Introduction
Collisions are everywhere in nature and technology — from billiard balls striking each other, to car crashes, to particles colliding inside accelerators. Every time two bodies collide, forces act for a short interval, causing changes in motion.
Physics classifies collisions broadly into elastic and inelastic collisions. Both conserve momentum, but they differ in whether kinetic energy is conserved. Understanding these differences is crucial in mechanics, engineering, astrophysics, and even daily life safety.
This article explains in detail:
- What collisions are.
- Types of collisions.
- Elastic vs. inelastic collisions.
- Mathematical treatment.
- Real-life examples and applications.
Part 1: What is a Collision?
A collision occurs when two (or more) bodies exert forces on each other for a short time, leading to changes in their velocities.
- Collisions can be head-on (linear), oblique, or even multi-particle.
- The study of collisions uses Newton’s laws, momentum conservation, and energy principles.
Part 2: Laws Governing Collisions
- Law of Conservation of Linear Momentum
- In an isolated system (no external force), total momentum before collision = total momentum after collision.
- Law of Conservation of Energy
- Total energy is always conserved, but mechanical energy (kinetic + potential) may not always remain constant.
- Coefficient of Restitution (e)
- Measures “elasticity” of collision.
- e=1e = 1e=1 → Perfectly elastic collision.
- 0<e<10 < e < 10<e<1 → Inelastic collision.
- e=0e = 0e=0 → Perfectly inelastic collision (bodies stick together).
Part 3: Elastic Collisions
3.1 Definition
A collision is elastic if:
- Momentum is conserved.
- Kinetic energy is also conserved.
3.2 Characteristics
- No loss of kinetic energy (only redistributed).
- No permanent deformation or heat generation.
- Occurs mostly in atomic/molecular or idealized systems.
3.3 Mathematical Treatment (1D Elastic Collision)
Consider two bodies of masses m1,m2m_1, m_2m1,m2 with initial velocities u1,u2u_1, u_2u1,u2. After collision, velocities are v1,v2v_1, v_2v1,v2.
From momentum conservation: m1u1+m2u2=m1v1+m2v2m_1 u_1 + m_2 u_2 = m_1 v_1 + m_2 v_2m1u1+m2u2=m1v1+m2v2
From kinetic energy conservation: 12m1u12+12m2u22=12m1v12+12m2v22\frac{1}{2} m_1 u_1^2 + \frac{1}{2} m_2 u_2^2 = \frac{1}{2} m_1 v_1^2 + \frac{1}{2} m_2 v_2^221m1u12+21m2u22=21m1v12+21m2v22
Solving, we get: v1=(m1−m2)u1+2m2u2m1+m2v_1 = \frac{(m_1 – m_2)u_1 + 2m_2 u_2}{m_1 + m_2}v1=m1+m2(m1−m2)u1+2m2u2 v2=(m2−m1)u2+2m1u1m1+m2v_2 = \frac{(m_2 – m_1)u_2 + 2m_1 u_1}{m_1 + m_2}v2=m1+m2(m2−m1)u2+2m1u1
3.4 Examples of Elastic Collisions
- Collisions between gas molecules.
- Electron-electron scattering.
- Steel balls in Newton’s cradle (nearly elastic).
- Billiard balls (approximately elastic).
Part 4: Inelastic Collisions
4.1 Definition
A collision is inelastic if:
- Momentum is conserved.
- Kinetic energy is not conserved (some is lost to heat, sound, deformation).
4.2 Characteristics
- Part of kinetic energy converts into other forms.
- Objects may deform permanently.
- Most real-life collisions are inelastic.
4.3 Types of Inelastic Collisions
- Partially Inelastic Collision – Bodies do not stick but KE decreases.
- Perfectly Inelastic Collision – Bodies stick together and move with common velocity.
4.4 Mathematical Treatment (Perfectly Inelastic Collision)
If two masses m1,m2m_1, m_2m1,m2 with initial velocities u1,u2u_1, u_2u1,u2 collide and stick together with final velocity vvv: m1u1+m2u2=(m1+m2)vm_1 u_1 + m_2 u_2 = (m_1 + m_2)vm1u1+m2u2=(m1+m2)v v=m1u1+m2u2m1+m2v = \frac{m_1 u_1 + m_2 u_2}{m_1 + m_2}v=m1+m2m1u1+m2u2
Kinetic energy after collision: KEf=12(m1+m2)v2KE_f = \frac{1}{2}(m_1 + m_2)v^2KEf=21(m1+m2)v2
Since KEf<KEiKE_f < KE_iKEf<KEi, some energy is lost.
4.5 Examples of Inelastic Collisions
- Car crashes.
- Clay balls colliding and sticking together.
- Meteor hitting Earth.
- Sports: Kicking a football (deformation + heat).
Part 5: Differences Between Elastic & Inelastic Collisions
| Feature | Elastic Collision | Inelastic Collision |
|---|---|---|
| Momentum | Conserved | Conserved |
| Kinetic Energy | Conserved | Not conserved |
| Energy Transformation | No energy lost to heat, sound, deformation | KE partly converted to heat, sound, deformation |
| Coefficient of Restitution (e) | e=1e = 1e=1 | 0≤e<10 \leq e < 10≤e<1 |
| Nature | Ideal, microscopic, rare in daily life | Common in real-world scenarios |
| Examples | Gas molecules, Newton’s cradle, billiards | Car accidents, clay collisions, meteor strikes |
Part 6: Numerical Examples
Example 1: Elastic Collision
A 2 kg ball moving at 4 m/s collides elastically with a 3 kg ball at rest. Find their velocities after collision.
Solution: u1=4, u2=0, m1=2, m2=3u_1 = 4, \; u_2 = 0, \; m_1 = 2, \; m_2 = 3u1=4,u2=0,m1=2,m2=3 v1=(2−3)4+2(3)(0)5=−45=−0.8 m/sv_1 = \frac{(2-3)4 + 2(3)(0)}{5} = \frac{-4}{5} = -0.8 \, m/sv1=5(2−3)4+2(3)(0)=5−4=−0.8m/s v2=(3−2)(0)+2(2)(4)5=165=3.2 m/sv_2 = \frac{(3-2)(0) + 2(2)(4)}{5} = \frac{16}{5} = 3.2 \, m/sv2=5(3−2)(0)+2(2)(4)=516=3.2m/s
👉 Ball 1 rebounds at –0.8 m/s, Ball 2 moves at 3.2 m/s.
Example 2: Perfectly Inelastic Collision
Two bodies of 5 kg and 3 kg move towards each other with velocities 6 m/s and –4 m/s. Find their common velocity after sticking. v=(5)(6)+(3)(−4)5+3=30−128=188=2.25 m/sv = \frac{(5)(6) + (3)(-4)}{5+3} = \frac{30 – 12}{8} = \frac{18}{8} = 2.25 \, m/sv=5+3(5)(6)+(3)(−4)=830−12=818=2.25m/s
👉 Final velocity = 2.25 m/s in the direction of the heavier body.
Part 7: Applications of Collision Theory
- Engineering Safety
- Car crash testing uses inelastic collision principles to design crumple zones that absorb energy.
- Sports Science
- Elasticity of balls (tennis, basketball) determines bounce behavior.
- Astronomy
- Meteor impacts are modeled as inelastic collisions.
- Elastic scattering studied in nuclear/particle physics.
- Everyday Life
- Playing billiards or pool.
- Throwing clay or mud.
- Sound generation when objects strike.
Part 8: Graphical Understanding
- Elastic Collision Graph: KE before = KE after.
- Inelastic Collision Graph: KE decreases after collision, though total energy remains constant.
Graphs of relative velocity vs. time also highlight the coefficient of restitution.
Part 9: Key Takeaways
- All collisions conserve momentum (isolated system).
- Elastic collisions also conserve kinetic energy.
- Inelastic collisions lose some KE to heat, sound, or deformation.
- Perfectly inelastic collisions involve objects sticking together.
- Coefficient of restitution defines the elasticity of collision.
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