Method of images: infinite line of charge above plate

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Homework Help Overview

The problem involves an infinite line of charge with charge density λ positioned parallel to and above an infinite grounded conducting plate. The objective is to determine the induced charge density σ on the plate. The context is rooted in electrostatics and the method of images.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of the method of images to represent the system, considering the potential contributions from both the line charge and its image. There is confusion regarding the correct distances to use in the potential equations and how to satisfy boundary conditions. Some participants suggest clarifying the distances involved in the potential calculations.

Discussion Status

The discussion is ongoing with participants exploring different interpretations of the distances involved in calculating the potential. Some guidance has been offered regarding the need to express distances correctly, but no consensus has been reached on the final approach to the problem.

Contextual Notes

There are indications of confusion regarding the setup of the problem and the application of boundary conditions. The thread has also experienced movement between different forum categories, which may have contributed to the discussion dynamics.

zweebna
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Homework Statement


An infinite line of charge with charge density λ is parallel to and a distance d above an infinite grounded conducting plate. What is the charge density σ that is induced in the plate? For simplicity, consider the line of charge to lie along the line x = 0.

Homework Equations


##V_{line} = \frac {\lambda}{2 \pi \epsilon_0} ln(\frac{s_1}{s_2})##
##\sigma = -\epsilon_0 \frac {\delta V}{\delta n}##

The Attempt at a Solution


So by the method of images, I know this problem is (for z>0) equivalent to an infinite line of charge density λ a distance d above z=0, and an infinite line of charge density -λ a distance d below z=0. I know the potential for an infinite line charge is ##V = \frac {\lambda}{2 \pi \epsilon_0} ln(\frac{s_1}{s_2})##, where I believe ##s_2## would be the distance from the line and ##s_1## is an arbitrary point where ##V \rightarrow 0##. I can then add together the potentials for these line charges:
$$V = \frac {\lambda}{2 \pi \epsilon_0} ln(\frac{s_1}{s_2}) - \frac {\lambda}{2 \pi \epsilon_0} ln(\frac{s_1}{s_2})$$
Now I'm confused. I can't just set the distance ##s_2## to be ##d## as this results in a potential of zero at all points. I can't set one to ##z+d## and one to ##z-d## as that doesn't seem to satisfy boundary conditions (##V=0## when ##z=0##, ##V \rightarrow 0## when ##z \rightarrow \infty##).

I know that once I can get the potential, then I can get the induced charge by taking the partial derivative with respective to ##z## at ##z=0##, but I'm confused about getting the potential.
 
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##s_2## is the distance from the line to the point you want to know the potential at. The ##s_2## in your second term is not the same as that in your first so do not call them the same thing. Instead, express the distance from the point you want to compute the potential for to the lines and use those values.
 
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Orodruin said:
##s_2## is the distance from the line to the point you want to know the potential at. The ##s_2## in your second term is not the same as that in your first so do not call them the same thing. Instead, express the distance from the point you want to compute the potential for to the lines and use those values.
So if the point where we're computing potential is ##0<z<d##, then in the first term it would be ##d-z## and in the second term it would be ##z+d##?PS
What forum should this be in? Since posting it's been moved from intro to advanced, back to intro, and now it's back in advanced.
 
Last edited:
zweebna said:
So if the point where we're computing potential is ##0<z<d##, then in the first term it would be ##d-z## and in the second term it would be ##z+d##?
Are you not forgetting some directions?
 
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Orodruin said:
Are you not forgetting some directions?
Ah you're right. So the first time is ##\sqrt{x^2+y^2+(d+z)^2}## and the second term is ##\sqrt{x^2+y^2+(d-z)^2}##? Thank you I think I have it.
 
zweebna said:
Ah you're right. So the first time is ##\sqrt{x^2+y^2+(d+z)^2}## and the second term is ##\sqrt{x^2+y^2+(d-z)^2}##? Thank you I think I have it.

Almost, remember that you want the distance to the line charge. What you have given is the distance to a particular point.
 
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Orodruin said:
Almost, remember that you want the distance to the line charge. What you have given is the distance to a particular point.
Ah so since the line is along ##x=0## would I just ignore the y component? So they are ##\sqrt{x^2+(d+z)^2}## and ##\sqrt{x^2+(d-z)^2}##?
 
zweebna said:
Ah so since the line is along ##x=0## would I just ignore the y component? So they are ##\sqrt{x^2+(d+z)^2}## and ##\sqrt{x^2+(d-z)^2}##?
Right.
 
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Orodruin said:
Right.
Thank you!
 
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zweebna said:
What forum should this be in? Since posting it's been moved from intro to advanced, back to intro, and now it's back in advanced.
I think your thread was used for a forum moderation investigation/experiment which is why it got moved so often. I was the original one who moved it to advanced physics because I felt it belonged here.
 

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