Centrifugal pump
Reciprocating pump
Jet pump
Air lift pump
D. Air lift pump
Directly proportional to H1/2
Inversely proportional to H1/2
Directly proportional to H3/2
Inversely proportional to H3/2
Manometric efficiency
Mechanical efficiency
Overall efficiency
Volumetric efficiency
Smoothen flow
Reduce acceleration to minimum
Increase pump efficiency
Save pump from cavitations
Adjustable blades
Backward curved blades
Vaned diffusion casing
Inlet guide blades
Directly proportional to N
Inversely proportional to N
Directly proportional to N²
Inversely proportional to N²
Kept fully closed
Kept fully open
Irrespective of any position
Kept 50% open
(w Hm) / (Q × ηo)
(w Hm Q) / ηo
(w Q) / (Hm × ηo)
(w Q ηo) / Hm
Casing
Delivery pipe
Suction pipe
Impeller
Air lift pump
Jet pump
Hydraulic coupling
Hydraulic press
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
Give high discharge
Produce high heads
Pump viscous fluids
All of these
Have identical velocities
Are equal in size and shape
Are identical in shape, but differ only in size
None of the above
No flow will take place
Cavitation will be formed
Efficiency will be low
Excessive power will be consumed
0 to 4.5
10 to 100
80 to 200
250 to 300
Low velocity
High velocity
Low pressure
High pressure
Smoothen the flow
Reduce suction head
Increase delivery head
Reduce acceleration head
Impeller diameter
Speed
Fluid density
Both (A) and (B) above
Closed
Open
Depends on starting condition and flow desired
Could be either open or closed
(W/p) × (A/a)
(p/W) × (a/A)
(W/p) × (a/A)
(p/W) × (A/a)
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
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
Directly as the air or gas density
Inversely as square root of density
Inversely as density
As square of density
Medium head application from 24 to 180 m
Low head installation up to 30 m
High head installation above 180 m
All types of heads
Lift and resultant force
Drag and resultant force
Lift and tangential force
Lift and drag
Discharge a diameter
Head a speed²
Head a diameter
Power a speed⁴
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
Low head
High head
High head and low discharge
Low head and high discharge
Diameter
Square of diameter
Cube of diameter
Fourth power of diameter
Have identical velocities
Are equal in size and shape
Are identical in shape, but differ only in size
Have identical forces
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.