Momentum, Impulse, and Conservation
Key Takeaways
- Momentum is a vector quantity equal to mass times velocity, so sign and direction must be tracked in one-dimensional collisions.
- Impulse equals change in momentum and can be found from net force times time or from area under a force-time graph.
- Total momentum is conserved for an isolated system with no net external force, even though individual objects can gain or lose momentum.
- Kinetic energy is not automatically conserved in every collision; sticking collisions conserve momentum but usually transform some mechanical energy.
- Safety designs reduce average force by increasing stopping time while producing the same required change in momentum.
Momentum as a System Model
Momentum is the quantity that connects mass and velocity in an interaction. The 2025 Physics Reference Tables give p = mv. Because velocity is a vector, momentum is a vector. A cart moving east and the same cart moving west have momenta with opposite signs if east is chosen as positive.
The educator guide's Forces and Interactions claim includes models that explain momenta of systems and changes to systems. That means the Regents can ask for calculations, but it can also ask whether a collision model, graph, or explanation correctly tracks the system.
Momentum Basics
Momentum increases when mass increases, velocity magnitude increases, or both. A low-mass object can have large momentum if it moves fast. A massive object can have large momentum even at modest speed.
| Quantity | Relationship | Direction? | Unit check |
|---|---|---|---|
| Momentum | p = mv | Yes | kg*m/s |
| Impulse | Fnet t = m delta v | Yes | Ns or kgm/s |
| Momentum change | final momentum - initial momentum | Yes | kg*m/s |
| System total momentum | vector sum of object momenta | Yes | kg*m/s |
Use signs for one-dimensional problems. If east is positive, west is negative. Write that convention before adding momenta. Most wrong collision answers come from adding speeds without direction.
Impulse Means Momentum Change
Impulse is the change in momentum of an object. The reference tables show the impulse-momentum relationship as net force times time interval equals mass times change in velocity. The force must be the net force over the time interval being considered.
A force-time graph gives impulse as area under the graph. Rectangles, triangles, and trapezoids may appear in data-based questions. The unit N*s is equivalent to kg*m/s, which confirms that impulse and momentum change describe the same physical change.
If the force changes during a collision, the graph area is more reliable than multiplying peak force by total time. Peak force is not the same as average force unless the graph supports that model.
Why Time Matters in Safety Designs
Safety devices such as mats, padding, helmets, crumple zones, and airbags do not eliminate the needed momentum change. A moving object still must go from its initial momentum to a smaller final momentum, often zero.
They reduce average force by increasing stopping time. Since impulse equals force times time, a longer time interval can produce the same momentum change with a smaller average force. This is a common engineering connection in Regents-style explanations.
A strong answer says that the momentum change is the same for the same initial and final velocities, but the longer stopping time lowers the average net force. That links the design choice to the physics relationship.
Conservation of Momentum
Total momentum is conserved when the chosen system is isolated, meaning there is no net external force during the interaction or external forces are negligible during the short interval. Internal forces between objects can be large, but they occur in equal and opposite pairs within the system.
For two colliding carts, choose both carts as the system. The force of cart A on cart B and the force of cart B on cart A are internal. They change individual momenta, but their effects cancel in the system total.
Momentum conservation is written as total momentum before equals total momentum after. This is a vector statement. In one dimension, keep signs. In two dimensions, momentum must be conserved separately in perpendicular directions.
Collision Types
An elastic collision conserves both total momentum and kinetic energy. An inelastic collision conserves total momentum but not kinetic energy. A perfectly inelastic collision is the special case where objects stick together after impact.
The Regents does not require a label before reasoning. If two carts stick, use a shared final velocity and conserve momentum for the system if external forces are negligible. Do not assume kinetic energy stays the same. Some mechanical energy may become thermal energy, sound, deformation, or internal energy.
Explosions and recoil use the same conservation idea. If a system starts at rest and internal forces push parts apart, the final momenta must add to zero. The more massive part usually moves more slowly than the less massive part.
Solving a One-Dimensional Collision
Use a compact setup:
- Choose a positive direction.
- Write initial momentum for each object with signs.
- Add to get total initial momentum.
- Write final momentum for each object with signs.
- Set total before equal to total after if the system is isolated.
- Solve for the unknown velocity and include direction.
This setup avoids treating velocity as only speed. It also makes it clear whether the answer should be east, west, upward, downward, or opposite the original motion.
Constructed-Response Evidence
For a claim about conservation, identify the system boundary and the external-force condition. A statement like momentum is conserved because it is a collision is incomplete. The better statement is that total momentum of the two-cart system is conserved because external forces during the short collision are negligible.
For a force-time graph, cite the area. For a design question, cite the stopping time and average force relationship. For a recoil question, cite the initial total momentum and the need for final momenta to balance.
Common Momentum Traps
- Forgetting momentum direction.
- Conserving speed instead of momentum.
- Assuming kinetic energy is conserved in a sticking collision.
- Using peak force instead of graph area for impulse.
- Choosing a system with an important external force and still claiming conservation.
- Saying third-law forces cancel on one object instead of within the system total.
Momentum is a systems topic. Once the system boundary and direction convention are clear, the equations become much easier to use correctly.
A 0.40 kg cart moving east at 5.0 m/s sticks to a 0.60 kg cart moving west at 1.0 m/s. If east is positive and external forces are negligible, what is the velocity of the combined carts just after the collision?