Step 1: Recall the dipole moment.
An electric dipole is two equal and opposite charges a small distance apart. Its dipole moment is one charge times the separation: \[ p = q\,d \]
Step 2: Recall the torque formula.
In a uniform field $E$, the torque on a dipole tilted by angle $\theta$ to the field is: \[ \tau = pE\sin\theta \]
Step 3: Find the dipole moment.
With $q = 10^{-6}$ C and $d = 0.05$ m: \[ p = (10^{-6})(5\times10^{-2}) = 5\times10^{-8}\ \text{C}\,\text{m} \]
Step 4: Set the angle.
To make the dipole perpendicular to the field, $\theta = 90^{\circ}$, so $\sin 90^{\circ} = 1$. This is also the maximum torque case.
Step 5: Put in the field.
With $E = 3\times10^{5}\ \text{NC}^{-1}$: \[ \tau = (5\times10^{-8})(3\times10^{5})(1) \]
Step 6: Compute.
\[ \tau = 15\times10^{-3}\ \text{N}\,\text{m} \] \[ \boxed{\tau = 15\times10^{-3}\ \text{N}\,\text{m}} \]