Linear Momentum
Defines momentum as p = mv, establishes it as a vector quantity, and introduces the collision and explosion models for analyzing interactions by comparing initial and final system states.
Unit 4 is about how objects exchange momentum during interactions. You learn to define momentum, calculate impulse as an integral of force over time, apply conservation of momentum to collisions and explosions, and classify collisions by what happens to kinetic energy.
Fiveable's AP Physics C: Mechanics Unit 4 review covers 4 topics, with guided practice questions for the unit.
Defines momentum as p = mv, establishes it as a vector quantity, and introduces the collision and explosion models for analyzing interactions by comparing initial and final system states.
Derives impulse as the integral of net force over time and connects it to change in momentum through the impulse-momentum theorem. Covers graphical interpretation of force-time and momentum-time graphs.
Establishes that total momentum is constant in isolated systems, introduces center-of-mass velocity, and applies conservation component-wise to 1D and 2D collisions and explosions.
Classifies collisions by kinetic energy behavior: elastic (KE conserved), inelastic (KE decreases), and perfectly inelastic (objects stick). Momentum is conserved in all cases.
Try AP-style questions on unit 4, then use the review notes below for anything you miss.
A timed, AP-style test built only from unit 4 questions — multiple choice plus free response, scored with AI feedback. Use the standard format or build your own.
Linear momentum is defined as p = mv. Because velocity is a vector, momentum has both magnitude and direction. For a system of objects, total momentum is the vector sum of individual momenta. Collisions and explosions are modeled by comparing the system's momentum just before and just after the interaction, treating each object as a point mass.
If a 2 kg object moves at 3 m/s east and a 1 kg object moves at 6 m/s west, what is the total momentum of the system?
| Interaction type | Internal forces | Objects after |
|---|---|---|
| Collision | Large, short-duration | Separate or stuck |
| Explosion | Internal forces push apart | Separate, moving in opposite directions |
The net external force on a system equals the rate of change of its momentum: F_net = dp/dt. Impulse J is the integral of net force over a time interval, J = integral from t1 to t2 of F_net(t) dt, and equals the change in momentum delta p. Impulse is a vector in the direction of the net force. Graphically, impulse is the area under a force-time curve, and net force is the slope of a momentum-time graph.
A force varies with time as shown on a graph. How would you find the impulse delivered between t = 0 and t = 4 s without a constant force?
| Graph type | Slope represents | Area represents |
|---|---|---|
| Force vs. time | Rate of change of force | Impulse (delta p) |
| Momentum vs. time | Net external force | Not directly used |
When the net external force on a system is zero, total momentum is conserved: the sum of initial momenta equals the sum of final momenta. Internal forces between objects cancel by Newton's third law, so they do not change total system momentum. The center-of-mass velocity is v_cm = (sum of m_i * v_i) / (sum of m_i), and it remains constant in the absence of a net external force. Conservation applies component-wise in 2D problems.
A 3 kg cart moving at 4 m/s east collides with a stationary 1 kg cart. If they stick together, what is the final velocity of the combined system?
| Condition | Is momentum conserved? | Reason |
|---|---|---|
| No net external force | Yes | Internal forces cancel by Newton's third law |
| Net external force present | No | External impulse changes total momentum |
| Explosion (internal forces only) | Yes | No net external force on the system |
Momentum is conserved in all collisions when the system is isolated. The collision type is determined by what happens to kinetic energy. In an elastic collision, total kinetic energy is the same before and after. In an inelastic collision, total kinetic energy decreases because nonconservative forces convert some kinetic energy into heat, sound, or deformation. In a perfectly inelastic collision, the objects stick together and share a common final velocity.
Two objects collide and stick together. Is kinetic energy conserved? How do you find the final velocity?
| Collision type | Momentum conserved? | KE conserved? | Objects after |
|---|---|---|---|
| Elastic | Yes | Yes | Separate |
| Inelastic | Yes | No (decreases) | Separate |
| Perfectly inelastic | Yes | No (maximum loss) | Stuck together |
| Term | Definition |
|---|---|
| collision | A model for an interaction between objects in which the internal forces are much larger than any net external force, so only initial and final states need to be analyzed. |
| explosion | A model for an interaction in which forces internal to a system push objects within that system apart; total system momentum is conserved. |
| impulse-momentum theorem | States that the impulse delivered to an object equals its change in momentum: J = integral of F_net dt = delta p. |
| perfectly inelastic collision | A collision in which the objects stick together and move with the same final velocity; kinetic energy loss is at its maximum for that momentum exchange. |
| area under the curve | On a force-time graph, the area under the curve equals the impulse delivered to the object during that time interval. |
| object model | A simplifying model that treats each object as a point mass, ignoring size and internal structure, which is valid for analyzing collisions. |
Miss rates come from Fiveable multiple-choice practice.
Momentum has direction. In 1D problems, assign positive and negative signs based on direction before calculating. In 2D, split into x- and y-components and conserve each separately.
Impulse is the integral of force over time, not force alone. A large force over a short time and a small force over a long time can deliver the same impulse. Always multiply or integrate with the time interval.
Kinetic energy is only conserved in elastic collisions. In any inelastic collision, including perfectly inelastic ones, total kinetic energy decreases. Momentum is always conserved in an isolated system regardless of collision type.
Conservation of momentum requires that the net external impulse on the system is zero. If gravity, friction, or another external force acts during the interaction and is not negligible, total momentum changes.
When objects stick together, they share one final velocity. Set up m1v1 + m2v2 = (m1 + m2)*v_f and solve for v_f. Do not use separate final velocities for each object.
AP Physics C: Mechanics problems frequently give a force as a function of time and ask you to integrate to find impulse, or present a force-time graph and ask for the area. Be ready to set up and evaluate definite integrals and to read graphical data accurately.
Free-response problems often require you to apply conservation of momentum to find a post-collision velocity, then use that result in a separate energy or kinematics calculation. Recognizing which conservation law applies at each stage is the central skill.
Exam questions ask you to explain in words why momentum is or is not conserved in a given scenario. A complete answer names the system, identifies whether a net external force acts, and references Newton's third law for internal force cancellation.
Open the individual guides for Unit 4 when you want a closer review of one topic.
Use AP-style practice after you review the notes so you can check what you understand.
Practice free-response reasoning and compare your answer with scoring guidance.
Watch past review streams filtered to Unit 4 when you want a video walkthrough.
Open the Fiveable one-page unit review, then explore visual cheatsheets for a quick refresher.
Estimate your broader AP score goal after you review the course and exam format.

Print the unit cheatsheets ($3) for Unit 4. Yours to keep, no subscription needed.
get printablesThe AP Physics C: Mechanics Unit 4 progress check in AP Classroom includes both MCQ and FRQ parts drawn from all four unit topics: Linear Momentum, Change in Momentum and Impulse, Conservation of Linear Momentum, and Elastic and Inelastic Collisions. The MCQ section tests conceptual understanding and calculation, while the FRQ part asks you to set up and solve multi-step problems involving impulse-momentum and collision scenarios. For the progress check, focus on applying the impulse-momentum theorem correctly and distinguishing elastic from inelastic collisions. You can find matched practice problems at AP Physics C: Mechanics Unit 4.
Unit 4 FRQs in AP Physics C: Mechanics most often come from Conservation of Linear Momentum and Elastic and Inelastic Collisions, so those two topics should anchor your free-response practice. A typical FRQ will ask you to define a system, justify why momentum is conserved, set up conservation equations, and solve for an unknown velocity or energy loss. To practice effectively:
- Write out your system definition and conservation statement before calculating
- Show all vector directions explicitly, since momentum is a vector quantity
- Practice both perfectly inelastic and elastic collision setups, as each has a different equation structure
- Check your work by verifying units and the reasonableness of your answer Find FRQ-style practice problems at AP Physics C: Mechanics Unit 4.
The best place to find AP Physics C: Mechanics Unit 4 practice questions, including multiple-choice and practice test problems, is AP Physics C: Mechanics Unit 4. That page has resources covering all four topics: Linear Momentum, Change in Momentum and Impulse, Conservation of Linear Momentum, and Elastic and Inelastic Collisions. For MCQ practice, look for questions that ask you to calculate impulse, compare momentum before and after a collision, or identify whether kinetic energy is conserved. These are the most common question formats for this unit on the actual exam.
Start with the impulse-momentum theorem in Topic 4.2 before moving to conservation laws, since understanding how force and time change momentum makes Topic 4.3 much more intuitive. Unit 4 rewards students who practice setting up problems systematically rather than jumping straight to equations. A solid study plan for this unit:
1. Build the foundation first. Make sure you can define momentum as a vector and apply p = mv in multiple dimensions before tackling collisions.
2. Master the impulse-momentum theorem. Practice interpreting force-time graphs and calculating impulse from area under the curve.
3. Drill conservation of momentum. Write out system definitions and justify conservation conditions every time, not just when the problem asks you to.
4. Separate collision types clearly. Know that elastic collisions conserve both momentum and kinetic energy, while inelastic collisions conserve only momentum.
5. Do timed FRQ practice. Since this unit is 10-20% of the exam, free-response problems here are high value. All four topics are organized at AP Physics C: Mechanics Unit 4.