MCQMediumJEE 2023Biot–Savart Law

JEE Physics 2023 Question with Solution

As shown in the figure, a current of 2A2 \, \text{A} flowing in an equilateral triangle of side 43cm4\sqrt{3} \, \text{cm}. The magnetic field at the centroid OO of the triangle is:

Equilateral triangle carrying current 2 A along all three sides, with centroid O marked inside and current directions shown on each side.
  • A

    43×104T4\sqrt{3} \times 10^{-4} \, \text{T}

  • B

    43×105T4\sqrt{3} \times 10^{-5} \, \text{T}

  • C

    3×104T\sqrt{3} \times 10^{-4} \, \text{T}

  • D

    33×105T3\sqrt{3} \times 10^{-5} \, \text{T}

Answer

Correct answer:D

Step-by-step solution

Standard Method

Given: Current in each side is 2A2 \, \text{A} and the triangle is equilateral with side 43cm4\sqrt{3} \, \text{cm}.

Find: Magnetic field at the centroid OO.

From the geometry used in the solution,

dtan60=23d \tan 60^\circ = 2\sqrt{3}

So,

d=2cmd = 2 \, \text{cm}

The magnetic field at the centroid due to the three sides is

B=3×μ0i2πdsin60B = 3 \times \frac{\mu_0 i}{2\pi d} \sin 60^\circ

Substituting the given values,

B=3×2×107×22×102×32B = 3 \times \frac{2 \times 10^{-7} \times 2}{2 \times 10^{-2}} \times \frac{\sqrt{3}}{2}

Therefore,

B=33×105TB = 3\sqrt{3} \times 10^{-5} \, \text{T}

So, the correct option is D.

Geometry and Substitution

Given: An equilateral triangle of side 43cm4\sqrt{3} \, \text{cm} carries current 2A2 \, \text{A}.

Find: The net magnetic field at centroid OO.

For an equilateral triangle, the perpendicular distance from the centroid to each side is the same. Using the relation shown in the extracted solution,

dtan60=23d \tan 60^\circ = 2\sqrt{3}

Since tan60=3\tan 60^\circ = \sqrt{3}, we get

d3=23d \sqrt{3} = 2\sqrt{3} d=2cm=2×102md = 2 \, \text{cm} = 2 \times 10^{-2} \, \text{m}

Now, field due to one side at the centroid is taken as

B1=μ0i2πdsin60B_1 = \frac{\mu_0 i}{2\pi d} \sin 60^\circ

All three sides contribute equally and in the same direction at the centroid, so

B=3B1=3×μ0i2πdsin60B = 3B_1 = 3 \times \frac{\mu_0 i}{2\pi d} \sin 60^\circ

Substituting μ0/4π=107\mu_0/4\pi = 10^{-7}, i=2Ai = 2 \, \text{A}, d=2×102md = 2 \times 10^{-2} \, \text{m}, and sin60=32\sin 60^\circ = \frac{\sqrt{3}}{2},

B=3×2×107×22×102×32B = 3 \times \frac{2 \times 10^{-7} \times 2}{2 \times 10^{-2}} \times \frac{\sqrt{3}}{2} B=33×105TB = 3\sqrt{3} \times 10^{-5} \, \text{T}

Therefore, the magnetic field at the centroid is 33×105T3\sqrt{3} \times 10^{-5} \, \text{T}, and the correct option is D.

Common mistakes

  • Using the side length itself as the distance in Biot-Savart law is incorrect. The required distance is the perpendicular distance from the centroid to each side, which here is d=2cmd = 2 \, \text{cm}.

  • Forgetting to add the contribution of all three sides leads to an answer smaller by a factor of 33. Each side produces the same magnetic field magnitude at the centroid, so the total field is 3B13B_1.

  • Not converting cm to m gives the wrong power of 1010. Before substitution, use 2cm=2×102m2 \, \text{cm} = 2 \times 10^{-2} \, \text{m}.

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