How Does the Electric Field Vary with Distance in a Cylindrical Shell?

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Homework Help Overview

The discussion revolves around the electric field generated by an infinitely long cylindrical metallic shell with a line of charge along its axis. Participants are exploring how the electric field varies with distance from the line of charge, particularly focusing on the implications of Gauss's law.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the application of Gauss's law to derive the electric field as a function of distance, with some emphasizing the need to express the field in terms of charge per unit length. There are attempts to clarify the behavior of the electric field in different regions relative to the cylindrical shell.

Discussion Status

The conversation includes various interpretations of the electric field's behavior, with some participants providing hints and corrections. There is a recognition of the need to express the electric field mathematically, and some participants have indicated understanding of the concepts involved.

Contextual Notes

Participants are considering the implications of an infinitely long cylindrical shape, which allows for uniformity in the electric field due to symmetry. There are discussions about edge effects if the charge were finite, and some participants are questioning the intuitive understanding of the electric field's dependence on the radius.

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Homework Statement



Consider an infinitely long cylindrical metallic shell with a line of charge within and
coincides with the axis of the cylindrical shell as shown in Figure . How does E field vary
with r?


Homework Equations



E.A=q/[tex]\epsilon[/tex]

E=E field, A = surface area

The Attempt at a Solution



The Electric field within the inner circle of cylinder +Q pointing toward outer space.assuming charge at the wire is +Q. however the the area inside the thickness of the pipes has ZERO Electric field because the inner surface of the pipe is induced with -Q, while the outer surface is having total charge of +Q.

Area surrounding the pipe surface having E field pointing outward.

http://img441.imageshack.us/img441/2706/wiredinapipevi8.th.jpg
is this explanation make sense, or how should i write in a more presentable manner? thanks
 
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What you say is correct (except that you use Q instead of the charge per unit length), but you didn't do what was asked: Express the field as a function of r.

Hint: Call the charge per unit length [itex]\lambda[/itex]. Use Gauss's law to find an expression for E(r) in each of those three regions.
 
Well your explanation is quite correct, but you would also want to give the exact expression for the electric field at varying distances from the line of charge. Just use Gauss' law.

Edit: I am gettin old for this lol
 
Doc Al said:
What you say is correct (except that you use Q instead of the charge per unit length), but you didn't do what was asked: Express the field as a function of r.

Hint: Call the charge per unit length [itex]\lambda[/itex]. Use Gauss's law to find an expression for E(r) in each of those three regions.

hi Dr. Al. ok, here is the derivation of the E(r) and r relationship.

[tex]\Phi[/tex]=E A = Q / [tex]\epsilon[/tex].

therefore, E = [tex]\frac{\lambda}{2\pi\epsilon*r}[/tex].

[just couldn't get the latex working]
The E field is = lamba / (2*pi*r*epsilon) ]


From this, we predicted the E field is inversely proportional to the distance from the wire to the pipe, r. however the only exception is when E field is inside the wall of the pipe. it is ZERO as mention above.
 
Last edited:
arunbg said:
Well your explanation is quite correct, but you would also want to give the exact expression for the electric field at varying distances from the line of charge. Just use Gauss' law.

Edit: I am gettin old for this lol



LOL, my explanation is at post #4. thanks for the reply.
 
Looks good to me! (I'd mention that you used a cylindrical Gaussian surface. If its length is L, the charge within that surface is [itex]\lambda[/itex] L.)
 
Doc Al said:
Looks good to me! (I'd mention that you used a cylindrical Gaussian surface. If its length is L, the charge within that surface is [itex]\lambda[/itex] L.)

yeah, q= [itex]\lambda[/itex]* length
while derive it, length was cancel out with the cylinder length.

btw, my final doubt is, since we are ask to consider a INFINATELY long cylindrical shape, we still consider it as length, L. which only this that my explanation can establish.
 
Cosidering an infinitely long cylinder allows you to assume that the field is uniform and radial (by symmetry) in your Gaussian section, regardless of where along the axis you place it. If the pipe or line charge were finite, and you were near the end, you'd expect some non-radial components (edge effects).
 
Doc Al said:
Cosidering an infinitely long cylinder allows you to assume that the field is uniform and radial (by symmetry) in your Gaussian section, regardless of where along the axis you place it. If the pipe or line charge were finite, and you were near the end, you'd expect some non-radial components (edge effects).

Hi Doc, i finally got the whole big picture of this. just a minor clarification, [regardless of where along the axis you place it.] are you referring to the position of the charged wires is not necessary at the centre of the pipe? because i feel this is not real intituitive, as the formula suggest, the E field do depend on the radius.correct me if i m wrong and misinterpret the meaning.


{If the pipe or line charge were finite, and you were near the end, you'd expect some non-radial components (edge effects)} this part i can understand. thanks again.
 
  • #10
hi Doc, i finally got your meaning of your post #08. please marked this thread as solved!.thanks .
 
  • #11
Excellent. (Looks like I forgot to respond to your last post. Oops! But you have it now.)

As far as marking the thread solved, you should be able to do it: Click on thread tools and you should see an option. :cool:
 

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