A.2.16—Linear momentum conservation
- Syllabus
- First assessment 2025
- Objective
- —
- Level
- SL
Momentum
Linear momentum is
p=mv
It is a vector. For an isolated system, total momentum is conserved before and after an interaction.
Check the system
Momentum is conserved when the resultant external impulse on the chosen system is negligible. Internal forces can change individual momenta while leaving the vector total unchanged.
Use signs or components
Choose a positive direction and conserve momentum component-by-component. A negative final velocity means motion opposite to the chosen positive direction.
Common trap
Do not conserve kinetic energy automatically. Momentum conservation and kinetic-energy conservation are separate claims.
[ 1 ]
Cart X , of mass 2 kg , is moving at a speed of 3 m s−1 to the right and collides on a horizontal track with cart Y of mass 1 kg.Y is initially stationary.
The velocity of Y immediately after the collision is 4 m s−1 to the right. What is the velocity of X immediately after the collision?
Build the force model
Choose the system, draw a labelled free-body diagram, classify the interactions and resolve components. Apply Newton’s laws with the correct boundary: contact forces, field forces, friction, tension, buoyancy and restoring forces each have their own direction and conditions.
Track momentum
Use ec p=mec v, ec J=\Deltaec p and momentum conservation only after checking external impulse. Distinguish elastic and inelastic collisions, explosions and energy transfer.
Track circular motion
The inward resultant provides ac=v2/r=ω2r. It may come from tension, gravity, normal, friction or a field force. Angular and linear descriptions are linked by v=ωr=2πr/T.
Final checks
Ask: Which body is the system? Which forces are external? Is mass constant? Is acceleration uniform or radial? Is kinetic energy conserved, transferred or increased?