(2/3) Cd × b × √(2gH)
(2/3) Cd × b × √(2g) × H
(2/3) Cd × b × √(2g) × H3/2
(2/3) Cd × b × √(2g) × H2
C. (2/3) Cd × b × √(2g) × H3/2
Surface tension force
Viscous force
Gravity force
Elastic force
0.5
0.4
0.515
0.5
Steady flow
Unsteady flow
Laminar flow
Turbulent flow
C.G. of body
Center of pressure
Center of buoyancy
Metacentre
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
Adhesion
Cohesion
Viscosity
Compressibility
Reynold's number
Froude's number
Weber's number
Euler's number
The size of orifice is large
The velocity of flow is large
The available head of liquid is more than 5 times the height of orifice
The available head of liquid is less than 5 times the height of orifice
Pressure
Distance
Density
Flow
Inversely proportional to H3/2
Directly proportional to H3/2
Inversely proportional to H5/2
Directly proportional to H5/2
Incompressible
Viscous and incompressible
Inviscous and compressible
Inviscous and incompressible
10 m/sec²
9.81 m/sec²
9.75 m/sec²
9 m/sec
Less than
More than
Equal to
None of these
Capillary tube method
Orifice type viscometer
Rotating cylinder method
All of these
Coincides with its centre of gravity
Lies above its centre of gravity
Lies below its centre of gravity
Lies between the centre of buoyancy and centre of gravity
More
Less
Same
More or less depending on size of glass tube
10 kg
100 kg
1000 kg
1 kg
Continuity equation
Bernoulli's equation
Pascal's law
Archimedess principle
Q = Cd × bH₁ × √(2gh)
Q = Cd × bH2 × √(2gh)
Q = Cd × b (H2 - H1) × √(2gh)
Q = Cd × bH × √(2gh)
Pascal's law
Archimedess principle
Principle of floatation
Bernoulli's theorem
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
The flow is steady
The flow is streamline
Size and shape of the cross section in a particular length remain constant
Size and cross section change uniformly along length
Centre of gravity
Centre of pressure
Metacentre
Centre of buoyancy
At the inlet
At the outlet
At the summit
At any point between inlet and outlet
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
Inversely proportional to H3/2
Directly proportional to H3/2
Inversely proportional to H5/2
Directly proportional to H5/2
Cd × a × √(2gH)
Cd × a × √(2g) × H3/2
Cd × a × √(2g) × H2
Cd × a × √(2g) × H5/2
400 kg/cm²
4000 kg/cm²
40 × 10⁵ kg/cm²
40 × 10⁶ kg/cm²
There is no loss of energy of the liquid flowing
The velocity of flow is uniform across any cross-section of the pipe
No force except gravity acts on the fluid
All of the above
Streamline flow
Turbulent flow
Steady flow
Unsteady flow