Surface charge density due to point charge

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Homework Help Overview

The discussion revolves around calculating the surface charge density due to a point charge using the method of images. Participants are examining the relationship between electric fields and surface charge density, as well as the discrepancies between provided solutions and their understanding of the problem.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the calculation of electric fields from both real and imaginary charges, questioning the factors involved in the vertical components and the disappearance of certain terms in the equations. There is also mention of using Gauss's theorem to relate electric fields to surface charge density.

Discussion Status

Some participants are exploring the mathematical relationships and concepts involved, while others are clarifying their understanding of the method of images and its application. One participant expresses that they have gained clarity from the responses provided.

Contextual Notes

There is mention of discrepancies between the lecturer's solution and the problem sheet, as well as concerns about missing steps in the provided solution. Participants are navigating these uncertainties while discussing the problem.

NewtonianAlch
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Homework Statement


Using the method of images, solve the following

image.jpg

The Attempt at a Solution



I have very little idea on how to solve this. I looked up various methods online and none seem to be what the lecturer has used.

This is the solution he posted up, but as usual it is missing 300 steps and also seems to differ to the short answer he has given in the actual problem sheet, although I figured because of the 2 sin θ, the 2 and 4 cancel, leaving only 2 at the bottom. And ε disappears because for finding ρ (surface charge density) we multiply the E-field by ε.

However I don't understand how a 2sinθ came to be and then abruptly disappears.

Any help appreciated.

image.jpg
 
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The electric fields from the two charges (the real and the imaginary one) go along the lines in the sketch (one is marked with "E". The magnitude is calculated with the usual formula, and their vertical component is sin(theta) of their magnitude. You have two charges, both have their vertical component in the same direction, therefore you get a factor of 2 there.

To get rid of the angle, he uses sin(theta)=d/R. You can see the d in the numerator, and R is converted to sqrt(d^2+r^2) in the denominator. The factor of 2 seems to be missing there.
And ε disappears because for finding ρ (surface charge density) we multiply the E-field by ε.
Right.
 
If I may add, and pardon if it's superfluous info:
Two main ideas here:

1. E field just above a conducting surface is εE = σ where σ is surface charge density. The direction of E is normal to, and away from, the conductor if the surface charge density is +. This is easily shown using Gauss's theorem. If the surface charge is -, then the direction is into the plane.

2. The concept of imaging which is as shown on the proffered answer sheet. The basis is that the potetial anywhere along the sheet is constant (equipotential surface) if the image charge is added and the presence of the sheet ignored.
 
Thanks for the responses, I understand it clearly now!
 

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