700°C
2000°C
1500°C
1000°C
A. 700°C
Single stage compression
Multistage compression without intercooling
Multistage compression with intercooling
None of these
Equal to
Less than
Greater than
None of these
Compression ratio
Expansion ratio
Compressor efficiency
Volumetric efficiency
W₁/W₂ = n₂(n₁ - 1)/n₁(n₂ - 1)
W₁/W₂ = n₁(n₂ - 1)/n₂(n₁ - 1)
W₁/W₂ = n₁/n₂
W₁/W₂ = n₂/n₁
Liquid hydrogen
High speed diesel oil
Kerosene
Methyl alcohol
Isothermal
Polytropic
Isentropic
Any one of these
To increase the output
To increase the efficiency
To save fuel
To reduce the exit temperature
6000 KW
15 KW
600 KW
150 KW
Increases
Decreases
Remain unaffected
May increase or decrease depending on compressor capacity
Parallel
Perpendicular
Inclined
None of these
10 : 1
15 : 1
20 : 1
60 : 1
1 : 1.2
1 : 2
1 : 5
1 : 10
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
Equal to
Less than
More than
None of these
Back pressure
Critical pressure
Discharge pressure
None of these
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
Slip factor
Velocity factor
Velocity coefficient
None of the above
Same
Lower
Higher
None of these
Increases the thermal efficiency
Increases the compressor work
Increases the turbine work
Decreases the thermal efficiency
Before the intercooler
After the intercooler
Between the aftercooler and receiver
Before first stage suction
Closed cycle
Open cycle
Both of the above
Closed/open depending on other considerations
(p₁ - p₂)/2
(p₁ + p₂)/2
p₁/p₂
p₁ p₂
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
High calorific value
Ease of atomisation
Low freezing point
Both (A) and (C) above
The propulsive matter is caused to flow around the propelled body
Propulsive matter is ejected from within the propelled body
Its functioning does not depend on presence of air
All of the above
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
Brayton or Atkinson cycle
Rankine cycle
Carnot cycle
Erricson cycle
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
Atmospheric conditions at any specific location
20°C and 1 kg/cm² and relative humidity 36%
0°C and standard atmospheric conditions
15°C and 1 kg/cm²
7 : 1
15 : 1
30 : 1
50 : 1.