Work, Energy and Power

Physics · Class 11

Lesson 10 of 10 · 17 min

Chapter review

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Must-know facts

18 facts

  1. 1W = F·d = Fd cos θ; zero when force and displacement are perpendicular.
  2. 2Work by friction on a sliding body and by gravity on a rising body is negative.
  3. 31 kWh = 3.6 × 10⁶ J; 1 eV = 1.6 × 10⁻¹⁹ J; 1 erg = 10⁻⁷ J; 1 hp = 746 W.
  4. 4Work-energy theorem: W_net = ΔK, valid for constant and variable forces.
  5. 5K = ½mv² = p²/2m; K ∝ p² for fixed mass.
  6. 6A rise of x% in momentum raises K by ((1 + x/100)² − 1) × 100%.
  7. 7Work by a variable force = area under the F-x graph.
  8. 8Conservative force: path-independent work, zero work round a closed path; F = −dV/dx.
  9. 9Friction and air resistance are non-conservative.
  10. 10Gravitational PE near the surface = mgh; spring PE = ½kx².
  11. 11Mechanical energy is conserved only when non-conservative forces do no work.
  12. 12Stopping distance on a rough floor d = v²/(2μ_k g), independent of mass.
  13. 13Vertical circle on a string: minimum speed √(5gL) at the bottom and √(gL) at the top.
  14. 14P = dW/dt = F·v.
  15. 15Momentum is conserved in all collisions; kinetic energy only in elastic ones.
  16. 16Equal masses in a 1D elastic collision exchange velocities.
  17. 17Fraction of KE transferred by m₁ to m₂ (at rest) in a 1D elastic collision = 4m₁m₂/(m₁ + m₂)².
  18. 18Perfectly inelastic collision gives the largest KE loss; bodies move together afterwards.

Common traps

Where marks are lost

Writing W = Fd when the force acts at an angle to the displacement.

Always include cos θ, where θ is the angle between force and displacement: W = Fd cos θ.

Using mgh = ½mv² when part of the path is rough.

Subtract the work done against friction: mgh − W_friction = ½mv² at the end. On a horizontal rough stretch of length d, W_friction = μ_k m g d.

Assuming that if momentum rises by 30% then kinetic energy rises by 30%.

K = p²/2m, so K scales with p²: (1.3)² = 1.69, a 69% rise.

Believing each body keeps its own kinetic energy in an elastic collision.

Only the total kinetic energy is the same before and after; energy is transferred from one body to the other.

Thinking kinetic energy is conserved at every instant during an elastic collision.

During contact some kinetic energy is stored as deformation energy; it is fully returned only once the bodies separate.

Treating the kilowatt hour as a unit of power.

kWh = power × time, so it measures energy: 1 kWh = 3.6 × 10⁶ J.

Forgetting efficiency in pump or motor questions, or dividing the wrong way.

Input power = useful output power ÷ efficiency; input is always the larger number.

Assigning potential energy to friction.

Potential energy exists only for conservative forces. Work done by friction depends on the path, so it cannot be written as a change of a position function.

Taking the potential energy of a spring as ½kx when finding its maximum compression.

Spring potential energy is ½kx²; the maximum compression from speed v is x_m = v√(m/k).

Formulas

16 to know

Scalar product

A·B = AB cos θ = AxBx + AyBy + AzBz

θ is the angle between A and B.

Work by a constant force

W = F·d = Fd cos θ

SI unit joule (N m).

Work by a variable force

W = ∫ F(x) dx from x_i to x_f

Area under the F-x graph.

Kinetic energy

K = ½mv² = p²/2m

Always ≥ 0.

Work-energy theorem

K_f − K_i = W_net

W_net includes work by every force, conservative or not.

Conservative force from potential energy

F(x) = −dV/dx

One-dimensional form.

Gravitational potential energy near the surface

V(h) = mgh

h measured from the chosen zero level.

Conservation of mechanical energy

K_i + V_i = K_f + V_f

Only when conservative forces alone do work.

Spring force (Hooke's law)

F_s = −kx

k in N m⁻¹.

Spring potential energy

V(x) = ½kx²

Same for extension and compression x.

Work by a spring

W_s = −½k(x_f² − x_i²)

Negative when the spring is stretched further.

Power

P_av = W/t; P = dW/dt = F·v

1 W = 1 J s⁻¹; 1 hp = 746 W.

Efficiency

η = useful output power / input power

Always less than 1 in practice.

1D elastic collision, m₂ initially at rest

v₁f = (m₁ − m₂)v₁ᵢ/(m₁ + m₂); v₂f = 2m₁v₁ᵢ/(m₁ + m₂)

Momentum and total KE both conserved.

Completely inelastic collision, m₂ at rest

v = m₁v₁ᵢ/(m₁ + m₂); ΔK = ½[m₁m₂/(m₁ + m₂)]v₁ᵢ²

Bodies stick together; ΔK is the kinetic energy lost.

Vertical circle on a string

v_bottom(min) = √(5gL); v_top(min) = √(gL)

L is the string length.

Key terms

14 terms

Scalar product
A product of two vectors that gives a scalar, AB cos θ.
Work
The product of a force and the component of displacement along it.
Joule
The work done when a force of 1 N moves its point of application 1 m along the force.
Kinetic energy
The energy a body has because it is moving, ½mv².
Work-energy theorem
The net work done on a body equals the change in its kinetic energy.
Potential energy
Stored energy that depends on the position or configuration of a system.
Conservative force
A force whose work between two points does not depend on the path taken.
Non-conservative force
A force, such as friction, whose work depends on the path and which reduces mechanical energy.
Mechanical energy
Kinetic energy plus potential energy of a system.
Spring constant
The force per unit extension of a spring; a measure of its stiffness.
Power
Work done, or energy transferred, per unit time.
Elastic collision
A collision in which total kinetic energy after impact equals that before.
Inelastic collision
A collision in which some kinetic energy is converted to other forms.
Completely inelastic collision
An inelastic collision in which the bodies move together after impact.
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