Narcol2000
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Given the mean energy of a system in a heat bath is
[tex] \bar{E} = - \frac{\partial ln(Z)}{\partial \beta}[/tex]
Where Z is the partition function and [tex]\beta = k_BT[/tex]
Why is the standard deviation of E defined by:
[tex] (\Delta E)^2 = \frac{\partial^2 ln(Z)}{\partial \beta ^2}[/tex]
I can't seem to find any proof of how the second derivative is related to the standard deviation.
[tex] \bar{E} = - \frac{\partial ln(Z)}{\partial \beta}[/tex]
Where Z is the partition function and [tex]\beta = k_BT[/tex]
Why is the standard deviation of E defined by:
[tex] (\Delta E)^2 = \frac{\partial^2 ln(Z)}{\partial \beta ^2}[/tex]
I can't seem to find any proof of how the second derivative is related to the standard deviation.