Definition and conservation of momentum
Conservation of momentum
Isolated system and internal forces
A system is said to be isolated (or pseudo-isolated) if the sum of the external forces acting on it is zero or negligible. Internal forces (between parts of the system, for example during a collision) have, by the principle of reciprocal actions, no effect on the total momentum: they cancel each other out in pairs.
Conservation theorem
If the resultant of the external forces is zero, then dP/dt = 0, so:
P_before = P_after = constant
This is the law of conservation of momentum, which holds for any isolated system, regardless of the type of internal interaction (collision, explosion, chemical reaction, etc.).
Example: recoil of a firearm
A rifle of mass M = 4 kg fires a bullet of mass m = 10 g at a velocity v = 400 m/s. Before the shot, P = 0. After the shot:
MV + mv = 0 -> V = -(mv)/M = -(0.01400)/4 = -1 m/s
The rifle recoils at 1 m/s in the opposite direction to the bullet.
Summary table
| Situation | Is P conserved? | Condition |
|---|---|---|
| Collision between two marbles on a frictionless table | Yes | Sum of external forces is zero (weight balanced by the normal reaction) |
| Free fall of two bodies colliding | No, vertically | Weight is a non-zero external force |
| Explosion of a shell in flight | Yes, as an approximation | Very large internal forces outweigh the weight during the very short duration of the explosion |
Classic pitfall
Conservation applies to the system as a whole, not to each part separately: the momentum of each sub-part may change over time; only the total sum remains constant.

