Finding the magnetic field B given the vector potential A ?

In summary, the conversation is about a problem involving the magnetic vector potential and proving a given form for B. The individual has found the curl of A, but is unsure of how to reach the given form of B. It is mentioned that there is no given information about the scalar potential and a connection is made to Maxwell's third equation. It is also mentioned that there is some freedom in the choice of A and the possibility of assuming a gauge where the scalar potential is zero.
  • #1
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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  • #2
How is ##\vec E## related to ##\vec A##? Are you given any information about the scalar potential ##\varphi##?
 
  • #3
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}##
 
  • #4
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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