Q. The magnetic needle of an oscillation magnetometer makes 10 oscillations per min under the action of earth’s magnetic field alone. When a bar magnet is placed at some distance along the axis of the needle, it makes 14 oscillations per min. If the bar magnet is turned so that its poles interchange their positions, then the new frequency of oscillation of the needle is

A) $10\ vibs$-$m^{- 1}$
B) 2 $vibs$-$m^{- 1}$
C) 4 $vibs$-$m^{- 1}$
D) 20 $vibs$-$m^{- 1}$
Explanation

(b) In the first case, $T_{1} = \frac{60}{10} = 6$ s
$T_{1} = 2\pi\sqrt{\frac{I}{MH}} = 6$ …(i)
In the second case, $T_{2} = \frac{60}{14} = \frac{30}{7}$ s
If $B$ magnetic induction due to external magnet, then
$T_{2} = 2\pi\sqrt{\frac{I}{M(H + B)}} = \frac{30}{7}$ ….(ii)
Dividing Eq. (i) by Eq. (ii), we get
$\frac{6}{30/7} = \sqrt{\frac{H + B}{H}} = \sqrt{1 + \frac{B}{H}}$
or $\left( \frac{7}{5} \right)^{2} = 1 + \frac{B}{H}$
or $\ \frac{B}{H} = \frac{49}{25} - 1 = \frac{24}{25}$
If $n$ is number of vibrations/min in the third case when polarity of external magnet is reversed, then
$T_{3} = \frac{60}{n} = 2\pi\sqrt{\frac{I}{M(H - B)}}$ …(iii)
Dividing Eq. (i) by Eq. (iii), we get
$\frac{60}{60/n} = \sqrt{\frac{H - B}{H} = \sqrt{1 - \frac{B}{H}} = \sqrt{1 - \frac{24}{25}}}$
$\frac{n}{10} = \frac{1}{5},n = 2\ vibs - \min^{- 1}{.\ }$

Dr. Abubacker
Reviewed by Dr. Abubacker

Physics Educator & NEET/JEE Specialist

Ph.D. in Physics with 19+ years of teaching experience.