- #1
Narcol2000
- 25
- 0
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.