Mean energy of system with ## E = \alpha |x|^n ##

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SUMMARY

The discussion focuses on deriving the mean energy of a system defined by the energy equation \( E = \alpha |x|^n \), where \( n \) is a positive integer and \( \alpha > 0 \). The mean energy \( \langle E \rangle \) is expressed as \( \langle E \rangle = \xi k_B T \), with \( \xi \) being a numerical constant. The integral for \( \langle E \rangle \) is evaluated using the formula \( \langle E \rangle = \frac{\int_{-\infty}^{\infty} Ee^{-\beta E}}{\int_{-\infty}^{\infty} e^{-\beta E}} \), and the discussion suggests using a change of variable, specifically \( y = x^n \), to simplify the integral.

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  • Understanding of statistical mechanics concepts, particularly mean energy calculations.
  • Familiarity with integrals involving exponential functions and their properties.
  • Knowledge of the Boltzmann constant \( k_B \) and its role in thermodynamics.
  • Experience with symbolic computation tools, such as Mathematica, for solving complex integrals.
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  • Research techniques for evaluating integrals involving exponential decay, particularly in statistical mechanics.
  • Learn about the properties of even functions and their implications in integral calculations.
  • Explore the application of change of variables in integral calculus to simplify complex expressions.
  • Investigate the numerical constant \( \xi \) and its significance in the context of mean energy calculations.
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Homework Statement


If the energy ##E## of a system behaves like ## E = \alpha |x|^n##, where ## n =1, 2, 3, \dots ## and ## \alpha > 0##, show that ## \langle E \rangle = \xi k_B T ##, where ##\xi## is a numerical constant.

Homework Equations


$$ \langle E \rangle = \frac{ \int_{- \infty}^{ \infty} Ee^{-\beta E}}{\int_{-\infty}^{ \infty} e^{-\beta E}},$$ where ## \beta = \frac{1}{k_BT}.##

The Attempt at a Solution


Since the integral is even, it can be written as $$\frac{ \int_{0}^{ \infty} \alpha x^n e^{-\beta \alpha x^n}}{\int_{0}^{ \infty} e^{-\beta \alpha x^n}},$$

It can also be written as

$$ \frac{ \frac{ \partial}{ \partial \beta} \left ( \int_{0}^{ \infty} - e^{-\beta \alpha x^n} \right ) } {\int_{0}^{ \infty} e^{-\beta \alpha x^n}}$$

where the partial derivative was taken outside the integral.

I have no idea how to solve the integral. Mathematica didn't draw up anything useful.
 
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Have you tried a change of variable e.g. y=xn?
 
I think I did try it, but it didn't look like it could result in anything useful.
 

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