0.375
0.5
0.707
0.855
D. 0.855
Surface tension
Cohesion of the liquid
Adhesion of the liquid molecules and the molecules on the surface of a solid
All of the above
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
Metres² per sec
kg sec/metre
Newton-sec per metre
Newton-sec per metre
High velocity
High pressure
Weak material
Low pressure
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
ML°T⁻²
ML°T
ML r²
ML²T²
0.375
0.5
0.707
0.855
Directly
Inversely
Both A and B
None of these
The pressure on the wall at the liquid level is minimum
The pressure on the bottom of the wall is maximum
The pressure on the wall at the liquid level is zero, and on the bottom of the wall is maximum
The pressure on the bottom of the wall is zer
0° C
0° K
4° C
20° C
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
Remain same
Increases
Decreases
Shows erratic behaviour
Expands
Does not change
Contracts
None of these
Decrease
Increase
Remain unchanged
Depend upon the characteristics of liquid
Inversely proportional to H3/2
Directly proportional to H3/2
Inversely proportional to H5/2
Directly proportional to H5/2
Adhesion
Cohesion
Surface tension
Viscosity
Equal to
One-fourth
One-third
One-half
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
Real fluid
Ideal fluid
Newtonian fluid
Non-Newtonian fluid
200 kg/m3
400 kg/m3
600 kg/m3
800 kg/m3
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
d = (D⁵/8fl)1/2
d = (D⁵/8fl)1/3
d = (D⁵/8fl)1/4
d = (D⁵/8fl)1/5
Increases
Decreases
Remain unaffected
Unpredictable
Specific weight
Mass density
Specific gravity
None of these
dQ/Q = (1/2) × (dH/H)
dQ/Q = (3/4) × (dH/H)
dQ/Q = (dH/H)
dQ/Q = (3/2) × (dH/H)
Weight of the liquid displaced
Pressure with which the liquid is displaced
Viscosity of the liquid
Compressibility of the liquid
Neutral equilibrium
Stable equilibrium
Unstable equilibrium
None of these
0.8
1
1.2
1.6
Pressure force
Elastic force
Surface tension force
Viscous force
dp/ρ + g.dz + v.dv = 0
dp/ρ - g.dz + v.dv = 0
ρ.dp + g.dz + v.dv = 0
ρ.dp - g.dz + v.dv = 0