Question:

A bar magnet placed in a uniform magnetic field making an angle $\theta$ with the field experiences a torque. If the angle made by the magnet with the field is doubled, the torque experienced by the magnet increases by $41.4\%$. The initial angle made by the magnet with the magnetic field is

Updated On: Jul 4, 2024
  • $60^{\circ}$
  • $30^{\circ}$
  • $90^{\circ}$
  • $45^{\circ}$
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The Correct Option is D

Solution and Explanation

As we know, torque in a magnetic field,
$ \tau =M B\, \sin \,\theta$
if $ \theta=\theta_{1},$
then $\tau_{1}=M B\, \sin\, \theta_{1} \dots$(i)
Similarly, if $\theta=\theta_{2}$ then
$\tau_{2}=M B\, \sin\, \theta_{2}=M B\, \sin \,2 \theta_{1} $
$\left(\because\right.$ Given, $\left.\theta_{2}=2 \theta_{1}\right)$
Given $\therefore \tau_{2}=\tau_{1}+\tau_{1} \times \frac{41.4}{100}$
$=1.414 \tau_{1}=\sqrt{2} \tau_{1}$
$\Rightarrow \sqrt{2} \tau_{1}=M B\, \sin \,2 \theta_{1} \dots$(ii)
From Eqs. (i) and (ii), we get
$ \frac{1}{\sqrt{2}}=\frac{\sin\, \theta_{1}}{\sin \,2 \theta_{1}} $
$\Rightarrow \sin \,2 \theta_{1}=\sqrt{2} \sin\, \theta_{1} \dots$(iii)
As we know that $\sin \,2 \theta=2 \,\sin \,\theta \,\cos\, \theta$
Hence, $2 \,\sin \,\theta_{1} \,\cos \,\theta_{1}=\sqrt{2} \sin \,\theta_{1}$
$2 \,\cos \,\theta=\sqrt{2}$
$ \Rightarrow \cos\, \theta=\frac{1}{\sqrt{2}} $
$\Rightarrow \theta=45^{\circ}$
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Concepts Used:

Magnetic Field

The magnetic field is a field created by moving electric charges. It is a force field that exerts a force on materials such as iron when they are placed in its vicinity. Magnetic fields do not require a medium to propagate; they can even propagate in a vacuum. Magnetic field also referred to as a vector field, describes the magnetic influence on moving electric charges, magnetic materials, and electric currents.

A magnetic field can be presented in two ways.

  • Magnetic Field Vector: The magnetic field is described mathematically as a vector field. This vector field can be plotted directly as a set of many vectors drawn on a grid. Each vector points in the direction that a compass would point and has length dependent on the strength of the magnetic force.
  • Magnetic Field Lines: An alternative way to represent the information contained within a vector field is with the use of field lines. Here we dispense with the grid pattern and connect the vectors with smooth lines.

Properties of Magnetic Field Lines

  • Magnetic field lines never cross each other
  • The density of the field lines indicates the strength of the field
  • Magnetic field lines always make closed-loops
  • Magnetic field lines always emerge or start from the north pole and terminate at the south pole.