1
1.2
0.8
0.75
D. 0.75
0.5 a. √2gH
0.707 a. √2gH
0.855 a. √2gH
a. √2gH
In a compressible flow, the volume of the flowing liquid changes during the flow
A flow, in which the volume of the flowing liquid does not change, is called incompressible flow
When the particles rotate about their own axes while flowing, the flow is said to be rotational flow
All of the above
Increases
Decreases
Remain unaffected
Unpredictable
p/sinα
2p/sinα
p/2sinα
2p/sin (α/2)
Below the center of gravity
Below the center of buoyancy
Above the center of buoyancy
Above the center of gravity
Moving
Viscous
Viscous and static
Viscous and moving
50 %
56.7 %
66.67 %
76.66 %
Centre of gravity
Centre of pressure
Metacentre
Centre of buoyancy
The fluid is non - viscous, homogeneous and incompressible
The velocity of flow is uniform over the section
The flow is continuous, steady and along the stream line
All of the above
Increase
Remain unaffected
May increase or decrease depending on the characteristics of liquid
Decrease
To control the pressure variations due to rapid changes in the pipe line flow
To eliminate water hammer possibilities
To regulate flow of water to turbines by providing necessary retarding head of water
All of the above
Z + p/w + v²/2g = constant
Z + p/w - v²/2g = constant
Z - p/w + v²/2g = constant
Z - p/w - v²/2g = constant
Resistance to shear stress is small
Fluid pressure is zero
Linear deformation is small
Only normal stresses can exist
Metres² per sec
kg-sec/metre
Newton-sec per metre²
Newton-sec per meter
Venturimeter
Orifice meter
Pitot tube
All of these
Critical velocity
Velocity of approach
Sub-sonic velocity
Super-sonic velocity
0.384 Cd × L × H1/2
0.384 Cd × L × H3/2
1.71 Cd × L × H1/2
1.71 Cd × L × H3/2
400 kg/cm²
4000 kg/cm²
40 × 10⁵ kg/cm²
40 × 10⁶ kg/cm²
Steady
Streamline
Turbulent
Unsteady
Less than 2000
Between 2000 and 2800
More than 2800
None of these
Comparing two identical equipments
Designing models so that the result can be converted to prototypes
Comparing similarity between design and actual equipment
Hydraulic designs
Buoyancy, gravity
Buoyancy, pressure
Buoyancy, inertial
Inertial, gravity
dQ/Q = 3/2 × (dH/H)
dQ/Q = 2 × (dH/H)
dQ/Q = 5/2 × (dH/H)
dQ/Q = 3 × (dH/H)
At C.G. of body
At center of pressure
Vertically upwards
At metacentre
Pressure force
Elastic force
Gravity force
Viscous force
(q/g)1/2
(q²/g)1/3
(q³/g)1/4
(q⁴/g)1/5
Neutral
Stable
Unstable
None of these
Equal to
Less than
More than
None of these
Less than
More than
Equal to
None of these
Avoid interruption in the flow
Increase discharge
Increase velocity
Maintain pressure difference