CBSE • Class 11 • Physics
Work, Energy and Power
Work-energy theorem, power, collisions, and conservation ideas.
Chapter 5
Verified Curriculum Topic
What is Work, Energy and Power?
Work-energy theorem, power, collisions, and conservation ideas.
Work, Energy and Power matters because it connects theory, equations, and real physical behaviour. At Class 11 level, students are typically expected to explain concepts precisely, apply laws correctly, and interpret numerical or experimental questions with confidence.
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Summary
The One Thing
Work describes energy transfer by a force through displacement; the net work changes an object’s kinetic energy. Conservation of energy and momentum then provides the framework for analysing power, mechanical-energy changes and collisions.
Reactions, Processes and Experiments
| What happens | Equation or process | What you observe | Type |
|---|---|---|---|
| A constant force acts through a displacement. | W = F s cos theta | Work depends on the force component parallel to the displacement. | Work by a constant force |
| A variable force acts through a displacement. | W = integral F dot dr | Work is represented by the area under a force-displacement graph. | Work by a variable force |
| A force has a component in the direction of displacement, such as gravity acting on a falling object. | Positive work | The object’s kinetic energy increases when the net work is positive. | Positive work |
| A force has a component opposite to displacement, such as friction acting on a moving block. | Negative work | The object’s kinetic energy decreases when the net work is negative. | Negative work |
| There is no displacement, or the force is perpendicular to displacement, as for centripetal force in uniform circular motion. | Zero work | No energy is transferred by that force through displacement. | Zero work |
| The net work done on an object changes its kinetic energy. | W_net = Delta K = K_f - K_i | Positive net work increases kinetic energy; negative net work decreases it. | Work-energy theorem |
| The work-energy theorem is written using initial and final speeds. | W_net = Delta K = 1/2 m(v^2 - u^2) | The change in kinetic energy is determined by the change in speed. | Work-energy theorem |
| An object possesses energy because it is moving. | K = 1/2 mv^2 | Kinetic energy increases with the square of speed. | Kinetic energy |
| An object stores energy because of its position near Earth’s surface. | U = mgh | The energy depends on mass, height and the chosen reference level, where U = 0. | Gravitational potential energy |
| A spring is extended or compressed. | U = 1/2 kx^2 | Energy is stored in the spring; it depends on the spring constant and the extension or compression. | Elastic potential energy |
| Kinetic and potential energies are combined. | E = K + U | Mechanical energy is the sum of kinetic and potential energy. | Mechanical energy |
| Only conservative forces act. | K_i + U_i = K_f + U_f | The total mechanical energy remains constant. | Conservation of mechanical energy |
| A conservative force acts between two positions. | Work depends only on the initial and final positions, not on the path followed. | Work done around a closed path is zero. | Conservative force |
| A non-conservative force acts along a path. | Work depends on the path followed. | Mechanical energy is transferred into other forms; friction commonly produces heat. | Non-conservative force |
| The conservative force is related to potential energy in one dimension. | F = -dU/dx | The force acts in the direction of decreasing potential energy. | Force-potential-energy relation |
| Kinetic friction acts on a moving object. | Work done by kinetic friction generally depends on the path length. | The work is generally negative and mechanical energy is converted into heat. | Work by friction |
| A normal force acts perpendicular to displacement. | No work is done when the normal force is perpendicular to displacement. | The normal force does no work in this case. | Work by a normal force |
| A surface or point of contact moves while a normal force acts. | A normal force can do work if the surface or point of contact is moving. | Energy transfer by the normal force may occur. | Work by a normal force |
| Work is completed or energy is transferred over a time interval. | P_avg = W/t | Greater work in the same time, or the same work in less time, means greater average power. | Average power |
| Work or energy transfer is considered at an instant. | P = dW/dt = F dot v | Instantaneous power depends on force and velocity. | Instantaneous power |
| Energy or work is measured in SI units. | 1 J = 1 N m | The joule is the SI unit of work and energy. | SI unit of work and energy |
| Power is measured in SI units. | 1 W = 1 J/s | The watt is the SI unit of power. | SI unit of power |
| Electrical energy is expressed in commercial units. | 1 kWh = 3.6 x 10^6 J | A kilowatt-hour measures energy, not power. | Energy unit |
| Energy changes form within an isolated system. | Energy is neither created nor destroyed, but it may be transferred or transformed. | The total energy of the isolated system remains constant. | Conservation of energy |
| Objects undergo a short-duration interaction involving large forces. | A collision is a short-duration interaction during which momentum is exchanged. | The objects experience large interaction forces over a short time. | Collision |
| Objects collide in an isolated system with no external net force. | p_initial = p_final | Total linear momentum before and after the collision is the same. | Momentum conservation |
| Momentum conservation follows from Newton’s laws when external impulse is absent. | The net external impulse on the system is zero. | The system’s total momentum remains constant. | Momentum conservation |
| Two objects stick together after impact. | v = (m_1u_1 + m_2u_2)/(m_1 + m_2) | The objects move together with a common velocity; kinetic-energy loss is maximum for the given initial conditions. | One-dimensional perfectly inelastic collision |
| Both momentum and total kinetic energy remain constant during impact. | Momentum and total kinetic energy are conserved. | No kinetic energy is converted into heat, sound or deformation in the ideal model. | Elastic collision |
| Momentum remains constant but kinetic energy does not. | Some initial kinetic energy changes into heat, sound, deformation, or other forms of energy. | Momentum is conserved, while total kinetic energy decreases. | Inelastic collision |
| The relative speeds of two colliding objects are compared along the line of impact. | e = relative speed of separation / relative speed of approach | The coefficient characterises the separation relative to the approach. | Coefficient of restitution |
Key Terms
- Work: Energy transferred when a force produces displacement. For a constant force,
W = F s cos theta, wherethetais the angle between force and displacement. - Positive Work: Work done when a force has a component in the direction of displacement, such as gravity acting on a falling object.
- Negative Work: Work done when a force has a component opposite to displacement, such as friction acting on a moving block.
- Zero Work: Work done when there is no displacement or when the force is perpendicular to displacement, as in uniform circular motion for centripetal force.
- Kinetic Energy: Energy possessed by an object because of its motion:
K = 1/2 mv^2. - Potential Energy: Stored energy due to position or configuration. Near Earth’s surface, gravitational potential energy is
U = mgh. - Work-Energy Theorem: The net work done on an object equals its change in kinetic energy:
W_net = Delta K = K_f - K_i. - Conservative Force: A force whose work depends only on the initial and final positions, not on the path followed. Gravitational and elastic forces are examples.
- Non-Conservative Force: A force whose work depends on the path. Friction is a common example because it converts mechanical energy into heat.
- Mechanical Energy: The sum of kinetic and potential energies:
E = K + U. - Conservation of Mechanical Energy: When only conservative forces act, the total kinetic and potential energy remains constant:
K_i + U_i = K_f + U_f. - Power: The rate at which work is done or energy is transferred. Average power is
P_avg = W/t; instantaneous power isP = dW/dt = F dot v. - Collision: A short-duration interaction between objects during which large forces act and momentum is exchanged.
- Momentum Conservation: In an isolated system with no external net force, total linear momentum remains constant:
p_initial = p_final. - Elastic Collision: A collision in which both momentum and total kinetic energy are conserved.
- Inelastic Collision: A collision in which momentum is conserved but kinetic energy is not conserved.
- Perfectly Inelastic Collision: A collision in which the objects stick together after impact. Momentum is conserved, but kinetic-energy loss is maximum for the given initial conditions.
- Coefficient of Restitution: The ratio of relative speed of separation to relative speed of approach along the line of impact:
e = relative speed of separation / relative speed of approach.
Easily Confused
- Positive work vs negative work: Positive work has a force component in the direction of displacement; negative work has a component opposite to displacement.
- Zero work vs negative work: Zero work occurs when displacement is absent or the force is perpendicular to it; negative work occurs when the force opposes displacement.
- Work vs power: Work measures energy transferred; power measures the rate at which the transfer occurs.
- Conservative force vs non-conservative force: Conservative-force work is path-independent and is zero around a closed path; non-conservative-force work depends on path.
- Mechanical-energy conservation vs total-energy conservation: Mechanical energy remains constant only when non-conservative forces do no net work, whereas total energy remains conserved because energy may be transferred or transformed.
- Momentum conservation vs kinetic-energy conservation: Momentum is conserved in an isolated collision, but kinetic energy is conserved only in an elastic collision.
- Elastic collision vs inelastic collision: Both involve momentum conservation in an isolated system, but only an elastic collision conserves total kinetic energy.
- Inelastic collision vs perfectly inelastic collision: In every perfectly inelastic collision the objects stick together; ordinary inelastic collisions need not have this outcome.
- Average power vs instantaneous power: Average power is
P_avg = W/tover a time interval; instantaneous power isP = dW/dt = F dot vat a particular instant. - Joule vs watt: A joule measures work or energy, whereas a watt measures power;
1 W = 1 J/s. - Kinetic energy vs momentum: Kinetic energy is a scalar,
K = 1/2 mv^2; momentum is conserved in isolated collisions and is represented byp_initial = p_final.
What Gets Asked
- Calculate the work done by a constant force using
W = F s cos theta; marks are lost by using the full force instead of its component along the displacement. - Determine whether work is positive, negative or zero in situations involving gravity, friction, centripetal force or a normal force; the key distinction is the angle between force and displacement.
- Apply the work-energy theorem using
W_net = Delta K = 1/2 m(v^2 - u^2); the common error is confusing net work with the work done by one individual force. - Use
K_i + U_i = K_f + U_ffor systems involving gravitational or elastic potential energy; this equation applies only when non-conservative forces do no net work. - Compare processes or machines using
P_avg = W/torP = dW/dt = F dot v; completing the same work in less time means greater power, not greater work. - Analyse collisions using momentum conservation and identify whether kinetic energy is also conserved; momentum conservation alone does not establish that a collision is elastic.
Flashcards
Quick quiz
Which expression gives the work done by a constant force?
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What is Work, Energy and Power in CBSE Class 11 Physics?
Work-energy theorem, power, collisions, and conservation ideas.
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