Work, Energy, and Power

W = Fs cos θ; KE, GPE, EPE; conservation of energy; P = Fv; efficiency

# Work, Energy, and Power — IB Physics

The concepts of work, energy, and power provide a powerful alternative to Newton's laws for solving mechanics problems, particularly where forces vary or where we don't need to know about individual forces.


1. Work Done

W=Fscosθ\boxed{W = Fs\cos\theta}

  • WW = work (J)
  • FF = force (N)
  • ss = displacement (m)
  • θ\theta = angle between FF and ss

Work is a scalar. 1 J = 1 N·m.

If θ=90°\theta = 90°: W=0W = 0 (force perpendicular to motion).

2. Kinetic Energy

KE=12mv2KE = \frac{1}{2}mv^2

Work-Energy Theorem

Wnet=ΔKEW_{\text{net}} = \Delta KE

The net work done on an object equals its change in kinetic energy.

3. Gravitational Potential Energy

ΔGPE=mgΔh\Delta GPE = mg\Delta h

4. Elastic Potential Energy

EPE=12ke2EPE = \frac{1}{2}ke^2

Where kk = spring constant, ee = extension/compression.

5. Conservation of Energy

Total energy is conserved in an isolated system.

With only conservative forces: KEi+PEi=KEf+PEfKE_i + PE_i = KE_f + PE_f

With friction/drag: KEi+PEi=KEf+PEf+WfrictionKE_i + PE_i = KE_f + PE_f + W_{\text{friction}}

6. Power

P=Wt=ΔEtP = \frac{W}{t} = \frac{\Delta E}{t}

For constant force and velocity: P=FvP = Fv

Units: watts (W).

7. Efficiency

η=useful output energy/powertotal input energy/power×100%\eta = \frac{\text{useful output energy/power}}{\text{total input energy/power}} \times 100\%

Worked Example: Example 1

Problem

A 60 kg skier descends 200 m vertically. Starting from rest, find speed at bottom if friction does 30 kJ of work.

mgh=12mv2+Wfmgh = \frac{1}{2}mv^2 + W_f 60(9.81)(200)=12(60)v2+3000060(9.81)(200) = \frac{1}{2}(60)v^2 + 30000 117720=30v2+30000117720 = 30v^2 + 30000 v=87720/30=2924=54.1v = \sqrt{87720/30} = \sqrt{2924} = 54.1 m/s

Solution

Worked Example: Example 2

Problem

A 1500 kg car at 30 m/s: engine power 50 kW, drag force 1200 N.

Driving force: F=P/v=50000/30=1667F = P/v = 50000/30 = 1667 N Net force: 16671200=4671667 - 1200 = 467 N Acceleration: a=467/1500=0.311a = 467/1500 = 0.311 m/s²

Max speed (when Fdrive=FdragF_{\text{drive}} = F_{\text{drag}}): vmax=P/Fdrag=50000/1200=41.7v_{\max} = P/F_{\text{drag}} = 50000/1200 = 41.7 m/s

Solution

Worked Example: Example 3

Problem

A motor lifts a 500 kg load 20 m in 30 s. Efficiency is 75%. Find input power.

Useful output: W=mgh=500(9.81)(20)=98100W = mgh = 500(9.81)(20) = 98100 J Output power: Pout=98100/30=3270P_{\text{out}} = 98100/30 = 3270 W Input power: Pin=3270/0.75=4360P_{\text{in}} = 3270/0.75 = 4360 W

Solution

9. Practice Questions

    1. A 50 N force pulls a box 10 m at 30° to the horizontal. Calculate the work done. (2 marks)
    1. A 2 kg mass falls 5 m from rest. Find its speed just before hitting the ground (ignore air resistance). (2 marks)
    1. A pump raises 200 kg of water per minute through 15 m. Calculate the minimum power. (3 marks)
    1. A car engine has 40% efficiency and burns fuel at 0.004 kg/s (fuel energy = 45 MJ/kg). Find the useful power. (3 marks)

    Answers

    1. W=50(10)cos30°=433W = 50(10)\cos30° = 433 J.

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Summary

  • W=FscosθW = Fs\cos\theta; work-energy theorem: Wnet=ΔKEW_{\text{net}} = \Delta KE
  • Conservation: KEi+PEi=KEf+PEf+WfrictionKE_i + PE_i = KE_f + PE_f + W_{\text{friction}}
  • P=W/t=FvP = W/t = Fv
  • Efficiency = useful output / total input × 100%

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