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Display information for equation id:math.2507.53 on revision:2507

* Page found: Das ideale Gas (eq math.2507.53)

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\begin{align}

& Z=\frac{1}{N!}\frac{1}{{{\hbar }^{3N}}}\int_{V}^{{}}{{}}{{d}^{3}}{{q}_{1}}...\int_{V}^{{}}{{}}{{d}^{3}}{{q}_{N}}\int_{{{R}^{3}}}^{{}}{{}}{{d}^{3}}{{p}_{1}}...\int_{{{R}^{3}}}^{{}}{{}}{{d}^{3}}{{p}_{N}}\exp \left( -\frac{\beta }{2m}\sum\limits_{i}^{{}}{{}}{{p}_{i}}^{2} \right)=\frac{1}{N!}{{\left[ V\Phi \left( \beta  \right) \right]}^{N}} \\

& \Rightarrow \Psi =-\ln Z=\frac{F(T,V)}{kT}=-N\ln \left[ V\Phi \left( \beta  \right) \right]+\ln N!\approx -N\ln \Phi \left( \beta  \right)-N\ln \frac{V}{N}-N \\

\end{align}

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Z=1N!13NVd3q1...Vd3qNR3d3p1...R3d3pNexp(β2mipi2)=1N![VΦ(β)]NΨ=lnZ=F(T,V)kT=Nln[VΦ(β)]+lnN!NlnΦ(β)NlnVNN
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