Energy and Momentum in Collisions

Energy and Momentum

Energy and momentum both relate to forces that act on objects, but they are different concepts. The simplest difference between energy and momentum is that energy is a scalar quantity and momentum is a vector. Work and energy (which are equivalent concepts, according to the work-energy theorem) do not have a direction associated with their values (the definition of a scalar). In contrast, momentum has a direction as well as a value (the definition of a vector).

The difference between energy and momentum can be better understood using the related quantity impulse, which was discussed in the previous section. Impulse is equal to a net force, Energy and momentum 1, applied over an interval of time Energy and momentum 2,

Energy and momentum 3

The impulse-momentum theorem states that impulse is also equal to a change in momentum,

Energy and momentum 4

In this formula, Energy and momentum 5 is the momentum at time t1, and Energy and momentum 6 is the momentum at time t2. The Greek letter Energy and momentum 7 ("delta") is used to mean "the change in". Using these formulas, the change in momentum can be written,

Energy and momentum 8

Therefore, a change in momentum is the result of a net force applied for an amount of time.

Work is equivalent to a net force applied over a distance. If this distance is expressed as a difference between two displacements, Energy and momentum 9, then the formula for work is,

Energy and momentum 10

By the work-energy theorem, work is equal to a change in kinetic energy,

Energy and momentum 11

Using these formulas, the change in kinetic energy can be written,

Energy and momentum 12

Now, the formulas for the change in momentum and the change in kinetic energy can be compared. The change in momentum is,

Energy and momentum 8

The change in kinetic energy is,

Energy and momentum 12

These formulas show that the change in kinetic energy is related to the distance over which a force acts, whereas the change in momentum is related to the time over which a force acts.

An example is the collision between a tennis racket and a tennis ball. The force of contact is the result of the tennis player accelerating the tennis racket toward an incoming ball. When the ball makes contact with the racket, the racket strings bend, the ball compresses, and they briefly travel together. The time they travel together may only be a small fraction of a second, but that brief time is what determines the change in momentum. During this time, the tennis racket travels forward. The distance the racket travels while the ball is in contact determines the change in kinetic energy.

What the above example shows is that momentum and energy are different quantities. What it also shows is that they both change as a result of the same collision. For that reason, they can examined in combination to understand a collision.

Objects involved in a collision exert forces on each other. If these forces are the only ones that act on the objects, then the system can be considered closed or isolated. In this case, the system is said to have only internal forces. In the real world, there are many collisions in which the internal forces are significantly greater than external forces. For example, the air resistance around a bowling ball hitting the pins is a tiny effect compared to the force of the collision. The external forces can be neglected, and the system can be assumed to be closed.

In a system that is closed, or assumed to be closed, momentum is conserved. We will normally assume this to be true for any collisions in AP Physics. However, there are different types of collisions, depending whether or not energy is conserved.

Inelastic Collisions

In an inelastic collision, momentum is conserved, but energy is not. Usually, energy is lost to the system as a result of heating, vibration, deformation of the objects, or other effects. For example, in a collision between two cars, part of the energy of the collision is transferred to bending the metal. Energy is absorbed by the structure of the cars.

If Energy and momentum 5 is the total momentum before a collision, and Energy and momentum 6 is the momentum after, then for inelastic collisions,

Inelastic collisions 1

In a previous section, a formula for energy non-conservation was presented,

Inelastic collisions 2

In this formula, K1 is the kinetic energy at some initial time, U1 is the potential energy at the initial time, Inelastic collisions 3 is "other" work, which is either gained or lost to the system, K2 is the kinetic energy at some later time, and U2 is the potential energy at the later time. If the times are taken to be immediately before and immediately after a collision, then the position before and after is the same. Potential energy is associated with position, so the potential energy before and after must be the same,

Inelastic collisions 4  (immediately before and after a collision)

For an inelastic collision, the energy non-conservation formula is therefore,

Inelastic collisions 5

If energy is lost to the system during the collision, Inelastic collisions 3 must have a negative value.

These formulas can be re-written for a collision between two objects:

  • Object A with mass mA, pre-collision velocity Inelastic collisions 6, and post-collision velocity Inelastic collisions 7

  • Object B with mass mB, pre-collision velocity Inelastic collisions 8, and post-collision velocity Inelastic collisions 9

The inelastic collision momentum formula is,

Inelastic collisions 10

The inelastic collision energy formula is,

Inelastic collisions 11

Perfectly Inelastic Collisions

A special case of inelastic collision is called the "perfectly" or "completely" inelastic collision. In a perfectly inelastic collision, two objects collide and stick together. The momentum of the objects before the collision is conserved, but the total energy is not conserved. The final velocity of the combined objects depends on the masses and velocities of the two objects that collided. The objects remain stuck together, so the final velocities must be equal,

Perfectly inelastic collisions 1

For simplicity, the final velocity of the combined objects can be labeled Perfectly inelastic collisions 2.

The perfectly inelastic collision momentum formula is,

Perfectly inelastic collisions 3

The inelastic collision energy formula is,

Perfectly inelastic collisions 4

Elastic Collisions

In an elastic collision, both momentum and energy are conserved. In this case, the forces between the colliding objects are conservative. An example of real objects that have (approximately) elastic collisions are billiard balls. These compress at the collision site for an instant, but then spring back. They momentarily store elastic potential energy, but then it is converted back to kinetic energy. No energy is lost during the collision, so there is no work lost to "other" sources,

Perfectly inelastic collisions 5

The elastic collision momentum formula is,

Inelastic collisions 10

The elastic collision energy formula is,

Perfectly inelastic collisions 6

Collisions Summary

The momentum and energy conservation rules for collisions can be written in a concise way as follows:

In a collision in which the external forces can be neglected (a closed system), momentum is conserved. This is almost always assumed in AP Physics problems.

In elastic collisions only, kinetic energy is also conserved. The total kinetic energy before the collision is equal to the total kinetic energy after.



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