100 cm3
250 cm3
500 cm3
1000 cm3
Surface tension
Capillarity
Viscosity
Shear stress in fluids
Quasi-static
Steady state
Laminar
Uniform
Pascal law
Newton's law of viscosity
Boundary layer theory
Continuity equation
Pascal's law
Archimedess principle
D-Alembert's principle
None of these
Venturimeter
Orifice plate
Nozzle
All of the above
0.001
0.01
0.1
1
Atmospheric pressure
Pressure in pipes and channels
Pressure in Venturimeter
Difference of pressures between two points in a pipe
Increases
Decreases
Remain constant
Increases first up to certain limit and then decreases
Sub-sonic flow
Sonic flow
Super-sonic flow
Hyper-sonic flow
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
Cd × a × √(2gH)
Cd × a × √(2g) × H3/2
Cd × a × √(2g) × H2
Cd × a × √(2g) × H5/2
Increase
Remain unaffected
May increase or decrease depending on the characteristics of liquid
Decrease
Directly proportional to the area of the vessel containing liquid
Directly proportional to the depth of liquid from the surface
Directly proportional to the length of the vessel containing liquid
Inversely proportional to the depth of liquid from the surface
Tension at the base
Overturning of the wall or dam
Sliding of the wall or dam
All of these
Circular
Square
Rectangular
Trapezoidal
d = (D⁵/8fl)1/2
d = (D⁵/8fl)1/3
d = (D⁵/8fl)1/4
d = (D⁵/8fl)1/5
At the centre of gravity
Above the centre of gravity
Below be centre of gravity
Could be above or below e.g. depending on density of body and liquid
Less than 2000
Between 2000 and 2800
More than 2800
None of these
Any weight, floating or immersed in a liquid, is acted upon by a buoyant force
Buoyant force is equal to the weight of the liquid displaced
The point through which buoyant force acts, is called the center of buoyancy
Center of buoyancy is located above the center of gravity of the displaced liquid
π w ω² r²/4g
π w ω² r³/4g
π w ω² r⁴/4g
π w ω² r²/2g
It is the best liquid
The height of barometer will be less
Its vapour pressure is so low that it may be neglected
Both (B) and (C)
Neutral equilibrium
Stable equilibrium
Unstable equilibrium
None of these
Equal to
Directly proportional
Inversely proportional
None of these
Surface tension force
Viscous force
Gravity force
Elastic force
Viscosity
Air resistance
Surface tension forces
Atmospheric pressure
Equal to
Double
Three to four times
Five to six times
Low pressure
Moderate pressure
High pressure
Atmospheric pressure
Less than unity
Unity
Between 1 and 6
None of these
Shear stress to shear strain
Increase in volume to the viscosity of fluid
Increase in pressure to the volumetric strain
Critical velocity to the viscosity of fluid