Flow vs. swept volume
Pressure in cylinder vs. swept volume
Flow vs. speed
Pressure vs. speed
B. Pressure in cylinder vs. swept volume
Geometric similarity
Kinematic similarity
Dynamic similarity
None of these
Proportional to diameter of impeller
Proportional to speed of impeller
Proportional to diameter and speed of impeller
None of the above
P/ √H
P/ H
P/ H3/2
P/ H²
Lift and resultant force
Drag and resultant force
Lift and tangential force
Lift and drag
102 watts
75 watts
550 watts
735 watts
10-15°
20-25°
30-40°
50-60°
(w Hm) / (Q × ηo)
(w Hm Q) / ηo
(w Q) / (Hm × ηo)
(w Q ηo) / Hm
Straight
Bent forward
Bent backward
Radial
Centrifugal
Axial flow
Reciprocating
Mixed flow
0.25 kW
0.75 kW
1.75 kW
3.75 kW
2 to 4
4 to 8
8 to 16
16 to 24
High discharge
High head
Pumping of viscous fluids
High head and high discharge
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
Delivers unit discharge under unit head
Delivers unit discharge under unit speed
Develops unit power under unit head
Develops unit power under unit speed
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.
Horizontal
Nearly horizontal
Steep
First rise and then fall
Hydraulic
Mechanical
Overall
None of these
Ratio of actual discharge to the theoretical discharge
Sum of actual discharge and the theoretical discharge
Difference of theoretical discharge and the actual discharge
Product of theoretical discharge and the actual discharge
Smoothen the flow
Reduce suction head
Increase delivery head
Reduce acceleration head
Directly as the air or gas density
Inversely as square root of density
Inversely as density
As square of density
waV/2g × sinθ
waV/g × sinθ
waV²/2g × sin2θ
waV²/g × sinθ
To break the jet of water
To bring the runner to rest in a short time
To change the direction of runner
None of these
0.50 to 0.65
0.65 to 0.75
0.75 to 0.85
0.85 to 0.90
24.8 r.p.m.
48.2 r.p.m
82.4 r.p.m.
248 r.p.m
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
Equal to
1.2 times
1.8 times
Double
Allow the water to enter the runner without shock
Allow the water to flow over them, without forming eddies
Allow the required quantity of water to enter the turbine
All of the above
Directly proportional to H1/2
Inversely proportional to H1/2
Directly proportional to H3/2
Inversely proportional to H3/2