Increases the thermal efficiency
Increases the compressor work
Increases the turbine work
Decreases the thermal efficiency
A. Increases the thermal efficiency
They can generate very high thrust
They have high propulsion efficiency
These engines can work on several fuels
They are not air breathing engines
Multistage compression
Cold water spray
Both (A) and (B) above
Fully insulating the cylinder
Reduced
Increased
Zero
None of these
200°C
500°C
700°C
1000°C
Isothermal compression
Isentropic compression
Polytropic compression
None of these
Reciprocating compressor
Centrifugal compressor
Axial flow compressor
Turbo compressor
Isothermal compression
Adiabatic compression
Isentropic compression
Polytropic compression
Highly heated atmospheric air
Solids
Liquid
Plasma
In the diffuser only
In the impeller only
In the diffuser and impeller
In the inlet guide vanes only
Cools the delivered air
Results in saving of power in compressing a given volume to given pressure
Is the standard practice for big compressors
Enables compression in two stages
Compressor efficiency
Isothermal efficiency
Volumetric efficiency
Mechanical efficiency
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
Equal to
Less than
More than
None of these
Vacuum
Atmospheric air
Compressed air
Oxygen alone
Increase velocity
Make the flow streamline
Convert pressure energy into kinetic energy
Convert kinetic energy into pressure energy
Remove impurities from air
Reduce volume of air
Cause moisture and oil vapour to drop out
Cool the air
Compressor efficiency
Volumetric efficiency
Isothermal efficiency
Mechanical efficiency
The propulsive matter is caused to flow around the propelled body
Propulsive matter is ejected from within the propelled body
Its functioning does not depend on presence of air
All of the above
Less
More
Same
May be less or more depending on ambient conditions
p₂ = p₁ × p₃
p₂ = p₁/p₃
p₂ = p₁ × p₂
p₂ = p₃/p₁
Equal to
Less than
More than
None of these
Low frontal area
Higher thrust
High pressure rise
None of these
Equal to
Less than
More than
None of these
Work factor
Slip factor
Degree of reaction
Pressure coefficient
Higher
Lower
Same
None of the above
30 : 1
40 : 1
50 : 1
60 : 1
Back pressure
Critical pressure
Discharge pressure
None of these
Diffuser inlet radius
Diffuser outlet radius
Impeller inlet radius
Impeller outlet radius
Vi = Vo
Vt > Vo
U < Vo
V = Uo
Atmospheric
Slightly more than atmospheric
Slightly less than atmospheric
Pressure slightly less than atmospheric and temperature slightly more than atmospheric