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Question: A weightless rod of length \[2l\] carries two equal masses \(m\) one second at lower end \(A\) and t...

A weightless rod of length 2l2l carries two equal masses mm one second at lower end AA and the other at the middle of the rod at BB . The rod can rotate in a vertical plane about a fixed horizontal axis passing through CC . What horizontal velocity must be imparted to the mass at AA so that it just completes the vertical circle.
A. 485gl\sqrt {\dfrac{{48}}{5}gl}
B. 455gl\sqrt {\dfrac{{45}}{5}gl}
C. 405gl\sqrt {\dfrac{{40}}{5}gl}
D. 355gl\sqrt {\dfrac{{35}}{5}gl}

Explanation

Solution

In this question first we will find the potential energy and then kinetic energy and then we will apply law of conservation of energy and then compare to get the horizontal velocity that must be imparted to the mass at AA so that it just completes the vertical circle.

Formula used:
K.E.=12mv2K.E. = \dfrac{1}{2}m{v^2}
Where,
mm is the mass and
vv is the velocity.
P.E=mghP.E = mgh
gg is the acceleration due to gravity and
hh is the height.

Complete step by step solution:

Given,
Length of the rod is 2l2l
And mass is given mm
Let the initial velocity given to the mass at A be uu
Then, the velocity of mass at B is u2\dfrac{u}{2}
As the system moves from initial position to final position.
Then, there is an increase in potential energy
And that is
P.Etotal=(mgh)A+(mgh)BP.{E_{total}} = {(mgh)_A} + {(mgh)_B}
Now substituting the value, we get,
P.Etotal=mg4l+mg2l P.Etotal=6mgl  P.{E_{total}} = mg4l + mg2l \\\ P.{E_{total}} = 6mgl \\\
We know that from law of conservation of energy potential energy is equal to kinetic energy
So,

6mgl=mvB22+mvA22 6mgl=12m(u2)2+12mu2  6mgl = \dfrac{{mv_B^2}}{2} + \dfrac{{mv_A^2}}{2} \\\ \Rightarrow 6mgl = \dfrac{1}{2}m{\left( {\dfrac{u}{2}} \right)^2} + \dfrac{1}{2}m{u^2} \\\

Where, velocity of mass at B is u2\dfrac{u}{2} substituting and further solving the equation,

6mgl=18mu2+12mu2 6mgl=58mu2  \Rightarrow 6mgl = \dfrac{1}{8}m{u^2} + \dfrac{1}{2}m{u^2} \\\ \Rightarrow 6mgl = \dfrac{5}{8}m{u^2} \\\

Now, cross multiplying to find uu

u2=485lg u=485gl  \Rightarrow {u^2} = \dfrac{{48}}{5}lg \\\ \Rightarrow u = \sqrt {\dfrac{{48}}{5}gl} \\\

So, the horizontal velocity must be imparted to the mass at AA so that it just completes the vertical circle 485gl\sqrt {\dfrac{{48}}{5}gl}
Hence, the correct option is A.

Note:
The potential energy of point A is (mgh)A=4mgl{(mgh)_A} = 4mgl because if we see in the diagram that the distance between final and initial position is 4l4l so we have put hh as 4l4l .You must remember the conservation of energy to solve this question.