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Question: What is the terminal speed of the bar? ![](https://www.vedantu.com/question-sets/bfddbcc8-e27e-41f...

What is the terminal speed of the bar?

\left( A \right)\dfrac{{mgR}}{{{B^2}{l^2}\sin \phi }} \\\ \left( B \right)\dfrac{{mgR\cos \phi }}{{{B^2}{l^2}{{\sin }^2}\phi }} \\\ \left( C \right)\dfrac{{mgR\sin \phi }}{{{B^2}{l^2}{{\cos }^2}\phi }} \\\ \left( D \right)\dfrac{{mgR\sin \phi }}{{{B^2}{l^2}\cos \phi }} \\\

Explanation

Solution

Hint : In order to solve the question, we are going to equate the magnetic field with the gravitational force, as in this condition only the bar will attain a terminal velocity. The terminal velocity is then derived from the equation by simplifying it and further solving the equation.
The formula used here is
Gravitational force is given by mgsinϕmg\sin \phi
And magnetic force is given by IlbcosϕIlb\cos \phi
Here, mgsinϕ=Ilbcosϕmg\sin \phi = Ilb\cos \phi
Here mm is the mass of the bar, gg is the acceleration of gravity, BB is the magnetic force, ll is the length of the rod, bb is the breadth, ϕ\phi is the angle.
The current in the bar II is given as
I=BlvcosϕRI = \dfrac{{Blv\cos \phi }}{R}

Complete Step By Step Answer:
The bar attains the terminal velocity when the magnetic field is balanced by the gravitational force, so if we equate the two forces then, the equation becomes
mgsinϕ=Ilbcosϕmg\sin \phi = Ilb\cos \phi
Here mm is the mass of the bar, gg is the acceleration of gravity, BB is the magnetic force, ll is the length of the rod, bb is the breadth, ϕ\phi is the angle.
Where on left hand side, we have the gravitational force and on the right hand side, we have the magnetic field
The current in the bar II is given as
I=BlvcosϕRI = \dfrac{{Blv\cos \phi }}{R}
Using this relation in the above equation
mgsinϕ=B2l2vcos2ϕRmg\sin \phi = \dfrac{{{B^2}{l^2}v{{\cos }^2}\phi }}{R}
Rearranging the terms we get, the relation for velocity
v=mgRsinϕB2l2cos2ϕv = \dfrac{{mgR\sin \phi }}{{{B^2}{l^2}{{\cos }^2}\phi }}
Hence, the terminal speed of the bar v=mgRsinϕB2l2cos2ϕv = \dfrac{{mgR\sin \phi }}{{{B^2}{l^2}{{\cos }^2}\phi }}
Hence, option (C)mgsinϕRB2l2cos2ϕ\left( C \right)\dfrac{{mg\sin \phi R}}{{{B^2}{l^2}{{\cos }^2}\phi }} is correct.

Note :
Terminal velocity is the steady speed that is achieved by the freely falling objects under gravity in air or in some medium. In this question, it is a very important step to see what all forces are acting on the bar and then checking the condition of equilibrium where the terminal velocity can be attained.