Has no effect on
Decreases
Increases
None of these
B. Decreases
Same
More
Less
Zero
High calorific value
Ease of atomisation
Low freezing point
Both (A) and (C) above
Increases
Decreases
Remain constant
First decreases and then increases
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
Reduced volume flow rate
Increased volume flow rate
Lower suction pressure
Lower delivery pressure
34 %
50 %
60 %
72 %
Exit nozzle, which is a constant volume process
Exit nozzle, which is essentially an isentropic process
Turbine blades, which is a constant volume process
Turbine blades, which is essentially an isentropic process
Work required to compress the air isothermally to the actual work required to compress the air for the same pressure ratio
Isothermal power to the shaft power or B.P. of the motor or engine required to drive the compressor
Volume of free air delivery per stroke to the swept volume of the piston
Isentropic power to the power required to drive the compressor
Isothermal compression
Isentropic compression
Polytropic compression
None of these
Same
One-half
One fourth
One sixth
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
Zero
Less
More
Same
0.5 kg
1.0 kg
1.3 kg
2.2 kg
Brayton or Atkinson cycle
Carnot cycle
Rankine cycle
Erricson cycle
Liquid hydrogen
High speed diesel oil
Kerosene
Methyl alcohol
75 %
85 %
90 %
99 %
These are used to dampen pulsations
These act as reservoir to take care of sudden demands
These increase compressor efficiency
These knock out some oil and moisture
Increase in net output but decrease in thermal efficiency
Increase in thermal efficiency but decrease in net output
Increase in both thermal efficiency and net output
Decrease in both thermal efficiency and net output
Vacuum
Atmospheric air
Compressed air
Oxygen alone
Two times
Three times
Four times
Six times
1 bar
16 bar
64 bar
256 bar
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
3.5 : 1
5 : 1
8 : 1
12 : 1
Low frontal area
Higher thrust
High pressure rise
None of these
D₁/D₂ = (p₁ p₃)1/2
D₁/D₂ = (p₁/p₃)1/4
D₁/D₂ = (p₁ p₃)1/4
D₁/D₂ = (p₃/p₁)1/4
Increases the thermal efficiency
Increases the compressor work
Increases the turbine work
Decreases the thermal efficiency
Equal to
Less than
More than
None of these
Isothermal
Isentropic
Adiabatic
Isochoric
Ratio of shaft output of the air motor to the shaft input to the compressor
Ratio of shaft input to the compressor to the shaft output of air motor
Product of shaft output of air motor and shaft input to the compressor
None of the above
Can be driven at a very high speed
Produces uniform torque
Has more efficiency
All of these