Question
Question: A bar magnet of magnetic moment \(M\) is placed at right angles to a magnetic induction \(B\). If a ...
A bar magnet of magnetic moment M is placed at right angles to a magnetic induction B. If a force F is experienced by each pole of the magnet, the length of the magnet will be
A. FMB
B. MBF
C. BMF
D. MBF
Solution
The question states that a bar magnet is placed at right angles to a magnetic induction. So, we shall use the formula of torque experienced by a bar magnet when it interacts with the magnetic induction which is given as τ=M×B where τ is the torque, M is the magnetic moment and B is magnetic induction.Also, we will use the relation that expresses torque in terms of the force experienced by a body which is given as τ=r×F where F is the force experienced by each pole of the magnet and r is the distance from each pole from the point of rotation.We will then use the fact that the magnet and magnetic induction are placed at right angles. So, θ=900 .Then we shall equate both the relations to get the answer.
Complete step by step answer:
The torque on a bar magnet with a given magnetic moment when placed in a magnetic induction is given as τ=M×B where τ is the torque, M is the magnetic moment and B is magnetic induction.This can be rewritten as,
τ=MBsinθ
Now it is given that θ=900
⇒τ=MBsin900
⇒τ=MB.......(1)
Now, the basic definition of torque says that it is the cross product of the force experienced at the point in consideration and the distance from the axis of rotation.
τ=r×F
where F is the force experienced by each pole of the magnet and r is the distance from each pole from the point of rotation.
Hence, r=L
where L is the length of the bar magnet.
τ=L×F
This can be rewritten as τ=LFsinθ
Now it is given that θ=900
⇒τ=LFsin900
⇒τ=LF.......(2)
From (1) and (2) we get,
LF=MB
∴L=FMB
Hence, option A is the correct answer.
Note: While dealing with cross products, the direction of every physical quantity in a particular physical relation must be known or derived. In this question, the direction of magnetic moment and magnetic induction was perpendicular. And since, the cross product always gives a perpendicular vector, all the three quantities-torque, magnetic moment and magnetic were mutually perpendicular. This makes it a special case and can be used directly in many numericals based on the same concept.