Conservation of Linear Momentum (CoM): For any direct collision between two spheres of masses and , the principle states that . This principle remains valid for every individual stage of a multiple collision problem, provided no external forces act on the system.
Newton's Experimental Law (Restitution): The relationship between relative speeds is defined by the coefficient of restitution , where . This law is applied independently to each impact to relate the velocities before and after the collision.
Impulse-Momentum Relationship: When a particle hits a wall, the change in momentum is caused by the impulse from the wall. The wall is treated as having infinite mass, meaning the particle's speed after impact is simply in the opposite direction.
| Feature | Particle-Particle Collision | Particle-Wall Collision |
|---|---|---|
| Momentum | Conserved between the two particles | Not conserved (wall is fixed) |
| Velocity Change | Both particles change velocity | Only the particle changes direction |
| Equation Used | ||
| Separation Speed | Difference between both final velocities | Final speed of the particle only |
Diagramming Each Stage: Draw separate 'Before' and 'After' diagrams for every single collision. Labeling velocities clearly with subscripts (e.g., for A after the first hit) prevents confusing values between different stages of the problem.
Consistent Sign Convention: Choose one direction (usually left-to-right) as positive and stick to it throughout all calculations. A negative result for a velocity indicates a change in direction, which is vital when checking if a second collision is possible.
Feasibility Checks: Always compare final velocities at the end of the problem. If a question asks 'Will there be another collision?', you must show an inequality, such as , to justify your conclusion mathematically.
Sanity Check: In a smooth system with , the total kinetic energy must decrease or stay constant. If your calculated velocities show an increase in energy, there is likely a sign error in your restitution equation.