Step 1: Formula for Torque.
The torque \(\tau\) on a current-carrying coil in a magnetic field is given by:
\[ \tau = N I A B \sin\theta \]
Where:
- \(N\) is the number of turns.
- \(I\) is the current.
- \(A\) is the area of the coil.
- \(B\) is the magnetic field strength.
- \(\theta\) is the angle between the normal to the coil area and the magnetic field.
Step 2: Identify the angle \(\theta\).
The problem states "the plane of the coil is in the direction of magnetic field". This means the area vector (which is normal to the plane) is perpendicular to the magnetic field.
Therefore, \(\theta = 90^\circ\), and \(\sin 90^\circ = 1\).
The torque is maximum: \(\tau = N I A B\).
Step 3: Calculation.
Given:
\(N = 200\)
\(I = 3 \, \text{mA} = 3 \times 10^{-3} \, \text{A}\)
Side \(a = 10 \, \text{cm} = 0.1 \, \text{m} \implies \text{Area } A = a^2 = (0.1)^2 = 0.01 \, \text{m}^2\)
\(B = 2 \, \text{T}\)
\[ \tau = 200 \times (3 \times 10^{-3}) \times 0.01 \times 2 \]
\[ \tau = 1200 \times 10^{-5} \, \text{Nm} \]
\[ \tau = 12 \times 10^{-3} \, \text{Nm} \]