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Direct impact and Newton's law of restitutionEdexcel International A Level Further Maths: Revision notes

Section 1

Direct impact and conservation of momentum

A direct impact is a collision between two particles (or smooth spheres) whose velocities before and after the collision lie along the line of centres, so everything happens in one dimension. Draw a diagram showing the velocities before and after, choose one direction as positive and write every velocity as a signed value. During the impact the only horizontal forces are the equal and opposite impulses between the particles, so total momentum is conserved whatever the value of ee: m1u1+m2u2=m1v1+m2v2.m_1u_1+m_2u_2=m_1v_1+m_2v_2. Conservation of momentum alone gives one equation in two unknowns v1,v2v_1,v_2, so a second equation is always needed.

Key termsdirect impactline of centresconservation of momentum
Common mistake

Forgetting signs: a particle moving in the negative direction has a negative velocity. Fix the positive direction on the diagram first.

Section 2

Newton's law of restitution

Newton's law of restitution gives the second equation. For a direct impact between two particles: speed of separation=e×speed of approach,i.e. v2−v1=e (u1−u2),\text{speed of separation}=e\times\text{speed of approach},\qquad\text{i.e. }v_2-v_1=e\,(u_1-u_2), where particle 2 is the one ahead in the positive direction. The coefficient of restitution ee depends only on the materials of the two particles. Check the sign: after the impact, particle 1 cannot be ahead of particle 2, so v2−v1≥0v_2-v_1\ge0. Solving the momentum and restitution equations simultaneously gives v1v_1 and v2v_2. A quick check: substitute both answers back into both equations.

Key termsNewton's law of restitutioncoefficient of restitutionspeed of approachspeed of separation
Exam tip

Write restitution as (velocity of the front particle after) −- (velocity of the back particle after) =e×=e\times (their relative speed before). Then it is always positive.

Section 3

The inequalities 0≤e≤10\le e\le1

The coefficient of restitution satisfies 0≤e≤10\le e\le1.

  • e=1e=1: perfectly elastic. Speed of separation equals speed of approach and no kinetic energy is lost.
  • e=0e=0: inelastic. The particles do not separate; they move together with a common velocity (they coalesce).
  • 0<e<10<e<1: partially elastic. Kinetic energy is lost. A value of ee above 11 would mean kinetic energy is gained in a collision, which cannot happen, so a calculated e>1e>1 shows an error. If a quadratic such as e2=14e^2=\frac14 appears, reject the negative root and take e=12e=\frac12. Imposing 0≤e≤10\le e\le1 on a result such as vB=23+15e4v_B=\frac{23+15e}{4} gives the range of possible final speeds.
Key termsperfectly elasticinelasticcoalesce
Common mistake

Accepting a negative or greater-than-1 value of ee. Always check 0≤e≤10\le e\le1 and reject values outside it.

Section 4

Loss of mechanical energy

Momentum is always conserved, but kinetic energy is lost whenever e<1e<1 (sound, heat and deformation). On a smooth horizontal surface there is no change in potential energy, so the loss of mechanical energy is ΔE=(12m1u12+12m2u22)−(12m1v12+12m2v22).\Delta E=\left(\tfrac12m_1u_1^2+\tfrac12m_2u_2^2\right)-\left(\tfrac12m_1v_1^2+\tfrac12m_2v_2^2\right). Calculate the kinetic energy of each particle before and after, then subtract; the answer must be positive (or zero if e=1e=1). A negative answer means a calculation error. The impulse on a particle is its change of momentum. In the worked example below, the impulse on BB is 3(3)−3(0)=93(3)-3(0)=9 N s.

Key termskinetic energyimpulseloss of mechanical energy
Common mistake

Leaving out the 12\frac12 in the kinetic energy, or squaring the sum of velocities instead of squaring each velocity separately.

Section 5

Worked example

AA (22 kg, 55 m s−1^{-1}) hits BB (33 kg, at rest) with e=0.5e=0.5. Momentum: 10=2vA+3vB10=2v_A+3v_B. Restitution: vB−vA=0.5(5)=2.5v_B-v_A=0.5(5)=2.5. Substituting vA=vB−2.5v_A=v_B-2.5: 10=5vB−510=5v_B-5, so vB=3v_B=3 and vA=0.5v_A=0.5 m s−1^{-1}, both in the original direction. Kinetic energy before =25=25 J, after =0.25+13.5=13.75=0.25+13.5=13.75 J, so 11.2511.25 J is lost. Method: (1) diagram with a positive direction; (2) momentum equation; (3) restitution equation; (4) solve; (5) check vB≥vAv_B\ge v_A and that the energy loss is positive.

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Exam questions on Direct impact and Newton's law of restitution

  1. Particle AA of mass 22 kg moves with speed 55 m s−1^{-1} along a straight line on a smooth horizontal surface and collides directly with particle BB of mass 33 kg, which is at rest. The coefficient of restitution between the particles is 0.50.5.
    Find the magnitude of the impulse exerted by AA on BB in the collision.2 marks
  2. Particles PP and QQ, of mass 33 kg and 55 kg, move towards each other along the same straight line on a smooth horizontal surface with speeds 44 m s−1^{-1} and 22 m s−1^{-1} respectively. They collide directly. After the collision the direction of motion of PP is reversed and its speed is 11 m s−1^{-1}.
    Find the total kinetic energy lost in the collision.2 marks
  3. Two smooth spheres AA and BB of equal radii and masses mm and 3m3m lie on a smooth horizontal table. Sphere AA is projected with speed uu directly towards BB, which is at rest. The coefficient of restitution between the spheres is ee.
    Show that the speed of BB immediately after the collision is (1+e)u4\frac{(1+e)u}{4}.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).