a) Assume it's an Otto cycle process:
The compression 1-2 from the beginning is adiabatic:
pVγ=pVcp/cV= const.Calculate the volume at point 2 (end of 1-2 adiabatic process):
p2=p1(V2V1)cp/cV= =101⋅9.11.006/0.716=2248 kN/m2.
Apply the ideal gas law to find the temperature at point 2:
T1p1V1=T2p2V2,
T2=T1p1V1p2V2= =(18+273)⋅1012248⋅9.11=712 K. The process 2-3 is at constant volume, so the temperature at point 3 is:
T3=T2p2p3=712⋅22484500=1452 K.The pressure at point 4 (3-4 is adiabatic expansion):
p4=p3(V4V3)cp/cV= =4500⋅9.11.006/0.7161=202 kN/m2. Temperature at 4:
T4=T1p1p4=(18+273)⋅101202=582 K.
b) The thermal efficiency:
η=1−nγ−11=1−9.11.006/0.716−11=0.59. c) The theoretical output in kW can be calculated from the following reasoning: the cycle is repeated 3000 times a minute, or 3000/60=50 times a second. The work done per one cycle is
W1=cV[(T3−T2)−(T4−T1)]==0.716[(1452−712)−(582−(18+273))]==321 J. 50 cycles per second will produce power (which is work per time, i.e. watt=joule/second):
P=NW1=50⋅321=16074 W. d) The mean effective pressure can be calculated through the displacement volume Vd, number of revolutions per power stroke nc (2 for a 4-stroke engine), revolutions per second N and power output P in watts:
pme=VdNncP=V1(1−9.11)⋅502⋅16074=240 779 Pa.
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