The suction pressure should be high
The delivery pressure should be high
The suction pressure should be low
The delivery pressure should be low
A. The suction pressure should be high
waV/2g × sinθ
waV/g × sinθ
waV²/2g × sin2θ
waV²/g × sinθ
waV / 2g
waV / g
waV² / 2g
waV² / g
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
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
Suction lift + Loss of head in suction pipe due to friction + Delivery lift + Loss of head in delivery pipe due to friction + Velocity head in the delivery pipe
Workdone per kN of water Losses within the impeller
Energy per kN at outlet of impeller Energy per kN at inlet of impeller
All of the above
Double
Three times
Four times
Five times
Directly proportional to N
Inversely proportional to N
Directly proportional to N²
Inversely proportional to N²
39.2 %
49.2 %
68.8 %
84.8 %
Centrifugal pump
Reciprocating pump
Jet pump
Air lift pump
Same
0.75 B.H.P.
B.H.P./0.75
1.5 B.H.P.
(W/p) × (A/a)
(p/W) × (a/A)
(W/p) × (a/A)
(p/W) × (A/a)
Propeller turbine
Francis turbine
Impulse turbine
None of the above
Kinetic head
Velocity head
Manometric head
Static head
Propeller turbine
Francis turbine
Impulse turbine
Any one of the above
0.15 to 0.3
0.4 to 0.5
0.6 to 0.9
1 to 1.5
L.A.N
2 L.A.N
(L.A.N)/60
(2 L.A.N)/60
Have identical velocities
Are equal in size and shape
Are identical in shape, but differ only in size
Have identical forces
Centrifugal pump
Reciprocating pump
Jet pump
Airlift pump
Decreases
Increases
Remain same
None of these
Pelton wheel with one nozzle
Pelton wheel with two or more nozzles
Kaplan turbine
Francis turbine
Potential Energy
Strain Energy
Kinetic energy
None of these
High discharge
High head
Pumping of viscous fluids
High head and high discharge
Impeller diameter
Speed
Fluid density
Both (A) and (B) above
Q/√H
Q/H
Q/H3/2
Q/H²
2 to 4
4 to 8
8 to 16
16 to 24
Power absorbing machines
Power developing machines
Energy transfer machines
Energy generating machines
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.
The suction pressure should be high
The delivery pressure should be high
The suction pressure should be low
The delivery pressure should be low
Two
Four
Six
Eight
Power produced by the turbine to the energy actually supplied by the turbine
Actual work available at the turbine to the energy imparted to the wheel
Workdone on the wheel to the energy (or head of water) actually supplied to the turbine
None of the above