Pressure coefficient
Work coefficient
Polytropic reaction
Slip factor
A. Pressure coefficient
Increases with increase in compression ratio
Decreases with increase in compression ratio
Is not dependent upon compression ratio
May increase/decrease depending on compressor capacity
(v₁² -v₂²)/2g
(v₁ - v₂)²/2g
(v₁² -v₂²)/g
(v₁ - v₂)²/g
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
Brayton or Atkinson cycle
Carnot cycle
Rankine cycle
Erricson cycle
To accommodate Valves in the cylinder head
To provide cushioning effect
To attain high volumetric efficiency
To provide cushioning effect and also to avoid mechanical bang of piston with cylinder head
Pressure coefficient
Work coefficient
Polytropic reaction
Slip factor
Centrifugal compressor
Axial compressor
Pumps
All of the above
More power
Less power
Same power
More/less power depending on other factors
Decreases
Increases
Does not change
None of these
Inlet whirl velocity
Outlet whirl velocity
Inlet velocity of flow
Outlet velocity of flow
Net work output and work done by turbine
Net work output and heat supplied
Work done by turbine and heat supplied
Work done by turbine and net work output
Remain same
Decrease
Increase
None of the above
Vacuum
Atmospheric air
Compressed air
Oxygen alone
Start-stop motor
Constant speed unloader
Relief valve
Variable speed
Slip factor
Velocity factor
Velocity coefficient
None of the above
Increases
Decreases
First increases and then decreases
First decreases and then increases
Indicated power
Brake power
Frictional power
None of these
Pulsejet requires no ambient air for propulsion
Ramjet engine has no turbine
Turbine drives compressor in a Turbojet
Bypass turbojet engine increases the thrust without adversely affecting, the propulsive efficiency and fuel economy
Low
High
Same
Low/high depending on make and type
Reciprocating compressor
Centrifugal compressor
Axial flow compressor
Turbo compressor
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
Isothermal
Isentropic
Adiabatic
Isochoric
Higher
Lower
Equal
Cant be compared
A.C. electric motor
Compressed air
Petrol engine
Diesel engine
Pressure drop across the valves
Superheating in compressor
Clearance volume and leakages
All of these
700°C
2000°C
1500°C
1000°C
Same
Lower
Higher
None of these
Vi = Vo
Vt > Vo
U < Vo
V = Uo
W₁/W₂ = n₂(n₁ - 1)/n₁(n₂ - 1)
W₁/W₂ = n₁(n₂ - 1)/n₂(n₁ - 1)
W₁/W₂ = n₁/n₂
W₁/W₂ = n₂/n₁
0.5 kg
1.0 kg
1.3 kg
2.2 kg