Straight line
Parabolic curve
Hyperbolic curve
Elliptical
A. Straight line
Only when the fluid is frictionless
Only when the fluid is incompressible and has zero viscosity
When there is no motion of one fluid layer relative to an adjacent layer
Irrespective of the motion of one fluid layer relative to an adjacent layer
Concave
Convex
Plane
None of these
Equal to
Less than
More than
None of these
Surface tension
Capillarity
Viscosity
Shear stress in fluids
Specific gravity = gravity × density
Dynamic viscosity = kinematic viscosity × density
Gravity = specific gravity × density
Kinematic viscosity = dynamic viscosity × density
Minimum
Maximum
Zero
Could be any value
Smooth and streamline flow
Laminar flow
Steady flow
Highly turbulent flow
The pressure at any location reaches an absolute pressure equal to the saturated vapour pressure of the liquid
Pressure becomes more than critical pressure
Flow is increased
Pressure is increased
Compressibility
Surface tension
Cohesion
Adhesion
Pressure in pipe, channels etc.
Atmospheric pressure
Very low pressures
Difference of pressure between two points
Adhesion
Cohesion
Viscosity
Compressibility
ω.r/2g
ω².r²/2g
ω.r/4g
ω².r²/4g
The metal piece will simply float over the mercury
The metal piece will be immersed in mercury by half
Whole of the metal piece will be immersed with its top surface just at mercury level
Metal piece will sink to the bottom
2.89 kN
8.29 kN
9.28 kN
28.9 kN
Directly proportional to (radius)2
Inversely proportional to (radius)2
Directly proportional to (radius)4
Inversely proportional to (radius)4
One-half
One-third
Two-third
None of these
1
5
7
6
Less than
More than
Equal to
None of these
1/2 × depth
1/2 × breadth
1/2 × sloping side
1/4 × (depth + breadth)
Pressure head
Velocity head
Pressure head + velocity head
Pressure head - velocity head
Less man the vapour pressure over the plane surface
Equal to the vapour pressure over the plane surface
Greater than the vapour pressure over the plane surface
Zero
Increases
Decreases
Remain unaffected
Unpredictable
To control the pressure variations due to rapid changes in the pipe line flow
To eliminate water hammer possibilities
To regulate flow of water to turbines by providing necessary retarding head of water
All of the above
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
Centre of gravity
Centre of depth
Centre of pressure
Centre of immersed surface
One-dimensional flow
Two-dimensional flow
Three-dimensional flow
Four-dimensional flow
1/RN
4/RN
16/RN
64/RN
Steady flow
Uniform flow
Streamline flow
Turbulent flow
Metacentre
Center of pressure
Center of buoyancy
Center of gravity
Up-thrust
Reaction
Buoyancy
Metacentre