The work done to rotate a dipole in an electric field is given by the equation:
\[
W = -\vec{p} \cdot \vec{E} (\cos \theta_2 - \cos \theta_1)
\]
Where:
- \( \vec{p} \) is the dipole moment,
- \( \vec{E} \) is the electric field,
- \( \theta_1 \) and \( \theta_2 \) are the initial and final angles of the dipole.
For the given case, since the dipoles are arranged symmetrically and rotated through 90° in the clockwise direction, the net work done is zero.
Thus, the correct answer is:
\[
\boxed{\text{Zero}}
\]