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Question: The track shown in figure is frictionless. The block B of mass 2m is lying at rest and the block A o...

The track shown in figure is frictionless. The block B of mass 2m is lying at rest and the block A of mass m is pushed along the truck with some speed. The collision between A and B is perfectly elastic. With what velocity should the block A be started to get the sleeping man awakened.

Explanation

Solution

The kinetic energy is defined as the energy of a body by the virtue of its motion. The potential energy is the energy of the body by the virtue of its height. Conservation of momentum says that the sum of momentum of two bodies will be conserved before and after the collision.

Complete step by step solution:
It is given in the problem that the track is frictionless, the block B of mass 2m is lying at rest and the block A of mass m is pushed along the truck with some speed. The collision between A and B is perfectly elastic. We need to tell with what velocity should the block A be started to get the sleeping man awakened.

Let the initial velocity of the block A isu1{u_1}, the velocity of block A after collision beu2{u_2}, the initial velocity of the block B bev1{v_1}, the velocity of the block A after collision is vv'.

The change in the potential energy will equal the kinetic energy of block A.
mgh+12m×u12=12m×u22\Rightarrow mgh + \dfrac{1}{2}m \times {u_1}^2 = \dfrac{1}{2}m \times {u_2}^2

The mass of the block A is m and the initial and final velocity of the block A is u1{u_1} andu2{u_2}.

mgh=12m×u2212m×u12 \Rightarrow mgh = \dfrac{1}{2}m \times {u_2}^2 - \dfrac{1}{2}m \times {u_1}^2
u22=u12+2gh\Rightarrow {u_2}^2 = {u_1}^2 + 2gh
u2=u12+2gh\Rightarrow {u_2} = \sqrt {{u_1}^2 + 2gh}………eq. (1)

For motion of block B.
The kinetic energy of the block will get converted into potential energy.

12×2m×v12=2m×g×h \Rightarrow \dfrac{1}{2} \times 2m \times {v_1}^2 = 2m \times g \times h
v12=2×g×h\Rightarrow {v_1}^2 = 2 \times g \times h
v1=2gh\Rightarrow {v_1} = \sqrt {2gh}………eq. (2)

Applying conservation of energy for the collision of block A and B.

mu2=mv+2m×v1 \Rightarrow m{u_2} = mv' + 2m \times {v_1}
u2=v+2×v1\Rightarrow {u_2} = v' + 2 \times {v_1}………eq. (3)

Replacing equation (1) in equation (3)

u2=v+2×2gh\Rightarrow {u_2} = v' + 2 \times \sqrt {2gh}
u2v=2×2gh\Rightarrow {u_2} - v' = 2 \times \sqrt {2gh}………eq. (4)

The kinetic energy of the block A and B before and after the collision.

12m×u22=12m×(v)2+12(2m)×v12 \Rightarrow \dfrac{1}{2}m \times {u_2}^2 = \dfrac{1}{2}m \times {\left( {v'} \right)^2} + \dfrac{1}{2}\left( {2m} \right) \times {v_1}^2
u22=(v)2+2×v12\Rightarrow {u_2}^2 = {\left( {v'} \right)^2} + 2 \times {v_1}^2
u22(v)2=+2×v12\Rightarrow {u_2}^2 - {\left( {v'} \right)^2} = + 2 \times {v_1}^2………eq. (5)

Replacing the value of equation (2) in equation (5) we get.

u22(v)2=+2×(2gh)2 \Rightarrow {u_2}^2 - {\left( {v'} \right)^2} = + 2 \times {\left( {\sqrt {2gh} } \right)^2}
u22(v)2=+2×2gh\Rightarrow {u_2}^2 - {\left( {v'} \right)^2} = + 2 \times 2gh
u22(v)2=4gh\Rightarrow {u_2}^2 - {\left( {v'} \right)^2} = 4gh………eq. (6)

Dividing equation (6) by equation (4).

u22(v)2u2v=4gh22gh \Rightarrow \dfrac{{{u_2}^2 - {{\left( {v'} \right)}^2}}}{{{u_2} - v'}} = \dfrac{{4gh}}{{2\sqrt {2gh} }}
(u2v)×(u2+v)u2v=2gh\Rightarrow \dfrac{{\left( {{u_2} - v'} \right) \times \left( {{u_2} + v'} \right)}}{{{u_2} - v'}} = \sqrt {2gh}
u2+v=2gh\Rightarrow {u_2} + v' = \sqrt {2gh}………eq. (7)

Adding equation (4) and equation (7) we get.

(u2v)+(u2+v)=2×2gh+2gh\Rightarrow \left( {{u_2} - v'} \right) + \left( {{u_2} + v'} \right) = 2 \times \sqrt {2gh} + \sqrt {2gh}
2×u2=3×2gh\Rightarrow 2 \times {u_2} = 3 \times \sqrt {2gh}
u2=32×2gh\Rightarrow {u_2} = \dfrac{3}{2} \times \sqrt {2gh}………eq. (8)

Equating equation (1) and equation (8) we get.

u12+2gh=32×2gh\Rightarrow \sqrt {{u_1}^2 + 2gh} = \dfrac{3}{2} \times \sqrt {2gh}

squaring on both sides we get,

(u12+2gh)2=94×(2gh)2 \Rightarrow {\left( {\sqrt {{u_1}^2 + 2gh} } \right)^2} = \dfrac{9}{4} \times {\left( {\sqrt {2gh} } \right)^2}
u12+2gh=94×(2gh)\Rightarrow {u_1}^2 + 2gh = \dfrac{9}{4} \times \left( {2gh} \right)
u12+2gh=92×(gh)\Rightarrow {u_1}^2 + 2gh = \dfrac{9}{2} \times \left( {gh} \right)
2(u12+2gh)=9gh\Rightarrow 2\left( {{u_1}^2 + 2gh} \right) = 9gh
2u12+4gh=9gh\Rightarrow 2{u_1}^2 + 4gh = 9gh
2u12=5gh\Rightarrow 2{u_1}^2 = 5gh
u1=5gh2\Rightarrow {u_1} = \sqrt {\dfrac{{5gh}}{2}}
u1=25gh\Rightarrow {u_1} = \sqrt {2 \cdot 5gh}.

The velocity with which the block A should be pushed is equal to

u1=25gh{u_1} = \sqrt {2 \cdot 5gh} .

Note: It is advisable for the students to remember and understand the concept of conservation of energy students should also remember the formula of the kinetic and potential energy. Whenever an object falls from a height then the kinetic energy gets converted into potential energy of the object.