quantumkiko
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Consider a gas contained in volume V at temperature T. The gas is composed of N distinguishable particles at zero rest mass, so that the energy E and momentum p are related by E = pc. The number of single-particle energy states in the range p to p + dp is 4\pi Vp^2 dp. Find the equation of state and the internal energy of the gas and compare with an ordinary (ideal?) gas.
In how I understand the problem, you must integrate 4\pi Vp^2 dp and E = pc to get the partition function Z(E) then use the entropy S = k_b ln Z to get the equation of state given by
\left(\frac{\partial S}{\partial V}\right)_{N, E} = \frac{P}{T}
and the internal energy by,
\left(\frac{\partial}{\partial E}\right)_{N, V} = \frac{1}{T}.
Did I understand the problem correctly?
In how I understand the problem, you must integrate 4\pi Vp^2 dp and E = pc to get the partition function Z(E) then use the entropy S = k_b ln Z to get the equation of state given by
\left(\frac{\partial S}{\partial V}\right)_{N, E} = \frac{P}{T}
and the internal energy by,
\left(\frac{\partial}{\partial E}\right)_{N, V} = \frac{1}{T}.
Did I understand the problem correctly?
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