Displacement Electric Field Outside Dielectric Material

Click For Summary
SUMMARY

The discussion centers on the behavior of the displacement field (D-field) and electric field (E-field) in and around dielectric materials, specifically in the context of a conducting sphere and surrounding dielectric. Inside the conducting sphere (region 1), both the D-field and E-field are zero. In region 2, within the dielectric, the D-field exists, while outside the dielectric (region 3), the D-field is determined by the equation D(r>R) = q/(4*pi*r^2), where ε(r) is equal to 1. The continuity of the electric field across boundaries and the relationship between bound and free charges are also discussed, emphasizing the importance of understanding charge density and current density in static cases.

PREREQUISITES
  • Understanding of electric displacement field (D-field) and electric field (E-field) concepts
  • Familiarity with dielectric materials and their properties
  • Knowledge of Gauss's Law and its application in electrostatics
  • Basic understanding of charge density and current density in electrostatics
NEXT STEPS
  • Study the relationship between bound charge density and polarization in dielectrics
  • Learn about the continuity conditions for electric fields at material boundaries
  • Explore the implications of the continuity equation in static electric fields
  • Investigate the effects of different permittivities on D-field and E-field distributions
USEFUL FOR

Students and professionals in electrical engineering, physicists studying electrostatics, and anyone interested in the behavior of electric fields in dielectric materials.

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: 173
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
960
  • · Replies 6 ·
Replies
6
Views
2K
Replies
14
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
Replies
10
Views
2K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 11 ·
Replies
11
Views
2K
Replies
23
Views
4K
Replies
1
Views
2K