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Answer: \(B = \dfrac{\mu_0 I \theta}{4\pi R}\) at the centre of an arc; for a full loop \(B = \dfrac{\mu_0 I}{2R}\).

For a circular arc of radius \(R\) carrying current \(I\) and subtending angle \(\theta\) (in radian) at its centre, the Biot–Savart law gives (each element \(dl\) is perpendicular to the radius, \(dl = R\,d\theta\)):

\[B = \int \frac{\mu_0}{4\pi}\frac{I\,dl}{R^2} = \frac{\mu_0 I}{4\pi R^2}(R\theta) = \frac{\mu_0 I\theta}{4\pi R}\]

directed perpendicular to the plane of the arc.

Circular loop: a complete loop is an arc with \(\theta = 2\pi\):

\[B = \frac{\mu_0 I (2\pi)}{4\pi R} = \frac{\mu_0 I}{2R}\]

For a coil of \(N\) turns, \(B = \dfrac{\mu_0 N I}{2R}\).

Doubtly AI · 28 Oct 2026 AI-verified · Oct 2026 Report
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