Electric field at point Gauss law

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Homework Help Overview

The discussion revolves around finding the electric field at a point due to a point charge using Gauss's law. Participants are examining the integration process involved in deriving the electric field expression.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the integration techniques required to solve the problem, particularly focusing on the power rule and the implications of variable dependencies in integration. There are questions about the validity of certain steps in the integration process and the context of the formulas presented.

Discussion Status

The discussion is ongoing, with participants providing insights into the integration process and questioning the assumptions made in the problem setup. Some participants express confusion about the integration steps and the relevance of the provided formulas, while others suggest revisiting the problem's context.

Contextual Notes

There are indications that the problem may contain errors or inconsistencies, as some participants point out discrepancies in the integration limits and the application of Gauss's law. The original poster mentions that the exercise includes screenshots of solutions that may not align with their handwritten notes.

Pual Black
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Homework Statement



We won't to find out the electric field at a point p due to a point charge q placed at o as shown in the figure
[/B]
IMG_11300006.jpg
Consider a sphere of radius r passing through the point p. Let the electric field at p be E then by Gauss law

IMG_113006.jpg
my problem is how we get the last step? I don't understand how he integrate it.

The Attempt at a Solution



i tried it and found a solution but not sure if its correct although i got the same result

IMG_1134.jpg
[/B]

sorry that i don't used LATEX but I'm not used with it and i can't write the whole question with LATEX
 
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You need to learn the rules for integration (and differentiation) of ##x^n##. Try this: Power Rule
 
Looks as if the power rule is known, but the concept of integration causes difficulties: substitution ##x=r^{-3}## is carried out ok initially (*), but the much better (or rather, the 'right') substitution ##x = r^{-2}##, leading to ##dx =-2\; r^{-3}dr## and hence ##\int r^{-3} dr = -{1\over2}\int dx## is overseen.

(*) Later on, the swap ##\int {x\over r^{-4}}\; dx = {1\over r^{-4}} \int x\; dx## is unforgivable: r is not a constant but depends on x !
 
If r is not constant and depends on x. Therefore i can't put the ##r^4## outside the integration. Right??
 
Indeed you can not !
 
Ok so how to get this solution?
Any idea??
I want the the same result ##E=\frac{q}{4 \pi \epsilon r^2}##
 
OK, we have to make a step back. Your "Consider a sphere of radius r passing through the point p. Let the electric field at p be E then by Gauss law " continues with a picture with formulas that seem to be out of context: at P there is no charge, so div E is zero there !

Where does this snippet come from? It also integrates from ## r=-\infty## to ## r=\infty## which is very weird, since r can't be negative. Then it equates that to ##2\int_0^\infty\ ##, then inserts a ##- {1\over 3 }## from nowhere (re-check the power rule)!

So, stepping back and trying to find the correct path:

Gauss law replaces a surface integral of E by a volume integral of rho. Indeed ##\nabla \vec E = {\rho\over \epsilon_0} ##, but ## \rho \ne q\big /{4\over 3}\pi r^3\ ## ! That is ##\rho## for a uniformly charged sphere with radius r !

In this simple case the volume integral of rho simply yields q. Frome there use rotation symmetry and gauss law to get to E.


Another thing: note that div E is not ## dE\over dr## !

Divergence in spherical coordinates tells us that

for rotational symmetry ##\nabla\cdot\vec E = {1\over r^2}\; {\partial (r^2E_r)\over \partial r}##

(
as you can check: div E = 0 for the desired result for E

and conversely: with rotational symmetry, Er2 is constant outside the area where charge is present.​
).

[edit] forgot the divergence link, inserted it.
 
Pual Black said:
Ok so how to get this solution?
Any idea??
Sure. Learn how to integrate ##x^n##; in particular, ##\frac{1}{x^3} = x^{-3}##. (No fancy substitutions needed.)

See the link I gave about the power rule.
 
Doc Al said:
Sure. Learn how to integrate ##x^n##; in particular, ##\frac{1}{x^3} = x^{-3}##. (No fancy substitutions needed.)

See the link I gave about the power rule.

I know how to use the power rule.
If you see my solution ;) @BvU
Thank you for your help. Looks like this question is a mess. The whole question is wrong
I will now use your information and maybe i will get a right solution.
 
  • #10
Pual Black said:
I know how to use the power rule.
If you see my solution
Then why did you say the following?
Pual Black said:
my problem is how we get the last step? I don't understand how he integrate it.
The last step was integrating 1/x3.

I guess I missed something. (Sorry about that!)
 
  • #11
Yes that's right but if you try to integrate the last step you will not get the same result. Therefore i said that i don't understand it. But as BvU told me the whole question has mistakes.
 
  • #12
So is the picture with the formulas from a different exercise ? Or did you do a part of the solution in TeX and then switch to handwritten ?
 
  • #13
No the two pictures ( figure and Tex ) are from exercise. Just the handwriting is mine. But the exercise it is not from one source cause the exercise has the soltuion from a screenshot. It has text and image ( the soultion and the figure ) are screenshots.
 
  • #14
So, do we have the "all clear"now, or is there still some thing unfinished ?
 
  • #15
Thank you very much. Its clear now
 

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