Ch 7 Work, Energy, and Simple Machines Question Answer Class 9

Welcome to ” Ch 7 Work Energy and Simple Machines Question Answer Class 9“.

Here’s a natural and simple version:

We have written the answers in a way that makes them easy to understand.

Here is what makes this guide different:

  • NCERT Backed: Every single answer includes the exact page and equation number from your official NCERT textbook, so you can cross-verify instantly.
  • Visual Learning: We have added clear, step-by-step diagrams and infographics to help you visualise trickier concepts like changing power, balanced levers, and energy graphs.
  • Quick Revision: For a complete breakdown of the formulas and theories behind these questions, make sure to read our quick notes on this same chapter.

Let’s dive in!

Table of Contents

State whether True or False.


(i) Work is said to be done when a force is applied, even if the object
does not move.
(ii) Lifting a bucket vertically upward results in positive work done
on the bucket.
(iii) The SI unit for both work and energy is joule (J).
(iv) A motionless stretched rubber band has kinetic energy.
(v) Energy can change from one form to another.

(i) FALSE
Work needs BOTH force AND displacement.
No movement = No work done.

(ii) TRUE
(iii) TRUE
(iv) FALSE
A stretched rubber band at rest has Potential Energy
(stored elastic energy), NOT kinetic energy.
Kinetic energy requires motion.

Two-panel educational diagram illustrating potential vs kinetic energy using a rubber band. The left panel shows a person holding a stretched rubber band at rest labeled "Potential Energy (stored elastic energy)". The right panel shows the rubber band being released and moving forward labeled "Kinetic Energy".



(v) TRUE

QuantitySI Unit
WorkJoule (J)
EnergyJoule (J)
PowerWatt (W)
Educational chart from studyless.in showing five examples of energy conversion with colorful icons. The examples are:Food converts to Mechanical energy (muscles).Electrical energy converts to Light (light bulb).Electrical energy converts to Thermal energy (heater).Mechanical energy converts to Sound (bell).Potential energy converts to Kinetic energy (falling object).

Fill in the blanks.


(i) Work done = _ × _ (in the direction of force).
(ii) 1 joule of work is done when a force of ______newton displaces an object by 1 metre in the direction of the force.

(iii) The expression for kinetic energy of a body of mass m and velocity v is_______ .
(iv) The potential energy of an object of mass m at a small height h
from the Earth’s surface is_______ .

(v) Power is defined as the______________at which work is done.

(i)Work done = Force × Displacement (in the direction of force)
(ii)1 joule of work is done when a force of 1 newton displaces an object by 1 metre in the direction of the force.
(iii) The expression for kinetic energy of a body of mass m and velocity v is ½mv²
(iv) The potential energy of an object of mass m at a small height h from the Earth’s surface is mgh
(v) Power is defined as the rate at which work is done.

BlankAnswerFormula
(i)Force × DisplacementW = F × s
(ii)1 newton1 J = 1 N × 1 m
(iii)½mv²K = ½mv²
(iv)mghU = mgh
(v)rateP = W/t

When a ball thrown upwards reaches its highest point, tick which of
the following statement(s) are correct?


(i) The force acting on the ball is zero.
(ii) The acceleration of the ball is zero.
(iii) Its kinetic energy is zero.
(iv) Its potential energy is maximum.

Analysis at the Highest Point:

StatementTrue/FalseReason
(i) Force acting on the ball is zeroFALSEGravity (mg) always acts downward
(ii) Acceleration of the ball is zeroFALSEg = 10 m/s² downward always acts
(iii) Kinetic energy is zeroTRUEKE = ½mv²; v = 0 at top, so KE = 0
(iv) Potential energy is maximumTRUEHeight is maximum, so U = mgh is maximum

Correct answers: (iii) and (iv)

Illustration of a boy throwing a ball vertically upward into the sky, tracking the ball's motion as it rises straight up against a light blue background. Class 9

For each of the following situations, identify the energy transformation
that takes place:

(i) a truck moving uphill,
(ii) unwinding of a watch
spring,
(iii) photosynthesis in green leaves,
(iv) water flowing from
a dam,
(v) burning of a matchstick,
(vi) explosion of a firecracker,
(vii) speaking into a microphone,
(viii) a glowing electric bulb, and
(ix) a solar panel.

Energy from one form to another…”

SituationEnergy Transformation
(i) Truck moving uphillChemical (fuel) → Kinetic + Potential
(ii) Unwinding of a watch springElastic Potential → Mechanical (Kinetic)
(iii) Photosynthesis in green leavesLight → Chemical
(iv) Water flowing from a damPotential → Kinetic → Electrical
(v) Burning of a matchstickChemical → Thermal + Light
(vi) Explosion of a firecrackerChemical → Thermal + Light + Sound
(vii) Speaking into a microphoneSound → Electrical
(viii) A glowing electric bulbElectrical → Light + Thermal
(ix) A solar panelLight → Electrical

Imp – Rule: Energy changes form but is never created or destroyed.

A student is slowly lifted straight up in an elevator from the ground
level to the top floor of a building. Later, the same student climbs the
staircase, all the way to the top. Given that the height of the building is
h = 72.5 m, acceleration due to gravity is g = 10 m s-2, and student’s mass
is m = 50 kg.


(i) Find the gain in the potential energy if the student is lifted straight up
up to the top.
(ii) Find the gain in the potential energy when the student climbs the
stairs to the same top.
(iii) What do you conclude about the dependence of the potential
energy on the path taken?

(i) Potential energy gained in the elevator:

U = mgh = 50 kg × 10 m/s² × 72.5 m = 36,250 J

(ii) Potential energy gained climbing stairs:

U = mgh = 50 kg × 10 m/s² × 72.5 m = 36,250 J

(iii) Conclusion:

Potential energy does NOT depend on the path taken. It depends only on the height gained (h), mass (m), and gravity (g).

Diagram illustrating a student's mass and path to calculate gravitational potential energy. On the left, an elevator lifts a 50 kg student straight up to the top floor of a 72.5-meter-tall building. On the right, the same student climbs a zig-zag staircase to reach the exact same height.

A crane lifts a mass m to the 10th floor of a building in a certain time. It then raises the same mass to the 20th floor of the same building in double the time. How much more energy and power are required? Assume that the height of all floors is equal.

10th Floor20th Floor
Height10H20H
Energy (= mgh)10mgH20mgH
Timet2t
Power (= Energy/Time)10mgH/t20mgH/2t = 10mgH/t

Energy required for 20th floor = 2 × energy for 10th floor (double the energy)

Power required = SAME (the extra height is exactly balanced by double the time)

Simple conclusion:

  1. More energy needed: 2 times more
  2. More power needed: No change (same power)

Which factors determine the energy required to raise a flag from the ground to the top of a tall flagpole using a pulley? Does raising the flag slowly or quickly change the amount of work done? If the speed at which the flag is raised is doubled, how does the power requirement change? Explain your answers.

Factors that determine energy required:

FactorEffect
Mass of flag (m)More mass = More energy
Height of flagpole (h)More height = More energy
Gravity (g)Fixed at ~10 m/s² on Earth

Energy = mgh (speed does NOT affect energy required)

Does raising slowly or quickly change the work done?

No. The work done (energy) is the same regardless of speed. W = mgh in both cases.

If speed is doubled, how does power change?

An educational infographic from studyless.in illustrating how doubling speed affects power when covering the same height.Left Panel (Speed Doubled): Shows a red car with a speedometer accelerating from speed "$v$" to speed "$2v$" to represent "Speed is doubled."Right Panel (Time Halved): Shows a building of height "$h$" alongside two stopwatches. It demonstrates that when lifting an object to the same height at double the speed, the time taken is cut in half (from time "$t$" to time "$t/2$").Bottom Section (Formula & Conclusion): Displays the formula $\text{Power} = \frac{\text{Work}}{\text{Time}}$ to explain that with the same work done in half the time, the power doubles. A green checkmark notes "Same Work, Half Time," leading to a bold conclusion: "POWER DOUBLES" next to a rising bar graph.

Power doubles when speed is doubled.

A man of mass 60 kg rides a scooter of mass 100 kg. He accelerates the scooter to a velocity v. The next day, his son with a mass of 40 kg joins him as a passenger. If the scooter reaches the same speed on both days in the same time interval, what is the ratio of the fuel of the tank used on the two days? Assume that the energy transfer to the scooter happens entirely due to fuel, and no other losses occur due to air resistance and friction.

Since fuel energy converts entirely to kinetic energy:

Day 1: Total mass = 60 + 100 = 160 kg

KE1=½×160×v2=80v2KE₁ = ½ × 160 × v² = 80v²

Day 2: Total mass = 60 + 40 + 100 = 200 kg

KE2=½×200×v2=100v2KE₂ = ½ × 200 × v² = 100v²
Ratio of fuel used=KE1:KE2=80v2:100v2=4:5AnsRatio\ of\ fuel\ used = KE₁ : KE₂ = 80v² : 100v² = 4 : 5 \\ Ans

The family uses more fuel on Day 2 because a greater total mass needs more energy to reach the same speed.

On a seesaw with sliding seats, a child is sitting on one side and an adult on the other side. The adult weighs twice that of the child. The seesaw however is balanced. Draw a figure which depicts this situation showing the distances from the fulcrum where the child and the adult are seated.

Let child’s weight = W, Adult’s weight = 2W

For balance:W×L1=2W×L2L1=2×L2For\ balance: W × L₁ = 2W × L₂ → L₁ = 2 × L₂
An educational diagram illustrating a balanced seesaw with a child and an adult. On the left, a child labeled "CHILD (W)" sits at a distance of "2x" from the center. On the right, an adult labeled "ADULT (2W)" sits at a shorter distance of "x" from the central triangle labeled "FULCRUM".

If the adult sits 1 m from the fulcrum → the child sits 2 m from the fulcrum.

A ball of mass 2 kg is thrown up with a velocity of 20 m s–1.


(i) Identify the sign of the work done by gravity on the ball during its
upward motion and its downward motion.
(ii) If the ball reaches a height of 19.4 m, how much work was done by
air resistance (assume g = 10 m s–2).

(i) Sign of work done by gravity:

PhaseDirection of gravityDirection of motionWork done by gravity
UpwardDownward ↓Upward ↑Negative
DownwardDownward ↓Downward ↓Positive

(ii) Work done by air resistance (ball reaches 19.4 m, g = 10 m/s²):

InitialKE=½×2×202=400 JInitial\\ KE = ½ × 2 × 20² = 400\ J
PEat19.4m=mgh=2×10×19.4=388 J\newline PE \\at \\19.4 m = mgh = 2 × 10 × 19.4 = 388\ J


KE at top = 0 J (ball momentarily at rest)

Using Work-Energy Theorem:

Work done by all forces = Change in KE

Work by gravity (upward)=mgh=388 JWork\ by\ gravity\ (upward) = −mgh = −388\ J


Total work=0400=400 JTotal\ work = 0 − 400 = −400\ J


Work by air resistance=400(388)=12 JWork\ by\ air\ resistance = −400 − (−388) = −12\ J

Air resistance did −12 J of work (it opposes motion, so negative).

A 10.0 kg block is moving on horizontal floor with negligible friction. As shown in the Fig. 7.37, a variable force is applied on the block in its direction of motion from its position at 0 m till 4 m. If the block had a kinetic energy of 180 J when it was at 0 m, find the block’s speed

Q11 class 9 ch 11 A 10.0 kg block is moving on horizontal floor with negligible
friction. As shown in the Fig. 7.37, a variable force is applied
on the block in its direction of motion from its position at
0 m till 4 m. If the block had a kinetic energy of 180 J when
it was at 0 m, find the block’s speed (i) at 0 m, and (ii) at 4 m.
Does the block have negative acceleration in any portion of
its motion?

(i) at 0 m, and

(ii) at 4 m.


Does the block have negative acceleration in any portion of its motion?

(i) Speed at 0 m:

KE=½ mv2KE = ½\ mv²
180=½×10×v2180 = ½ × 10 × v²
v2=36v² = 36
v=6m/sv = 6 m/s

(ii) Speed at 4 m:

From Fig. 7.37 (force-displacement graph), the area under the graph from 0 to 4 m:

  • From 0 to 2 m: triangle with base 2, height 50 N → Area = ½ × 2 × 50 = 50 J
  • From 2 to 3 m: triangle above zero → +25 J
  • From 3 to 4 m: triangle below zero → −25 J

Total work done by force = 50 J

Final KE=180+50=230JFinal\ KE = 180 + 50 = 230 J

½×10×v2=230½ × 10 × v² = 230

v2=46v² = 46

v6.78m/sv ≈ 6.78 m/s

Does block have negative acceleration?

Yes. Between 3 m and 4 m, the force is negative (from graph), meaning the force opposes motion. This causes negative acceleration (deceleration) in that portion.

The gravitational attraction on the surface of the Moon (lunar surface) is about 1/6th of that on the surface of the Earth. An astronaut can throw a ball up to a height of 8 m from the surface of the Earth. How far up will the ball thrown with the same upward velocity travel from the surface of the Moon?

Using conservation of energy:

KE at bottom = PE at top

½ mv2=mgh½\ mv² = mgh

therefore, h = v²/2g

Since the initial velocity (v) is the same on both Earth and Moon:

Height on Earth=v2/(2g)=8mHeight\ on\ Earth = v²/(2g) = 8 m
Height on Moon=v22×g6=6×v22g=6×8=48 m \begin{aligned} \text{Height on Moon} &= \frac{v^2}{2 \times \frac{g}{6}} \\ &= 6 \times \frac{v^2}{2g} \\ &= 6 \times 8 \\ &= 48 \text{ m} \end{aligned}

The ball goes 6 times higher on the Moon because gravity is 6 times weaker.

A 1000 kg car is moving along a road at a constant speed. Suddenly, the driver notices some obstruction ahead and applies the brakes to come to a complete stop. The graphical representation of motion of the car starting from the instant the driver spots the traffic ahead is shown in Fig. 7.38.

13. A 1000 kg car is moving along a road at a constant speed.
Suddenly, the driver notices some obstruction ahead and
applies the brakes to come to a complete stop. The graphical
representation of motion of the car starting from the instant
the driver spots the traffic ahead is shown in Fig. 7.38.
(i) Describe how the car moves between positions A and B.
(ii) Calculate the kinetic energy of the car at A.
(iii) State the work done by the brakes in bringing the car to
a halt between B and C.
(iv) What does the kinetic energy of the car transform into?


(i) Describe how the car moves between positions A and B.
(ii) Calculate the kinetic energy of the car at A.
(iii) State the work done by the brakes in bringing the car to
a halt between B and C.
(iv) What does the kinetic energy of the car transform into?

(i) How car moves between A and B:

The car moves at constant speed (35 m/s). No acceleration. The driver sees the obstruction but hasn’t braked yet (reaction time period).

(ii) Kinetic energy at A:

KE=12mv2=12×1000×352=12×1000×1225=612,500 J \begin{align*} KE &= \tfrac{1}{2} mv^2 \\ &= \tfrac{1}{2} \times 1000 \times 35^2 \\ &= \tfrac{1}{2} \times 1000 \times 1225 \\ &= 612,\!500 \text{ J} \end{align*}

(iii) Work done by brakes (B to C):

At B:
KE = 612,500 J;

At C:
KE = 0 J

Work done by brakes = Change in KE = 0 − 612,500 = −612,500 J

Brakes do negative work of 612,500 J (they oppose motion).

(iv) What does kinetic energy transform into?

KE transforms into thermal energy (heat) due to friction between brake pads and wheels, and between tyres and the road. Some may also convert to sound energy.

The potential energy-displacement graph of a 0.5 kg ball moving along a frictionless track is shown in Fig. 7.39. At O, the velocity of the ball is 0 m s–1 and potential energy is 30 J. Calculate the velocity of the ball at P, Q and R.

14. The potential energy-displacement graph of a 0.5 kg ball
moving along a frictionless track is shown in Fig. 7.39. At O,
the velocity of the ball is 0 m s–1 and potential energy is 30 J.
Calculate the velocity of the ball at P, Q and R.

Since the track is frictionless:

Total mechanical energy = constant = 30 J (at O, all PE)

From Fig. 7.39:

  • At P: PE = 20 J
  • At Q: PE = 30 J
  • At R: PE = 40 J

At P:

KE=3020=10 J12×0.5×v2=10v2=40v=40v6.32 m/s \begin{align*} KE &= 30 – 20 = 10 \text{ J} \\ \frac{1}{2} \times 0.5 \times v^2 &= 10 \\ v^2 &= 40 \\ v &= \sqrt{40} \\ v &\approx 6.32 \text{ m/s} \end{align*}

At Q:

KE=3030=0 Jv=0 m/s(momentarily at rest, like a turning point) \begin{aligned} KE &= 30 – 30 = 0 \text{ J} \\ v &= 0 \text{ m/s} \\ &\quad \text{(momentarily at rest, like a turning point)} \end{aligned}

At R:

KE=3040=10 J KE = 30 – 40 = -10 \text{ J}

Since KE cannot be negative, the ball cannot reach point R. It will turn back before reaching R (it doesn’t have enough energy).

PointPE (J)KE (J)Speed (m/s)
O3000
P2010~6.32
Q3000
R40Cannot reach

A coconut of mass 1.5 kg falls from the top of a coconut tree onto the wet sand on a beach. The height of the tree is 10 m. On impact, the coconut comes to rest by making a depression in the sand.

(i) Calculate the velocity of the coconut just before it hits the sand.
(ii) Assume that the average resistive force of sand is 3000 N and all of
the coconut’s energy is used to create the depression in the sand.
Calculate the depth of the depression the coconut makes in the
sand. Assume g = 10 m s–2.

(i) Velocity just before hitting sand:

Using conservation of mechanical energy:

PE at top = KE at bottom:

mgh=12mv2v2=2ghv2=2×10×10v2=200v=20014.14 m/s \begin{aligned} mgh &= \frac{1}{2} mv^2 \\ v^2 &= 2gh \\ v^2 &= 2 \times 10 \times 10 \\ v^2 &= 200 \\ v &= \sqrt{200} \approx 14.14 \text{ m/s} \end{aligned}

(ii) Depth of depression in sand:

KE just before impact

KE=12mv2=12×1.5×200=150 J \begin{aligned} KE &= \frac{1}{2} mv^2 \\ &= \frac{1}{2} \times 1.5 \times 200 \\ &= 150 \text{ J} \end{aligned}

This energy is used against the resistive force of sand:

Work done by sand = Force × depth

150=3000×dd=1503000=0.05 m=5 cm \begin{aligned} 150 &= 3000 \times d \\ d &= \frac{150}{3000} \\ &= 0.05 \text{ m} \\ &= 5 \text{ cm} \end{aligned}


Bonus: Master Summary Table — All Key Formulas from Chapter 7
ConceptFormulaUnitPage
Work doneW = F × sJoule (J)117
Kinetic EnergyK = ½mv²Joule (J)122
Potential EnergyU = mghJoule (J)125
Mechanical EnergyME = KE + PEJoule (J)126
PowerP = W/tWatt (W)129
Mechanical AdvantageMA = Load/EffortNo unit130
Inclined Plane MAMA = L/hNo unit132
Lever balanceF₁×d₁ = F₂×d₂133

Study Tip:
The single most important idea in this chapter is the Work-Energy Theorem — work done on an object equals the change in its energy. Every question, directly or indirectly, comes back to this one idea.

FAQs: Ch 7 Work Energy and Simple Machines Question Answer Class 9

Please keep your class 9 NCERT textbook, Exploration. You will need it to refer again and again to the below FAQs.

Link to textbooks – NCERT Books class 9

What is the difference between work, energy, and power in science — and why does it matter for Grade 9 exams?

Work and energy share the same unit (Joule), but they are not the same thing. Work is the process of transferring energy. Energy is what an object possesses. Power tells you how fast that transfer happens.
Real-life example from the chapter (Page 129): Carrying your school bag up stairs in 1 minute vs. 5 minutes — same work is done both times, but running up requires MORE power because less time is taken.
Why this matters for exams: Questions frequently test whether students confuse these three. The Work-Energy Theorem (W = ΔE) ties all three together elegantly.

These three terms are related but measure different things:

TermScientific DefinitionFormulaUnit
WorkForce × Displacement in direction of forceW = F × sJoule (J)
EnergyCapacity to do workKE = ½mv² / PE = mghJoule (J)
PowerRate at which work is doneP = W/tWatt (W)
Work Done on Object
Change in Energy of Object
how fast it happens
POWER
Power = Work ÷ Time | Energy change = Work done

When is work done equal to zero? Give three real-life examples with a scientific explanation.

Work is zero in exactly three situations, all following from W = F × s:

SituationWhy Work = ZeroReal Example
Force = 0Nothing to multiply displacement withObject floating in space
Displacement = 0Object doesn’t movePushing a rigid wall
Force ⊥ DisplacementNo component of force in direction of motionCarrying a box while walking horizontally

The wall-pushing paradox (Page 118, Section 7.1.1):

You push a wall hard. You feel tired. Yet science says you did zero work on the wall.

Why? Your muscles expand and contract repeatedly, using your body’s internal energy, which causes fatigue. But the wall didn’t move, so no scientific work was done ON the wall.

The carrying-a-box paradox (Page 118, Section 7.1.1):

A girl carries a box horizontally. She applies force upward (to hold the box). The box moves horizontally. These two directions are perpendicular (90°). Result: zero work done by her holding force on the box.

Force Direction (↑)
90°
Displacement Direction (→)
= ZERO WORK
Work = Force × Displacement × cos(90°) = 0

What is the conservation of mechanical energy, and how does a simple pendulum demonstrate it perfectly?

Conservation of Mechanical Energy states:
The total mechanical energy (KE + PE) of an object remains constant when no external forces (like friction) act on it.
The Pendulum — Nature’s Perfect Demonstration
(Page 127, Section 7.4.3):

Point P (extreme left) Point Q (bottom) Point R (extreme right)
KE = 0 KE = Maximum KE = 0
PE = Maximum (mgh) PE = 0 PE = Maximum (mgh)
ME = mgh ME = mgh ME = mgh
KE = Kinetic Energy  |  PE = Potential Energy  |  ME = Mechanical Energy

Key insight: At every single point of the swing, KE + PE = constant = mgh

Why does a real pendulum eventually stop? Friction at the support and air resistance steal energy away as heat and sound. This does NOT violate conservation of energy — it just means energy converts to other forms.

The slide problem (Example 7.8, Page 128): Using this principle, the speed of a child at the bottom of any slide of height h is:

v = √(2gh)

Three remarkable facts follow:

  1. The mass of the child doesn’t matter.
  2. The shape of the slide doesn’t matter.
  3. Only the HEIGHT matters.

This is why this principle is so powerful — it bypasses all the complicated intermediate steps of motion.

How do simple machines make work easier without reducing the total work done? Explain with a pulley, an inclined plane, and a lever.

The Golden Rule of Simple Machines (Page 135):
Machines do NOT create or reduce energy. They only redistribute force and distance. If force decreases, distance must increase — so total work stays the same.

Work In = Work Out
(ignoring friction)
Force × Distance = CONSTANT
Less Force needed More Distance to cover
Work = Force × Distance

Comparison of Three Simple Machines:

MachineWhat it ChangesMechanical AdvantageReal Examples
Fixed PulleyDirection of force only= 1 (no force reduction)Flag hoisting, wells
Inclined PlaneReduces force needed= L/h (always > 1)Ramps, mountain roads, wheelchair ramps
LeverReduces force OR increases distance= Effort arm / Load armSeesaw, scissors, bottle opener

The Inclined Plane insight (Page 132, Eq. 7.13):

MA = L/h

A ramp that is 50 cm long, lifting something 30 cm high has MA = 50/30 = 1.67. You need only 60% of the force you’d need to lift directly.

The Lever insight (Page 134, Eq. 7.16):

MA = Effort arm / Load arm

Sit farther from the fulcrum on a seesaw → you need less force to lift someone heavier sitting closer.

Three Classes of Levers at a glance:

ClassWhat’s in the MiddleExamples
Class IFulcrumScissors, seesaw, crowbar
Class IILoadBottle opener, wheelbarrow
Class IIIEffortTweezers, broom, hammer

Why perpetual motion machines are impossible (Page 135): Real machines always lose energy to friction as heat. You can never get more work out than you put in. This is non-negotiable physics.

What is the Work-Energy Theorem, and how can it solve problems that Newton’s Laws cannot solve easily?

The Work-Energy Theorem (Page 120, Eq. 7.3):
Work done on an object = Change in its energy
W = ΔKE = ½mv² − ½mu²
Why this theorem is a game-changer:
Newton’s Laws require you to know forces at every instant of motion. The Work-Energy Theorem only needs the starting point and ending point — it skips everything in between.

Newton’s Laws Approach
Find force at every instant
Apply F = ma at each step
Integrate over entire path
Work-Energy Approach
Just compare START and END
W = ΔKE (one equation)
Done in seconds

Proof that KE = ½mv² (Page 122, Section 7.4.1):

Starting from v² = u² + 2as and W = F × s = ma × s:

W = ma × (v² − u²)/2a = ½m(v² − u²)

When u = 0: W = ½mv² = KE gained

Three real problems this theorem solves instantly:

Problem 1 — Aircraft landing (Example 7.6, Page 123):

A jet of 15,000 kg stopped by a wire over 100 m. Find approach speed. → Wire’s work = Change in KE → Solved in 3 lines.

Problem 2 — Escape ramp (Example 7.9, Page 128):

Truck with failed brakes, find the minimum ramp length. → KE of truck = Work by sand + PE gained → 20 m answer.

Problem 3 — Velocity doubling (Example 7.4, Page 122):

If velocity doubles, KE becomes 4 times (because KE ∝ v²).

Velocity changeKE change
×2×4
×3×9
×½×¼

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