An electric dipole of dipole moment \( 1.0 \times 10^{-12} \ \text{Cm} \) lies along the x-axis. An electric field of magnitude \( 2.0 \times 10^4 \ \text{NC}^{-1} \) is switched on at an instant in the region. The unit vector along the electric field is \( \frac{\sqrt{3}}{2} \hat{i} + \frac{1}{2} \hat{j} \). The magnitude of the torque acting on the dipole at that instant is:
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To find torque on a dipole in a non-parallel field, compute the cross product \( \vec{p} \times \vec{E} \) or use \( \tau = pE \sin\theta \) where \( \theta \) is the angle between dipole and field directions.