Charged Sphere with a Hole - Check my work?

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Homework Help Overview

The problem involves a uniformly charged spherical shell with a hole, where the charge density is zero in a specific region. The objective is to determine the electric field as a function of the position along the z-axis, considering the effects of both the charged sphere and the disk created by the hole.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • The original poster attempts to use the principle of superposition to combine the electric fields from the charged sphere and the disk with a negative charge density. Some participants question the validity of the equations used for different regions along the z-axis.

Discussion Status

Participants are exploring the conditions under which the equations for the electric fields apply, particularly regarding the regions inside and outside the sphere. There is a recognition of the need to adjust the equations based on the position of the disk relative to the origin.

Contextual Notes

There is a discussion about the implications of Gauss' Law for the electric field inside the sphere, particularly concerning the lack of enclosed charge. The original poster expresses uncertainty about the direction of the electric field contributions from the disk.

Raen
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Charged Sphere with a Hole -- Check my work?

Homework Statement



You have a spherical shell of radius a and charge Q. Your sphere is uniformly charged except for the region where θ<= 1° (which has σ = 0).
Imagine that your fi eld point is somewhere on the positive z-axis (so z could be larger or smaller than a). Determine E as a function of z.

I believe I can represent this as a uniformly charged sphere without a hole and a thin disk with a charge density of -σ. Then the law of superposition let's me add the two together. I think I did it right, but before I go on to the computer program portion of the assignment, I'd love if somebody would double-check my logic and work. If you see an error, please let me know. If you think it's correct, let me know that, too.

Homework Equations



sin(1°) = r/a Where r is the radius of the disk. r = sin(1°)a = 0.017a

E field of a sphere: E(r) = Q/(4∏r2ε0) = σa2/(r2ε0)

E field of a disk: E(z) = q/(2∏ε0(0.017a2)*(1-z2/(√z2+(0.017a)2))

The Attempt at a Solution



Along the z-axis, the E field of the sphere can be written as E(z) = σa2/(z2ε0)

Therefore, Etotal = σa2/(z2ε0) + q/(2∏ε0(0.017a2)*(1-z2/(√z2+(0.017a)2))

or

Etotal = σ/ε0*(a2/z2 - 1/2 + z/√(z2 + (0.017a)2)

Is this correct? I'm sorry if it's messy and thank you, thank you in advance.
 
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Both equations (for disk+sphere) are true in a specific range of z (inside or outside?) only.
It might be useful to calculate the field for both cases individually.
 


I know the equation I have for the sphere contribution only works outside of the sphere, because the electric field inside a (normal) uniformly charged sphere is zero. The field around the disk, though, I thought would look the same in both directions. That would make the Etotal in my initial post the Etotal outside the sphere, while inside the sphere it would be

Etotal = -σ/(2ε0)*(1-z/√(z2+(0.017a)2))
 


The magnitude is the same, but the direction is not.
 


Right, it would be in the opposite direction...but now I'm confused. Going by Gauss' Law, inside the sphere the E field will still be zero, won't it? Even with the little disk there's still no enclosed charge inside the sphere and therefore no E field...
 


Raen said:


E field of a disk: E(z) = q/(2∏ε0(0.017a2)*(1-z2/(√z2+(0.017a)2))



This holds if the disk's center is at the origin, at z=0. But this disk is at z = a , so in your equation make the substitution z → z-a . I think that the rest are correct...
 

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