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
C. The water enters the wheel at the outer periphery and then flows towards the centre of the wheel
Manometric efficiency
Mechanical efficiency
Overall efficiency
Volumetric efficiency
Pelton wheel
Kaplan turbine
Francis turbine
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
0 to 4.5
10 to 100
80 to 200
250 to 300
Inlet of draft rube
Blade inlet
Guide blade
Penstock
[wa (V - v)]/2g
[wa (V - v)]/g
[wa (V - v)²]/2g
[wa (V - v²)]/g
Accumulating oil
Supplying large quantities of oil for very short duration
Generally high pressures to operate hydraulic machines
Supplying energy when main supply fails
Horizontal
Nearly horizontal
Steep
First rise and then fall
Speed and power developed
Discharge and power developed
Speed and head of water
Speed, power developed and head of water
Low head
High head
High head and low discharge
Low head and high discharge
Friction loss
Cavitations
Static head
Loss of kinetic energy
0.25 m3/s
0.5 m3/s
1.5 m3/s
2.5 m3/s
At the top
At the bottom
At the canter
From sides
N√P / H3/2
N√P / H²
N√P / H5/4
N√P / H3
24.8 r.p.m.
48.2 r.p.m
82.4 r.p.m.
248 r.p.m
Diameter of jet to the diameter of Pelton wheel
Velocity of jet to the velocity of Pelton wheel
Diameter of Pelton wheel to the diameter of jet
Velocity of Pelton wheel to the velocity of jet
Suction pipe is short and pump is running at low speeds
Delivery pipe is long and pump is running at high speeds
Suction pipe is short and delivery pipe is long and the pump is running at low speeds
Suction pipe is long and delivery pipe is short and the pump is running at high speeds
2 to 4
4 to 8
8 to 16
16 to 24
Centrifugal
Axial flow
Mixed flow
Reciprocating
The suction pressure should be high
The delivery pressure should be high
The suction pressure should be low
The delivery pressure should be low
Power absorbing machines
Power developing machines
Energy transfer machines
Energy generating machines
P/ √H
P/ H
P/ H3/2
P/ H²
Low velocity
High velocity
Low pressure
High pressure
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
Same
0.75 B.H.P.
B.H.P./0.75
1.5 B.H.P.
Ratio of diameters
Square of ratio of diameters
Inverse ratio of diameters
Square of inverse ratio of diameters
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
0.25 kW
0.75 kW
1.75 kW
3.75 kW
4
6
8
12
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