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Reading Time: 6 min
Last Updated: March 19, 2026
Main Ideas: 4
Reading Time: 6 min
Last Updated: March 19, 2026
Main Ideas: 4

Topic 4.4 Notes – Elastic and Inelastic Collisions

Verified for 2027 AP® Physics C: Mechanics Exam
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Collisions are short interactions where objects exert large forces on each other for a brief time. In an isolated system, momentum is always conserved during a collision. The difference between elastic and inelastic collisions comes down to what happens to the system’s kinetic energy.

1. What Makes a Collision Elastic or Inelastic

A collision means objects interact strongly for a short time. If the system is isolated, the net external impulse is zero, so total momentum is conserved.

What changes from one type to another is the behavior of kinetic energy (KE).

Elastic Collisions

An elastic collision is one where the total kinetic energy of the system is the same before and after:

KEinitial=KEfinal KE_{\text{initial}} = KE_{\text{final}}

That does not mean each object keeps the same kinetic energy.

  • One object can lose KE while the other gains it.
  • The system total stays the same.
  • No lasting deformation, heat, or sound energy remains after the interaction.

Atomic and molecular collisions are often modeled as elastic. On AP problems, if they say “elastic,” you immediately know you can conserve both momentum and kinetic energy.

Here’s the big conceptual point students miss:
Even in elastic collisions, individual kinetic energies usually change. It’s the total that stays constant.

Inelastic Collisions

An inelastic collision is one where the total kinetic energy decreases:

KEfinal<KEinitial KE_{\text{final}} < KE_{\text{initial}}

Momentum is still conserved if the system is isolated.

Where did the “missing” kinetic energy go?

  • Thermal energy (microscopic motion)
  • Sound
  • Deformation (internal energy)

Total energy is still conserved. It’s just not all kinetic anymore.

On tests, if they don’t say “elastic,” assume kinetic energy is not conserved unless clearly stated.

Perfectly Inelastic Collisions

A perfectly inelastic collision is a special case:

  • The objects stick together
  • They move with the same final velocity
  • The maximum possible kinetic energy is lost (while still conserving momentum)

If two objects stick, you already know it’s perfectly inelastic. That single phrase tells you the entire setup.

For example, imagine m1m_{1} sliding toward a stationary m2m_{2} on a frictionless surface. After the collision, they stick and move together with a common velocity vfv_{f}.

Perfectly inelastic collision on a frictionless surface

2. The Two Governing Principles

Everything in collision problems comes from these two ideas.

Conservation of Momentum

For an isolated system:

m1v1i+m2v2i=m1v1f+m2v2f m_{1} v_{1i} + m_{2} v_{2i} = m_{1} v_{1f} + m_{2} v_{2f}

  • Always true (elastic or inelastic)
  • It’s a vector equation
  • In 1D, use signs carefully
  • In 2D, conserve x and y components separately

Momentum conservation comes from Newton’s Third Law. Internal forces cancel in pairs.

Conservation of Kinetic Energy (Elastic Only)

Only for elastic collisions:

12m1v1i2+12m2v2i2=12m1v1f2+12m2v2f2 \frac{1}{2}m_{1} v_{1i}^{2} + \frac{1}{2}m_{2} v_{2i}^{2} = \frac{1}{2}m_{1} v_{1f}^{2} + \frac{1}{2}m_{2} v_{2f}^{2}

This gives you a second equation to solve for unknown final velocities.

If you use this in an inelastic collision, your answer will be wrong even if your algebra is perfect.

Kinetic Energy Change

For inelastic cases:

KElost=KEinitial−KEfinal KE_{\text{lost}} = KE_{\text{initial}} - KE_{\text{final}}

You’re often asked to compute this after finding the final velocity from momentum.

3. Solving Collision Problems

The setup depends entirely on the collision type.

Elastic Collision in 1D

You need two equations:

  1. Momentum conservation
  2. Kinetic energy conservation

Example setup (no numbers, just structure):

  • Write m1v1i+m2v2i=m1v1f+m2v2fm_{1} v_{1i} + m_{2} v_{2i} = m_{1} v_{1f} + m_{2} v_{2f}
  • Write the KE equation
  • Solve simultaneously

Patterns worth remembering:

  • Equal masses, one initially at rest → velocities exchange.
  • A much lighter object tends to bounce back with large speed change.

These patterns show up in conceptual multiple-choice questions.

Perfectly Inelastic Collision

Objects share a final velocity vfv_{f}:

m1v1i+m2v2i=(m1+m2)vf m_{1} v_{1i} + m_{2} v_{2i} = (m_{1} + m_{2}) v_{f}

Steps:

  1. Solve for vfv_{f}
  2. Compute KE before
  3. Compute KE after
  4. Subtract to find energy lost

No kinetic energy conservation equation here. Ever.

General Inelastic (Not Sticking)

  • Momentum conserved
  • KE not conserved
  • Final velocities are usually given or partially known

Never assume they move together unless told explicitly.

4. Comparing Elastic and Inelastic Collisions

FeatureElasticInelasticPerfectly Inelastic
Momentum conservedYesYesYes
Kinetic energy conservedYesNoNo
Objects stick togetherNoNoYes
KE lost0SomeMaximum possible

One last conceptual insight:
Momentum conservation comes from symmetry and internal forces. Kinetic energy conservation depends on whether nonconservative processes occur during impact.

On FRQs, graders look for you to clearly state which conservation laws apply before writing equations. That single sentence can earn a point.

Key Takeaways

Momentum is conserved in all isolated collisions, regardless of type.
In elastic collisions, total kinetic energy is conserved, but individual object kinetic energies usually change.
In inelastic collisions, some kinetic energy becomes thermal, sound, or deformation energy.
If objects stick together, use m1v1i+m2v2i=(m1+m2)vfm_{1} v_{1i} + m_{2} v_{2i} = (m_{1}+m_{2})v_{f} and do not use kinetic energy conservation.
Equal-mass elastic collisions with one object initially at rest result in a velocity swap.

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