Liquid hydrogen
High speed diesel oil
Kerosene
Methyl alcohol
C. Kerosene
Mass flow rate
Pressure ratio
Change in load
Stagnation pressure at the outlet
Low frontal area
Higher thrust
High pressure rise
None of these
34 %
50 %
60 %
72 %
1 : 1
2 : 1
4 : 1
1 : 6
Closed cycle
Open cycle
Both of the above
Closed/open depending on other considerations
Vi = Vo
Vt > Vo
U < Vo
V = Uo
Carries its own oxygen
Uses surrounding air
Uses compressed atmospheric air
Does not require oxygen
Less power requirement
Better mechanical balance
Less loss of air due to leakage past the cylinder
Lower volumetric efficiency
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
1 - k + k (p₁/p₂)1/n
1 + k - k (p₂/p₁)1/n
1 - k + k (p₁/p₂) n- 1/n
1 + k - k (p₂/p₁) n-1/n
A.C. electric motor
Compressed air
Petrol engine
Diesel engine
Brayton or Atkinson cycle
Rankine cycle
Carnot cycle
Erricson cycle
Gas turbine is a self starting unit
Gas turbine does not require huge quantity of water like steam plant
Exhaust losses in gas turbine are high due to large mass flow rate
Overall efficiency of gas turbine plant is lower than that of a reciprocating engine
Back pressure
Critical pressure
Discharge pressure
None of these
Compression ratio
Expansion ratio
Compressor efficiency
Volumetric efficiency
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
At very high speed
At very slow speed
At average speed
At zero speed
Free air delivery
Compressor capacity
Swept volume
None of these
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
Slip factor
Velocity factor
Velocity coefficient
None of the above
1
1.2
1.3
1.4
Lowest
Highest
Anything
Atmospheric
Less
More
Same
More/less depending on compressor capacity
1 bar
16 bar
64 bar
256 bar
D₁/D₂ = (p₁ p₃)1/2
D₁/D₂ = (p₁/p₃)1/4
D₁/D₂ = (p₁ p₃)1/4
D₁/D₂ = (p₃/p₁)1/4
200°C
500°C
700°C
1000°C
Increase temperature
Reduce turbine size
Increase power output
Increase speed
Centrifugal compressor
Axial compressor
Pumps
All of the above
Increases thermal efficiency
Allows high compression ratio
Decreases heat loss is exhaust
Allows operation at very high altitudes
In a two stage reciprocating air compressor with complete intercooling, maximum work is saved.
The minimum work required for a two stage reciprocating air compressor is double the work required for each stage.
The ratio of the volume of free air delivery per stroke to the swept volume of the piston is called volumetric efficiency.
None of the above