Step 1: Electric Dipole and Dipole Moment.
An electric dipole consists of two equal and opposite charges separated by a small distance. The dipole moment \( \vec{p} \) is given by:
\[
\vec{p} = q \times \vec{d}
\]
where:
- \( q \) is the charge,
- \( \vec{d} \) is the displacement vector between the charges.
Step 2: Potential Energy of the Dipole.
The potential energy \( U \) of a dipole in a uniform electric field \( E \) is given by:
\[
U = - \vec{p} \cdot \vec{E}
\]
where \( \vec{p} \) is the dipole moment and \( \vec{E} \) is the electric field.
For \( \theta = 30^\circ \),
\[
U = - p E \cos(\theta)
\]
Substitute the values:
\[
U = - (2 \times 10^{-8} \, \text{C} \cdot \text{m}) \times (2 \times 10^5 \, \text{V/m}) \times \cos(30^\circ)
\]
\[
U = - 2 \times 10^{-8} \times 2 \times 10^5 \times \frac{\sqrt{3}}{2}
\]
\[
U = - 1.732 \times 10^{-3} \, \text{J}
\]
Step 3: Moment of the Couple.
The moment \( \tau \) of the couple acting on the dipole is given by:
\[
\tau = p E \sin(\theta)
\]
Substitute the values:
\[
\tau = (2 \times 10^{-8} \, \text{C} \cdot \text{m}) \times (2 \times 10^5 \, \text{V/m}) \times \sin(30^\circ)
\]
\[
\tau = 2 \times 10^{-8} \times 2 \times 10^5 \times \frac{1}{2}
\]
\[
\tau = 2 \times 10^{-3} \, \text{N} \cdot \text{m}
\]