Find the electric field of a charged arc a distance R away

AI Thread Summary
The discussion focuses on calculating the electric field from a charged arc, specifically addressing the integration limits for the x-component of the electric field. It is established that integrating from 0 to π/2 yields different results compared to integrating from -π/4 to π/4, with the latter providing the correct answer. The symmetry of the problem indicates that the y-components of the electric field cancel out, simplifying the analysis. Participants explore how to set up integrals for both components and clarify that the total electric field's magnitude does not involve θ after integration. The conversation concludes with an emphasis on understanding the contributions of each component and the role of symmetry in the calculations.
Jaccobtw
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Homework Statement
find electric field of a quarter circle charged arc at point located the same distance from all points on the arc
Relevant Equations
$$dQ = \lambda R d \theta$$
$$dE_x = \frac{k_e dQ}{R^2} cos \theta$$
define charge at an infinitesimal length of arc

$$dQ = \lambda R d \theta$$We only care about the x component of the electric field because the y components cancel due to symmetry

$$dE_x = \frac{k_e dQ}{R^2} cos \theta$$

Integrate to add up the infinitesimal parts. A quarter circle means 90 degrees so integrate from 0 to pi/2.$$\int dE_x=\int_{0}^{\frac{\pi}{2}} \frac{k_e \lambda R d \theta}{R^2} cos \theta$$

PROBLEM: I get two different answers when I integrate from 0 to pi/2 and -pi/4 to pi/4. The right answer came from when I used -pi/4 to pi/4.

Doe anyone know why you can't integrate from 0 to pi/2?

Thanks
 
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Jaccobtw said:
PROBLEM: I get two different answers when I integrate from 0 to pi/2 and -pi/4 to pi/4. The right answer came from when I used -pi/4 to pi/4.

Doe anyone know why you can't integrate from 0 to pi/2?

Thanks
If the quarter circle goes from ##\theta = 0## to ##\theta = \pi/2##, would there be a net y-component of the electric field as well as a net x-component of the field at the point where you are calculating the field? I'm assuming ##\theta = 0## corresponds to the positive x-axis.
 
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TSny said:
If the quarter circle subtends the angle between ##\theta = 0## amd ##

If the quarter circle goes from ##\theta = 0## to ##\theta = \pi/2##, would there be a net y-component of the electric field as well as a net x-component of the field at the point where you are calculating the field? I'm assuming ##\theta = 0## corresponds to the positive x-axis.
I think this makes sense. Do you mind explaining why I also get the right answer if i integrate from 0 to pi/4 twice?
 
Jaccobtw said:
Do you mind explaining why I also get the right answer if i integrate from 0 to pi/4 twice?
Can you see why integrating from ##-\pi/4## to ##0## contributes the same amount to ##E_x## as integrating from ##0## to ##\pi/4##?
 
TSny said:
Can you see why integrating from ##-\pi/4## to ##0## contributes the same amount to ##E_x## as integrating from ##0## to ##\pi/4##?
Never mind. I think I get it. How could you set up the integral if you wanted to use pi/2 to 0
 
Jaccobtw said:
How could you set up the integral if you wanted to use pi/2 to 0
If the quarter circle extends from the x-axis to the y-axis, so that ##\theta## varies from ##0## to ##\pi/2##, then the integral that you set up will give you ##E_x## when integrated from ##\theta = 0## to ##\theta = \pi/2##. (But think about the sign of ##E_x##.)

How would you set up the integral to get ##E_y## for this case? How would you combine ##E_x## and ##E_y## to get the total electric field?

Why didn't you need to worry about ##E_y## when you integrated from ##-\pi/4## to ##\pi/4##?
 
TSny said:
Why didn't you need to worry about ##E_y## when you integrated from ##-\pi/4## to ##\pi/4##?
Because the y components cancel. I'm confused about how I'd set it up for 0 to pi/2 though to get the magnitude of the electric field. I thought it would be ##cos^2 \theta + sin^2 \theta## but and I got an answer that's kinda close but still off. Any ideas?
 
Jaccobtw said:
Because the y components cancel.
Yes, for the case of ##-\pi/4## to ##\pi/4##, the net y component is zero

Jaccobtw said:
I'm confused about how I'd set it up for 0 to pi/2 though to get the magnitude of the electric field. I thought it would be ##cos^2 \theta + sin^2 \theta## but and I got an answer that's kinda close but still off. Any ideas?
1647355240508.png

For this case, what do you get when you evaluate the integral for ##E_x##? Similarly, what do you get for ##E_y##?

Neither of these components will have ##\theta## in the answer. (##\theta## was the integration variable and the integrals have been done.) So, when you combine ##E_x## and ##E_y## to get the magnitude of the total electric field vector, ##\cos^2 \theta + \sin^2 \theta## will not come into play.
 
TSny said:
Yes, for the case of ##-\pi/4## to ##\pi/4##, the net y component is zeroView attachment 298399
For this case, what do you get when you evaluate the integral for ##E_x##? Similarly, what do you get for ##E_y##?

Neither of these components will have ##\theta## in the answer. (##\theta## was the integration variable and the integrals have been done.) So, when you combine ##E_x## and ##E_y## to get the magnitude of the total electric field vector, ##\cos^2 \theta + \sin^2 \theta## will not come into play.
I honestly have no idea
 
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You said in your first post that you worked out ##E_x## for the case where ##\theta## ranges from ##0## to ##\pi/2##. But you didn't state what you got for the answer for ##E_x##. What did you get?

Setting up an integral for ##E_y## should be very similar. Can you show the integral that you would evaluate to obtain ##E_y##?

Alternately, using symmetry you should be able to see how ##E_y## compares to ##E_x## without actually carrying out the integration for ##E_y##.
 
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