
molybdenum 95.94 | |
neodymium 144.24 | |
neon 20.1797 | |
neptunium 237.0482 | |
nickel 58.6934 | |
niobium 92.90638 | |
nitrogen 14.00674 | |
nobelium 259.1009 # Longest lived | |
osmium 190.23 | |
oxygen 15.9994 | |
palladium 106.42 | |
phosphorus 30.973762 | |
platinum 195.08 | |
plutonium 244.0642 # Longest lived. 239.05 | |
polonium 208.9824 # Longest lived. 209.98 | |
potassium 39.0983 | |
praseodymium 140.90765 | |
promethium 144.9127 # Longest lived. 146.92 | |
protactinium 231.03588 | |
radium 226.0254 | |
radon 222.0176 # Longest lived | |
rhenium 186.207 | |
rhodium 102.90550 | |
rubidium 85.4678 | |
ruthenium 101.07 | |
samarium 150.36 | |
scandium 44.955910 | |
selenium 78.96 | |
silicon 28.0855 | |
silver 107.8682 | |
sodium 22.989768 | |
strontium 87.62 | |
sulfur 32.066 | |
tantalum 180.9479 | |
technetium 97.9072 # Longest lived. 98.906 | |
tellurium 127.60 | |
terbium 158.92534 | |
thallium 204.3833 | |
thorium 232.0381 | |
thullium 168.93421 | |
tin 118.710 | |
titanium 47.867 | |
tungsten 183.84 | |
uranium 238.0289 | |
vanadium 50.9415 | |
xenon 131.29 | |
ytterbium 173.04 | |
yttrium 88.90585 | |
zinc 65.39 | |
zirconium 91.224 | |
# Average molecular weight of air | |
# | |
# The atmospheric composition listed is from NASA Earth Fact Sheet (accessed | |
# 28 August 2015) | |
# http://nssdc.gsfc.nasa.gov/planetary/factsheet/earthfact.html | |
# Numbers do not add up to exactly 100% due to roundoff and uncertainty Water | |
# is highly variable, typically makes up about 1% | |
air 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 | |
# | |
# 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 | |
Tm Tim # Abbreviations | |
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 | |
# http://www.scinet.co.jp/sci/sanwa/kakizaki-essay54.html | |
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 | |
# | |
# http://wyoming.hp.infoseek.co.jp/zatugaku/zamoney.html | |
# 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 pronounciation 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 | |
# | |
# 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 Brittanica 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 | |
!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 | |
!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 | |
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 | |
¢ cent | |
£ britainpound | |
¥ japanyen | |
€ euro | |
₩ southkoreawon | |
₪ israelnewshekel | |
₤ lira | |
₨ rupee | |
Ω ohm # Ohm symbol U+2126 | |
Ω ohm # Greek capital omega U+03A9 | |
℧ mho | |
ʒ dram # U+0292 | |
℈ scruple | |
℥ ounce | |
℔ lb | |
ℎ h | |
ℏ hbar | |
‰ 1|1000 | |
‱ 1|10000 | |
′ ' # U+2032 | |
″ " # U+2033 | |
# | |
# 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 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. | |
# | |
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