Can a rotating dielectric disc be polarized?

AI Thread Summary
A rotating dielectric disc can indeed become polarized, even without an external electric or magnetic field. The discussion reveals that while the disc may not have free charges, polarization can occur due to the accelerated motion of the dielectric, which causes a displacement of charge centers. This polarization is influenced by inertial forces acting differently on electrons and nuclei. The participants explore the relationship between rotational frequency and polarization, suggesting that centrifugal force can be treated as an electric field. Ultimately, the complexity of the forces involved means that polarization will not be uniform across the disc.
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Can a rotating dielectric disc be polarized? No external electric or magnetic field .
 
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Of course it can. If it was previously polarized, the rotation will not necessarily destroy the polarization.
But I suspect this is not what you mean to ask. Do you mean if the disk can become polarized due to rotation?
 
nasu said:
Do you mean if the disk can become polarized due to rotation?

Yes, I do.
 
How do you think that polarization of a dielectric happens in presence of an electric field?
 
I think polarisation should be appear due to electric field, which is created by
reclined free light weight charges (electrons), due to the centrifugal force. But if we have ideal dielecrtic, where we can get this FREE charges?

Or another way. Polarisation can happen due to mechanical deformation of the piezoelectric, but this is not the case.
 
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A dielectric has no free charges. Still can be polarized in electric fields.
You don't need free charges to have polarization.
 
nasu said:
Still can be polarized in electric fields.
You don't need free charges to have polarization.

Of course, but where I get this field? Assumption of the problem - is no electric field, only a rotation disk.
 
  • #10
Yeah, but do you understand that you don't need free charge?
You said that you don't understand the paper and one of the reasons is that there is not free charge in dielectric.
The paper says right in the beginning that accelerated motion of the dielectric can result in polarization. You may find it easier to think about it in terms of inertial forces, in the accelerated frame. The inertial forces will be different for the light electrons than for the heavy nuclei so it may result in a slight displacement of the centers of mass of the two types of charges. This is polarization.
 
  • #11
Now I see. Thank you. How can I calculate polarisation depend on rotational frequency?
 
  • #12
I think centrifugal force - is the some kind of electric field:
##m\omega^2 r = eE##
Then polarisation is equal to ##P = \frac{\epsilon - 1}{4\pi} \frac{m}{e}\omega^2 r##

So, I can also find charge density as ##\rho = -div \vec P##
 
  • #13
I think you should take the difference in force between electron and nucleus but in first approximation it may be OK.
The problem is that the force is not uniform and so neither is polarization.
But again, the change in r will be small at the level of few atomic distances.
 
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