Low head
High head
High head and low discharge
Low head and high discharge
D. Low head and high discharge
Directly as fan speed
Square of fan speed
Cube of fan speed
Square root of fan speed
Directly proportional
Inversely proportional
4th power
None of these
2V/(vr - v)
2V/(vr + v)
V/(vr - v)
V/(vr + v)
39.2 %
49.2 %
68.8 %
84.8 %
Low head of water
High head of water
Medium head of water
High discharge
10 r.p.m.
20 r.p.m.
40 r.p.m.
80 r.p.m.
Waste valve closes suddenly
Supply pipe is long
Supply pipe is short
Ram chamber is large
Directly as fan speed
Square of fan speed
Cube of fan speed
Square root of fan speed
Delivers unit discharge under unit head
Delivers unit discharge under unit speed
Develops unit power under unit head
Develops unit power under unit speed
Decreases
Increases
Remain same
None of these
Same quantity of liquid
0.75 Q
Q/0.75
1.5 Q
0.15 to 0.3
0.4 to 0.5
0.6 to 0.9
1 to 1.5
0.25 kW
0.75 kW
1.75 kW
3.75 kW
Directly proportional to N
Inversely proportional to N
Directly proportional to N²
Inversely proportional to N²
39.2 %
48.8 %
84.8 %
88.4 %
Directly proportional to H1/2
Inversely proportional to H1/2
Directly proportional to H3/2
Inversely proportional to H3/2
Centrifugal pump
Axial flow pump
Mixed flow pump
Reciprocating pump
Give high discharge
Produce high heads
Pump viscous fluids
All of these
Screw pump
Gear pump
Cam and piston pump
Plunger pump
Air lift pump
Jet pump
Hydraulic coupling
Hydraulic press
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.
Propeller turbine
Francis turbine
Impulse turbine
Any one of the above
At full load
At which there will be no damage to the runner
Corresponding to maximum overload permissible
At which the turbine will run freely without load
Smoothen flow
Reduce acceleration to minimum
Increase pump efficiency
Save pump from cavitations
24.8 r.p.m.
48.2 r.p.m
82.4 r.p.m.
248 r.p.m
Velocity of flow at inlet to the theoretical jet velocity
Theoretical velocity of jet to the velocity of flow at inlet
Velocity of runner at inlet to the velocity of flow at inlet
None of the above
Strain
Pressure
Kinetic
None of these
waV/2g × sinθ
waV/g × sinθ
waV²/2g × sin2θ
waV²/g × sinθ
Q/√H
Q/H
Q/H3/2
Q/H²
Flow vs. swept volume
Pressure in cylinder vs. swept volume
Flow vs. speed
Pressure vs. speed