Solving Charged Circular Arc Problem: Q, R, \Delta E_x

In summary, the electric field at the origin due to the charge element located at an angle subtended by an angular interval in quadrant 4 is 151205 N/C.
  • #1
Punchlinegirl
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A uniformly charged circular arc AB is of radius R covers a quarter of a circle and is located in the second quadrant. The total charge on the arc is Q > 0. This problem has 4 parts, I got the first 2.
1. The direction of the electric field E due to the charge distribution at the origin is in quadrant 4.
2. Determine [tex] \Delta E_x [/tex], the x-component of the electric field vector at the origin O due to the charge element [tex] \Delta q [/tex] locate at an angle [tex] \theta [/tex] subtended by an angular interval [tex]\theta [/tex].
[tex] \Delta E_x = kQ/R^2 * 2\Delta \theta / \pi * cos \theta [/tex]
3. Find E_x, the electric field at the origin due to the full arc length for the case where Q= 2.3 [tex]\mu C[/tex] and R= 0.37 m. Answer in units of N/C.

I have no idea how to find the value for theta. Can someone tell me what I should do?
 
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  • #2
You're not looking for *a* value of theta, you're looking for a range of values. That's because you have to integrate the expression that you found in part 2.

So between what two angles is the second quadrant bounded?
 
  • #3
The arc is bounded between [tex] \pi [/tex] and [tex] \pi /2 [/tex].
so when I go to integrate it, would it just be the integral just be 2 [tex] \Delta \theta cos \theta [/tex]? Since kQ/r^2 [tex] \pi [/tex] is all constant?
 
  • #4
Your latex isn't loading for me...
cos(theta) is NOT constant, but all the other terms are.
you have to integrate cos(theta) from 0 to pi/2 .
 
  • #5
So if I integrate I get
[tex] KQ/r^2 2 \Delta/ \pi sin \theta [/tex] from pi/2 to 0.
I'm assuming Delta pi would just be pi/2-0= pi/2.
So plugging in gives me,
2.3 x 10^-6 k/(.37)^2 * 2(pi/2)/pi * sin pi/2
Which = 151205 N/C
This isn't right.. I think my delta theta is messed up.
Also, why wouldn't the bounds be pi and pi/2 since it's located in the 2nd quadrant?
 
  • #6
What? [tex] \Delta \theta = d \theta [/tex] , which is your integration variable!

We can't tell where you're measuring theta from , without a diagram.
The result is the same, either way.
 
  • #7
anyone?
 

FAQ: Solving Charged Circular Arc Problem: Q, R, \Delta E_x

What is the "Charged Circular Arc Problem"?

The Charged Circular Arc Problem refers to a physics problem that involves calculating the electric field at a point due to a charged particle moving along a circular arc. This problem is commonly encountered in electromagnetism and is important in understanding the behavior of charged particles in electric and magnetic fields.

How are Q, R, and ΔEx related in the Charged Circular Arc Problem?

In the Charged Circular Arc Problem, Q represents the charge of the particle, R represents the radius of the circular arc, and ΔEx represents the change in the x-component of the electric field at a point. These variables are related through mathematical equations and can be used to solve the problem.

What is the significance of solving the Charged Circular Arc Problem?

Solving the Charged Circular Arc Problem is important in understanding the behavior of charged particles in electric and magnetic fields. It allows scientists to predict and control the movement of charged particles, which is crucial in many areas such as particle accelerators, electronics, and medical imaging.

What are the key steps in solving the Charged Circular Arc Problem?

The key steps in solving the Charged Circular Arc Problem include identifying the variables (Q, R, and ΔEx), understanding the equations that relate these variables, and applying these equations to calculate the electric field at a specific point. It is also important to properly consider the direction and magnitude of the electric field at different points along the circular arc.

Are there any real-world applications of the Charged Circular Arc Problem?

Yes, there are many real-world applications of the Charged Circular Arc Problem. Some examples include the design and operation of particle accelerators, the analysis of magnetic fields in motors and generators, and the calculation of electric fields in electronic devices. Additionally, this problem has applications in medical imaging techniques such as magnetic resonance imaging (MRI).

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