According to the Biot-Savart law, the magnetic induction (\(B\)) at the centre of a circular arc of wire with radius \(r\), carrying a current \(I\), and subtending an angle \(\theta\) (in radians) at the centre is given by:
\[ B = \frac{\mu_0 I \theta}{4\pi r} \]
where \(\mu_0\) is the permeability of free space.
Magnetic Induction at the Centre of a Circular Loop:
To find the magnetic induction at the centre of a full circular loop, we consider the arc to be a complete circle.
For a complete circle, the angle \(\theta\) subtended at the centre is \(2\pi\) radians.
Substituting \(\theta = 2\pi\) into the formula for a circular arc:
\[ B_{loop} = \frac{\mu_0 I (2\pi)}{4\pi r} \]
\[ B_{loop} = \frac{\mu_0 I}{2r} \]
This is the formula for the magnetic induction at the centre of a current-carrying circular loop.