Expands
Does not change
Contracts
None of these
C. Contracts
It gives maximum discharge for a given cross-sectional area and bed slope
It has minimum wetted perimeter
It involves lesser excavation for the designed amount of discharge
All of the above
Equal to
Directly proportional
Inversely proportional
None of these
Sub-sonic flow
Sonic flow
Super-sonic flow
Hyper-sonic flow
C.G. of body
Center of pressure
Center of buoyancy
Metacentre
Steady
Streamline
Turbulent
Unsteady
0.8
1
1.2
1.6
1.84 (L - 0.1nH)H3/2
1.84 (L - nH)H2
1.84 (L - 0.1nH)H5/2
1.84 (L - nH)H3
(8/15) Cd. 2g. H
(8/15) Cd. 2g. H3/2
(8/15) Cd. 2g. H²
(8/15) Cd. 2g. H5/2
Centre of gravity
Centre of pressure
Metacentre
Centre of buoyancy
(q/g)1/2
(q²/g)1/3
(q³/g)1/4
(q⁴/g)1/5
Any weight, floating or immersed in a liquid, is acted upon by a buoyant force
Buoyant force is equal to the weight of the liquid displaced
The point through which buoyant force acts, is called the center of buoyancy
Center of buoyancy is located above the center of gravity of the displaced liquid
Reynold's number
Froude's number
Weber's number
Mach number
Gauge pressure
Absolute pressure
Positive gauge pressure
Vacuum pressure
Has the dimensions of 1/pressure
Increases with pressure
Is large when fluid is more compressible
Is independent of pressure and viscosity
Principle of conservation of mass holds
Velocity and pressure are inversely proportional
Total energy is constant throughout
The energy is constant along a streamline but may vary across streamlines
At the inlet
At the outlet
At the summit
At any point between inlet and outlet
There is excessive leakage in the pipe
The pipe bursts under high pressure of fluid
The flow of fluid through the pipe is suddenly brought to rest by closing of the valve
The flow of fluid through the pipe is gradually brought to rest by closing of the valve
Specific weight
Specific volume
Specific speed
Specific gravity
Below the center of gravity
Below the center of buoyancy
Above the center of buoyancy
Above the center of gravity
Shear stress and the rate of angular distortion
Shear stress and viscosity
Shear stress, velocity and viscosity
Pressure, velocity and viscosity
Head of water (h)
h²
V/T
h/2
The head loss for all the pipes is same
The total discharge is equal to the sum of discharges in the various pipes
The total head loss is the sum of head losses in the various pipes
Both (A) and (B)
Metacentre
Center of pressure
Center of buoyancy
Center of gravity
Above it
Below it
At same point
Above or below depending on area of body
Up-thrust
Reaction
Buoyancy
Metacentre
Velocity of flow is very high
Discharge is difficult to measure
Mach number is between 1 and 6
None of these
Gravity, pressure and viscous
Gravity, pressure and turbulent
Pressure, viscous and turbulent
Gravity, viscous and turbulent
2.4 m above the hydraulic gradient
6.4 m above the hydraulic gradient
10.0 m above the hydraulic gradient
5.0 above the hydraulic gradient
Energy
Work
Mass
Length
200 kg/m3
400 kg/m3
600 kg/m3
800 kg/m3