- #1
Hoofbeat
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Hi, I have the following question on my problem sheet, and I just want to check that my answer to it is correct as I need to use the result in a later problem. If someone could confirm it is correct, or point out mistakes/erros that would be great.
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Q. Derive the wave equation for E in empty space (Form the curl of Maxwell II and use a vector identity.). Find the condition that the plane wave E = eyEycos(wt - kx) is a solution (k=2pi/lamda). Use Maxwell II to find the B field associated with this electric field.
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A. I've done the derivation fine to get:
Laplacian E = epsilon-0.mu-0. d^2E/dt^2 [these are partial derivatives]
this is the same as d^2E/dx^2 = (1/c^2).(d^2E/dt^2) which can be solved using separation of variables to get E = eyEycos(wt - kx).
To find the associated B field, we used Maxwell II, ie. curlE = -dB/dt.
CurlE = -keyEysin(wt - kx)
B = integral - [curl E] dt
B = k/w. eyEycos(wt - kx)
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Thanks
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Q. Derive the wave equation for E in empty space (Form the curl of Maxwell II and use a vector identity.). Find the condition that the plane wave E = eyEycos(wt - kx) is a solution (k=2pi/lamda). Use Maxwell II to find the B field associated with this electric field.
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A. I've done the derivation fine to get:
Laplacian E = epsilon-0.mu-0. d^2E/dt^2 [these are partial derivatives]
this is the same as d^2E/dx^2 = (1/c^2).(d^2E/dt^2) which can be solved using separation of variables to get E = eyEycos(wt - kx).
To find the associated B field, we used Maxwell II, ie. curlE = -dB/dt.
CurlE = -keyEysin(wt - kx)
B = integral - [curl E] dt
B = k/w. eyEycos(wt - kx)
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Thanks