Understanding the Concept:
A current-carrying magnetic loop experiences a mechanical torque ($\tau$) when placed in an external magnetic field, given by:
\[
\tau = NIAB\sin\theta
\]
where $\theta$ represents the angle between the normal vector (perpendicular) of the coil's area plane and the magnetic field lines. If the problem states the angle relative to the plane of the coil itself ($\alpha$), then $\theta = 90^\circ - \alpha$, converting the formula to $\tau = NIAB\cos\alpha$.
Step 1: Verify standard values and angles.
We are given:
Number of turns, $N = 300$
Current, $I = 2\text{ A}$
Radius, $r = 10\text{ cm} = 0.1\text{ m}$
Field strength, $B = 0.7\text{ T}$
Angle of plane with field, $\alpha = 30^\circ$
The angle $\theta$ for our standard formula is:
\[
\theta = 90^\circ - 30^\circ = 60^\circ
\]
Step 2: Calculate loop area ($A$) and evaluate torque magnitude.
\[
A = \pi r^2 = \pi \times (0.1)^2 = 0.01\pi\text{ m}^2
\]
Plugging all values into the torque formula:
\[
\tau = 300 \times 2 \times (0.01\pi) \times 0.7 \times \sin(60^\circ)
\]
\[
\tau = 6\pi \times 0.7 \times \frac{\sqrt{3}}{2} = 2.1 \times \sqrt{3} \times \pi
\]
Substitute $\sqrt{3} \approx 1.732$ and $\pi \approx 3.1416$:
\[
\tau \approx 2.1 \times 1.732 \times 3.1416 = 3.6372 \times 3.1416 \approx 11.42\text{ N m}
\]