Unit 5 · Topic 04
Collisions in one and two dimensions
In an isolated system, every collision conserves total momentum. Total kinetic energy is conserved only in elastic collisions.
Unit 5CollisionsOpen navigation
Concept 01
What is conserved
Essential The minimum you should retain
An elastic collision conserves P and K; an inelastic collision conserves P but not K.
UnderstandInterpret and connect
In a perfectly inelastic collision the bodies stick and share one final velocity.
DeepenFormulation and conditions
Lost K becomes deformation, sound, or internal energy; momentum is not lost.
ExploreConnections for further study
Classifying the collision determines which additional equations are available.
Every isolated case conserves P; only elastic conserves K and perfectly inelastic shares v_f.
Concept 02
One final velocity
Essential The minimum you should retain
When bodies stick, their combined mass moves with v_f=(m_1v_1i+m_2v_2i)/(m_1+m_2).
UnderstandInterpret and connect
Velocity signs are essential when adding initial momentum.
DeepenFormulation and conditions
The balance conserves P, while comparing K_i and K_f generally shows a decrease.
ExploreConnections for further study
This is the limiting case of maximum kinetic-energy loss compatible with the given momentum.
Worked example
Two cars stick together
A 1200 kg car moves at +12 m/s and an 800 kg car at -5.0 m/s.
- m_1=1200 kg
- v_1=+12 m/s
- m_2=800 kg
- v_2=-5.0 m/s
Calculate shared final velocity.
- Initial momentum
P_i=1200(12)+800(-5)=10400 kg·m/s.
- Final mass
m_1+m_2=2000 kg.
- Calculation
v_f=10400/2000=5.20 m/s.
- Interpretation
Positive sign is the first car's direction.
Mathematical relation
Perfectly inelastic collision
Shared velocity after the bodies stick.
Momentum is conserved, kinetic energy generally is not.
DeepenVariables, conditions, and checks
Variables
- v_f
- shared final velocity; usual unit: m/s
Conditions of application
- Isolated 1D collision; bodies stick.
Dimensional check
m/s.
Concept 03
Two laws, two unknowns
Essential The minimum you should retain
A one-dimensional elastic collision conserves momentum and kinetic energy.
UnderstandInterpret and connect
With sufficient initial data, both laws determine the two final velocities.
DeepenFormulation and conditions
The formulas for a target initially at rest depend on the mass ratio.
ExploreConnections for further study
Velocity exchange occurs only for equal masses in this special case.
Worked example
Head-on elastic collision
m_1=2.0 kg at +6.0 m/s hits m_2=4.0 kg at rest.
- m_1=2.0 kg
- v_1i=+6.0 m/s
- m_2=4.0 kg
- v_2i=0
Find both final velocities.
- Model
Use elastic 1D formulas for a target at rest.
- First mass
v_1f=((2-4)/(2+4))6=-2.0 m/s.
- Second mass
v_2f=(2·2/(2+4))6=4.0 m/s.
- Check
P_i=P_f=12 kg·m/s and K_i=K_f=36 J.
Mathematical relation
Elastic collision in 1D
The two conservation laws for an elastic collision.
Both equations determine final velocities.
DeepenVariables, conditions, and checks
Variables
- P
- total momentum; usual unit: kg·m/s
- K
- total kinetic energy; usual unit: J
Conditions of application
- Isolated elastic one-dimensional collision.
Dimensional check
Each equality preserves its units.
Concept 04
Conserve components
Essential The minimum you should retain
In two dimensions, P_x and P_y are separately conserved when external impulse is negligible.
UnderstandInterpret and connect
Conserving only the magnitude |P| is not enough.
DeepenFormulation and conditions
Final vectors must close the same vector polygon as initial momentum.
ExploreConnections for further study
Momentum gives two equations; angles, elasticity, or other data may be needed to close the problem.
The initial vector is the sum of the two final vectors; the polygon closes in x and y.
Concept review
Common errors
Each warning includes a concrete way to review the reasoning, not only an incorrect-answer marker.
Conserving K in every collision.
K is conserved only in elastic collisions; P may also be conserved in inelastic ones.
Saying an inelastic collision loses momentum.
An isolated system conserves P while part of K changes form.
Conserving only |P| in two dimensions.
Conserve P_x and P_y separately.
Applying velocity exchange to every collision.
It is a special elastic 1D equal-mass case.