(H - hf )/H
H/(H - hf )
(H + hf )/H
H/(H + hf )
A. (H - hf )/H
Planes of the body are completely smooth
Space around the body is completely filled with the fluid
Fluid particles do not exert any influence on one another
All of the above
0.34 times
0.67 times
0.81 times
0.95 times
Increase in viscosity of gas
Increase in viscosity of liquid
Decrease in viscosity of gas
Decrease in viscosity of liquid
(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
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
Steady uniform flow
Steady non-uniform flow
Unsteady uniform flow
Unsteady non-uniform flow
Neutral equilibrium
Stable equilibrium
Unstable equilibrium
None of these
One dimensional flow
Uniform flow
Steady flow
Turbulent flow
Viscosity of a fluid is that property which determines the amount of its resistance to a shearing force
Viscosity is due primarily to interaction between fluid molecules
Viscosity of liquids decreases with increase in temperature
Viscosity of liquids is appreciably affected by change in pressure
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 energy + kinetic energy + potential energy
Pressure energy - (kinetic energy + potential energy)
Potential energy - (pressure energy + kinetic energy
Kinetic energy - (pressure energy + potential energy)
Lesser
Greater
Same
None of these
Suction pressure
Vacuum pressure
Negative gauge pressure
All of these
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
Increases
Decreases
Remain constant
Increases first up to certain limit and then decreases
At the Centroid
Above the Centroid
Below the Centroid
At metacentre
A × M × m1/2 × i2/3
A × M × m2/3 × i1/2
A1/2 × M2/3 × m × i
A2/3 × M1/3 × m × i
Surface tension
Compressibility
Capillarity
Viscosity
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
Cannot be compressed
Occupy definite volume
Are not affected by change in pressure and temperature
None of the above
μ π³ N² R² /1800 t
μ π³ N² R⁴ /1800 t
μ π³ N² R² /3600 t
μ π³ N² R⁴ /3600 t
Density of liquid
Specific gravity of liquid
Compressibility of liquid
Surface tension of liquid
Vertical line
Horizontal line
Inclined line with flow downward
In any direction and in any location
d/6
d/4
d/2
d
Less than unity
Unity
Between 1 and 6
None of these
1 Pa
91 Pa
981 Pa
9810 Pa
Incompressible
Compressible
Viscous
None of these
Higher
Lower
Same as
None of these
Internal
External
Both A and B
None of these
Comparing two identical equipments
Designing models so that the result can be converted to prototypes
Comparing similarity between design and actual equipment
Hydraulic designs