Maxwell's Equations: B-field induced from changing E-field

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Homework Help Overview

The discussion revolves around a problem involving a parallel plate capacitor with circular plates, where a sinusoidal potential difference is applied. The participants are exploring the relationship between the changing electric field and the induced magnetic field as described by Maxwell's equations.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • The original poster attempts to calculate the induced magnetic field using Maxwell's equations, specifically applying the relationship between the electric field and the magnetic field. Some participants question the correctness of the electric field calculation and the assumptions made regarding the geometry of the capacitor.

Discussion Status

There is an ongoing exploration of the problem, with participants providing feedback on the original poster's approach. Some guidance has been offered regarding the need to clarify what is being solved for, and there is acknowledgment of errors in the calculations presented. The discussion reflects a collaborative effort to refine the understanding of the problem.

Contextual Notes

Participants note potential errors in the setup, including the distance used in calculations and the specific parameters of the capacitor. There is a recognition of the complexity of the problem and the challenges faced in deriving the correct expressions.

Bryon
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Homework Statement


Parallel plate capacitor with circular plates with radius of 26mm and a plate separation of 6mm. A sinusiodal potential difference is applied across the capacitors plates with Vmax = 170V at a frequency of 60Hz.

170sin(2*pi*60Hz*t)

Homework Equations


V = ∫E∙dl = El (l is the distance)

Maxwell-Ampere
∫B∙dl = u0(I + ε0(dΦe/dt))

A = pi*r^2

e/dt = dEA/dt = A(dE/dt)

The Attempt at a Solution




B2*pi*r = u00*A(dE/dt)

E = 170sin(2*pi*60Hz*t)/(0.003)V/M (I used the distance between the plates to find the e-field).

dE/dt 170sin(2*pi*60Hz) = 20400*pi*cos(120*pi*t)/(0.003)

∫B∙dl = B*2*pi*r

B*2*pi*0.013 = u00*(pi*0.026^2)* 20400*pi*cos(120*pi*t)/(0.003)

B = 6.17711x10^-12 T

I thought I was on the right track, but it turns out that this was not correct. I think this was my best approach to the problem and at this point I do not know what else to try. I have a feeling that the electric field is not correct but I do not see what is wrong with it. Any suggestions?
 
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Anyone? I know, its a toughy, but I figured a second pair of eyes could point me in the right direction.
 
Wow, no one. Well, at least I am not alone! lol
 
You didnt state what you are solving for. I am assuming the maximum strength of the b field?
 
Thanks! I was forgetting something. lol. I also noticed I made another error when I copied it over from my work...Yeah, I'm frustrated with this one and all the others problems that are asking about the magnetic field.

(a) What is amplitude of the induced magnetic field a distance 13 mm from the center axis joining the plates?

B2*pi*r = u0 *ε0*A(dE/dt)

E = 170sin(2*pi*60Hz*t)/(0.003)V/M (I used the distance between the plates to find the e-field).

dE/dt 170sin(2*pi*60Hz) = 20400*pi*cos(120*pi*t)/(0.006) <---should be 6mm instead of the 3mm
∫B∙dl = B*2*pi*r

B*2*pi*0.013 = u0 *ε0*(pi*0.026^2)* 20400*pi*cos(120*pi*t)/(0.006)

B = 9.83117439x10^-13 T
 
Last edited:

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