Collision Momentum Calculator
Calculate velocities after elastic or inelastic collisions using conservation of momentum.
Momentum Conservation Governs Isolated Collisions
During a short collision, total momentum of an isolated system is conserved even though kinetic energy may or may not be conserved. In one dimension, m1u1+m2u2=m1v1+m2v2. Elastic collisions also conserve total kinetic energy, while perfectly inelastic collisions leave the objects moving together and lose the maximum kinetic energy consistent with momentum conservation.
Velocity signs are essential because momentum is a vector. In two or three dimensions, momentum conservation must be applied separately to each component. Kinetic energy that is not conserved in an inelastic collision becomes deformation, heat, sound, and internal energy.
| Symbol | Meaning | Why it appears / units |
|---|---|---|
| m | Mass | kg. |
| u | Initial velocity | m/s with sign for direction. |
| v | Final velocity | m/s with sign for direction. |
| p | Momentum | kg·m/s; vector quantity. |
Momentum conservation comes from negligible external impulse during the collision interval. It does not imply each object keeps its own momentum; objects exchange momentum through large internal forces.
Momentum conservation is a signed check. Compute m1v1+m2v2 before and after using the same positive direction. For a perfectly inelastic collision both objects share one final velocity, which must lie between the initial velocities when the masses are positive.
Worked Examples
Common Mistakes
Only elastic collisions conserve total kinetic energy. Momentum conservation is more general for isolated collision systems.
Opposite directions must carry opposite signs in one-dimensional momentum equations.
If a large external force acts over the collision interval, system momentum changes by that external impulse.
Frequently Asked Questions
Formula Explorer connections
Interpretation: This relationship connects motion, force, momentum, work or energy in a mechanical system. Assumption: Choose a consistent reference direction and unit system. The model may assume constant acceleration, rigid bodies, negligible losses or an isolated system.