2nd-Law Analysis of Otto Cycles Consider an engine operating on the ideal Otto cycle with a compression ratio of 8. At the beginning of the compression process, air is at 100 kPa and 17°C. During the constant-volume heat-addition process, 800 kJ/kg of heat is transferred to air from a source at 1700 K and waste heat is rejected to the surroundings at 290 K. Accounting for the variation of specific heats of air with temperature, determine (a) the exergy destruction associated with each of the four processes and the cycle and (b) the second-law efficiency of this cycle. P. kPa

Elements Of Electromagnetics
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2nd-Law Analysis of Otto Cycles
Consider an engine operating on the ideal Otto cycle with a compression ratio of
8. At the beginning of the compression process, air is at 100 kPa and 17°C. During
the constant-volume heat-addition process, 800 kJ/kg of heat is transferred to air
from a source at 1700 K and waste heat is rejected to the surroundings at 290 K.
Accounting for the variation of specific heats of air with temperature, determine
(a) the exergy destruction associated with each of the four processes and the
cycle and (b) the second-law efficiency of this cycle.
P. kPa
Isentropic
in
Jout
Isentropic
100
38
V = V =
V = V4
Transcribed Image Text:2nd-Law Analysis of Otto Cycles Consider an engine operating on the ideal Otto cycle with a compression ratio of 8. At the beginning of the compression process, air is at 100 kPa and 17°C. During the constant-volume heat-addition process, 800 kJ/kg of heat is transferred to air from a source at 1700 K and waste heat is rejected to the surroundings at 290 K. Accounting for the variation of specific heats of air with temperature, determine (a) the exergy destruction associated with each of the four processes and the cycle and (b) the second-law efficiency of this cycle. P. kPa Isentropic in Jout Isentropic 100 38 V = V = V = V4
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