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A current loop consists of two identical semicircular parts each of radius RR, one lying in the xyx-y plane, and the other in the xzx-z plane. If the current in the loop is ii, what will be the resultant magnetic field due to the two semicircular parts at their common centre?

A

\frac{\mu_0 i}{2\sqrt{2} R}

B

\frac{\mu_0 i}{2 R}

C

\frac{\mu_0 i}{4 R}

D

\frac{\mu_0 i}{\sqrt{2} R}

Step-by-Step Solution

  1. Magnetic Field of a Semicircle: The magnetic field at the center of a full circular loop carrying current ii is B=μ0i2RB = \frac{\mu_0 i}{2R}. For a semicircular arc (half a loop), the magnitude is half of this: Bsemi=12μ0i2R=μ0i4RB_{semi} = \frac{1}{2} \frac{\mu_0 i}{2R} = \frac{\mu_0 i}{4R}.
  2. Direction: The direction of the magnetic field follows the right-hand rule .
  • For the semicircle in the xyx-y plane, the axis is the zz-axis, so the field B1\vec{B}_1 is along the zz-direction (k^\hat{k}).
  • For the semicircle in the xzx-z plane, the axis is the yy-axis, so the field B2\vec{B}_2 is along the yy-direction (j^\hat{j}).
  1. Superposition: The two fields are perpendicular to each other. The resultant magnitude BnetB_{net} is the vector sum: Bnet=B12+B22=(μ0i4R)2+(μ0i4R)2B_{net} = \sqrt{B_1^2 + B_2^2} = \sqrt{\left(\frac{\mu_0 i}{4R}\right)^2 + \left(\frac{\mu_0 i}{4R}\right)^2} Bnet=μ0i4R2=μ0i22RB_{net} = \frac{\mu_0 i}{4R} \sqrt{2} = \frac{\mu_0 i}{2\sqrt{2} R} .
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