What is the electric field on the axis of a uniformly polarized cylinder?

  • Thread starter Thread starter jdstokes
  • Start date Start date
  • Tags Tags
    Cylinder
Click For Summary
SUMMARY

The discussion centers on calculating the electric field on the axis of a uniformly polarized cylinder with radius 'a' and polarization 'P'. The initial approach utilized Gauss' law, leading to an incorrect conclusion of E = P/(4ε₀). However, the correct method involves integrating Coulomb's law for the bound surface charge, resulting in the correct electric field expression of E = P/(2ε₀). The error lies in the misapplication of Gauss' law for this specific geometry.

PREREQUISITES
  • Understanding of electric fields and polarization concepts
  • Familiarity with Gauss' law and its applications
  • Knowledge of Coulomb's law
  • Basic calculus for integration
NEXT STEPS
  • Study the derivation of electric fields from bound charges
  • Learn about the applications of Gauss' law in different geometries
  • Explore the concept of polarization in dielectric materials
  • Investigate the relationship between dipole moment and electric fields
USEFUL FOR

Students and professionals in physics, particularly those focusing on electromagnetism, as well as educators seeking to clarify concepts related to electric fields and polarization in materials.

jdstokes
Messages
520
Reaction score
1
Hi all,

I'd like to get your opinion on the validity of my working for the following problem. According to my lecturer the answer is incorrect, but I can't figure out where I'm going wrong.

A cylinder of radius a is uniformly polarized in a direction perpendicular to the axis. The magnitude of the dipole moment per unit volume is P. Determine the electric field on the axis of the cylinder.

To me this seems like a straightforward application of Gauss' law, namely

[itex] \int_{\mathrm{rectangle}}\vec{E} {\cdot} d \vec{A} + \int_{\textrm{half-cylinder}}\vec{E} {\cdot} d \vec{A} = \frac{2aP\ell}{\varepsilon_0}[/itex]

[itex] E (2a \ell) + \int_{-\pi/2}^{+\pi/2}E\cos\theta a \ell d\theta = \frac{2aP\ell}{\varepsilon_0} \Rightarrow[/itex]

[itex] E = \frac{P}{2\varepsilon_0}[/itex]

answer should by P / (4 epsilon).

Thanks

James
 
Physics news on Phys.org
Your use of Gauss is wrong.
Dimensionally, the answer must be proportional to P/epsilonnaught,
so any mistake will look close to right.
You have to integrate Coulomb's law for the bound surface charge.
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 5 ·
Replies
5
Views
4K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 8 ·
Replies
8
Views
3K
Replies
2
Views
2K
  • · Replies 7 ·
Replies
7
Views
8K
Replies
3
Views
2K
  • · Replies 7 ·
Replies
7
Views
4K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K