High h.p. and low weight
Low weight and small frontal area
Small frontal area and high h.p.
High speed and high h.p
B. Low weight and small frontal area
They can generate very high thrust
They have high propulsion efficiency
These engines can work on several fuels
They are not air breathing engines
Surrounding air
Compressed atmospheric air
Its own oxygen
None of these
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
Compressor efficiency
Volumetric efficiency
Isothermal efficiency
Mechanical efficiency
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
Increase of work ratio
Decrease of thermal efficiency
Decrease of work ratio
Both (A) and (B) above
Rise gradually towards the point of use
Drop gradually towards the point of use
Be laid vertically
Be laid exactly horizontally
W₁/W₂ = n₂(n₁ - 1)/n₁(n₂ - 1)
W₁/W₂ = n₁(n₂ - 1)/n₂(n₁ - 1)
W₁/W₂ = n₁/n₂
W₁/W₂ = n₂/n₁
Compressor pressure ratio
Highest pressure to exhaust pressure
Inlet pressure to exhaust pressure
Pressures across the turbine
One air stream
Two or more air streams
No air stream
Solid fuel firing
Same
Lower
Higher
None of these
Lower at low speed
Higher at high altitudes
Same at all altitudes
Higher at high speed
In two phases
In three phases
In a single phase
In the form of air and water mixture
Increases the thermal efficiency
Increases the compressor work
Increases the turbine work
Decreases the thermal 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
Increases with increase in compression ratio
Decreases with increase in compression ratio
Is not dependent upon compression ratio
May increase/decrease depending on compressor capacity
Inlet losses
Impeller channel losses
Diffuser losses
All of the above
3.5 : 1
5 : 1
8 : 1
12 : 1
Increases
Decreases
First increases and then decreases
First decreases and then increases
Equal to
Double
Three times
Six times
Mechanical efficiency
Volumetric efficiency
Isothermal efficiency
Adiabatic efficiency
Brayton or Atkinson cycle
Rankine cycle
Carnot cycle
Erricson cycle
Compressor capacity
Compression ratio
Compressor efficiency
Mean effective pressure
Has no effect on
Decreases
Increases
None of these
Vi = Vo
Vt > Vo
U < Vo
V = Uo
Low speeds
High speeds
Low altitudes
High altitudes
Equal to
Less than
More than
None of these
Isothermal
Isentropic
Adiabatic
Isochoric
kg/m²
kg/m³
m³/min
m³/kg
Inlet whirl velocity
Outlet whirl velocity
Inlet velocity of flow
Outlet velocity of flow