Define efficiency as: (a) (%) efficiency = (useful energy output) / (total energy input) (× 100%) (b) (%) efficiency = (useful power output) / (total power input) (× 100%) recall and use these equations

1.7.3 Energy Resources – Efficiency

Learning objectives (Cambridge 0625 wording)

  • State the definition of efficiency of energy transfer and write the two equivalent percentage formulas.
  • Use the formulas to calculate efficiency when energy or power values are given.
  • Interpret typical efficiency ranges for the main energy‑resource conversions listed in the syllabus (chemical, nuclear, hydro‑, wind‑, solar‑, bio‑fuels).
  • Explain the physical reasons for the efficiency of each resource and discuss the associated economic and environmental consequences.
  • Apply the concept of efficiency to exam‑style questions, including interpretation of tables, Sankey diagrams and simple graphs.

Definition and equivalent formulas

Efficiency (\(\eta\)) measures how well a device or system converts the energy (or power) supplied to it into useful output. It is expressed as a percentage.

Energy form

\[

\eta (\%) = \frac{\text{useful energy output}}{\text{total energy input}} \times 100\%

\]

Power form

\[

\eta (\%) = \frac{\text{useful power output}}{\text{total power input}} \times 100\%

\]

Because power is the rate of energy transfer \((P = \Delta E/\Delta t)\), the two equations give identical results.

Why efficiency matters (AO1 & AO2)

  • Cost of energy: Higher efficiency means less fuel or electricity is needed for the same amount of work.
  • Environmental impact: Unused energy is usually dissipated as waste heat, increasing CO₂, NOₓ or other emissions.
  • Design optimisation: Engineers try to maximise \(\eta\) while respecting material limits, safety and economic constraints.

Factors that reduce efficiency (common to all resources)

  • Thermodynamic (heat) losses: Limited by the Carnot efficiency \(\eta{\text{Carnot}} = 1 - \dfrac{T{\text{cold}}}{T_{\text{hot}}}\). Real cycles operate well below this limit.
  • Mechanical losses: Friction in bearings, gearboxes, blade‑tip drag, etc.
  • Electrical losses: Resistive heating in conductors, transformer core losses.
  • Material & conversion limits: Semiconductor band‑gap (PV), turbine blade aerodynamics, combustion completeness.
  • Operational factors: Part‑load operation, temperature, wind speed variability, shading of PV panels.

Typical efficiencies of the main energy‑resource conversions (AO1)

Resource / DeviceTypical efficiency
(% of input energy that becomes useful output)
Units (if applicable)Principal reasons for the range
Coal‑fired power station (steam‑turbine)30 – 38 %Large heat loss in boiler, flue gases and condenser; limited by Carnot cycle.
Natural‑gas combined‑cycle plant55 – 60 %Gas turbine (high‑\(T\)) + steam turbine recovers waste heat; higher \(T_{\text{hot}}\) raises Carnot limit.
Nuclear power station (steam‑turbine)30 – 35 %Thermodynamic cycle similar to coal; heat‑rejection dominates losses.
Hydroelectric dam (turbine‑generator)80 – 90 %Low mechanical friction; most gravitational potential energy is converted to electricity.
Wind turbine (rotor‑generator)30 – 45 %Betz limit (59 % theoretical max) plus gearbox, aerodynamic and electrical losses.
Solar photovoltaic (PV) panel10 – 25 % (commercial); >30 % (research cells)Band‑gap and carrier‑recombination limits; temperature and shading reduce output.
Bio‑fuel (ethanol, biodiesel) in an internal‑combustion engine20 – 30 %Similar thermodynamic cycle to gasoline; fuel quality and combustion efficiency affect range.
Petrol / diesel car (internal‑combustion engine)20 – 30 %Most energy lost as heat through exhaust and cooling system.
Electric motor (appliances, EVs)70 – 95 %DC brushed ≈ 70‑80 %; brush‑less AC or permanent‑magnet motors reach 90‑95 %.

Link to syllabus diagrams (Sankey / flow diagrams)

When drawing a Sankey diagram for a power plant, the width of each arrow represents the amount of energy. The efficiency is the ratio of the width of the “useful output” arrow to the total input width. This visual tool is explicitly required in the syllabus for assessing energy‑resource efficiency.

Worked example – using the energy and power forms (AO2)

A 6 kW electric heater raises the temperature of water. In 50 s it delivers 250 kJ of heat to the water.

  1. Energy form

    \[

    \eta = \frac{E{\text{useful}}}{E{\text{input}}}\times100

    =\frac{250\ \text{kJ}}{(6\ \text{kW}\times50\ \text{s})}\times100

    =\frac{250}{300}\times100 = 83\%

    \]

  2. Power form

    \[

    P{\text{useful}} = \frac{E{\text{useful}}}{t}= \frac{250\ \text{kJ}}{50\ \text{s}} = 5\ \text{kW}

    \]

    \[

    \eta = \frac{P{\text{useful}}}{P{\text{input}}}\times100

    =\frac{5\ \text{kW}}{6\ \text{kW}}\times100 = 83\%

    \]

Both approaches give the same result, confirming the equivalence of the two formulas.

Worked example – coal‑fired power plant (AO2)

Input chemical energy from coal: \(1.0\times10^{9}\ \text{J}\).

Electrical energy generated: \(3.2\times10^{8}\ \text{J}\).

\[

\eta = \frac{3.2\times10^{8}}{1.0\times10^{9}}\times100 = 32\%

\]

Thus 68 % of the coal’s energy is lost as heat in the boiler, flue gases and cooling water – a major source of thermal pollution.

Exam‑style practice (AO2 & AO3)

  1. Incandescent lamp – A 60 W lamp produces 12 W of visible light.

    \[

    \eta = \frac{12}{60}\times100 = 20\%

    \]

    Comment on why the efficiency is low (most energy emitted as infrared heat).

  2. Hydroelectric dam (table interpretation) – The table below shows the energy flow in a dam. Calculate the overall efficiency and state one advantage of this high efficiency.

StageEnergy (×10⁹ J)
Potential energy of water (input)5.0
Mechanical energy at turbine shaft4.5
Electrical energy generated4.2
Transmission losses0.2 (lost)

Solution: \(\eta = \dfrac{4.2}{5.0}\times100 = 84\%\). High efficiency reduces fuel‑equivalent cost and limits environmental impact.

  1. Car comparison (graph interpretation) – The graph below shows primary‑energy input (MJ) versus distance travelled for a gasoline car (25 % η) and an electric car (90 % η, electricity generated at 60 % η). Which vehicle uses less primary energy to travel 100 km? Explain, including the effect of the electricity‑generation stage.

Solution sketch (students should draw a bar chart):

Gasoline car: useful work = 100 km × energy per km; primary input = useful work / 0.25.

Electric car: useful work / 0.90 (motor) then divided by 0.60 (generation) → overall η = 0.54. Hence the electric car needs roughly half the primary energy of the gasoline car.

  1. Bio‑fuel engine – Useful work = 2.5 MJ, fuel energy input = 10 MJ.

    \[

    \eta = \frac{2.5}{10}\times100 = 25\%

    \]

    Compare with a typical diesel engine (≈ 30 %) and comment on why the difference is small.

Practical measurement of efficiency (AO3)

  • Laboratory set‑up: Use a calorimeter to measure the heat absorbed by water (ΔT) and a voltmeter/ammeter to record electrical input.

    \[

    \eta = \frac{m c \Delta T}{V I t}\times100

    \]

  • Key sources of error: Heat loss to surroundings, inaccurate timing, voltage drop in wires.
  • Students can relate this experiment to the definition of efficiency and to the real‑world losses discussed earlier.

Key take‑away (AO1)

Efficiency is a percentage that tells us how much of the supplied energy (or power) is turned into useful output. The two formulas – based on energy or on power – are mathematically identical. Knowing typical efficiency ranges, the physical reasons behind them, and being able to calculate and interpret efficiency are essential skills for the IGCSE 0625 exam and for evaluating real‑world energy systems.

Suggested diagram: A Sankey flow‑chart showing energy input → useful output → waste losses for a generic power plant (chemical, nuclear, or renewable).