- Aug 7, 2001
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I have a problem that's just kicking my ass.
A 6-cylinder gasoline engine has a displacement volume of 3 liters, a compression ration of 9.5 and operates at 4000rpm. The air-fuel mixture enters a cylinder at p=1atm and an ambient temperature of 27celsius. During combustion, the mixture reaches a temp of 1,350celsius. Calculate the power delivered by this engine.
So, in a PV diagram, we have a path from A-> B-> C-> D-> A. Since the process is cyclic, the internal energy goes to zero for the cycle. We know from A->B and C->D the process is adiabatic and the process from B->C and D->A is isometric.
The heat enters the system from B->C and heat is expelled from D->A.
So Qh is the process from B->C and Qc is the process from D->A.
W=Qh-Qc
Qh=Cv(Tc-Tb)
Qc=Cv(Ta-Td)
Is it wrong to assume Ta=Tb and Tc=Td since between these respective processes there is no heat exchanged? Also, how do we find the heat capacity at constant volume for an air-fuel mixture? Do we even need it? Also, should we treat the mixture as an ideal gas and use the given initial pressure to our advantage?
We know that for a single cylinder, the non-compressed volume is .5L*((10^-3*m^3)/L) and the compressed volume is .05263L*((10^-3*m^3)/L).
Any tips or points to another resource would be greatly appreciated. I just can't seem to figure this one out.
Once we find the work, the problem is just about done. We know that power is delivered every other revolution of the crankshaft. So this work, multiplied by the six cylinders and then solve P=dW/dT. The power is 'delivered' every 2/4000 minutes * 60 seconds/ minute or 3/100 seconds. So the power would be the Work of one cylinder, W1c, divided by (3/100)s, times six cylinders or 200W1c/second.
I've even tried applying the fact that for an adiabat, T1V1^(cp/cv -1)=T2V2^(cp/cv -1), to use, but I wasn't clear on what temps and points to use. Using points A and C respectively, I got a gamma = 1.75, which doesnt make any sense. That's a higher yield than a monotomic gas.
A 6-cylinder gasoline engine has a displacement volume of 3 liters, a compression ration of 9.5 and operates at 4000rpm. The air-fuel mixture enters a cylinder at p=1atm and an ambient temperature of 27celsius. During combustion, the mixture reaches a temp of 1,350celsius. Calculate the power delivered by this engine.
So, in a PV diagram, we have a path from A-> B-> C-> D-> A. Since the process is cyclic, the internal energy goes to zero for the cycle. We know from A->B and C->D the process is adiabatic and the process from B->C and D->A is isometric.
The heat enters the system from B->C and heat is expelled from D->A.
So Qh is the process from B->C and Qc is the process from D->A.
W=Qh-Qc
Qh=Cv(Tc-Tb)
Qc=Cv(Ta-Td)
Is it wrong to assume Ta=Tb and Tc=Td since between these respective processes there is no heat exchanged? Also, how do we find the heat capacity at constant volume for an air-fuel mixture? Do we even need it? Also, should we treat the mixture as an ideal gas and use the given initial pressure to our advantage?
We know that for a single cylinder, the non-compressed volume is .5L*((10^-3*m^3)/L) and the compressed volume is .05263L*((10^-3*m^3)/L).
Any tips or points to another resource would be greatly appreciated. I just can't seem to figure this one out.
Once we find the work, the problem is just about done. We know that power is delivered every other revolution of the crankshaft. So this work, multiplied by the six cylinders and then solve P=dW/dT. The power is 'delivered' every 2/4000 minutes * 60 seconds/ minute or 3/100 seconds. So the power would be the Work of one cylinder, W1c, divided by (3/100)s, times six cylinders or 200W1c/second.
I've even tried applying the fact that for an adiabat, T1V1^(cp/cv -1)=T2V2^(cp/cv -1), to use, but I wasn't clear on what temps and points to use. Using points A and C respectively, I got a gamma = 1.75, which doesnt make any sense. That's a higher yield than a monotomic gas.
