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# Difference between revisions of "Ideal gas Helmholtz energy function"

Carl McBride (talk | contribs) m (New page: From equations :<math>Q_{NVT}=\frac{1}{N!} \left( \frac{V}{\Lambda^{3}}\right)^N</math> and :<math>A=-k_B T \ln Q_{NVT}</math> one has :<math>A=-k_BT\left(\ln \frac{1}{N!} + N\ln\frac{V}...) |
Carl McBride (talk | contribs) m |
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:<math>Q_{NVT}=\frac{1}{N!} \left( \frac{V}{\Lambda^{3}}\right)^N</math> | :<math>Q_{NVT}=\frac{1}{N!} \left( \frac{V}{\Lambda^{3}}\right)^N</math> | ||

and | and | ||

− | :<math>A=-k_B T \ln Q_{NVT}</math> | + | :<math>\left.A\right.=-k_B T \ln Q_{NVT}</math> |

one has | one has | ||

:<math>A=-k_BT\left(\ln \frac{1}{N!} + N\ln\frac{V}{\Lambda^{3}}\right)</math> | :<math>A=-k_BT\left(\ln \frac{1}{N!} + N\ln\frac{V}{\Lambda^{3}}\right)</math> |