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The universal constant R that appears in the ideal gas law, Eq. (1, where P is the pressure, V the volume,
1. 
n the amount of substance, and T the thermodynamic (absolute) temperature. The gas constant is universal in that it applies to all gases, providing they are behaving ideally (in the limit of zero pressure). The gas constant is related to the more fundamental Boltzmann constant, k, by Eq. (2), where NA is the Avogadro
2. 
constant (the number of entities per mole). The best modern value in SI units is R = 8.314 472 (15) J/K · mol, where the number in parentheses represents the uncertainty in the last two digits. See also Gas.
According to the equipartition principle, at a temperature T, the average molar energy of each quadratic term in the expression for the energy is (1/2)RT; as a consequence, the translational contribution to the molar heat capacity of a gas at constant volume is (3/2)R; the rotational contribution of a linear molecule is R.
Largely because R is related to the Boltzmann constant, it appears in a wide variety of contexts, including properties unrelated to gases. Thus, it occurs in Boltzmann's formula for the molar entropy of any substance, Eq. (3), where W is the number of
3. 
arrangements of the system that are consistent with the same energy; and in the Nernst equation for the potential of an electrochemical cell, Eq. (4), where E° is a standard potential, F is
4. 
the Faraday constant, and Q is a function of the composition of the cell. The gas constant also appears in the Boltzmann distribution for the population of energy levels when the energy of a level is expressed as a molar quantity. See also Electrode potential; Entropy.
| Measures and Units: gas constant |
physics The constant of proportionality in the universal gas equation, = 8.314 472(15)~ J·(K·mole)-1 with relative standard uncertainty 1.7 × 10-6.
[Hartland A. Contemp. Phys. Vol. 29, 477 (1988)
| Wikipedia: Gas constant |
| Values of R [1] |
Units (V P T−1 n−1) |
|---|---|
| 8.314 472(15) | J K−1 mol−1 |
| 1.985 8775(34) | cal K−1 mol−1 |
| 8.314 472(15) × 107 | erg K−1 mol−1 |
| 8.314 472(15) | m3 Pa K−1 mol−1 |
| 8.314 472(15) | cm3 MPa K−1 mol−1 |
| 8.314 472 × 10−5 | m3 bar K−1 mol−1 |
| 8.205 746 × 10−5 | m3 atm K−1 mol−1 |
| 8.314 472 × 10−2 | L bar K−1 mol−1 |
| 0.082 057 46(14) | L atm K−1 mol−1 |
| 62.363 67(11) | L mmHg K−1 mol−1 |
| 62.363 67(11) | L Torr K−1 mol−1 |
| 6.132 440(10) | ft-lb K−1 g-mol−1 |
| 1545.349(3) | ft-lb R−1 lb-mol−1 |
| 10.731 59(2) | ft3 psi R−1 lb-mol−1 |
| 0.730 2413(12) | ft3 atm R−1 lb-mol−1 |
| 998.9701(17) | ft3 mmHg K−1 lb-mol−1 |
| 1.986 | Btu lb-mol−1 R−1 |
The gas constant (also known as the molar, universal, or ideal gas constant, denoted by the symbol R or R) is a physical constant which is featured in a large number of fundamental equations in the physical sciences, such as the ideal gas law and the Nernst equation. It is equivalent to the Boltzmann constant, but expressed in units of energy (i.e. the pressure-volume product) per kelvin per mole (rather than energy per kelvin per particle).
Its value is

The two digits in parentheses are the uncertainty (standard deviation) in the last two digits of the value. The relative uncertainty is 1.8 × 10−6.
The gas constant occurs in the ideal gas law, as follows:

where p is the absolute pressure, V is the volume of gas, n is the number of moles of gas, and T is thermodynamic temperature. The gas constant has the same units as molar entropy.
Contents |
The Boltzmann constant kB (often abbreviated k) may be used in place of the gas constant by working in pure particle count, N, rather than number of moles, n, since

where NA is the Avogadro constant. For example, the ideal gas law in terms of Boltzmann's constant is

| Rspecific for dry air |
Units |
|---|---|
| 287.058 | J kg−1 K−1 |
| 53.35 | ft lbf lbm−1 R−1 |
| 1716.6 | ft lbf slugm−1 R−1 |
| Based on a mean molar mass for dry air of 28.9645 g/mol. |
|
The specific gas constant of a gas or a mixture of gases (Rspecific) is given by the molar gas constant, divided by the molar mass (M) of the gas/mixture.

Just as the ideal gas constant can be related to the Boltzmann constant, so can the specific gas constant by dividing the Boltzmann constant by the molecular mass of the gas.

Another important relationship comes from thermodynamics. This relates the specific gas constant to the specific heats for a calorically perfect gas and a thermally perfect gas.
where cp is the specific heat for a constant pressure and cv is the specific heat for a constant volume.[2]
It is common, especially in engineering applications, to represent the specific gas constant by the symbol R. In such cases, the universal gas constant is usually given a different symbol such as R to distinguish it. In any case, the context and/or units of the gas constant should make it clear as to whether the universal or specific gas constant is being referred to.[3]
The U.S. Standard Atmosphere, 1976 (USSA1976) defines the gas constant R* as:[4][5]

The USSA1976 does recognize, however, that this value is not consistent with the cited values for the Avogadro constant and the Boltzmann constant.[5] This disparity is not a significant departure from accuracy, and USSA1976 uses this value of R* for all the calculations of the standard atmosphere. When using the ISO value of R, the calculated pressure increases by only 0.62 pascals at 11 kilometers (the equivalent of a difference of only 0.174 meters or 6.8 inches) and an increase of 0.292 Pa at 20 km (the equivalent of a difference of only 0.338 m or 13.2 in).[citation needed]
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