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Display information for equation id:math.2555.26 on revision:2555

* Page found: Das ideale Fermigas (eq math.2555.26)

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TeX (original user input): 

\to \sum\limits_{j}{{}}\to \left( \frac{V}{8{{\pi }^{3}}{{\hbar }^{3}}} \right)\int_{{}}^{{}}{{}}{{d}^{3}}p=\left( \frac{V}{{{h}^{3}}} \right)\int_{{}}^{{}}{{}}{{d}^{3}}p=\left( 2s+1 \right)\left( \frac{V}{{{h}^{3}}} \right)4\pi \int_{{}}^{{}}{{}}{{p}^{2}}dp

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→ ∑ j → ( V 8 ⁢ π 3 ⁢ ℏ 3 ) ⁢ ∫ d 3 ⁢ p = ( V h 3 ) ⁢ ∫ d 3 ⁢ p = ( 2 ⁢ s + 1 ) ⁢ ( V h 3 ) ⁢ 4 ⁢ π ⁢ ∫ p 2 ⁢ 𝑑 p → absent subscript 𝑗 → 𝑉 8 superscript 𝜋 3 superscript Planck-constant-over-2-pi 3 superscript 𝑑 3 𝑝 𝑉 superscript ℎ 3 superscript 𝑑 3 𝑝 2 𝑠 1 𝑉 superscript ℎ 3 4 𝜋 superscript 𝑝 2 differential-d 𝑝 {\displaystyle{\displaystyle\to\sum\limits_{j}{{}}\to\left(\frac{V}{8{{\pi}^{3% }}{{\hbar}^{3}}}\right)\int{{}}{{d}^{3}}p=\left(\frac{V}{{{h}^{3}}}\right)\int% {{}}{{d}^{3}}p=\left(2s+1\right)\left(\frac{V}{{{h}^{3}}}\right)4\pi\int{{}}{{% p}^{2}}dp}}

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→∑j→(V8π3ℏ3)∫d3p=(Vh3)∫d3p=(2s+1)(Vh3)4π∫p2dp

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