Figure 5: The force between the dipole and the magnet is repulsive and this follows from F = § Idl × B = F ll,net 6. The force on the current loop shown in figure 5 can be seen as follows [assume the magnetic field vector makes an angle of e with the vertical line everywhere on the parameter of the loop and note that fo* sino = - cos o1* = 0 similarly fo" sin o = 0] B + Bị = |B l(cos o, sin o, 0) - |B1|(0,0, 1) ; i = p = p(cos o, sin o, 0) = pp - de = dp = pdo(- sin o, cos o, 0) = pdøo f rat 1)) doIpl-|B1|(0, 0, 1) + |B|l(cos o, sin o, 0)] Ide x B = I[pdo(- sin o, cos o, 0)] x [|B|l(cos o, sin o, 0) – |B1|(0,0, 1)] -27Ip|B||(0, 0, 1) = F (True, False)

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Figure 5: The force between the dipole and the magnet is repulsive and this follows from
F = $ Ide x B
F,net
6. The force on the current loop shown in figure 5 can be seen as follows [assume the magnetic field vector makes an angle of 0 with the
vertical line everywhere on the parameter of the loop and note that (6* sin o = – cos ø|
= 0 similarly Só" sin o =
B| + B1 = |B|||(cos 4, sin o, 0) – |B1|(0,0, 1)
l = p = p(cos ø, sin ø, 0) = pp →
de = de = pdø(- sin ø, cos ø, 0)
pdøp
%3D
f Id :
B = | I[pdø(- sin ø, cos 4, 0)] × [[B|||(cos ¢, sin ø, 0) – |B1|(0, 0, 1)] / døIp[-|B1|(0,0, 1) + |B|||(cos o, sin ø, 0)]
%3D
-27IP|B|||(0, 0, 1) = F| (True, False)
Transcribed Image Text:ф В || || net Figure 5: The force between the dipole and the magnet is repulsive and this follows from F = $ Ide x B F,net 6. The force on the current loop shown in figure 5 can be seen as follows [assume the magnetic field vector makes an angle of 0 with the vertical line everywhere on the parameter of the loop and note that (6* sin o = – cos ø| = 0 similarly Só" sin o = B| + B1 = |B|||(cos 4, sin o, 0) – |B1|(0,0, 1) l = p = p(cos ø, sin ø, 0) = pp → de = de = pdø(- sin ø, cos ø, 0) pdøp %3D f Id : B = | I[pdø(- sin ø, cos 4, 0)] × [[B|||(cos ¢, sin ø, 0) – |B1|(0, 0, 1)] / døIp[-|B1|(0,0, 1) + |B|||(cos o, sin ø, 0)] %3D -27IP|B|||(0, 0, 1) = F| (True, False)
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