Directly as fan speed
Square of fan speed
Cube of fan speed
Square root of fan speed
B. Square of fan speed
To run the turbine full
To prevent air to enter the turbine
To increase the head of water by an amount equal to the height of the runner outlet above the tail race
To transport water to downstream
Proportional to diameter of impeller
Proportional to speed of impeller
Proportional to diameter and speed of impeller
None of the above
An axial flow
An inward flow
An outward flow
A mixed flow
Casing
Delivery pipe
Suction pipe
Impeller
Same quantity of liquid
0.75 Q
Q/0.75
1.5 Q
0.26
0.36
0.46
0.56
Same
0.75 B.H.P.
B.H.P./0.75
1.5 B.H.P.
High discharge
High head
Pumping of viscous fluids
High head and high discharge
At the top
At the bottom
At the canter
From sides
0 to 4.5
10 to 100
80 to 200
250 to 300
waV / 2g
waV / g
waV² / 2g
waV² / g
Give high discharge
Produce high heads
Pump viscous fluids
All of these
Q = π.D.Vf
Q = π.b.Vf
Q = π.D.bf.V
Q = D.b.Vf
waVr /g × (Vr + v)
waVr /g × (Vr - v)
waVr /g × (Vr + v)²
waVr /g × (Vr - v)²
Rotational flow
Radial
Forced spiral vortex flow
Spiral vortex flow
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.
[2(Vr - v) v]/ Vr²
2(Vr + v) v]/ Vr²
[(Vr - v) v]/ Vr
[(Vr + v) v]/ Vr
(D/2d) + 5
(D/2d) + 10
(D/2d) + 15
(D/2d) + 20
Power absorbing machines
Power developing machines
Energy transfer machines
Energy generating machines
Two jets
Two runners
Four jets
Four runners
Discharge a diameter
Head a speed²
Head a diameter
Power a speed⁴
Air lift pump
Jet pump
Hydraulic coupling
Hydraulic press
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
Designing new impeller
Trimming the impeller size to the required size by machining
Not possible
Some other alterations in the impeller
Pelton wheel
Kaplan turbine
Francis turbine
None of these
Propeller turbine
Francis turbine
Impulse turbine
None of the above
Waste valve closes suddenly
Supply pipe is long
Supply pipe is short
Ram chamber is large
Fourneyron turbine
Journal turbine
Thomson's turbine
Pelton wheel
Directly as the air or gas density
Inversely as square root of density
Inversely as density
As square of density
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