10° to 15°
15° to 20°
20° to 25°
25° to 30°
C. 20° to 25°
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
They have slow speeds
They are suitable even for low water heads
They give constant efficiency, even if the discharge is not constant
All of the above
Fourneyron turbine
Journal turbine
Thomson's turbine
Pelton wheel
Inlet of draft rube
Blade inlet
Guide blade
Penstock
Directly as fan speed
Square of fan speed
Cube of fan speed
Square root of fan speed
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
Give high discharge
Produce high heads
Pump viscous fluids
All of these
Closed
Open
Depends on starting condition and flow desired
Could be either open or closed
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
The reaction turbines are used for low head and high discharge.
The angle of taper on draft tube is less than 8°.
An impulse turbine is generally fitted slightly above the tail race.
A Francis turbine is an impulse turbine.
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
102 watts
75 watts
550 watts
735 watts
Waste valve closes suddenly
Supply pipe is long
Supply pipe is short
Ram chamber is large
[2(Vr - v) v]/ Vr²
2(Vr + v) v]/ Vr²
[(Vr - v) v]/ Vr
[(Vr + v) v]/ Vr
Horizontal
Nearly horizontal
Steep
First rise and then fall
Lift and resultant force
Drag and resultant force
Lift and tangential force
Lift and drag
waV/2g × sinθ
waV/g × sinθ
waV²/2g × sin2θ
waV²/g × sinθ
(w Hm) / (Q × ηo)
(w Hm Q) / ηo
(w Q) / (Hm × ηo)
(w Q ηo) / Hm
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
0 to 4.5
10 to 100
80 to 200
250 to 300
Net head
Absolute velocity
Blade velocity
Flow
0.15 to 0.3
0.4 to 0.5
0.6 to 0.9
1 to 1.5
Impeller diameter
Speed
Fluid density
Both (A) and (B) above
Speed and power developed
Discharge and power developed
Speed and head of water
Speed, power developed and head of water
39.2 %
49.2 %
68.8 %
84.8 %
Causes noise and vibration of various parts
Reduces the discharge of a turbine
Causes sudden drop in power output and efficiency
All of the above
Rectilinear flow
Radial flow
Free vortex motion
Forced vortex
0.25 m3/s
0.5 m3/s
1.5 m3/s
2.5 m3/s
Accumulating oil
Supplying large quantities of oil for very short duration
Generally high pressures to operate hydraulic machines
Supplying energy when main supply fails
(1 + cos φ)/2
(1 - cos φ)/2
(1 + sin φ)/2
(1 - sin φ)/2