Table 7.5 — EUs whose label begins with A-L
Label | Symbol | Quantity | Concept definition | EQ label | Code | Reference | Supplemental references |
AMP_PER_METRE | A/m | lineic electric current (linear electric current density) | The electric current in a conducting sheet divided by the width of the sheet. | LINEIC_ELECTRIC- _CURRENT |
1 | ISO 31-5:1992, 5-16.a | |
magnetic field strength | A vector quantity, the rotation (curl) of which is equal to the sum of the electric current density and the time derivative of the electric flux density. | ISO 31-5:1992, 5-17.a | |||||
magnetization | The extent to which a magnetic material is magnetized, given by the magnetic moment per unit volume. | ISO 31-5:1992, 5-28.a | |||||
AMP_PER_SQ_M_KELVIN_SQD | A/(m2 · K2) | thermionic emission current density | A vector quantity, the integral of whose normal component over a heated surface is equal to the net number of particles (electrons or ions) emitted from that surface, as a function of the thermodynamic temperature of that surface. | THERMION_EMISSION- _CUR_DENS |
2 | ISO 31-13:1992, 13-27.a | |
AMP_PER_SQ_METRE | A/m2 | areic electric current (electric current density) | A vector quantity, the integral of whose normal component over a given surface is equal to the electric current flowing through that surface. | AREIC_ELECTRIC- _CURRENT |
3 | ISO 31-5:1992, 5-15.a | |
AMPERE | A | current linkage | The net electric conduction current through a closed loop. | ELECTRIC_CURRENT | 4 | ISO 31-5:1992, 5-18.a | |
electric current | That constant electric current which, if maintained in two straight parallel conductors of infinite length, of negligible circular cross-section, and placed 1 metre apart in vacuum, would produce between these conductors a force equal to 2 x 10-7 newton per metre of length. SI base unit. |
ISO 31-0:1992, Table 1 | ISO 31-5:1992, 5-1.a | ||||
magnetic potential difference | On a given path, the magnetic potential difference between point 1 and point 2 is the line integral from 1 to 2 of the magnetic field strength along that path. | ISO 31-5:1992, 5-18.a | |||||
magnetomotive force | The work required to carry a magnetic pole of unit strength once around a magnetic circuit. | ISO 31-5:1992, 5-18.a | |||||
BECQUEREL | Bq | activity of a radio nuclide | The average number of spontaneous nuclear transitions from a particular energy state occurring in an amount of a radionuclide in a small time interval, divided by that interval. 1 Bq = 1 s-1. |
RADIONUCLIDE- _ACTIVITY |
10 | ISO 31-0:1992, Table 3 | ISO 31-9:1992, 9-33.a; ISO 31-10:1992, 10-49.a |
BECQUEREL_PER_CUBIC_METRE | Bq/m3 | volumic activity (activity concentration) | Activity of a radionuclide divided by the total volume of the sample. | VOLUMIC_ACTIVITY | 11 | ISO 31-9:1992, 9-35.a | |
BECQUEREL_PER_KG | Bq/kg | massic activity (specific activity) | Activity of a radionuclide divided by the total mass of the sample. | MASSIC_ACTIVITY | 12 | ISO 31-9:1992, 9-34.a | |
BEL | B | field quantity ratio (level difference) | Twice the common logarithm of a field quantity ratio. 1 B is the level of a field quantity when 2 lg (F/F0) = 1 where F and F0 represent two amplitudes of the same kind, F0 being a reference amplitude. 1 B = (1/2) ln 10 Np = 1,151 293 Np (approximately). |
FIELD_OR_POWER- _LEVEL_DIFF |
13 | ISO 31-2:1992, 2-9.b | |
power quantity ratio (level difference) | The common logarithm of a power quantity ratio. 1 B is the level of a power quantity when lg (P/P0) = 1 where P and P0 represent two powers, P0 being a reference power. |
ISO 31-2:1992, 2-10.b | |||||
sound power level | LW = 1/2 ln (P/P0) = 1/2 ln 10·lg (P/P0) where P is the root-mean-square of the sound power and the reference power p0 = 1 x 10-12 W. | ISO 31-7:1992, 7-22.a | |||||
sound pressure level | Lp = ln (p/p0) = ln 10·lg (p/p0) where p is the root-mean-square value of the sound pressure and the reference pressure p0 = 20 μPa. | ISO 31-7:1992, 7-21.a | |||||
CANDELA | cd | luminous intensity | The luminous intensity, in a given direction, of a source that emits monochromatic radiation of a frequency 540 x 1012 Hertz, and that has a radiant intensity in that direction of 1 / 683 watt per steradian. SI base unit. |
LUMINANCE_INTENSITY | 14 | ISO 31-0:1992, Table 1 | ISO 31-6:1992, 6-29.a |
CD_PER_SQ_METRE | cd/m2 | luminance | At a point on a surface and in a given direction, the luminous intensity of an element of the surface, divided by the area of the orthogonal projection of this element on a plane perpendicular to the given direction. | LUMINANCE | 15 | ISO 31-6:1992, 6-32.a | |
COULOMB | C | electric charge (quantity of electricity) | The integral of electric current over time. 1 C = 1 s · A. |
ELECTRIC_CHARGE | 16 | ISO 31-0:1992, Table 2 | ISO 31-5:1992, 5-2.a |
electric flux | Across a surface element, the scalar product of the electric flux density and the surface element. | ISO 31-5:1992, 5-8.a | |||||
elementary charge | The electric charge of a proton. | ISO 31-9:1992, 9-6.a | ISO 31-8:1992, 8-43.a | ||||
COULOMB_METRE | C · m | electric dipole moment | A vector quantity, the vector product of which with the electric field strength of a homogenous field is equal to the torque. 1 C · m = 1 m · s · A. |
ELECTRIC_DIPOLE- _MOMENT |
17 | ISO 31-5:1992, 5-14.a | |
electric dipole moment of a molecule | A vector quantity, the vector product of which with the electric field strength is equal to the torque. | ISO 31-8:1992, 8-32.a | |||||
COULOMB_METRE_SQD_PER_VOLT | C · m2/V | electric polarizability of a molecule | The induced electric dipole moment divided by electric field strength. 1 C · m2/V = 1 (s4 · A2)/kg. |
ELECTRIC- _POLARIZABILITY |
18 | ISO 31-8:1992, 8-33.a | |
COULOMB_PER_CUBIC_M | C/m3 | volume charge (volume density of charge, electric charge density) | The charge divided by volume. 1 C/m3 = 1 (s · A)/m3. |
VOLUME_DENSITY- _CHARGE |
19 | ISO 31-5:1992, 5-3.a | |
COULOMB_PER_KG | C/kg | exposure of ionizing radiation | The total electric charge of the ions of the same sign produced when all the electrons (negative and positive) liberated by photons in an element of air are stopped in air, divided by the mass of that element. 1 C/kg = 1 (s · A)/kg. |
EXPOSURE | 20 | ISO 31-10:1992, 10-58.a | |
COULOMB_PER_KG_SEC | C/(kg · s) | exposure rate of ionizing radiation | The exposure (ionizing radiation) divided by time. 1 C/(kg · s) = 1 A/kg. |
EXPOSURE_RATE | 21 | ISO 31-10:1992, 10-59.a | |
COULOMB_PER_MOLE | C/mol | molar charge | The charge carried per amount of substance. 1 C/mol = 1 (s · A)/mol. |
MOLAR_CHARGE | 22 | ISO 31-8:1992, 8-45.a | |
COULOMB_PER_SQ_M | C/m2 | areic charge (surface density of charge) | The charge divided by surface area. 1 C/m2 = 1 (s · A)/m2. |
SURFACE_DENSITY- _CHARGE |
23 | ISO 31-5:1992, 5-4.a | |
electric flux density | A vector quantity, the divergence of which is equal to the volumic charge. | ISO 31-5:1992, 5-7.a | |||||
electric polarization | A vector quantity equal to the electric dipole moment per unit volume of a material. | ISO 31-5:1992, 5-13.a | |||||
CUBIC_M_PER_CUBIC_M | m3/m3 | volume fraction (of B) | The volume of B divided by the volume of the mixture. 1 m3/m3 = 1. |
VOLUME_FRACTION | 24 | ISO 31-8:1992, 8-15.a | ISO 31-0:1992, 2.3.3 |
CUBIC_METRE | m3 | section modulus | The section modulus of a plane area (section) about an axis in its plane is the second moment of area divided by the distance from the axis to the most remote point of the area. | VOLUME | 25 | ISO 31-3:1992, 3-21.a | |
volume | The product of length, width and height. | ISO 31-1:1992, 1-6.a | |||||
CUBIC_METRE_PER_COULOMB | m3/C | reciprocal volumic charge (reciprocal charge density) | The volume divided by the charge. | RECIPROCAL_VOLUMIC- _CHARGE |
26 | ISO 31-13:1992, 13-20.a | |
CUBIC_METRE_PER_KG | m3/kg | specific volume | The volume divided by mass. | SPECIFIC_VOLUME | 27 | ISO 31-3:1992, 3-4.a | |
CUBIC_METRE_PER_MOLE | m3/mol | molar volume | The volume divided by the amount of substance. | MOLAR_VOLUME | 28 | ISO 31-8:1992, 8-6.a | |
CUBIC_METRE_PER_SEC | m3/s | recombination coefficient | The coefficient in the law of recombination. | VOLUME_FLOW_RATE | 29 | ISO 31-10:1992, 10-28.a | |
volume flow rate | The volume of matter which crosses a given surface, divided by time. | ISO 31-3:1992, 3-30.a | ISO 31-7:1992, 7-13.a | ||||
DAY | d | time | 1 d = 24 h = 86 400 s (exactly). | TIME | 31 | ISO 31-0:1992, Table 4 | ISO 31-1:1992, 1-7.d |
DB | dB | field quantity ratio (level difference) | A dimensionless quantity used to describe a comparison of field levels. 1 dB = 10-1 B (exactly) = 1,151 293 x 10-1Np (approximately). |
FIELD_OR_POWER- _LEVEL_DIFF |
32 | ISO 31-2:1992, 2-9.a (remarks) | |
power quantity ratio (level difference) | A dimensionless quantity used to describe a comparison of power levels. 1 dB = 10-1 B (exactly) = 1,151 293 x 10-1Np (approximately). |
ISO 31-2:1992, 2-10.a (remarks) | ISO 1000:1992, Annex A, 7-21 | ||||
DB_PER_METRE | dB/m | power ratio (level difference) gradient | The rate of power ratio change as a function of distance. | POWER_LEVEL_DIFF- _LEN_GRADIENT |
33 | ISO 31-0:1992, 2.3.2.2 (derived) | |
DB_PER_METRE_KHZ | dB/(m · kHz) | power ratio (level difference) distance and frequency gradient | The rate of power ratio change as a function of distance and spectral frequency. | POWER_LEVEL_DIFF- _LEN_FREQ |
34 | ISO 31-0:1992, 2.3.2.2 (derived) | |
DB_PER_OCTAVE | none | power ratio (level difference) frequency gradient | The rate of power ratio change as a function of spectral frequency octave. | POWER_LEVEL_DIFF- _FREQ_GRADIENT |
35 | ISO 31-0:1992, 2.3.2.2 (derived) | |
DB_PER_SQ_METRE | dB/m2 | areic power ratio (level difference) | The power level divided by area. | AREIC_POWER_LEVEL- _DIFF |
36 | ISO 31-0:1992, 2.3.2.2 (derived) | |
DB_PER_SQ_METRE_KHZ | dB/(m2 · kHz) | gradient of power ratio (level difference) distance and frequency gradient | The rate of change of power ratio change as a function of distance and spectral frequency. | GRAD_POWER_LEVEL- _DIFF_LEN_FREQ |
37 | ISO 31-0:1992, 2.3.2.2 (derived) | |
DB_REF_ONE_MICROPASCAL | dB (re 1 μPa) | pressure power quantity ratio (level) | 1 dB (re 1 μPa) is the level of a pressure power quantity when lg (P/P0) = 0,1 where P and P0 represent two pressure powers, P0 being a reference power of 1 μPa. | PRESSURE_POWER_LEVEL | 38 | ISO 31-0:1992, 2.3.2.2 (derived) | |
DECAY_RATE | %/min | decay constant (disintegration constant) | Probability of decay of an active species in a small time interval, divided by that interval. 1 %/min = 1 / 6 x 10-3 1/s (exactly). |
RATE | 39 | ISO 31-9:1992, 9-36.a | ISO 31-0:1992, 2.3.2.3 |
DEGREE_ARC | º | Bragg angle | The angle between an incident X-ray beam and a set of crystal planes for which the secondary radiation displays maximum intensity as a result of constructive interference. | PLANE_ANGLE | 40 | ISO 31-13:1992, 13-4.b | |
plane angle | The angle between two half-lines terminating at the same point is defined as the ratio of the length of the included arc of the circle (with its centre at that point) to the radius of that circle. 1º = (π / 180) rad (exactly). |
ISO 31-0:1992, Table 4 | ISO 31-1:1992, 1-1.b | ||||
DEGREE_C | ºC | thermodynamic temperature | A special name for the kelvin for use in stating values of Celsius temperature. t = T - T0 where T0 = 273,15 K (exactly). |
THERMO_TEMPERATURE | 41 | ISO 31-0:1992, Table 2 | ISO 31-4:1992, 4-2.a |
DEGREE_C_PER_HOUR | ºC/h | thermodynamic temperature change rate | The thermodynamic temperature change over an interval of time, divided by that time. 1 ºC/h = 1 / 3,6 x 10-3 K/s (exactly). |
THERMO_TEMP_CHANGE- _RATE |
42 | ISO 31-0:1992, 2.3.2.2 and 2.3.4 (derived) | |
DEGREE_C_PER_METRE | ºC/m | lineic thermodynamic temperature gradient | The thermodynamic temperature change over a distance, divided by that distance. 1 ºC/m = 1 K/m (exactly). |
LINEIC_THERMO_TEMP- _GRADIENT |
43 | ISO 31-0:1992, 2.3.2.2 (derived) | |
DEGREE_C_PER_SEC | ºC/s | thermodynamic temperature change rate | The thermodynamic temperature change over an interval of time, divided by that time. 1 ºC/s = 1 K/s (exactly). |
THERMO_TEMP_CHANGE- _RATE |
44 | ISO 31-0:1992, 2.3.2.2 (derived) | |
ELECTRONVOLT | eV | alpha disintegration energy | The sum of the kinetic energy of the alpha particle produced in the disintegration process and the recoil energy of the product atom in the reference frame in which the emitting nucleus is at rest before its disintegration. | ENERGY | 45 | ISO 31-9:1992, 9-38.b | |
average energy loss per ion pair formed (average energy loss per elementary charge of the same sign produced) | The initial kinetic energy of an ionizing charged particle, divided by the total ionization produced by that particle. | ISO 31-10:1992, 10-25.b | |||||
beta disintegration energy | Sum of the maximum beta particle energy and the recoil energy of the atom produced in the reference frame in which the emitting nucleus is at rest before its disintegration. | ISO 31-9:1992, 9-40.b | |||||
electron affinity | The energy difference between an electron at rest at infinity and an electron at the lowest level of the conduction band in an insulator or semiconductor. | ISO 31-13:1992, 13-26.b | |||||
energy | The kinetic energy acquired by an electron in passing through a potential difference of 1 volt in a vacuum. Its value is experimentally determined as 1,602 177 x 10-19 J (approximately). | ISO 31-0:1992, Table 6 | ISO 31-9:1992, 9-32.b | ||||
exchange integral | The interaction energy arising from electron exchange. | ISO 31-13:1992, 13-35.b | |||||
Fermi energy | In a metal, the highest energy of occupied states at zero thermodynamic temperature. | ISO 31-13:1992, 13-28.b | |||||
gap energy | Difference in energy between lowest level of conduction band and highest level of valence band. | ISO 31-13:1992, 13-28.b | |||||
maximum beta particle energy | Maximum energy of the energy spectrum in a beta disintegration process. | ISO 31-9:1992, 9-39.b | |||||
reaction energy | In a nuclear reaction, the sum of the kinetic and photon energies of the reaction products minus the sum of the kinetic and photon energies of the reactants. | ISO 31-10:1992, 10-1.b | |||||
resonance energy | Kinetic energy of an incident particle, in the reference frame of the target, corresponding to a resonance in a nuclear reaction. | ISO 31-10:1992, 10-2.b | |||||
work function | The energy difference between an electron at rest at infinity and an electron at the Fermi level in the interior of a substance. | ISO 31-13:1992, 13-25.b | |||||
ELECTRONVOLT_M_SQD | eV · m2 | total atomic stopping power | The total linear stopping power divided by the number density of the atoms in the substance. 1 eV · m2 = (1,602 177 33 ± 0,000 000 49) x 10-19 J · m2 (approximately). |
TOTAL_ATOMIC- _STOPPING_POWER |
46 | ISO 31-10:1992, 10-19.b | |
ELECTRONVOLT_M_SQD_PER_KG | (eV · m2)/kg | total mass stopping power | The total linear stopping power divided by the volumic mass of the substance. 1 (eV · m2)/kg = (1,602 177 33 ± 0,000 000 49) x 10-19 (J · m2)/kg (approximately). |
TOTAL_MASS- _STOPPING_POWER |
47 | ISO 31-10:1992, 10-20.b | |
ELECTRONVOLT_PER_METRE | eV/m | linear energy transfer | For an ionizing charged particle, the energy imparted locally to matter in traversing a small distance through the matter, divided by that distance. | TOTAL_LINEAR- _STOPPING_POWER |
48 | ISO 31-10:1992, 10-54.b | |
total linear stopping power | For an ionizing charged particle, the energy imparted locally to matter in traversing a small distance through the matter, divided by that distance; -dE/dx. 1 eV/m = (1,602 177 33 ± 0,000 000 49) x 10-19 J/m (approximately). |
ISO 31-10:1992, 10-18.b | |||||
FARAD | F | capacitance | The charge divided by potential difference. 1 F = 1 C/V = 1 (s4 · A2)/(m2 · kg). |
CAPACITANCE | 49 | ISO 31-0:1992, Table 2 | ISO 31-5:1992, 5-9.a |
FARAD_PER_METRE | F/m | permittivity | The ability of a material to resist the formation of an electric field within it. 1 F/m = 1 (s4 · A2)/(m3 · kg). |
PERMITTIVITY | 50 | ISO 31-5:1992, 5-10.a | |
GRAM | g | mass | For historical reasons the name of the base unit for mass, the kg, contains the name of the SI prefix "kilo". A gram is a special name given to unit kg x 10-3 that is used instead of "millikilogram". |
MASS | 55 | ISO 31-0:1992, 3.2.4 | |
GRAM_PER_CUBIC_CM | g/cm3 | mass concentration (of B) | The amount of substance of B divided by the volume of the mixture. | VOLUMIC_MASS | 56 | ISO 31-8:1992, 8-11.a | |
volumic mass (mass density) | The mass divided by the volume. 1 g/cm3 = 103 kg/m3 (exactly). |
ISO 31-3:1992, 3-2.b | ISO 31-0:1992, 2.3.2.3; ISO 31-7:1992, 7-8.a | ||||
GRAM_PER_CUBIC_M | g/m3 | mass concentration (of B) | The amount of substance of B divided by the volume of the mixture. | VOLUMIC_MASS | 57 | ISO 31-8:1992, 8-11.a | |
volumic mass (mass density) | The mass divided by the volume. 1 g/m3 = 10-3 kg/m3 (exactly). |
ISO 31-3:1992, 3-2.b | ISO 31-0:1992, 2.3.2.3; ISO 31-7:1992, 7-8.a | ||||
GRAM_PER_GRAM | g/g | mass fraction (of B) | The mass of B divided by the mass of the mixture. 1 g/g = 1 kg/kg = 1. |
MASS_FRACTION | 58 | ISO 31-8:1992, 8-12.a | ISO 31-0:1992, 2.3.3; ISO 31-0:1992, 2.3.2.3 |
GRAM_PER_KILOGRAM | g/kg | mass fraction (of B) | The mass of B divided by the mass of the mixture. 1 g/kg = 10-3 kg/kg = 10-3 (exactly). |
MASS_FRACTION | 59 | ISO 31-8:1992, 8-12.a | ISO 31-0:1992, 2.3.3; ISO 31-0:1992, 2.3.2.3 |
GRAY | Gy | absorbed dose of ionizing radiation | For any ionizing radiation, the energy imparted to an element of irradiated matter divided by the mass of this element. 1 Gy = 1 J/kg = 1 m2/s2. |
ABSORBED_DOSE | 60 | ISO 31-0:1992, Table 3 | ISO 31-10:1992, 10-51.a |
kerma | For indirectly ionizing (uncharged) particles, the sum of the initial kinetic energies of all charged particles liberated in an element of matter, divided by the mass of that element. | ISO 31-10:1992, 10-55.a | |||||
GRAY_PER_SECOND | Gy/s | absorbed dose rate of ionizing radiation | The absorbed dose of ionizing radiation over an interval of time, divided by that time. 1 Gy/s = 1 W/kg = 1 m2/s3. |
ABSORBED_DOSE_RATE | 61 | ISO 31-10:1992, 10-53.a | |
kerma rate | For indirectly ionizing (uncharged) particles, the sum of the initial kinetic energies of all charged particles liberated in an element of matter in a small interval of time, divided by the mass of that element and the interval of time. | ISO 31-10:1992, 10-56.a | |||||
HENRY | H | magnetic inductance | For a thin conducting loop, the magnetic flux through the loop, caused by an electric current in the loop, divided by that current. For two thin conducting loops (m and n), the magnetic flux through one loop, due to an electric current in the other loop, divided by that current. 1 H = 1 Wb/A = 1 (m2 · kg)/(s2 · A2). |
INDUCTANCE | 63 | ISO 31-0:1992, Table 2 | ISO 31-5:1992, 5-22.a |
permeance | The reciprocal of the reluctance of a magnetic circuit, determined by the magnetic flux divided by the magnetomotive force. | ISO 31-5:1992, 5-39.a | |||||
HENRY_PER_METRE | H/m | magnetic permeability | The ability of a substance to acquire magnetization when placed in a magnetic field. 1 H/m = 1 (m · kg)/(s2 · A2). |
MAGNETIC- _PERMEABILITY |
64 | ISO 31-5:1992, 5-24.a | |
HERTZ | Hz | frequency | The number of cycles divided by time. 1 Hz = 1 s-1. |
FREQUENCY | 65 | ISO 31-0:1992, Table 2 | ISO 31-2:1992, 2-3.a; ISO 31-6:1992, 6-1.a; ISO 31-7:1992, 7-2.a |
rotational frequency | The number of revolutions divided by time. 1 Hz = 1 s-1. |
ISO 31-5:1992, 5-41.a | |||||
HOUR | h | time | 1 h = 60 min = 3 600 s (exactly). | TIME | 66 | ISO 31-0:1992, Table 4 | ISO 31-1:1992, 1-7.c |
INT_SOLAR_FLUX_UNIT | none | international solar flux unit | The unit of radio emission from the <SUN>, measured at a wavelength of 10.7 cm (approximately 2 800 MHz). 1 SFU = 104 Jy = 10-22 W/(m2 · Hz) (exactly). |
FLUX_DENSITY | 67 | ISO 31-0:1992, 2.3.1 and 2.3.2 (derived) | |
INV_CUBIC_CM | 1/cm3 | volumetric entity density (any elementary entity: atoms, molecules, ions, electrons, other particles, or specified groups of such particles) | The number of molecules or particles divided by volume. 1/cm3 = 10-6 1/m3. |
VOLUMETRIC_ENTITY- _DENSITY |
68 | ISO 31-10:1992, 10-27.a | ISO 31-0:1992, 2.3.2.3 |
INV_CUBIC_CM_SEC | 1/(cm3 · s) | volumetric entity emittance or capture rate (any elementary entity: atoms, molecules, ions, electrons, other particles, or specified groups of such particles) | The number of molecules or particles divided by volume, per time. 1/(cm3 · s) = 10-6 1/(m3 · s). |
VOLUMETRIC_ENTITY- _EMIT_RATE |
69 | ISO 31-10:1992, 10-35.a | ISO 31-0:1992, 2.3.2.3 |
INV_CUBIC_METRE | 1/m3 | electron number density (volumic electron number) | The number density of electrons in conduction band. | VOLUMETRIC_ENTITY- _DENSITY |
70 | ISO 31-13:1992, 13-30.a | |
ion number density (ion density) | The number of positive or negative ions in a volume element, divided by that element. | ISO 31-10:1992, 10-27.a | |||||
neutron number density | The number of free neutrons in a volume element, divided by that element. | ISO 31-10:1992, 10-29.a | |||||
volumetric entity density (any elementary entity: atoms, molecules, ions, electrons, other particles, or specified groups of such particles) | The number of molecules or particles divided by their volume. | ISO 31-8:1992, 8-10.a | |||||
INV_CUBIC_METRE_EV | 1/(m3 · eV) | density of states | A function of the energy in a solid given by the number of permitted quantum states in the energy range between E and E + dE, per unit volume of the material. 1/(m3 · eV) = (6,241 5061 4 ± 0,0001 0011 9) x 1018 1/(m3 · J) (approximately). |
DENSITY_STATES | 71 | ISO 31-13:1992, 13-17.b | |
INV_CUBIC_METRE_JOULE | 1/(m3 · J) | density of states | A function of the energy in a solid given by the number of permitted quantum states in the energy range between E and E + dE, per unit volume of the material. | DENSITY_STATES | 72 | ISO 31-13:1992, 13-17.a | |
INV_CUBIC_METRE_SEC | 1/(m3 · s) | slowing-down density | The number density of neutrons slowing down past a given energy value in a small time interval, divided by that interval. | VOLUMETRIC_ENTITY- _EMIT_RATE |
73 | ISO 31-10:1992, 10-35.a | |
volumetric entity emittance or capture rate (any elementary entity: atoms, molecules, ions, electrons, other particles, or specified groups of such particles) | The number of molecules or particles divided by volume, per time. | ISO 31-10:1992, 10-34.a | |||||
INV_HENRY | 1/H | reluctance | The magnetic potential difference divided by magnetic flux. 1/H = 1 A/Wb = 1 (s2 · A2)/(m2 · kg). |
RELUCTANCE | 74 | ISO 31-5:1992, 5-38.a | |
INV_KELVIN | 1/K | cubic expansion coefficient | The coefficient of volumic expansion divided by the thermodynamic temperature change. | LINEAR_EXPANSION- _COEFF |
75 | ISO 31-4:1992, 4-3.a | |
linear expansion coefficient | The coefficient of linear expansion divided by the thermodynamic temperature change. | ISO 31-4:1992, 4-3.a | |||||
relative pressure coefficient | The coefficient of pressure change divided by the thermodynamic temperature change. | ISO 31-4:1992, 4-3.a | |||||
INV_METRE | 1/m | angular reciprocal lattice vector | A vector whose scalar products with all fundamental lattice vectors are integral multiples of 2π. | INV_LENGTH | 76 | ISO 31-13:1992, 13-2.a | |
angular repetency (angular wave number) | The reciprocal of the wavelength or the number of waves per unit angle along the direction of propagation. | ISO 31-2:1992, 2-7.b | ISO 31-6:1992, 6-5.b; ISO 31-7:1992, 7-7.b; ISO 31-13:1992, 13-10.b | ||||
curvature | The reciprocal of a radius of curvature. | ISO 31-1:1992, 1-4.a | |||||
fundamental reciprocal lattice vectors | The fundamental translation vectors for the reciprocal lattice. | ISO 31-13:1992, 13-2.a | |||||
linear attenuation coefficient (linear extinction coefficient) | The ratio of a quantity which is a function of distance divided by the distance between the measurements. | ISO 31-6:1992, 6-42.a | ISO 31-10:1992, 10-13.a | ||||
linear ionization by a particle | The number of elementary charges of the same sign produced over an element of length of the path of an ionizing charged particle, divided by that element. | ISO 31-10:1992, 10-23.a | |||||
repetency (wavenumber) | The reciprocal of the wavelength or the number of waves per unit length along the direction of propagation. | ISO 31-2:1992, 2-6.a | ISO 31-6:1992, 6-4.a; ISO 31-7:1992, 7-6.a | ||||
vergence (lens power) | The reciprocal of the distance between a point of reference and the point at which a pair of converging or diverging light rays intersect. | ISO 31-6:1992, 6-46.a | |||||
volumic cross-section (macroscopic cross-section) | Sum of the cross-sections for a reaction or process of a specified type over all atoms in a given volume, divided by that volume. | ISO 31-10:1992, 10-7.a | |||||
INV_MICRON | 1/μm | angular repetency (angular wave number) | The reciprocal of the wavelength or the number of waves per unit angle along the direction of propagation. 1 μm-1 = 106 1/m (exactly). |
INV_LENGTH | 77 | ISO 31-2:1992, 2-7.b | ISO 31-6:1992, 6-5.b; ISO 31-7:1992, 7-7.b; ISO 31-13:1992, 13-10.b |
repetency (wavenumber) | The reciprocal of the wavelength or the number of waves per unit length along the direction of propagation. | ISO 31-2:1992, 2-6.a | ISO 31-6:1992, 6-4.a; ISO 31-7:1992, 7-6.a | ||||
INV_MOLE | 1/mol | molar density (Avogadro constant) | The number of molecules divided by the amount of substance. | MOLAR_DENSITY | 78 | ISO 31-8:1992, 8-4.a | |
INV_PASCAL | 1/Pa | bulk compressibility | The reciprocal of the bulk modulus. | COMPRESSIBILITY | 79 | ISO 31-3:1992, 3-19.a | |
compressibility | The extent to which a material reduces its volume when it is subjected to compressive stresses. 1/Pa = 1 (m · s2)/kg. |
ISO 31-3:1992, 3-19.a | |||||
isentropic compressibility | At a constant value of entropy, the extent to which a material reduces its volume when it is subjected to compressive stresses. | ISO 31-4:1992, 4-5.a | |||||
isothermal compressibility | At a constant temperature, the extent to which a material reduces its volume when it is subjected to compressive stresses. | ISO 31-4:1992, 4-5.a | |||||
INV_RADIAN | 1/rad | reciprocal plane angle | The reciprocal of the angle between two half-lines terminating at the same point is the ratio of the radius of a circle (with its centre at that point) to the length of the included arc of that circle. 1 rad-1 = 1 m/m = 1. |
RECIPROCAL_PLANE- _ANGLE |
80 | ISO 31-0:1992, 2.3.2.2 (derived) | |
INV_SEC_STERADIAN | 1/(s · sr) | photon intensity | In a given direction from a source, the photon flux leaving the source, or an element of the source, in an element of solid angle containing the given direction, divided by that element of solid angle. | PHOTON_INTENSITY | 81 | ISO 31-6:1992, 6-24.a | |
INV_SECOND | 1/s | angular frequency | The frequency of rotation or vibration. | RATE | 82 | ISO 31-2:1992, 2-4.b | ISO 31-5:1992, 5-42.b; ISO 31-7:1992, 7-4.b |
angular frequency | The number of cycles or revolutions divided by time. | ISO 31-6:1992, 6-2.b | ISO 31-9:1992, 9-14.b; ISO 31-9:1992, 9-15.b; ISO 31-13:1992, 13-11.b | ||||
damping coefficient | The factor defining the rate of exponential amplitude decay in a periodic or acoustic system. | ISO 31-7:1992, 7-23.a | ISO 31-2:1992, 2-11.a | ||||
decay constant (disintegration constant) | Probability of decay in a small time interval, divided by that interval. | ISO 31-9:1992, 9-36.a | |||||
photon flux | The number of photons in an incident beam of light received by a surface over a time interval. | ISO 31-6:1992, 6-23.a | |||||
pulsatance | The angular velocity of a periodic quantity. | ISO 31-2:1992, 2-4.b | ISO 31-5:1992, 5-42.b; ISO 31-7:1992, 7-4.b | ||||
rotational frequency | The number of revolutions divided by time. | ISO 31-2:1992, 2-3.b | ISO 31-5:1992, 5-41.b | ||||
INV_SQ_CM_SEC_SR_EV | 1/(cm2 · s · sr · eV) | particle flux density within an energy range | At a point on a surface and in a given direction, the charged particle flux of an element of the surface within an energy range of 1 eV centered on a given particle energy, divided by the area of the orthogonal projection of this element on a plane perpendicular to the given direction, and divided by an element of solid angle containing the given direction. 1/(cm2 · s · sr · eV) = 10-6 1/(m2 · s · sr · eV) (exactly). |
PARTICLE_FLUX- _DENSITY |
83 | ISO 31-0:1992, 2.3.2.3 (derived) | |
INV_SQ_CM_SEC_SR_KEV | 1/(cm2 · s · sr · KeV) | particle flux density within an energy range | At a point on a surface and in a given direction, the charged particle flux of an element of the surface within an energy range of 1 KeV centered on a given particle energy, divided by the area of the orthogonal projection of this element on a plane perpendicular to the given direction, and divided by an element of solid angle containing the given direction. 1/(cm2 · s · sr · KeV) = 10-9 1/(m2 · s · sr · eV) (exactly, assuming an even distribution of particle energies). |
PARTICLE_FLUX- _DENSITY |
84 | ISO 31-0:1992, 2.3.2.3 (derived) | |
INV_SQ_CM_SEC_SR_MEV | 1/(cm2 · s · sr · MeV) | particle flux density within an energy range | At a point on a surface and in a given direction, the charged particle flux of an element of the surface within an energy range of 1 MeV centered on a given particle energy, divided by the area of the orthogonal projection of this element on a plane perpendicular to the given direction, and divided by an element of solid angle containing the given direction. 1/(cm2 · s · sr · MeV) = 10-12 1/(m2 · s · sr · eV) (exactly, assuming an even distribution of particle energies). |
PARTICLE_FLUX- _DENSITY |
85 | ISO 31-0:1992, 2.3.2.3 (derived) | |
INV_SQ_CM_SEC_STERADIAN | 1/(cm2 · s · sr) | photon luminance (photon radiance) | At a point on a surface and in a given direction, the photon intensity of an element of the surface, divided by the area of the orthogonal projection of this element on a plane perpendicular to the given direction. 1/(cm2 · s · sr) = 10-4 1/(m2 · s · sr) (exactly). |
PHOTON_LUMINANCE | 86 | ISO 31-6:1992, 6-25.a | ISO 31-0:1992, 2.3.2.3 |
INV_SQ_M_SEC_SR_EV | 1/(m2 · s · sr · eV) | particle flux density within an energy range | At a point on a surface and in a given direction, the charged particle flux of an element of the surface within an energy range of 1 eV centered on a given particle energy, divided by the area of the orthogonal projection of this element on a plane perpendicular to the given direction, and divided by an element of solid angle containing the given direction. | PARTICLE_FLUX- _DENSITY |
87 | ISO 31-0:1992, 2.3.2.2 (derived) | |
INV_SQ_M_SEC_STERADIAN | 1/(m2 · s · sr) | photon luminance (photon radiance) | At a point on a surface and in a given direction, the photon intensity of an element of the surface, divided by the area of the orthogonal projection of this element on a plane perpendicular to the given direction. | PHOTON_LUMINANCE | 88 | ISO 31-6:1992, 6-25.a | |
INV_SQ_METRE | 1/m2 | areal entity density (any elementary entity: atoms, molecules, ions, electrons, other particles, or specified groups of such particles) | At a given point in space, the number of particles incident on a small sphere, divided by the cross-sectional area of that sphere. | AREAL_ENTITY_DENSITY | 89 | ISO 31-6:1992, 6-28.a | |
particle fluence | At a given point in space, the number of particles incident on a small sphere, divided by the cross-sectional area of that sphere. | ISO 31-10:1992, 10-8.a | |||||
INV_SQ_METRE_SEC | 1/(m2 · s) | current density of particles | A vector quantity, the integral of whose normal component over any surface is equal to the net number of particles passing through that surface in a small time interval divided by that interval. | PARTICLE_CURRENT- _DENSITY |
90 | ISO 31-10:1992, 10-12.a | |
particle fluence rate (particle flux density) | At a given point in space, the number of particles incident on a small sphere in a small time interval, divided by the cross-sectional area of that sphere and by the time interval. | ISO 31-10:1992, 10-9.a | ISO 31-10:1992, 10-31.a | ||||
photon exitance | At a point on a surface, the photon flux leaving an element of the surface, divided by the area of that element and by the time interval. | ISO 31-6:1992, 6-26.a | |||||
photon irradiance | At a point on a surface, the photon flux incident on an element of the surface, divided by the area of that element and by the time interval. | ISO 31-6:1992, 6-27.a | |||||
INV_STERADIAN | 1/sr | reciprocal solid angle | The reciprocal of a solid angle of a cone is the ratio of the square of the radius of a sphere (with its centre at the apex of that cone) to the area cut out on a spherical surface. 1 sr-1 = 1 m2/m2 = 1. |
RECIPROCAL_SOLID- _ANGLE |
91 | ISO 31-0:1992, 2.3.2.2 (derived) | |
INV_STERADIAN_METRE | 1/(sr · m) | spectral reciprocal solid angle | The reciprocal of a solid angle of a cone is the ratio of the square of the radius of a sphere (with its centre at the apex of that cone) to the area cut out on a spherical surface, as a function of radiant wavelength. | SPECTRAL- _RECIPROCAL_SOLID- _ANGLE |
92 | ISO 31-0:1992, 2.3.2.2 (derived) | |
INV_STERADIAN_MICRON | 1/(sr · μm) | spectral reciprocal solid angle | The reciprocal of a solid angle of a cone is the ratio of the square of the radius of a sphere (with its centre at the apex of that cone) to the area cut out on a spherical surface, as a function of radiant wavelength. 1/(sr · μm) = 106 1/(sr · m) (exactly). |
SPECTRAL- _RECIPROCAL_SOLID- _ANGLE |
93 | ISO 31-0:1992, 2.3.2.2 (derived) | |
JANSKY | Jy | flux density | The amount of a given type of radiation that crosses a specified area within a specified period. 1 Jy = 10-26 W/(m2 · Hz) (exactly). |
FLUX_DENSITY | 94 | ISO 31-0:1992, 2.3.1 | |
JOULE | J | alpha disintegration energy | The sum of the kinetic energy of the alpha particle produced in the disintegration process and the recoil energy of the product atom in the reference frame in which the emitting nucleus is at rest before its disintegration. | ENERGY | 95 | ISO 31-9:1992, 9-38.a | |
average energy loss per ion pair formed (average energy loss per elementary charge of the same sign produced) | The initial kinetic energy of an ionizing charged particle, divided by the total ionization produced by that particle. | ISO 31-10:1992, 10-25.a | |||||
beta disintegration energy | Sum of the maximum beta particle energy and the recoil energy of the atom produced in the reference frame in which the emitting nucleus is at rest before its disintegration. | ISO 31-9:1992, 9-40.a | |||||
electron affinity | The energy difference between an electron at rest at infinity and an electron at the lowest level of the conduction band in an insulator or semiconductor. | ISO 31-13:1992, 13-26.a | |||||
energy | The amount of work. 1 J = 1 N·m = 1 (m2 · kg)/s2. |
ISO 31-0:1992, Table 2 | ISO 31-3:1992, 3-26.a | ||||
energy imparted | The energy imparted by ionizing radiation to the matter in a given volume is the difference between the sum of the energies of all the directly ionizing (charged) and indirectly ionizing (uncharged) particles which have entered the volume and the sum of the energies of all those which have left it, minus the energy equivalent of any increase in rest mass that has taken place in nuclear or elementary particle reactions within the volume. | ISO 31-10:1992, 10-50.a | |||||
enthalpy | Heat content. | ISO 31-4:1992, 4-20.a | |||||
exchange integral | The interaction energy arising from electron exchange. | ISO 31-13:1992, 13-35.a | |||||
Fermi energy | In a metal, the highest energy of occupied states at zero thermodynamic temperature. | ISO 31-13:1992, 13-28.a | |||||
gap energy | Difference in energy between lowest level of conduction band and highest level of valence band. | ISO 31-13:1992, 13-28.b | |||||
heat (quantity of heat) | Energy that is the result of the temperature difference between the boundary of a system and its surrounding environment. | ISO 31-4:1992, 4-6.a | |||||
level width | The uncertainty in energy (full width at half maximum) of an unstable state due to the finite lifetime of the state. | ISO 31-9:1992, 9-32.a | |||||
maximum beta particle energy | Maximum energy of the energy spectrum in a beta disintegration process. | ISO 31-9:1992, 9-39.a | |||||
mean energy imparted | The expectation value of the energy imparted. | ISO 31-10:1992, 10-50.a | |||||
radiant energy | The energy emitted, transferred or received as radiation. | ISO 31-6:1992, 6-7.a | |||||
reaction energy | In a nuclear reaction, the sum of the kinetic and photon energies of the reaction products minus the sum of the kinetic and photon energies of the reactants. | ISO 31-10:1992, 10-1.a | |||||
resonance energy | Kinetic energy of an incident particle, in the reference frame of the target, corresponding to a resonance in a nuclear reaction. | ISO 31-10:1992, 10-2.a | |||||
work function | The energy difference between an electron at rest at infinity and an electron at the Fermi level in the interior of a substance. | ISO 31-13:1992, 13-25.a | |||||
JOULE_METRE_SQD | J · m2 | total atomic stopping power | The total linear stopping power divided by the number density of the atoms in the substance. 1 J · m2 = 1 (m4 · kg)/s2. |
TOTAL_ATOMIC- _STOPPING_POWER |
96 | ISO 31-10:1992, 10-19.a | |
JOULE_METRE_SQD_PER_KG | (J · m2)/kg | total mass stopping power | The total linear stopping power divided by the volumic mass of the substance. 1 (J · m2)/kg = 1 m4/s2. |
TOTAL_MASS- _STOPPING_POWER |
97 | ISO 31-10:1992, 10-20.a | |
JOULE_PER_CUBIC_M | J/m3 | radiant energy density | The radiant energy in an element of volume, divided by that element. | ENERGY_DENSITY | 98 | ISO 31-6:1992, 6-8.a | |
sound energy density (volumic sound energy) | The mean sound energy in a given volume divided by that volume. | ISO 31-7:1992, 7-15.a | |||||
volumic electromagnetic energy (electromagnetic energy density) | The energy in an element of volume, divided by that element. 1 J/m3 = 1 kg/(m · s2). |
ISO 31-5:1992, 5-30.a | |||||
JOULE_PER_GRAM_K | J/(g · K) | massic entropy (specific entropy) | The heat entropy divided by mass. | SPECIFIC_HEAT- _CAPACITY |
99 | ISO 31-4:1992, 4-19.a | |
massic heat capacity (specific heat capacity) | The heat capacity divided by mass. 1 J/(g · K) = 103 J/(kg · K) (exactly). |
ISO 31-4:1992, 4-16.a | ISO 31-0:1992, 2.3.2.3 | ||||
JOULE_PER_KELVIN | J/K | Boltzmann constant | A constant equal to 1,38 x 10-23 J/K, used in statistical physics. | HEAT_CAPACITY | 100 | ISO 31-8:1992, 8-37.a | |
entropy | When a small quantity of heat dQ is received by a system the thermodynamic temperature of which is T, the entropy of the system is increased by dQ/T, provided that no irreversible change takes place in the system. | ISO 31-4:1992, 4-18.a | |||||
heat capacity | The quantity dQ/dT, when the temperature of a system is increased by dT as a result of the addition of a small quantity of heat dQ. 1 J/K = 1 (m2 · kg)/(s2 · K). |
ISO 31-4:1992, 4-15.a | |||||
JOULE_PER_KELVIN_MOLE | J/(K · mol) | molar entropy | The heat entropy divided by the amount of substance. | MOLAR_ENTROPY | 101 | ISO 31-8:1992, 8-9.a | |
molar gas constant | The universal constant of proportionality in the ideal gas law: pVm = RT. | ISO 31-8:1992, 8-36.a | |||||
molar heat capacity | The heat capacity divided by the amount of substance. 1 J/(K · mol) = 1 (m2 · kg)/(s2 · K · mol). |
ISO 31-8:1992, 8-8.a | |||||
JOULE_PER_KG | J/kg | specific energy | The energy divided by mass. 1 J/kg = 1 m2/s2. |
SPECIFIC_ENERGY | 102 | ISO 31-4:1992, 4-21.a | |
JOULE_PER_KG_KELVIN | J/(kg · K) | massic entropy (specific entropy) | The heat entropy divided by mass. | SPECIFIC_HEAT- _CAPACITY |
103 | ISO 31-4:1992, 4-19.a | |
massic heat capacity (specific heat capacity) | The heat capacity divided by mass. 1 J/(kg · K) = 1 m2/(s2 · K). |
ISO 31-4:1992, 4-16.a | |||||
JOULE_PER_KM | J/km | linear energy transfer | For an ionizing charged particle, the energy imparted locally to matter in traversing a small distance through the matter, divided by that distance. 1 J/km = 10-3 J/m (exactly). |
LINEAR_ENERGY- _TRANSFER |
104 | ISO 31-10:1992, 10-54.a | |
total linear stopping power | For an ionizing charged particle, the energy imparted locally to matter in traversing a small distance through the matter, divided by that distance; -dE/dx. 1 J/km = 1 x 10-3 J/m (exactly). |
ISO 31-10:1992, 10-18.a | ISO 31-0:1992, 2.3.2.3 | ||||
JOULE_PER_M_FOURTH_PWR | J/m4 | spectral concentration of radiant energy density (in terms of wavelength) | The radiant energy density in an infinitesimal wavelength interval, divided by the range of that interval. 1 J/m4 = 1 kg/(m2 · s2). |
SPECTRAL_RAD- _ENERGY_DENSITY |
105 | ISO 31-6:1992, 6-9.a | |
JOULE_PER_METRE | J/m | linear energy transfer | For an ionizing charged particle, the energy imparted locally to matter in traversing a small distance through the matter, divided by that distance. 1 J/m = 1 (m · kg)/s2. |
LINEAR_ENERGY- _TRANSFER |
106 | ISO 31-10:1992, 10-54.a | |
total linear stopping power | For an ionizing charged particle, the energy imparted locally to matter in traversing a small distance through the matter, divided by that distance; -dE/dx. | ISO 31-10:1992, 10-18.a | |||||
JOULE_PER_MOLE | J/mol | chemical potential | A partial molar Gibbs free energy; the change in Gibbs free energy when one mole of a substance is added to a very large amount of a sample. | MOLAR_ENERGY | 107 | ISO 31-8:1992, 8-17.a | |
molar thermodynamic energy | The thermodynamic energy divided by the amount of substance. 1 J/mol = 1 (m2 · kg)/(s2 · mol). |
ISO 31-8:1992, 8-7.a | |||||
JOULE_PER_SQ_METRE | J/m2 | energy fluence | At a given point in space, the sum of the energies, exclusive of rest energy, of all the particles incident on a small sphere, divided by the cross-sectional area of that sphere. | RADIANT_ENERGY- _FLUENCE |
108 | ISO 31-10:1992, 10-10.a | |
radiant energy fluence | At a given point in space, the radiant flux incident on a small sphere, divided by the cross-sectional area of that sphere. 1 J/m2 = 1 kg/s2. |
ISO 31-6:1992, 6-11.a | |||||
JOULE_SECOND | J · s | Planck constant | 1 J · s = 1 (m2 · kg)/s. | PLANCK_CONSTANT | 109 | ISO 31-9:1992, 9-7.a | |
KELVIN | K | thermodynamic temperature | The fraction 1 / 273,16 of the thermodynamic temperature of the triple point of water. SI base unit. |
THERMO_TEMPERATURE | 110 | ISO 31-0:1992, Table 1 | ISO 31-4:1992, 4-1.a; ISO 31-13:1992, 13-12.a; ISO 31-13:1992, 13-29.a; ISO 31-13:1992, 13-36.a |
KELVIN_PER_KM | K/km | lineic thermodynamic temperature gradient | The thermodynamic temperature difference divided by distance. 1 K/km = 10-3 K/m (exactly). |
LINEIC_THERMO_TEMP- _GRADIENT |
111 | ISO 31-0:1992, 2.3.2.2 and 2.3.2.3 (derived) | |
KELVIN_PER_METRE | K/m | lineic thermodynamic temperature gradient | The thermodynamic temperature difference divided by distance. | LINEIC_THERMO_TEMP- _GRADIENT |
112 | ISO 31-0:1992, 2.3.2.2 (derived) | |
KELVIN_PER_SEC | K/s | thermodynamic temperature change rate | The thermodynamic temperature change over an interval of time, divided by that time. | THERMO_TEMP_CHANGE- _RATE |
113 | ISO 31-0:1992, 2.3.2.2 and 2.3.4 (derived) | |
KELVIN_PER_WATT | K/W | thermal resistance | The temperature difference divided by heat flow rate. 1 K/W = 1 (m2 · kg · K)/s3. |
THERMAL_RESISTANCE | 114 | ISO 31-4:1992, 4-12.a | |
KG_METRE_PER_SEC | kg · m/s | momentum | The product of mass and velocity. | MOMENTUM | 115 | ISO 31-3:1992, 3-8.a | |
KG_METRE_SQD | kg · m2 | moment of inertia (about an axis) | The sum (integral) of the products of the elements of mass of a body and the squares of their distances from an axis. | MOMENT_INERTIA | 116 | ISO 31-3:1992, 3-7.a | |
KG_METRE_SQD_PER_SEC | (kg · m2)/s | moment of momentum (angular momentum) | The moment of momentum of a particle about a point is equal to the vector product of the radius vector from this point to the particle and the momentum of the particle. | ANGULAR_MOMENTUM | 117 | ISO 31-3:1992, 3-11.a | |
KG_PER_CUBIC_METRE | kg/m3 | mass concentration (of B) | The amount of substance of B divided by the volume of the mixture. | VOLUMIC_MASS | 118 | ISO 31-8:1992, 8-11.a | |
volumic mass (mass density) | The mass divided by the volume. | ISO 31-3:1992, 3-2.a | ISO 31-7:1992, 7-8.a | ||||
KG_PER_KG | kg/kg | mass fraction (of B) | The mass of B divided by the mass of the mixture. 1 kg/kg = 1. |
MASS_FRACTION | 119 | ISO 31-8:1992, 8-12.a | ISO 31-0:1992, 2.3.3 |
KG_PER_LITRE | kg/l | mass concentration (of B) | The amount of substance of B divided by the volume of the mixture. | VOLUMIC_MASS | 120 | ISO 31-8:1992, 8-11.b | |
volumic mass (mass density) | The mass divided by the volume. 1 kg/l = 10-3 kg/m3 (exactly). |
ISO 31-3:1992, 3-2.c | |||||
KG_PER_METRE | kg/m | lineic mass (linear density) | The mass divided by length. | LINEIC_MASS | 121 | ISO 31-3:1992, 3-5.a | |
KG_PER_MOLE | kg/mol | molar mass | The mass divided by the amount of substance. | MOLAR_MASS | 122 | ISO 31-8:1992, 8-5.a | |
KG_PER_SECOND | kg/s | mass flow rate | The mass of matter which crosses a given surface, divided by time. | MASS_FLOW_RATE | 123 | ISO 31-3:1992, 3-29.a | |
KG_PER_SQ_METRE | kg/m2 | areic mass (surface density) | The mass divided by area. | SURFACE_DENSITY | 124 | ISO 31-3:1992, 3-6.a | |
mean mass range | The mean linear range multiplied by the volumic mass of the substance. | ISO 31-10:1992, 10-22.a | |||||
KILOGRAM | kg | mass | The mass of the international prototype of the kilogram. SI base unit. |
MASS | 125 | ISO 31-0:1992, Table 1 | ISO 31-3:1992, 3-1.a; ISO 31-8:1992, 8-31.a; ISO 31-9:1992, 9-4.a; ISO 31-9:1992, 9-5.a; ISO 31-9:1992, 9-28.a; ISO 31-13:1992, 13-31.a |
KM_PER_HOUR | km/h | velocity | The distance divided by time. 1 km/h = 1 / 3,6 m/s (exactly). |
SPEED | 127 | ISO 31-1:1992, 1-10.b | |
LITRE | l, L (Both symbols are equally accepted.) |
volume | The product of length, width, and height. 1 l = 1 dm3 = 10-3 m3 (exactly). |
VOLUME | 130 | ISO 31-0:1992, Table 4 | ISO 31-1:1992, 1-6.b |
LITRE_PER_HOUR | L/h | volume flow rate | The volume of matter which crosses a given surface, divided by time. 1 L/h = 1 / 3,6 x 10-6 m3/s (exactly). |
VOLUME_FLOW_RATE | 131 | ISO 31-0:1992, 2.3.2.2 (derived) | |
LITRE_PER_SECOND | L/s | volume flow rate | The volume of matter which crosses a given surface, divided by time. 1 L/s = 10-3 m3/s (exactly). |
VOLUME_FLOW_RATE | 132 | ISO 31-0:1992, 2.3.2.2 (derived) | |
LUMEN | lm | luminous flux | The rate of light emission. 1 lm = 1 cd · sr. |
LUMINANCE_FLUX | 134 | ISO 31-0:1992, Table 2 | ISO 31-6:1992, 6-30.a |
LUMEN_HOUR | lm · h | quantity of light | The time integral of luminous flux. 1 lm · h = 3 600 lm · s (exactly). |
QUANTITY_LIGHT | 135 | ISO 31-6:1992, 6-31.b | |
LUMEN_PER_SQ_METRE | lm/m2 | luminous exitance | At a point on a surface, the luminous flux leaving an element of the surface, divided by the area of that element. | LUMINANCE_EXITANCE | 136 | ISO 31-6:1992, 6-33.a | |
LUMEN_PER_WATT | lm/W | luminous efficacy | The luminous flux divided by power (radiant flux). 1 lm/W = 1 (s3 · lm)/(m2 · kg). |
LUMINANCE_EFFICIENCY | 137 | ISO 31-6:1992, 6-36.a | |
LUMEN_SECOND | lm · s | quantity of light | The time integral of luminous flux. | QUANTITY_LIGHT | 138 | ISO 31-6:1992, 6-31.a | |
LUX | lx | illuminance | At a point on a surface, the luminous flux incident on an element of the surface, divided by the area of that element. 1 lx = 1 lm/m2. |
ILLUMINANCE | 139 | ISO 31-0:1992, Table 2 | ISO 31-6:1992, 6-34.a |
LUX_HOUR | lx · h | light exposure | The time integral of illuminance. 1 lx · h = 3 600 lx · s (exactly). |
LIGHT_EXPOSURE | 140 | ISO 31-6:1992, 6-35.b | |
LUX_SECOND | lx · s | light exposure | The time integral of illuminance. | LIGHT_EXPOSURE | 141 | ISO 31-6:1992, 6-35.a |