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Question

Question: The magnetic field at the centre of the circular coil of radius 1 cm and carrying current of 4 A is ...

The magnetic field at the centre of the circular coil of radius 1 cm and carrying current of 4 A is

A

8π3×104T\frac{8\pi}{3}\times10^{-4}T

B

8π3×105T\frac{8\pi}{3}\times10^{-5}T

C

2π×105T2\pi\times10^{-5}T

D

2π×104T2\pi\times10^{-4}T

Answer

2π×105T2\pi\times10^{-5}T

Explanation

Solution

The problem asks for the magnetic field at the center of a circular coil. However, the figure shows a circular arc, not a full coil. The current 'i' is shown flowing along the arc.

Given values: Radius of the circular arc, R=1 cm=1×102 mR = 1 \text{ cm} = 1 \times 10^{-2} \text{ m}. Current flowing through the arc, I=4 AI = 4 \text{ A}.

From the figure, an angle of 9090^\circ is marked between the radii OA and OB.

The angle explicitly marked in the diagram is 9090^\circ. So, the angle subtended by the current-carrying arc at the center is θ=90\theta = 90^\circ. In radians, θ=90×π180=π2\theta = 90^\circ \times \frac{\pi}{180^\circ} = \frac{\pi}{2} radians.

Using the formula for the magnetic field at the center of a circular arc: B=μ0I4πRθB = \frac{\mu_0 I}{4\pi R} \theta Substituting the values: B=(4π×107 T m/A)×(4 A)4π×(1×102 m)×π2B = \frac{(4\pi \times 10^{-7} \text{ T m/A}) \times (4 \text{ A})}{4\pi \times (1 \times 10^{-2} \text{ m})} \times \frac{\pi}{2} B=107×4102×π2B = \frac{10^{-7} \times 4}{10^{-2}} \times \frac{\pi}{2} B=4×105×π2B = 4 \times 10^{-5} \times \frac{\pi}{2} B=2π×105 TB = 2\pi \times 10^{-5} \text{ T}

This result matches option (c). The straight segments OA and OB do not contribute to the magnetic field at O because the point O lies on the line of these segments.