Step 1: Biot-Savart Law.
The magnetic field at the center of a current-carrying circular coil is derived using the Biot-Savart law. The Biot-Savart law states that the magnetic field \( d\vec{B} \) at a point due to an infinitesimal current element is:
\[
d\vec{B} = \frac{\mu_0}{4\pi} \frac{I d\vec{l} \times \hat{r}}{r^2}
\]
where:
- \( \mu_0 \) is the permeability of free space,
- \( I \) is the current,
- \( d\vec{l} \) is the infinitesimal length element of the wire,
- \( \hat{r} \) is the unit vector from the current element to the point where the magnetic field is being calculated,
- \( r \) is the distance from the current element to the point.
Step 2: Magnetic field at the center of the coil.
For a circular loop of radius \( R \), the magnetic field at the center of the loop due to a current \( I \) is given by:
\[
B = \frac{\mu_0 I}{2R}
\]
where:
- \( B \) is the magnetic field at the center of the coil,
- \( \mu_0 \) is the permeability of free space,
- \( I \) is the current flowing through the coil,
- \( R \) is the radius of the coil.
Step 3: Conclusion.
Thus, the intensity of the magnetic field at the center of a current-carrying circular coil is:
\[
B = \frac{\mu_0 I}{2R}
\]
Step 4: Law used.
The law used to derive this expression is the Biot-Savart law.