Effect of electrical field on heat capacity

Join the discussion
Registration is free. Start your own thread to ask a follow-up.
8 replies · 3K views
Shadowz
Messages
41
Reaction score
0

Homework Statement



Given the perfect gas molecules with permanent electrical dipole moment u in the field [tex]\epsilon[/tex].
The potential energy is [tex]U = -u\epsilon\cos\Theta[/tex]
Derive the additional effect of [tex]\epsilon[/tex] 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 [tex]q = \int_0^{2\pi} e^{-\beta U} d\Theta[/tex]

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 [tex]q = \int_0^{2\pi} e^{-\beta U} d\Theta[/tex]

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
[tex]sin \theta d\phi d\theta[/tex] and not just [tex]d\theta[/tex].
 
Hi,

Thank for your help. I agree.

So I tried

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

Is my limit of integration wrong?

Should it be

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

Thanks,
 
Last edited:
Shadowz said:
Hi,

Thank for your help. I agree.

So I tried

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

Is my limit of integration wrong?

Should it be

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

Thanks,
Well the thing is that you should have [tex]\cos \theta[/tex] instead of [tex]\cos \phi[/tex] 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 [tex]\hat{u}_z[/tex] whose scalar product with [tex]\hat{u}_r[/tex] gives [tex]\cos \theta[/tex].
 
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 [tex]r^2dr[/tex] 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.