Standard deviation of the energy of a system in a heat bath

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SUMMARY

The standard deviation of the energy of a system in a heat bath is defined as \((\Delta E)^2 = \frac{\partial^2 ln(Z)}{\partial \beta^2}\), where \(Z\) represents the partition function and \(\beta = k_BT\). This relationship is derived from statistical mechanics principles, specifically linking the second derivative of the logarithm of the partition function to the fluctuations in energy. Eric Poisson provides a detailed derivation in his "Statistical Physics II" notes, which are valuable for understanding this concept further.

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  • Understanding of statistical mechanics principles
  • Familiarity with partition functions in thermodynamics
  • Knowledge of derivatives in calculus
  • Basic concepts of heat baths and energy fluctuations
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  • Review Eric Poisson's "Statistical Physics II" notes for detailed derivations
  • Study the relationship between partition functions and thermodynamic properties
  • Explore the implications of energy fluctuations in statistical mechanics
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Physicists, students of statistical mechanics, and researchers interested in thermodynamic systems and energy fluctuations in heat baths.

Narcol2000
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Given the mean energy of a system in a heat bath is

<br /> \bar{E} = - \frac{\partial ln(Z)}{\partial \beta}<br />

Where Z is the partition function and \beta = k_BT

Why is the standard deviation of E defined by:

<br /> (\Delta E)^2 = \frac{\partial^2 ln(Z)}{\partial \beta ^2}<br />

I can't seem to find any proof of how the second derivative is related to the standard deviation.
 
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Eric Poisson has a derivation on p40 of his Statisical Physics II notes: http://www.physics.uoguelph.ca/~poisson/research/notes.html.
 
Thanks a lot those notes are also pretty useful in other respects as well.
 

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