State the principle of conservation of momentum.
Linear momentum, denoted by $\mathbf{p}$, is a vector quantity defined for a particle of mass $m$ moving with velocity $\mathbf{v}$:
$$\mathbf{p}=m\mathbf{v}$$The change in momentum of an object is equal to the impulse applied to it.
$$\Delta\mathbf{p} = \mathbf{J} = \int \mathbf{F}\,dt$$For a constant force $F$ acting over a time interval $\Delta t$:
$$\Delta\mathbf{p}=F\Delta t$$Statement: In an isolated system (i.e., a system on which no external net force acts), the total linear momentum remains constant.
$$\sum \mathbf{p}_{\text{initial}} = \sum \mathbf{p}_{\text{final}}$$This principle follows directly from Newton’s second and third laws and is valid for any interaction, whether the bodies collide or separate.
| Collision Type | Momentum | Kinetic Energy | Typical Example |
|---|---|---|---|
| Elastic | Conserved | Conserved | Billiard balls striking each other |
| Inelastic | Conserved | Not conserved (some lost as deformation, heat, sound) | Car crash where vehicles stick together |
| Perfectly Inelastic | Conserved | Maximum loss of kinetic energy | Two clay balls sticking together after impact |
Problem: A 2.0 kg cart moving at $3.0\ \text{m s}^{-1}$ collides head‑on with a 3.0 kg cart initially at rest. After the collision the two carts stick together. Find their common speed immediately after the collision.
Solution:
The combined system moves at $1.2\ \text{m s}^{-1}$ in the original direction of the 2.0 kg cart.