SoggyBottoms
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Homework Statement
A classical particle with mass m is in thermal equilibrium with a fluid at temperature T. The particle is stuck to a harmonic ('Hookean') spring and can only move on a horizontal line (-\infty < x < \infty). The position of the particle is x = 0 if the spring is in its equilibrium position, but thermal movement can cause it to stretch or compress. The probability distribution of finding the particle in position x is proportional to e^{-\frac{x^2}{2\sigma^2}}.
a) Calculate the spring constant C as a function of m, \sigma, k_b and/or T.
b) Calculate the average quadratic displacement of the particle.
The Attempt at a Solution
The probability of finding the particle in position x is proportional to e^{-\frac{x^2}{2\sigma^2}}. The energy of the spring is \frac{1}{2}C x^2, so the chance of finding the particle in position x is also proportional to e^{-\frac{1}{2}C x^2 \beta}. This gives \frac{1}{2}C x^2 \beta = \frac{x^2}{2\sigma^2} or C = \frac{k_B T}{\sigma^2}
Is this correct?
b) Do they mean finding \langle x^2 \rangle?
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