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Question: A magnetic rod with a length of 6.00 cm, radius 3.00 mm, and (uniform) magnetization \[2.70 \times {...

A magnetic rod with a length of 6.00 cm, radius 3.00 mm, and (uniform) magnetization 2.70×103A/m2.70 \times {10^3}A/m can turn about its center like a compass needle. It is placed in a uniform magnetic field B of magnitude 35.0 mT, such that the directions of its dipole moment and make an angle of 6868^\circ .
(a) What is the magnitude of the torque on the rod due to B?
(b) What is the change in the orientation energy of the rod if the angle changes to 3434^\circ ?

Explanation

Solution

Magnetization is also called magnetic polarization and is the vector field that represents the density of the induced magnetic dipole moments in a material. It depends on the size of the dipole moments of the atoms in a given substance and also the degree to which these dipole moments are aligned to each other.

Complete step by step solution:
Given data:
The length of the rod, L=6cm=6×102mL = 6cm = 6 \times {10^{ - 2}}m
The radius of the rod, R=3mm=3×103mR = 3mm = 3 \times {10^{ - 3}}m
Magnetization, M=2.70×103A/mM = 2.70 \times {10^3}A/m
Initial angle =68= 68^\circ
Final angle =34= 34^\circ
Magnetic field, B=35mT=35×103TB = 35mT = 35 \times {10^{ - 3}}T
The magnitude of the torque on the rod due to B =?
The change in the orientation energy of the rod =?
a) We know that the magnetic moment of the rod is given by,
μ=M×V\mu = M \times V
μ=M×πR2×L\Rightarrow \mu = M \times \pi {R^2} \times L
μ=2.70×103×π×(3×103)2×(6×102)\Rightarrow \mu = 2.70 \times 1{0^3} \times \pi \times {\left( {3 \times {{10}^{ - 3}}} \right)^2} \times \left( {6 \times {{10}^{ - 2}}} \right)
μ=4.57×103Am2\Rightarrow \mu = 4.57 \times {10^{ - 3}}A{m^2}
We know that the magnitude of the torque on the rod is given by,
τ=μBsinθ\tau = \mu B\sin \theta
τ=(4.57×103)(35×103)sin68\Rightarrow \tau = \left( {4.57 \times {{10}^{ - 3}}} \right)\left( {35 \times {{10}^{ - 3}}} \right)\sin 68^\circ
τ=1.48×104Nm\Rightarrow \tau = 1.48 \times {10^{ - 4}}Nm
Thus the magnitude of the torque on the rod due to B is 1.48×104Nm1.48 \times {10^{ - 4}}Nm.

b) Let ΔU\Delta U be the change in the orientation energy of the rod.
Then the change in the orientation energy of the rod is given by,
ΔU=μB(cosθfcosθi)\Delta U = - \mu B\left( {\cos {\theta _f} - \cos {\theta _i}} \right)
ΔU=4.57×103×35×103(cos34cos68)\Rightarrow \Delta U = - 4.57 \times {10^{ - 3}} \times 35 \times {10^{ - 3}}\left( {\cos 34^\circ - \cos 68^\circ } \right)
ΔU=72.9μJ\Rightarrow \Delta U = - 72.9\mu J
Thus the change in the orientation energy of the rod =72.9μJ = - 72.9\mu J.

Note: 1. Torque is a twisting force and is defined as the measure of how the force that is acting on an object causes it to rotate. Torque is a vector quantity. Unit of torque is newton-meter. Torque depends on the direction of the force on the axis.
2. The magnetic dipole is a tiny magnet of the microscopic to the subatomic dimensions which is equal to the flow of the electric charge around the loop.