Work required to move a charged ball

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Homework Help Overview

The problem involves calculating the work required to move a charged ball into the center of a charged ring. The context is electrostatics, specifically dealing with electric potential energy and work done in moving charges in an electric field.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the use of electric potential and energy equations, with some attempting to derive the potential energy from electric field calculations. There is also a focus on the integration process for determining energy contributions from the charge distribution on the ring.

Discussion Status

Some participants are exploring different methods to relate electric field and potential energy, while others are questioning the integration steps and the assumptions made about charge distribution. There is a mix of approaches being considered without a clear consensus on the best method to proceed.

Contextual Notes

Participants note potential confusion regarding the relationship between electric field and potential energy, as well as the relevance of the mass of the ball in the context of gravitational effects, which may not be directly related to the primary problem of electrostatics.

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Homework Statement


A ring of diameter 7.10 cm is fixed in place and carries a charge of 5.00 μC uniformly spread over its circumference. How much work does it take to move a tiny 3.40 μC charged ball of mass 1.70 g from very far away to the center of the ring?

Homework Equations


I tried using: W=-\Delta U

The Attempt at a Solution


We know that when the ball is very far away U=0J

Then to find the potential energy when the ball is in the center of the ring I did:
Change in charge is 5.00X10^{-9}C/2\pi(0.0710m)=1.12X10^{-8}C/m

\int \frac{k*q*dq}{r} ds from 0 to 2pi.

\frac{k*q*dq}{r} \int ds from 0 to 2pi.

\frac{8.988X10^{9}N*m^2/C^2*3.40X10^{-9}C*1.12*10^{-8}C/m}{0.0710m} \int ds from 0 to 2pi =3.031X10^-5J.

W=-\Delta U=-(3.031X10^-5J-0J)=-3.031X10^-5J
 
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I'm having trouble following your integral from the first line. I'm thinking V = kq/r for a point charge so dV = k/r*dq, where r is the radius of the ring.
Ah, you are doing energy E = QV so dE = QdV = kQ/r*dq
I'm using q for the charge on the ring, Q for the charge on the particle.
Your s must be something to do with the arc length going round the ring.
So dq = q/(2*pi*r)*ds
Using s = r*A where A is the angle running from 0 to 2pi, you get ds = r*dA and
dq = q/(2*pi)dA
so the integral is dE = kQq/(2*pi*r)*dA from A = 0 to 2*pi.
The nice thing about this integral is that nothing depends on the angle so
integral 0 to 2*pi of dA is just 2*pi.
E = kQq/r.
Well, I guess we didn't need to integrate at all! Because all the charge is the same distance from the center point.
 
I'm still slightly confused. So I can find E at the center of the ring using E=kQq/r. But, since W=-(U_f-U_i) how do I get U from E? Since E=kq/r^2 and U=kq_1*q_2/r would you just multiply the E you get by qr and if so what q would you use: the charge on the ring or the charge on the ball? Thanks for your help.
 
Try this approach. Find E as a function of r along the axis of the ring using integration. Then

V=-\int_{\infty}^{r}\mbox{Edr}

The work done is

W=Vq

Is the mass in a gravitational field also and if so what is the orientation of the ring axis with the field?
 

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