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Question: A bar magnet of length 10 m and magnetic moment 25 $Am^2$ is bent in the form of an arc as shown in ...

A bar magnet of length 10 m and magnetic moment 25 Am2Am^2 is bent in the form of an arc as shown in figure. The new magnetic dipole moment is

A

752Am2\frac{75}{2}Am^2

B

7532πAm2\frac{75\sqrt{3}}{2\pi}Am^2

C

252Am2\frac{25}{2}Am^2

D

2532πAm2\frac{25\sqrt{3}}{2\pi}Am^2

Answer

7532πAm2\frac{75\sqrt{3}}{2\pi}Am^2

Explanation

Solution

To solve this problem, we need to find the new effective length of the magnet after it's bent into an arc and then calculate the new magnetic dipole moment.

  1. Understand the initial state:

    • Length of the bar magnet, L=10mL = 10 \, \text{m}.
    • Magnetic moment, M=25Am2M = 25 \, \text{Am}^2.
    • For a straight bar magnet, the magnetic moment is given by M=m×LM = m \times L, where mm is the pole strength.
    • From this, we can find the pole strength: m=ML=25Am210m=2.5A mm = \frac{M}{L} = \frac{25 \, \text{Am}^2}{10 \, \text{m}} = 2.5 \, \text{A m}.
    • The pole strength (mm) remains constant when the magnet is bent.
  2. Understand the final state (bent magnet):

    • The magnet is bent into an arc subtending an angle θ=120\theta = 120^\circ at the center.
    • Convert the angle to radians: θ=120×π180=2π3\theta = 120^\circ \times \frac{\pi}{180^\circ} = \frac{2\pi}{3} radians.
    • The length of the arc is the original length of the magnet, L=10mL = 10 \, \text{m}.
    • For an arc, the length L=RθL = R\theta, where RR is the radius of the circle of which the arc is a part.
    • We can find the radius RR: R=Lθ=10m2π/3=302π=15πmR = \frac{L}{\theta} = \frac{10 \, \text{m}}{2\pi/3} = \frac{30}{2\pi} = \frac{15}{\pi} \, \text{m}.
  3. Calculate the new effective length (LL'):

    • The new magnetic dipole moment is determined by the straight-line distance between the two poles (ends of the arc). This distance is the chord length of the arc.
    • The chord length LL' for an arc subtending an angle θ\theta at the center of a circle with radius RR is given by L=2Rsin(θ2)L' = 2R \sin\left(\frac{\theta}{2}\right).
    • Calculate θ2\frac{\theta}{2}: θ2=1202=60\frac{\theta}{2} = \frac{120^\circ}{2} = 60^\circ.
    • L=2×(15π)×sin(60)L' = 2 \times \left(\frac{15}{\pi}\right) \times \sin(60^\circ).
    • We know sin(60)=32\sin(60^\circ) = \frac{\sqrt{3}}{2}.
    • L=2×15π×32=153πmL' = 2 \times \frac{15}{\pi} \times \frac{\sqrt{3}}{2} = \frac{15\sqrt{3}}{\pi} \, \text{m}.
  4. Calculate the new magnetic dipole moment (MM'):

    • The new magnetic dipole moment M=m×LM' = m \times L'.
    • M=2.5A m×153πmM' = 2.5 \, \text{A m} \times \frac{15\sqrt{3}}{\pi} \, \text{m}.
    • M=52×153π=7532πAm2M' = \frac{5}{2} \times \frac{15\sqrt{3}}{\pi} = \frac{75\sqrt{3}}{2\pi} \, \text{Am}^2.

The new magnetic dipole moment is 7532πAm2\frac{75\sqrt{3}}{2\pi} \, \text{Am}^2.