Finding the magnetic field B given the vector potential A ?

AI Thread Summary
The discussion revolves around deriving the magnetic field B from a given magnetic vector potential A. The user initially finds the curl of A but struggles to express B in the required form. Key points include the relationship between the electric field E and vector potential A, as well as the potential gauge freedom in choosing A and the scalar potential φ. The mention of Maxwell's equations highlights the connection between E and B, suggesting that the problem may assume φ = 0 in a charge-free region. Ultimately, understanding these relationships is essential for reaching the desired expression for B.
patric44
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Homework Statement
find B given the vector potential A
Relevant Equations
A = /hat(ρ)/ρ *φ(z,t)
hi guys
this seems like a simple problem but i am stuck reaching the final form as requested , the question is
given the magnetic vector potential
$$\vec{A} = \frac{\hat{\rho}}{\rho}\beta e^{[-kz+\frac{i\omega}{c}(nz-ct)]}$$
prove that
$$B = (n/c + ik/\omega)(\hat{z}×\vec{E})$$
simple enough i found the curl of A which came out to be :
$$B = \frac{\hat{\phi}}{\rho} \beta e^{-iwt} (-k+\frac{i\omega n}{c})e^{-kz+\frac{i\omega n z}{c}}$$
how do i reach the given form of B ?!
 
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How is ##\vec E## related to ##\vec A##? Are you given any information about the scalar potential ##\varphi##?
 
TSny said:
How is ##\vec E## related to ##\vec A##? Are you given any information about the scalar potential ##\varphi##?
no nothing else was given ?! , could it be related some how to maxwell third equation ##∇×E = -\frac{∂B}{∂t}##
 
patric44 said:
no nothing else was given ?! , could it be related some how to maxwell third equation ##∇×E = -\frac{∂B}{∂t}##
See here for how ##\vec E## is related to ##\vec A## and ##\varphi##. There is some freedom in the choice of ##\vec A## and ##\varphi## ("gauge freedom"). Maybe this problem is assuming a choice of gauge where ##\varphi = 0## at each point of the region of interest, which can be done if there is no charge in the region.
 
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