Line charge within a charged shell (basket case)

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Homework Help Overview

The problem involves an infinite line charge positioned within a thick insulating shell, with specific parameters for charge densities and radii. Participants are tasked with calculating the electric field components at a point outside the shell.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the application of Gauss' law and the integration of charge densities. There are attempts to derive expressions for the electric field components based on the given charge distributions.

Discussion Status

Some participants have provided guidance on how to approach the calculation of the electric field, suggesting methods to treat the system as point charges. Others express confusion about the integration process and the assumptions made regarding the charge distributions.

Contextual Notes

Participants mention constraints related to the lack of instruction from the instructor due to recent snow days, which has impacted their understanding of the material. There is also a reference to the difficulty of the course pacing and the resources available for learning.

hashbrowns808
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1. Homework Statement
An infinite line of charge with linear density λ1 = 6.8 μC/m is positioned along the axis of a thick insulating shell of inner radius a = 2.5 cm and outer radius b = 4.8 cm. The insulating shell is uniformly charged with a volume density of ρ = -667 μC/m3.

1) What is λ2, the linear charge density of the insulating shell?

-3.518247622μC/m

2) What is Ex(P), the value of the x-component of the electric field at point P, located a distance 8.1 cm along the y-axis from the line of charge?

0 N/C

3) What is Ey(P), the value of the y-component of the electric field at point P, located a distance 8.1 cm along the y-axis from the line of charge?

This is where I'm stuck.

Homework Equations


Gauss' law ∫E⋅dA=Q_enc/∈
I know there will be integrations in there but due to a week of snow days the instructor hasn't covered any of that, so I'm not sure if there is something else I'm missing, and I'm not finding any good material that I can extract something from.

The Attempt at a Solution


The first section to the homework was similar, but with a conducting shell. I figured that out with the help of Michael Van Biezen videos, but I don't get how to use charge densities, or how to integrate what.

E∫(πR2)L = ∫dQ/∈ (I'm using ∈ for epsilon naught)
dQ=λdV
dV=∫(from a-b)πL(Ra2-Rb2)
dQ=λπL∫(Ra2-Rb2)
EπR2 = (λπL∫(Ra[/SUB2]-Rb2))/∈
E = (λL∫ab(Ra2-Rb2))/R∈

That's what I have written on my paper. I'm just totally lost and desperate at this point. Like I said my teacher is expecting way too much without much instruction, and I'm sorry for short comings, but I just really need help.

Thanks!
 

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Ey(P) = 2*k(this is 9.0E9)*(Charge density of outer shell * area of outer cylinder + lambda of line) all divided by radius (.081m) let me know if this works out for you
 
marchcha said:
Ey(P) = 2*k(this is 9.0E9)*(Charge density of outer shell * area of cylinder (use length 1) + lambda of line) all divided by radius (.081m) let me know if this works out for you
******length of one is not even needed disregard that
 
marchcha said:
******length of one is not even needed disregard that

I got:

Ey(P) =( 2(8.99810^9)(-667π(.0482-.0252))/.081
= -780964101685
and it was incorrect.
 
hashbrowns808 said:
I got:

Ey(P) =( 2(8.99810^9)(-667π(.0482-.0252))/.081
= -780964101685
and it was incorrect.
what you are trying to do in this problem is act like the system is a point charge so take the lambda you found in the beginning and add it to the lambda given multiply it by two and k and then divide by the radius (0.081)
 
marchcha said:
what you are trying to do in this problem is act like the system is a point charge so take the lambda you found in the beginning and add it to the lambda given multiply it by two and k and then divide by the radius (0.081)

Ok so (((6.8x10^-6)+(-3.518x10^-6))2(8,99x10^9))/.081
=728522.9629

Got it. Thank you so much! I think I'll have to work out that integral backwards.
I'm asking this before I've figured out how to arrive at the formula you gave me, but why can I treat it as two point charges? The x components of the shell cancel, and y components < 0 (along y axis), is it just that the y-comp fields end up averaging to λ1? Does anyone know of a good link where I can learn more about this?

I use Flipit physics, and I find it difficult to follow at best, and like I said we're cramming 3 sections into 1 week, where we'd normally be doing half that, and the teacher hasn't been able to give us much help.

Again thanks Marchcha for the help.
 
hashbrowns808 said:
Ok so (((6.8x10^-6)+(-3.518x10^-6))2(8,99x10^9))/.081
=728522.9629

Got it. Thank you so much! I think I'll have to work out that integral backwards.
I'm asking this before I've figured out how to arrive at the formula you gave me, but why can I treat it as two point charges? The x components of the shell cancel, and y components < 0 (along y axis), is it just that the y-comp fields end up averaging to λ1? Does anyone know of a good link where I can learn more about this?

I use Flipit physics, and I find it difficult to follow at best, and like I said we're cramming 3 sections into 1 week, where we'd normally be doing half that, and the teacher hasn't been able to give us much help.

Again thanks Marchcha for the help.
Hey as a user of flipit physics I feel your pain. You treat it as two point charges because it is outside of the conductor.
 

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