0.5 kg
1.0 kg
1.3 kg
2.2 kg
C. 1.3 kg
The ratio of stroke volume to clearance volume
The ratio of the air actually delivered to the amount of piston displacement
Reciprocal of compression ratio
Index of compressor performance
Less
More
Same
More/less depending on compressor capacity
Isothermal compression
Adiabatic compression
Isentropic compression
Polytropic compression
20 - 30 %
40 - 50 %
60 - 70 %
70 - 90 %
Provides greater flexibility
Provides lesser flexibility
In never used
Is used when gas is to be burnt
Diffuser inlet radius
Diffuser outlet radius
Impeller inlet radius
Impeller outlet radius
Compressor
Heating chamber
Cooling chamber
All of these
High h.p. and low weight
Low weight and small frontal area
Small frontal area and high h.p.
High speed and high h.p
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
Atmospheric
Slightly more than atmospheric
Slightly less than atmospheric
Pressure slightly less than atmospheric and temperature slightly more than atmospheric
Same
Less
More
None of these
Gas turbine requires lot of cooling water
Gas turbine is capable of rapid start up and loading
Gas turbines has flat efficiency at part loads
Gas turbines have high standby losses and require lot of maintenance
Surrounding air
Compressed atmospheric air
Its own oxygen
None of these
Single stage compression
Multistage compression without intercooling
Multistage compression with intercooling
None of these
Standard air
Free air
Compressed air
Compressed air at delivery pressure
Decreasing the compression work
Increasing the compression work
Increasing the turbine work
Both (A) and (C) above
Jet velocity
Twice the jet velocity
Half the jet velocity
Average of the jet velocity
Does not change
Increases
Decreases
First decrease and then increase
200°C
500°C
700°C
1000°C
Increases as clearance volume increases
Decreases as clearance volume increases
Is independent of clearance volume
Increases as clearance volume decreases
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
Compressor efficiency
Isothermal efficiency
Volumetric efficiency
Mechanical efficiency
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
Carbonisation of coal
Passing steam over incandescent coke
Passing air and a large amount of steam over waste coal at about 65°C
Partial combustion of coal, coke, anthracite coal or charcoal in a mixed air steam blast
D₁/D₂ = (p₁ p₃)1/2
D₁/D₂ = (p₁/p₃)1/4
D₁/D₂ = (p₁ p₃)1/4
D₁/D₂ = (p₃/p₁)1/4
Compressor efficiency
Volumetric efficiency
Isothermal efficiency
Mechanical efficiency
Gauge discharge pressure to the gauge intake pressure
Absolute discharge pressure to the absolute intake pressure
Pressures at discharge and suction corresponding to same temperature
Stroke volume and clearance volume
Low speeds
High speeds
Low altitudes
High altitudes
Gas turbine plant
Petrol engine
Diesel engine
Solar plant
Increases
Decreases
Remain same
First increases and then decreases