Understanding the Concept:
An electric dipole placed in a uniform electric field experiences a turning torque ($\tau$) given by the vector cross product $\vec{\tau} = \vec{p} \times \vec{E}$, whose magnitude is:
\[
\tau = pE\sin\theta
\]
The potential energy ($U$) stored in the system due to this orientation is given by the dot product $U = -\vec{p} \cdot \vec{E}$, which expands to:
\[
U = -pE\cos\theta
\]
Step 1: Calculate the value of $pE$ using the torque formula.
We are given:
Electric field, $E = 10\text{ N C}^{-1}$
Angle, $\theta = 60^\circ$
Torque, $\tau = 8\sqrt{3}\text{ N m}$
Substitute these values into the torque expression:
\[
8\sqrt{3} = pE \sin(60^\circ)
\]
We know that $\sin(60^\circ) = \frac{\sqrt{3}}{2}$. Placing this in the equation:
\[
8\sqrt{3} = pE \left(\frac{\sqrt{3}}{2}\right) \implies pE = 8 \times 2 = 16\text{ N m}
\]
Step 2: Determine the potential energy ($U$).
Now, substitute the value of $pE = 16$ and $\theta = 60^\circ$ into the potential energy formula:
\[
U = -pE\cos(60^\circ)
\]
Since $\cos(60^\circ) = \frac{1}{2}$:
\[
U = -16 \times \frac{1}{2} = -8\text{ J}
\]