Concept:
The magnetic dipole moment of a current-carrying coil is one of the most important quantities in magnetism. It measures the strength of the magnetic effect produced by the current loop.
For a coil consisting of $N$ turns, carrying current $I$, and enclosing area $A$ per turn, the magnetic moment is given by
\[
M=NIA.
\]
Therefore, to calculate the magnetic moment, we must first determine the area enclosed by each turn of the loop.
In this problem, two different coils are formed using wires of different lengths:
• A circular coil having $3$ turns and current $3\text{ A}$.
• A square coil having $2$ turns and current $2\text{ A}$.
The magnetic moment of the circular coil is given. Using that information, we first determine the value of $L$, and then calculate the magnetic moment of the square coil.
Step 1: Analyze the circular coil and express its radius in terms of $L$.
The second wire has total length
\[
2L.
\]
This wire is bent into a circular coil having
\[
N_c=3
\]
turns.
Let the radius of each circular turn be $R$.
The circumference of one turn is
\[
2\pi R.
\]
Since there are $3$ turns, the total wire length used is
\[
3(2\pi R).
\]
But this total length is given as $2L$.
Hence,
\[
2L=3(2\pi R).
\]
Therefore,
\[
2L=6\pi R.
\]
Solving for $R$,
\[
R=\frac{L}{3\pi}.
\]
Step 2: Calculate the area enclosed by one circular turn.
The area of a circle is
\[
A_c=\pi R^2.
\]
Substituting
\[
R=\frac{L}{3\pi},
\]
we obtain
\[
A_c
=
\pi\left(\frac{L}{3\pi}\right)^2.
\]
\[
A_c
=
\pi\cdot\frac{L^2}{9\pi^2}.
\]
\[
A_c
=
\frac{L^2}{9\pi}.
\]
Thus, the area enclosed by one circular turn is
\[
A_c=\frac{L^2}{9\pi}.
\]
Step 3: Form the expression for the magnetic moment of the circular coil.
The circular coil has
\[
N_c=3,
\]
current
\[
I_c=3\text{ A},
\]
and area per turn
\[
A_c=\frac{L^2}{9\pi}.
\]
Using
\[
M=NIA,
\]
we get
\[
M_c
=
3\times3\times\frac{L^2}{9\pi}.
\]
\[
M_c
=
\frac{L^2}{\pi}.
\]
But the magnetic moment is given as
\[
M_c=\frac{4}{\pi}\text{ A}\cdot\text{m}^2.
\]
Therefore,
\[
\frac{L^2}{\pi}
=
\frac{4}{\pi}.
\]
Multiplying both sides by $\pi$,
\[
L^2=4.
\]
Hence,
\[
L=2\text{ m}.
\]
For the remaining calculations, we use
\[
L^2=4.
\]
Step 4: Analyze the square coil and determine its side length.
The first wire has total length
\[
L.
\]
It is bent into a square coil having
\[
N_s=2
\]
turns.
Let the side of each square be $a$.
The perimeter of one square is
\[
4a.
\]
Since there are two turns,
\[
L=2(4a).
\]
\[
L=8a.
\]
Thus,
\[
a=\frac{L}{8}.
\]
Step 5: Calculate the area enclosed by one square turn.
The area of a square is
\[
A_s=a^2.
\]
Substituting
\[
a=\frac{L}{8},
\]
we get
\[
A_s
=
\left(\frac{L}{8}\right)^2.
\]
\[
A_s
=
\frac{L^2}{64}.
\]
Step 6: Calculate the magnetic moment of the square coil.
The square coil has
\[
N_s=2,
\]
current
\[
I_s=2\text{ A},
\]
and area
\[
A_s=\frac{L^2}{64}.
\]
Using
\[
M=NIA,
\]
we obtain
\[
M_s
=
2\times2\times\frac{L^2}{64}.
\]
\[
M_s
=
\frac{4L^2}{64}.
\]
\[
M_s
=
\frac{L^2}{16}.
\]
Substituting
\[
L^2=4,
\]
we get
\[
M_s
=
\frac{4}{16}.
\]
\[
M_s
=
\frac{1}{4}.
\]
Therefore,
\[
M_s=0.25\text{ A}\cdot\text{m}^2.
\]
Final Answer:
The magnetic moment of the square loop is
\[
\boxed{0.25\text{ A}\cdot\text{m}^2}.
\]
Hence, the correct option is
\[
\boxed{\text{(D)}\;0.25\text{ A}\cdot\text{m}^2}.
\]