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Two objects of masses 100 g and 200 g are moving along the same line and direction with velocities of 2ms1 and 1ms1 respectively. They collide and after the collision, the first object moves at a velocity of 1.67ms1 . Determine the velocity of the second object.

Answer
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Hint:When an object ‘A' exerts a force on an object ‘B,' object B replies with a force of equal magnitude but opposite direction, according to Newton's third law. The law of conservation of momentum was derived from this concept by Newton. And in order to answer this question, we will apply this concept to arrive at our desired result.

Complete step by step answer:
Law of conservation of momentum states that- “For two or more bodies in an isolated system acting upon each other, their total momentum remains constant unless an external force is applied. Therefore, momentum can neither be created nor destroyed.”Following are the examples of law of conservation of momentum:
-Air-filled balloons
-System of gun and bullet
-Motion of rockets

Given:Mass of first object (m1)=100g=0.1kg
Mass of second object (m2)=200g=0.2kg
Velocity of m1 before collision (v1)=2ms1
Velocity of m2 before collision (v2)=1ms1
Velocity of m1 after collision (v3)=1.67ms1
We have to find out the velocity of m2 after collision i.e. v4
According to the law of conservation of momentum,
Total momentum before collision = Total momentum after collision
Therefore, m1v1+m2v2=m1v3+m2v4
Substituting the above values in the equation
2(0.1)+1(0.2)=1.67(0.1)+v4×(0.2)
0.4=0.167+0.2×v4
v4=1.165ms1

Hence, the velocity of m2 after collision is 1.165ms1.

Note:This law of conservation of momentum is true regardless of how difficult the force between particles is. Similarly, if there are multiple particles, the overall change in momentum is 0 since the momentum exchanged between each pair of particles sums to zero. All interactions, including collisions and separations induced by explosive forces, are subject to this conservation law. It can also be applied to situations where Newton's rules do not apply, such as in relativity theory and electrodynamics.