Year 11 Physics Module 2: Dynamics 35 min Lesson 7 of 15

Gravitational PE and Energy Conservation

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.

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Think First

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.

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Formula Reference — This Lesson

ΔU = mgΔh  |  KE₁ + U₁ = KE₂ + U₂
ΔU = change in gravitational PE (J)  |  Δh = vertical height change (m) Conservation: ½mv₁² + mgh₁ = ½mv₂² + mgh₂ (frictionless only)
Speed from height (v₁=0, frictionless): v = √(2gΔh)   |   With friction: KE₁ + U₁ = KE₂ + U₂ + Wfriction

E=mgh
Formula Reference — Gravitational PE and Energy Conservation

ΔU = mgΔh
Change in Gravitational Potential Energy
ΔU = change in PE (J) | m = mass (kg) | g = 9.8 m/s² | Δh = vertical height change (m)
Applies when: object moves vertically in a uniform gravitational field near Earth's surface. Δh is the vertical component only — not distance along a slope.
Common trap: Δh is the vertical height, not the path length. A ball rolling 10 m down a 30° slope rises (or falls) only 5 m vertically — use Δh = 5 m, not 10 m.
Emech = KE + U
Total Mechanical Energy
Emech = total mechanical energy (J) | KE = ½mv² | U = gravitational PE (= mgh above reference level)
Applies when: only conservative forces act (gravity, springs). Emech is conserved when no friction or air resistance is present.
Common trap: Emech is NOT conserved when friction or air resistance is present — these convert mechanical energy to thermal energy irreversibly.
KE₁ + U₁ = KE₂ + U₂
Conservation of Mechanical Energy
Subscript 1 = initial state | Subscript 2 = final state. Expanded: ½mv₁² + mgh₁ = ½mv₂² + mgh₂
Applies when: no friction, no air resistance, no non-conservative forces
Common trap: Using this equation when friction is present gives the wrong answer. If the problem mentions friction or air resistance, use Wnet = ΔKE instead, accounting for energy lost.
v = √(2gΔh)
Speed at bottom from height (mass cancels)
Derived from ½mv² = mgΔh — mass cancels, leaving v = √(2gΔh)
Applies when: object starts from rest, frictionless, and Δh is the total vertical drop
Common trap: This only works when the object starts from rest (v₁ = 0) and the surface is frictionless. If either condition fails, use the full conservation equation.

Know

  • ΔU = mgΔh for gravitational PE
  • Conservation of mechanical energy: KE₁ + U₁ = KE₂ + U₂
  • When mechanical energy IS and IS NOT conserved
  • v = √(2gΔh) for frictionless drop from rest

Understand

  • Why mass cancels from the conservation equation
  • Why speed at the bottom depends only on height — not mass
  • Why friction breaks conservation of mechanical energy
  • What "energy lost" to friction actually means physically

Can Do

  • Calculate PE at different heights along a track
  • Find speed at any point using KE₁ + U₁ = KE₂ + U₂
  • Calculate energy lost to friction from before/after data
  • Classify whether a scenario conserves mechanical energy

Choose how you work — type your answers below or write in your book.

Misconceptions to Fix

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.

Key Terms
ForceA push or pull acting on an object that can cause it to accelerate.
NewtonThe SI unit of force; 1 N = 1 kg·m/s².
WeightThe force due to gravity acting on a mass; W = mg.
Normal ForceThe perpendicular contact force exerted by a surface on an object.
FrictionA force that opposes relative motion between two surfaces in contact.
Net ForceThe vector sum of all forces acting on an object.
01Gravitational Potential Energy — ΔU = mgΔh

Gravitational Potential Energy — ΔU = mgΔh

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.

Rollercoaster car

Mass (kg): 500
Height (m): 40
PE (J): 196 000
Note: Top of 40 m drop

Rollercoaster car

Mass (kg): 500
Height (m): 20
PE (J): 98 000
Note: Halfway down

Rollercoaster car

Mass (kg): 500
Height (m): 0
PE (J): 0
Note: Bottom (reference level)

Water in Snowy Hydro dam

Mass (kg): 1 000 000
Height (m): 400
PE (J): 3 920 000 000
Note: Stored energy = 3.92 GJ per tonne
Australian Context — Snowy Hydro: The Snowy Mountains Scheme stores water at high elevation in large dams. Each tonne of water held 400 m above the turbines stores approximately 3.9 GJ of gravitational PE. When released, this PE converts to KE in the falling water, which then drives turbines to generate electricity. The height of the reservoir is the energy bank — ΔU = mgΔh at national scale.
02Conservation of Mechanical Energy

Conservation of Mechanical Energy

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:

$$KE_1 + U_1 = KE_2 + U_2$$ $$\tfrac{1}{2}mv_1^2 + mgh_1 = \tfrac{1}{2}mv_2^2 + mgh_2$$ At any two points on a frictionless track, the sum of KE and PE is the same.
Energy Conservation — Rollercoaster Track with Energy Bars

Why Mass Cancels

Starting from rest at height h and dropping to the reference level (h = 0):

$$\tfrac{1}{2}mv_1^2 + mgh_1 = \tfrac{1}{2}mv_2^2 + mgh_2$$ $$0 + mgh = \tfrac{1}{2}mv^2 + 0$$ $$mgh = \tfrac{1}{2}mv^2 \quad\Rightarrow\quad gh = \tfrac{1}{2}v^2 \quad\Rightarrow\quad \boxed{v = \sqrt{2gh}}$$ Mass cancels completely. Speed at the bottom depends only on the height of the drop — not on how heavy the object is. A 500 kg and a 5 kg rollercoaster car reach the same speed at the bottom of the same drop.
Vector Protocol — energy conservation problems
Step 1 — Define reference level (h = 0) and state it explicitly
Step 2 — Check: is friction present? If yes, do NOT use conservation — use Wnet = ΔKE
Step 3 — Write KE₁ + U₁ = KE₂ + U₂ before substituting any numbers
03Real Systems — Where Does the Energy Go?

Real Systems — Where Does the Energy Go?

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:

KE₁ + U₁ = KE₂ + U₂ + Elost
Where Elost = energy converted to heat and sound by friction and air resistance.
Elost = (KE₁ + U₁) − (KE₂ + U₂)
Ideal (frictionless)
147 000 J
147 000 J
24.2 m/s
0 J
Yes
Real (with friction)
147 000 J
100 000 J
20.0 m/s
47 000 J (32%)
No

Common Misconceptions

Friction destroys energy.
Energy is never destroyed — it is converted. Friction converts mechanical energy (KE + PE) into thermal energy (heat) and sound. The total energy of the universe is unchanged. Only mechanical energy decreases — total energy is conserved.
A heavier rollercoaster car goes faster because it has more PE at the top.
A heavier car does have more PE (PE = mgh — mass scales linearly). But it also has more mass to accelerate. The two effects cancel exactly — mass divides out and v = √(2gh) is independent of mass. Both cars reach the same speed.
Potential energy is stored in the object.
Gravitational PE is a property of the object-Earth system, not the object alone. It arises from the separation between the object and Earth. If Earth disappeared, the object would have no gravitational PE regardless of its height.
Interactive: Roller Coaster Energy Tracker
Interactive: Conservation of Energy (3D)
Interactive: KE and GPE vs Height

✏️ Worked Examples

Worked Example 1 Type 3 — Energy Transformation (frictionless)

Problem Setup

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.

  • v₁ = 0 m/s (starts from rest)
  • h₁ = 35 m (reference level: bottom = h = 0)
  • h₂ = 0 m (bottom)
  • Frictionless — conservation applies
  • Mass not given — check if it cancels

Solution

1
Reference level: h = 0 at bottom. Check: frictionless → use conservation.
Vector Protocol Steps 1 and 2. Define reference level first. Confirm no friction before choosing the equation.
2
KE₁ + U₁ = KE₂ + U₂ → 0 + mgh₁ = ½mv₂² + 0
Write the full conservation equation before substituting. KE₁ = 0 (at rest). U₂ = 0 (at reference level).
3
mgh = ½mv² → cancel m from both sides → gh = ½v²
Mass cancels — speed is independent of mass. This is the key physical insight of the lesson.
4
v = √(2gh) = √(2 × 9.8 × 35) = √686 = 26.2 m/s
Substitute and solve. 26.2 m/s = 94.3 km/h — from rest, with no engine, just gravity over 35 m.

What would change if...

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.

Worked Example 2 Type 3 — Energy Transformation (with friction loss)

Problem Setup

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?

  • m = 500 kg | v₁ = 0 | h₁ = 30 m | v₂ = 20 m/s | h₂ = 0
  • Path distance along track = 30 m (assume slope is steep)
  • Friction present — mechanical energy NOT conserved

Solution

1
Initial Emech = KE₁ + U₁ = 0 + mgh = 500 × 9.8 × 30 = 147 000 J
Total mechanical energy at the start. All PE, no KE (at rest).
2
Final Emech = KE₂ + U₂ = ½ × 500 × 20² + 0 = ½ × 500 × 400 = 100 000 J
Total mechanical energy at the bottom. All KE, no PE (at reference level).
3
Elost = 147 000 − 100 000 = 47 000 J (32% of initial energy)
Energy lost = initial total minus final total. This became thermal energy and sound — not destroyed.
4
Wfriction = F × s → F = Elost / s = 47 000 / 30 = 1567 N
Work done by friction = energy lost. W = Fs → rearrange for F. This is the average resistance force over the path.

What would change if...

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

Problem involves height change Is friction or air resistance present? Any non-conservative force acting No Use cons. KE1+U1=KE2+U2 Yes Not cons. Use W_net=ΔKE Starts from rest? Yes Mass cancels v=√(2gΔh) No Use full equation ½mv₁²+mgh₁ = ½mv₂²+mgh₂ Find E_lost = initial − final E_mech Avg. friction force F = E_lost ÷ s

Copy into your books

Gravitational PE

  • ΔU = mgΔh — vertical height only, not path length
  • PE = 0 at reference level (chosen for convenience)
  • Moving up: Δh positive → ΔU positive (PE increases)
  • Moving down: Δh negative → ΔU negative (PE decreases)

Conservation of Mechanical Energy

  • KE₁ + U₁ = KE₂ + U₂ (frictionless only)
  • Mass cancels → v = √(2gΔh) from rest
  • Speed at bottom depends only on height — not mass
  • Total mechanical energy is constant at every point

Real Systems with Friction

  • KE₁ + U₁ = KE₂ + U₂ + Elost
  • Elost = heat + sound (not destroyed)
  • Find Elost: initial Emech − final Emech
  • Find friction force: F = Elost / s (W = Fs)

When to Use Which Formula

  • No friction → use KE₁ + U₁ = KE₂ + U₂
  • Friction present → use Wnet = ΔKE or find Elost
  • From rest, frictionless → v = √(2gΔh)
  • Always define h = 0 reference level first

🏃 Activities

Activity 01 — Pattern A

Energy Bar Diagram — Rollercoaster Track

Draw PE and KE bar diagrams at five points on a frictionless rollercoaster track.

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):

PointHeight (m)PE (J)KE (J)Speed (m/s)
A — Start50
B — Quarter way down37.5
C — Bottom of drop0
D — Top of next hill30
E — Bottom of next valley10
  1. Complete the table. Use conservation of mechanical energy (frictionless).
  2. Draw side-by-side PE (blue) and KE (green) bar diagrams for each point. Total bar height should be constant.
  3. At which point is the car travelling fastest? At which is it slowest? Explain using energy.
  4. Could the car make it over a hill that is 55 m high? Explain using energy conservation.

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.

Complete the table and bar diagrams in your book
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Activity 02 — Pattern A

Classify: Does Mechanical Energy Conserve?

For each scenario, classify whether mechanical energy is conserved, state which formula to use, and justify your answer.

#ScenarioEmech conserved?Formula to useReason
1Pendulum swinging in vacuum
2Ball rolling down a rough ramp
3Skier on a frictionless icy slope
4Sky diver reaching terminal velocity
5Rollercoaster with friction forces
6Ball thrown vertically upward (no air resistance)
7Car coasting to a stop on flat road
8Water 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.

Complete the table in your book
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✅ Check Your Understanding

Revisit Your Thinking

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.

Annotate your initial prediction in your book
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Revisit Your Initial Thinking

Look back at what you wrote in the Think First section. What has changed? What did you get right? What surprised you?

MC

Multiple Choice

5 random questions from a replayable lesson bank — feedback shown immediately

AnalyseBand 3

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

Answer in your book — show full algebraic working
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ApplyBand 5

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

Answer in your book using the full conservation equation
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EvaluateBand 6

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

Answer in your book — show all four parts
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Comprehensive Answers

Activity 01 — Energy Bar Diagram Table

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.

Activity 02 — Classification

  1. Conserved — no friction in vacuum, only gravity. Use KE₁ + U₁ = KE₂ + U₂.
  2. Not conserved — rough ramp means friction. Use Wnet = ΔKE or find Elost.
  3. Conserved — frictionless ice, only gravity. Use conservation equation.
  4. Not conserved — air resistance acts. At terminal velocity, KE is constant but PE decreases — energy goes to heat via air resistance.
  5. Not conserved — friction forces present. Elost = initial Emech − final Emech.
  6. Conserved — no air resistance stated, only gravity. KE converts to PE on the way up; PE converts back on the way down.
  7. Not conserved — friction (rolling resistance, brakes) converts KE to heat. Final KE = 0 so all mechanical energy is lost.
  8. Not conserved — when water hits the pool, kinetic energy converts to heat, sound, and waves — not recoverable as mechanical energy. Conservation of total energy still holds.

Multiple Choice

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.

Short Answer — Model Answers

Q7 (3 marks):

KE₁ + U₁ = KE₂ + U₂ → 0 + mgh = ½mv² + 0
Divide both sides by m: gh = ½v²
Rearrange: v = √(2gh) — mass has cancelled completely

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):

Reference level: h = 0 at bottom. No friction → use conservation.
KE₁ + U₁ = KE₂ + U₂ → 0 + mgh₁ = ½mv₂² + mgh₂
Cancel m: g × 40 = ½v₂² + g × 12
9.8 × 40 − 9.8 × 12 = ½v₂² → 9.8 × 28 = ½v₂² → v₂² = 548.8 → v₂ = 23.4 m/s

Q9 (4 marks):

(a) sinθ = h/s = 15/60 = 0.25 → cosθ = √(1 − 0.0625) = 0.968. F_N = mg cosθ = 400 × 9.8 × 0.968 = 3794 N. f_k = μ_k × F_N = 0.3 × 3794 = 1138 N
(b) E_lost = f_k × s = 1138 × 60 = 68 280 J
(c) W_net = mgh − E_lost = (400 × 9.8 × 15) − 68 280 = 58 800 − 68 280 = −9480 J
Negative net work means the car would not reach the bottom under these conditions — friction is too large. (If the car does reach, start from v = 0: ½mv² = W_net only if W_net positive.)

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.

🏎️
Speed Race

Gravitational PE and Energy Conservation

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.

Mark lesson as complete

Tick when you have finished all activities and checked your answers.