To find the torque acting on the coil, we use the formula for the torque \( \tau \) on a current-carrying loop in a magnetic field: \(\tau = n \cdot I \cdot A \cdot B \cdot \sin(\theta)\). Here,
- \(n\) is the number of turns (\(n=50\)).
- \(I\) is the current (\(I=2 \, \text{A}\)).
- \(A\) is the area of the coil (\(A = \pi r^2\) with radius \(r=0.1 \, \text{m}\)).
- \(B\) is the magnetic field (\(B=0.5 \, \text{T}\)).
- \(\theta\) is the angle between the plane of the coil and the magnetic field. Since the coil is perpendicular to the field, \(\theta=90^\circ\), and \(\sin(90^\circ)=1\).
First, calculate the area \(A\):
\(A = \pi (0.1)^2 = 0.01\pi \, \text{m}^2\).
Now substitute the values 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, calculate the numeric value:
\(\tau = 0.5 \cdot 3.14 = 1.57/2 = 0.785 \, \text{N}\cdot\text{m}\).
The magnitude of the torque acting on the coil is
0.785 N·m.