Ch 8. Gas Power Cycle Multimedia Engineering Thermodynamics OttoCycle DieselCycle
 Chapter 1. Basics 2. Pure Substances 3. First Law 4. Energy Analysis 5. Second Law 6. Entropy 7. Exergy Analysis 8. Gas Power Cyc 9. Brayton Cycle 10. Rankine Cycle Appendix Basic Math Units Thermo Tables Search eBooks Dynamics Fluids Math Mechanics Statics Thermodynamics Author(s): Meirong Huang Kurt Gramoll ©Kurt Gramoll

 THERMODYNAMICS - CASE STUDY SOLUTION In Max's senior capstone design, the thermal efficiencies and the compression ratios of an ideal Otto cycle and an ideal Diesel cycle are required. Assumptions: Cold-air-standard assumption is valid for this analysis. The constant volume specific heat cv = 0.718 kJ/(kg-K), the constant pressur specific heat cP = 1.005 kJ/(kg-K) Model the cycle in the car engine as an ideal Otto cycle and an ideal Diesel cycle, respectively. P-v and T-s Diagram of the Otto Cycle (1) Determine the thermal efficiency and compression ratio using ideal Otto-cycle model The P-v and T-s diagrams of the ideal Otto cycle are shown on the left. The thermal efficiency and compression ratio using the Otto-cycle model has been determined in the previous section. They are:       Thermal efficiency: ηth, Otto = 53.3%       Compression ratio: r = 6.7 P-v and T-s Diagram of the Diesel Cycle (2) Determine the thermal efficiency and compression ratio using Diesel-cycle model The P-v and T-s diagrams of the ideal Diesel cycle are shown on the left. The previous section, the properties at the four states of an Otto cycle was determined. They are:       state 1: T1 = 15oC, P1 = 100 kPa (given)       State 2: T2 = 343.3oC       State 3: T3 = 1800oC (given)       State 4: T4 = 695.7oC The heat input to the cycle is:       qin,Otto = cv23 (T3 - T2) = 0.718(1800 - 343.3)                  = 1045.9 kJ In Diesel cycle, with the temperature limit is the same as In Otto cycle, temperature at state 1 and state 3 are:       T1 = 15oC       T3 = 1800oC Also, heat input is the same as in the ideal Otto cycle. In Diesel cycle, heat is input from the constant pressure cycle.       qin,Diesel = cP23 (T3 - T2) = 1.005 (1800 - T2)                    = 1045.9 kJ The temperature at state 2 can be determined from the above expression. That is,       T2 = 759.3oC = 1032.3 K The thermal efficiency of the ideal Diesel cycle is:        where r is the compression ratio and rc is the cutoff ratio.       r = v1/v2       rc = v3/v2 In Diesel cycle, process 1-2 is isentropic compression process. It gives,        Hence, the compression ratio of an ideal Diesel-cycle is 24.3, which is much higher than the compression ratio of an ideal Otto-cycle, which is 6.7. Process 2-3 in an ideal Diesel cycle is an constant pressure cycle. Thus,        It gives that the cutoff ratio equals 2.01. Substitute the compression ratio and cutoff ratio to the expression of thermal efficiency yields,        Also, the thermal efficiency of the ideal Diesel-cycle is much higher than the ideal Otto-cycle, which is 53.3%.