The combustion chamber in a rocket engine is directly analogous to the reservoir of a supersonic wind tunnel
The stagnation conditions exist at the combustion chamber
The exit velocities of exhaust gases are much higher than those in jet engine
All of the above
D. All of the above
Equal to
Less than
More than
None of these
p₂/p₁ = p₃/p₂ = p₄/p₃
p₃/p₁ = p₄/p₂
p₁ p₂ = p₃ p₄
p₁ p₃ = p₂ p₄
Increase
Decrease
Remain same
May increase or decrease depending on clearance volume
High calorific value
Ease of atomisation
Low freezing point
Both (A) and (C) above
Compression ratio
Expansion ratio
Compressor efficiency
Volumetric efficiency
0.1 bar and 20°C
1 bar and 20°C
0.1 bar and 40°C
1 bar and 40°C
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
Radial flow compressor
Axial flow compressor
Roots blower
Reciprocating compressor
Free air delivery
Compressor capacity
Swept volume
None of these
Isothermally
Polytropically
Isentropically
None of these
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
Isentropic compression
Isothermal compression
Polytropic compression
None of the above
Equal to
Double
Three times
Six times
20 - 30 %
40 - 50 %
60 - 70 %
70 - 90 %
At very high speed
At very slow speed
At average speed
At zero speed
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
3 m³/ mt.
1.5 m³/ mt.
18 m³/ mt.
6 m³/ mt.
10 to 40 %
40 to 60 %
60 to 70 %
70 to 90 %
Same
More
Less
Depends on other factors
200°C
500°C
700°C
1000°C
Reduction of speed of incoming air and conversion of part of it into pressure energy
Compression of inlet air
Increasing speed of incoming air
Lost work
Decreasing the compression work
Increasing the compression work
Increasing the turbine work
Both (A) and (C) above
Increase of work ratio
Decrease of thermal efficiency
Decrease of work ratio
Both (A) and (B) above
Atmosphere
Vacuum
Discharge nozzle
Back to the compressor
A.C. electric motor
Compressed air
Petrol engine
Diesel engine
Higher
Lower
Same
None of the above
1.03 kg/cm²
1.06 kg/cm²
1.00 kg/cm²
0.53 kg/cm²
Back pressure
Critical pressure
Discharge pressure
None of these
p₂ = (p₁ + p₃)/2
p₂ = p₁. p₃
P₂ = Pa × p₃/p₁
p₂ = Pa p₃/p₁