Given, magnetic momentum, m = 6 JT−1
External magnetic field, B = 0.44 T
θ1=600⇒cos θ1=cos 600=12.
(a) Work done in turning the magnet normal to the field,
W=−mB(cos θ2−cos θ1)
(i) Here, θ2=900
∴ W=+mB cosθ1
= 6×0.44×12=1.32 J
(ii) Here θ2=1800
∴ W=−mB(cos θ2−cos θ1)
W=−6×0.44(−1−12)
= 3.96 J
(b) Torque on magnet when moment is aligned opposite to the field,
τ=mB sin θ
putting the values,
= 6×0.44×sin 180∘
= 0(∵sin 180∘=0)