Concept:
Torque on dipole:
\[
\tau = pE \sin \theta
\]
Direction is perpendicular to both \(\vec{p}\) and \(\vec{E}\).
Step 1: Convert dipole moment.
\[
p = 400 \,\mu C m = 400 \times 10^{-6} = 4 \times 10^{-4}
\]
Step 2: Substitute values.
\[
\tau = (4 \times 10^{-4})(50)\sin 30^\circ
\]
Step 3: Simplify.
\[
\tau = 4 \times 10^{-4} \times 50 \times \frac{1}{2}
= 4 \times 10^{-4} \times 25 = 10^{-2}
\]
Step 4: Direction.
Torque direction is perpendicular to both \(\vec{E}\) and \(\vec{\mu}\).
Step 5: Conclusion.
\[
\boxed{10^{-2}\,\text{Nm, perpendicular to both}}
\]