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
C. The speed if the turbine runner is allowed to revolve freely without load and with the wicket gates wide open
Low head
High head
High head and low discharge
Low head and high discharge
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
Directly proportional to N
Inversely proportional to N
Directly proportional to N²
Inversely proportional to N²
Hydraulic
Mechanical
Overall
None of these
10-15°
20-25°
30-40°
50-60°
The centrifugal pump is suitable for large discharge and smaller heads.
The centrifugal pump requires less floor area and simple foundation as compared to reciprocating pump.
The efficiency of centrifugal pump is less as compared to reciprocating pump.
All of the above
Designing new impeller
Trimming the impeller size to the required size by machining
Not possible
Some other alterations in the impeller
Delivers unit discharge under unit head
Delivers unit discharge under unit speed
Develops unit power under unit head
Develops unit power under unit speed
waVr /g × (Vr + v)
waVr /g × (Vr - v)
waVr /g × (Vr + v)²
waVr /g × (Vr - v)²
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
Centrifugal
Axial flow
Reciprocating
Mixed flow
Horizontal
Nearly horizontal
Steep
First rise and then fall
39.2 %
49.2 %
68.8 %
84.8 %
40 %
50 %
60 %
80 %
0.25 m3/s
0.5 m3/s
1.5 m3/s
2.5 m3/s
102 watts
75 watts
550 watts
735 watts
24.8 r.p.m.
48.2 r.p.m
82.4 r.p.m.
248 r.p.m
0.25 kW
0.75 kW
1.75 kW
3.75 kW
Friction loss
Cavitations
Static head
Loss of kinetic energy
Net head
Absolute velocity
Blade velocity
Flow
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
Directly as the air or gas density
Inversely as square root of density
Inversely as density
As square of density
Give high discharge
Produce high heads
Pump viscous fluids
All of these
Proportional to diameter of impeller
Proportional to speed of impeller
Proportional to diameter and speed of impeller
None of the above
Strain
Pressure
Kinetic
None 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
waV/2g × sinθ
waV/g × sinθ
waV²/2g × sin2θ
waV²/g × sinθ
Directly proportional to diameter of its impeller
Inversely proportional to diameter of its impeller
Directly proportional to (diameter)² of its impeller
Inversely proportional to (diameter)² of its impeller
Pelton wheel
Francis turbine
Kaplan turbine
None of these
Radial
Axial
Centrifugal
Vortex