Electron flow over a conducting surface of variable resistivity

AI Thread Summary
The discussion revolves around understanding electron flow over a conducting surface with variable resistivity connected to a battery. The main question is whether the current density would follow a simple curve from point A to B or spread out to minimize mutual electric repulsion. The complexity of the problem suggests that variational calculus and possibly Maxwell's equations could be applied to analyze the flow paths. Participants acknowledge the challenge of the problem and express uncertainty about the systematic approach needed. Overall, the conversation highlights the need for a deeper exploration of current behavior in non-uniform resistivity scenarios.
fyzxfreak
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Hello fellow physics-people,

I was just thinking about the following setup:
We have a conducting surface (with smoothly varying resistivity) hooked up to some battery with the wires contacting the surface at two arbitrary points, A and B. How would we go about figuring out the current density?

Would the electrons flow in a simple curve from point A to B (to follow the path of least resistance) or would they spread out (as there might be a configuration in which parallel flow reduces mutual electric repulsion)?

Any ideas/suggestions? Thanks!
 
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I believe that the current would flow through a large area of the conductor. But I'm not sure.
 
Is there a systematic method of approaching this problem? i.e. application of Maxwell's equations, etc.

=EDIT= There'd definitely be some variational calculus involved (for the different paths from point A to point B). Yeah... this problem does not seem particularly simple anymore, haha.
 
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fyzxfreak said:
Is there a systematic method of approaching this problem? i.e. application of Maxwell's equations, etc.

I'm not knowledgeable enough to answer. I was basing my guess on knowing that the more conductor a current can flow through, the less the resistance overall. I would think this is balanced against the resistance caused by the longer path some of the current takes, resulting in an equilibrium somewhere. But all this is merely a guess.
 
It may be shown from the equations of electromagnetism, by James Clerk Maxwell in the 1860’s, that the speed of light in the vacuum of free space is related to electric permittivity (ϵ) and magnetic permeability (μ) by the equation: c=1/√( μ ϵ ) . This value is a constant for the vacuum of free space and is independent of the motion of the observer. It was this fact, in part, that led Albert Einstein to Special Relativity.
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