Step 1: Understanding the relation for mutual inductance.
The mutual inductance \( M \) is defined as the ratio of the induced emf (electromotive force) in a coil to the rate of change of current in another coil. The general relation is:
\[
\mathcal{E} = M \cdot \frac{dI}{dt}
\]
Where:
- \( \mathcal{E} \) is the induced emf, with the dimension of \( [\mathcal{E}] = \text{ML}^2 \text{T}^{-3} \text{A}^{-1} \).
- \( \frac{dI}{dt} \) is the rate of change of current, which has the dimension \( [\frac{dI}{dt}] = \text{A} \text{T}^{-1} \).
Step 2: Deriving the dimension of \( M \).
Using the formula \( \mathcal{E} = M \cdot \frac{dI}{dt} \), we can rearrange to find the dimension of mutual inductance \( M \):
\[
[M] = \frac{[\mathcal{E}]}{[dI/dt]} = \frac{\text{ML}^2 \text{T}^{-3} \text{A}^{-1}}{\text{A} \text{T}^{-1}} = \text{ML}^2 \text{T}^{-2} \text{A}^{-2}
\]
Step 3: Conclusion.
Therefore, the correct dimension for mutual inductance is \( \text{ML}^2 \text{T}^{-2} \text{A}^{-2} \), which corresponds to option (B).
Final Answer: (B) \( \text{ML}^2 \text{T}^{-2} \text{A}^{-2} \)