Linear momentum is a product of the mass (m) of an object and the velocity (v) of the object. If an object has higher momentum, then it harder to stop it. The formula for linear momentum is p = mv. The total amount of momentum never changes, and this property is called conservation of momentum. Let us study more about Linear momentum and conservation of momentum.

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## Linear Momentum of System of Particles

We know that the linear momentum of the particle is

p = mv

Newton’s second law for a single particle is given by,

F =Â \( \frac{dP}{dt} \)

where F is the force of the particle. For ‘ n ‘ no. of particles totalÂ linearÂ momentum is,

P = p_{1Â }+ p_{2Â }+…..+p_{n}

each of momentum is written asÂ m_{1Â }v_{1Â }+ m_{2}v_{2Â }+ ………..+m_{n}v_{n}. We know that velocity of the centreÂ of mass is V =Â Â Î£Â \( \frac{m_i v_i}{M} \),

mv =Â Î£Â m_{i}v_{i}

So comparing these equations we get,

P = M V

Therefore we can say that the total linear momentum of a system of particles is equal to the product of the total mass of the system and the velocity of its center of mass. Differentiating the above equation we get,

\( \frac{dP}{dt} \) = MÂ \( \frac{dV}{dt} \) = MA

dv/dt is acceleration of centre of mass, MA is the force external. So,

\( \frac{dP}{dt} \) = F_{ext}

This above equation is nothing but Newton’s second law to a system of particles. If the total external force acting on the system is zero,

F_{extÂ }= 0 then,Â \( \frac{dP}{dt} \) = 0

This means that P = constant. So whenever the total force acting on the system of a particle is equal to zero then the total linear momentum of the system is constant or conserved. This is nothing but the law of conservation of total linear momentum of a system of particles.

**Browse more Topics under System Of Particles And Rotational Dynamics**

- Introduction to Rotational Dynamics
- Vector Product of Two Vectors
- Centre of Mass
- Motion of Centre of Mass
- Moment of Inertia
- Theorems of Parallel and Perpendicular Axis
- Rolling Motion
- Angular Velocity and Angular Acceleration
- Torque and Angular Momentum
- Equilibrium of a Rigid Body
- Angular Momentum in Case of Rotation About a Fixed Axis
- Dynamics of Rotational Motion About a Fixed Axis
- Kinematics of Rotation MotionÂ about a Fixed Axis

## Conservation of Total Linear Momentum of a System of Particles

Let us take the example of radioactive decay. What is radioactive decay? It is a process where an unstable nucleusÂ splits up in relatively stable nuclei releasing a huge amount of energy.

Suppose there is a parent nucleusÂ which is unstable and it wants to become stable, in order to attain stabilityÂ it will emitÂ Î± particle and another daughter nucleus.

This daughter nucleus is much more stable than the parent nucleus. This what radioactive decay is. Now suppose the parent nucleus is at rest and also the mass of theÂ Î± is ‘ m ‘ and the daughter nucleus is M.

So the mass of the parent nucleus will be **m + M.Â **Here everything that is happening is not due to the external force but all that happens is due to the internal force. So hereÂ F_{extÂ }= 0, we can say that

\( \frac{dP}{dt} \) = 0Â â‡’Â P = constant

## Solved Questions For You

Q1.Â Which of the following are practical applications of the law of conservation of linear momentum?

- When a man jumps out of the boat on the shore, the boat is pushed slightly away from the shore.
- The person left in the frictionless surface can get away from it by blowing air out of its mouth or by throwing some object in the direction opposite to the direction in which he wants to move.
- Recoiling of a gun
- None of these

Solution:Â A, B, and C

Q2.Â Two unequal masses are tiedÂ together with a compressed spring. When the cord is burnt with a matchstick releasing the spring; the two masses fly apart with equal :

- Momentum
- Acceleration
- Speed
- Kinetic energy

Solution: A. Initially, two unequal masses are tied together with a compressed spring. Then the cord is burnt with the matchstick and the spring released due to this the two masses fly apart and acquire velocities in inverse proportional to their masses and hence fly with equal momentum.

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