๐ผ
7.1 Introduction & Work Done by a Constant Force
In everyday life, we use the word “work” loosely — studying
hard, lifting bags, or running. But in science, work (เคाเคฐ्เคฏ) has a very
precise meaning!
๐ฌ Scientific Definition
of Work
Work is done when a force applied on an object causes the
object to move (displace) in the direction of the force. Both force AND
displacement are needed!
W = F × s
Where: W = Work done (J)
| F = Force applied (N) | s =
Displacement in direction of force (m)
๐
๐ Work ∝
Force AND Work ∝ Displacement
๐ซ When is Work Done ZERO?
- No
force: F = 0 → W = 0 (trivially obvious)
- No
displacement: s = 0 → W = 0. Example: Pushing a rigid wall — no
matter how hard you push, if the wall doesn’t move, W = 0!
- Force
⊥ Displacement: When force and
displacement are perpendicular (90°). Example: Carrying a bag while
walking horizontally — the upward force you apply is perpendicular to
horizontal motion → W = 0 by that force.
⚠️
➕➖ Positive and Negative Work
๐
๐ Force-Displacement
Graph
F(N)s(m)101Area = Work Done= 10 N × 1 m = 10 JWork = area
under F-s graph
Work done = Area under Force-Displacement graph
๐ก
⚡
7.2 The Work-Energy Theorem
When you do work on an object, what happens? The object
gains energy (เคเคฐ्เคा) —
the capacity to do further work. A moving cricket ball hits the wickets. A
flowerpot raised high can damage things below when dropped. Both gained energy
from the work done on them.
Work-Energy Theorem:
Work done on an object = Change in its energy
W = ฮE
๐
๐ฏ Energy Transfers in
Action
- Positive
work done on object → it gains energy
- Negative
work done on object → it loses energy
- Energy
transferred from one object to another during collisions (e.g., carom
striker → white coin → black coin)
๐ฌ
๐
๐
7.3 Forms of Energy
Energy doesn’t exist in just one form — it comes in many
varieties and can convert from one to another!
|
Form of Energy |
Definition |
Example |
|
Mechanical Energy |
Due to motion or position of objects |
Moving car, falling ball |
|
Thermal
(Heat) Energy |
Makes
things warm or hot |
Boiling
water, fire |
|
Light Energy |
Allows us to see |
Sunlight, electric bulb |
|
Sound
Energy |
Vibrations
of air molecules |
Bell
ringing, music |
|
Electrical Energy |
Related to position/motion of charges |
Electric current in wire |
|
Chemical
Energy |
Stored
in chemical bonds of fuels/food |
Food,
petrol, coal |
|
Nuclear Energy |
Stored in nuclei of atoms |
Nuclear reactor, Sun |
๐ Energy Conversions
๐ก
⚙️
7.4 Mechanical Energy — Kinetic & Potential
๐ 7.4.1 Kinetic Energy (เคเคคिเค เคเคฐ्เคा)
The energy possessed by an object due to its motion is
called kinetic energy (KE). Any moving object — a bicycle, a
bullet, a flowing river — has kinetic energy.
Kinetic Energy Formula:
K = ½mv²
๐
Example: An Indian cricketer bowled at 154.8
km/h (≈ 43 m/s). Mass of ball = 0.2 kg. Find KE.
✅ K = 184.9 J
๐ก
๐️ 7.4.2 Potential Energy
(เคธ्เคฅिเคคिเค เคเคฐ्เคा)
The energy stored in an object due to its position
or deformation is called potential energy (PE).
๐ Gravitational Potential
Energy Formula
U = mgh
๐
Example: A fielder threw a cricket ball (0.2 kg)
10 m high in the air (g = 10 m/s²). Find PE at the top.
U = mgh = 0.2 × 10 × 10
✅ U = 20 J
Ground (PE = 0)hBallPE = mghKE = 0PE decreasingKE
increasingPE = 0KE = mgh (max)Total Mechanical Energy = mgh (CONSTANT
throughout!)
Free fall: PE converts to KE, but total mechanical energy
stays the same
♻️
7.4.3 Conservation of Mechanical Energy
Mechanical Energy = Kinetic Energy + Potential
Energy
E_mechanical = KE + PE = ½mv² + mgh = constant
(when no friction or external forces act)
๐
๐ข Understanding
Conservation — Free Fall
|
Position |
Potential Energy |
Kinetic Energy |
Total (ME) |
|
At top (height h) |
mgh |
0 |
mgh |
|
Midway
(height h/2) |
mg(h/2) |
mg(h/2) |
mgh |
|
At ground (height 0) |
0 |
mgh |
mgh |
๐ก Pendulum — Conservation
in Action
A simple pendulum is a perfect example! At the extreme
positions (P and R), the bob has only PE and zero KE. At the bottom (Q), it has
only KE and zero PE. The total energy remains the same throughout!
PQROnly PEKE = 0Only KEPE = 0Only PEKE = 0Total ME =
constant at all points
Simple Pendulum — Conservation of Mechanical Energy
๐ฟ Velocity at Bottom of a
Slide
Using Conservation of Energy: A child slides
down a slide of height h.
✅ v = √(2gh) — velocity depends
ONLY on height, not mass or shape of slide!
⚠️
๐
⚡
7.5 Power (เคถเค्เคคि)
Running up a flight of stairs and walking up slowly — you do
the same work in both cases. But they feel very different!
That difference is described by power (เคถเค्เคคि).
๐
P = W / t
๐ง
๐งฎ Solved Examples
Example 1: A weightlifter lifts 75 kg by 2 m in
5 seconds. Find power (g = 10 m/s²).
✅ Power = 300 W
Example 2: A 1000 kg car accelerates from rest
to 72 km/h (= 20 m/s) in 10 s. Find engine power.
✅ Power = 20,000 W = 20 kW
๐ก
๐ง
7.6 Simple Machines — Pulley, Inclined Plane & Lever
Simple machines help us do work more easily — they can
change the magnitude or direction of the force needed, but
they do NOT reduce the total work done!
Mechanical Advantage (MA) = Load / Effort
๐ก 7.6.1 Pulley (เคिเคฐเคจी)
A pulley is a wheel with a groove that guides a rope. It
changes the direction or magnitude of the applied force.
Fixed Pulley (MA=1)Load↓ EffortDirection changes only
Pulley System (MA>1) Load → Effort Smaller
effort, larger load
Fixed pulley changes direction. Pulley system gives
mechanical advantage > 1
๐ 7.6.2 Inclined Plane (เคเคจเคค เคคเคฒ)
An inclined plane is a ramp that lets you raise a heavy load
to a height using LESS force — but over a LONGER distance.
MA of Inclined Plane = L / h
๐ฃ️
Example: An inclined ramp raises an object over
a 30 cm step. Width of ramp = 40 cm. Find MA.
✅ Mechanical Advantage = 1.67
๐ฉ 7.6.3 Lever (เคเคค्เคคोเคฒเค)
A lever is a rigid bar that can rotate about a fixed point
called the fulcrum (เคเคงाเคฐ
เคฌिंเคฆु).
Levers let you lift heavy loads with a small effort by trading force for
distance.
F₁ × d₁ = F₂ × d₂
MA = Effort Arm / Load Arm
Lever Principle: effort × effort arm =
load × load arm
MA of Lever = Load/Effort = Effort Arm / Load Arm
๐ Three Classes of Levers
|
Class |
Arrangement |
Examples |
MA |
|
Class I |
Fulcrum BETWEEN load and effort |
Scissors, crowbar, seesaw, pliers, balance scale |
Can be >1, =1, or <1 |
|
Class
II |
Load
BETWEEN fulcrum and effort |
Lemon
squeezer, wheelbarrow, bottle opener |
Always
> 1 |
|
Class III |
Effort BETWEEN fulcrum and load |
Tweezers, broom, hammer, oar, tongs |
Always < 1 (speed/distance advantage) |
Seesaw Example: AC = EC = 2 m, BC = DC = 1 m.
Child of 15 kg sits at A. Where should 30 kg child sit?
✅ The 30 kg child should sit at D
(1 m from fulcrum C)
⚠️
๐
๐
Quick Revision Summary
๐
Important Exam Questions with Answers
Q1. Define work. When is work done said to be zero? Give
two examples. (CBSE / 3 Marks)
Work is done when a constant force applied on an object
causes a displacement in the direction of the force. W = F × s. Work is zero
when: (i) displacement is zero — e.g., pushing a rigid wall, (ii) force and
displacement are perpendicular — e.g., carrying a box while walking (upward
force, horizontal displacement).
Q2. Derive the expression for kinetic energy of an object
of mass m moving with velocity v. (CBSE / 3 Marks)
Starting from kinematics: v² = u² + 2as → s = (v²−u²)/2a.
Work done W = F×s = ma × (v²−u²)/2a = ½m(v²−u²). If initial velocity u=0, W =
½mv². By work-energy theorem, this work equals kinetic energy: K = ½mv².
Q3. State the law of conservation of mechanical energy
and verify it for a freely falling body. (CBSE / 5 Marks)
The total mechanical energy (KE + PE) of a system remains
constant if only conservative forces act on it. For a freely falling body of
mass m dropped from height h: At top: PE = mgh, KE = 0, ME = mgh. At midpoint
h/2: PE = mgh/2, v² = 2g(h/2) = gh → KE = ½mv² = mgh/2, ME = mgh. At ground: PE
= 0, v² = 2gh → KE = mgh, ME = mgh. Total ME = mgh at all points. Hence
verified.
Q4. A ball of mass 0.5 kg is thrown upward with velocity
20 m/s. Calculate its (i) KE at the point of throw, (ii) maximum height reached
(g = 10 m/s²). (CBSE / 3 Marks)
(i) KE = ½mv² = ½ × 0.5 × (20)² = ½ × 0.5 × 400 = 100 J.
(ii) At max height, all KE converts to PE: mgh = 100 J → h = 100/(0.5 × 10) =
20 m.
Q5. Explain with an example the three classes of levers.
(CBSE / 3 Marks)
Class I Lever: Fulcrum between load and effort. Example:
Scissors — the pivot (fulcrum) is at the center, hands apply effort, blades
exert force on the load (paper). Class II Lever: Load between fulcrum and
effort. Example: Wheelbarrow — the wheel is the fulcrum, the load sits in the
middle, and hands at the handles apply effort. Class III Lever: Effort between
fulcrum and load. Example: Tweezers — the closed end is the fulcrum, fingers
apply effort at the middle, and the tip grips the load.