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Ideal gas law
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The ideal gas law is the equation of state of a hypothetical ideal gas, first stated by Benoît Paul Émile Clapeyron in 1834. The law is derived from the fact that in the ideal state of any gas a given number of its "particles" occupy the same volume, and that volume changes are inverse to pressure changes and linear to temperature changes.
The state of an amount of gas is determined by its pressure, volume, and temperature according to the equation:
where
is the absolute pressure of the gas,
is the volume of the gas,
is the number of moles of gas,
is the universal gas constant,
is the absolute temperature.
The value of the ideal gas constant, R, is found to be as follows.
The ideal gas law mathematically follows from a statistical mechanical treatment of primitive identical particles (point particles without internal structure) which do not interact, but exchange momentum (and hence kinetic energy) in elastic collisions.
Since it neglects both molecular size and intermolecular attractions, the ideal gas law is most accurate for monoatomic gases at high temperatures and low pressures.

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Encyclopedia
The ideal gas law is the equation of state of a hypothetical ideal gas, first stated by Benoît Paul Émile Clapeyron in 1834. The law is derived from the fact that in the ideal state of any gas a given number of its "particles" occupy the same volume, and that volume changes are inverse to pressure changes and linear to temperature changes.
The state of an amount of gas is determined by its pressure, volume, and temperature according to the equation:
where
is the absolute pressure of the gas,
is the volume of the gas,
is the number of moles of gas,
is the universal gas constant,
is the absolute temperature.
The value of the ideal gas constant, R, is found to be as follows.
| R | = | 8.314472 | J·mol-1·K-1 |
>| = | 8.314472 | m3·Pa·K-1·mol-1 | | = | 8.314472 | kPa·L·mol-1·K-1 | | = | 0.08205746 | L·atm·K-1·mol-1 | | = | 62.36367 | L·mmHg·K-1·mol-1 | | = | 10.73159 | ft3·psi·°R-1·lb-mol-1 | | = | 1545.3490 | ft·lbf·°R-1·lb-mol-1 (for air) |
The ideal gas law mathematically follows from a statistical mechanical treatment of primitive identical particles (point particles without internal structure) which do not interact, but exchange momentum (and hence kinetic energy) in elastic collisions.
Since it neglects both molecular size and intermolecular attractions, the ideal gas law is most accurate for monoatomic gases at high temperatures and low pressures. The neglect of molecular size becomes less important for larger volumes, i.e., for lower pressures. The relative importance of intermolecular attractions diminishes with increasing thermal kinetic energy i.e., with increasing temperatures. More sophisticated equations of state, such as the van der Waals equation,
allow deviations from ideality caused by molecular size and intermolecular forces to be taken into account.
Alternative Forms
As the amount of substance could be given in mass instead of moles, sometimes an alternative form of the ideal gas law is useful. The number of moles is equal to the mass divided by the molar mass :
-
By replacing , we get:
-
from where
- .
This form of the ideal gas law is very useful because it links pressure, density , and temperature in a unique formula independent from the quantity of the considered gas.
In statistical mechanics the following molecular equation is derived from first principles:
-
Here is Boltzmann's constant, and is the actual number of molecules, in contrast to the other formulation, which uses , the number of moles. This relation implies that , and the consistency of this result with experiment is a good check on the principles of statistical mechanics.
From here we can notice that for an average particle mass of times the
atomic mass constant (i.e., the mass is u)
and since , we find that the ideal gas law can be rewritten as:
Calculations
The table below essentially simplifies the ideal gas equation for a particular processes, thus making this equation easier to solve using numerical methods.
A thermodynamic process is defined as a system that moves from state 1 to state 2, where the state number is denoted by subscript. As shown in the first column of the table, basic thermodynamic processes are defined such that one of the gas properties (P,V,T, or S) is constant throughout the process.
For a given thermodynamics process, in order to specify the extent of a particular process, one of the properties ratios (listed under the column labeled "known ratio") must be specified (either directly or indirectly). Also, the property for which the ratio is known must be distinct from the property held constant in the previous column (otherwise the ratio would be unity, and not enough information would be available to simplify the gas law equation).
In the final three columns, the properties (P,V,T) at state 2 can be calculated from the properties at state 1 using the equations listed.
| Process | Constant | Known ratio | P2 | V2 | T2 |
|---|
| Isobaric process | Pressure | V2/V1 | P2 = P1 | V2 = V1 (V2/V1) | T2 = T1 (V2/V1) | | " | " | T2/T1 | P2 = P1 | V2 = V1 (T2/T1) | T2 = T1 (T2/T1) | | Isochoric process | Volume | P2/P1 | P2 = P1 (P2/P1) | V2 = V1 | T2 = T1 (P2/P1) | | " | " | T2/T1 | P2 = P1 (T2/T1) | V2 = V1 | T2 = T1 (T2/T1) | | Isothermal process | Temperature | P2/P1 | P2 = P1 (P2/P1) | V2 = V1 / (P2/P1) | T2 = T1 | | " | " | V2/V1 | P2 = P1 / (V2/V1) | V2 = V1 (V2/V1) | T2 = T1 | Isentropic process (Reversible adiabatic process) | | P2/P1 | P2 = P1 (P2/P1) | V2 = V1 (P2/P1) -1/ | T2 = T1 (P2/P1)(-1)/ | | " | " | V2/V1 | P2 = P1 (V2/V1) - | V2 = V1 (V2/V1) | T2 = T1 (V2/V1)1- | | " | " | T2/T1 | P2 = P1 (T2/T1)/(-1) | V2 = V1 (T2/T1) 1/(1-) | T2 = T1 (T2/T1) |
a. In an isentropic process, system entropy (Q) is constant. Under these conditions, P1 V1 = P2 V2, where is defined as the heat capacity ratio, which is constant for an ideal gas. The value used for is typically 1.4 for diatomic gases like nitrogen (N2) and oxygen (O2), (and air, which is 99% diatomic). Also is typically 1.6 for monatomic gases like the noble gases helium (He), and argon (Ar). In internal combustion engines varies between 1.35 and 1.15, depending on constitution gases and temperature.
Derivations
Empirical The ideal gas law can be derived from combining two empirical gas laws: the combined gas law and Avogadro's law. The combined gas law states that
where C is a constant which is directly proportional to the amount of gas, n (Avogadro's law). The proportionality factor is the universal gas constant, R, i.e. .
Hence the ideal gas law
-
Theoretical The ideal gas law can also be derived from first principles using the kinetic theory of gases, in which several simplifying assumptions are made, chief among which are that the molecules, or atoms, of the gas are point masses, possessing mass but no significant volume, and undergo only elastic collisions with each other and the sides of the container in which both linear momentum and kinetic energy are conserved.
Derivation from the statistical mechanics Let q = (qx, qy, qz) and p = (px, py, pz) denote the position vector and momentum vector of a particle of an ideal gas,respectively, and let F denote the net force on that particle, then
where the first equality is Newton's second law, and the second line uses Hamilton's equations and the equipartition theorem. Summing over a system of N particles yields
By Newton's third law and the ideal gas assumption, the net force on the system is the force applied by the walls of their container, and this force is given by the pressure P of the gas. Hence
where dS is the infinitesimal area element along the walls of the container. Since the divergence of the position vector q is
the divergence theorem implies that
where dV is an infinitesimal volume within the container and V is the total volume of the container.
Putting these equalities together yields
which immediately implies the ideal gas law for N particles:
where n=N/NA is the number of moles of gas and R=NAkB is the gas constant.
The readers are referred to the comprehensive article
where an alternative statistical mechanics derivation of the ideal-gas
law, using the
relationship between
the Helmholtz free energy
and
the partition function,
but without using the
equipartition theorem, is provided.
See also
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