Step 1: Understanding the Concept
A dipole in a uniform field feels a torque \(\tau=pE\sin\theta\), where \(p=q\times\ell\) and \(\ell\) is the length of the dipole.
Step 2: Key Formula or Approach
\[ \tau=q\,\ell\,E\sin\theta \Rightarrow q=\frac{\tau}{\ell E\sin\theta} \]
Step 3: Detailed Explanation
\(\ell=3\ \text{cm}=0.03\) m, \(E=5\times10^4\) N/C, \(\sin60^{\circ}=\dfrac{\sqrt3}{2}\).
\[ \ell E\sin\theta=0.03\times5\times10^4\times\frac{\sqrt3}{2}=750\sqrt3 \]
\[ q=\frac{9\sqrt3}{750\sqrt3}=0.012=1.2\times10^{-2}\ \text{C} \]
Final Answer:
The charge on the dipole is \(1.2\times10^{-2}\) C, option (B).
\[ \boxed{1.2\times10^{-2}\ \text{C (B)}} \]