Surface tension force
Viscous force
Gravity force
Elastic force
B. Viscous force
10-2 m2/s
10-3 m2/s
10-4 m2/s
10-6 m2/s
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
K.ρ
K/ρ
ρ/K
None of these
9.81 kN/m3
9.81 × 103 N/m3
9.81 × 10-6 N/mm3
Any one of these
Same as
Lower than
Higher than
None of these
(2A√H₁)/(Cd × a√2g)
(2AH₁)/(Cd × a√2g)
(2AH₁3/2)/(Cd × a√2g)
(2AH₁²)/(Cd × a√2g)
Negligible
Same as buoyant force
Zero
None of the above
Directly proportional to its distance from the centre
Inversely proportional to its distance from the centre
Directly proportional to its (distance)2 from the centre
Inversely proportional to its (distance)2 from the centre
In a compressible flow, the volume of the flowing liquid changes during the flow
A flow, in which the volume of the flowing liquid does not change, is called incompressible flow
When the particles rotate about their own axes while flowing, the flow is said to be rotational flow
All of the above
Steady
Unsteady
Both A and B
None of these
The weight of the body
More than the weight of the body
Less than the weight of the body
Weight of the fluid displaced by the body
Pressure force
Elastic force
Gravity force
Viscous force
Resultant force acting on a floating body
Equal to the volume of liquid displaced
Force necessary to keep a body in equilibrium
The resultant force on a body due to the fluid surrounding it
One stoke
One centistoke
One poise
One centipoise
Equal to
One-fourth
One-third
One-half
Velocity
(Velocity)2
(Velocity)3
(Velocity)4
1
5
7
6
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
500 kg
1000 kg
1500 kg
2000 kg
Specific gravity = gravity × density
Dynamic viscosity = kinematic viscosity × density
Gravity = specific gravity × density
Kinematic viscosity = dynamic viscosity × density
10 m/sec
25 m/sec
2 m/sec
50 m/sec
Real
Ideal
Newtonian
Non-Newtonian
The center of buoyancy is located at the center of gravity of the displaced liquid
For stability of a submerged body, the center of gravity of body must lie directly below the center of buoyancy
If C.G. and center of buoyancy coincide, the submerged body must lie at neutral equilibrium for all positions
All floating bodies are stable
Be horizontal
Make an angle in direction of inclination of inclined plane
Make an angle in opposite direction to inclination of inclined plane
Any one of above is possible
When its meatcentric height is zero
When the metacentre is above C.G.
When its e.g. is below its center of buoyancy
Metacentre has nothing to do with position of e.g. for determining stability
Cylindrical shape
Convergent shape
Divergent shape
Convergent-divergent shape
Adhesion
Cohesion
Viscosity
Compressibility
Inversely proportional to H3/2
Directly proportional to H3/2
Inversely proportional to H5/2
Directly proportional to H5/2
Double
Four times
Eight times
Sixteen times