Can someone check my setup for finding E.dl?

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Homework Help Overview

The discussion revolves around evaluating the line integral of the electric field \(\oint \vec{E} \cdot \vec{dl}\) around a square path centered at the origin, due to a point charge +Q located at the origin. Participants are examining the setup and expressions for the electric field at various points along the square path.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the expressions for the electric field at different segments of the square and question the correctness of the setup, including the integration limits and the assignment of coordinates. There is also exploration of symmetry in the problem and its implications for the integral.

Discussion Status

The discussion is active, with participants providing feedback on the original poster's setup and suggesting considerations regarding symmetry. Some participants express uncertainty about specific aspects of the integration process, while others highlight the importance of recognizing the contributions from different segments of the path.

Contextual Notes

There are indications of potential missing information, such as the need for proper notation and clarity in the setup. Participants are also navigating assumptions about the symmetry of the electric field and the implications for the integral's evaluation.

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Homework Statement


A point charge +Q exists at the origin. Find \oint \vec{E} \cdot \vec{dl} around a square centered around the origin. I know the answer is 0, but can someone check my setup?

Homework Equations


E=\frac{Q(\vec{R}-\vec{R'})}{4\pi E_0 |\vec{R}-\vec{R'}|^3}

The Attempt at a Solution

upload_2018-4-15_0-41-44.png
[/B]

For E1 and E3, R = \hat{x}x+\hat{y}\frac{a}{2} and R' = 0
E1 = E3 = \frac{Q\hat{x}x+\hat{y}\frac{a}{2}}{4\pi E_0(x^2+\frac{a^2}{4})^{3/2}}
dl1=dl3 = \hat{x}dx

E2=E4=\frac{Q\hat{x}\frac{a}{2}+\hat{y}y}{4\pi E_0(y^2+\frac{a^2}{4})^{3/2}}
dl2=dl4 = \hat{y}dy
 

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Apart from misssing brackets :smile: ?
And asssuming the obvious integration limits ?
And assuming (from the picture) E1 is for (a/2, 0) to (a/2,a/2) -- in which case you mixed up 1,3 with 2,4 ?

However, not bad for a first thread! Hello EM, :welcome:
 
BvU said:
Apart from misssing brackets :smile: ?
And asssuming the obvious integration limits ?
And assuming (from the picture) E1 is for (a/2, 0) to (a/2,a/2) -- in which case you mixed up 1,3 with 2,4 ?

However, not bad for a first thread! Hello EM, :welcome:
E1 is the line segment from (a/2,-a/2) to (a/2, a/2)
 
Of course, but there ##\vec {dl} = (0, dy)##
 
BvU said:
Of course, but there ##\vec {dl} = (0, dy)##
That is because x stays constant and y changes right?
 
Correct. And the expression for E1 has a constant ##x={a\over 2}## and a varying ##y##
 
BvU said:
Correct. And the expression for E1 has a constant ##x={a\over 2}## and a varying ##y##
So would this setup be correct?
E1 = E3 = \frac{Q}{4\pi E_0} \frac{\hat{x}{x}+\hat{y}\frac{a}{2}}{(x^2+\frac{a^2}{4})^{3/2}}
dl1=dl3 = \hat{y}dy

E2 = E4 = \frac{Q}{4\pi E_0}\frac{\hat{x}\frac{a}{2}+\hat{y}{y}}{(y^2+\frac{a^2}{4})^{3/2}}
dl2=dl4 = \hat{x}dx
 
:wink: You sound as if you hesitate. Have you not convinced yourself?
 
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BvU said:
:wink: You sound as if you hesitate. Have you not convinced yourself?
So now that I have this:
\int_{\frac{-a}{2}}^{\frac{a}{2}} \frac{\hat{x}\frac{a}{2}+\hat{y}y}{(\frac{a^2}{4}+y^2)^{3/2}}dy
How do I integrate this?
 
  • #10
Do you realize you have written two integrals ?
 
  • #11
BvU said:
Do you realize you have written two integrals ?
\int_{\frac{-a}{2}}^{\frac{a}{2}}\frac{\hat{x}\frac{a}{2}}{(\frac{a^2}{4}+y^2)^{3/2}}dy+\int_{\frac{-a}{2}}^{\frac{a}{2}}\frac{\hat{y}y}{(\frac{a^2}{4}+y^2)^{3/2}}dy
 
  • #12
Yes, so one component in the ##\hat x## direction and one in the ##\hat y## direction.
I am too lazy to work out the integral, so I try to sneak my way out: what about the second one, in the ##\hat y## direction ?
 
  • #13
Just to make sure: we see that we don't have to find a primitive to establish the value...
 
  • #14
BvU said:
Just to make sure: we see that we don't have to find a primitive to establish the value...
What does this mean?
For E1 and E3, the x^ direction integral canceled out.

For E2 and E4, the y^ direction integral canceled out.I am left with:
<br /> \int_{\frac{-a}{2}}^{\frac{a}{2}}\frac{\hat{x}\frac{a}{2}}{(\frac{a^2}{4}+y^2)^{3/2}}dy - \int_{\frac{a}{2}}^{\frac{-a}{2}}\frac{\hat{x}\frac{a}{2}}{(\frac{a^2}{4}+y^2)^{3/2}}dy+<br /> \int_{\frac{a}{2}}^{\frac{-a}{2}}\frac{\hat{y}\frac{a}{2}}{(\frac{a^2}{4}+x^2)^{3/2}}dx-\int_{\frac{-a}{2}}^{\frac{a}{2}}\frac{\hat{y}\frac{a}{2}}{(\frac{a^2}{4}+x^2)^{3/2}}dx<br />
 
  • #15
Being lazier than @BvU, I would use symmetry and note that the four line integrals along each side must be equal because if one rotated the square by 90o or 180o or 270o while you were not looking at it, you wouldn't know the difference. So there is only one integral to do. But wait, there is another symmetry to consider. Do you see what it is?
 
  • #16
kuruman said:
Being lazier than @BvU, I would use symmetry and note that the four line integrals along each side must be equal because if one rotated the square by 90o or 180o or 270o while you were not looking at it, you wouldn't know the difference. So there is only one integral to do. But wait, there is another symmetry to consider. Do you see what it is?
I don't see it...
 
  • #17
You know that each of the four line integrals gives you the same number by symmetry. You also know that the result around the closed loop is zero. What does this say about the line integral along one of the sides? How can you get that number? Hint: Look at segment E2. Consider two points on it at ##+x## and ##-x##. What is ##\vec E \cdot d\vec l## at these points?
 
  • #18
kuruman said:
Being lazier than @BvU
Impossible :-p . Apart from that: We both want to exploit symmetry. Can be done from the math side and/or from the physics side
 

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