AIR STANDARD CYCLE

5.3 Thermal Efficiency of Otto Cycle

5.4 Important Observations

Process 2โ€“3: Constant Pressure Heat Addition

  • Fuel is injected into the highly compressed air
  • Combustion occurs while pressure remains constant
  • Volume increases as heat is added
  • Temperature rises further

Process 3โ€“4: Isentropic Expansion (Power Stroke)

  • High-pressure gases expand adiabatically
  • Work is produced
  • Pressure and temperature drop
  • Volume increases to maximum

Process 4โ€“1: Constant Volume Heat Rejection

  • Heat is rejected at constant volume
  • Pressure and temperature decrease
  • The system returns to initial state

6.3 Cut-off Ratio

ฯ=V3V2\rho = \frac{V_3}{V_2}

6.4 Thermal Efficiency of Diesel Cycle

ฮทdiesel=1โˆ’1rฮณโˆ’1โ‹…ฯฮณโˆ’1ฮณ(ฯโˆ’1)\eta_{diesel} = 1 – \frac{1}{r^{\gamma-1}} \cdot \frac{\rho^{\gamma} – 1}{\gamma(\rho – 1)}

6.5 Observations

  • Efficiency depends on compression ratio and cut-off ratio
  • Higher cut-off ratio reduces efficiency

7.1 Definition

This cycle represents modern high-speed diesel engines more accurately.

7.2 Processes of Dual Cycle

  1. Isentropic compression
  2. Constant volume heat addition
  3. Constant pressure heat addition
  4. Isentropic expansion
  5. Constant volume heat rejection

9. Air Standard Efficiency


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