Nonconducting spherical shell with uniform charge

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SUMMARY

The discussion focuses on determining the electric field within a nonconducting spherical shell with a uniform charge distribution, specifically for the region where the radius r falls between r1 and r0. Participants clarify that the electric field inside the cavity (r < r1) is zero, while the electric field outside the shell is given by the formula Q/(4πE0r²). The correct charge density is established as Q/(4π/3(r0³ - r1³)), leading to the derivation of the electric field formula for the shell region using Gauss's Law.

PREREQUISITES
  • Understanding of Gauss's Law
  • Familiarity with electric fields and charge distributions
  • Knowledge of spherical coordinates and volume charge density
  • Basic calculus for deriving electric field equations
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  • Study the application of Gauss's Law in nonuniform charge distributions
  • Learn about electric field calculations in spherical coordinates
  • Explore the concept of charge density and its implications in electrostatics
  • Investigate the behavior of electric fields in different geometrical configurations
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Students and educators in physics, particularly those focusing on electrostatics, as well as engineers and researchers dealing with electric field calculations in spherical geometries.

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)
 
Last edited:
  • #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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