How to find the potential of a field that has regions of non-zero curl

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SUMMARY

This discussion focuses on the challenges of finding the potential in regions with non-zero curl in electrostatics. It establishes that in cases where the curl of the electric field E is non-zero, such as in the presence of a static magnetic field B within an infinite wire, a global potential cannot be constructed. The solution requires integrating the field only in simply connected regions, explicitly excluding areas with non-zero curl, as these violate the conditions necessary for defining a potential. The conversation emphasizes that traditional methods for conservative fields do not apply in these scenarios.

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kated
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Homework Statement
I want to find the potential of a field at a point where the curl of the field is zero but there are regions(for example far away from the point that interest us) that have non zero curl.
Relevant Equations
E=-gradV
curl E = Ω ≠ 0
We know that in electrostatics, there is path independency for line integral of E, so E is a conservative field and thus we have E=-gradV. Integrating this from ro(reference point of our choice) to the point r we are studying, along a random path, we get the solution of the above equation, e.g. the potential V. But, there are some areas (possibly far away from
the point r that interests us) where the curl E is not zero, e.g., curl E = Ω ≠ 0 , with Ω
being a vector field perpendicular to the plane, which only exists in these areas, then
how would we solve again Α=gradΛ, to find the scalar function Λ at point r? (how will the previous (usual)
solution change/get corrected?) Consider the (unusual) case where Ω is a static
(time-independent) field.
 
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You cannot construct a global potential in this situation. The best you can do is to integrate the field in a region that is simply connected and excludes the region with non-zero curl.
 
What do you mean by excluding the region with non-zero curl? Doesn't it affect the result? If for example I have an infinite wire with width=d(y=0, y=d) with B a magnetic field that exist only inside the wire and is perpedicular to the plane, and we want to find the potential at a point r far away and above from the wire then if we choose a path starting below the wire where B=0 and ending at r(again B=0) but the path goes through the wire doesnt this affect the result? I mean if we do the same process we do when we are talking about conservative fields isnt the result 0 which does not satisfy the system? How can we correct this?
 
kated said:
What do you mean by excluding the region with non-zero curl? Doesn't it affect the result? If for example I have an infinite wire with width=d(y=0, y=d) with B a magnetic field that exist only inside the wire and is perpedicular to the plane, and we want to find the potential at a point r far away and above from the wire then if we choose a path starting below the wire where B=0 and ending at r(again B=0) but the path goes through the wire doesnt this affect the result?
Of course it does. The region where the curl is non-zero is then not simply connected, thereby violating the explicit requirement:
Orodruin said:
The best you can do is to integrate the field in a region that is simply connected and excludes the region with non-zero curl.


kated said:
I mean if we do the same process we do when we are talking about conservative fields isnt the result 0 which does not satisfy the system? How can we correct this?
You can't. In your non-simply-connected region, it is generally not possible to write the field as the derivative of a potential because the region is not simply connected.
 

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