
Step 1: Use relation between torque and rate of change of potential energy
For a magnetic dipole in a uniform magnetic field, torque is related to potential energy by:
τ = − dU / dθ
Hence, the work done in rotating the dipole between two positions is equal to the area under the torque–angle curve.
Step 2: Find the magnetic interaction energy MB
Given torque at θ = 30°:
τ = MB sin θ
0.016 = MB × sin 30°
0.016 = MB × 1/2
MB = 0.032 J
Step 3: Work done as area under τ–θ curve
The torque varies with angle as:
τ = MB sin θ
Work done by an external agent in rotating the magnet from θ = 0° to θ = 180° is:
W = ∫₀π MB sin θ dθ
Step 4: Perform the integration
W = MB [ −cos θ ]₀π
W = MB [ −cos π + cos 0 ]
W = MB [ −(−1) + 1 ]
W = 2MB
Step 5: Substitute value of MB
W = 2 × 0.032
W = 0.064 J
Final Answer:
The work done by the external agent is
0.064 J
Consider two arrangements of wires. Find the ratio of magnetic field at the centre of the semi–circular part.