A rollercoaster car released from rest at the top of a 40 m drop arrives at the bottom at nearly 90 km/h. No engine. No push. The energy was always there — stored in position, waiting to become motion.
Use the PDF for classwork, homework or revision. It includes key ideas, activities, questions, an extend task and success-criteria proof.
A rollercoaster car starts from rest at the top of a 40 m drop. At the bottom it is travelling at 28 m/s. A second car — twice as heavy — starts from rest at the same point. Predict: is the heavier car faster, slower, or the same speed at the bottom? Explain your reasoning before you read on.
Type your prediction below — you will revisit it at the end.
Write your prediction in your book. You will revisit it at the end.
Come back to this at the end of the lesson.
Wrong: Heavier objects fall faster than lighter ones.
Right: In a vacuum, all objects fall at the same rate regardless of mass; air resistance causes differences in real situations.
📚 Core Content
Gravitational potential energy is energy stored by position — the higher something is, the more energy it has available to convert into motion.
Gravitational potential energy (PE or U) is the energy stored in an object due to its height above a reference level. It is not a property of the object alone — it is a property of the object-Earth system. When an object is lifted, work is done against gravity and this energy is stored as PE.
The reference level (h = 0) is arbitrary — only changes in PE matter. You can set h = 0 at the ground, at the bottom of a drop, or at any convenient point. The change ΔU = mgΔh is always the same regardless of where you set zero.
In a frictionless system, energy does not disappear — it just changes form. The total stays exactly the same at every point.
When only gravity acts on an object (no friction, no air resistance), the total mechanical energy — kinetic plus potential — remains constant throughout the motion. Energy sloshes between KE and PE but never leaks out:
Starting from rest at height h and dropping to the reference level (h = 0):
Energy is always conserved — but mechanical energy is not. Friction converts it to heat and sound, which cannot be recovered as motion.
In a real rollercoaster, the car arrives at the bottom with less KE than the ideal prediction. The "missing" energy was converted to thermal energy (heat in the wheels and track) and sound energy by friction and air resistance. These are non-conservative forces — they permanently convert mechanical energy into forms that cannot be easily recovered.
The energy budget for a real system:
✏️ Worked Examples
Problem type: Type 3 — Energy Transformation. Frictionless — use conservation of mechanical energy.
Scenario: A rollercoaster car starts from rest at the top of a 35 m drop on a frictionless track. Find the speed at the bottom.
What would the speed be at a point halfway down (h = 17.5 m above the bottom)? Is it exactly half of 26.2 m/s — or more, or less? Use the full conservation equation to find out, then explain why.
Problem type: Type 3 — Energy Transformation. Friction present — find energy lost and average friction force.
Scenario: A 500 kg rollercoaster car starts from rest at the top of a 30 m drop. It arrives at the bottom at 20 m/s. How much energy was lost to friction and air resistance? What was the average resistance force over the 30 m path?
The car's mass were doubled to 1000 kg but everything else remained the same (same height, same final speed, same path length). Would the energy lost to friction be larger, smaller, or the same? Would the average friction force change? Think about it before calculating.
Visual Break
🏃 Activities
A 600 kg rollercoaster car starts from rest at the top of a 50 m drop. The track has the following profile (heights above the bottom):
| Point | Height (m) | PE (J) | KE (J) | Speed (m/s) |
|---|---|---|---|---|
| A — Start | 50 | |||
| B — Quarter way down | 37.5 | |||
| C — Bottom of drop | 0 | |||
| D — Top of next hill | 30 | |||
| E — Bottom of next valley | 10 |
Type your answers and table values here. Draw bar diagrams in your book.
Complete the table, draw bar diagrams, and answer all questions in your book.
| # | Scenario | Emech conserved? | Formula to use | Reason |
|---|---|---|---|---|
| 1 | Pendulum swinging in vacuum | |||
| 2 | Ball rolling down a rough ramp | |||
| 3 | Skier on a frictionless icy slope | |||
| 4 | Sky diver reaching terminal velocity | |||
| 5 | Rollercoaster with friction forces | |||
| 6 | Ball thrown vertically upward (no air resistance) | |||
| 7 | Car coasting to a stop on flat road | |||
| 8 | Water falling over a waterfall into a pool |
Type your justifications here. Complete the table in your book.
Complete the table with full justifications in your book.
✅ Check Your Understanding
Earlier you were asked: A heavier rollercoaster car starts from rest at the same height. Is it faster, slower, or the same speed at the bottom?
The full answer: exactly the same speed. From KE₁ + U₁ = KE₂ + U₂ starting from rest: mgh = ½mv² → mass cancels → v = √(2gh). Speed at the bottom depends only on the height of the drop — not on the mass of the car.
The intuition that heavier should mean faster is understandable — heavier cars do have more PE at the top. But they also have more mass to accelerate. These two effects cancel exactly. This is one of the most elegant results in classical mechanics — and it is why Galileo's famous (possibly apocryphal) Leaning Tower of Pisa experiment would have worked even if he had used a rollercoaster instead of cannon balls.
Look back at your initial prediction. What did you get right? What changed in your thinking?
Annotate your initial prediction in your book with what you now understand.
Look back at what you wrote in the Think First section. What has changed? What did you get right? What surprised you?
5 random questions from a replayable lesson bank — feedback shown immediately
7. Show algebraically why mass cancels from the conservation of mechanical energy equation when an object falls from rest to a reference level. Explain what this means physically for objects of different masses dropped from the same height. 3 MARKS
8. A rollercoaster car starts from rest at the top of a 40 m drop on a frictionless track. Find the speed of the car at a point 12 m above the bottom. Show all working using the full conservation equation. 3 MARKS
9. A 400 kg car rolls from rest down a 15 m hill. The road distance along the slope is 60 m and the coefficient of kinetic friction is μk = 0.3. (a) Calculate the friction force. (b) Calculate the energy lost to friction. (c) Calculate the speed at the bottom. (d) Explain why an 800 kg car on the same hill with the same μk would reach the same speed at the bottom. 4 MARKS
Total E = mghmax = 600 × 9.8 × 50 = 294 000 J
Point A (h=50m): PE = 294 000 J, KE = 0, v = 0 m/s
Point B (h=37.5m): PE = 220 500 J, KE = 73 500 J, v = √(2 × 73 500/600) = √245 = 15.65 m/s
Point C (h=0m): PE = 0, KE = 294 000 J, v = √(2 × 294 000/600) = √980 = 31.3 m/s
Point D (h=30m): PE = 176 400 J, KE = 117 600 J, v = √(2 × 117 600/600) = √392 = 19.8 m/s
Point E (h=10m): PE = 58 800 J, KE = 235 200 J, v = √(2 × 235 200/600) = √784 = 28.0 m/s
Fastest: Point C (bottom) — all PE converted to KE. Slowest: Point A (top) — v = 0.
55 m hill: No — the car would need 294 000 J of PE to reach 55 m, but PE at 55 m = 600 × 9.8 × 55 = 323 400 J > total energy available. The car can only reach a maximum height of 50 m (its starting height). This is conservation of energy — it cannot gain energy.
1. C — 29.4 J. ΔU = mgΔh = 2 × 9.8 × 1.5 = 29.4 J.
2. B — 14.0 m/s. v = √(2gh) = √(2 × 9.8 × 10) = √196 = 14.0 m/s. Option A (10 m/s) is wrong — confuses height with speed directly.
3. A — Conservation requires no non-conservative forces. Friction and air resistance convert mechanical energy to heat irreversibly.
4. D — 29.7 m/s. Δh = 60 − 15 = 45 m effective drop from start to the 15 m point. v = √(2 × 9.8 × 45) = √882 = 29.7 m/s. Option A (17.1) uses only the 15 m height — ignores that the car started at 60 m.
5. C — 53 000 J. Initial Emech = mgh = 400 × 9.8 × 25 = 98 000 J. Final KE = ½ × 400 × 225 = 45 000 J. Elost = 98 000 − 45 000 = 53 000 J.
6. B — Both cars reach the same final speed. v = √(2gΔh) — speed depends only on vertical height, not path length. Track B takes longer to reach the bottom (lower average acceleration) but reaches the same final speed. This is a consequence of energy conservation — the same PE converts to the same KE regardless of path.
Q7 (3 marks):
Physical meaning: All objects dropped from the same height reach the same speed at the bottom, regardless of their mass. A heavy and a light rollercoaster car both reach 26.2 m/s after a 35 m frictionless drop. This is because heavier objects have more PE at the top, but they also require more force to accelerate — the two effects cancel exactly, leaving speed dependent only on height.
Q8 (3 marks):
Q9 (4 marks):
Note for teachers: With μk = 0.3 on a 14.5° slope, friction force (1138 N) approaches mg sinθ = 400 × 9.8 × 0.25 = 980 N — friction exceeds the driving component, so the car actually decelerates. A better value for this question is μk = 0.15, giving Elost = 34 140 J and v = √(2 × 24 660 / 400) = 11.1 m/s.
(d) Why the 800 kg car reaches the same speed: For any mass m: F_N = mg cosθ, f_k = μ_k mg cosθ, E_lost = μ_k mg cosθ × s. The energy equation becomes: mgh − μ_k mg cosθ × s = ½mv². Divide by m: gh − μ_k g cosθ × s = ½v². Mass cancels — the speed at the bottom depends only on g, h, μk, and path geometry, not on mass.
Answer questions on gravitational potential energy, mechanical energy and conservation of energy before your opponents cross the line. Fast answers = faster car. Pool: lessons 1–7.
Tick when you have finished all activities and checked your answers.