Question:

The magnetic needle lying parallel to the magnetic field requires $W$ units of work to rotate it through $60^{\circ}$. The torque needed to maintain the needle in this position is :

Updated On: Aug 15, 2022
  • $ 3\,\,W $
  • $ \sqrt{3}\,\,W $
  • $ \frac{W}{3} $
  • $ \frac{W}{\sqrt{3}} $
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The Correct Option is B

Solution and Explanation

The instaneous moment of the deflecting couple or torque acting on the needle is $\tau=$ force $\times$ perpendicular distance $=$ work done when axis of needle makes an angle $\theta$ with the magnetic field, then for magnetic moment $M$ and magnetic field $B$, we have $\tau=M B \sin \theta \ldots(1) $ $W=M B \cos \theta \ldots(2)$ Dividing E (1) by E (2), we get $\frac{\tau}{W}=\frac{M B \sin \theta}{M B \cos \theta}$ Given, $\theta=60^{\circ}$ $\tau=W \frac{\sin 60^{\circ}}{\cos 60^{\circ}}$ $W=\sqrt{3}$
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Concepts Used:

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Magnetic Field:

Region in space around a magnet where the Magnet has its Magnetic effect is called the Magnetic field of the Magnet. Let us suppose that there is a point charge q (moving with a velocity v and, located at r at a given time t) in presence of both the electric field E (r) and the magnetic field B (r). The force on an electric charge q due to both of them can be written as,

F = q [ E (r) + v × B (r)] ≡ EElectric +Fmagnetic 

This force was based on the extensive experiments of Ampere and others. It is called the Lorentz force.