Understanding the Magnetic Field Boundary Conditions for an Infinite Cylinder

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Homework Statement



An infinite cylinder (radius a) with a uniform volume charge density rho_v is given. The axis of the cylinder coincides with the z axis. The following magnetic field exists:

B=B0cos(wt+a) for r<=a (i.e., inside the cylinder and on its walls)
B=0 for r>a (i.e., outside the cylinder)

One asks:

1) What is the magnetic vector potential everywhere
2) What is the electric field everywhere
3) What can one learn from the magnetic field boundary conditions


The Attempt at a Solution



Unfortunately, I do not have any clue how to address this question. There is a static charge which generated a static electric field, and there is an induced electric field due to the alternating magnetic field. Is the overall electric field a superposition of the two electric fields or am I mistaken ? Do the boundary conditions imply that the cylinder behaves as an ideal solenoid ? Do I only need to find the rotor of the magnetic field to get the magnetic vector potential ?

Thank you for the help !
 
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It's straightforth once you use Maxwell's equations (with vector potential).
 
To solve this, I first used the units to work out that a= m* a/m, i.e. t=z/λ. This would allow you to determine the time duration within an interval section by section and then add this to the previous ones to obtain the age of the respective layer. However, this would require a constant thickness per year for each interval. However, since this is most likely not the case, my next consideration was that the age must be the integral of a 1/λ(z) function, which I cannot model.
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