Nonconducting spherical shell with uniform charge

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Homework Help Overview

The discussion revolves around determining the electric field within a nonconducting spherical shell that has a spherical cavity. The problem specifically addresses the region between the inner radius (r1) and the outer radius (r0) of the shell, with a uniform charge distribution.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the application of Gauss's law and the implications of charge density in deriving the electric field. There are questions about the correct expression for charge density and how to calculate the enclosed charge within a Gaussian surface.

Discussion Status

Participants are actively engaging with the problem, questioning assumptions about charge density and the relationship between electric field and charge. Some have provided guidance on using Gaussian surfaces and the implications of the charge distribution, but no consensus has been reached on the final expression for the electric field.

Contextual Notes

There are discussions about the correctness of the charge density formula and the need for clarity in the mathematical expressions used. Participants are also exploring the implications of the spherical shell's geometry on the electric field calculations.

ooohffff
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Homework Statement


Suppose the nonconducting sphere of Example 22-4 has a spherical cavity of radius r1 centered at the sphere's center (see the figure). Assuming the charge Q is distributed uniformly in the "shell" (between r = r1 and r = r0), determine the electric field as a function of r for the following conditions.

r1 < r < r0

22-31.gif


Homework Equations


Gauss's law

The Attempt at a Solution



I know the electric field is 0 in the inner cavity. The electric field outside of the shell is Q/(4pi*E0*r^2). How would I derive the equation for the electric field inside the shell? Charge per unit volume should be p=Q/(4/3*pi(r0-r1)^3) right?
 
Last edited:
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ooohffff said:

Homework Statement


Suppose the nonconducting sphere of Example 22-4 has a spherical cavity of radius r1 centered at the sphere's center (see the figure). Assuming the charge Q is distributed uniformly in the "shell" (between r = r1 and r = r0), determine the electric field as a function of r for the following conditions.

r1 < r < r0

22-31.gif


Homework Equations


Gauss's law

The Attempt at a Solution



I know the electric field is 0 in the inner cavity. The electric field outside of the shell is Q/(4pi*E0*r^2). How would I derive the equation for the electric field inside the shell? Charge per unit volume should be p=Q/(4/3*pi(r0-r1)^3) right?
That charge density is incorrect.

A3 - B3 ≠ (A - B)3 .
 
SammyS said:
That charge density is incorrect.

A3 - B3 ≠ (A - B)3 .

Mmm yes, your'e right it should be Q/(4pi/3(r0^3-r1^3)). But where do you go from there?
 
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ooohffff said:
Mmm yes, your'e right it should be Q/(4pi/3(r0^3-r1^3)). But where do you go from there?
How much charge there interior to a sphere of radius, r, where r1 < r < r0 .
 
SammyS said:
How much charge there interior to a sphere of radius, r, where r1 < r < r0 .

Could you rephrase that and be more specific?
 
Would it be the same as the electric field outside the sphere?
 
ooohffff said:
Would it be the same as the electric field outside the sphere?
No, electric charge is not equal to electric field.

You want to find what the electric field is interior to the "shell". That's where r1 < r < r0 .

You mention Gauss's Law.
 
SammyS said:
No, electric charge is not equal to electric field.

You want to find what the electric field is interior to the "shell". That's where r1 < r < r0 .

You mention Gauss's Law.

Right its

∫E⋅da=qenc0

So I keep getting E4πr^2=qenc0

so that would mean E would equal the same as the electric field as the outside of the sphere, which I know is wrong. What am I doing wrong?
 
ooohffff said:
Right its

∫E⋅da=qenc0

So I keep getting E4πr^2=qenc0

so that would mean E would equal the same as the electric field as the outside of the sphere, which I know is wrong. What am I doing wrong?
For r between r1 and r0, what do use for your Gaussian surface?
 
  • #10
SammyS said:
For r between r1 and r0, what do use for your Gaussian surface?

Would it be r1^2 instead of r^2?
 
  • #11
ooohffff said:
Would it be r1^2 instead of r^2?
No.

If you want to know the electric field at a distance r from the origin, use s sphere of radius r.

How much electric charge is enclosed within this sphere?

In the case of your problem the only charge inside this sphere resides in the spherical shell with inner radius r1 and outer radius r. Right ?

So, how much charge is that ?
 
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  • #12
So if charge density =

Q/ (4π/3 ( r03-r13)) = qenc/(4π/3 (r3-r13)).

Then,

Q(r3-r13) = qenc (r03-r13)

qenc = [Q(r3-r13)] / (r03-r13)

E4πr2 = Q(r3-r13)] / ε0(r03-r13)

E = Q(r3-r13)] / 4πr2ε0(r03-r13)
 
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  • #13
Can someone verify this?
 
  • #14
ooohffff said:
Can someone verify this?
Patience.

ooohffff said:
So if charge density =

Q/ (4π/3 ( r03-r13)) = qenc/(4π/3 (r3-r13)).

Then,

Q(r3-r13) = qenc (r03-r13)

qenc = [Q(r3-r13)] / (r03-r13)

E4πr2 = Q(r3-r13)] / ε0(r03-r13)

E = Q(r3-r13)] / [4πr2ε0(r03-r13) ]

That's the right idea. To be perfectly correct, the entire denominator should be enclosed in parentheses, else use some other grouping symbol.
 
  • #15
SammyS said:
Patience.
That's the right idea. To be perfectly correct, the entire denominator should be enclosed in parentheses, else use some other grouping symbol.

Haha, thank you SammyS!
 

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