Step 1: Recall definition of magnetic dipole moment.
The magnetic dipole moment of a current loop is defined as
\[
m = I \cdot A,
\]
where:
- $I$ is the current flowing in the loop (Ampere),
- $A$ is the vector area of the loop (m$^2$).
Thus, the magnitude of $m$ depends on how much current flows and the area enclosed by that current.
Step 2: Derive SI units.
\[
[m] = [I] \cdot [A] = \text{Ampere} \times \text{m}^2.
\]
So the unit is A·m$^2$.
Step 3: Why not other options?
- Option (B): A·m$^{-1}$ → This is the unit of magnetic field strength $H$, not dipole moment.
- Option (C): Wb·m$^{-2}$ → This is the unit of magnetic flux density $B$ (Tesla), not dipole moment.
- Option (D): Wb·m$^2$ → This would correspond to flux multiplied by area, which is not relevant here.
Step 4: Physical meaning.
A magnetic dipole moment represents the strength of a magnetic source. A higher value means a stronger tendency to align with an external magnetic field.
Final Answer:
\[
\boxed{\text{A m}^2}
\]