Surface bound charge on the outer surface of a dielectric

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SUMMARY

The discussion focuses on calculating the displacement vector and surface bound charges in a cylindrical glass dielectric surrounding a one-dimensional conducting wire with a homogeneous charge density λ. The displacement vector D inside the dielectric is derived as D = λ/2πr, where r is the radius. For surface bound charges, the relationship D = εE + P is established, leading to the conclusion that surface bound charge density σ can be expressed as σ = P·n, where P is the dipole moment and n is the normal vector. The dielectric constant and electric susceptibility of glass are suggested as key factors for further analysis.

PREREQUISITES
  • Understanding of electric displacement vector (D) in dielectrics
  • Knowledge of surface bound charge density (σ) and its relation to polarization (P)
  • Familiarity with Gaussian surfaces in electrostatics
  • Concept of dielectric constants and electric susceptibility
NEXT STEPS
  • Study the derivation of the electric displacement vector in dielectrics
  • Learn about the relationship between polarization and surface bound charges
  • Explore the concepts of dielectric constant and electric susceptibility in materials
  • Investigate the application of Gaussian surfaces in electrostatic problems
USEFUL FOR

Students and professionals in physics or electrical engineering, particularly those focusing on electrostatics, dielectrics, and charge distribution in materials.

JKC

Homework Statement



With regards to a one dimensional conducting wire with a homogeneous charge density λ surrounded by a cylindrical glass dielectric of radius R, find:

(a). The displacement vector inside the dielectric

(b). The surface bound charges on the surface of the dielectric

Sorry for the lack of equations and mathematical explanation. Trying to put everything mathematically and graphically would have been quite long. Rest assure I have everything that I'm describing in the attempt written in the correct notation on paper.[/B]

Homework Equations



Included in attempt

The Attempt at a Solution



(a).

Drawing a cylindrical Gaussian surface inside the dielectric of radius r and length L.

Surface integral (displacement vector, D) dot product dS (differential of surface) = charge enclosed

dS = 2πr L

Qenc= λ L

⇒ surface integral D (2πr L) = λ L

D = λ/2πr

For the displacement vector D(bar) = λ/2πr r(bar)

(b).

I'm slightly confused as to where to approach this one from:

D(vector) = εE(field vector) + P(vector)

E and P are the electric field and dipole moment.Surface bound charge = σ = P(vector) n(normal vector)

σ = σbound + σfreeFrom here on I don't really know how to approach this problem. Apologies for the scrappy attempt.
 
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OK for part (a)

For part (b) try to make use of either the dielectric constant of the glass or the electric susceptibility of the glass.
 
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