THE BOLTZMANN DISTRIBUTION
belongs to the phase space (Rd)N At temperature T, each particle particle has average kinetic energy dk BT 2 (assume the particle is mono-atomic, k B is the Boltzmann constant) Therefore the total kinetic energy satis es XN i=1 P2 i 2m = Ndk BT 2 Where mis the mass of each gas particle. Therefore at temperature T, the state
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