Conservation of
Linear Momentum
Discover why total momentum stays constant in isolated systems, and master the principle behind collisions and explosions.
What Is Momentum?
Momentum is a vector quantity that describes the "quantity of motion" an object possesses. It depends on both mass and velocity:
Impulse and Newton's Second Law
Newton's Second Law can be rewritten in terms of momentum. The net force on an object equals the rate of change of its momentum:
Impulse (\( \vec{J} \)) is the product of force and the time interval over which it acts. It equals the change in momentum of the object.
Internal vs External Forces
To apply conservation of momentum, you must define a system of objects and classify every force:
The Conservation Law
The Two-Object Equation
For a system of two objects with no net external force, conservation of momentum gives us:
Elastic vs Inelastic Collisions
Momentum is conserved in all collisions (assuming an isolated system). The distinction lies in whether kinetic energy is also conserved:
| Elastic | Inelastic | Perfectly Inelastic | |
|---|---|---|---|
| Momentum Conserved? | Yes | Yes | Yes |
| KE Conserved? | Yes | No | No (max loss) |
| Objects After | Bounce apart | May deform | Stick together |
| Example | Billiard balls | Car crash (bounce) | Catching a ball |
Perfectly Inelastic Collisions
When objects stick together after colliding, they share a common final velocity \( v_f \). This simplifies the conservation equation:
Additional worked example
The following is a separate example from the long-form lesson. Its values may differ from the example already on this slide.
A 1200 kg car traveling east at 15 m/s collides with a 900 kg car traveling west at 10 m/s. The cars lock bumpers and slide together after the collision. Determine the velocity of the combined wreckage immediately after impact, and calculate the fraction of kinetic energy lost.
Show answer and explanation
Step 1 — Define the System & Coordinate Axis: The system consists of both cars. Define east as the positive direction. Car 1: m₁ = 1200 kg, v₁ᵢ = +15 m/s. Car 2: m₂ = 900 kg, v₂ᵢ = −10 m/s (west is negative). Since the collision happens quickly and friction during the collision is negligible compared to the enormous internal forces, the system is approximately isolated during the impact. Step 2 — Write Conservation of Momentum: Because the cars stick together (perfectly inelastic), they share a common final velocity vf. The conservation equation is: m₁v₁ᵢ + m₂v₂ᵢ = (m₁ + m₂)vf. Step 3 — Substitute and Solve for vf: (1200)(+15) + (900)(−10) = (1200 + 900)vf → 18000 − 9000 = 2100 × vf → 9000 = 2100 × vf → vf = 9000 / 2100 ≈ 4.29 m/s. vf ≈ +4.3 m/s (east) Step 4 — Calculate Initial and Final Kinetic Energies: KE_initial = ½m₁v₁ᵢ² + ½m₂v₂ᵢ² = ½(1200)(15²) + ½(900)(10²) = 135000 + 45000 = 180000 J. KE_final = ½(2100)(4.29²) ≈ ½(2100)(18.38) ≈ 19300 J. Step 5 — Determine the Fraction of KE Lost: Fraction lost = (KE_initial − KE_final) / KE_initial = (180000 − 19300) / 180000 ≈ 0.893. Approximately 89% of the original kinetic energy is converted into thermal energy, sound, and permanent deformation of the vehicles. This dramatic energy loss is characteristic of perfectly inelastic collisions, yet momentum is perfectly conserved. ≈ 89% of KE is lost

Explosions and Recoil
An explosion is the reverse of a perfectly inelastic collision: one object splits into two or more pieces. If the system starts at rest, total momentum before is zero:
The pieces fly off in opposite directions with momenta that are equal in magnitude. A cannon recoiling after firing a shell is a classic example: the heavy cannon moves slowly backward while the lighter shell moves quickly forward.
How to Solve Momentum Problems
Example 1: Simple Collision
A 4 kg cart moving at 6 m/s to the right collides with a 2 kg cart at rest. After the collision, the 4 kg cart moves at 2 m/s to the right. Find the final velocity of the 2 kg cart.
Example 2: Perfectly Inelastic
A 5 kg ball moving at 3 m/s right collides with a 3 kg ball moving at 2 m/s left. They stick together. Find \( v_f \).
Example 3: Cannon Recoil
A 500 kg cannon fires a 5 kg shell at 200 m/s forward. Both start at rest. Find the recoil velocity of the cannon.
Momentum in Two Dimensions
Momentum is a vector, so conservation applies independently to each component:
Common Mistakes to Avoid
Summary of Key Equations
| Scenario | Equation | Key Condition |
|---|---|---|
| General (2 objects) | \( m_1v_{1i} + m_2v_{2i} = m_1v_{1f} + m_2v_{2f} \) | \( F_{\text{ext}} = 0 \) |
| Perfectly Inelastic | \( m_1v_{1i} + m_2v_{2i} = (m_1+m_2)v_f \) | Objects stick together |
| Explosion / Recoil | \( 0 = m_1v_{1f} + m_2v_{2f} \) | Starts from rest |
| Elastic (extra eq.) | \( \tfrac{1}{2}m_1v_{1i}^2 + \tfrac{1}{2}m_2v_{2i}^2 = \tfrac{1}{2}m_1v_{1f}^2 + \tfrac{1}{2}m_2v_{2f}^2 \) | KE also conserved |
Question 1 of 5
A 3 kg object moving at 4 m/s collides with a 1 kg object at rest. They stick together. What is their final velocity?
Question 2 of 5
Which quantity is always conserved in any collision within an isolated system?
Question 3 of 5
A 60 kg astronaut floating at rest in space throws a 5 kg tool at 6 m/s. What is the astronaut's recoil speed?
Question 4 of 5
Two identical 2 kg balls collide head-on. Ball A moves right at 5 m/s and Ball B moves left at 3 m/s. After collision, Ball A moves right at 1 m/s. What is Ball B's final velocity?
Question 5 of 5
A 10 kg cart moving at 4 m/s collides with a 10 kg stationary cart. They stick together. How much kinetic energy is lost?