Effect of electrical field on heat capacity

AI Thread Summary
The discussion revolves around deriving the effect of an electric field on the heat capacity of perfect gas molecules with a permanent electrical dipole moment. Participants emphasize the importance of computing the partition function, initially using an incorrect angular measure that leads to confusion with Bessel functions. Correcting the integration limits and the use of cosine in the exponential is highlighted, with the consensus that the radial component does not need to be included. The final result involves a function with sinh, indicating progress in the calculations. Overall, the thread focuses on clarifying the mathematical approach to the problem.
Shadowz
Messages
41
Reaction score
0

Homework Statement



Given the perfect gas molecules with permanent electrical dipole moment u in the field \epsilon.
The potential energy is U = -u\epsilon\cos\Theta
Derive the additional effect of \epsilon on the heat capacity.

I need some hints, please help. Thanks.
 
Physics news on Phys.org
Hi,

You have to compute the partition function first...do you know how to do that?
 
Hi,

So my attempt was to compute q = \int_0^{2\pi} e^{-\beta U} d\Theta

But this gives me the Bessel function, so I am not sure if I am on the right track.
 
Shadowz said:
Hi,

So my attempt was to compute q = \int_0^{2\pi} e^{-\beta U} d\Theta

But this gives me the Bessel function, so I am not sure if I am on the right track.
No because you are in 3D and the angular measure you have to use is
sin \theta d\phi d\theta and not just d\theta.
 
Hi,

Thank for your help. I agree.

So I tried

\int_0^{2\pi}\int_0^{\pi} e^{-\beta \mu \epsilon \cos\Phi}sin\Theta d\Theta d\Phi
but still gets the Bessel function.

Is my limit of integration wrong?

Should it be

\int_0^{2\pi}\int_0^{\pi}\int_0^\infty e^{-\beta \mu \epsilon \cos\Phi} r^2 drsin\Theta d\Theta d\Phi

Thanks,
 
Last edited:
Shadowz said:
Hi,

Thank for your help. I agree.

So I tried

\int_0^{2\pi}\int_0^{\pi} e^{-\beta \mu \epsilon \cos\Phi}sin\Theta d\Theta d\Phi
but still gets the Bessel function.

Is my limit of integration wrong?

Should it be

\int_0^{2\pi}\int_0^{\pi}\int_0^\infty e^{-\beta \mu \epsilon \cos\Phi} r^2 drsin\Theta d\Theta d\Phi

Thanks,
Well the thing is that you should have \cos \theta instead of \cos \phi in the exponential. The reason for that is that you have an external field which point toward a non varying direction. In spherical basis and coordinates the only vector that fulfill this criteria is \hat{u}_z whose scalar product with \hat{u}_r gives \cos \theta.
 
Thanks, I got it. So we won't need r^2dr in the integral. I get the result that has sinh in it.
 
Shadowz said:
Thanks, I got it. So we won't need r^2dr in the integral. I get the result that has sinh in it.
No you don't need the r^2dr part in the integral because your dipole has a fixed "length" and therefore its length shouldn't be taken as a degree of freedom.
I don't know exactly the result but a sinh sounds good to me.
 
Ya right. Thank you. The rest is easy, I think.
 
Back
Top