IC engine performance and combustion basics

Indicated, brake and friction power, mean effective pressure, mechanical, thermal and volumetric efficiencies, bsfc, Morse test, air–fuel ratio and SI/CI combustion and knock, with engine-test examples.

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Why it matters

Engine test beds, emission calibration and gensets all come down to a handful of numbers: brake power, mean effective pressure, specific fuel consumption and the efficiencies linking them. A mechatronics engineer working on engine control units, dynamometers or hybrid powertrains reads these numbers daily. Combustion basics — air–fuel ratio, knock, ignition delay — explain why the controller does what it does with spark timing, injection timing and boost.

Key ideas

Power terms.

  • Indicated power (IP): power developed by the gas on the pistons, from the indicator (p–V) diagram.
  • Brake power (BP): power at the crankshaft, measured with a dynamometer from torque and speed.
  • Friction power (FP) = IP − BP: bearing and piston-ring friction, valve train, pumping losses and accessories. Found by a Morse test (multi-cylinder engines), a Willan's line (fuel-rate plot extrapolated to zero load, CI engines), motoring, or IP − BP.

Mean effective pressure. Indicated MEP is the constant pressure that, acting over each power stroke, gives IP; brake MEP (bmep) gives BP. bmep is the best size-independent measure of how hard an engine works: about 8–12 bar for naturally aspirated SI engines and 15–25 bar for turbocharged diesels.

Efficiencies.

  • Mechanical η_m = BP/IP (typically 0.75–0.90 at full load, falling at part load because friction stays roughly constant).
  • Brake thermal η_bth = BP / (ṁ_f × CV); indicated thermal η_ith = IP / (ṁ_f × CV); η_bth = η_m × η_ith.
  • Relative (efficiency) ratio = η_ith / η_air-standard.
  • Volumetric η_v = actual air inducted ÷ air that would fill the swept volume at ambient (or intake) density. It governs the maximum power of a naturally aspirated engine; turbo- or supercharging raises it above 1.

Specific fuel consumption. bsfc = ṁ_f / BP, in kg/kWh or g/kWh; it is inversely proportional to η_bth. Typical: SI ≈ 250–300 g/kWh, CI ≈ 190–230 g/kWh.

Heat balance. Fuel energy goes to brake power, cooling water, exhaust gas, and unaccounted losses (radiation, friction heat). A typical petrol engine: about 25–30 % BP, 30 % coolant, 30–35 % exhaust.

Combustion basics.

  • Stoichiometric air–fuel ratio: the exact air needed for complete combustion. About 14.7:1 for petrol and 14.5:1 for diesel by mass. Equivalence ratio φ = (F/A)_actual / (F/A)_stoich; φ > 1 is rich, φ < 1 is lean.
  • SI combustion: spark → ignition lag (flame kernel) → turbulent flame propagation → afterburning. Timing is set so peak pressure occurs about 10–15° after TDC (MBT timing).
  • SI knock: auto-ignition of the unburnt end gas ahead of the flame, producing pressure waves and the "pinging" sound. Promoted by high compression ratio, advanced spark, high intake temperature and low-octane fuel. Resisted by high octane number, retarded spark and a compact chamber. Do not confuse with pre-ignition, ignition by a hot spot before the spark.
  • CI combustion: fuel injected into hot compressed air → ignition delay → rapid (premixed) combustion → controlled (diffusion) combustion → after-burning. Diesel knock comes from too long a delay: fuel accumulates, then burns all at once. It is reduced by a high cetane number, higher compression ratio and higher intake temperature — the opposite of SI knock remedies.
  • Exhaust emissions: CO and HC from rich or incomplete combustion; NOx from high peak temperatures; soot (PM) from rich zones in diesel sprays. A three-way catalyst needs φ ≈ 1, which is why closed-loop lambda control exists.

Formulas

BP = 2π N T / 60 — W; N in rpm, T (torque) in N·m. IP = p_mi L A n K — W; p_mi: indicated MEP (Pa), L: stroke (m), A: piston area (m²), n: power strokes per second per cylinder (N/60 for two-stroke, N/120 for four-stroke), K: number of cylinders. The same form with bmep gives BP. FP = IP − BP η_m = BP / IP η_bth = BP / (ṁ_f CV) — ṁ_f in kg/s, CV: calorific value (kJ/kg), BP in kW. bsfc = ṁ_f / BP — kg/kWh when ṁ_f is in kg/h and BP in kW. η_bth = 3600 / (bsfc × CV) — bsfc in kg/kWh, CV in kJ/kg. η_v = ṁ_a / (ρ_a V_s n_i) — ṁ_a: air mass flow (kg/s), ρ_a: ambient air density (kg/m³), V_s: total swept volume (m³), n_i: intake strokes per second (N/120 for a four-stroke engine). V_s = (π/4) D² L K — total swept volume (m³), D: bore (m). IP (Morse test) = K × BP_all − Σ BP_(cylinder i cut) φ = (F/A)_actual / (F/A)_stoich

Worked examples

Example 1 (standard, engine test). A four-cylinder four-stroke petrol engine (bore 80 mm, stroke 90 mm) gives 120 N·m at 3000 rpm and uses 9 kg/h of petrol (CV = 44 000 kJ/kg) and 140 kg/h of air (ambient density 1.18 kg/m³). Find BP, bmep, bsfc, η_bth, η_v and the air–fuel ratio.

  1. BP = 2π N T / 60 = 2π × 3000 × 120/60 = 37 699 W = 37.70 kW.
  2. V_s = (π/4) D² L K = 0.7854 × 0.08² × 0.09 × 4 = 1.8096 × 10⁻³ m³.
  3. Cycles per second = N/120 = 25. bmep = BP/(V_s × 25) = 37 699/(1.8096 × 10⁻³ × 25) = 833 300 Pa = 8.33 bar.
  4. bsfc = ṁ_f / BP = 9/37.70 = 0.2387 kg/kWh.
  5. η_bth = 3600/(bsfc × CV) = 3600/(0.2387 × 44 000) = 0.343.
  6. Swept-volume air rate = 1.8096 × 10⁻³ × 25 = 0.04524 m³/s; actual = (140/3600)/1.18 = 0.03296 m³/s; η_v = 0.03296/0.04524 = 0.729.
  7. A/F = 140/9 = 15.6 (slightly lean of stoichiometric 14.7).

BP ≈ 37.7 kW, bmep ≈ 8.33 bar, bsfc ≈ 0.239 kg/kWh, η_bth ≈ 34.3 %, η_v ≈ 72.9 %, A/F ≈ 15.6

Example 2 (GATE level, Morse test). A four-cylinder engine gives 30 kW with all cylinders firing at constant speed. With cylinders 1, 2, 3 and 4 cut out in turn (speed restored each time), BP is 21.2, 21.0, 21.4 and 21.6 kW. Find IP and η_m.

  1. IP of cylinder i = BP_all − BP_(i cut): 8.8, 9.0, 8.6 and 8.4 kW.
  2. IP = K × BP_all − Σ BP_cut = 4 × 30 − (21.2 + 21.0 + 21.4 + 21.6) = 120 − 85.2 = 34.8 kW.
  3. η_m = BP / IP = 30/34.8 = 0.862; FP = 4.8 kW.

IP = 34.8 kW, η_m ≈ 86.2 %

Example 3 (stoichiometric A/F of octane). C₈H₁₈ + 12.5 (O₂ + 3.76 N₂) → 8 CO₂ + 9 H₂O + 47 N₂.

  1. Air per kmol fuel = 12.5 × 4.76 = 59.5 kmol × 28.97 kg/kmol = 1723.7 kg.
  2. Fuel = 8 × 12.011 + 18 × 1.008 = 114.2 kg.
  3. A/F = 1723.7/114.2 = 15.1.

(A/F)_stoich ≈ 15.1 (commercial petrol, a blend, is about 14.7)

Common mistakes

  • Using N instead of N/2 power strokes for a four-stroke engine in IP = p_m L A n K.
  • Mixing kW and W, or kg/h and kg/s, in bsfc and η_bth.
  • Calling knock "premature combustion". SI knock is auto-ignition of the end gas after the spark; pre-ignition is a separate problem.
  • Applying SI knock remedies (lower r, lower intake temperature) to diesel knock, which needs the opposite.
  • Using air–fuel ratio by volume (moles) when the question means by mass.
  • Ignoring that mechanical efficiency drops sharply at part load.

For GATE ME

Questions are usually short numericals: BP from torque and speed, IP and bmep from cylinder geometry, η_m, η_bth, bsfc, η_v, Morse test, and stoichiometric air–fuel ratios from a fuel formula. Conceptual questions test knock in SI and CI engines, octane and cetane numbers, and the effect of operating variables. Practise one compact test-data problem that chains all of these, keeping units explicit.

Quick check

  1. An engine delivers 50 N·m at 3600 rpm. What is its brake power?
  2. IP = 40 kW, FP = 6 kW. Find η_m.
  3. bsfc = 0.25 kg/kWh and CV = 42 000 kJ/kg. Find η_bth.
  4. Does a higher cetane number increase or decrease diesel knock?
  5. How many power strokes per minute does one cylinder of a four-stroke engine make at 3000 rpm?

Answers: 1. 2π × 3600 × 50/60 ≈ 18.85 kW. 2. BP = 34 kW, η_m = 34/40 = 85 %. 3. 3600/(0.25 × 42 000) ≈ 34.3 %. 4. Decrease (shorter ignition delay). 5. 1500.

Try answering each one aloud before you open it.

  1. 1.What is an internal combustion (IC) engine?Concept

    An internal combustion (IC) engine is a type of engine where the combustion of fuel occurs within a confined space called a combustion chamber. This process generates high-temperature and high-pressure gases, which expand and apply force to engine components like pistons, converting chemical energy into mechanical work.

  2. 2.Explain the four-stroke cycle in an IC engine.Concept

    The four-stroke cycle in an IC engine consists of four distinct strokes: intake, compression, power, and exhaust. During the intake stroke, the intake valve opens, and the piston moves down, drawing in an air-fuel mixture. In the compression stroke, the piston moves up, compressing the mixture. The power stroke begins when the spark plug ignites the compressed mixture, forcing the piston down. Finally, during the exhaust stroke, the exhaust valve opens, and the piston moves up, expelling the combustion gases.

  3. 3.Why is a spark plug used in a gasoline engine?Application

    A spark plug is used in a gasoline engine to ignite the air-fuel mixture within the combustion chamber. It generates a spark at the right moment during the compression stroke, initiating the combustion process. This ignition is crucial for converting the chemical energy of the fuel into mechanical energy, driving the engine's pistons.

  4. 4.What happens if the air-fuel mixture in an IC engine is too rich?Application

    If the air-fuel mixture in an IC engine is too rich, it means there is more fuel than necessary compared to the air. This can lead to incomplete combustion, resulting in higher emissions of unburned hydrocarbons and carbon monoxide. It can also cause fouling of spark plugs and reduce engine efficiency and performance.

  5. 5.Explain the concept of knocking in IC engines.Concept

    In an SI engine, knock is auto-ignition of the unburnt end gas ahead of the spark-initiated flame; the sudden pressure rise sets up pressure waves that give the metallic ping, overheat the piston and can erode it. It is promoted by high compression ratio, advanced spark, hot intake air and low-octane fuel, and controlled by knock sensors that retard the spark. In a CI engine, diesel knock comes from too long an ignition delay, so accumulated fuel burns at once; it is reduced by high cetane fuel and higher compression temperature — the opposite remedies.

  6. 6.Why is a turbocharger used in some IC engines?Application

    A turbocharger is used in some IC engines to increase the engine's power output without increasing its size. It works by using exhaust gases to drive a turbine, which in turn compresses the intake air. This allows more air (and thus more fuel) to enter the combustion chamber, resulting in more powerful combustion and increased engine efficiency.

  7. 7.What is the role of a carburetor in an IC engine?Concept

    A carburetor is a device in an IC engine that mixes air with a fine spray of liquid fuel to create a combustible air-fuel mixture. It regulates the ratio of air to fuel, ensuring optimal combustion for different engine operating conditions. Although modern engines often use fuel injection systems, carburetors were widely used in older engines.

  8. 8.What is the effect of increasing the compression ratio on the performance of an IC engine?Application

    Increasing the compression ratio in an IC engine generally improves its thermal efficiency, as it allows the engine to extract more mechanical energy from a given amount of fuel. However, higher compression ratios can also lead to increased risk of knocking, requiring careful design and possibly higher-octane fuel to prevent engine damage.

  9. 9.A four-stroke engine with a total displacement of 2 litres produces 100 kW of brake power at 3000 rpm. Determine its brake mean effective pressure.Numerical

    For a four-stroke engine, BP = bmep × V_s × N/120, since each cylinder fires once every two revolutions. So bmep = BP × 120/(V_s × N) = 100 000 × 120/(0.002 × 3000) = 2 000 000 Pa, or 2 MPa (20 bar). That is a realistic value only for a highly boosted engine; naturally aspirated petrol engines are nearer 10 bar.

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