Magnetic Vector Potential Around a Wire Carrying Current

AI Thread Summary
The discussion centers on the magnetic vector potential, defined by the equation B = ∇ × A, and its visualization around a straight wire carrying a constant electric current. Participants reference Fitzpatrick's equations to understand this concept better, noting that the magnetic vector potential is not unique and is subject to gauge conditions. A follow-up question arises regarding the Lagrangian of a charged particle in an electromagnetic field, specifically whether the term should include -qφ or +qφ. The conversation concludes with a reference to an equation from a different source that clarifies the earlier confusion. Overall, the thread explores the theoretical aspects of magnetic vector potential and its implications in electromagnetism.
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Until about ten minutes ago I had never heard of the magnetic vector potential \vec A, defined such that

\vec B = \nabla \times \vec A.

I am having trouble visualizing this. What would the magnetic vector potential field look like around a straight wire carrying a (constant) electric current?
 
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Thanks atyy, that's a great reference.
 
Follow up:

Is the Lagrangian of a charged particle in an electromagnetic field

L = \frac {1}{2}m( \dot x ^2 + \dot y^2 + \dot z^2 ) - q \phi + q (\dot x A_x + \dot y A_y + \dot z A_z) ?

(I'm not sure if that should be -q \phi or + q \phi.) If so, is this good for both static and changing EM fields?

Edit: oh wait, here it is. Equation 1.34. at

http://www.ks.uiuc.edu/Services/Class/PHYS480/qm_PDF/chp1.pdf

All set, then.
 
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