What Is the Mathematical Definition of the Microcanonical Partition Function?

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Homework Statement


Does anyone know the mathematical definition of the microcanonical partition function?
I've seen
\Omega = {E_0\over{N!h^{3n}}}\int d^{3N}q d^{3N}p \delta(H - E)
where H=H(p,q) is the Hamiltonian. This looks like a useful definition.
Only thing is I don't know what E_0 is.

Homework Equations


The Attempt at a Solution

 
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The microcanonical partition function is just a count of the number of states that satisfy extensive constraints on volume, energy, etc. The probability of each state is then trivially one over the partition function.
 
But in the case of a classical system the number of states is uncountable because the position and momenta are continuous.
 
In which case you can still calculate the phase space volume and the probability distribution is uniform over that volume --- it's the obvious generalisation.
 
Ok. Good. Now I see why my "hint" was to bring the constant energy surface in phase space into a sphere (because I know how to find the volume of a sphere).

Thank you very much genneth.
 
To solve this, I first used the units to work out that a= m* a/m, i.e. t=z/λ. This would allow you to determine the time duration within an interval section by section and then add this to the previous ones to obtain the age of the respective layer. However, this would require a constant thickness per year for each interval. However, since this is most likely not the case, my next consideration was that the age must be the integral of a 1/λ(z) function, which I cannot model.
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