Field with rot = 0 but non conservative.

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SUMMARY

The discussion centers on the nature of a vector field F in a multiply-connected region of R², specifically addressing the conditions under which a field can be considered conservative. Despite the curl of F being zero, indicating potential expressibility as -∇φ, the presence of a singularity at the origin (0,0) prevents the field from being path-independent. The conversation emphasizes that line integrals around closed curves enclosing the singularity do not yield zero, while those that do not enclose it do. The analysis suggests using cylindrical coordinates to explore the multi-valued potential across the excluded half-plane.

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Homework Statement
I want to know what is the problem with this field and why it is not conservative.
Relevant Equations
The curl.
1601189002933.png
x and y are different than 0
As you can check, rot (del x F) is equal zero. Immediately someone could imagine this is a conservative field. But it is not, it is not path independent in certain occasions.
I just know one way, involving polygonal, but there is not another way to check if F is conservative?
 
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The curl is ##\vec{0}##, which means that you can express ##\vec{F} = -\nabla \phi## wherever ##\vec{F}## is defined, however you have a singularity at the origin ##(x,y) = (0,0)##. That means that any line integral around a closed curve that encloses the origin is not necessarily zero. If the closed curve does not enclose the singular point, then the line integral will be zero.
 
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etotheipi said:
The curl is ##\vec{0}##, which means that you can express ##\vec{F} = -\nabla \phi## wherever ##\vec{F}## is defined, however you have a singularity at the origin ##(x,y) = (0,0)##. That means that any line integral around a closed curve that encloses the origin is not necessarily zero. If the closed curve does not enclose the singular point, then the line integral will be zero.
You unearthed a quote from Kleppner that was I don’t know where in my brain, involving a function similar to this with the same problem lol! The brain is a bizarre thing, and thank you ;) This is a more logic way to evaluate the functions
 
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The original field is defined on ##\mathbb{R}^2## with the ##3##-axis excluded. That's a multiply-connected region, i.e., you cannot shrink all closed curves continuously to a single point. Any closed curve with the ##z## axis intersecting all surfaces with this curve as a boundary cannot be contracted to a single point in a continuous way. Any other closed curve, however can.

You can easily show that in any open simply connected part of where a vector field is defined, which fulfills ##\vec{\nabla} \times \vec{V}=0## has a potential, ##\vec{V}=-\vec{\nabla} \phi##, when restricted to this open simply-connected region.

In your case you can get a maximal such region, by just excluding not only the ##3##-axis from the domain of the vector field but an entire half-plane with the ##3##-axis as a boundary. You can find a unique potential in this restricted domain, but it will have a jump across the excluded half-plane by a constant ##2 \pi##.

It's a good exercise to do the calculation to find this kind of "muti-valued potential".

Hint: Work in cylinder coordinates with some arbitrary domain for ##\varphi \in [\alpha,\alpha+ 2 \pi[## with ##\alpha \in [-\pi,\pi]## arbitrary. Note that cylinder coordinates are singular along the ##3##-axis!
 
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