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Diesel cycle efficiency compared with Otto

Short answer

T2=953 K, T3=2097 K, T4=905 K; heat added 1150 kJ/kg, rejected 434 kJ/kg; efficiency 62.2%; mep 880 kPa. At the same compression ratio the Otto cycle is more efficient (68.5%), but practical CI engines use higher ratios and outperform SI engines.

A Diesel cycle has a compression ratio of 18 and a cut-off ratio of 2.2. Air at the start of compression is at 100 kPa and 300 K. Using cp=1.005c_p = 1.005 kJ/kg K, cv=0.718c_v = 0.718 kJ/kg K and γ=1.4\gamma = 1.4, find the temperatures at the end of each process, the heat added and rejected per kg, the thermal efficiency and the mean effective pressure. Compare the efficiency with that of an Otto cycle of the same compression ratio and explain the result.

The Diesel cycle has isentropic compression (1-2), constant-pressure heat addition (2-3), isentropic expansion (3-4) and constant-volume heat rejection (4-1).

 p
 |      2________3
 |     /         \
 |    /           \
 |   /             \
 |  /               4
 | /              _/
 |/____1________/____ v

Temperatures

T2=T1rγ−1=300×180.4=953.3 KT3=ρ T2=2.2×953.3=2097.3 KT4=T3(ρr)γ−1=2097.3×(2.218)0.4=904.7 K\begin{aligned} T_2 &= T_1 r^{\gamma-1} = 300 \times 18^{0.4} = 953.3\ \text{K} \\ T_3 &= \rho\, T_2 = 2.2 \times 953.3 = 2097.3\ \text{K} \\ T_4 &= T_3 \left(\frac{\rho}{r}\right)^{\gamma-1} = 2097.3 \times \left(\frac{2.2}{18}\right)^{0.4} = 904.7\ \text{K} \end{aligned}

Heat and efficiency

Qin=cp(T3−T2)=1.005(2097.3−953.3)=1149.7 kJ/kgQout=cv(T4−T1)=0.718(904.7−300)=434.2 kJ/kgWnet=1149.7−434.2=715.5 kJ/kgη=715.51149.7=0.622\begin{aligned} Q_{in} &= c_p (T_3 - T_2) = 1.005(2097.3 - 953.3) = 1149.7\ \text{kJ/kg} \\ Q_{out} &= c_v (T_4 - T_1) = 0.718(904.7 - 300) = 434.2\ \text{kJ/kg} \\ W_{net} &= 1149.7 - 434.2 = 715.5\ \text{kJ/kg} \\ \eta &= \frac{715.5}{1149.7} = 0.622 \end{aligned}

Check with the formula:

η=1−1180.4×2.21.4−11.4×1.2=1−13.178×2.01571.68=0.622\eta = 1 - \frac{1}{18^{0.4}} \times \frac{2.2^{1.4} - 1}{1.4 \times 1.2} = 1 - \frac{1}{3.178} \times \frac{2.0157}{1.68} = 0.622

Mean effective pressure

v1=0.287×300100=0.861 m3/kg,v2=0.86118=0.0478mep=715.50.861−0.0478=880 kPa\begin{aligned} v_1 &= \frac{0.287 \times 300}{100} = 0.861\ \text{m}^3/\text{kg}, \quad v_2 = \frac{0.861}{18} = 0.0478 \\ \text{mep} &= \frac{715.5}{0.861 - 0.0478} = 880\ \text{kPa} \end{aligned}

Comparison with Otto

For r=18r = 18: ηOtto=1−18−0.4=0.685\eta_{Otto} = 1 - 18^{-0.4} = 0.685, which is higher than the Diesel value of 0.622.

PointOttoDiesel
Heat additionconstant volumeconstant pressure
Efficiency at same rr68.5%62.2%
Reasonall heat added at highest temperaturepart of heat added while piston moves down

At the same compression ratio the Otto cycle is more efficient. In practice an SI engine cannot use r=18r = 18 because of knock, while a CI engine compresses only air and can. So real Diesel engines (r = 16-22) are more efficient than petrol engines (r = 8-10).

Answer: T2=953T_2 = 953 K, T3=2097T_3 = 2097 K, T4=905T_4 = 905 K; Qin=1150Q_{in} = 1150 kJ/kg, Qout=434Q_{out} = 434 kJ/kg; η=62.2%\eta = 62.2\%; mep = 880 kPa.

✓ Answer checked by Claude Opus 5.5 (high effort)

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