1. Conservation Laws Summary
| Quantity | Elastic Collision | Inelastic Collision |
|---|---|---|
| Momentum | Conserved | Conserved |
| Kinetic Energy | Conserved | Not conserved |
| Total Energy | Conserved (always) | Conserved (always) |
| Coefficient of Restitution (e) | [e = 1] | [0 ≤ e < 1] |
2. Key Differences (Tabular Form)
| Property | Elastic Collision | Inelastic Collision |
|---|---|---|
| Definition | Both momentum & kinetic energy conserved | Only momentum conserved |
| Coefficient of Restitution | [e = 1] | [0 ≤ e < 1] |
| Kinetic Energy | Same before and after collision | Partly converted into heat, sound, deformation |
| Deformation | Temporary | Permanent |
| Example | Billiard balls, gas molecules | Car crash, clay balls, football hitting wall |
| Velocity Relation | [ v_2 – v_1 = u_1 – u_2 ] | [ v_2 – v_1 = e(u_1 – u_2) ] |
| Energy Loss | No loss | Partial loss |
| Nature | Ideal, rare in real life | Common in real situations |
| Post-Collision Behavior | Bodies bounce apart | Bodies may move together |
| Mathematical Indicator | [ e = 1 ] | [ e < 1 ] |
3. Examples
(a) Elastic Collisions
- Collision of two identical steel balls.
- Gas molecule collisions in a container.
- Atomic or subatomic particle scattering.
(b) Inelastic Collisions
- A ball of clay hitting a wall and sticking.
- Car crash deformation.
- Bullet embedding into a wooden block.
4. Energy Distribution
Let initial total kinetic energy = [ E_i ] and final = [ E_f ].
- In elastic collisions, [ E_i = E_f ].
- In inelastic collisions, [ E_i > E_f ], and the loss [ (E_i – E_f) ] goes into:
- Internal deformation
- Heat and sound energy
- Vibration of molecules
5. Real-World Applications
| Elastic Collisions | Inelastic Collisions |
|---|---|
| Study of gas molecules in kinetic theory | Design of crumple zones in vehicles |
| Rutherford scattering experiments | Ballistics and momentum transfer |
| Newton’s cradle toy | Sports impacts (e.g., cricket ball hitting bat) |
6. Conceptual Questions
1. Is momentum conserved in all types of collisions?
Yes, momentum is always conserved in all collisions, provided no external force acts on the system.
2. Why is kinetic energy not conserved in inelastic collisions?
Because some kinetic energy converts into heat, sound, or deformation energy.
3. Can an inelastic collision ever become elastic?
No, because energy loss is unavoidable once deformation occurs.
4. What does perfectly inelastic mean?
It means the colliding bodies stick together and move with a common velocity after collision.
5. In which type of collision is coefficient of restitution less than 1?
In inelastic collisions.
6. Can energy be created or destroyed during a collision?
No, total energy is conserved. Only its form changes.
7. Why are molecular collisions nearly elastic?
Because internal deformation is negligible at that microscopic scale.
8. What happens to velocity directions after a perfectly elastic collision?
The bodies exchange their velocities if their masses are equal.
9. Is sound energy in collisions part of kinetic energy?
No, it’s a form of vibrational energy — converted from lost kinetic energy.
10. Why are most real-world collisions inelastic?
Because perfect elasticity is impossible due to inevitable heat and deformation losses.
7. FAQs / Common Misconceptions
1. If kinetic energy is not conserved, does it mean momentum isn’t conserved?
No, momentum conservation is independent of energy conservation; it always holds true.
2. Can a ball bouncing on the floor be considered elastic?
Not perfectly — some energy is lost, so it’s partially elastic (e.g., e ≈ 0.8 for rubber).
3. Is the coefficient of restitution zero for all inelastic collisions?
No, it’s zero only for perfectly inelastic collisions; for others, [0 < e < 1].
4. Can an elastic collision occur in real life?
Almost never perfectly, but some collisions (like atomic or molecular) are nearly elastic.
5. Does “energy lost” in an inelastic collision disappear?
No, it transforms into heat, sound, or deformation — total energy remains constant.