How Does Charge Distribution Affect Electric Potential in a Metallic Shell?

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Homework Help Overview

The discussion revolves around the electric potential and charge distribution in a metallic shell with a central point charge. The problem involves determining the location of the equipotential surface, calculating the electric potential of the shell, and expressing the potential as a function of distance from the center.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the implications of charge distribution within and outside the metallic shell, questioning the nature of electric potential at the center and within the shell. There are discussions about using Gaussian surfaces to find electric fields and potential, as well as concerns about unit conversions and calculation methods.

Discussion Status

Participants are actively engaging with the problem, raising questions about the assumptions regarding electric potential and charge distribution. Some guidance has been offered regarding the use of Gaussian surfaces and the interpretation of potential within different regions of the shell.

Contextual Notes

There are indications of confusion regarding the definitions of electric potential and the behavior of conductors, particularly in relation to the charge distribution and the implications of using certain values for calculations.

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Homework Statement


A +30 mC point charge sits at the center of a spherical thick metallic shell, of 4.0 cm inner radius and 2.0 cm thickness. The net charge of the shell is -50mC. a.) Determine the location of the 0 volt equipotential surface. b.) calculate the electric potential of the metallic shell. c.) Give the expression for the electric potential in the entire space, V(r) as a function of the distance from the center. Sketch the graph of V(r)


Homework Equations


V = kQ/r
E = kQ/r2



The Attempt at a Solution



a.) I believe the location will be anywhere inside the metallic shell, because it is a conductor.

b.) V = kQ/r = ((8.99 x 109 N(m/C2)(-50mC))/(2.0cm)
= 2247.5V
i don't think this is right. i think my biggest issue is converting units.

c.) For this i think it is the sum of the electric potential of the inside and the electric potential of the outside.
V = ((8.99 x 109 N(m/C2)(+30mC))/(2.0cm) + ((8.99 x 109 N(m/C2)(-50mC))/(2.0cm)
= ?
 
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Zarrey said:
a.) I believe the location will be anywhere inside the metallic shell, because it is a conductor.
I'm not sure whether you mean within the space enclosed by the metallic shell, within the body (annulus) of the shell, or both. But the answer is wrong in each interpretation.
In the annulus there is no field, but there would be a potential. I would suggest starting by figuring out the potential just outside the shell, then thinking about what that implies for the potential in the annulus, and finally consider the potential within the cavity.
As a hint for the first step, what is the potential (or what is the field if that's easier) outside a uniformly charged thin shell?
 
If i were to find the field just outside i would do:

Qtotal/(4πε0r2) ??

what would i use for r? my teacher has told us in the past if we were to solve for something that is slightly larger than something else, in this case the gaussian surface, to use +1.0 cm larger than the radius. would it be safe to solve using 7.0cm as the r value?
 
Last edited:
Zarrey said:
If i were to find the field just outside i would do:

Qtotal/(4πε0r2) ??
Yes. By symmetry, the charges at the shell can be considered as many thin spherical shells with uniform charge. (Actually, all the charge will be on either the outer surface or the inner surface, right?). So all charges less then r from the centre can be treated as though at the centre for this calculation.
what would i use for r? my teacher has told us in the past if we were to solve for something that is slightly larger than something else, in this case the gaussian surface, to use +1.0 cm larger than the radius. would it be safe to solve using 7.0cm as the r value?
Strange advice. I mean at an infinitesimal distance outside, so just use 6cm.
 
would the answer for letter a.) be the center then because if you were to find the potential the r value would be 0 which would cause the answer to be infinite?

for b.) would you use Va - Vb?

when i go to plug in my equation in my calculator i try to do conversions on the fly. when i find the answer its an outrageous amount, over a million usually, so i think i am doing something wrong.
 
Zarrey said:
would the answer for letter a.) be the center then because if you were to find the potential the r value would be 0 which would cause the answer to be infinite?
The potential must be zero because it's infinite? Weird logic.
for b.) would you use Va - Vb?
Let's get past (a) first.
when i go to plug in my equation in my calculator i try to do conversions on the fly. when i find the answer its an outrageous amount, over a million usually, so i think i am doing something wrong.
And if you happen to get something reasonable you presume it's right? Not a recommended approach. Monkeys on typewriters come to mind.
 
Ok so working on a then.

am i wrong in saying that the center will cause no electric potential? the value of r would be 0 which would cause the whole denominator to be 0, which would cause the equation to be undefined.

from what i understand the metallic shell is a conductor. and conductors do not carry a charge on the inside. and if you were to use the equation and plug 0 in for Q it would cause the equation the equal 0.

i don't know if any of this is correct. I have been having problems in physics recently because most of my attention was focused on one of my other classes.
 
Zarrey said:
am i wrong in saying that the center will cause no electric potential?
Yes (that's wrong).
from what i understand the metallic shell is a conductor. and conductors do not carry a charge on the inside.
No charge on the interior of the conductor. In this case that is the annulus between the inner surface and the outer surface. Those two surfaces will carry charges.
 

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