Strain
Pressure
Kinetic
None of these
B. Pressure
To store pressure energy which may be supplied to a machine later on
To increase the intensity of pressure of water by means of energy available from a large quantity of water at a low pressure
To lift larger load by the application of a comparatively much smaller force
All of the above
Full load speed
The speed at which turbine runner will be damaged
The speed if the turbine runner is allowed to revolve freely without load and with the wicket gates wide open
The speed corresponding to maximum overload permissible
Centrifugal pump
Reciprocating pump
Jet pump
Airlift pump
No flow will take place
Cavitation will be formed
Efficiency will be low
Excessive power will be consumed
Radial
Axial
Centrifugal
Vortex
In an impulse turbine, the water impinges on the buckets with pressure energy.
In a reaction turbine, the water glides over the moving vanes with kinetic energy.
In an impulse turbine, the pressure of the flowing water remains unchanged and is equal to atmospheric pressure.
In a reaction turbine, the pressure of the flowing water increases after gliding over the vanes.
Q = π.D.Vf
Q = π.b.Vf
Q = π.D.bf.V
Q = D.b.Vf
Directly as the air or gas density
Inversely as square root of density
Inversely as density
As square of density
Volute casing
Volute casing with guide blades
Vortex casing
Any one of these
Manometric efficiency
Mechanical efficiency
Overall efficiency
Volumetric efficiency
Diameter
Square of diameter
Cube of diameter
Fourth power of diameter
Pelton wheel with one nozzle
Pelton wheel with two or more nozzles
Kaplan turbine
Francis turbine
39.2 %
49.2 %
68.8 %
84.8 %
(w Hm) / (Q × ηo)
(w Hm Q) / ηo
(w Q) / (Hm × ηo)
(w Q ηo) / Hm
Velocity of flow at inlet to the theoretical jet velocity
Theoretical velocity of jet to the velocity of flow at inlet
Velocity of runner at inlet to the velocity of flow at inlet
None of the above
Energy available at the impeller to the energy supplied to the pump by the prime mover
Actual workdone by the pump to the energy supplied to the pump by the prime mover
Energy supplied to the pump to the energy available at the impeller
Manometric head to the energy supplied by the impeller per kN of water
Suction lift + Loss of head in suction pipe due to friction + Delivery lift + Loss of head in delivery pipe due to friction + Velocity head in the delivery pipe
Workdone per kN of water Losses within the impeller
Energy per kN at outlet of impeller Energy per kN at inlet of impeller
All of the above
Have identical velocities
Are equal in size and shape
Are identical in shape, but differ only in size
None of the above
Have identical velocities
Are equal in size and shape
Are identical in shape, but differ only in size
Have identical forces
The water flows parallel to the axis of the wheel
The water enters at the centre of the wheel and then flows towards the outer periphery of the wheel
The water enters the wheel at the outer periphery and then flows towards the centre of the wheel
The flow of water is partly radial and partly axial
Ratio of diameters
Square of ratio of diameters
Inverse ratio of diameters
Square of inverse ratio of diameters
Increases with increase in pressure
Decreases with increase in pressure
More or less remains constant with increase in pressure
Unpredictable
Propeller turbine
Francis turbine
Impulse turbine
Any one of the above
Directly as the air or gas density
Inversely as square root of density
Inversely as density
As square of density
0.15 to 0.3
0.4 to 0.5
0.6 to 0.9
1 to 1.5
Greater than 15°
Greater than 8°
Greater than 5°
Less than 8°
Decreases
Increases
Remain same
None of these
Kept fully closed
Kept fully open
Irrespective of any position
Kept 50% open
Ratio of the actual power produced by the turbine to the energy actually supplied by the turbine
Ratio of the actual work available at the turbine to the energy imparted to the wheel
Ratio of the work done on the wheel to the energy of the jet
None of the above
Hydraulic
Mechanical
Overall
None of these