Displacement Electric Field Outside Dielectric Material

Click For Summary

Homework Help Overview

The discussion revolves around the behavior of the displacement electric field (D-field) and electric field (E-field) in and around a dielectric material, particularly focusing on the regions inside and outside a conducting sphere and the dielectric. Participants explore the implications of charge distributions and the continuity of electric fields across boundaries.

Discussion Character

  • Conceptual clarification, Assumption checking, Exploratory

Approaches and Questions Raised

  • Participants discuss the nature of the D-field outside the dielectric material and question the assumptions regarding permittivity in that region. There are inquiries about the continuity of the electric field across different surfaces and the role of bound and free charges in determining the fields.

Discussion Status

The discussion is active, with participants providing insights into the relationships between D and E fields, as well as the implications of charge density and polarization. Some guidance has been offered regarding the continuity of the fields and the conditions under which they change, but multiple interpretations are still being explored.

Contextual Notes

Participants are navigating the complexities of static charge distributions and the effects of polarization on the fields. There is an emphasis on understanding the implications of the continuity equation in a static scenario, along with the definitions of bound and free charges.

RyanUSF
Messages
10
Reaction score
0
Homework Statement
You have a conducting sphere (Region 1) of radius a carrying free charge q > 0 surrounded by a neutral dielectric shell (Region 2) of relative permittivity ε(r) = α/r, r ≥ R, where α is a constant with dimension of length, and vacuum outside (Region 3).

Find Displacement field everywhere.
Relevant Equations
D = ε_0*ε(r)*E
Where ε_0 is permittivity of free space, and ε(r) is the relative permittivity, and E is the electric field.
I know that inside region 1, the D-field is zero as it is a conducting sphere, the E-field must be zero. It makes sense that in region 2 (inside the dielectric) there is a D-field.

My question is, is there a D-field outside the dielectric material (r>R)? Obviously there will be an E-field, but now there is only the permittivity of free space, ε(r) is 0 correct? So is the D-field zero outside dielectric material or is it continuous?
 

Attachments

  • dielectric.png
    dielectric.png
    5.5 KB · Views: 177
Physics news on Phys.org
The equation you quote is good everywhere. What does it tell you? What you say about ##\epsilon (r) ## is incorrect. It is 1
 
  • Like
Likes   Reactions: RyanUSF
So with that being said, the D field outside (region 3) essentially becomes the what the electric field would be in that region (multiplied by ε_0 of course). D (r>R) = q/(4*pi*r^2), units of C/m^2 look good.
 
Also do you understand the continuity question? There are bound (polarization) charges and free charges, and you need to understand which is important for D and for E so tell me about it.
 
The continuity equation states that the change in bound charge density with respect to time will equal the negative value of the divergence of bound current density.

For this problem it is a static case so it makes sense, change in charge density is 0 and there is no current density.

The bound charge density will relate to the polarization.
 
RyanUSF said:
The continuity equation states that the change in bound charge density with respect to time will equal the negative value of the divergence of bound current density.
True but not complete.
Is the E field contiuous across the inner (r=a) surface)? By how much does it change?
 
hutchphd said:
True but not complete.
Is the E field contiuous across the inner (r=a) surface)? By how much does it change?
For r<a the electric field must be 0. At r=a there is a surface charge over the sphere giving an E(r=a)=q/4*pi*ε_0*a^2. a<r<R E will change by dividing by ε(r).
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
981
  • · Replies 6 ·
Replies
6
Views
2K
Replies
14
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
Replies
10
Views
2K
  • · Replies 2 ·
Replies
2
Views
4K
  • · Replies 11 ·
Replies
11
Views
2K
Replies
23
Views
4K
Replies
1
Views
2K