Store the energy of water
Increase the pressure of water
To lift water from deep wells
To lift small quantity of water to a greater height when a large quantity of water is available at a smaller height
D. To lift small quantity of water to a greater height when a large quantity of water is available at a smaller height
At full load
At which there will be no damage to the runner
Corresponding to maximum overload permissible
At which the turbine will run freely without load
Allow the water to enter the runner without shock
Allow the water to flow over them, without forming eddies
Allow the required quantity of water to enter the turbine
All of the above
Equal to
1.2 times
1.8 times
Double
39.2 %
48.8 %
84.8 %
88.4 %
Q = π.D.Vf
Q = π.b.Vf
Q = π.D.bf.V
Q = D.b.Vf
Slow speed pump with radial flow at outlet
Medium speed pump with radial flow at outlet
High speed pump with radial flow at outlet
High speed pump with axial flow at outlet
Diameter
Square of diameter
Cube of diameter
Fourth power of diameter
Kept fully closed
Kept fully open
Irrespective of any position
Kept 50% open
An axial flow
An inward flow
An outward flow
A mixed flow
Directly as the air or gas density
Inversely as square root of density
Inversely as density
As square of density
Centrifugal
Axial flow
Reciprocating
Mixed flow
0 to 4.5
10 to 100
80 to 200
250 to 300
Directly proportional to H1/2
Inversely proportional to H1/2
Directly proportional to H3/2
Inversely proportional to H3/2
The wheel runs entirely by the weight of water
The wheel runs entirely by the impulse of water
The wheel runs partly by the weight of water and partly by the impulse of water
None of the above
Discharge a diameter
Head a speed²
Head a diameter
Power a speed⁴
Ratio of diameters
Square of ratio of diameters
Inverse ratio of diameters
Square of inverse ratio of diameters
Two cylinders, two rams and a storage device
A cylinder and a ram
Two coaxial rams and two cylinders
A cylinder, a piston, storage tank and control valve
Ratio of actual discharge to the theoretical discharge
Sum of actual discharge and the theoretical discharge
Difference of theoretical discharge and the actual discharge
Product of theoretical discharge and the actual discharge
0.15 to 0.3
0.4 to 0.5
0.6 to 0.9
1 to 1.5
Low velocity
High velocity
Low pressure
High pressure
To break the jet of water
To bring the runner to rest in a short time
To change the direction of runner
None of these
No flow will take place
Cavitation will be formed
Efficiency will be low
Excessive power will be consumed
Greater than 15°
Greater than 8°
Greater than 5°
Less than 8°
4
6
8
12
0 to 25 m
25 m to 250 m
Above 250 m
None of these
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
Impulse turbines
Reaction turbines
Axial flow turbines
Mixed flow turbines
[wa (V - v)]/2g
[wa (V - v)]/g
[wa (V - v)²]/2g
[wa (V - v²)]/g
Q/√H
Q/H
Q/H3/2
Q/H²
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