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JEE Main 2025 · Physics · Magnetic Effects of Current · medium

A long wire carrying current I comes in along a straight line, goes round a semicircle of radius R and goes out along a second straight line. The two…

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A long wire carrying current II comes in along a straight line, goes round a semicircle of radius RR and goes out along a second straight line. The two straight segments are semi-infinite, parallel to each other and perpendicular to the diameter of the semicircle; each begins at an end of the diameter and extends away from the semicircle. The magnetic field at the centre of the semicircle is
  1. A. μ0I4R(1−2π)\dfrac{\mu_0 I}{4R}\left(1-\dfrac{2}{\pi}\right)
  2. B. μ0I4R\dfrac{\mu_0 I}{4R}
  3. C. μ0I4R(1+2π)\dfrac{\mu_0 I}{4R}\left(1+\dfrac{2}{\pi}\right)
  4. D. μ0I2R(1+1π)\dfrac{\mu_0 I}{2R}\left(1+\dfrac{1}{\pi}\right)
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Answer: (C) μ0I4R(1+2π)\dfrac{\mu_0 I}{4R}\left(1+\dfrac{2}{\pi}\right)

The semicircle gives B1=μ0I4RB_1 = \dfrac{\mu_0 I}{4R}. Each straight semi-infinite wire ends at the foot of the perpendicular from the centre (distance RR), so each gives μ0I4πR\dfrac{\mu_0 I}{4\pi R}. Applying the right-hand rule to the three parts, the current goes up the left wire, clockwise round the arc, and down the right wire, so all three fields point into the plane and add: B=μ0I4R+2⋅μ0I4πR=μ0I4R(1+2π)B = \dfrac{\mu_0 I}{4R} + 2\cdot\dfrac{\mu_0 I}{4\pi R} = \dfrac{\mu_0 I}{4R}\left(1+\dfrac{2}{\pi}\right).
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