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
D. The resultant force on a body due to the fluid surrounding it
100 cm3
250 cm3
500 cm3
1000 cm3
Specific gravity of liquids
Specific gravity of solids
Specific gravity of gases
Relative humidity
U-tube with water
Inclined U-tube
U-tube with mercury
Micro-manometer with water
Minimum
Maximum
Zero
Could be any value
Directly proportional to (radius)2
Inversely proportional to (radius)2
Directly proportional to (radius)4
Inversely proportional to (radius)4
Decreases
Increases
Remain same
None of these
4.5 kN/m3
6 kN/m3
7.5 kN/m3
10 kN/m3
Specific weight
Mass density
Specific gravity
None of these
Same as
Less than
More than
None of these
It is easier to see through the glass tube
Glass tube is cheaper than a metallic tube
It is not possible to conduct this experiment with any other tube
All of the above
Real
Ideal
Newtonian
Non-Newtonian
Venturimeter
Orifice plate
Nozzle
All of the above
d = (D⁵/8fl)1/2
d = (D⁵/8fl)1/3
d = (D⁵/8fl)1/4
d = (D⁵/8fl)1/5
One dimensional flow
Uniform flow
Steady flow
Turbulent flow
Suction pressure
Vacuum pressure
Negative gauge pressure
All of these
Triangular
Rectangular
Square
Trapezoidal
v₁²/2g
v₂²/2g
0.5 v₁²/2g
0.375 v₂²/2g
0.384 Cd × L × H1/2
0.384 Cd × L × H3/2
1.71 Cd × L × H1/2
1.71 Cd × L × H3/2
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
0.34 times
0.67 times
0.81 times
0.95 times
Real fluid
Ideal fluid
Newtonian fluid
Non-Newtonian fluid
More
Less
Same
More or less depending on size of glass tube
Equal to
Less than
More than
None of these
Neutral equilibrium
Stable equilibrium
Unstable equilibrium
None of these
Bottom surface of the body
C.G. of the body
Metacentre
All points on the surface of the body
Path line
Stream line
Steak line
Potential line
Boyle's law
Archimedes principle
Pascal's law
Newton's formula
(bd²/12) + x
(d²/12 x) + x
b²/12 + x
d²/12 + x
Sub-sonic velocity
Super-sonic velocity
Lower critical velocity
Higher critical velocity
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