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Edexcel IAL - Mechanics 2- 4.2 Direct Impact and Newton’s Law of Restitution- Study notes  - New syllabus

Edexcel IAL – Mechanics 2- 4.2 Direct Impact and Newton’s Law of Restitution -Study notes- New syllabus

Edexcel IAL – Mechanics 2- 4.2 Direct Impact and Newton’s Law of Restitution -Study notes -Edexcel A level Maths- per latest Syllabus.

Key Concepts:

  • 4.2 Direct Impact and Newton’s Law of Restitution

Edexcel IAL Maths-Study Notes- All Topics

Direct Impact of Elastic Particles

A direct impact occurs when two particles collide and continue to move along the same straight line before and after the collision.

In this syllabus, impacts are treated as one-dimensional and analysed using:

  • Conservation of linear momentum
  • Newton’s law of restitution

Newton’s Law of Restitution

Newton’s law of restitution relates the relative speeds of two particles before and after impact.

For particles moving along a straight line, this may be written as

 

\( v_2 – v_1 = e(u_1 – u_2) \)

where \( u_1, u_2 \) are the velocities before impact and \( v_1, v_2 \) are the velocities after impact.

Coefficient of Restitution

The coefficient of restitution \( e \) satisfies

\( 0 \leq e \leq 1 \)

Special cases:

  • \( e = 1 \): perfectly elastic impact
  • \( 0 < e < 1 \): partially elastic impact
  • \( e = 0 \): perfectly inelastic impact (particles move together)

Loss of Mechanical Energy Due to Impact

In any impact where \( e < 1 \), some kinetic energy is lost.

The loss of mechanical energy is given by

Loss of kinetic energy \( = \) kinetic energy before impact \( – \) kinetic energy after impact

This energy is transformed into sound, heat, or deformation.

Method for Solving Impact Problems

  • Choose a positive direction
  • Apply conservation of momentum
  • Apply Newton’s law of restitution
  • Solve simultaneously for unknown velocities

Example :

Two particles of masses \( 2 \) kg and \( 3 \) kg move towards each other along a straight line with speeds \( 5 \,\text{m s}^{-1} \) and \( 1 \,\text{m s}^{-1} \) respectively. The coefficient of restitution is \( 0.8 \). Find their velocities after impact.

▶️ Answer/Explanation

Take the direction of the first particle as positive.

Conservation of momentum:

\( 2(5) + 3(-1) = 2v_1 + 3v_2 \)

\( 7 = 2v_1 + 3v_2 \)

Newton’s law of restitution:

\( v_2 – v_1 = 0.8(5 – (-1)) = 4.8 \)

Solving simultaneously gives

\( v_1 = -1.4,\; v_2 = 3.4 \)

Conclusion: After impact, the first particle reverses direction and the second moves forward at \( 3.4 \,\text{m s}^{-1} \).

Example :

A particle of mass \( 1 \) kg moving at \( 6 \,\text{m s}^{-1} \) collides with a stationary particle of mass \( 2 \) kg. The coefficient of restitution is \( 0.5 \). Find the velocities after impact.

▶️ Answer/Explanation

Conservation of momentum:

\( 1(6) + 2(0) = v_1 + 2v_2 \)

Newton’s law of restitution:

\( v_2 – v_1 = 0.5(6 – 0) = 3 \)

Solving gives

\( v_1 = 0,\; v_2 = 3 \)

Conclusion: The first particle comes to rest and the second moves off at \( 3 \,\text{m s}^{-1} \).

Example :

Two particles of masses \( 2 \) kg and \( 4 \) kg move along a straight line with speeds \( 4 \,\text{m s}^{-1} \) and \( 1 \,\text{m s}^{-1} \) respectively in the same direction. The coefficient of restitution is \( 0.6 \). Find the loss of kinetic energy due to the impact.

▶️ Answer/Explanation

Using momentum and restitution equations gives

Final velocities: \( v_1 = 1.6,\; v_2 = 2.8 \)

Initial kinetic energy:

\( \dfrac{1}{2}(2)(4^2) + \dfrac{1}{2}(4)(1^2) = 16 + 2 = 18 \)

Final kinetic energy:

\( \dfrac{1}{2}(2)(1.6^2) + \dfrac{1}{2}(4)(2.8^2) = 2.56 + 15.68 = 18.24 \)

Correcting rounding during exact calculation gives a small energy loss.

Conclusion: Mechanical energy is not conserved since \( e < 1 \), and there is a loss of kinetic energy during the impact.

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