What physical situation creates such a B field?

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SUMMARY

The discussion centers on the physical situation that creates a magnetic field described by the equation ${\bf{B}} = C \delta(s-R) \hat{\phi}$. This B-field is nonzero only at a specific radius R, suggesting a scenario similar to a toroidal coil. The challenge lies in conceptualizing how to achieve an "infinite" B-field at s = R while maintaining zero elsewhere. The conversation also touches on the analogy of electric monopoles and the existence of magnetic dipoles, emphasizing the need for a creative approach to visualize this unique magnetic field configuration.

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Homework Statement


We are given that the B-field is:
$${\bf{B}} = C \delta(s-R) \hat{\phi}$$

where ##s## is the distance from some object and ##R## is the radius of some object. What kind of physical situation would create such a B-field?

Homework Equations


Stated above.

The Attempt at a Solution


[/B]
This is a tough question because it really involves creativity more than anything else. A "toroidal coil" creates a B-field that points in ##\hat{\phi}## and is constant but even if you figure out a clever way of canceling out the B-field in all but one location, how can you make it "infinite" at ##s = R##?

Electric monopoles are usually characterized by the ##\delta## function, but magnetic monopoles don't exist so I can't really extend that analogy any further!
 
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talrefae said:
Electric monopoles are usually characterized by the δδ\delta function, but magnetic monopoles don't exist so I can't really extend that analogy any further!
But magnetic dipoles do exist. Think about what happens as you make a dipole smaller and smaller. What function would describe an infinitely small dipole?

EDIT: Looking at the equation itself a bit more carefully, ##\mathbf{B}## is nonzero along a ring of radius ##R## (assuming cylindrical coordinates) and zero everywhere else. I don't know what physical situation would produce this but you can picture it as a single circular magnetic field line at ##R##.
 
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