Ideal compression
Adiabatic compression
Isentropic compression
Isothermal compression
D. Isothermal compression
The ratio of the discharge pressure to the inlet pressure of air is called compressor efficiency
The compression ratio for the compressor is always greater than unity
The compressor capacity is the ratio of workdone per cycle to the stroke volume
During isothermal compression of air, the workdone in a compressor is maximum
Isothermal
Polytropic
Isentropic
Any one of these
Rotor to static enthalpy rise in the stator
Stator to static enthalpy rise in the rotor
Rotor to static enthalpy rise in the stage
Stator to static enthalpy rise in the stage
Is self operating at zero flight speed
Is not self operating at zero flight speed
Requires no air for its operation
Produces a jet consisting of plasma
H.P. compressor is connected to H.P. turbine and L.P. compressor to L.P. turbine
H.P. compressor is connected to L.P. turbine and L.P. compressor is connected to H.P. turbine
Both the arrangements can be employed
All are connected in series
Net work output and heat supplied
Net work output and work done by turbine
Actual heat drop and isentropic heat drop
Net work output and isentropic heat drop
Collect more air
Convert kinetic energy of air into pressure energy
Provide robust structure
Beautify the shape
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
Centrifugal type
Reciprocating type
Lobe type
Axial flow type
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
700°C
2000°C
1500°C
1000°C
Multistage compression
Cold water spray
Both (A) and (B) above
Fully insulating the cylinder
Less
More
Same
May be less or more depending on ambient conditions
Better lubrication is possible advantages of multistage
More loss of air due to leakage past the cylinder
Mechanical balance is better
Air can be cooled perfectly in between
In two phases
In three phases
In a single phase
In the form of air and water mixture
D₁/D₂ = (p₁ p₃)1/2
D₁/D₂ = (p₁/p₃)1/4
D₁/D₂ = (p₁ p₃)1/4
D₁/D₂ = (p₃/p₁)1/4
Atmospheric
Slightly more than atmospheric
Slightly less than atmospheric
Pressure slightly less than atmospheric and temperature slightly more than atmospheric
Does not change
Increases
Decreases
First decrease and then increase
Less power requirement
Better mechanical balance
Less loss of air due to leakage past the cylinder
Lower volumetric efficiency
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
550 km/hr
1050 km/hr
1700 km/hr
2400 km/hr
Lower heating value
Higher heating value
Heating value
Higher calorific value
Higher
Lower
Equal
Cant be compared
Equal to
Double
Three times
Six times
p₂ = (p₁ + p₃)/2
p₂ = p₁. p₃
P₂ = Pa × p₃/p₁
p₂ = Pa p₃/p₁
Large quantity of air at high pressure
Small quantity of air at high pressure
Small quantity of air at low pressure
Large quantity of air at low pressure
Isothermal
Adiabatic
Polytropic
None of the above
To cool the air during compression
To cool the air at delivery
To enable compression in two stages
To minimise the work of compression
Larger air handling ability per unit frontal area
Higher pressure ratio per stage
Aerofoil blades are used
Higher average velocities
Stainless steel
High alloy steel
Duralumin
Timken, Haste alloys