A × M × m1/2 × i2/3
A × M × m2/3 × i1/2
A1/2 × M2/3 × m × i
A2/3 × M1/3 × m × i
B. A × M × m2/3 × i1/2
Maximum
Minimum
Zero
Nonzero finite
The resultant force acting on a floating body
The resultant force on a body due to the fluid surrounding it
Equal to the volume of liquid displaced
The force necessary to maintain equilibrium of a submerged body
Narrow-crested weir
Broad-crested weir
Ogee weir
Submerged weir
Does not change
Increases
Decreases
None of these
Weir
Notch
Orifice
None of these
4μvl/wd²
8μvl/wd²
16μvl/wd²
32μvl/wd²
At
Above
Below
None of these
Metres² per sec
kg-sec/metre
Newton-sec per metre²
Newton-sec per meter
(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
2A × √H₁/Cd × a × √(2g)
2A × √H₂/Cd × a × √(2g)
2A × (√H₁ - √H₂)/Cd × a × √(2g)
2A × (√H3/2 - √H3/2)/Cd × a × √(2g)
Z + p/w + v²/2g = constant
Z + p/w - v²/2g = constant
Z - p/w + v²/2g = constant
Z - p/w - v²/2g = constant
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 pleasure
Equal to
Less than
More than
None of these
1
5
7
6
Increases
Decreases
Remain unaffected
Unpredictable
ρ ω2 r2
2ρ ω2 r2
ρ ω2 r2/2
ρ ω2 r2/4
Fluid
Water
Gas
Ideal fluid
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
Newton's law of motion
Newton's law of viscosity
Pascal' law
Continuity equation
Weight of the liquid displaced
Pressure with which the liquid is displaced
Viscosity of the liquid
Compressibility of the liquid
Cannot be compressed
Occupy definite volume
Are not affected by change in pressure and temperature
None of the above
Equal to
Directly proportional
Inversely proportional
None of these
More
Less
Same
More or less depending on size of glass tube
Viscosity
Air resistance
Surface tension forces
Atmospheric pressure
0.34 times
0.67 times
0.81 times
0.95 times
Specific weight
Mass density
Specific gravity
None of these
Surface tension
Capillarity
Viscosity
Shear stress in fluids
Acts in the plane of the interface normal to any line in the surface
Is also known as capillarity
Is a function of the curvature of the interface
Decreases with fall in temperature
103 kN/m2
10.3 m of water
760 mm of mercury
All of these
Adhesion
Cohesion
Surface tension
Viscosity