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Gauss' Law for a coaxial cable

  1. May 6, 2016 #1
    1. The problem statement, all variables and given/known data

    I have attached the problem

    2. Relevant equations

    E*A = Qenc/ E0

    3. The attempt at a solution

    At the moment I am looking at the problem more conceptually and seeing what is happening at each point and I wanted to know If I was on the right track.

    r<a

    As all charge would reside on the outside of the inner conductor there would be no electric field

    a<r<R

    The electric field would be q/(2pi*r*E1*E0)

    R<r<b

    The electric field would be q/(2pi*r*E2*E0)

    b<r<c

    This is the part that has me puzzled , I thought the inner conductor charge(q) and outer conductor charge (-q) would cancel each other , so there would be no field present? Is this part mean to represent the outer rubber shielding of a coaxial cable?

    c<r

    Would the electric field also be zero outside of the cable due to the two charges cancelling?


    Thanks
     

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  3. May 6, 2016 #2

    TSny

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    OK for the fields you've derived so far.

    For b<r<c you are inside the outer conductor.

    No, I don't think so. Can you see why the net charge of the system is not zero? [EDIT: The field might indeed be zero outside! To get the field outside of the cable use the same method you used for inside.]
     
    Last edited: May 6, 2016
  4. May 6, 2016 #3
    Do the charges not cancel as at any point beyond b you will be at two different distances from the respective charges , hence the electric fields will have a different magnitude?

    For b<r<c would you add the two electric fields?
     
  5. May 6, 2016 #4

    TSny

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    The two conductors have equal and opposite charge. But there could be some induced charge at certain locations of the dielectric. I haven't worked it out.
    Actually, for the field outside the outer conductor, I now think that the field might be zero. I'll try to find time to work on it. But I think you should think about any induced charges in the dielectrics.
    For b<r<c you are inside the outer conducting sheet. What do you know about E inside a conductor?
     
  6. May 6, 2016 #5

    TSny

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    OK, you don't need to worry about the values of the induced charge on the surfaces of the dielectrics in order to answer the questions. You have already worked out the fields inside the dielectrics. You just need to find the field outside the outer conductor. You should be able to do this using the same method that you used for the other regions.
     
  7. May 7, 2016 #6
    Thanks , I have managed to solve the numerical parts as like you say , they are concerned with the fields in the dialectrics.I have checked the answers and the electric fields are shown to be 0 at the point r>b but I don't understand why this would be the case , is it as simple as drawing a Gaussian surface at r=c and saying the enclosed charge would be +q and -q therefore 0?
     
  8. May 7, 2016 #7

    TSny

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    There are two separate regions where r > b that you should consider. First, the region inside the outer conducting sheet: b < r < c. Points in this region are inside the conducting material of the sheet. So, deducing E and D in this region is easy.

    The other region is r > c which consists of all points outside the cable. Here you can use your Gaussian surface and use the fact that the total charge enclosed is zero. Note that there are induced charges on the surfaces of the dielectrics as well as the "free" charge q and -q on the conductors. But, the total induced charge must be zero because the net charge of the dielectrics is zero.
     
  9. May 8, 2016 #8
    Could you expand on the first part ,where b < r < c , what is the significance of points in this region being inside the conducting sheet?

    Thanks
     
  10. May 8, 2016 #9

    TSny

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  11. May 8, 2016 #10
    Last edited by a moderator: May 7, 2017
  12. May 8, 2016 #11

    TSny

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    OK, you are very welcome.
     
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