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Momentum in two dimensions and collisionsEdexcel International A Level Physics: Revision notes

Section 1

Conservation of momentum in two dimensions

Momentum is a vector, so in a collision the total momentum is conserved in every direction, provided there is no resultant external force. In two dimensions, resolve each momentum into two perpendicular components (for example xx and yy) and conserve each separately:

∑px (before)=∑px (after)\sum p_x \text{ (before)} = \sum p_x \text{ (after)} and ∑py (before)=∑py (after)\sum p_y \text{ (before)} = \sum p_y \text{ (after)}

For a mass mm moving at speed vv at angle θ\theta to the xx axis, px=mvcos⁡θp_x = mv\cos\theta and py=mvsin⁡θp_y = mv\sin\theta.

Key termsconservation of momentum
Exam tip

Choose axes along the initial motion of one object. If a body starts at rest, its initial perpendicular momentum is zero, which simplifies the equations.

Section 2

Elastic and inelastic collisions

In an elastic collision the total kinetic energy is the same before and after. In an inelastic collision some kinetic energy is transferred to thermal energy, sound or deformation, so total kinetic energy decreases.

Momentum is conserved in both types, so to decide, calculate the total kinetic energy before and after and compare. Kinetic energy is a scalar, so add the values for each object. Never resolve kinetic energy into components.

Key termselastic collisioninelastic collision
Common mistake

Do not say momentum is lost in an inelastic collision. Momentum is conserved; it is kinetic energy that is not.

Section 3

Kinetic energy and momentum

For a non-relativistic particle Ek=12mv2E_k = \tfrac12 mv^2 and p=mvp = mv, so v=p/mv = p/m. Substituting:

Ek=12m(pm)2=p22mE_k = \tfrac12 m\left(\dfrac{p}{m}\right)^2 = \dfrac{p^2}{2m}

This is useful when momentum is known but not speed, and it shows that for the same momentum the lighter object has more kinetic energy.

Section 4

Worked example

A 0.16 kg puck moving at 5.0 m s⁻¹ hits an identical stationary puck. The first moves off at 3.0 m s⁻¹ at 53° to its original direction.

  • Perpendicular: second puck has 3.0sin⁡53∘=2.43.0\sin 53^\circ = 2.4 m s⁻¹ in the opposite sense
  • Along line: 5.0−3.0cos⁡53∘=3.25.0 - 3.0\cos 53^\circ = 3.2 m s⁻¹
  • Speed =3.22+2.42=4.0= \sqrt{3.2^2 + 2.4^2} = 4.0 m s⁻¹
  • EkE_k before =2.0= 2.0 J; after =12(0.16)(3.02+4.02)=2.0= \tfrac12(0.16)(3.0^2 + 4.0^2) = 2.0 J, so the collision is elastic.

Section 5

Core Practical 10: collisions of small spheres

Roll one ball bearing into a stationary one on a smooth table top and film from above with a scale in view. ICT analysis (video analysis software or a strobe-style stills sequence) gives positions at equal time intervals, so speeds and angles can be found before and after the collision.

  1. Calculate the velocities of both spheres before and after.
  2. Resolve into components and check that total momentum is conserved.
  3. Calculate EkE_k before and after to decide whether the collision is elastic.

Sources of error include friction, spin and measurement uncertainty in the angles.

Key termsvideo analysis

Must Know

  • Momentum is conserved in each direction; resolve into perpendicular components
  • Elastic: kinetic energy conserved; inelastic: kinetic energy decreases
  • Momentum is conserved in both types of collision
  • Ek=p2/2mE_k = p^2/2m
  • Compare total kinetic energy before and after to decide

That's the notes covered.

Carry on to the next subtopic.

Exam questions on Momentum in two dimensions and collisions

  1. On a frictionless air table a puck of mass 0.16 kg moving at 5.0 m s⁻¹ collides with an identical stationary puck. After the collision the first puck moves at 3.0 m s⁻¹ at 53° to its original direction of motion, and the second puck moves off on the other side of the original line of motion.
    Determine whether the collision is elastic.2 marks
  2. A spring-loaded plunger gives each of two trolleys, X of mass 0.50 kg and Y of mass 2.0 kg, a momentum of 3.0 kg m s⁻¹ along a frictionless track.
    Derive an expression for the kinetic energy of a non-relativistic particle in terms of its momentum p and mass m, and use it to calculate the kinetic energy of trolley Y.2 marks
  3. In Core Practical 10 a student films a ball bearing of mass 0.028 kg moving at 0.60 m s⁻¹ across a smooth table top as it collides with an identical stationary ball bearing, and uses video analysis software to measure the motion. After the collision the first ball bearing moves at 0.30 m s⁻¹ at 40° to its original direction, and the second moves off on the other side of the original line of motion.
    Calculate the speed and direction of motion of the second ball bearing 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).