Year 11 Physics Module 2: Dynamics 25 min Lesson 8 of 15

Power

An athlete and a walker climb the same stairs. They do the same work. But the athlete does it in 4 seconds — the walker takes 40. Same energy, very different power.

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Think First

A 70 kg athlete sprints up a 5 m staircase in 4 seconds. A 70 kg person walks up the same staircase in 40 seconds. Who does more work? Who is more powerful? Are the answers to these two questions the same?

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Formula Reference — This Lesson

$P = \Delta E/\Delta t$  |  $P = Fv\cos\theta$
P = power (W = J/s)  |  ΔE = energy transferred (J)  |  Δt = time (s) F = force (N)  |  v = velocity (m/s)  |  θ = angle between F and v
Lifting vertically: $P = mgh/\Delta t$   |   Find F from P and v: $F = P/v$ (when $\theta = 0°$)   |   Units: 1 kW = 1000 W

P=Fv
Formula Reference — Power

$P = \Delta E/\Delta t$
Average Power
P = power (W) | ΔE = energy transferred or work done (J) | Δt = time taken (s)
Applies when: total energy transferred and total time are known. Use for average power over an interval.
Common trap: ΔE must include ALL energy transferred — work against gravity, friction, air resistance. Using only one component gives a partial answer.
$P = Fv\cos\theta$
Instantaneous Power
P = power (W) | F = force (N) | v = velocity (m/s) | θ = angle between force and velocity vectors
Applies when: force and velocity are known at a specific instant. For horizontal motion with horizontal force, θ = 0° so P = Fv.
Common trap: At constant velocity, use Fdrive = Fresistance (Newton 1) first — then P = Fdrive × v. Do not use mass × g as the force unless lifting vertically.
$P = mgh/\Delta t$
Power Lifting Against Gravity
Derived from P = W/Δt = mgh/Δt. Only valid for purely vertical lifting.
Applies when: lifting an object vertically at constant speed (or finding average power over a vertical lift)
Common trap: Only accounts for work against gravity — ignores any horizontal motion or friction. For a runner going upstairs, this underestimates total power.
1 W = 1 J/s
Unit of Power
Watt (W) = joule per second. 1 kilowatt (kW) = 1000 W. 1 megawatt (MW) = 10⁶ W.
Common usage: car engines rated in kW, power stations in MW, human muscles in W
Common trap: W for watts and W for work (joules) use the same letter. Context and units distinguish them — power answers in W (watts), energy/work answers in J (joules).

Know

  • P = ΔE/Δt — average power definition
  • P = Fv cosθ — power from force and velocity
  • P = mgh/Δt — shortcut for vertical lifting
  • Unit: watt (W) = joule per second (J/s)

Understand

  • Why power and work are different quantities
  • Why P = Fv at constant velocity uses driving force = resistance force
  • Why power increases as speed increases at constant force
  • Why the same work can be done at different power levels

Can Do

  • Calculate average power from work and time
  • Calculate power at constant velocity using P = Fv
  • Calculate power lifting against gravity
  • Identify which power formula applies in a given context

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

Misconceptions to Fix

Wrong: Action and reaction forces cancel each other out on the same object.

Right: Action-reaction pairs act on DIFFERENT objects, so they never cancel; this is why motion occurs.

01Power — P = ΔE/Δt

Power — P = ΔE/Δt

Power is not about how much energy you use — it is about how fast you use it. A slow engine and a fast engine can do the same work; the fast one is more powerful.

Power is the rate of energy transfer — the amount of energy transferred per unit time. Its SI unit is the watt (W), where 1 W = 1 J/s.

Back to the staircase: both the athlete and the walker climb the same 5 m height at 70 kg. Both do W = mgh = 70 × 9.8 × 5 = 3430 J of work against gravity. But:

Athlete P = ΔE/Δt = 3430/4 = 857.5 W
Walker P = ΔE/Δt = 3430/40 = 85.75 W

Same work done. Athlete is 10× more powerful — because they do it 10× faster.
Approximate Power Output
~70 W
~700–1000 W
~400 W sustained
~80–150 kW
~200 MW
~2000 MW (2 GW)
Note
Mechanical power output
Short bursts only
~5–6 W/kg body mass
Peak power at high RPM
Per turbine unit
Total electrical output
02Power from Force and Velocity — P = Fv cosθ

Power from Force and Velocity — P = Fv cosθ

At constant velocity, the engine's power output tells you exactly how hard it is fighting all the resistances — because the driving force exactly equals the total resistance.

Derivation

Starting from P = W/Δt and W = Fs cosθ:

$$P = \frac{W}{\Delta t} = \frac{Fs\cos\theta}{\Delta t} = F \cdot \frac{s}{\Delta t} \cdot \cos\theta = Fv\cos\theta$$ For horizontal force and horizontal motion: $\theta = 0°$, $\cos 0° = 1$, so $P = Fv$
Power at Constant Velocity — P = Fdrive × v

Power vs Speed at Constant Resistance

Speed (m/s)Resistance force (N)Power required (W)Power in kW
108008 0008 kW
2080016 00016 kW
3080024 00024 kW
4080032 00032 kW

Notice: doubling speed doubles the power required to maintain constant velocity against the same resistance. This is why highway driving consumes significantly more fuel than city driving even at constant speed.

Vector Protocol — power problems at constant velocity
Step 1 — Is velocity constant? If yes, apply Newton 1: Fdrive = Fresistance
Step 2 — Identify the angle between force and velocity (usually 0° for horizontal motion)
Step 3 — Apply P = Fv cosθ and state answer in watts (W) or kilowatts (kW)
03Power in Real-World Contexts

Power in Real-World Contexts

Every time something moves against a resistive force — gravity, friction, air resistance — energy is being transferred at a rate measured in watts.

Uniformly accelerated motion

Formula to use: P = Fv (instantaneous) or P = W/Δt (average)
Key feature: If F is constant and v increases, P = Fv increases — power is not constant during acceleration
Example: Car engine accelerating from 0 to 30 m/s — power output increases as speed rises

Lifting against gravity

Formula to use: P = mgh/Δt
Key feature: All work done against gravity — PE increases at rate P
Example: Construction crane lifting 500 kg load 20 m in 40 s: P = 500×9.8×20/40 = 2450 W

Against air resistance and rolling resistance

Formula to use: P = Fdrag × v
Key feature: All power output goes to overcoming resistance at constant v
Example: Cyclist at 10 m/s with 80 N drag: P = 800 W. Crouch → reduce drag → less power needed
Why cyclists crouch Air resistance force scales approximately with v², making it the dominant resistance at high speeds. Crouching reduces the frontal area, which reduces the drag force. Since P = Fdrag × v, reducing Fdrag directly reduces the power needed to maintain any given speed — this is why professional cyclists maintain a low aerodynamic position throughout a race.

Common Misconceptions

More powerful means more force.
Power depends on both force AND velocity — P = Fv. A small electric motor running at high speed can have more power than a large crane moving slowly. High force at low speed and low force at high speed can produce identical power outputs.
Power is constant during acceleration.
If a constant force is applied during acceleration, v increases, so P = Fv increases continuously. Power output grows as the object speeds up. Only at constant velocity is the instantaneous power constant (assuming constant resistance).
W in watts and W for work are the same thing.
W as a symbol means watts (the unit of power). W as a variable means work done (measured in joules). They are completely different quantities. Always check context and units — "P = 500 W" means 500 watts; "W = 500 J" means 500 joules of work.
Interactive: Power Output Comparator
Interactive: Power — P = F × v (3D)
Worked Example 1 Type 4 — Power

Problem Setup

Problem type: Type 4 — Power. Vertical lifting against gravity.

Scenario: A 65 kg athlete runs up a 4 m high flight of stairs in 3.2 s. Calculate the average power output against gravity.

  • m = 65 kg | h = 4 m | Δt = 3.2 s
  • Work against gravity only (as stated)
  • Use P = mgh/Δt

Solution

1
W = mgh = 65 × 9.8 × 4 = 2548 J
Work done against gravity — all of this energy goes into gravitational PE.
2
P = W/Δt = 2548/3.2 = 796 W
Average power = total energy transferred divided by time. Units: J/s = W.
3
P ≈ 796 W (about 0.8 kW)
For context: this is about 10× a person's resting metabolic rate and only sustainable for short bursts.

What would change if...

The athlete's actual total power output is greater than 796 W — why? Name at least two other forms of energy expenditure not accounted for in this calculation.

Worked Example 2 Type 4 — Power

Problem Setup

Problem type: Type 4 — Power at constant velocity. Find driving force from Newton 1, then apply P = Fv.

Scenario: A car travels at constant 30 m/s. The total resistive force is 800 N. Calculate: (a) the engine's driving force, (b) the engine's power at this speed, (c) the power output if speed increased to 40 m/s with the same resistive force.

  • v = 30 m/s (constant)
  • Fresistance = 800 N
  • Constant velocity → Newton 1 applies

Solution

1
Constant v → Newton 1: Fnet = 0 → Fdrive = Fresistance = 800 N
At constant velocity there is no acceleration, so all forces balance. Fdrive exactly cancels Fresistance.
2
(a) Fdrive = 800 N
Already found in Step 1.
3
(b) P = Fdrive × v = 800 × 30 = 24 000 W = 24 kW
P = Fv with θ = 0° (horizontal force, horizontal motion). Convert to kW for clarity.
4
(c) P = 800 × 40 = 32 000 W = 32 kW
Same resistance force, higher speed → higher power. 33% speed increase → 33% power increase (linear relationship when F is constant).

What would change if...

If the car accelerates from 30 m/s to 40 m/s with the engine still supplying the same 800 N driving force, is the power output constant, increasing, or decreasing during the acceleration? Use P = Fv to explain what happens as v changes.

Power problem Is it a vertical lifting problem? Yes P = mgh ÷ t No Is work or energy given directly? Yes P = W ÷ t No Is velocity constant? Yes Newton 1: F_drive=F_resist No — P = Fv·cosθ P = Fv cosθ — state answer in watts

Copy into your books

Power Formulae

  • P = ΔE/Δt — average power from energy and time
  • P = Fv cosθ — instantaneous power from force and velocity
  • P = mgh/Δt — lifting against gravity (vertical only)
  • Unit: watt (W) = joule per second (J/s)

Constant Velocity Key Step

  • Constant v → Newton 1 → Fdrive = Fresistance
  • Then P = Fdrive × v
  • Doubling v doubles P (if Fresist unchanged)
  • θ = 0° for horizontal force and horizontal motion

Power During Acceleration

  • If F is constant and v increases: P = Fv increases
  • Power is NOT constant during acceleration
  • Use P = W/Δt for average power over an interval
  • Use P = Fv for instantaneous power at a given speed

Key Vocabulary

  • Power: rate of energy transfer (W = J/s)
  • Work: total energy transferred (J) — not a rate
  • Average power: total energy ÷ total time
  • Instantaneous power: power at a specific moment
Activity 01 — Pattern B

Power Comparison Table

Complete the table by identifying the correct formula, calculating power, and expressing in appropriate units.

#ScenarioFormulaWorkingPower (W or kW)
1Person runs up stairs: m = 70 kg, h = 3 m, Δt = 2.5 s
2Crane lifts 800 kg load 15 m in 60 s
3Car at constant 25 m/s, Fresistance = 600 N
4Cyclist at constant 12 m/s, Fdrag = 90 N
5Motor does 50 000 J of work in 25 s
6Pump lifts 200 kg of water 8 m per minute

Type your working for each row here. Complete the table in your book.

Complete the table in your book showing the formula and full working for each row.

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Activity 02 — Pattern B (Error-spot)

Find and Fix the Errors

A student's power calculation contains four deliberate errors. Identify each, explain why it is wrong, and write the correct working.

Problem A 1200 kg car travels at constant 20 m/s. The total resistance force is 500 N. Calculate the engine's power output.

Student's working (contains 4 errors):

"The car is at constant speed, so it is in equilibrium.
The driving force equals the car's weight: Fdrive = mg = 1200 × 9.8 = 11 760 N
Power = F × v = 11 760 × 20 = 235 200 W
Converting to kW: 235 200 W ÷ 100 = 2352 kW
Therefore the engine's power output is 2352 kW."

For each error: (a) identify what is wrong, (b) explain why using physics reasoning, (c) write the correct version.

Type your error analysis below — find all four.

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Revisit Your Thinking

Earlier you were asked: Who does more work — the athlete or the walker? Who is more powerful? Are these the same question?

The answers: both do exactly the same work — W = mgh = 70 × 9.8 × 5 = 3430 J. Work depends only on force and displacement, not time. But the athlete is 10× more powerful — Pathlete = 3430/4 = 857.5 W vs Pwalker = 3430/40 = 85.75 W.

The two questions have different answers because work and power are fundamentally different quantities. Work measures the total energy transferred. Power measures the rate. You can do the same work at any power level — it just takes longer at lower power. This distinction matters enormously in engineering: a 100 W motor and a 10 000 W motor can both lift the same load to the same height, but the powerful one does it 100 times faster.

Look back at your initial prediction. What did you get right? What changed?

Annotate your initial prediction in your book with what you now understand.

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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

UnderstandBand 3

7. Explain the difference between work and power, using the staircase example from the lesson. Include numerical values in your explanation. 3 MARKS

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ApplyBand 5

8. A cyclist travels at constant 8 m/s against a total resistance of 120 N. (a) Calculate the cyclist's power output. (b) Using the same power output, calculate how long it would take the cyclist to climb a 60 m vertical hill (assume all power goes against gravity, m = 75 kg). 3 MARKS

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EvaluateBand 6

9. A car engine has a maximum power output of 150 kW. At a constant highway speed of 110 km/h, the total resistive force acting on the car is 1200 N. (a) Calculate the engine's power output at this speed. (b) Calculate the reserve power available. (c) If the driver uses the full engine power at 110 km/h, explain what would happen to the car's motion and why — use Newton's Second Law in your answer. 4 MARKS

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Comprehensive Answers

Activity 01 — Power Table

  1. P = mgh/Δt = 70×9.8×3/2.5 = 2058/2.5 = 823.2 W
  2. P = mgh/Δt = 800×9.8×15/60 = 117 600/60 = 1960 W = 1.96 kW
  3. Constant v → Fdrive = 600 N. P = Fv = 600×25 = 15 000 W = 15 kW
  4. Constant v → Fdrive = 90 N. P = Fv = 90×12 = 1080 W = 1.08 kW
  5. P = ΔE/Δt = 50 000/25 = 2000 W = 2 kW
  6. 200 kg per 60 s, h = 8 m. P = mgh/Δt = 200×9.8×8/60 = 15 680/60 = 261.3 W

Activity 02 — Four Errors

Error 1 — Used weight instead of resistance force: At constant velocity, the driving force equals the resistance force (500 N) — not the weight. Newton 1 states Fnet = 0, so Fdrive = Fresistance = 500 N. The car's weight acts vertically and is irrelevant to horizontal power calculations on a flat road.

Error 2 — Correct power calculation using wrong force: P = F × v = 500 × 20 = 10 000 W = 10 kW. The student's P = 235 200 W is wrong because Fdrive was wrongly taken as mg.

Error 3 — Wrong conversion to kW: The student divided by 100 instead of 1000. 1 kW = 1000 W, not 100 W. Correct conversion: 10 000 W ÷ 1000 = 10 kW.

Error 4 — Stated conclusion using incorrect value: The final answer of 2352 kW flows from all previous errors. The correct answer is 10 kW — a 150 kW car engine provides ample reserve power above this at 20 m/s.

Multiple Choice

1. B — 300 W. P = ΔE/Δt = 6000/20 = 300 W. Option A (120 000 W) multiplies instead of dividing.

2. C — 25 000 W. P = Fv = 1000 × 25 = 25 000 W = 25 kW.

3. A — 1 watt = 1 joule per second. Option D (1000 J/s) describes a kilowatt, not a watt.

4. D — 1058.4 W. P = mgh/Δt = 90×9.8×6/5 = 5292/5 = 1058.4 W. Option C (882 W) uses g = 9.8 but Δt incorrectly. Option B (540 W) uses incorrect formula.

5. B — P = Fv. If F is constant and v increases, P increases proportionally. A constant force does NOT produce constant power during acceleration.

6. C — Work done by both = mgh = 100×9.8×10 = 9800 J. Motor A: P = 9800/20 = 490 W. Motor B: P = 9800/5 = 1960 W = 4× Motor A. Same work, different power, different time. Option A is wrong — work done is the same for both (only energy transferred depends on force and displacement, not time).

Short Answer — Model Answers

Q7 (3 marks): Work is the total energy transferred by a force through a displacement — it depends only on the force and the distance moved, not on time. Power is the rate of doing work — the amount of energy transferred per second. In the staircase example, both the athlete and walker climb the same 5 m at 70 kg, doing the same work: W = mgh = 70 × 9.8 × 5 = 3430 J. However the athlete (Δt = 4 s) has power P = 3430/4 = 857.5 W, while the walker (Δt = 40 s) has P = 3430/40 = 85.75 W — 10× less. Same work, very different power.

Q8 (3 marks):

(a) Constant v → Newton 1 → F_drive = F_resist = 120 N. P = F_drive × v = 120 × 8 = 960 W
(b) P = mgh/Δt → Δt = mgh/P = (75 × 9.8 × 60) / 960 = 44 100 / 960 = 45.9 s

Q9 (4 marks):

(a) 110 km/h = 110/3.6 = 30.56 m/s. At constant v: F_drive = F_resist = 1200 N. P = 1200 × 30.56 = 36 667 W ≈ 36.7 kW
(b) Reserve power = 150 kW − 36.7 kW = 113.3 kW available for acceleration
(c) At full power (150 kW) at v = 30.56 m/s: F_drive_new = P_max/v = 150 000/30.56 = 4908 N. F_net = F_drive_new − F_resist = 4908 − 1200 = 3708 N (forward). By Newton 2: F_net = ma > 0, so the car accelerates forward. The car is no longer at constant velocity — it speeds up until either the driver reduces power back to 36.7 kW to maintain 110 km/h, or the car reaches a new higher constant speed where P = 150 kW exactly balances resistance at that speed.
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