Brayton or Atkinson cycle
Carnot cycle
Rankine cycle
Erricson cycle
A. Brayton or Atkinson cycle
Vacuum
Atmospheric air
Compressed air
Oxygen alone
Compressor efficiency
Isentropic efficiency
Euler's efficiency
Pressure coefficient
Pressure coefficient
Work coefficient
Polytropic reaction
Slip factor
No flow of air
Fixed mass flow rate regardless of pressure ratio
Reducing mass flow rate with increase in pressure ratio
Increased inclination of chord with air steam
Zero
Less
More
Same
p₂ = p₁ × p₃
p₂ = p₁/p₃
p₂ = p₁ × p₂
p₂ = p₃/p₁
Net work output and work done by turbine
Net work output and heat supplied
Work done by turbine and heat supplied
Work done by turbine and net work output
Increases the thermal efficiency
Increases the compressor work
Increases the turbine work
Decreases the thermal efficiency
0.1 %
0.5 %
1 %
5 %
Centrifugal pump
Reciprocating pump
Turbine
Sliding vane compressor
Larger air handling ability per unit frontal area
Higher pressure ratio per stage
Aerofoil blades are used
Higher average velocities
1 : 1
2 : 1
4 : 1
1 : 6
Directly proportional to clearance volume
Greatly affected by clearance volume
Not affected by clearance volume
Inversely proportional to clearance volume
Reduction of speed of incoming air and conversion of part of it into pressure energy
Compression of inlet air
Increasing speed of incoming air
Lost work
They can generate very high thrust
They have high propulsion efficiency
These engines can work on several fuels
They are not air breathing engines
Mass flow rate
Pressure ratio
Change in load
Stagnation pressure at the outlet
Isothermally
Adiabatically
Isentropically
Isochronically
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
Closed cycle gas turbine is an I.C engine
Gas turbine uses same working fluid over and over again
Ideal efficiency of closed cycle gas turbine plant is more than Carnot cycle efficiency
Thrust in turbojet is produced by nozzle exit gases.
Free air delivery
Compressor capacity
Swept volume
None of these
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
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
High calorific value
Ease of atomisation
Low freezing point
Both (A) and (C) above
Less
More
Same
May be less or more depending on ambient conditions
Is self operating at zero flight speed
Is not self operating at zero flight speed
Requires no air for its operation
Produces a jet consisting of plasma
W₁/W₂ = n₂(n₁ - 1)/n₁(n₂ - 1)
W₁/W₂ = n₁(n₂ - 1)/n₂(n₁ - 1)
W₁/W₂ = n₁/n₂
W₁/W₂ = n₂/n₁
The atmosphere
A source at 0°C
A source of low temperature air
A source of high temperature air
Lowest
Highest
Anything
Atmospheric
Actual volume of the air delivered by the compressor when reduced to normal temperature and pressure conditions
Volume of air delivered by the compressor
Volume of air sucked by the compressor during its suction stroke
None of the above
Decreases
Increases
Does not change
None of these