(a) Magnetic moment, M = 1.5 J T-1
Magnetic field strength, B = 0.22 T
(i) Initial angle between the axis and the magnetic field, θ1 = 0°
Final angle between the axis and the magnetic field, θ2 = 90°
The work required to make the magnetic moment normal to the direction of magnetic field is given as:
\(W = -MB(\cos\theta_2-\cos\theta_1)\)
= -1.5 \(\times\) 0.22(cos 90°-cos 0°)
= -0.33(0-1)
= 0.33 J
(ii) Initial angle between the axis and the magnetic field, θ1 = 0°
Final angle between the axis and the magnetic field, θ2 = 180°
The work required to make the magnetic moment opposite to the direction of magnetic field is given as:
\(W = -MB(\cos\theta_2-\cos\theta_1)\)
= -1.5 \(\times\) 0.22(cos 180°-cos 0°)
= -0.33(-1-1)
= 0.66 J
(b) For case (i): θ = θ2 = 90°
∴ Torque, τ =\(MB\sin\theta\)
= 1.5 \(\times\) 0.22 sin 90°
= 0.33 J
For case (ii): θ = θ2 = 180°
∴ Torque, τ = \(MB\sin\theta\)
= \(MB\sin\) 180° = 0 J
A current-carrying coil is placed in an external uniform magnetic field. The coil is free to turn in the magnetic field. What is the net force acting on the coil? Obtain the orientation of the coil in stable equilibrium. Show that in this orientation the flux of the total field (field produced by the loop + external field) through the coil is maximum.
Magnets are used in many devices like electric bells, telephones, radio, loudspeakers, motors, fans, screwdrivers, lifting heavy iron loads, super-fast trains, especially in foreign countries, refrigerators, etc.
Magnetite is the world’s first magnet. This is also called a natural magnet. Though magnets occur naturally, we can also impart magnetic properties to a substance. It would be an artificial magnet in that case.
Read More: Magnetism and Matter