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Conservation of Momentum

Benjamin Crowell · Simple Nature · Ch. 2

Momentum p = mv is conserved in every isolated system. Impulse (force times time) changes momentum. Collisions split into elastic (KE conserved) and inelastic (KE lost to heat/deformation). The center of mass moves at constant velocity regardless.

Momentum

Momentum is mass times velocity: p = mv. It is a vector quantity. A truck moving slowly can have the same momentum as a bullet moving fast. The total momentum of an isolated system never changes.

Before m1 p1 m2 p2 After p_total p1 + p2 before = p1' + p2' after
Scheme

Impulse

Impulse J = F * dt equals the change in momentum. A large force over a short time (baseball bat) and a small force over a long time (airbag) can produce the same impulse. The airbag spreads the force over more time, reducing peak force on your body.

Scheme

Elastic and inelastic collisions

In an elastic collision, both momentum and kinetic energy are conserved. In a perfectly inelastic collision, the objects stick together: momentum is conserved but kinetic energy is lost to deformation and heat. Most real collisions fall between these extremes.

Scheme

Center of mass

The center of mass of a system moves at constant velocity when no external forces act. Individual pieces can bounce, spin, and fragment, but the center of mass glides on serenely. This is why conservation of momentum is really about the center of mass.

Scheme
Neighbors
Ready for the real thing? Read Crowell's chapter.