Increases
Decreases
Remain unaffected
May increase or decrease depending on compressor capacity
A. Increases
In two phases
In three phases
In a single phase
In the form of air and water mixture
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
Diffuser inlet radius
Diffuser outlet radius
Impeller inlet radius
Impeller outlet radius
Single stage compression
Multistage compression without intercooling
Multistage compression with intercooling
None of these
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
W₁/W₂ = n₂(n₁ - 1)/n₁(n₂ - 1)
W₁/W₂ = n₁(n₂ - 1)/n₂(n₁ - 1)
W₁/W₂ = n₁/n₂
W₁/W₂ = n₂/n₁
One stroke
Two strokes
Three strokes
Four strokes
Cool the air
Decrease the delivery temperature for ease in handling
Cause moisture and oil vapour to drop out
Reduce volume
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
Increase in flow
Decrease in flow
Increase in efficiency
Increase in flow and decrease in efficiency
Forward curved
Backward curved
Radial
None of these
Decreasing the compression work
Increasing the compression work
Increasing the turbine work
Both (A) and (C) above
Decreases net output but increases thermal efficiency
Increases net output but decreases thermal efficiency
Decreases net output and thermal efficiency both
Increases net output and thermal efficiency both
Brayton or Atkinson cycle
Carnot cycle
Rankine cycle
Erricson cycle
1 : 1.2
1 : 2
1 : 5
1 : 10
Compressor efficiency
Isentropic efficiency
Euler's efficiency
Pressure coefficient
Power consumption per unit of air delivered is low
Volumetric efficiency is high
It is best suited for compression ratios around 7:1
The moisture in air is condensed in the intercooler
p₂ = (p₁ + p₃)/2
p₂ = p₁. p₃
P₂ = Pa × p₃/p₁
p₂ = Pa p₃/p₁
Adiabatic temperature drop in the stage
Total temperature drop
Total temperature drop in the stage
Total adiabatic temperature drop
0.1 %
0.5 %
1.0 %
5 %
Low frontal area
Higher thrust
High pressure rise
None of these
0.5 kg
1.0 kg
1.3 kg
2.2 kg
Liquid hydrogen
High speed diesel oil
Kerosene
Methyl alcohol
Mass flow rate
Pressure ratio
Change in load
Stagnation pressure at the outlet
Free air delivery
Compressor capacity
Swept volume
None of these
Equal to
Less than
More than
None of these
Ammonia and water vapour
Carbon dioxide
Nitrogen
Hydrogen
Conversion of pressure energy into kinetic energy
Conversion of kinetic energy into pressure energy
Centripetal action
Generating pressure directly
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
Less
More
Same
May be less or more depending on ambient conditions