MCQEasyJEE 2025Biot–Savart Law

JEE Physics 2025 Question with Solution

Let B1B_1 be the magnitude of magnetic field at the center of a circular coil of radius RR carrying current II. Let B2B_2 be the magnitude of magnetic field at an axial distance xx from the center. For x:R=3:4x : R = 3 : 4, B2B1\frac{B_2}{B_1} is:

  • A

    4:54 : 5

  • B

    16:2516 : 25

  • C

    64:12564 : 125

  • D

    25:1625 : 16

Answer

Correct answer:C

Step-by-step solution

Standard Method

Given: A circular coil of radius RR carries current II. Magnetic field at the center is B1B_1 and magnetic field at axial distance xx is B2B_2. Also, x:R=3:4x : R = 3 : 4.

Find: The ratio B2B1\frac{B_2}{B_1}.

For a circular coil, the magnetic field at the center is

B1=μ0I2RB_1 = \frac{\mu_0 I}{2R}

and the magnetic field at a point on its axis is

B2=μ0IR22(R2+x2)3/2B_2 = \frac{\mu_0 I R^2}{2(R^2 + x^2)^{3/2}}

Now form the ratio:

B2B1=μ0IR22(R2+x2)3/2μ0I2R\frac{B_2}{B_1} = \frac{\frac{\mu_0 I R^2}{2(R^2 + x^2)^{3/2}}}{\frac{\mu_0 I}{2R}}

Cancel the common factor μ0I2\frac{\mu_0 I}{2}:

B2B1=R3(R2+x2)3/2\frac{B_2}{B_1} = \frac{R^3}{(R^2 + x^2)^{3/2}}

Given

xR=34    x=3R4\frac{x}{R} = \frac{3}{4} \implies x = \frac{3R}{4}

Substitute this in the ratio:

B2B1=R3(R2+(3R4)2)3/2\frac{B_2}{B_1} = \frac{R^3}{\left(R^2 + \left(\frac{3R}{4}\right)^2\right)^{3/2}} B2B1=R3(R2+9R216)3/2=R3(25R216)3/2\frac{B_2}{B_1} = \frac{R^3}{\left(R^2 + \frac{9R^2}{16}\right)^{3/2}} = \frac{R^3}{\left(\frac{25R^2}{16}\right)^{3/2}}

Now evaluate the denominator:

(25R216)3/2=(5R4)3=125R364\left(\frac{25R^2}{16}\right)^{3/2} = \left(\frac{5R}{4}\right)^3 = \frac{125R^3}{64}

Therefore,

B2B1=R3125R3/64=64125\frac{B_2}{B_1} = \frac{R^3}{125R^3/64} = \frac{64}{125}

Therefore, the correct option is C and the ratio is 64125\frac{64}{125}.

Using the standard axial field formula

Given: Radius of coil RR, current II, and axial distance ratio x:R=3:4x:R = 3:4.

Find: The value of B2B1\frac{B_2}{B_1}.

Concept used: The magnetic field is maximum at the center of a circular coil and decreases along the axis. Use the field expressions at the center and at an axial point.

  1. At the center,
B1=μ0I2RB_1 = \frac{\mu_0 I}{2R}
  1. On the axis at distance xx,
B2=μ0IR22(R2+x2)3/2B_2 = \frac{\mu_0 I R^2}{2(R^2 + x^2)^{3/2}}
  1. Divide the second expression by the first:
B2B1=μ0IR22(R2+x2)3/2μ0I2R=R3(R2+x2)3/2\frac{B_2}{B_1} = \frac{\frac{\mu_0 I R^2}{2(R^2 + x^2)^{3/2}}}{\frac{\mu_0 I}{2R}} = \frac{R^3}{(R^2 + x^2)^{3/2}}
  1. From x:R=3:4x:R = 3:4,
x=3R4x = \frac{3R}{4}
  1. Substitute into the ratio:
B2B1=R3(R2+9R216)3/2=R3(25R216)3/2\frac{B_2}{B_1} = \frac{R^3}{\left(R^2 + \frac{9R^2}{16}\right)^{3/2}} = \frac{R^3}{\left(\frac{25R^2}{16}\right)^{3/2}}
  1. Simplify:
(25R216)3/2=125R364\left(\frac{25R^2}{16}\right)^{3/2} = \frac{125R^3}{64}

So,

B2B1=R3125R3/64=64125\frac{B_2}{B_1} = \frac{R^3}{125R^3/64} = \frac{64}{125}

Therefore, the ratio is 64125\frac{64}{125}.

Common mistakes

  • Using the magnetic field formula for a straight wire or a solenoid is incorrect because the geometry here is a circular coil. Use the center-field and axial-field formulas for a circular current loop instead.

  • Taking x:R=3:4x:R = 3:4 as x=3Rx = 3R or R=4xR = 4x is wrong because it ignores the ratio properly. The correct substitution is x=3R4x = \frac{3R}{4}.

  • Forgetting the power 32\frac{3}{2} in (R2+x2)3/2(R^2 + x^2)^{3/2} leads to an incorrect ratio. Keep the full axial field expression before simplifying.

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