Power Plant Engineering · Lesson 3 of 6
Internal Combustion Engines
The Otto, Diesel, and Dual air-standard cycles, compression ratio and air-standard efficiency, indicated and brake power, mean effective pressure, thermal and mechanical efficiency, and specific fuel consumption, worked in SI units for the MELE.
15 min read · Super EaFree lesson
Internal combustion (IC) engines are the second big block of the Industrial and Power Plant Engineering paper. The theory rests on three air-standard cycles (Otto, Diesel, Dual), and the practice rests on a handful of power and efficiency formulas. If you can compute an air-standard efficiency from a compression ratio and turn a torque and speed into brake power, you have most of the marks. Work in SI: pressure in kPa or Pa, power in kW, torque in N-m, speed in rev/s or rad/s.
The three air-standard cycles
Each cycle is an idealization of a real engine, using air as the working fluid with a constant specific-heat ratio k = 1.4.
Otto cycle (spark-ignition, gasoline): heat is added at constant volume. Its efficiency depends only on compression ratio:
eta_Otto = 1 minus 1/r^(k minus 1)Diesel cycle (compression-ignition): heat is added at constant pressure. Its efficiency adds a cut-off correction:
eta_Diesel = 1 minus (1/r^(k minus 1)) x [(rc^k minus 1) / (k(rc minus 1))]where rc is the cut-off ratio (the volume ratio during constant-pressure heat addition).
Dual (mixed) cycle: heat is added partly at constant volume and partly at constant pressure, the most realistic model of a modern high-speed diesel. Its efficiency lies between the Otto and Diesel values.
At the same compression ratio, the Otto cycle is the most efficient of the three, but real spark-ignition engines are limited to low compression ratios (about 8 to 11) by knock, while diesels run at 14 to 22, which is why diesels are more efficient in practice.
Compression ratio and air-standard efficiency
The compression ratio is the ratio of cylinder volume at bottom dead center to that at top dead center:
r = (Vc + Vs) / Vc
where Vc is the clearance (top dead center) volume and Vs is the swept (displacement) volume. A cylinder with Vc = 0.0001 m3 and Vs = 0.0009 m3 has r = (0.0001 + 0.0009)/0.0001 = 10.
Worked example (Otto): with r = 9 and k = 1.4, eta = 1 minus 1/9^0.4. Since 9^0.4 = 2.408, eta = 1 minus 0.415 = 0.585, or 58.5%. At r = 6 the same formula gives 51.2%: efficiency climbs with compression ratio.
Worked example (Diesel): with r = 16, cut-off ratio rc = 2, and k = 1.4, eta = 1 minus (1/16^0.4)[(2^1.4 minus 1)/(1.4(2 minus 1))]. Here 16^0.4 = 3.031, 2^1.4 = 2.639, so eta = 1 minus (0.330)(1.639/1.4) = 1 minus 0.330 x 1.171 = 1 minus 0.386 = 0.614, or 61.4%.
Indicated and brake power
Two power levels matter:
Indicated power (IP) is the power developed inside the cylinders by the gas on the piston:
IP = pmi x L x A x n x N_cwhere pmi is the indicated mean effective pressure, L the stroke, A the piston area, n the number of cylinders, and N_c the number of power strokes per second per cylinder (for a four-stroke engine, N_c = N/2 with N in rev/s).
Brake power (BP) is the useful power at the output shaft:
BP = 2 x pi x N x T = T x omegawith N in rev/s, T the torque in N-m, and omega in rad/s.
Worked example: an engine delivers 200 N-m of torque at 2,400 rpm. Then omega = 2 x pi x 2,400/60 = 251.3 rad/s, so BP = 200 x 251.3 = 50,265 W, about 50.3 kW.
The gap between IP and BP is the friction power (FP): IP = BP + FP.
Mean effective pressure
The mean effective pressure (MEP) is the constant pressure that, acting over the swept volume, would do the same net work as the real cycle:
MEP = net work per cycle / swept volume
Worked example: a cylinder does 900 J of net work per cycle in a swept volume of 0.0006 m3. MEP = 900/0.0006 = 1,500,000 Pa = 1,500 kPa (1.5 MPa). MEP is a fair way to compare engines of different size because it removes the effect of displacement.
Thermal, mechanical, and overall efficiency
Brake thermal efficiency is useful shaft power over the fuel's energy rate:
eta_bth = BP / (mf x HHV)Worked example: BP = 50 kW, fuel rate mf = 12 kg/h = 0.003333 kg/s, HHV = 44,000 kJ/kg. Fuel power = 0.003333 x 44,000 = 146.7 kW, so eta_bth = 50/146.7 = 0.341, or 34.1%.
Mechanical efficiency is brake power over indicated power:
eta_mech = BP / IPIf BP = 50 kW and IP = 60 kW, then eta_mech = 50/60 = 0.833, or 83.3%. The missing 10 kW is friction power.
Specific fuel consumption
Specific fuel consumption (SFC) is the fuel burned per unit of output, the standard measure of an engine's thirst:
SFC = mf / BP
Worked example: mf = 12 kg/h and BP = 50 kW give SFC = 12/50 = 0.24 kg per kWh. A lower SFC means a more economical engine, and SFC is inversely related to brake thermal efficiency.
Exam-day strategy
- Otto efficiency needs only r: eta = 1 minus 1/r^0.4 for air. Diesel adds the cut-off correction, which always makes it less efficient than an Otto of the same r.
- Compression ratio is (Vc + Vs)/Vc: total over clearance, not swept over clearance.
- Brake power from torque is BP = 2 x pi x N x T. Convert rpm to rev/s (divide by 60) first.
- Keep IP, BP, and FP straight: IP = BP + FP, and mechanical efficiency is BP/IP.
- SFC = mf/BP; brake thermal efficiency = BP/(mf x HHV). Watch units: put mf in kg/s and HHV in kJ/kg to get power in kW.
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Internal Combustion Engines: quick check
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An engine develops a torque of 250 N-m at 2,000 rpm. Its brake power is closest to:
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