MCQEasyJEE 2024Biot–Savart Law

JEE Physics 2024 Question with Solution

Two insulated circular loops A and B of radius aa, carrying a current II in anticlockwise direction, are arranged perpendicular to each other. The magnitude of the magnetic induction at the center will be:

  • A

    2μ0I/a\sqrt{2}\,\mu_0 I/a

  • B

    μ0I/(2a)\mu_0 I/(2a)

  • C

    μ0I2/a\mu_0 I\sqrt{2}/a

  • D

    2μ0I/a2\mu_0 I/a

Answer

Correct answer:C

Step-by-step solution

Standard Method

Given: Two insulated circular loops A and B of radius aa each carry current II and are perpendicular to each other.

Find: The magnitude of the net magnetic induction at the common center.

For one circular loop, the magnetic field at the center is

B=μ0I2aB = \frac{\mu_0 I}{2a}

The direction of this field is perpendicular to the plane of the loop by the right-hand thumb rule.

For loop A,

BA=μ0I2aB_A = \frac{\mu_0 I}{2a}

For loop B,

BB=μ0I2aB_B = \frac{\mu_0 I}{2a}

Since the two loops are perpendicular, the magnetic field vectors at the center are also perpendicular to each other.

Using vector addition,

Bnet=BA2+BB2|\vec{B}_{\text{net}}| = \sqrt{B_A^2 + B_B^2}

Substituting,

Bnet=(μ0I2a)2+(μ0I2a)2|\vec{B}_{\text{net}}| = \sqrt{\left(\frac{\mu_0 I}{2a}\right)^2 + \left(\frac{\mu_0 I}{2a}\right)^2} Bnet=2(μ0I2a)2|\vec{B}_{\text{net}}| = \sqrt{2\left(\frac{\mu_0 I}{2a}\right)^2} Bnet=2μ0I2a=μ0I2a|\vec{B}_{\text{net}}| = \frac{\sqrt{2}\mu_0 I}{2a} = \frac{\mu_0 I}{\sqrt{2}a}

Therefore, the magnitude of the magnetic induction at the center is 2μ0I2a\frac{\sqrt{2}\mu_0 I}{2a}.

The solution working does not match the listed option C. Based on the extracted source, option A is also not equivalent to this value as written, and the printed answer key appears inconsistent with the worked solution.

Using Perpendicular Resultant

Given: Each loop produces magnetic field of magnitude μ0I2a\frac{\mu_0 I}{2a} at the center.

Find: Resultant magnetic field when the two fields are perpendicular.

Let the field due to one loop be

B=μ0I2aB = \frac{\mu_0 I}{2a}

Because the loops are in mutually perpendicular planes, their magnetic fields at the center are mutually perpendicular.

So,

Bnet=B2+B2B_{\text{net}} = \sqrt{B^2 + B^2} Bnet=2B2=2BB_{\text{net}} = \sqrt{2B^2} = \sqrt{2}\,B Bnet=2(μ0I2a)B_{\text{net}} = \sqrt{2}\left(\frac{\mu_0 I}{2a}\right) Bnet=μ0I2aB_{\text{net}} = \frac{\mu_0 I}{\sqrt{2}a}

Thus, the correct magnitude from the solution is μ0I2a\frac{\mu_0 I}{\sqrt{2}a}.

Common mistakes

  • Adding the two magnetic fields directly as BA+BBB_A + B_B is incorrect because the two field vectors are perpendicular, not parallel. Use the Pythagorean relation BA2+BB2\sqrt{B_A^2 + B_B^2} instead.

  • Using the wrong formula for the magnetic field at the center of a circular loop is a common error. The correct expression is B=μ0I2aB = \frac{\mu_0 I}{2a}, not the formula for a long straight wire.

  • Ignoring direction and treating anticlockwise current as only a magnitude-based statement leads to mistakes. First determine the field direction using the right-hand thumb rule, then combine the vectors.

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