Solving Electric Field of an Insulating Slab

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Homework Help Overview

The problem involves calculating the electric field of an insulating slab with a specified charge density, using Gauss's Law. The slab has a thickness of 2d and is oriented parallel to the yz-plane. The charge density varies with position, and the question seeks to determine the electric field in different regions of space.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the integration limits and the interpretation of the volume element in the context of the slab's symmetry. There are questions about the consistency of the integration approach and the implications of the charge distribution.

Discussion Status

Some participants have provided guidance on the integration limits, suggesting that integrating from 0 to d may be sufficient due to the symmetry of the problem. There is an ongoing exploration of the correct interpretation of the volume element and its implications for the calculations.

Contextual Notes

There are mentions of difficulties with the presentation of the problem, including the use of images versus typed equations. Participants are encouraged to clarify their reasoning and ensure consistency in their mathematical expressions.

little neutrino
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Homework Statement


A slab of insulating material has thickness 2d and is oriented so that its faces are parallel to the yz-plane and given by the planes x = d and x = -d. The y- and z- dimensions of the slab are very large compared to d and may be treated as essentially infinite.

Homework Equations


The charge density of the slab is given by ρ(x) = ρ0 * (x/d)^2 , where ρ0 is a positive constant. Using Gauss Law, find the electric field due to the slab (magnitude and direction) at all points in space.

The Attempt at a Solution


Attached is a picture of my attempted solution. I don't know why both my answers are off by a factor of 2, could somebody explain?
The answer given is: |x| > d: (ρ0d)/(3ε) ; |x| < d: (ρ0x^3)/(3εd^2).
Thanks![/B]
 

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Unfortunately the image of your working comes out sideways.
It is not recommended to post images of handwritten working (though yours is more legible than most). Please type algebra into the post, preferably with latex.
Anyway... early on you write ##V = \pi r^2 (2x)##, then later integrate x from -d to +d. Seems inconsistent.
 
Sorry but I don't understand what you mean... Could you elaborate?
I integrated from -d to +d because if |x| > d, there will only be charges on the insulating material until d.
 
little neutrino said:
Sorry but I don't understand what you mean... Could you elaborate?
I integrated from -d to +d because if |x| > d, there will only be charges on the insulating material until d.
Think about what your expression ##dV = 2\pi r^2 dx## means for some x. What does that volume consist of? Where is the 2 coming from? Now consider the dV you get for -x. Is it right to integrate x from -d to +d?
 
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Oh... Is it correct if I visualize it this way: for each dx, there will be dV of 2 circles of area πr^2, one on the + x-axis and the other on the - x-axis, because the line of symmetry is taken at the origin. So I should integrate from 0 to d or -d to 0, because the other side of the pillbox is already taken care of by the equation dV = 2πr^2 dx ?

*sorry about the presentation I'll learn how to use latex soon!
 
little neutrino said:
there will be dV of 2 circles of area πr^2, one on the + x-axis and the other on the - x-axis, because the line of symmetry is taken at the origin. So I should integrate from 0 to d or -d to 0, because the other side of the pillbox is already taken care of by the equation dV = 2πr^2 dx ?
Yes, 0 to d is adequate.
 
Ok thanks! :)
 

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