10 kg
100 kg
1000 kg
1 kg
A. 10 kg
Less
More
Equal
Less at low temperature and more at high temperature
Reynold's number
Froude's number
Weber's number
Euler's number
dQ/Q = 3/2 × (dH/H)
dQ/Q = 2 × (dH/H)
dQ/Q = 5/2 × (dH/H)
dQ/Q = 3 × (dH/H)
Moving
Viscous
Viscous and static
Viscous and moving
9.81 kN/m3
9.81 × 103 N/m3
9.81 × 10-6 N/mm3
Any one of these
Double
Four times
Eight times
Sixteen times
Sink to bottom
Float over fluid
Partly immersed
Be fully immersed with top surface at fluid surface
Higher
Lower
Same
Higher/lower depending on temperature
N-m/s2
N-s/m2
Poise
Stoke
Below the center of gravity
Below the center of buoyancy
Above the center of buoyancy
Above the center of gravity
1000 N/m3
10000 N/m3
9.81 × 103 N/m3
9.81 × 10⁶ N/m3
Steady flow
Turbulent flow
Laminar flow
Non-uniform flow
A × M × m1/2 × i2/3
A × M × m2/3 × i1/2
A1/2 × M2/3 × m × i
A2/3 × M1/3 × m × i
Pascal law
Newton's law of viscosity
Boundary layer theory
Continuity equation
Directly
Inversely
Both A and B
None of these
Real fluid
Ideal fluid
Newtonian fluid
Non-Newtonian fluid
Critical flow
Turbulent flow
Tranquil flow
Torrential flow
Steady uniform flow
Steady non-uniform flow
Unsteady uniform flow
Unsteady non-uniform flow
Straight line
Parabolic curve
Hyperbolic curve
Elliptical
On the surface at which resultant pressure acts
On the surface at which gravitational force acts
At which all hydraulic forces meet
Similar to metacentre
Less than
Same as
More than
None of these
p/sinα
2p/sinα
p/2sinα
2p/sin (α/2)
Velocity
(Velocity)2
(Velocity)3
(Velocity)4
Real fluid
Ideal fluid
Newtonian fluid
Non-Newtonian fluid
Constant
Variable
Zero
Zero under limiting conditions
1 and 2.5
2.5 and 4
4 and 6
1 and 6
Sub-sonic velocity
Super-sonic velocity
Lower critical velocity
Higher critical velocity
Surface tension
Cohesion of the liquid
Adhesion of the liquid molecules and the molecules on the surface of a solid
All of the above
Higher
Lower
Same
None of these
The horizontal component of the hydrostatic force on any surface is equal to the normal force on the vertical projection of the surface
The horizontal component acts through the center of pressure for the vertical projection
The vertical component of the hydrostatic force on any surface is equal to the weight of the volume of the liquid above the area
The vertical component passes through the center of pressure of the volume