Total energy per unit discharge
Total energy measured with respect to the datum passing through the bottom of the channel
Total energy measured above the horizontal datum
Kinetic energy plotted above the free surface of water
B. Total energy measured with respect to the datum passing through the bottom of the channel
0.62
0.76
0.84
0.97
It is incompressible
It has uniform viscosity
It has zero viscosity
It is at rest
tanθ = a/g
tanθ = 2 a/g
tanθ = a/2g
tanθ = a2/2g
ω.r/2g
ω².r²/2g
ω.r/4g
ω².r²/4g
It has low vapour pressure
It is clearly visible
It has low surface tension
It can provide longer column due to low density
flv²/2gd
flv²/gd
3flv²/2gd
4flv²/2gd
Narrow crested weir
Broad crested weir
Ogee weir
Submerged weir
Continuity equation
Bernoulli's equation
Pascal's law
Archimedess principle
Crest
Nappy
Sill
Weir top
Pressure in pipes, channels etc.
Atmospheric pressure
Very low pressure
Difference of pressure between two points
Boyle's law
Archimedes principle
Pascal's law
Newton's formula
(2A√H₁)/(Cd × a√2g)
(2AH₁)/(Cd × a√2g)
(2AH₁3/2)/(Cd × a√2g)
(2AH₁²)/(Cd × a√2g)
The pressure at any location reaches an absolute pressure equal to the saturated vapour pressure of the liquid
Pressure becomes more than critical pressure
Flow is increased
Pressure is increased
Gas law
Boyle's law
Charles law
Pascal's law
Venturimeter
Orifice plate
Pitot tube
Rotameter
Velocity of liquid
Atmospheric pressure
Pressure in pipes and channels
Difference of pressure between two points in a pipe
Linear
Parabolic
Hyperbolic
Inverse type
Surface tension
Adhesion
Cohesion
Viscosity
Steady flow
Unsteady flow
Laminar flow
Uniform flow
Volumetric strain
Volumetric index
Compressibility
Adhesion
1 %
1.5 %
2 %
2.5 %
(μπ²N/60t) × (R₁ - R₂)
(μπ²N/60t) × (R₁² - R₂²)
(μπ²N/60t) × (R₁³ - R₂³)
(μπ²N/60t) × (R₁⁴ - R₂⁴)
Less than unity
Unity
Between 1 and 6
More than 6
One dimensional flow
Uniform flow
Steady flow
Turbulent flow
Double
Four times
Eight times
Sixteen times
Absolute temperature
Temperature
Density
Modulus of elasticity
4μvl/wd²
8μvl/wd²
16μvl/wd²
32μvl/wd²
The pressure below the nappe is atmospheric
The pressure below the nappe is negative
The pressure above the nappe is atmospheric
The pressure above the nappe is negative
14π R1/2/15Cd × a √(2g)
14π R3/2/15Cd × a √(2g)
14π R5/2/15Cd × a √(2g)
14π R7/2/15Cd × a √(2g)
One-dimensional flow
Two-dimensional flow
Three-dimensional flow
Four-dimensional flow