Does a Circular Capacitor with a Dielectric Radiate an Electromagnetic Field?

Click For Summary
SUMMARY

The discussion focuses on the analysis of a circular capacitor with a dielectric constant ε, specifically addressing its electromagnetic properties when fed by a time-harmonic current I0. Key findings include the magnetic field distribution inside the capacitor, the computation of the complex Poynting vector, and the demonstration that the capacitor does not radiate an electromagnetic field. The discussion also highlights the relationship between the time-average of the real Poynting vector and the stored energy density, confirming that grad(S) - iwW = 0 in the far field.

PREREQUISITES
  • Understanding of electromagnetic field theory
  • Familiarity with Poynting vector calculations
  • Knowledge of time-harmonic currents and complex notation
  • Basic concepts of capacitors and dielectric materials
NEXT STEPS
  • Study the derivation of the Poynting vector in electromagnetic theory
  • Learn about the properties of dielectric materials in capacitors
  • Explore Feynman's Lectures on Electromagnetism for deeper insights
  • Investigate the implications of surface current density in circular capacitors
USEFUL FOR

Electrical engineers, physicists, and students studying electromagnetic theory, particularly those interested in capacitor design and electromagnetic field analysis.

Noname
Messages
1
Reaction score
0
Member has been warned not to remove the template.
Hi guys,
Consider a circular capacitor with a disk of radius a and plate separation d, as shown in the figure below. Assuming the capacitor is filled with a dielectric constant epsilon and the capacitor is fed by a time harmonic current I0
(a) Find the magnetic field distribution inside the capacitor assuming that the electric field is constant.
(b) Compute the complex Poynting vector and prove that the capacitor does not radiate an electromagnetic field. (Hint: S=(1/2)ExH ; only Re[S ] radiates an electromagnetic field.)
(c) Compute the total stored energy density W and show that far away from the center (kr<< 1): grad(S)-iwW = 0
(d) Find the surface current density as a function of radial distance on the top plate.

I don't really know how to do the (b). I have S=(1/2)ExH. I think I need to write E and H in complex, I have E=Eo*exp(iwt) and H=Ho*exp(iwt). But I can't prove S is only an imaginary part.

Sans titre.jpg
 

Attachments

  • Sans titre.jpg
    Sans titre.jpg
    9.7 KB · Views: 871
Physics news on Phys.org
Normally, for time-harmonic fields the time-average of the real Poynting vector is:

##\langle \mathbf{S} \rangle=\frac{1}{2}\Re\left( \mathbf{E}^{\dagger} \times \mathbf{H}\right)##

So, I guess, the complex Poynting vector you want is ##\mathbf{E}^{\dagger} \times \mathbf{H}##, i.e. you are missing the complex conjugation (which will remove ##\exp\left(i \omega t\right)##)
 
Feynman treats this problem, (without the dielectric material), in his lectures. See Fig. 27-3 and thereabouts. http://www.feynmanlectures.caltech.edu/II_27.html ## \\ ## He uses a slightly different type of units, but you should find it good reading.
 

Similar threads

  • · Replies 8 ·
Replies
8
Views
2K
Replies
14
Views
3K
Replies
6
Views
3K
  • · Replies 20 ·
Replies
20
Views
4K
  • · Replies 4 ·
Replies
4
Views
963
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 8 ·
Replies
8
Views
5K
  • · Replies 5 ·
Replies
5
Views
2K