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Question: Two particles \(A\) and \(B\) are placed as shown in the figure. The particle \(A\), on the top of t...

Two particles AA and BB are placed as shown in the figure. The particle AA, on the top of the tower, is projected horizontally with a velocity uuand the particle BB is projected along the surface towards the tower, simultaneously. If both particles meet each other, then the speed of projection of particle BB is [ignore any friction]

A.dg2Hud\sqrt {\dfrac{g}{{2H}}} u
B.dg2Hd\sqrt {\dfrac{g}{{2H}}}
C.dg2Hud\sqrt {\dfrac{g}{{2H}}} - u
D.uu

Explanation

Solution

In the diagram as both the objects are moving with different velocities, we need to solve the question considering the non-inertial frame of reference. We need to write the equation of particle in the x-direction and then write the direction of motion of a particle in the Y direction. Then we need to use the two equations to solve the question.

Complete step by step answer:
As we can see from the diagram that object AA moves with velocity uu and object BB moves with velocity vv.
Since object AAis thrown horizontally and object BB is thrown upwards, they must meet at a point.
Therefore, we consider non-inertial frame of reference of BB, thus the relative velocity of AA with respect to BB is written as: v+uv + u
We know the velocity of an object when multiplied by time, giving us the distance travelled by it.
Therefore, in the x-axis,
(v+u)t=d(v + u)t = d
On rearranging the equation, we get:
t=d/(u+v)t = d/(u + v)
On squaring both sides, we get:
t2=d2/(u+v)2{t^2} = {d^2}/{(u + v)^2}
Now, let us consider the Y-axis:
The distance travelled can be obtained as:
s=uot+12at2s = {u_o}t + \dfrac{1}{2}a{t^2}
Where ss is the distance travelled in the Y-axis, aa is the acceleration, uo{u_o}is the initial velocity.
Now, in this case, uo{u_o} is zero as the object is thrown.
Thus,
H=12at2H = \dfrac{1}{2}a{t^2}
In this case, the acceleration implies the acceleration due to gravity.
Now, substituting the value of t2{t^2}as obtained from the equation of X-axis, we get:
H=12g(d2/(u+v)2)H = \dfrac{1}{2}g({d^2}/{(u + v)^2})
Thus,
On solving the equation, we obtain:
v=dg2Huv = d\sqrt {\dfrac{g}{{2H}}} - u
This is the required solution.
Option (C ) Is correct.

Note:
Non-inertial frame of reference is used when a body accelerates with respect to the inertial frame. In the case of the inertial frame, the laws of motion remain the same, whereas in the case of the non-inertial frame the laws of motion vary from one frame to another. In the non-inertial frame, it gives rise to pseudo force.