Coefficient of restitution and collisionsAQA A-Level Further Maths: Revision notes
Section 1
Newton's experimental law
For two bodies in a direct collision (along the line of motion), Newton's experimental law says where is the coefficient of restitution, a dimensionless constant that depends on the materials. With velocities before and after, along the same positive direction: . The values of satisfy . If the collision is perfectly elastic (no kinetic energy lost). If the bodies do not separate (they coalesce or move together). For some kinetic energy is lost.
Using the sum of the speeds as the speed of approach for particles moving in the same direction. Use velocities with signs: approach is .
Section 2
Direct collisions between two particles
To find two unknown velocities after a collision you need two equations:
- Conservation of momentum: .
- Newton's experimental law: . Solve them simultaneously. Example: equal masses , at m s⁻¹ chasing at m s⁻¹, . Momentum: . Newton: . So and m s⁻¹. For equal masses and a target at rest, the results are and .
Choose a positive direction, write both equations with signs, then solve by substitution or by adding and subtracting.
Section 3
Impact with a fixed smooth surface
When a particle hits a fixed smooth surface directly, the surface has infinite effective mass and does not move, so Newton's law gives with the direction reversed. Momentum is not conserved (the wall provides an impulse). Example: a ball at m s⁻¹ rebounds at m s⁻¹, so . Hitting a second wall of the same material, it rebounds at m s⁻¹. After impacts the speed is times the original.
Applying conservation of momentum to the ball alone. Momentum is not conserved when the wall exerts an impulse.
Section 4
Kinetic energy and restitution
Kinetic energy lost in a collision KE before KE after. For a fixed surface, KE after KE before, so the fraction lost is . For the fraction lost is . For two particles, calculate KE before and after using the actual speeds. In the example above the KE before is and after is , so is lost. If , KE is conserved. Kinetic energy never increases in a collision, which is why .
For a wall impact, the KE after is times the KE before, so you can find the fraction lost without knowing the mass.
Section 5
Successive collisions
In problems with three or more bodies, work through the collisions in order, using the speeds from the first collision as the starting speeds for the next. A further collision between two bodies occurs only if the one behind is moving faster than the one in front, or if they are moving towards each other (for example after rebounding from a wall). Example: spheres of equal mass then then in a line. After hits at speed , and . After hits , and . catches again if , which is true for .
Compare velocities after each collision. If the body behind is faster, or they approach, there is a further collision.
That's the notes covered.
Carry on to the next subtopic.
Exam questions on Coefficient of restitution and collisions
- A ball is moving at m s⁻¹ directly towards a fixed smooth vertical wall. It hits the wall and rebounds directly with speed m s⁻¹.After rebounding, the ball hits a second fixed smooth wall, parallel to the first and made of the same material, directly. Find the speed of the ball after it rebounds from the second wall.2 marks
- Two smooth spheres and , each of mass , move in the same direction along a straight line on a smooth horizontal surface. is moving at m s⁻¹ and is ahead of it, moving at m s⁻¹. The spheres collide directly. The coefficient of restitution between them is .Find, in terms of , the kinetic energy lost in the collision.2 marks
- A particle of mass , moving at , collides directly with a particle of mass moving at in the opposite direction on a smooth horizontal surface. The coefficient of restitution between and is .Find the speeds of and after the collision.3 marks
Written by the Exaim team, led by Shaun Daswani (Head of Upper Secondary, Improve ME Institute; MSc Financial Mathematics, Imperial College London; BSc, UCL) and Jason Daswani (operational lead, Improve ME Institute; LSE).