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A bar magnet of length L and magnetic dipole moment M is bent in the form of an arc as shown in figure. The new magnetic dipole moment will be:

A

M

B

3M/\pi

C

2M/\pi

D

M/2

Step-by-Step Solution

  1. Original Magnetic Moment: The magnetic dipole moment (MM) of a bar magnet is the product of its pole strength (mm) and its length (LL). M=m×LM = m \times L
  2. Bent Magnet Geometry: When the magnet is bent into an arc, the length of the arc remains LL. Let the radius of the arc be RR and the angle subtended at the center be θ\theta (in radians). L=Rθ    R=LθL = R\theta \implies R = \frac{L}{\theta}
  3. New Magnetic Moment (MM'): The new magnetic moment is the product of the pole strength (mm) and the straight-line distance (chord) between the two poles. The chord length is given by 2Rsin(θ/2)2R \sin(\theta/2). M=m×(2Rsin(θ/2))M' = m \times (2R \sin(\theta/2))
  4. Substitution: Substituting R=L/θR = L/\theta: M=m×2(Lθ)sin(θ/2)=2(mL)θsin(θ/2)=2Mθsin(θ/2)M' = m \times 2 \left( \frac{L}{\theta} \right) \sin(\theta/2) = \frac{2(mL)}{\theta} \sin(\theta/2) = \frac{2M}{\theta} \sin(\theta/2)
  5. Determining the Angle: Based on the probable answer 3M/π3M/\pi, we test the angle θ=60=π/3\theta = 60^\circ = \pi/3 radians. M=2Mπ/3sin(60/2)=6Mπsin(30)M' = \frac{2M}{\pi/3} \sin(60^\circ/2) = \frac{6M}{\pi} \sin(30^\circ) M=6Mπ×12=3MπM' = \frac{6M}{\pi} \times \frac{1}{2} = \frac{3M}{\pi} This confirms the magnet is bent into an arc subtending 6060^\circ at the center.
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