The torque \( \tau \) on a current-carrying coil in a magnetic field is given by \(\tau = n \cdot I \cdot A \cdot B \cdot \sin(\theta)\). The parameters are:
- Number of turns, \(n=50\).
- Current, \(I=2 \, \text{A}\).
- Coil area, \(A = \pi r^2\) with \(r=0.1 \, \text{m}\).
- Magnetic field strength, \(B=0.5 \, \text{T}\).
- Angle \(\theta\) between the coil's plane and the magnetic field. With the coil perpendicular to the field, \(\theta=90^\circ\), so \(\sin(90^\circ)=1\).
The coil's area is first computed:
\(A = \pi (0.1)^2 = 0.01\pi \, \text{m}^2\).
Next, these values are substituted into the torque formula:
\(\tau = 50 \cdot 2 \cdot 0.01\pi \cdot 0.5 \cdot 1 = 0.5\pi \, \text{N}\cdot\text{m}\).
Finally, the numerical value is calculated:
\(\tau = 0.5 \cdot 3.14 = 1.57/2 = 0.785 \, \text{N}\cdot\text{m}\).
The resulting torque magnitude on the coil is
0.785 N·m.