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Question: The work done in turning a magnet of magnetic moment M by an angle of \(90^\circ \)from the meridian...

The work done in turning a magnet of magnetic moment M by an angle of 9090^\circ from the meridian is n times the corresponding work done to turn it through an angle of 6060^\circ
A. n=12n = \dfrac{1}{2}
B. n=2n = 2
C. n=14n = \dfrac{1}{4}
D. n=1n = 1

Explanation

Solution

Concept of work done in moving a magnetic dipole from one angle to another angle in a uniform magnetic field.Also we have to use the formula W=mB(cosθ1cosθ2)W = mB\left( {\cos {\theta _1} - \cos {\theta _2}} \right)

Complete step by step answer:
Whenever a magnetic dipole or magnet is placed in a magnetic field, it experiences a torque.
Let is consider a magnet of length2l2l, placed in uniform magnetic field B\overrightarrow B with magnetic dipole momentm\overrightarrow m . Then, torque C acting on it is given by,
C=m×B\overrightarrow C = \overrightarrow m \times \overrightarrow B Or C=mB sinθC = mB{\text{ sin}}\theta …… (i)
Whose θ\theta is the angle the magnet is placed with the magnetic field? This torque will tend to align the dipole in direction of B.\overrightarrow B . If the dipole is rotated against torque action, work is to be done.
The work done in turning the dipole through a small angle do is given by
dW=Cdθ=mBsinθdθdW = Cd\theta = mB\sin \theta d\theta … (From (i))
If dipole is rotated from initial position θ=θ1\theta = {\theta _1}to θ=θ2\theta = {\theta _2}, then work done is
W=dW=θ1θ2mBsinθdθ=mB[cosθ]θ1θ2W = \int {dW = \int\limits_{{\theta _1}}^{{\theta _2}} {mB\sin \theta d\theta = mB\left[ { - \cos \theta } \right]_{{\theta _1}}^{{\theta _2}}} }

    W=mB(cosθ2cosθ)     W=mB(cosθ1cosθ2)  \implies W = - mB\left( {\cos {\theta _2} - \cos \theta } \right) \\\ \implies W = mB\left( {\cos {\theta _1} - \cos {\theta _2}} \right) \\\

Now, at magnetic meridian, angle =0= 0^\circ
Work done in rotating magnet of magnetic moment, M from magnetic moment
i.e. θ1=0{\theta _1} = 0^\circ to θ=90\theta = 90^\circ is
W1=MB(cosθcosθ90){W_1} = MB\left( {\cos \theta - \cos \theta 90} \right)
W1=MB(10){W_1} = MB\left( {1 - 0} \right)
W1=MB{W_1} = MB….. (ii)
Work done in rotating from magnetic meridian, θ1=0{\theta _1} = 0^\circ to θ=60\theta = 60^\circ is
W2=MB(cos0cos60) W2=MB(10.5)  {W_2} = MB\left( {\cos 0^\circ - \cos 60^\circ } \right) \\\ {W_2} = MB\left( {1 - 0.5} \right) \\\
W2=0.5MB{W_2} = 0.5MB ….. (iii)
According to question
W1=nW2{W_1} = n{W_2}
MB=n×0.5MBMB = n \times 0.5MB….. (From (ii) and (iii))
1=n×12 n=2  1 = n \times \dfrac{1}{2} \\\ n = 2 \\\

So, the correct answer is “Option B”.

Note:
Magnetic meridian is the vertical plane passing through the magnetic axis of a freely suspended small magnet and the earth’s magnetic field acts in the direction of magnetic meridian. That’s why, θ1=0{\theta _1} = 0^\circ not9090^\circ .