FOUNDATION 01
What Is Momentum?
Momentum is a vector quantity associated with the motion of a particle. It depends on both the particle's mass and its velocity.
Because velocity is a vector, momentum is also a vector. Therefore, the direction of momentum is the same as the direction of the particle's velocity.
Never treat velocities as positive simply because the particles are moving. You must choose a positive direction and assign negative signs to velocities in the opposite direction.
FOUNDATION 02
Choosing a Positive Direction
Most collision questions become much easier once a positive direction has been chosen.
For example, suppose particle A moves to the right and particle B moves to the left. We may choose right as positive.
If A has velocity 8 m/s to the right, its velocity is +8 m/s. If B has velocity 5 m/s to the left, its velocity is −5 m/s.
SIGN-CONVENTION EXAMPLE
A particle of mass 3 kg travels at 6 m/s to the left. Take right as positive.
Since left is negative:
v = −6 m/s
Therefore:
p = mv = 3(−6)
p = −18 kg m s−1
Write your chosen positive direction before starting a collision calculation. This prevents most sign errors.
CORE THEORY 03
Conservation of Momentum
When considering a system of particles, the total momentum remains constant if the resultant external force acting on the system is zero.
For two particles with masses m1 and m2, initial velocities u1 and u2, and final velocities v1 and v2:
This equation is one of the central tools for collision questions. It is a vector equation, so signs matter.
Forces during a collision are internal forces within the chosen system. By Newton's third law, the forces the particles exert on each other are equal and opposite, so their impulses cancel when the whole system is considered.
When can we use conservation of momentum?
- The system must be clearly defined.
- The resultant external impulse on the system must be negligible or zero over the time interval being considered.
- Internal forces between the particles do not destroy total momentum conservation.
CORE THEORY 04
Impulse and Change in Momentum
Impulse measures the effect of a force acting over a time interval. It is equal to the change in momentum.
If the force is constant:
Therefore:
| Quantity | Meaning | Unit |
|---|---|---|
| I | Impulse | N s |
| F | Force | N |
| t | Time interval | s |
| mv − mu | Change in momentum | kg m s−1 |
1 N s = 1 kg m s−1.
CORE THEORY 05
Direct Impact
A collision is called a direct impact when the particles move along the same straight line before and after the collision.
This is the standard collision model used throughout Mechanics 2.
The motion of both particles can be represented using one straight line, so their velocities can be treated using signed one-dimensional quantities.
A typical problem gives the masses and velocities before impact and then asks for one or both velocities after impact.
CORE THEORY 06
Newton's Law of Restitution
For two particles undergoing a direct collision, Newton's law of restitution relates the relative speed of separation to the relative speed of approach.
The coefficient of restitution is normally denoted by e. For the usual collision model:
If particle 1 is initially moving faster than particle 2 and they are approaching one another, then:
provided the chosen positive direction is such that particle 1 is moving in the positive direction towards particle 2.
The safest method is always to identify the actual relative speed of approach and relative speed of separation from the motion described in the question.
CORE THEORY 07
Coefficient of Restitution: Physical Meaning
e = 1
The relative speed of separation equals the relative speed of approach.
This corresponds to a perfectly elastic collision in the idealised model.
e = 0
The relative speed of separation is zero.
The particles have the same velocity immediately after impact and therefore move together.
For 0 < e < 1, some kinetic energy is lost during the collision, although momentum is still conserved for an isolated system.
Momentum conservation does NOT mean kinetic energy conservation. These are different physical principles.
CORE THEORY 08
Elastic and Inelastic Collisions
The coefficient of restitution gives useful information about the nature of a collision.
Elastic collision
Momentum is conserved.
Kinetic energy is also conserved.
For the ideal one-dimensional case: e = 1.
Inelastic collision
Momentum is conserved for an isolated system.
Kinetic energy is not conserved.
For 0 ≤ e < 1, relative separation is reduced.
The change in kinetic energy can be found by comparing the total kinetic energy before and after the collision.
Do not automatically write a kinetic-energy equation in every collision question. Momentum is the conservation equation. Kinetic energy is only conserved when the collision is elastic or when the question explicitly gives enough information to use it.
CORE THEORY 09
The Standard Collision System
Suppose two particles have masses m1 and m2. Before impact their velocities are u1 and u2, and after impact their velocities are v1 and v2.
If the particles approach each other and then separate:
The two equations usually provide the two unknown final velocities.
Typical exam structure
WORKED EXAMPLE 01
Finding Both Velocities After Impact
FULL EXAM-STYLE SOLUTION
A particle A of mass 2 kg moves with velocity 6 m/s towards particle B, which has mass 3 kg and is initially at rest. The coefficient of restitution between the particles is 0.5. Find the velocities of A and B after the collision.
Take the direction of A's initial motion as positive.
Therefore:
uA = 6, uB = 0
Step 1 — Conservation of momentum
2(6) + 3(0) = 2vA + 3vB
Therefore:
12 = 2vA + 3vB
Step 2 — Newton's law of restitution
Relative speed of approach:
6 − 0 = 6
Relative speed of separation:
vB − vA
Therefore:
0.5 = (vB − vA) / 6
So:
vB − vA = 3
Step 3 — Solve simultaneously
vB = vA + 3
Substitute into momentum:
12 = 2vA + 3(vA + 3)
12 = 5vA + 9
3 = 5vA
vA = 0.6
Therefore:
vB = 3.6
A moves at 0.6 m/s and B moves at 3.6 m/s in the positive direction.
WORKED EXAMPLE 02
A Collision With Opposite Initial Directions
SIGN CONVENTION MATTERS
Particle A of mass 4 kg moves at 5 m/s to the right. Particle B of mass 2 kg moves at 3 m/s to the left. The coefficient of restitution is 0.5. Find their velocities after impact.
Take right as positive.
uA = 5
uB = −3
Momentum
4(5) + 2(−3) = 4vA + 2vB
20 − 6 = 4vA + 2vB
14 = 4vA + 2vB
Restitution
Before impact, the particles approach each other at:
5 − (−3) = 8 m/s
So the separation speed is:
0.5 × 8 = 4 m/s
After impact A is expected to be moving to the left relative to B, so:
vB − vA = 4
Therefore:
vB = vA + 4
Substitute:
14 = 4vA + 2(vA + 4)
14 = 6vA + 8
6vA = 6
vA = 1
Therefore:
vB = 5
A moves at 1 m/s to the right and B moves at 5 m/s to the right.
WORKED EXAMPLE 03
Finding the Coefficient of Restitution
FIND e
Two particles approach each other with speeds 7 m/s and 2 m/s. After collision they separate with speeds 1 m/s and 3 m/s. Find the coefficient of restitution.
The relative speed of approach is:
7 + 2 = 9 m/s
The relative speed of separation is:
3 + 1 = 4 m/s
Therefore:
e = 4 / 9
e = 4/9
When two particles move towards each other, their relative speed of approach is usually the sum of their speeds if those speeds are stated as positive magnitudes.
WORKED EXAMPLE 04
Impulse During a Collision
MOMENTUM CHANGE
A 3 kg particle moves at 8 m/s to the right before collision and at 2 m/s to the left after collision. Find the impulse acting on the particle.
Take right as positive.
u = 8
v = −2
Impulse = mv − mu
= 3(−2) − 3(8)
= −6 − 24
Impulse = −30 N s
The negative sign means the impulse acts to the left.
Impulse depends on the change in velocity, so direction must be included.
CORE THEORY 14
Collision and Kinetic Energy
Momentum is conserved in an isolated collision, but kinetic energy may decrease.
For an elastic collision:
For an inelastic collision, the final kinetic energy is smaller than the initial kinetic energy.
It may be transformed into internal energy, deformation, sound, heat or other forms of energy. Total energy is still conserved; it is kinetic energy that is not necessarily conserved.
CORE THEORY 15
Perfectly Inelastic Collision
A perfectly inelastic collision is the special case where the particles have zero relative speed of separation.
Therefore:
The particles move together immediately after impact.
Conservation of momentum can then be used to find their common velocity.
EXAMPLE — PARTICLES STICK TOGETHER
A 2 kg particle moving at 6 m/s collides with a stationary 4 kg particle. They move together after collision. Find their common velocity.
Momentum before:
2(6) + 4(0) = 12
Momentum after:
(2 + 4)v = 6v
Therefore:
12 = 6v
v = 2 m/s
CORE THEORY 16
When Will Two Particles Actually Collide?
A collision can only occur if the particles are moving towards each other along the same line.
For example, if particle A is behind particle B and both move in the same direction, A will catch B only if A has the greater speed.
If A is initially a distance d behind B and their velocities remain constant, the time to collision is found using relative speed:
Do not automatically assume that two particles mentioned in the same question will collide. Check their relative positions and velocities.
CORE THEORY 17
Repeated Collisions
Some Mechanics 2 problems involve a particle colliding with another particle, after which the particles move away and may later collide with other objects.
The safest strategy is to treat each collision as a separate event.
Collision 1 → new velocities → motion → Collision 2 → new velocities. Never mix the equations from different collisions.
EXAM METHOD 18
The Universal Collision Method
For most two-particle direct-impact questions, this procedure will keep your working organised.
COMMON ERRORS 19
Mistakes That Cost Marks
1. Ignoring direction
Momentum is a vector. Writing every velocity as positive can destroy the momentum equation.
2. Using speed instead of velocity
Restitution uses relative speeds, but momentum uses signed velocities.
3. Reversing approach and separation
Always identify what happens before and after impact.
4. Assuming kinetic energy is conserved
Momentum conservation is the standard principle. Kinetic energy requires an elastic collision.
5. Forgetting the mass
A heavier particle can have greater momentum even when moving more slowly.
6. Misinterpreting a negative answer
A negative velocity is not automatically a wrong answer. It indicates motion opposite to the chosen positive direction.
7. Using e incorrectly
The coefficient of restitution is a ratio of relative speeds, not simply the ratio of the two individual final speeds.
DEEPER CONNECTION 20
Momentum, Impulse and Force
Momentum and impulse are closely connected to Newton's laws.
If a force acts for a short time during a collision, the impulse is the area under a force-time graph.
For a constant force:
For a variable force, the area must be determined using the appropriate geometry or integration where applicable.
A large force acting for a very short time can produce the same impulse as a smaller force acting for a longer time.
DEEPER CONNECTION 21
Why Newton's Restitution Law Works
Newton's law of restitution does not say that the velocities after collision are simply a fixed percentage of the velocities before collision.
Instead, it compares the motion of the two particles relative to one another.
This is important because a collision concerns the relative motion between the particles rather than the motion of either particle by itself.
Momentum controls the overall motion of the system, while restitution controls how much relative motion is recovered after impact.
WORKED EXAMPLE 05
Finding e From a Complete Collision
MULTI-STAGE REASONING
A particle A moves at 10 m/s towards a stationary particle B. After impact A moves at 2 m/s in the same direction and B moves at 6 m/s in the same direction. Find the coefficient of restitution.
Before impact, the relative speed of approach is:
10 − 0 = 10 m/s
After impact, the relative speed of separation is:
6 − 2 = 4 m/s
Therefore:
e = 4/10
e = 0.4
EXAM CHECK 23
How to Check Your Final Answer
Before moving to the next part of the question, perform a quick physical check.
- Does the momentum equation balance?
- Are the particles moving apart after the collision?
- Is the coefficient of restitution between 0 and 1 for the usual collision model?
- Have you interpreted negative velocities correctly?
- If the collision is elastic, is kinetic energy conserved?
- Are your units correct?
If your calculated coefficient of restitution is greater than 1, do not immediately accept it. Recheck your relative approach and separation speeds and your sign convention.
PRACTICE 24
Collision Practice Bank
Show solution
p = mv
= 5 × 4
p = 20 kg m s−1
Show solution
I = m(v − u)
= 3(9 − 5)
I = 12 N s
Show solution
2(8) + 3(0) = (2 + 3)v
16 = 5v
v = 3.2 m/s
Show solution
Approach speed = 9 + 4 = 13 m/s
Separation speed = 3 + 2 = 5 m/s
e = 5/13
Show solution
Momentum:
4(7) = 4v1 + 2v2
28 = 4v1 + 2v2
Restitution:
v2 − v1 = 0.5(7)
v2 − v1 = 3.5
v2 = v1 + 3.5
28 = 4v1 + 2(v1 + 3.5)
28 = 6v1 + 7
v1 = 3.5
v2 = 7
v1 = 3.5 m/s, v2 = 7 m/s
Show solution
Impulse depends on the change in momentum, and momentum depends on velocity including direction. Therefore the final velocity must be assigned the correct sign before calculating mv − mu.
Show solution
Momentum is conserved because the internal forces during the collision provide equal and opposite impulses. Kinetic energy, however, may be transformed into other forms such as heat, sound and deformation.
Show solution
Relative speed = 8 − 5 = 3 m/s
t = distance / relative speed
t = 12/3
t = 4 s
MASTER SUMMARY 25
Collision Formula Atlas
FINAL EXAM CHECKLIST 26
Before You Submit a Collision Question
- Have I chosen a positive direction?
- Have I used signed velocities in the momentum equation?
- Have I written total momentum before and after impact?
- Have I correctly identified the relative speed of approach?
- Have I correctly identified the relative speed of separation?
- Have I used the coefficient of restitution in the correct direction?
- Have I solved the simultaneous equations accurately?
- Have I interpreted negative velocities correctly?
- If the collision is elastic, have I checked kinetic energy?
- Are all final quantities given with appropriate units?
- Does the physical situation make sense?
Do not memorise collision equations as isolated formulas. Understand the physical story: momentum describes the total motion of the system, while restitution describes how the relative motion changes during impact.