Directly as the air or gas density
Inversely as square root of density
Inversely as density
As square of density
A. Directly as the air or gas density
Same
0.75 B.H.P.
B.H.P./0.75
1.5 B.H.P.
(w Hm) / (Q × ηo)
(w Hm Q) / ηo
(w Q) / (Hm × ηo)
(w Q ηo) / Hm
Propeller turbine
Francis turbine
Impulse turbine
None of the above
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
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
Geometric similarity
Kinematic similarity
Dynamic similarity
None of these
10-15°
20-25°
30-40°
50-60°
Adjustable blades
Backward curved blades
Vaned diffusion casing
Inlet guide blades
0.50 to 0.65
0.65 to 0.75
0.75 to 0.85
0.85 to 0.90
Kinetic head
Velocity head
Manometric head
Static head
[wa (V - v)]/2g
[wa (V - v)]/g
[wa (V - v)²]/2g
[wa (V - v²)]/g
Have identical velocities
Are equal in size and shape
Are identical in shape, but differ only in size
Have identical forces
Friction loss
Cavitations
Static head
Loss of kinetic energy
Directly as the air or gas density
Inversely as square root of density
Inversely as density
As square of density
175.4 r.p.m.
215.5 r.p.m.
241.5 r.p.m.
275.4 r.p.m
Centrifugal pump
Mixed flow pump
Axial flow pump
Any one of the above
An axial flow
An inward flow
An outward flow
A mixed flow
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
Diameter
Square of diameter
Cube of diameter
Fourth power of diameter
39.2 %
48.8 %
84.8 %
88.4 %
Centrifugal pump
Reciprocating pump
Air lift pump
Screw pump
No flow will take place
Cavitation will be formed
Efficiency will be low
Excessive power will be consumed
N√P / H3/2
N√P / H²
N√P / H5/4
N√P / H3
To transport water downstream without eddies
To convert the kinetic energy to flow energy by a gradual expansion of the flow cross-section
For safety of turbine
To increase flow rate
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.
Power absorbing machines
Power developing machines
Energy transfer machines
Energy generating machines
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
Waste valve closes suddenly
Supply pipe is long
Supply pipe is short
Ram chamber is large
The suction pressure should be high
The delivery pressure should be high
The suction pressure should be low
The delivery pressure should be low
0.15 to 0.3
0.4 to 0.5
0.6 to 0.9
1 to 1.5