1 %
1.5 %
2 %
2.5 %
D. 2.5 %
w
wh
w/h
h/w
dQ/Q = (1/2) × (dH/H)
dQ/Q = (3/4) × (dH/H)
dQ/Q = (dH/H)
dQ/Q = (3/2) × (dH/H)
Maximum
Minimum
Zero
Nonzero finite
Neutral
Stable
Unstable
None of these
Remain same
Increases
Decreases
Shows erratic behaviour
At the inlet
At the outlet
At the summit
At any point between inlet and outlet
Specific weight
Mass density
Specific gravity
None of these
Specific gravity = gravity × density
Dynamic viscosity = kinematic viscosity × density
Gravity = specific gravity × density
Kinematic viscosity = dynamic viscosity × density
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
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
Orifice plate
Venturimeter
Rotameter
Pitot tube
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
Surface tension
Cohesion of the liquid
Adhesion of the liquid molecules and the molecules on the surface of a solid
All of the above
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
Higher
Lower
Same as
None of these
Negligible
Same as buoyant force
Zero
None of the above
Less than twice
More than twice
Less than three times
More than three times
14π R1/2/15Cd × a √(2g)
14π R3/2/15Cd × a √(2g)
14π R5/2/15Cd × a √(2g)
14π R7/2/15Cd × a √(2g)
0.5 a. √2gH
0.707 a. √2gH
0.855 a. √2gH
a. √2gH
Inertia force
Viscous force
Gravity force
All of these
Concave
Convex
Plane
None of these
Surface tension
Viscosity
Friction
Cohesion
Viscosity
Air resistance
Surface tension forces
Atmospheric pressure
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
Varies as the square of the radial distance
Increases linearly as its radial distance
Increases as the square of the radial distance
Decreases as the square of the radial distance
At the Centroid
Above the Centroid
Below the Centroid
At metacentre
19.24 kPa
29.24 kPa
39.24 kPa
49.24 kPa
1 Pa
91 Pa
981 Pa
9810 Pa
Pressure
Flow
Shape
Volume
Sinθ
1/Sinθ
Cosθ
1/Cosθ