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Answer: At the centre of an arc of radius \(R\) subtending angle \(\phi\) (in radian), \(B = \dfrac{\mu_0 I \phi}{4\pi R}\).

Consider a wire bent into a circular arc of radius \(R\) with centre C, carrying current \(I\), the arc subtending angle \(\phi\) at C. Take a small element \(d\vec{l}\) of the arc. The position vector \(\vec{r}\) from the element to C has magnitude \(R\) and is perpendicular to \(d\vec{l}\) (radius is perpendicular to the tangent), so \(\theta = 90^\circ\).

By Biot–Savart law,

\[dB = \frac{\mu_0}{4\pi}\frac{I\,dl\sin 90^\circ}{R^2} = \frac{\mu_0}{4\pi}\frac{I\,dl}{R^2}\]

For every element the field at C has the same direction (perpendicular to the plane of the arc), so the magnitudes add. With \(dl = R\,d\phi\):

\[B = \int dB = \frac{\mu_0 I}{4\pi R^2}\int_0^{\phi} R\,d\phi = \frac{\mu_0 I \phi}{4\pi R}\]

Direction: perpendicular to the plane of the arc, given by the right-hand thumb rule. For a full circle \(\phi = 2\pi\) and \(B = \dfrac{\mu_0 I}{2R}\).

Doubtly AI · 27 Oct 2026 AI-verified · Oct 2026 Report
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