2L

Elastic and inelastic collisions

Classifying collisions as elastic, inelastic or completely inelastic by comparing kinetic energy before and after, where the lost kinetic energy goes, one-dimensional elastic collisions, Newton's cradle, and the two-stage analysis of the ballistic pendulum.

Lift one ball of a Newton's cradle and let it go. One ball flies out the far end, at almost the same speed. Why not two balls at half the speed? That would conserve momentum too. The answer is energy: only one ball out at full speed also keeps the kinetic energy the same, and the steel balls are springy enough that very little is lost.

Momentum is conserved in every collision in a closed system. Kinetic energy is not. Comparing the kinetic energy before and after is how physicists classify a collision, and it tells you how much energy went into sound, heat and bent metal.

Three kinds of collision

TypeMomentumKinetic energyExamples
Elasticconservedconserved: $\Sigma K_{before} = \Sigma K_{after}$gas molecules, atoms and subatomic particles; very nearly, steel balls and billiard balls
Inelasticconservedsome lost: $\Sigma K_{after} \lt \Sigma K_{before}$most real collisions: a ball bouncing, cars bumping
Completely inelasticconservedmaximum possible loss; objects stick togethera bullet lodging in a block, a rugby tackle, coupling train carriages
Momentum is conserved in all three kinds of collision. Kinetic energy is conserved only in an elastic collision.

Kinetic energy "lost" in an inelastic collision isn't destroyed. It becomes thermal energy (the objects warm slightly), sound, and the work done permanently deforming the objects. Total energy is always conserved.

A completely inelastic collision doesn't always lose all the kinetic energy. If the total momentum isn't zero, the combined object must still be moving, so some kinetic energy remains. It is the maximum loss allowed by conservation of momentum.

Testing whether a collision is elastic

Worked example: classifying a collision

A 0.50 kg trolley moving at 2.0 m s⁻¹ hits a stationary 1.5 kg trolley. Afterwards the 0.50 kg trolley moves backwards at 1.0 m s⁻¹. Find the velocity of the 1.5 kg trolley and decide whether the collision is elastic.

$0.50(2.0) = 0.50(-1.0) + 1.5v$, so $1.5v = 1.5$ and $v = 1.0$ m s⁻¹ forwards.
momentum
$\tfrac12(0.50)(2.0)^2 = 1.0$ J.
KE before
$\tfrac12(0.50)(1.0)^2 + \tfrac12(1.5)(1.0)^2 = 0.25 + 0.75 = 1.0$ J.
KE after
Kinetic energy is conserved, so the collision is elastic.
conclusion
Worked example: a completely inelastic collision

A 1200 kg car at 20 m s⁻¹ rear-ends a stationary 800 kg car and they move off together. What fraction of the kinetic energy is lost?

$1200(20) = 2000v$, so $v = 12$ m s⁻¹.
momentum
Before: $\tfrac12(1200)(20)^2 = 2.40 \times 10^5$ J. After: $\tfrac12(2000)(12)^2 = 1.44 \times 10^5$ J.
kinetic energies
$\dfrac{2.40 - 1.44}{2.40} = 0.40$, so 40% of the kinetic energy becomes heat, sound and crumpled metal.
fraction lost

Elastic collisions in one dimension

For a head-on elastic collision you have two equations (momentum and kinetic energy) and can solve for both final velocities. Three results are worth remembering for a moving object A hitting a stationary object B:

  • Equal masses: A stops and B moves off with A's original velocity. They swap velocities.
  • A much heavier than B: A barely slows, and B shoots off at almost twice A's speed.
  • A much lighter than B: A bounces back at almost its original speed, and B hardly moves.

Newton's cradle is the equal-mass case in a chain. Each ball passes its velocity to the next, so one ball in gives one ball out. Two balls in give two balls out, because that is the only outcome that conserves both momentum and kinetic energy.

A Newton's cradle with five steel balls on a black background, one ball swung out on each side
A Newton's cradle. The collisions between the hardened steel balls are close to elastic, but a little kinetic energy is lost each time as sound and heat, so the swinging gradually dies away.Photo: Sheila Sund, CC BY 2.0

The ballistic pendulum

Before electronic timers, the speed of a bullet was measured by firing it into a heavy wooden block hanging on strings and measuring how high the block swung. The analysis has two separate stages, and using the right conservation law for each stage is the whole trick.

A ballistic pendulum. The bullet lodges in the block (momentum conserved), then the block swings up (mechanical energy conserved).
  1. The collision is completely inelastic. Kinetic energy is not conserved (most becomes heat and deformation), but momentum is: $mu = (m + M)V$.
  2. The swing involves no collision. Only gravity does work (string tension is perpendicular to the motion), so mechanical energy is conserved: $\tfrac12(m + M)V^2 = (m + M)gh$, giving $V = \sqrt{2gh}$.
Worked example: speed of a pellet

A 10 g pellet is fired into a 2.0 kg hanging block, which rises 11.4 cm. Find the pellet's speed and the percentage of its kinetic energy lost in the collision.

$V = \sqrt{2gh} = \sqrt{2 \times 9.8 \times 0.114} = 1.49$ m s⁻¹.
swing (energy)
$u = \dfrac{(m + M)V}{m} = \dfrac{2.010 \times 1.49}{0.010} = 3.0 \times 10^2$ m s⁻¹.
collision (momentum)
Before: $\tfrac12(0.010)(300)^2 = 450$ J. After: $\tfrac12(2.010)(1.49)^2 = 2.24$ J. About 99.5% is lost in the collision.
energy check
Using energy conservation for the whole process ($\tfrac12 mu^2 = (m + M)gh$) would give $u = 21$ m s⁻¹, wrong by a factor of 14.
the trap
An old engraving of a tall wooden tripod with a heavy block hanging from a pivot at the top and a strip of tape trailing below
Benjamin Robins invented the ballistic pendulum in 1742. A ribbon pulled out through a slot recorded how far the heavy block swung.Photo: Benjamin Robins, Public domain
InteractiveBallistic pendulum
Try this
  • Fire a 10 g bullet at 300 m/s into a 2.0 kg block. The block moves off at 1.493 m/s and rises 11.4 cm. The kinetic energy drops from 450 J to 2.24 J, a 99.5% loss.
  • Double the block's mass to 4.0 kg: $V$ halves (to 0.748 m/s) and the rise drops to a quarter (2.9 cm).
  • Turn on Measure mode. Fire, read the rise, work out the bullet speed with the two-stage method, then press Reveal to check.
  • Try 20 g at 500 m/s into a 1.0 kg block: the block would swing right over the top.

Test yourself

  1. In an elastic collision,

  2. A 2.0 kg ball at 3.0 m s⁻¹ hits a stationary 1.0 kg ball. Afterwards the 2.0 kg ball moves at 1.0 m s⁻¹ and the 1.0 kg ball at 4.0 m s⁻¹, both forwards. The collision is

  3. A 0.020 kg bullet at 400 m s⁻¹ embeds in a 4.0 kg block at rest on ice. The speed of the block afterwards is

  4. In the previous question, the percentage of kinetic energy lost is about

Label the ballistic pendulum.

bulletblock at restrise hblock + bulletCollision: momentum conserved. Swing: mechanical energy conserved.

Classify each collision.

In every collision in a closed system, total is conserved. If total kinetic energy is also conserved, the collision is . When objects stick together the collision is completely . In a head-on elastic collision between equal masses, the objects swap . Kinetic energy lost in a collision is transformed into heat, sound and .

6 marks

A student fires a 5.0 g dart at a 0.25 kg block hanging from a light string. The dart sticks in the block, which rises 18 cm. (a) Calculate the speed of the dart. (3 marks) (b) Compare the collision with an elastic collision, using calculations of kinetic energy to support your answer. (3 marks)