Einstein solid, Sterling approximation

[nicksauce]

Homework Statement

Use Sterling's approximation to show that the multiplicity of an Einstein solid, for any large values of N and q is approximately
\Omega(N,q) = \frac{(\frac{q+N}{q})^q(\frac{q+N}{N})^N}{\sqrt{2\pi q(q+N)/N}}

Homework Equations

\Omega(N,q) = \frac{(N+q-1)!}{q!(N-1)!}
\ln(x!) \simeq x\ln(x) - x

The Attempt at a Solution

I see where the terms in the numerator come from, but I cannot see where the terms in the denominator come from. Specifically, the squareroot, and the factor of 2 pi*q. When I grind out the math, I get that the denominator should be (q+N)/N. Help anyone?

 

[nicksauce]

Solved it... Turns out I had to use the other Sterling's approximation

N! = N^Ne^{-N}\sqrt{2\pi N}

 

[Rainbow Child]

Sterling' s approximation is

n! \approx \sqrt{2\,\pi\,n}\left(\frac{n}{e}\right)^n

To get your formula fist get rid of 1 at (N+q-1)!,\,(N-1)!

I think that in the formula

\Omega(N,q) = \frac{(\frac{q+N}{q})^q(\frac{q+N}{N})^N}{\sqrt{2\pi q(q+N)/N}}

the denominator must be \sqrt{2\,\pi\,q\,N/(q+N)}

 

[Rainbow Child]

You solved it while I was typing!

 

[nicksauce]

Thanks... it's the thought that counts anyway!