obanion
Automotive
- Jan 1, 2004
- 101
Which of these equations which I have been given correctly describe the amount of work done by a turbine?
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W=work
PR=pressure ratio of turbine inlet to outlet
delta(v)=change in volume
W=PR*delta(V)
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POWER = { mdot * k * R * T1 * [1 - (P2/P1)^((k-1)/k)] } / { 1 - k }
POWER = shaft horsepower required, in kJ/sec.
mdot = mass flow rate of air (in kg/sec)
k = ratio of specific heats for air (around 1.395 for air in the temperature ranges we're talking about)
R = the universal gas constant for air (0.287 kJ/kg-K)
T1 = the air inlet temperature to the compressor (in degrees K)
P2/P1 = the pressure ratio for the turbo outlet to inlet (in absolute, not gauge, pressures)
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The results are FAR different. The first suggests that using a very small turbine wheel and housing, using a small total flow rate (about 10% of what's going through the compressor), will effectively drive a large compressor, so long as there is lots of pressure at the turbine inlet. Say 100psi or more. Now, obviously this isn't a good idea for a typical turbo, connected through the exhaust stream. But if you were blowing CO2 gas through there, no problem.
The other equation suggests the opposite, that it would take a insane amount of CO2 to drive the process, so much that usage isn't practical.
Basically I'm trying to determine if you have a super small turbine (rated for 6lb/min at 3:1 PR), and a large compressor (rated for 70lb/min), could the turbine produce sufficient power by passing 5-10lb/min of CO2, at 100-200psi of backpressure?
__________________
W=work
PR=pressure ratio of turbine inlet to outlet
delta(v)=change in volume
W=PR*delta(V)
__________________
POWER = { mdot * k * R * T1 * [1 - (P2/P1)^((k-1)/k)] } / { 1 - k }
POWER = shaft horsepower required, in kJ/sec.
mdot = mass flow rate of air (in kg/sec)
k = ratio of specific heats for air (around 1.395 for air in the temperature ranges we're talking about)
R = the universal gas constant for air (0.287 kJ/kg-K)
T1 = the air inlet temperature to the compressor (in degrees K)
P2/P1 = the pressure ratio for the turbo outlet to inlet (in absolute, not gauge, pressures)
__________________
The results are FAR different. The first suggests that using a very small turbine wheel and housing, using a small total flow rate (about 10% of what's going through the compressor), will effectively drive a large compressor, so long as there is lots of pressure at the turbine inlet. Say 100psi or more. Now, obviously this isn't a good idea for a typical turbo, connected through the exhaust stream. But if you were blowing CO2 gas through there, no problem.
The other equation suggests the opposite, that it would take a insane amount of CO2 to drive the process, so much that usage isn't practical.
Basically I'm trying to determine if you have a super small turbine (rated for 6lb/min at 3:1 PR), and a large compressor (rated for 70lb/min), could the turbine produce sufficient power by passing 5-10lb/min of CO2, at 100-200psi of backpressure?