Elastic properties of the pipe material
Elastic properties of the liquid flowing through the pipe
Speed at which the valve is closed
All of the above
D. All of the above
(H - hf )/H
H/(H - hf )
(H + hf )/H
H/(H + hf )
Plus
Minus
Divide
None of these
Ratio of inertial force to force due to viscosity
Ratio of inertial force to force due to gravitation
Ratio of inertial force to force due to surface tension
All the four ratios of inertial force to force due to viscosity, gravitation, surface tension, and elasticity
Red wood
Say bolt
Engler
Orsat
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
51 cm
50 cm
52 cm
52.2 cm
H/3
H/2
2H/3
3H/4
π w ω² r²/4g
π w ω² r³/4g
π w ω² r⁴/4g
π w ω² r²/2g
Real fluid
Ideal fluid
Newtonian fluid
Non-Newtonian fluid
The metacentre should lie above the center of gravity
The center of buoyancy and the center of gravity must lie on the same vertical line
A righting couple should be formed
All the above are correct
Critical velocity
Velocity of approach
Sub-sonic velocity
Super-sonic velocity
Pressure in pipe, channels etc.
Atmospheric pressure
Very low pressures
Difference of pressure between two points
Steady flow
Uniform flow
Streamline flow
Turbulent flow
(8/15) Cd. 2g. H
(8/15) Cd. 2g. H3/2
(8/15) Cd. 2g. H²
(8/15) Cd. 2g. H5/2
Centre of pressure
Centre of buoyancy
Metacentre
None of these
Weber's number is the ratio of inertia force to elastic force.
Weber's number is the ratio of gravity force to surface tension force.
Weber's number is the ratio of viscous force to pressure force.
Weber's number is the ratio of inertia force to surface tension force.
Above it
Below it
At same point
Above or below depending on area of body
Steady
Unsteady
Uniform
Laminar
Real
Ideal
Newtonian
Non-Newtonian
Real fluid
Ideal fluid
Newtonian fluid
Non-Newtonian fluid
Tensile stress
Compressive stress
Shear stress
Bending stress
Q = Cd × bH₁ × √(2gh)
Q = Cd × bH2 × √(2gh)
Q = Cd × b (H2 - H1) × √(2gh)
Q = Cd × bH × √(2gh)
Low pressure
Moderate pressure
High pressure
Atmospheric pressure
Path line
Stream line
Steak line
Potential line
Inertia force
Viscous force
Gravity force
Pressure force
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
At C.G. of body
At center of pressure
Vertically upwards
At metacentre
Avoid the tendency of breaking away the stream of liquid
To minimise frictional losses
Both (A) and (B)
None of these
Venturimeter
Orifice plate
Hot wire anemometer
Pitot tube
Pascal law
Newton's law of viscosity
Boundary layer theory
Continuity equation