81.
A vibration magnetometer placed in magnetic meridian has a small bar magnet. The magnet executes oscillations with a time period of $$2\,s$$ in the earth’s horizontal magnetic field of $$24\,\mu T.$$ When a horizontal field of $$18\,\mu T$$ is produced opposite to the earth’s field by placing a current carrying wire, the new time period of magnet will be
Problem Solving Strategy
Find out the relation of time period with the earth’s horizontal magnetic field and then compare it for the two given cases.
Time period in vibration magnetometer is given by
$$\eqalign{
& T = 2\pi \sqrt {\frac{I}{{M \times {B_H}}}} \cr
& \Rightarrow T \propto \frac{1}{{\sqrt {{B_H}} }} \cr
& {\text{So, for two different cases}} \cr
& \Rightarrow \frac{{{T_1}}}{{{T_2}}} = \sqrt {\frac{{{{\left( {{B_H}} \right)}_2}}}{{{{\left( {{B_H}} \right)}_1}}}} \cr
& \Rightarrow \frac{2}{{{T_2}}} = \sqrt {\frac{{18}}{{24}}} \cr
& \therefore T = 2.3\,s \approx 2\,s \cr} $$
82.
A $$10\,cm$$ long bar magnet of magnetic moment $$1.34\,A{m^2}$$ is placed in the magnetic meridian with its south pole pointing geographical south. The neutral point is obtained at a distance of $$15\,cm$$ from the centre of the magnet. Calculate the horizontal component of earth’s magnetic field.
83.
A permanent magnet in the shape of a thin cylinder of length $$10\,cm$$ has magnetisation $$\left( M \right) = {10^6}A{m^{ - 1}}.$$ Its magnetization current $${I_M}$$ is
84.
An example of a perfect diamagnet is a superconductor. This implies that when a superconductor is put in a magnetic field of intensity $$B,$$ the magnetic field $${B_s}$$ inside the superconductor will be such that :
Magnetic field inside the superconductor is zero. Diamagnetic substances are repelled in external magnetic field.
85.
If a bar magnet of pole strength $$m$$ and magnetic moment $$M$$ is cut perpendicular to its axis in two equal halves then its new pole strength $$m’$$ and magnetic moment $$M’$$ are respectively
When a bar magnet cut perpendicular to its axis into two equal parts then $$m' = m$$ and length $$\ell ' = \frac{\ell }{2}$$
$$\therefore M' = m\ell ' = m\frac{\ell }{2} = \frac{M}{2}$$
86.
A magnetic needle lying parallel to a magnetic field requires $$W$$ units of work to turn it through $${60^ \circ }.$$ The torque required to maintain the needle in this position will be
87.
Needles $${N_1},{N_2}$$ and $${N_3}$$ are made of a ferromagnetic, a paramagnetic and a diamagnetic substance respectively. A magnet when brought close to them will
A
attract $${N_1}$$ and $${N_2}$$ strongly but repel $${N_3}$$
B
attract $${N_1}$$ strongly, $${N_2}$$ weakly and repel $${N_3}$$ weakly
C
attract $${N_1}$$ strongly, but repel $${N_2}$$ and $${N_3}$$ weakly
Ferromagnetic substance has magnetic domains whereas paramagnetic substances have magnetic dipoles which get attracted to a magnetic field.
Diamagnetic substances do not have magnetic dipole but in the presence of external magnetic field due to their orbital motion of electrons these substances are repelled.
88.
A watch glass containing some powdered substance is placed between the pole pieces of a magnet. Deep concavity is observed at the centre. The substance in the watch glass is
89.
Time periods of vibration of two bar magnets in sum and difference positions are $$4\,\sec$$ and $$6\,\sec$$ respectively. The ratio of their magnetic moments $$\frac{{{M_1}}}{{{M_2}}}$$ is
90.
A circular coil of $$16$$ turns and radius $$10\,cm$$ carries a current of $$0.75\,A$$ and rest with its plane normal to an external magnetic field of $$5.0 \times {10^{ - 2}}T.$$ The coil is free to rotate about its stable equilibrium position with a frequency of $$2.0\,{s^{ - 1}}$$ Compute the moment of inertia of the coil about its axis of rotation.
The magnetic moment of the coil is
$$M = NIA = 16 \times 0.75 \times \pi \times {\left( {0.1} \right)^2} = 0.377\,A{m^2}$$
If $$K$$ be the moment of inertia of the coil about its axis of rotation, then its period of oscillation in a magnetic field $$B$$ is given by
$$T = 2\pi \sqrt {\frac{K}{{MB}}} $$
or its frequency $$v$$ is $$ = \frac{1}{T} = \frac{1}{{2\pi }}\sqrt {\frac{{MB}}{K}} $$
This gives $$K = \frac{{MB}}{{4{\pi ^2}{v^2}}}$$
Given that $$B = 5.0 \times {10^{ - 2}}T,M = 0.377\,A{\text{ - }}{m^2}\,{\text{and}}\,v = 2{s^{ - 1}}$$
$$\therefore K = \frac{{0.377 \times 5.0 \times {{10}^{ - 2}}}}{{4 \times {{\left( {3.14} \right)}^2} \times {{\left( 2 \right)}^2}}} = 1.2 \times {10^{ - 4}}kg{m^2}$$