A current-carrying coil experiences a torque due to a magnetic field. The value of the torque is 80% of the maximum possible torque. The angle between the magnetic field and the normal to the plane of the coil is
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Maximum torque occurs when the coil is perpendicular to the field (\(\theta = 90^\circ\)). At any other angle, use \(\sin\theta\) to find torque.
The torque on a coil in a magnetic field is given by:
\[
\tau = \tau_{\max} \sin\theta
\]
Given that \( \tau = 0.8 \tau_{\max} \), we solve for \( \theta \):
\[
\sin\theta = 0.8
\]
\[
\theta = \sin^{-1}(0.8)
\]
Using trigonometric identities,
\[
\tan\theta = \frac{4}{3}
\]
Thus, the correct answer is \( \tan^{-1} \left(\frac{4}{3}\right) \).