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N.B.: Symbols have their usual meaning. All the problems carry equal weightage.
Electrostatics:
be the distance from the center to a side.
B. Find the magnetic field at the center of a regular n-sided polygon carrying a steady current I.
Again, et b be the distance from the center to a side.
C. Show that the magnetic field obtained for the polygon reduces to the result for a circular loop
for n → ∞.
A at an arbitrary point ~r = x
i + y
j + z
k due to a
circular loop carrying a steady current I. Assume the loop be on the x − y plane, its center be at
the origin, and its radius be b.
B. Determine the magnetic field (
x
i + B y
j + B z
k) from the above vector potential
C. Show that for a small loop (b r), the vector potential takes the form
A(~r) '
μ 0
4 π
m~×~r
r
3
B(~r) of a static case can have a local minimum,
but never a local maximum, in a source free region (where ∇ ·
B = 0 and ∇ ×
1
.
B. Show that
I
2
c
[d~r
′
× (~r
′
· ∇)
B(~r) − ~r
′
× (d~r
′
· ∇)
B(~r)] = ( m~ × ∇) ×
B(~r).
B(~r) be the magnetic field produced by a steady current distribution of the current
density J(~r) that lies entirely inside a spherical volume V of radius R. Show that the magnetic
moment due to the current distribution is m~ =
3
2 μ 0
V
B(~r)d
3
~r.
B. Using the above result show that the magnetic field at ~r due to a point magnetic dipole of the
dipole moment m~ located at ~r = 0 is
B(~r) =
μ 0
4 π
3(ˆr· m~)ˆr− m~
r
3
8 π
3
mδ~
3
(~r)
∀~r.
1
Refer to Thomson’s theorem for magnetostatics.