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* Page found: Das ideale Fermigas (eq math.2555.63)

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\begin{align}

& \bar{N}=\frac{2}{3}\frac{\left( 2s+1 \right)}{2}\left( \frac{V}{{{h}^{3}}} \right)4\pi {{\left( 2m\mu  \right)}^{\frac{3}{2}}}\left[ 1+\frac{{{\pi }^{2}}}{8}{{\left( \frac{kT}{\mu } \right)}^{2}} \right]=\frac{2}{3}\frac{\left( 2s+1 \right)}{2}\left( \frac{V}{{{h}^{3}}} \right)4\pi {{\left( 2m{{E}_{F}} \right)}^{\frac{3}{2}}} \\

& \Rightarrow {{\left( \mu  \right)}^{\frac{3}{2}}}\left[ 1+\frac{{{\pi }^{2}}}{8}{{\left( \frac{kT}{\mu } \right)}^{2}} \right]\approx {{\left( {{E}_{F}} \right)}^{\frac{3}{2}}} \\

& \Rightarrow \mu \approx {{E}_{F}}{{\left[ 1+\frac{{{\pi }^{2}}}{8}{{\left( \frac{kT}{\mu } \right)}^{2}} \right]}^{-\frac{2}{3}}} \\

\end{align}

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N¯=23(2s+1)2(Vh3)4π(2mμ)32[1+π28(kTμ)2]=23(2s+1)2(Vh3)4π(2mEF)32(μ)32[1+π28(kTμ)2](EF)32μEF[1+π28(kTμ)2]23
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