Work Energy and Power Class 11 Notes | Formulas, Numericals & PYQs

Work, Energy and Power Class 11 Notes – Complete NEET Physics Guide
NEET Physics Class 11 – Chapter 5 Work, Energy and Power

Work, Energy and Power Class 11 Notes – Complete NEET Physics Guide

These Work, Energy and Power class 11 notes are crafted for NEET aspirants who need conceptual depth, exam-focused formulas, and zero wasted effort. Every time you push a box, lift a book, or ride a bicycle, the physics of this chapter is at work. While kinematics described how objects move and Laws of Motion explained why they move, this chapter quantifies the energy exchange behind every physical interaction. With 2–3 direct questions appearing in NEET every year from Work, Energy and Power, mastery of this chapter is non-negotiable for a top Physics score.

01

Concept of Work – Force, Displacement and the Angle Between Them

In physics, work has a precise meaning that differs from everyday usage. Work is done only when a force causes a displacement in the object on which it acts. Holding a heavy bag stationary — however tiring — does zero work in the physics sense.

Work Done by a Constant Force
W = F · s · cosθ
W = F⃗ · s⃗   (dot product form)
[SI Unit: Joule (J) = N·m]

The angle θ is between the force vector and the displacement vector. This angle is the most commonly mishandled element in NEET work problems.

Angle (θ) cos θ Work Done Example
+1 Positive (maximum) Pushing a box in the direction of motion
90° 0 Zero Normal force on a horizontally moving object
180° −1 Negative (maximum magnitude) Friction opposing sliding motion
NEET Trap
Gravity does zero work on a horizontally moving object. Gravity does negative work when an object moves upward. Both are tested frequently in assertion-reason and statement-based MCQs.
02

Work Done by a Variable Force

When force changes with displacement, the simple formula W = Fs cosθ cannot be directly applied. Instead, the work done is calculated as the area under the Force-Displacement (F-x) graph.

Work by Variable Force
W = ∫ F · dx   (from x₁ to x₂)
Graphically: W = Area under F-x curve

Spring Force – The Classic Variable Force

The spring force follows Hooke’s Law: F = –kx, where k is the spring constant and x is the extension or compression. The work done in stretching a spring from natural length is:

W_spring = ½kx²
This equals the elastic potential energy stored in the spring.
Graph Interpretation Tip
In NEET, F-x graphs appear as triangles, trapezoids, or irregular shapes. Calculate the area systematically — triangular area = ½ × base × height. Negative area means negative work done by that force.
03

Kinetic Energy and the Work-Energy Theorem

Kinetic energy is the energy possessed by a body by virtue of its motion. It depends on both the mass and the square of the speed — making speed the dominant factor.

Kinetic Energy
KE = ½mv²
KE = p²/2m   (in terms of momentum p = mv)
[KE is always positive — a scalar quantity]

Work-Energy Theorem

The net work done on an object by all forces equals the change in its kinetic energy. This is one of the most powerful shortcuts in Work, Energy and Power class 11 problem-solving — it bypasses the need to find acceleration and use kinematics separately.

W_net = ΔKE = KE_final – KE_initial = ½mv² – ½mu²
  • If W_net is positive → object speeds up (KE increases)
  • If W_net is negative → object slows down (KE decreases)
  • If W_net is zero → speed remains constant (KE unchanged)
Exam Strategy
Whenever a problem gives you initial and final speeds and asks for the net work done — apply the Work-Energy Theorem directly. It is significantly faster than resolving forces and applying kinematics step by step.
04

Potential Energy – Stored Energy and Conservative Forces

Potential energy is energy stored in a system due to the position or configuration of its components. It is always defined relative to a reference point and is associated exclusively with conservative forces.

Types of Potential Energy
Gravitational PE: U = mgh
Elastic PE (spring): U = ½kx²
Relation with force: F = –dU/dx

Conservative vs Non-Conservative Forces

Property Conservative Force Non-Conservative Force
Work depends on path? No – path-independent Yes – path-dependent
Work in closed loop Zero Non-zero
Potential energy defined? Yes No
Examples Gravity, spring force, electrostatic Friction, air resistance, viscosity
Key Distinction
Potential energy can only be defined for conservative forces. Friction is a non-conservative force — energy lost to friction is converted to heat and cannot be recovered as mechanical energy.
05

Conservation of Mechanical Energy

The total mechanical energy of a system — the sum of kinetic and potential energy — remains constant when only conservative forces act on it. This is the Law of Conservation of Mechanical Energy, one of the most frequently applied principles in Work, Energy and Power class 11 notes.

Conservation of Mechanical Energy
KE + PE = constant (only conservative forces)
½mv₁² + mgh₁ = ½mv₂² + mgh₂
ΔKE + ΔPE = 0   →   ΔKE = –ΔPE

Free Fall – The Classic Demonstration

A ball dropped from height h has maximum PE and zero KE at the top. As it falls, PE converts to KE. Just before hitting the ground, all energy is kinetic. At any intermediate height h’, using conservation:

v = √(2g(h – h’)) at height h’ above the ground
v = √(2gh) just before hitting the ground
When Conservation Fails
If friction or air resistance is present, mechanical energy is not conserved. The energy dissipated as heat equals the work done by friction: W_friction = –f × d. Total energy (mechanical + thermal) is always conserved — mechanical energy alone is not.
06

Power – The Rate of Doing Work

Power measures how quickly work is done. Two machines doing the same amount of work differ in power if they take different amounts of time — the faster one has more power. This concept is central to engineering and real-world physics applications.

Power Formulas
Average Power: P = W/t
Instantaneous Power: P = F · v · cosθ = F⃗ · v⃗
[SI Unit: Watt (W) = J/s]
1 horsepower (hp) = 746 W
  • Instantaneous power = dot product of force and velocity vectors
  • For a vehicle moving at constant velocity on a rough road: P = f_friction × v
  • Efficiency η = (useful power output / total power input) × 100%
Common Error
Students often confuse power with force. A feather and a boulder falling from the same height gain the same speed (ignoring air resistance), but the boulder requires far more power from any machine to lift it to that height in the same time — because W = mgh is larger for the boulder.
07

Collisions – Elastic, Inelastic and the Coefficient of Restitution

A collision is a short-duration interaction between two bodies during which they exert large forces on each other. Momentum is always conserved in collisions (no external net force on system). Kinetic energy conservation depends on the type of collision.

Property Elastic Collision Inelastic Collision Perfectly Inelastic
Momentum conserved? Yes Yes Yes
KE conserved? Yes No (partially lost) No (maximum loss)
Bodies stick together? No No Yes
Example Billiard balls, molecular collisions Most real-world collisions Bullet embedding in a block
Elastic Collision – 1D (equal masses, m₁ = m₂)
After collision: v₁’ = 0   and   v₂’ = u₁
Velocities exchange completely — the striking object stops,
the struck object moves with the initial velocity of the striker.

Coefficient of Restitution: e = (v₂’ – v₁’) / (u₁ – u₂)
e = 1 (elastic)  |  e = 0 (perfectly inelastic)  |  0 < e < 1 (inelastic)
NEET PYQ Pattern
Perfectly inelastic collision problems — where a bullet embeds into a block on a surface — appear almost every alternate year. Use momentum conservation to find final velocity, then use Work-Energy Theorem to find displacement against friction.

Maximum KE Loss in Inelastic Collision

KE_loss = ½ × (m₁m₂)/(m₁+m₂) × (u₁ – u₂)²
Maximum when bodies stick together (perfectly inelastic).
08

Numerical Framework – Step-by-Step Problem Approach

NEET problems in Work, Energy and Power follow predictable patterns. Use this structured approach to eliminate errors and save time under exam pressure.

  1. Identify all forces acting on the object (gravity, friction, applied, spring, normal)
  2. Check if conservation of energy applies — are all forces conservative?
  3. If yes, apply: KE₁ + PE₁ = KE₂ + PE₂
  4. If friction present, use: KE₁ + PE₁ = KE₂ + PE₂ + |W_friction|
  5. For power problems, first find work done, then divide by time (or use P = Fv)
  6. For collisions, always apply momentum conservation first, then energy conservation if elastic
With friction on a surface (block sliding distance d):
½mv₁² + mgh₁ = ½mv₂² + mgh₂ + μmg cosθ × d

Spring-block system (block compresses spring by x):
½mv² = ½kx²   →   v = x√(k/m)
09

Conceptual Practice Questions – Test Your Understanding

  1. A person carrying a heavy load walks on a horizontal road. How much work does the normal force from the ground do on the person?
  2. A body is moved along a closed loop by a conservative force. What is the net work done?
  3. Two objects of equal mass collide head-on elastically, one initially at rest. What are the final velocities?
  4. A spring is compressed by x₁ and then by 2x₁. Compare the work done in the two cases.
  5. A car engine applies force F and the car moves at constant velocity v on a rough road. What is the power of the engine?
  6. A ball is thrown upward with velocity v. At what height is the kinetic energy equal to the potential energy?
  7. In a perfectly inelastic collision, is it possible for all the kinetic energy to be lost? Under what conditions?
10

PYQ Trends – What NEET Actually Asks from This Chapter

NEET Pattern – Most Repeated

Work-Energy Theorem applied to a block on a rough inclined plane or horizontal surface — find final speed or stopping distance. Almost guaranteed every year in some form.

NEET Pattern – Energy Conservation

Free fall, pendulum, or spring-block problems using conservation of mechanical energy. One question nearly every year — straightforward but requires clean formula application.

NEET Pattern – Collisions

Perfectly inelastic collision (bullet-block), or elastic collision with equal masses. Question may involve finding velocity, height reached after collision, or maximum compression of spring.

NEET Pattern – Power

A vehicle of given mass accelerates from rest — find power at a given speed, or time to reach a given speed given constant power. Appears roughly every alternate year.

NEET Pattern – Variable Force (F-x Graph)

Area under F-x graph to find work done — often a trapezoidal or triangular graph. Tests conceptual understanding of integration without requiring calculus knowledge.

Revision Priority
For NEET, focus on: Work-Energy Theorem with friction, elastic and perfectly inelastic collisions, conservation of mechanical energy in spring-block and free-fall systems, and the power formula P = Fv.
11

Formula Summary – Quick Revision Sheet for Work, Energy and Power

Work, Energy and Power – All Key Formulas

  • Work by constant force: W = Fs cosθ
  • Work by variable force: W = area under F-x graph = ∫F dx
  • Kinetic energy: KE = ½mv² = p²/2m
  • Work-Energy Theorem: W_net = ΔKE = ½mv² – ½mu²
  • Gravitational PE: U = mgh
  • Elastic PE (spring): U = ½kx²
  • Spring force: F = –kx (Hooke’s Law)
  • Conservation: KE₁ + PE₁ = KE₂ + PE₂ (conservative forces only)
  • Average power: P = W/t
  • Instantaneous power: P = Fv cosθ
  • Efficiency: η = (P_output / P_input) × 100%
  • Coefficient of restitution: e = (v₂’ – v₁’) / (u₁ – u₂)
  • KE loss in perfectly inelastic collision: ½(m₁m₂)/(m₁+m₂) × (u₁–u₂)²
  • Potential energy and force: F = –dU/dx
12

Common Mistakes and Conceptual Traps

Mistake The Correct Understanding
Assuming work is always positive Work is a scalar but can be negative. Friction and opposing gravity both do negative work on a moving object.
Ignoring the angle θ in W = Fs cosθ Always identify the angle between force and displacement vectors — not the angle the force makes with horizontal (unless displacement is horizontal).
Applying KE = ½mv² with wrong v v is the speed of the object, not its component. Use the resultant speed, not just the horizontal or vertical component.
Momentum not conserved in inelastic collision Momentum is ALWAYS conserved in any collision (elastic or inelastic) when no external net force acts. Only KE may not be conserved.
Confusing average power and instantaneous power Average power = total work / total time. Instantaneous power = F·v at that specific moment. For constant force and velocity, both are equal.
Applying energy conservation when friction is present When friction acts, total mechanical energy is not conserved. Subtract work done by friction: KE₁ + PE₁ = KE₂ + PE₂ + |W_friction|.
13

Frequently Asked Questions – Work, Energy and Power Class 11

What is the Work-Energy Theorem and why is it useful in NEET? +
The Work-Energy Theorem states that the net work done on an object equals its change in kinetic energy: W_net = ΔKE = ½mv² – ½mu². Its power in NEET problems lies in bypassing force resolution and kinematics. Whenever you know initial and final speeds, or need to find work done against friction, this theorem gives the answer in a single step without needing acceleration or time.
Why is work zero even when force is applied in some cases? +
Work is zero when: (1) there is no displacement — for example, pushing a wall, (2) the force is perpendicular to displacement — for example, the normal force on a horizontally sliding block, or (3) the displacement is zero even if force is applied — for example, a stationary object under any force. All three scenarios satisfy W = Fs cosθ = 0 through different mechanisms.
Is momentum conserved in all types of collisions? +
Yes. Momentum is conserved in all collisions — elastic, inelastic, and perfectly inelastic — provided there is no net external force on the system during the collision. This follows directly from Newton’s Third Law: the internal forces of the collision are equal and opposite, so total momentum of the system remains unchanged. Kinetic energy, however, is only conserved in elastic collisions.
What is the difference between elastic potential energy and gravitational potential energy? +
Gravitational PE (U = mgh) is stored due to the position of an object in a gravitational field — it depends on height above a reference level. Elastic PE (U = ½kx²) is stored in a deformed elastic body (spring, rubber band) due to its configuration. Both are forms of potential energy associated with conservative forces, and both are fully recoverable as kinetic energy when the system returns to its reference state.
How many questions from Work, Energy and Power appear in NEET? +
Typically 2 to 3 questions from Work, Energy and Power appear in NEET Physics annually. These usually include one conceptual question (work done by specific forces, energy conservation concept) and one or two numerical problems (collision, spring-block, work against friction, power of an engine). The chapter is consistently high-yield and should be thoroughly prepared, including F-x graph interpretation and collision types.
Can kinetic energy ever be negative? +
No. Kinetic energy is always non-negative. KE = ½mv², and since m is always positive and v² is always non-negative (the square of any real number), KE is always greater than or equal to zero. KE = 0 only when the object is at rest. If a calculation yields negative KE, there is an error in the problem setup or arithmetic.

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Table of Contents — Physics Class 11

Table of Contents

Physics — Class 11

01Units and MeasurementsGo to page
02Motion in a Straight LineGo to page
03Motion in a PlaneGo to page
04Laws of MotionGo to page
05Work, Energy and PowerGo to page
06System of Particles and Rotational MotionGo to page
07GravitationGo to page
08Mechanical Properties of SolidsGo to page
09Mechanical Properties of FluidsGo to page
10Thermal Properties of MatterGo to page
11ThermodynamicsGo to page
12Kinetic TheoryGo to page
13OscillationsGo to page
14WavesGo to page

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