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Display information for equation id:math.2555.38 on revision:2555

* Page found: Das ideale Fermigas (eq math.2555.38)

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TeX (original user input): 

\bar{N}=\left( 2s+1 \right)\left( \frac{V}{{{h}^{3}}} \right)4\pi \int_{0}^{\infty }{{}}dp{{p}^{2}}\frac{1}{\left( {{e}^{\beta \left( \frac{{{p}^{2}}}{2m}-\mu  \right)}}+1 \right)}

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N ¯ = ( 2 ⁢ s + 1 ) ⁢ ( V h 3 ) ⁢ 4 ⁢ π ⁢ ∫ 0 ∞ 𝑑 p ⁢ p 2 ⁢ 1 ( e β ⁢ ( p 2 2 ⁢ m - μ ) + 1 ) ¯ 𝑁 2 𝑠 1 𝑉 superscript ℎ 3 4 𝜋 superscript subscript 0 differential-d 𝑝 superscript 𝑝 2 1 superscript 𝑒 𝛽 superscript 𝑝 2 2 𝑚 𝜇 1 {\displaystyle{\displaystyle\bar{N}=\left(2s+1\right)\left(\frac{V}{{{h}^{3}}}% \right)4\pi\int_{0}^{\infty}{{}}dp{{p}^{2}}\frac{1}{\left({{e}^{\beta\left(% \frac{{{p}^{2}}}{2m}-\mu\right)}}+1\right)}}}

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MathML (1.838 KB / 428 B) :

N¯=(2s+1)(Vh3)4π∫0∞dpp21(eβ(p22m−μ)+1)

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