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How do momentum and impulse describe collisions, and what does the coefficient of restitution add?

Linear momentum and impulse, conservation of momentum in collisions, Newton's experimental law with the coefficient of restitution, and kinetic energy lost in impacts.

A CCEA A2 Further Maths Mechanics answer on linear momentum and impulse, conservation of momentum in collisions, Newton's experimental law with the coefficient of restitution, and the kinetic energy lost in an impact.

Generated by Claude Opus 4.813 min answer

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  1. What this dot point is asking
  2. The answer
  3. Examples in context
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What this dot point is asking

CCEA wants you to use linear momentum and impulse, apply the conservation of momentum to direct collisions, use Newton's experimental law with the coefficient of restitution ee, and find the kinetic energy lost in an impact.

The answer

Momentum and impulse

Conservation of momentum

Newton's experimental law (restitution)

Kinetic energy lost

Examples in context

Example 1. Crumple zones in cars. A crumple zone lengthens the time over which a crash brings the car to rest, and since impulse =Ft== Ft = change in momentum, a longer time means a smaller force on the occupants. The impulse-momentum principle is a safety-engineering tool.

Example 2. Newton's cradle. The clicking spheres approximate e=1e = 1 collisions, so both momentum and kinetic energy are very nearly conserved, which is why one ball out gives one ball out. Real cradles slowly stop because ee is just below 11 and a little energy is lost each impact.

Try this

Q1. Find the momentum of a 4kg4\,\text{kg} mass moving at 3m s13\,\text{m s}^{-1}. [1 mark]

  • Cue. p=mv=4×3=12kg m s1p = mv = 4 \times 3 = 12\,\text{kg m s}^{-1}.

Q2. What value of ee describes a perfectly elastic collision? [1 mark]

  • Cue. e=1e = 1.

Q3. Two equal masses coalesce; one was at 6m s16\,\text{m s}^{-1}, the other at rest. Find their common speed. [2 marks]

  • Cue. m(6)+m(0)=2mvm(6) + m(0) = 2mv, so v=3m s1v = 3\,\text{m s}^{-1}.

Exam-style practice questions

Practice questions written in the style of CCEA exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

CCEA A2 20207 marksA particle of mass 3kg3\,\text{kg} moving at 4m s14\,\text{m s}^{-1} collides directly with a particle of mass 2kg2\,\text{kg} moving in the opposite direction at 1m s11\,\text{m s}^{-1}. They coalesce on impact. Find their common velocity after the collision.
Show worked answer →

Take the direction of the 3kg3\,\text{kg} particle as positive, so the 2kg2\,\text{kg} particle has velocity 1m s1-1\,\text{m s}^{-1}.

Conservation of momentum: total momentum before equals total momentum after. Let the common velocity be vv:

3(4)+2(1)=(3+2)v.3(4) + 2(-1) = (3 + 2)v.

122=5v10=5vv=2m s1.12 - 2 = 5v \Rightarrow 10 = 5v \Rightarrow v = 2\,\text{m s}^{-1}.

The combined mass moves at 2m s12\,\text{m s}^{-1} in the original direction of the 3kg3\,\text{kg} particle.

Markers reward the sign convention, the conservation-of-momentum equation, and the common velocity of 2m s12\,\text{m s}^{-1}.

CCEA A2 20188 marksA smooth sphere AA of mass 2kg2\,\text{kg} moving at 5m s15\,\text{m s}^{-1} collides directly with a stationary smooth sphere BB of mass 3kg3\,\text{kg}. The coefficient of restitution is 0.60.6. Find the velocities of AA and BB after the collision.
Show worked answer →

Let the velocities after be vAv_A and vBv_B (positive in the original direction of AA).

Conservation of momentum: 2(5)+3(0)=2vA+3vB2(5) + 3(0) = 2v_A + 3v_B, so 10=2vA+3vB10 = 2v_A + 3v_B.

Newton's experimental law: the speed of separation equals ee times the speed of approach. Approach speed =50=5= 5 - 0 = 5, so separation speed vBvA=0.6×5=3v_B - v_A = 0.6 \times 5 = 3.

From the second equation vB=vA+3v_B = v_A + 3. Substitute: 10=2vA+3(vA+3)=5vA+910 = 2v_A + 3(v_A + 3) = 5v_A + 9, so vA=0.2m s1v_A = 0.2\,\text{m s}^{-1} and vB=3.2m s1v_B = 3.2\,\text{m s}^{-1}.

Both are positive, so both move in the original direction. Markers reward the momentum equation, the restitution equation, and both final velocities.

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