Line charge within a charged shell (basket case)

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SUMMARY

The discussion revolves around calculating the electric field components at a point near an infinite line charge and a charged insulating shell. The linear charge density of the insulating shell, λ2, is determined to be -3.518 μC/m. The x-component of the electric field, Ex(P), is confirmed to be 0 N/C, while the y-component, Ey(P), is calculated to be approximately 728,522.96 N/C using the formula Ey(P) = (2 * k * (λ1 + λ2)) / r, where k is the Coulomb's constant (8.99 x 10^9 N m²/C²) and r is the distance from the line charge.

PREREQUISITES
  • Understanding of Gauss' Law and its application in electrostatics.
  • Familiarity with electric field calculations for line charges and charged shells.
  • Knowledge of charge density concepts, including linear and volume charge densities.
  • Basic integration techniques relevant to electrostatics problems.
NEXT STEPS
  • Study the application of Gauss' Law in different geometries, particularly for cylindrical symmetry.
  • Learn about the concept of superposition in electric fields, especially with multiple charge distributions.
  • Explore resources on integrating charge densities to find electric fields, focusing on cylindrical coordinates.
  • Investigate the behavior of electric fields in conductors versus insulators, particularly in electrostatic scenarios.
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Students studying electromagnetism, particularly those tackling problems involving electric fields from charged objects, as well as educators seeking to clarify concepts related to Gauss' Law and charge distributions.

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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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