The magnetic moment \( \mu \) of a current loop is defined as:
\[
\mu = I A
\]
where \( I \) is the current and \( A \) is the area of the loop. The magnetic field \( B \) produced by a current \( I \) at the centre of a circular loop of radius \( r \) is given by:
\[
B = \frac{\mu_0 I}{2r}
\]
From this, we can solve for \( I \):
\[
I = \frac{2r B}{\mu_0}
\]
Now, substitute this value of \( I \) into the equation for the magnetic moment:
\[
\mu = \left( \frac{2r B}{\mu_0} \right) A
\]
Since the area \( A \) of the loop is related to the radius by \( A = \pi r^2 \), substitute \( r = \sqrt{\frac{A}{\pi}} \) into the equation:
\[
\mu = \frac{2B A}{\mu_0} \sqrt{\frac{A}{\pi}}
\]
Thus, the magnetic moment of the loop is:
\[
\mu = \frac{2BA}{\mu_0} \sqrt{\frac{A}{\pi}}
\]