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Exercises · 4.13

Q.(a) A circular coil of 3030 turns and radius 8.0 cm8.0\ \text{cm} carrying a current of 6.0 A6.0\ \text{A} is suspended vertically in a uniform horizontal magnetic field of magnitude 1.0 T1.0\ \text{T}. The field lines make an angle of 60∘60^\circ with the normal of the coil. Calculate the magnitude of the counter torque that must be applied to prevent the coil from turning.

(b) Would your answer change, if the circular coil in
(a) were replaced by a planar coil of some irregular shape that encloses the same area? (All other particulars are also unaltered.)
Rajasthan RbseTextbookSubjective· 3mImportance★★★★★est
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The counter torque required to hold the coil stationary equals the magnetic torque acting on it. Using τ=NIABsin⁡θ\tau = N I A B \sin\theta, the magnitude is 3.13 N⋅m3.13\ \text{N·m}, and the shape of the coil does not matter as long as the area is the same.

Why magnetic torque?

A current-carrying loop in a magnetic field experiences a torque that tries to rotate it so that its normal aligns with the field. This torque arises because the field exerts opposite forces on opposite sides of the loop, creating a couple. The magnitude of this torque depends on the number of turns NN, the current II, the area AA of the loop, the field strength BB, and the angle θ\theta between the field and the normal to the coil.

The formula is:

τ=NIABsin⁡θ\tau = N I A B \sin\theta

To keep the coil from turning, we must apply an equal and opposite torque — a counter torque — of the same magnitude.


Step-by-step solution

1. Identify the given data

  • Number of turns: N=30N = 30
  • Radius of coil: r=8.0 cm=0.08 mr = 8.0\ \text{cm} = 0.08\ \text{m}
  • Current: I=6.0 AI = 6.0\ \text{A}
  • Magnetic field: B=1.0 TB = 1.0\ \text{T}
  • Angle between field and normal: θ=60∘\theta = 60^\circ

2. Compute the area of the coil

The coil is circular, so its area is:

A=πr2=π(0.08)2=π×0.0064=0.020106 m2A = \pi r^2 = \pi (0.08)^2 = \pi \times 0.0064 = 0.020106\ \text{m}^2

(Keep a few extra digits for accuracy; we'll round at the end.)

3. Apply the torque formula

τ=NIABsin⁡θ\tau = N I A B \sin\theta

Substitute the values:

τ=30×6.0×0.020106×1.0×sin⁡60∘\tau = 30 \times 6.0 \times 0.020106 \times 1.0 \times \sin 60^\circ

We know sin⁡60∘=32≈0.8660\sin 60^\circ = \frac{\sqrt{3}}{2} \approx 0.8660.

So:

τ=30×6.0×0.020106×0.8660\tau = 30 \times 6.0 \times 0.020106 \times 0.8660

4. Calculate step by step

First, 30×6.0=18030 \times 6.0 = 180.

Then 180×0.020106=3.61908180 \times 0.020106 = 3.61908.

Finally, 3.61908×0.8660=3.134 N⋅m3.61908 \times 0.8660 = 3.134\ \text{N·m} (rounded to three significant figures).

Watch out

A common mistake is to use the angle between the field and the plane of the coil instead of the normal. Here the field makes 60∘60^\circ with the normal, so θ=60∘\theta = 60^\circ directly. If the angle with the plane were given, you'd use its complement.

5. Answer for part (a)

The counter torque required is 3.13 N⋅m3.13\ \text{N·m}.


Part (b): Does shape matter? …

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