On the practice problems for the final, for the first problem, consider problem 6 on the current problem set. You should be able to show for any pair potential u(r) that B2 can be written as
-2 pi Integral(0 to infinity) [ exp(-beta u(r)) - 1] r^2 dr
where r is the scalar distance between two particles.
Wednesday, December 5, 2007
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