# Conservation of Momentum

#### Topics

• Conservation of linear momentum
• Law of conservation of linear momentum
• Applications of the law of conservation of linear momentum

## Notes

Law of conservation of Momentum:
From Newtons third law of motion we know that whenever a force is applied on a body there will be an equal and opposite reaction. Action and reaction forces result in change in velocities of both the bodies which in turn change the momentum of the bodies.

In an elastic collision the initial momentum of the bodies before collision is found to be equal to the final momentum of the bodies after collision.

Law of conservation of motion states that if a group of bodies are exerting force on each other. ie. Interacting with each other, their total momentum remains constant before and after the collision provided there is no external force acting on them.

Suppose two objects (two balls A and B, say) of masses mA and mB are travelling in the same direction along a straight line at different velocities uA and uB, respectively [Fig.(a)]. And there are no other external unbalanced forces acting on them. Let uA > uB and the two balls collide with each other as shown in Fig.(b). During collision which lasts for a time t, the ball A exerts a force FAB on ball B and the ball B exerts a force FBA on ball A. Suppose vA and vB are the velocities of the two balls A and B after the collision, respectively [Fig.(c)].

the momenta (plural of momentum) of ball A before and after the collision are mAuA and mAvA, respectively. The rate of change of its momentum (or FAB) during collision will be

"m"_"A"("v"_"A" - "u"_"A")/"t"

Similarly, the rate of change of momentum of ball B=(FBA) during the collison will be

"m"_"B"("v"_"B" - "u"_"B")/"t"

According to the third law of motion, the force FAB exerted by ball A on ball B and the force FBA exerted by the ball B on ball A must be equal and opposite to each other. Therefore, FAB = – FBA or

"m"_"A"("v"_"A" - "u"_"A")/"t"= "m"_"B"("v"_"B" - "u"_"B")/"t"

This gives,
mAuA + mBuB = mAvA + mBvB

Since (mAuA + mBuB) is the total momentum of the two balls A and B before the collision and (mAvA + mBvB) is their total momentum after the collision, we observe that the total momentum of the two balls remains unchanged or conserved provided no other external force acts. As a result of this ideal collision experiment, we say that the sum of momenta of the two objects before collision is equal to the sum of momenta after the collision provided there is no external unbalanced force acting on them. This is known as the law of conservation of momentum. This statement can alternatively be given as the total momentum of the two objects is unchanged or conserved by the collision.

## Conservation of Momentum

• In an isolated system, the total momentum is conserved.

Example 1. In a Spinning top, total momentum = 0. For every point, there is another point on the opposite side that cancels its momentum.

Example 2. Bullet fired from a Rifle
Initially, momentum = 0
Later, the trigger is pulled, bullet gains momentum in àdirection, but this is cancelled by rifle’s ß momentum. Therefore, total momentum = 0

During the process, the chemical energy in gunpowder gets converted into heat, sound and chemical energy.

Example 3. Rocket propulsion
Initially, mass of rocket: M. It just started moving with velocity v
Initial momentum = Mv

Later, gases are ejected continuously in opposite direction with a velocity relative to rocket in downward direction giving a forward push to the rocket.

Mass of the rocket becomes (M-m)
Velocity of the rocket becomes (v + v’)
Final momentum = (M –m) (v + v’)
Thus, Mass × velocity = constant

Collision of Bodies

Let the two bodies 1 & 2 have momentum p_1 & p_2 before they collided with each other. After collision their momentum are p_1’ and p_2’ respectively.

By Newton’s Second law,
F = (dp)/(dt)

For 1: F_(12) = (p_1’ – p_1) /(∆t)
For 2: F_(21) = (p_2’ – p_2) /(∆t)

By Newton’s Third law,
F _(12) = - F_(21)
(p_1’ – p_1)/(∆t) = (p_2’ – p_2) /(∆t)
(p_1’ – p_1) = (p_2’ – p_2)
p_1’ + p_2’ = p_1 + p_2

Conclusion:
Final momentum of the system = Initial momentum of the system

Problem: A railway truck A of mass 3 × 104 kg travelling at 0.6 m/s collides with another truck B of half its mass moving in the opposite direction with a velocity of 0.4 m/s. If the trucks couple automatically on collision, find the common velocity with which they move.
Solution.
M1 = 3 × 104 kg
m2 = ½ of mass of A = 1.5 × 104 kg
u1 = 0.6 m/s
u2 = -0.4 m/s

Before collision:
m1u1 + m2u2 = 3 × 104 × 0.6 + 1.5 × 104 ×(-0.4) = 1.2 × 104 kg m/s

After collision:
(m1+ m2) v = 4.5 × 104v kg m/s

As per conservation of momentum,
1.2 × 104 = 4.5 × 104v
V = 1.2/ 4.5 = 0.27 m/s
Therefore, the common velocity is 0.27m/s

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