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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 speed of separation=e×speed of approach,\text{speed of separation}=e\times\text{speed of approach}, where ee is the coefficient of restitution, a dimensionless constant that depends on the materials. With velocities uA,uBu_A,u_B before and vA,vBv_A,v_B after, along the same positive direction: vB−vA=e(uA−uB)v_B-v_A=e(u_A-u_B). The values of ee satisfy 0≤e≤10\le e\le1. If e=1e=1 the collision is perfectly elastic (no kinetic energy lost). If e=0e=0 the bodies do not separate (they coalesce or move together). For 0<e<10<e<1 some kinetic energy is lost.

Key termscoefficient of restitutionperfectly elastic
Common mistake

Using the sum of the speeds as the speed of approach for particles moving in the same direction. Use velocities with signs: approach is uA−uBu_A-u_B.

Section 2

Direct collisions between two particles

To find two unknown velocities after a collision you need two equations:

  1. Conservation of momentum: m1u1+m2u2=m1v1+m2v2m_1u_1+m_2u_2=m_1v_1+m_2v_2.
  2. Newton's experimental law: v2−v1=e(u1−u2)v_2-v_1=e(u_1-u_2). Solve them simultaneously. Example: equal masses mm, AA at 55 m s⁻¹ chasing BB at 11 m s⁻¹, e=0.5e=0.5. Momentum: vA+vB=6v_A+v_B=6. Newton: vB−vA=0.5(5−1)=2v_B-v_A=0.5(5-1)=2. So vB=4v_B=4 and vA=2v_A=2 m s⁻¹. For equal masses and a target at rest, the results are vA=u(1−e)2v_A=\frac{u(1-e)}{2} and vB=u(1+e)2v_B=\frac{u(1+e)}{2}.
Key termsspeed of approachspeed of separation
Exam tip

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 speed after=e×speed before,\text{speed after}=e\times\text{speed before}, with the direction reversed. Momentum is not conserved (the wall provides an impulse). Example: a ball at 88 m s⁻¹ rebounds at 55 m s⁻¹, so e=58e=\frac58. Hitting a second wall of the same material, it rebounds at 58×5=3.125\frac58\times5=3.125 m s⁻¹. After nn impacts the speed is ene^n times the original.

Key termsfixed smooth surface
Common mistake

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 =e2×=e^2\times KE before, so the fraction lost is 1−e21-e^2. For e=58e=\frac58 the fraction lost is 1−2564=39641-\frac{25}{64}=\frac{39}{64}. For two particles, calculate KE before and after using the actual speeds. In the example above the KE before is 13m13m and after is 10m10m, so 3m3m is lost. If e=1e=1, KE is conserved. Kinetic energy never increases in a collision, which is why e≤1e\le1.

Key termskinetic energy lost
Exam tip

For a wall impact, the KE after is e2e^2 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 AA then BB then CC in a line. After AA hits BB at speed uu, vA=u(1−e)2v_A=\frac{u(1-e)}{2} and vB=u(1+e)2v_B=\frac{u(1+e)}{2}. After BB hits CC, vB′=u(1−e2)4v_B'=\frac{u(1-e^2)}{4} and vC=u(1+e)24v_C=\frac{u(1+e)^2}{4}. AA catches BB again if vA>vB′v_A>v_B', which is true for e<1e<1.

Key termsfurther collision
Exam tip

Compare velocities after each collision. If the body behind is faster, or they approach, there is a further collision.

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Exam questions on Coefficient of restitution and collisions

  1. A ball is moving at 88 m s⁻¹ directly towards a fixed smooth vertical wall. It hits the wall and rebounds directly with speed 55 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
  2. Two smooth spheres AA and BB, each of mass mm, move in the same direction along a straight line on a smooth horizontal surface. AA is moving at 55 m s⁻¹ and BB is ahead of it, moving at 11 m s⁻¹. The spheres collide directly. The coefficient of restitution between them is 0.50.5.
    Find, in terms of mm, the kinetic energy lost in the collision.2 marks
  3. A particle PP of mass 2m2m, moving at 4u4u, collides directly with a particle QQ of mass mm moving at uu in the opposite direction on a smooth horizontal surface. The coefficient of restitution between PP and QQ is 15\frac15.
    Find the speeds of PP and QQ after the collision.3 marks
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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).