Explaining the Context of $\nabla\times A=0$ with a Uniform Y-Component of A

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I came across in a journal that for a \nabla\times A=0 where A is vector, if y-component of that A is uniform then author claims that y-component of curl of a A is zero?
Can anyone explain the above context?
 
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Are you sure that's what's being claimed? Because it isn't true; the y-component of the curl is independent of the y-component of the vector. Maybe there is something extra assumed about A? Can you link to the article or attach the relevant section?
 
how to attach the pdf?
 
see Eq. (7) and previous statement connecting to that...
 

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The vanishing of the curl is what is assumed here (it's Ampere's law without currents). Then \partial_z H_x =\partial_x H_z is just taking the y-component of the curl. The uniformity of the y-component of H is a separate conclusion, and comes from the assumption that nothing depends on y ("the wave is not modulated transversely"). Then the x- and z-components of the curl give you z- and x-independence of Hy respectively.

Hope that helps.
 
Dear henry_m

Please clearly elucidate this statement "Then the x- and z-components of the curl give you z- and x-independence of Hy respectively."
 
saravanan13 said:
Please clearly elucidate this statement "Then the x- and z-components of the curl give you z- and x-independence of Hy respectively."

Yeah sure, sorry that wasn't very clear.

We're assuming the curl of H vanishes from the physics. The x-component of this says that \partial_y H_z=\partial_z H_y. But H is y-independent by assumption, so \partial_y H_z=0, and hence \partial_z H_y is zero. This means that H_y is independent of z.

If you do the same for the z-component of the curl, you find that H_y is independent of x.

Finally, we're assuming H is independent of y. So H_y is independent of x,y, and z, and hence uniform.
 
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