Back pressure
Critical pressure
Discharge pressure
None of these
C. Discharge pressure
Work factor
Slip factor
Degree of reaction
Pressure coefficient
2 : 1
4 :1
61 : 1
9 : 1
10 bar
20 bar
30 bar
50 bar
Compressor efficiency
Isothermal efficiency
Volumetric efficiency
Mechanical efficiency
Reciprocating compressor
Centrifugal compressor
Axial flow compressor
Turbo compressor
Thrust power and fuel energy
Engine output and propulsive power
Propulsive power and fuel input
Thrust power and propulsive power
Before intercooler
After intercooler
After receiver
Between after-cooler and air receiver
Does not change
Increases
Decreases
First decrease and then increase
From an air conditioned room maintained at 20°C
From outside atmosphere at 1°C
From coal yard side
From a side where cooling tower is located nearby
Compressor pressure ratio
Highest pressure to exhaust pressure
Inlet pressure to exhaust pressure
Pressures across the turbine
Same
More
Less
Zero
D₁/D₂ = p₁ p₂
D₁/D₂ = p₁/p₂
D₁/D₂ = p₂/p₁
None of these
Carbonisation of coal
Passing steam over incandescent coke
Passing air and a large amount of steam over waste coal at about 65°C
Partial combustion of coal, eke, anthracite coal or charcoal in a mixed air steam blast
Parallel
Perpendicular
Inclined
None of these
To supply base load requirements
To supply peak load requirements
To enable start thermal power plant
In emergency
Isothermal
Adiabatic
Polytropic
None of the above
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
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
Constant volume
Constant temperature
Constant pressure
None of these
Back pressure
Critical pressure
Discharge pressure
None of these
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
The combustion chamber in a rocket engine is directly analogous to the reservoir of a supersonic wind tunnel
The stagnation conditions exist at the combustion chamber
The exit velocities of exhaust gases are much higher than those in jet engine
All of the above
The atmosphere
A source at 0°C
A source of low temperature air
A source of high temperature air
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
Isothermal h.p. to the BHP of motor
Isothermal h.p. to adiabatic h.p.
Power to drive compressor to isothermal h.p.
Work to compress air isothermally to work for actual compression
Increase
Decrease
Remain same
May increase or decrease depending on clearance volume
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
Rise gradually towards the point of use
Drop gradually towards the point of use
Be laid vertically
Be laid exactly horizontally
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
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