Step 1: Biot-Savart Law.
The Biot-Savart law gives the expression for the magnetic field produced by a small current element. It is given by:
\[
d\vec{B} = \frac{\mu_0}{4\pi} \frac{I \, d\vec{l} \times \hat{r}}{r^2}
\]
where:
- \( d\vec{B} \) is the infinitesimal magnetic field produced by the current element,
- \( I \) is the current through the conductor,
- \( d\vec{l} \) is the infinitesimal length vector of the current element,
- \( \hat{r} \) is the unit vector from the current element to the point of observation,
- \( r \) is the distance from the current element to the point of observation,
- \( \mu_0 \) is the permeability of free space.
Step 2: Magnetic Field Due to a Current Carrying Circular Loop.
The magnetic field at the center of a circular loop of radius \( r \), carrying a current \( I \), is given by the formula:
\[
B = \frac{\mu_0 I}{2r}
\]
This expression is derived using the Biot-Savart law by integrating over the entire loop.
Step 3: Magnetic Moment of the Current Loop.
The magnetic moment \( \mu \) of a current loop is given by:
\[
\mu = I \cdot A
\]
where:
- \( I \) is the current,
- \( A \) is the area of the loop.
For a circular loop, the area \( A = \pi r^2 \), so the magnetic moment becomes:
\[
\mu = I \cdot \pi r^2
\]