Pressure in pipes, channels etc.
Atmospheric pressure
Very low pressure
Difference of pressure between two points
A. Pressure in pipes, channels etc.
Equal to
Double
Three to four times
Five to six times
Supersonics, as with projectile and jet propulsion
Full immersion or completely enclosed flow, as with pipes, aircraft wings, nozzles etc.
Simultaneous motion through two fluids where there is a surface of discontinuity, gravity forces, and wave making effect, as with ship's hulls
All of the above
Less man the vapour pressure over the plane surface
Equal to the vapour pressure over the plane surface
Greater than the vapour pressure over the plane surface
Zero
Gas law
Boyle's law
Charles law
Pascal's law
Below the center of gravity
Below the center of buoyancy
Above the center of buoyancy
Above the center of gravity
Open channel/pipe flow
Compressibility of fluids
Conservation of mass
Steady/unsteady flow
Plus
Minus
Divide
Multiply
Specific weight
Specific mass
Specific gravity
Specific density
1/16 to 1/8
1/8 to 1/4
1/4 to 1/3
1/3 to 1/2
Equal to
Less than
More than
None of these
Density of liquid
Specific gravity of liquid
Compressibility of liquid
Surface tension of liquid
Pressure in pipes, channels etc.
Atmospheric pressure
Very low pressure
Difference of pressure between two points
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
(μπ²N/60t) × (R₁ - R₂)
(μπ²N/60t) × (R₁² - R₂²)
(μπ²N/60t) × (R₁³ - R₂³)
(μπ²N/60t) × (R₁⁴ - R₂⁴)
Does not change
Increases
Decreases
None of these
ρ ω2 r2
2ρ ω2 r2
ρ ω2 r2/2
ρ ω2 r2/4
Half the depth
Half the breadth
Twice the depth
Twice the breadth
Increases
Decreases
Remain constant
Increases first up to certain limit and then decreases
Critical flow
Turbulent flow
Tranquil flow
Torrential flow
(2/3) × Cd (L - nH) × √(2gh)
(2/3) × Cd (L - 0.1nH) × √(2g) × H3/2
(2/3) × Cd (L - nH) × √(2g) × H²
(2/3) × Cd (L - nH) × √(2g) × H5/2
It is easier to see through the glass tube
Glass tube is cheaper than a metallic tube
It is not possible to conduct this experiment with any other tube
All of the above
2gH
H × √(2g)
2g × √H
√(2gh)
Ratio of absolute viscosity to the density of the liquid
Ratio of density of the liquid to the absolute viscosity
Product of absolute viscosity and density of the liquid
Product of absolute viscosity and mass of the liquid
Energy/unit area
Velocity/unit area
Both of the above
It has no units
2 metres of water column
3 metres of water column
3.5 metres of water column
4 m of water column
Gravitational force is equal to the up-thrust of the liquid
Gravitational force is less than the up-thrust of the liquid
Gravitational force is more than the up-thrust of the liquid
None of the above
Equal to
Less than
More than
None of these
Incompressible
Compressible
Viscous
None of these
wA
wx
wAx
wAx/sinθ
Cohesion
Adhesion
Viscosity
Surface tension