The general equation for conservation of linear momentum for a system of particles is:

Where:

If the kinetic energy is conserved in the system of particles then

Note that the velocity terms in the above equation are the magnitude of the velocities of the individual particles, with respect to an inertial reference frame (ground).

In a collision between particles, kinetic energy is conserved if the particles behave elastically during the collisions. This means that, during impact, the particles deform elastically; meaning they behave like perfectly elastic springs, absorbing and releasing the same energy during impact.

To help illustrate this concept consider the following analogy, where a spring is attached to a block, and another block collides with it. Both blocks are moving on a flat frictionless surface and no external forces are acting on the blocks in the direction of motion. The spring is a mathematical representation of the "springiness" of the particles as they collide.

There are three distinct stages:

In this stage, the total energy in the system is given by

The energy of the blocks is equal to their kinetic energy. The energy of the spring is zero since it is at its equilibrium (unstretched) length.

Therefore,

In this stage, the total energy in the system is given by

The energy of the blocks is equal to their kinetic energy. The energy of the spring is equal to its stored energy due to it being compressed.

Therefore,

where

Since the spring is assumed to be elastic, energy is conserved at this stage. Therefore, by the law of conservation of energy

In this stage, the total energy in the system is given by

The energy of the blocks is equal to their kinetic energy. The energy of the spring is zero since it is once again at its equilibrium (unstretched) length.

Therefore,

Since the spring is assumed to be elastic it has returned 100% of its energy to the system (stored during stage 2). Therefore, by the law of conservation of energy

As a result,

Stage 1 and stage 3 represent the initial and final states of the system, and from the above equation we can write

Therefore, for an elastic collision kinetic energy is conserved.

General equations can be developed for the elastic collision between two particles.

From equation (1) for the conservation of linear momentum we have

This equation can be expressed as its corresponding (scalar) equations along Cartesian

From equation (2) for the conservation of kinetic energy we have

For the special case of a head on elastic collision in one dimension, we can solve equations (3) and (4) for the final velocities of the two particles:

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