Adiabatic temperature drop in the stage
Total temperature drop
Total temperature drop in the stage
Total adiabatic temperature drop
C. Total temperature drop in the stage
Remain same
Decrease
Increase
None of the above
1 bar
16 bar
64 bar
256 bar
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
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
3 m³/ mt.
1.5 m³/ mt.
18 m³/ mt.
6 m³/ mt.
Isothermal compression
Isentropic compression
Polytropic compression
None of these
Lower power consumption per unit of air delivered
Higher volumetric efficiency
Decreased discharge temperature
All of the above
Constant volume
Constant temperature
Constant pressure
None of these
Isothermal
Isentropic
Adiabatic
Isochoric
Compressor efficiency
Isentropic efficiency
Euler's efficiency
Pressure coefficient
Centrifugal
Reciprocating
Axial
Screw
Radial flow compressor
Axial flow compressor
Roots blower
Reciprocating compressor
Large gas turbines employ axial flow compressors
Axial flow compressors are more stable than centrifugal type compressors but not as efficient
Axial flow compressors have high capacity and efficiency
Axial flow compressors have instability region of operation
Free air delivery
Compressor capacity
Swept volume
None of these
20 - 30 %
40 - 50 %
60 - 70 %
70 - 90 %
75 %
85 %
90 %
99 %
High calorific value
Ease of atomisation
Low freezing point
Both (A) and (C) above
Increase of work ratio
Decrease of thermal efficiency
Decrease of work ratio
Both (A) and (B) above
N.T.P. conditions
Intake temperature and pressure conditions
0°C and 1 kg/cm²
20°C and 1 kg/cm²
Inlet whirl velocity
Outlet whirl velocity
Inlet velocity of flow
Outlet velocity of flow
Compressor work and turbine work
Output and input
Actual total head temperature drop to the isentropic total head drop from total head inlet to static head outlet
Actual compressor work and theoretical compressor work
Large discharge at high pressure
Low discharge at high pressure
Large discharge at low pressure
Low discharge at low pressure
0.1 bar and 20°C
1 bar and 20°C
0.1 bar and 40°C
1 bar and 40°C
p₂/p₁ = p₃/p₂ = p₄/p₃
p₃/p₁ = p₄/p₂
p₁ p₂ = p₃ p₄
p₁ p₃ = p₂ p₄
Small quantities of air at high pressures
Large quantities of air at high pressures
Small quantities of air at low pressures
Large quantities of air at low pressures
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
p₂ = (p₁ + p₃)/2
p₂ = p₁. p₃
P₂ = Pa × p₃/p₁
p₂ = Pa p₃/p₁
550 km/hr
1050 km/hr
1700 km/hr
2400 km/hr
Same
Less
More
None of these
Centrifugal pump
Reciprocating pump
Turbine
Sliding vane compressor