It requires very big cylinder
It does not increase pressure much
It is impossible in practice
Compressor has to run at very slow speed to achieve it
D. Compressor has to run at very slow speed to achieve it
0.1 bar and 20°C
1 bar and 20°C
0.1 bar and 40°C
1 bar and 40°C
Ammonia and water vapour
Carbon dioxide
Nitrogen
Hydrogen
Compressor efficiency
Isentropic efficiency
Euler's efficiency
Pressure coefficient
Employing intercooler
By constantly cooling the cylinder
By running compressor at very slow speed
By insulating the cylinder
Increase first at fast rate and then slow
Increase first at slow rate and then fast
Decrease continuously
First increase, reach maximum and then decrease
20 - 30 %
40 - 50 %
60 - 70 %
70 - 90 %
As large as possible
As small as possible
About 50% of swept volume
About 100% of swept volume
Compression index
Compression ratio
Compressor efficiency
Mean effective pressure
The compression ratio in each stage should be same
The intercooling should be perfect
The workdone in each stage should be same
All of the above
Mass
Energy
Flow
Linear momentum
They can generate very high thrust
They have high propulsion efficiency
These engines can work on several fuels
They are not air breathing engines
Radial flow compressors
Axial flow compressors
Pumps
All of these
Atmospheric
Slightly more than atmospheric
Slightly less than atmospheric
Pressure slightly less than atmospheric and temperature slightly more than atmospheric
High nickel alloy
Stainless steel
Carbon steel
High alloy steel
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
Isothermal h.p. to the BHP of motor
Isothermal h.p. to adiabatic h.p.
Power to drive compressor to isothermal h.p.
Work to compress air isothermally to work for actual compression
Highly heated atmospheric air
Solids
Liquid
Plasma
Back pressure
Critical pressure
Discharge pressure
None of these
Forward curved
Backward curved
Radial
None of these
Temperature during compression remains constant
No heat leaves or enters the compressor cylinder during compression
Temperature rise follows a linear relationship
Work done is maximum
p₂ = p₁ × p₃
p₂ = p₁/p₃
p₂ = p₁ × p₂
p₂ = p₃/p₁
0.1 %
0.5 %
1.0 %
5 %
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
Increase
Decrease
Remain unaffected
Other factors control it
Control temperature
Control output of turbine
Control fire hazards
Increase efficiency
Inlet whirl velocity
Outlet whirl velocity
Inlet velocity of flow
Outlet velocity of flow
Adding heat exchanger
Injecting water in/around combustion chamber
Reheating the air after partial expansion in the turbine
All of the above
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
Pressure ratio
Pressure coefficient
Degree of reaction
Slip factor
Increases as clearance volume increases
Decreases as clearance volume increases
Is independent of clearance volume
Increases as clearance volume decreases