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Magnetic Scalar Potential is Defined as U ( → R 2 ) − U ( → R 1 ) = - ∫ → R 2 → R 1 → B . → D L Apply this Equation to a Closed Curve Enclosing a Long Straight Wire.

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प्रश्न

Magnetic scalar potential is defined as `U(vec r_2) - U(vec r_1) = - ∫_vec(r_1)^vec(r_2)` `vec (B) . dvec(l)`

Apply this equation to a closed curve enclosing a long straight wire. The RHS of the above equation is then `-u_0 i` by Ampere's law. We see that `U(vec(r_2)) ≠ U(vec(r_1))` even when `vec r_2 =vec r_1` .Can we have a magnetic scalar potential in this case?

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उत्तर

No, we cannot have a magnetic scalar potential here.

Ampere's law is a method of calculating magnetic field due to current distribution. On the other hand, magnetic scalar potential requires a magnetic field due to pole strength m.
Potential at a distance r is given by `(u_0m)/(4pir)`

As there is no current distribution, no magnetic field due to poles or the pole strength is present. That is why we cannot have a magnetic scalar potential in this case.

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पाठ 36: Permanent Magnets - Short Answers [पृष्ठ २७५]

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एचसी वर्मा Concepts of Physics Volume 1 and 2 [English]
पाठ 36 Permanent Magnets
Short Answers | Q 8 | पृष्ठ २७५
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