Mechanics of particles and systems Foundations of particle mechanics Theorem
Conservation of momentum
Builds on Newton's laws of motionMomentum
Statement
Let point particles have masses and positions , and let their motion obey Newton's second law. Let be the force of particle on particle . Suppose that no external force acts, so that the net force on particle is . Suppose that these forces obey Newton's third law, for all . Then the total momentum is constant in .
Remarks
The proof: , and the terms cancel in pairs, since . As a consequence, the centre of mass , with , moves with constant velocity . Example: a gun of mass at rest fires a bullet of mass at velocity ; the gun recoils at velocity . If external forces act, the same computation gives , so changes; for instance a falling system gains downward momentum. Without the third law the conclusion fails: two particles with give .
Going deeper
For a student
Momentum conservation is the main tool for collisions, where the forces are unknown and brief but act in equal and opposite pairs. In Lagrangian mechanics it follows from invariance of the Lagrangian under translations, an instance of Noether's theorem. It also lets one pass to the centre-of-mass frame, which separates the motion of the system as a whole from its internal motion.
Reading path
To understand this page from the ground up, read these 24 pages in order. The foundations come first.
Show the path as a graph
- no evidence level
- Derivative concept
- Differential equation concept
- Euclidean space object
- Euclidean vector concept
- Function concept
- Interval concept
- Ordinary differential equation concept
- Velocity concept
- Ordinary differential equation definition
- Classical mechanics concept
- Lipschitz condition definition
- Momentum concept
- Inertial frame of reference concept
- Solution of an ordinary differential equation definition
- Newton's laws of motion statement
- Initial value problem definition
- Picard–Lindelöf hypotheses definition
- Picard operator definition
- An iterate of the Picard operator is a contraction statement
- Integral equation form of an initial value problem statement
- Picard–Lindelöf theorem statement
- Classical mechanics definition
- Momentum definition
- Conservation of momentum statement
Where this leads
2 pages build on this one.
Further reading
About this page
| Tag | T1SHG5MD9R |
|---|---|
| URI | m2://T1SHG5MD9R |
| Kind | statement, theorem |
| Writing | W0 stub |
| MSC | 70A05, 70F10 |
| Status | This copy of the site has no build data. Run m2 status T1SHG5MD9R. |
| About | Momentum |
| Uses | Newton's laws of motion, Momentum |
| Changed | 3 November 2026 |
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