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)
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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