Lowest
Highest
Anything
Atmospheric
D. Atmospheric
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
Low speeds
High speeds
Low altitudes
High altitudes
Employing intercooler
By constantly cooling the cylinder
By running compressor at very slow speed
By insulating the cylinder
Increases
Decreases
Remains same
Increases/decreases depending on compressor capacity
3.5 : 1
5 : 1
8 : 1
12 : 1
Work factor
Slip factor
Degree of reaction
Pressure coefficient
Lowest
Highest
Anything
Atmospheric
Same as isothermal
Same as adiabatic
Better than isothermal and adiabatic
In between isothermal and adiabatic
The ratio of stroke volume to clearance volume
The ratio of the air actually delivered to the amount of piston displacement
Reciprocal of compression ratio
Index of compressor performance
p₂/p₁ = p₃/p₂ = p₄/p₃
p₃/p₁ = p₄/p₂
p₁ p₂ = p₃ p₄
p₁ p₃ = p₂ p₄
At very high speed
At very slow speed
At average speed
At zero speed
200°C
500°C
700°C
1000°C
p₂ = (p₁ + p₃)/2
p₂ = p₁. p₃
P₂ = Pa × p₃/p₁
p₂ = Pa p₃/p₁
Equal to zero
In the direction of motion of blades
Opposite to the direction of motion of blades
Depending on the velocity
Slip factor
Velocity factor
Velocity coefficient
None of the above
Gauge discharge pressure to the gauge intake pressure
Absolute discharge pressure to the absolute intake pressure
Pressures at discharge and suction corresponding to same temperature
Stroke volume and clearance volume
Equal to
Double
Three times
Six times
To increase the output
To increase the efficiency
To save fuel
To reduce the exit temperature
Compresses 3 m³/min of standard air
Compresses 3 m³/ min of free air
Delivers 3 m³/ min of compressed air
Delivers 3 m³/ min of compressed air at delivery pressure
Compressor pressure ratio
Highest pressure to exhaust pressure
Inlet pressure to exhaust pressure
Pressures across the turbine
700°C
2000°C
1500°C
1000°C
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
1 : 1
2 : 1
4 : 1
1 : 6
Atmosphere
Back to the compressor
Discharge nozzle
Vacuum
The propulsive matter is ejected from within the propelled body
The propulsive matter is caused to flow around the propelled body
Its functioning does not depend upon presence of air
None of the above
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
Mass
Energy
Flow
Linear momentum
As large as possible
As small as possible
About 50% of swept volume
About 100% of swept volume
Turbojet
Turbo-propeller
Rocket
Ramjet
kg/m²
kg/m³
m³/min
m³/kg