39.2 %
49.2 %
68.8 %
84.8 %
A. 39.2 %
Sum
Difference
Product
None of these
Centrifugal pump
Reciprocating pump
Air lift pump
Screw pump
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
Directly proportional
Inversely proportional
4th power
None of these
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
Slow speed with radial flow at outlet
Medium speed with radial flow at outlet
High speed with radial flow at outlet
High speed with axial flow at outlet
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
Strain
Pressure
Kinetic
None of these
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
Ratio of diameters
Square of ratio of diameters
Inverse ratio of diameters
Square of inverse ratio of diameters
Low head of water
High head of water
Medium head of water
High discharge
Smoothen flow
Reduce acceleration to minimum
Increase pump efficiency
Save pump from cavitations
Give high discharge
Produce high heads
Pump viscous fluids
All of these
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
Q = π.D.Vf
Q = π.b.Vf
Q = π.D.bf.V
Q = D.b.Vf
Geometric similarity
Kinematic similarity
Dynamic similarity
None of these
Propeller turbine
Francis turbine
Impulse turbine
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
Propeller turbine
Francis turbine
Impulse turbine
Any one of the above
Kept fully closed
Kept fully open
Irrespective of any position
Kept 50% open
0.25 kW
0.75 kW
1.75 kW
3.75 kW
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
39.2 %
48.8 %
84.8 %
88.4 %
At the level of tail race
Little above the tail race
Slightly below the tail race
About 2.5 m above the tail race to avoid cavitations.
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
An axial flow
An inward flow
An outward flow
A mixed flow
Kinetic head
Velocity head
Manometric head
Static head
Impulse turbines
Reaction turbines
Axial flow turbines
Mixed flow turbines
Diameter
Square of diameter
Cube of diameter
Fourth power of diameter