2gH
H × √(2g)
2g × √H
√(2gh)
D. √(2gh)
Double
Four times
Eight times
Sixteen times
Frictional force
Viscosity
Surface friction
All of the above
0.384 Cd × L × H1/2
0.384 Cd × L × H3/2
1.71 Cd × L × H1/2
1.71 Cd × L × H3/2
Sill or crest
Nappe or vein
Orifice
None of these
Equal to
One-half
Three fourth
Double
Plus
Minus
Divide
Multiply
Internal
External
Both A and B
None of these
Mass of liquid displaced
Viscosity of the liquid
Pressure of the liquid displaced
Depth of immersion
Plus
Minus
Divide
None of these
Directly
Inversely
Both A and B
None of these
Directly proportional
Inversely proportional
Square root of velocity
None of these
Maximum at the centre and minimum near the walls
Minimum at the centre and maximum near the walls
Zero at the centre and maximum near the walls
Maximum at the centre and zero near the walls
The direction and magnitude of the velocity at all points are identical
The velocity of successive fluid particles, at any point, is the same at successive periods of time
The magnitude and direction of the velocity do not change from point to point in the fluid
The fluid particles move in plane or parallel planes and the streamline patterns are identical in each plane
Pressure force
Elastic force
Surface tension force
Viscous force
Energy
Work
Mass
Length
Q = Cd × a × 2gh
Q = (2/3). Cd × a × h
Q = (Cd × a)/√(2gh)
Q = (3Cd × a)/√(2h)
Sub-sonic velocity
Super-sonic velocity
Lower critical velocity
Higher critical velocity
0.1 N-s/m2
1 N-s/m2
10 N-s/m2
100 N-s/m2
Remains constant
Increases
Decreases
Depends upon mass of liquid
Specific weight
Specific volume
Specific speed
Specific gravity
Pressure
Flow
Shape
Volume
Real fluid
Ideal fluid
Newtonian fluid
Non-Newtonian fluid
Equal to
Less than
More than
None of these
1.84 (L - 0.1nH)H3/2
1.84 (L - nH)H2
1.84 (L - 0.1nH)H5/2
1.84 (L - nH)H3
Surface tension
Capillarity
Viscosity
Shear stress in fluids
Wake
Drag
Lift
Boundary layer
The liquid particles at all sections have the same velocities
The liquid particles at different sections have different velocities
The quantity of liquid flowing per second is constant
Each liquid particle has a definite path
Real
Ideal
Newtonian
Non-Newtonian
Real fluid
Ideal fluid
Newtonian fluid
Non-Newtonian fluid
The horizontal component of the hydrostatic force on any surface is equal to the normal force on the vertical projection of the surface
The horizontal component acts through the center of pressure for the vertical projection
The vertical component of the hydrostatic force on any surface is equal to the weight of the volume of the liquid above the area
The vertical component passes through the center of pressure of the volume