How Does Connecting Two Spheres Affect Charge Distribution?

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Homework Help Overview

The problem involves two conducting spheres, one charged and the other initially uncharged, and examines how connecting them with a wire affects the charge distribution. The context is rooted in electrostatics, specifically focusing on electric potential and charge distribution in conductive materials.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the relationship between charge distribution and electric potential when the spheres are connected. There are attempts to derive formulas relating charge, radius, and electric potential. Questions arise about the nature of electric potential and electric field in determining force per unit charge.

Discussion Status

Some participants have provided insights into the equations governing electric potential and charge distribution, while others are exploring the implications of the instructor's comments regarding equal potential across the spheres. The discussion reflects a mix of conceptual understanding and mathematical exploration, with no explicit consensus reached.

Contextual Notes

Participants are working under the assumption that the spheres are far apart relative to their sizes, and there is a focus on understanding the implications of connecting the spheres via a wire. The discussion also highlights the challenge of finding relevant equations in textbooks related to the problem.

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Homework Statement



In the figure, r1 = 2 and r2 = 8 cm. Before the conducting spheres are connected by the wire a charge of 6.0×10-7 C is placed on the smaller sphere while the larger sphere is uncharged. Calculate the charge on the smaller sphere after the wire is connected. Assume that the separation of the spheres is very large compared to their radii.

(Figure shows a small sphere on the left with a wire attaching it to a larger sphere on the right)

Homework Equations


The Attempt at a Solution

When the spheres are wired together the charge travels to the larger one also, and is now spread evenly along the surface of both spheres. The charge on the smaller one should be the fraction of the surface area of the small sphere over the total surface area of both spheres times the total charge, q.

q * 4pir1^2 / (4pir1^2 + 4pir2^2) = qr1^2 / (r1^2 + r2^2).

--Instructor reply: "The charge distribution is not a simple function of the ratio of the surface areas. The key for this problem is that the wire means that the skins for both spheres will be at the same electric potential."

--- me, now: I don't know what to do... T_T
 
Last edited:
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What is the electric potential just above the surface of a charged conducting sphere?
 
gneill said:
What is the electric potential just above the surface of a charged conducting sphere?

I think it's pretty high because there is a lot of force acting on a test charge at that point, and so there is a lot of potential energy per charge, which is electric potential.
 
Is potential or electric field the one that decides force per unit charge?
 
A formula would be nice. Something involving the charge on the sphere, q, and the radius of the sphere, R.
 
Piyu said:
Is potential or electric field the one that decides force per unit charge?

It's electric field.
 
gneill said:
A formula would be nice. Something involving the charge on the sphere, q, and the radius of the sphere, R.

yeah, I know. Do we have anything that has area and q? I don't know. We have these formulas for electric potential symmetry --for shereical: delV = kQ (1/rf - 1/ri)

and planar, but I don't think it's planar. I don't know what equation to use..

I can't find any equations in my book relating V to A and Q...

or E to A and Q either, because E = kq/r^2 for outside the surface of a conducting sphere...
 
My instructor says that the electric potential for both spheres is the same...

this ended in the correct answer... typed it out because I got it wrong at first because I made an algebra mistake, caught while typing it...

so V1 = V2
kq1/r1 = kq2/r2, q1 + q2 = qT --> q2 = qT - q1

q1 = (qT - q1)r1/r2

q1 = r1qT/r2 - r1q1/r2

q1 +
 
Last edited:
Ok, just wanted to add some feed back for people who didn't get what you did ; )

First, think of qTotal as the sum of q1 old + q2 old. Remember that q2 old is 0, so qTotal is just q1 old.

We now look at our equation
dv1 = dv2
k*q1/r1 = k*q2/r2

We are trying to solve for q1. qTotal is still equal to q1 new + q2 new. This means that we can substitute it in.

q2 = (r2/r1)*q1

Remember qTotal = q1+q2

q2 = qTotal - q1

qTotal - q1 = (r2/r1)*q1
qTotal = q1 + (r2/r1)*q1
qTotal = q1 (1 + r2/r1)

q1 = qTotal/(1 + r2/r1)

You know qTotal, r2, and r1, so just plug and chug.
 

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