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Gas constant
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== Relationship with the Boltzmann constant == The [[Boltzmann constant]] ''k''<sub>B</sub> (alternatively ''k'') may be used in place of the molar gas constant by working in pure particle count, ''N'', rather than amount of substance, ''n'', since : <math>R = N_\text{A} k_\text{B},</math> where ''N''<sub>A</sub> is the [[Avogadro constant]]. For example, the [[ideal gas law]] in terms of the Boltzmann constant is : <math>pV = Nk_\text{B} T,</math> where ''N'' is the number of particles (molecules in this case), or to generalize to an inhomogeneous system the local form holds: : <math>p = n k_\text{B} T,</math> where ''n'' = ''N''/''V'' is the [[number density]]. Finally, by defining the [[kinetic energy]] associated to the temperature, : <math>T := k_\text{B} T,</math> the equation becomes simply : <math>p = n T,</math> which is the form usually encountered in statistical mechanics and other branches of theoretical physics.
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