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E-field from Time Varying B-field of Current Loop

  1. Jul 17, 2008 #1
    I am trying to calculate the E-field from a varying B-field. The B-field is from a current loop.

    [tex]\vec{B}(\vec{r},t)=\vec{B_{0}}(\vec{r})Sin(\omega t)[/tex]

    where [tex]\vec{B_{0}}=[/tex] B-field for current loop

    Now since B is varying with time there should be an electric field. Since B is harmonic E should also vary harmonically but with a phase delay. I am assuming that omega is small enough and the length scales are small enough that this can be treated quasi-static. If I assume E takes this form...
    [tex]\vec{E}(\vec{r},t)=\vec{E_{0}}(\vec{r})Cos(\omega t)[/tex]

    then faraday's equation gives
    [tex]\nabla \times \vec{E_{0}}=-\omega \vec{B_{0}}[/tex]
    I tried to solve for E this way but I am not sure if it is possible to do analytically since it involves elliptic integrals. I attempted to integrate using Mathematica but that didn't work either. I can go into more detail on this approach but I do not feel like it will work.

    The other way I attempted was to us ampere's equation. This would give [tex]\nabla \times \vec{B_{0}}=-\frac{\omega}{c^{2}} \vec{E_{0}}[/tex]
    This seemed like it would be nice and easy but it didn't work out either. Here is what I did.
    [tex]\nabla \times \vec{B_{0}}=\frac{1}{r}(\frac{\partial B_{z}}{\partial \theta}-r\frac{\partial B_{\theta}}{\partial z})\hat{e_{r}} +
    (\frac{\partial B_{r}}{\partial z} - \frac{\partial B_{z}}{\partial r})\hat{e_{\theta}} +
    \frac{1}{r}(\frac{\partial}{\partial r} (r B_{\theta}) - \frac{\partial B_{r}}{\partial \theta} )\hat{e_{z}}[/tex]
    well we already know [tex]\vec{B_{\theta}}=0[/tex] and that there is no dependence on [tex]\theta[/tex] for [tex]\vec{B_{r}}[/tex] and [tex]\vec{B_{z}}[/tex] so
    [tex]\nabla \times \vec{B_{0}}= (\frac{\partial B_{r}}{\partial z} - \frac{\partial B_{z}}{\partial r})\hat{e_{\theta}}[/tex]
    I first tried to take these derivative by hand but after I had worked it all out (it gets kind of long) I decided to let Mathematica do it and see what it gave. I attached the notebook. Well Mathematica give 0 as the derivative. Right off the bat that does not seem right since looking that the vector field it is obvious that there should be a theta component in the curl. Also this would suggest that there is no E-field from a changing B-field which isn't right either.

    I do not really want to finish working through the derivatives by hand since they are messy and this point I will have no idea if I am right since if they cancel then it agrees with mathematica but seems unphysical and if they don't cancel then it would probably but to messy to know if it is right.

    Any ideas on how to determine the E-field in this case? I would be exterminly happy also if someone was to just point to the literature where this has already been treated. I had a hard time searching for it since I don't know the proper keywords to use.

    This problem is a part of the research that I am working on. I will be using these fields in a particle tracing code. It has really had me stuck for a while.

    Thank you very much for any help or suggestions. I am willing to provide any clarifications that are necessary.
     

    Attached Files:

    Last edited: Jul 17, 2008
  2. jcsd
  3. Jul 17, 2008 #2
    So you have a loop with ac current and you wish to find the E field. Off the cuff, here is how I'd approach it. Ampere's law, AL, relates the magnetic field with the current, B as a function of I. Ohm's law, OL, relates the current density with the electric field, J = sigma*E, where J is in amp/m^2, and sigma is conductivity in mho/m. Then there is Faraday's law, FL.

    The boundary condition that must be met is that the E field must comply with OL. The line integral of the E field around the loop equals the voltage around the loop along a particular path, and OL is V=I*R. You should be able to solve it. If the loop is superconducting, then the E field generated by the ac B field exactly cancels the E field of the generating source, hence the net is zero, in compliance with OL.

    Have I helped? BR.
     
  4. Jul 18, 2008 #3
    I believe what you are referring is the E-field in the loop. The E that is responsible for the current. But I am not interested in the inside of the current loop. Maybe I am misunderstanding what you are suggesting but I do not feel like it would produce the E-field in the regions about the current loop.

    I just want the fields that result from the time varying B.

    A recent thought that I have was that I could use the magnetic potential to get E.
    [tex]\vec{B}=\nabla \times \vec{A}[/tex]
    I pointed out before that since the fields are harmonic in time then
    [tex] \nabla \times \vec{E_{0}}=-\omega \vec{B_{0}} [/tex]
    so
    [tex] \nabla \times \vec{E_{0}}=\nabla \times (-\omega \vec{A})[/tex]
    so
    [tex] \vec{E_{0}} = -\omega \vec{A} + \nabla f [/tex] where f is a scalar field
    right? Well the magnetic potential is given for a current loop in Jackson EM. I am not sure how I would begin to determine [tex] \nabla f [/tex]. Looking at the fields with Matlab it seems that [tex] \nabla f = 0[/tex] but I have no way to show it.

    Any suggestions?
     
  5. Jul 18, 2008 #4
    E = - dA/dt. This relation is for time varying magnetic fields with no charges present. With charges present, the E field is E = - grad V.

    If both charges and time varying magnetic fields are present:

    E = - grad V - dA/dt.
     
  6. Jul 18, 2008 #5
    Ah ok good. That is what I had figured. I was later able to reason that my scalar field must be zero everywhere since it would correspond with charges. So it is good that you pointed it out because now I know I was thinking about it correctly. Thank you.
     
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