Same
One-half
One fourth
One sixth
D. One sixth
High calorific value
Ease of atomisation
Low freezing point
Both (A) and (C) above
Increases with decrease in compression ratio
Decreases with decrease in compression ratio
Increases with increase in compression ratio
Decreases with increase in compression ratio
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
In gas turbine plants
For operating pneumatic drills
In starting and supercharging of I.C. engines
All of the above
To accommodate Valves in the cylinder head
To provide cushioning effect
To attain high volumetric efficiency
To provide cushioning effect and also to avoid mechanical bang of piston with cylinder head
Brayton or Atkinson cycle
Carnot cycle
Rankine cycle
Erricson cycle
Large gas turbines use radial inflow turbines
Gas turbines have their blades similar to steam turbine
Gas turbine's blade will appear as impulse section at the hub and as a reaction section at tip
Gas turbines use both air and liquid cooling
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
Thrust and range of aircraft
Efficiency of the engine
Both (A) and (B)
None of these
1.03 kg/cm²
1.06 kg/cm²
1.00 kg/cm²
0.53 kg/cm²
There is no pressure drop in the intercooler
The compression in both the cylinders is polytropic
The suction and delivery of air takes place at constant pressure
All of the above
3 m³/ mt.
1.5 m³/ mt.
18 m³/ mt.
6 m³/ mt.
Atmospheric conditions at any specific location
20°C and 1 kg/cm² and relative humidity of 36%
0°C and standard atmospheric conditions
15°C and 1 kg/cm²
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
In two phases
In three phases
In a single phase
In the form of air and water mixture
Thrust power and fuel energy
Engine output and propulsive power
Propulsive power and fuel input
Thrust power and propulsive power
It is inefficient
It is bulky
It requires cooling water for its operation
None of the above
D₁/D₂ = p₁ p₂
D₁/D₂ = p₁/p₂
D₁/D₂ = p₂/p₁
None of these
Compressor capacity
Compression ratio
Compressor efficiency
Mean effective pressure
Top side of main
Bottom side of main
Left side of main
Right side of main
Equal to
Less than
More than
None of these
Two times
Three times
Four times
Six times
Control temperature
Control output of turbine
Control fire hazards
Increase efficiency
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
Compressor efficiency
Isothermal efficiency
Volumetric efficiency
Mechanical efficiency
Inlet whirl velocity
Outlet whirl velocity
Inlet velocity of flow
Outlet velocity of flow
H.P. compressor is connected to H.P. turbine and L.P. compressor to L.P. turbine
H.P. compressor is connected to L.P. turbine and L.P. compressor is connected to H.P. turbine
Both the arrangements can be employed
All are connected in series
As large as possible
As small as possible
About 50% of swept volume
About 100% of swept volume
Lower heating value
Higher heating value
Heating value
Higher calorific value
Zero
Less
More
Same