Electric motor
Engine
Either (A) or (B)
None of these
C. Either (A) or (B)
Single stage compression
Multistage compression without intercooling
Multistage compression with intercooling
None of these
Increases
Decreases
Remain constant
First decreases and then increases
Gas turbine
I.C engine
Compressor
Air motor
W₁/W₂ = n₂(n₁ - 1)/n₁(n₂ - 1)
W₁/W₂ = n₁(n₂ - 1)/n₂(n₁ - 1)
W₁/W₂ = n₁/n₂
W₁/W₂ = n₂/n₁
0.5 kg
1.0 kg
1.3 kg
2.2 kg
Large quantity of air at high pressure
Small quantity of air at high pressure
Small quantity of air at low pressure
Large quantity of air at low pressure
Same
Less
More
None of these
Compressor capacity
Compression ratio
Compressor efficiency
Mean effective pressure
Lower at low speed
Higher at high altitudes
Same at all altitudes
Higher at high speed
34 %
50 %
60 %
72 %
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
Isothermal compression
Isentropic compression
Polytropic compression
None of these
Injecting water into the compressor
Burning fuel after gas turbine
Injecting ammonia into the combustion chamber
All of the above
Equal to zero
In the direction of motion of blades
Opposite to the direction of motion of blades
Depending on the velocity
Compression ratio
Work ratio
Pressure ratio
None of these
Same
Higher
Lower
Dependent on other factors
Work factor
Slip factor
Degree of reaction
Pressure coefficient
Isothermally
Adiabatically
Isentropically
Isochronically
Decreasing the compression work
Increasing the compression work
Increasing the turbine work
Both (A) and (C) above
Atmospheric
Slightly more than atmospheric
Slightly less than atmospheric
Pressure slightly less than atmospheric and temperature slightly more than atmospheric
Lowest
Highest
Anything
Atmospheric
Equal to
Less than
Greater than
None of these
Pressure coefficient
Work coefficient
Polytropic reaction
Slip factor
Increases the thermal efficiency
Increases the compressor work
Increases the turbine work
Decreases the thermal efficiency
p₂ = (p₁ + p₃)/2
p₂ = p₁. p₃
P₂ = Pa × p₃/p₁
p₂ = Pa p₃/p₁
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
Mass
Energy
Flow
Linear momentum
Reduced volume flow rate
Increased volume flow rate
Lower suction pressure
Lower delivery pressure
In one cylinder
In two cylinders
In a single cylinder on both sides of the piston
In two cylinders on both sides of the piston
Paucity of O2
Increasing gas temperature
High specific volume
High friction losses