Can a rotating dielectric disc be polarized?

Click For Summary

Discussion Overview

The discussion revolves around the question of whether a rotating dielectric disc can become polarized in the absence of an external electric or magnetic field. Participants explore the implications of rotation on polarization, examining theoretical and conceptual aspects of dielectric materials.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that a rotating dielectric disc can retain its polarization if it was previously polarized.
  • Others question whether the rotation itself can induce polarization in the absence of an external field.
  • A participant references a paper suggesting that accelerated motion of the dielectric can lead to polarization, prompting further inquiry into the mechanisms involved.
  • Concerns are raised about the nature of polarization in dielectrics, particularly regarding the absence of free charges and the role of inertial forces in creating polarization.
  • One participant suggests a relationship between centrifugal force and electric field, proposing a formula for calculating polarization based on rotational frequency.
  • Another participant notes that the force acting on electrons and nuclei is not uniform, which may affect the resulting polarization.

Areas of Agreement / Disagreement

Participants express differing views on whether rotation can induce polarization in a dielectric without an external field. While some agree that polarization can occur due to inertial effects, others remain skeptical about the conditions necessary for this to happen. The discussion does not reach a consensus.

Contextual Notes

Participants highlight limitations in understanding the mechanisms of polarization in dielectrics, particularly regarding the assumptions about free charges and the uniformity of forces acting on different charge types.

sergiokapone
Messages
306
Reaction score
17
Can a rotating dielectric disc be polarized? No external electric or magnetic field .
 
Physics news on Phys.org
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.
 
Last edited:
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.
 

Similar threads

  • · Replies 5 ·
Replies
5
Views
1K
  • · Replies 5 ·
Replies
5
Views
2K
Replies
5
Views
2K
  • · Replies 5 ·
Replies
5
Views
1K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 18 ·
Replies
18
Views
1K
  • · Replies 6 ·
Replies
6
Views
6K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 12 ·
Replies
12
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K