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Question: The magnetic field induction at the centre of a regular polygon having n sides is (The polygon is in...

The magnetic field induction at the centre of a regular polygon having n sides is (The polygon is inscribed in a circle of radius 'a' metre. The side of the polygon carries a current of I amp)(Current is clockwise)

A

2Inatanπ/n×107\frac{2In}{a} \tan \pi/n \times 10^{-7} tesla(outward)

B

2Inatanπ/n×107\frac{2In}{a} \tan \pi/n \times 10^{-7} tesla(inward)

C

Inatanπ/n×107\frac{In}{a} \tan \pi/n \times 10^{-7} tesla(inward)

D

Inatanπ/n×107\frac{In}{a} \tan \pi/n \times 10^{-7} tesla (outward)

Answer

2Inatanπ/n×107\frac{2In}{a} \tan \pi/n \times 10^{-7} tesla (inward)

Explanation

Solution

The magnetic field at the center of a regular polygon with 'n' sides, inscribed in a circle of radius 'a', carrying current 'I', is the sum of magnetic fields due to each side.

  1. Perpendicular distance from center to a side: d=acos(π/n)d = a \cos(\pi/n).

  2. Angles subtended by half a side at the center: θ1=θ2=π/n\theta_1 = \theta_2 = \pi/n.

  3. Magnetic field due to one side: Bside=μ0I4πd(sinθ1+sinθ2)=μ0I4πacos(π/n)(2sin(π/n))=μ0I2πatan(π/n)B_{side} = \frac{\mu_0 I}{4\pi d} (\sin\theta_1 + \sin\theta_2) = \frac{\mu_0 I}{4\pi a \cos(\pi/n)} (2\sin(\pi/n)) = \frac{\mu_0 I}{2\pi a} \tan(\pi/n).

  4. Total magnetic field: Btotal=n×Bside=nμ0I2πatan(π/n)B_{total} = n \times B_{side} = n \frac{\mu_0 I}{2\pi a} \tan(\pi/n).

  5. Substitute μ0=4π×107\mu_0 = 4\pi \times 10^{-7}: Btotal=2Inatan(π/n)×107B_{total} = \frac{2In}{a} \tan(\pi/n) \times 10^{-7} Tesla.

  6. Direction: For clockwise current, by Right-Hand Thumb Rule, the field at the center is inward.