Using density of states D(E) = (2s + 1)/ω0), which generalizes equation (9-27) to account for multiple allowed spin states (see Exercise 52), the definition Nω0(2s + 1) ≡ 6, and
solve for B in distributions (9-32) and (9-33)—careful use of ± will cut your work by about half. Then plug back in and show that for a system of simple hannonic oscillators, the distributions become
You will need the following integral:∫∞0(Bez±1)-1dz±ln(1±1/B)
We need at least 10 more requests to produce the solution.
0 / 10 have requested this problem solution
The more requests, the faster the answer.