Theory — Momentum and Its Conservation
Linear Momentum
Momentum is the product of an object's mass and its velocity. It is a vector — its sign carries the direction of motion. A heavy, fast object has a large momentum and is hard to stop; a light or slow one has little. Momentum, not speed, measures "how much motion" an object carries.
Units: kilogram-metres per second (kg·m/s)
Sign convention: rightward positive, leftward negative
Conservation of Momentum
When two objects interact and no outside (external) force acts on the pair, the total momentum of the system is unchanged by the interaction. During a collision the two objects push on each other with equal and opposite forces (Newton's third law), so whatever momentum one gains, the other loses. The total before equals the total after.
(u = velocity before, v = velocity after)
Elastic vs Inelastic Collisions
Collisions differ in what happens to the kinetic energy. In an elastic collision the objects bounce apart and the total kinetic energy is conserved. In an inelastic collision some kinetic energy is converted into heat, sound, or deformation, so the total kinetic energy decreases. In a perfectly inelastic collision the objects stick together and move as one — the maximum kinetic energy is lost (though momentum is still conserved).
Elastic: ΣKE_before = ΣKE_after
Inelastic: ΣKE_after < ΣKE_before (energy lost to heat/sound)
Perfectly inelastic: objects stick → v = (m₁u₁ + m₂u₂)/(m₁+m₂)
Elastic collision
Objects bounce apart. Momentum conserved AND kinetic energy conserved. Idealized — like hard spheres or air-track gliders with bumpers.
Inelastic collision
Objects may stick or deform. Momentum conserved, but kinetic energy decreases (lost to heat, sound, deformation). Perfectly inelastic = stick together.
| Quantity | Elastic | Inelastic | Perfectly inelastic |
|---|---|---|---|
| Total momentum | conserved | conserved | conserved |
| Total kinetic energy | conserved | decreases | decreases (maximum loss) |
| After collision | bounce apart | bounce / partly stick | move together as one |
Instructions — Running the Virtual Experiment
The Collision Lab tab lets you set up and watch collisions; the Data Table tab logs the before-and-after momentum and energy. Record every reading in your lab notebook.
Simulation — Two-Ball Collisions
Setup
Trial setup
| Type | p before | p after | KE before | KE after |
|---|---|---|---|---|
| No trials yet — set up a collision and click "Run & record". | ||||
Team Questions
Example Lab Report
Sample report demonstrating the expected format and level of detail. Use as a guide for your own submission.
Collisions and Momentum: Conservation of Momentum and Kinetic Energy
Physics | Section: [Your Section] | Date: [Date]
Lab Members: [Names of all members present]
Purpose
To investigate one-dimensional collisions between two balls and to verify that total linear momentum is conserved in every collision, while total kinetic energy is conserved only in elastic collisions. The lab compares elastic and perfectly inelastic collisions for a range of masses and velocities.
Theory
When no external force acts on a two-body system, the total momentum before a collision equals the total momentum after. Kinetic energy, however, is conserved only when the collision is elastic; in inelastic collisions some kinetic energy is converted to heat, sound, and deformation.
m₁u₁ + m₂u₂ = m₁v₁ + m₂v₂ (always)
Perfectly inelastic: v = (m₁u₁ + m₂u₂)/(m₁ + m₂)
For the elastic case the two final velocities are found from conservation of both momentum and kinetic energy; for the perfectly inelastic case the two balls share one final velocity.
Calculations — Sample: m₁ = 2 kg at u₁ = +3 m/s, m₂ = 1 kg at rest
Momentum before: p = (2)(3) + (1)(0) = 6 kg·m/s
KE before: KE = ½(2)(3²) + 0 = 9 J
Elastic after: v₁ = [(m₁−m₂)u₁]/(m₁+m₂) = (1·3)/3 = 1 m/s; v₂ = (2m₁u₁)/(m₁+m₂) = (12)/3 = 4 m/s. Check: p = (2)(1)+(1)(4) = 6 kg·m/s ✓; KE = ½(2)(1²)+½(1)(4²) = 1 + 8 = 9 J ✓
Perfectly inelastic after: v = 6/(2+1) = 2 m/s. Check: p = (3)(2) = 6 kg·m/s ✓; KE = ½(3)(2²) = 6 J (3 J lost to heat/sound)
Results Table — Collision Trials
| Type | p before (kg·m/s) | p after (kg·m/s) | KE before (J) | KE after (J) |
|---|---|---|---|---|
| Elastic | 6.0 | 6.0 | 9.0 | 9.0 |
| Inelastic (stick) | 6.0 | 6.0 | 9.0 | 6.0 |
| Elastic (equal mass) | 4.0 | 4.0 | 8.0 | 8.0 |
In the equal-mass elastic head-on trial the moving ball stopped and transferred all its velocity to the struck ball, as predicted for equal masses.
Discussion
In every trial the total momentum after the collision equaled the total momentum before, confirming conservation of momentum regardless of collision type. The kinetic energy behaved differently: in the elastic trials the total kinetic energy after matched the value before (9.0 J before and after), but in the perfectly inelastic trial the kinetic energy dropped from 9.0 J to 6.0 J. The missing 3.0 J was converted to heat, sound, and permanent deformation when the balls stuck together.
The equal-mass elastic collision produced the familiar result that the incoming ball stops while the target ball moves off with the incoming ball's original velocity — a complete exchange of velocity that conserves both momentum and kinetic energy. These results confirm that momentum conservation is universal, while kinetic-energy conservation is the special signature of an elastic collision.
Conclusion
The experiment verified that total linear momentum is conserved in all collisions, elastic and inelastic alike, and that total kinetic energy is conserved only in elastic collisions. Perfectly inelastic collisions conserve momentum but lose the most kinetic energy, consistent with the conversion of mechanical energy into other forms.
Practice Questions
Show all work and include units in your answers.