Small quantities of air at high pressures
Large quantities of air at high pressures
Small quantities of air at low pressures
Large quantities of air at low pressures
D. Large quantities of air at low pressures
Isothermal compression
Adiabatic compression
Isentropic compression
Polytropic compression
34 %
50 %
60 %
72 %
They can generate very high thrust
They have high propulsion efficiency
These engines can work on several fuels
They are not air breathing engines
Actual volume of the air delivered by the compressor when reduced to normal temperature and pressure conditions
Volume of air delivered by the compressor
Volume of air sucked by the compressor during its suction stroke
None of the above
Radial flow
Axial flow
Centrifugal
None of the above
Increases as clearance volume increases
Decreases as clearance volume increases
Is independent of clearance volume
Increases as clearance volume decreases
Vi = Vo
Vt > Vo
U < Vo
V = Uo
Decreases
Increases
Does not change
None of these
No propeller
Propeller in front
Propeller at back
Propeller on the top
Forward curved
Backward curved
Radial
None of these
Atmosphere
Back to the compressor
Discharge nozzle
Vacuum
Less
More
Same
May be less or more depending upon speed
Centrifugal
Reciprocating
Axial
Screw
Compressor work and turbine work
Output and input
Actual total head temperature drop to the isentropic total head drop from total head inlet to static head outlet
Actual compressor work and theoretical compressor work
Closed cycle
Open cycle
Both of the above
Closed/open depending on other considerations
The flow of air is parallel to the axis of the compressor
The static pressure of air in the impeller increases in order to provide centripetal force on the air
The impeller rotates at high speeds
The maximum efficiency is higher than multistage axial flow compressors
The reciprocating compressors are best suited for high pressure and low volume capacity
The effect of clearance volume on power consumption is negligible for the same volume of discharge
Both (A) and (B)
None of these
Work factor
Slip factor
Degree of reaction
Pressure coefficient
Isothermal
Isentropic
Adiabatic
Isochoric
20 - 30 %
40 - 50 %
60 - 70 %
70 - 90 %
Pressure ratio
Pressure coefficient
Degree of reaction
Slip factor
Backward curved blades has poor efficiency
Backward curved blades lead to stable performance
Forward curved blades has higher efficiency
Forward curved blades produce lower pressure ratio
Air stream blocking the passage
Motion of air at sonic velocity
Unsteady, periodic and reversed flow
Air stream not able to follow the blade contour
Start-stop motor
Constant speed unloader
Relief valve
Variable speed
Pressure ratio
Maximum cycle temperature
Minimum cycle temperature
All of the above
Thrust power and fuel energy
Engine output and propulsive power
Propulsive power and fuel input
Thrust power and propulsive power
Indicated power
Brake power
Frictional power
None of these
Standard air
Free air
Compressed air
Compressed air at delivery pressure
Has no effect on
Decreases
Increases
None of these
Jet velocity
Twice the jet velocity
Half the jet velocity
Average of the jet velocity