(q/g)1/2
(q²/g)1/3
(q³/g)1/4
(q⁴/g)1/5
B. (q²/g)1/3
2.89 kN
8.29 kN
9.28 kN
28.9 kN
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
(q/g)1/2
(q²/g)1/3
(q³/g)1/4
(q⁴/g)1/5
Less than
More than
Equal to
None of these
Absolute pressure
Velocity of fluid
Flow
Rotation
Remains constant
Increases
Decreases
Depends upon mass of liquid
1.84 (L - 0.1nH)H3/2
1.84 (L - nH)H2
1.84 (L - 0.1nH)H5/2
1.84 (L - nH)H3
p = T × r
p = T/r
p = T/2r
p = 2T/r
Steady flow
Uniform flow
Streamline flow
Turbulent flow
Low pressure
High pressure
Moderate pressure
Vacuum pressure
Elastic properties of the pipe material
Elastic properties of the liquid flowing through the pipe
Speed at which the valve is closed
All of the above
Triangular
Rectangular
Square
Trapezoidal
Less than unity
Unity
Between 1 and 6
More than 6
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
0° C
0° K
4° C
20° C
Avoid interruption in the flow
Increase discharge
Increase velocity
Maintain pressure difference
Centroid of the volume of fluid vertically above the body
Centre of the volume of floating body
Center of gravity of any submerged body
Centroid of the displaced volume of fluid
Pascal's law
Archimedess principle
Principle of floatation
Bernoulli's theorem
There is no loss of energy of the liquid flowing
The velocity of flow is uniform across any cross-section of the pipe
No force except gravity acts on the fluid
All of the above
Decreases linearly with elevation
Remain constant
Varies in the same way as the density
Increases exponentially with elevation
wH
wH/2
wH2/2
wH2/3
Up-thrust
Reaction
Buoyancy
Metacentre
The bodies A and B have equal stability
The body A is more stable than body B
The body B is more stable than body A
The bodies A and B are unstable
(μπ²N/60t) × (R₁ - R₂)
(μπ²N/60t) × (R₁² - R₂²)
(μπ²N/60t) × (R₁³ - R₂³)
(μπ²N/60t) × (R₁⁴ - R₂⁴)
Maximum at the centre and minimum near the walls
Minimum at the centre and maximum near the walls
Zero at the centre and maximum near the walls
Maximum at the centre and zero near the walls
The direction and magnitude of the velocity at all points are identical
The velocity of successive fluid particles, at any point, is the same at successive periods of time
The magnitude and direction of the velocity do not change from point to point in the fluid
The fluid particles move in plane or parallel planes and the streamline patterns are identical in each pleasure
Q = (2/3) Cd × b × √(2g) × (H2 - H1)
Q = (2/3) Cd × b × √(2g) × (H2 1/2 - H1 1/2)
Q = (2/3) Cd × b × √(2g) × (H2 3/2 - H1 3/2)
Q = (2/3) Cd × b × √(2g) × (H2 2 - H1 2)
Law of gravitation
Archimedes principle
Principle of buoyancy
All of the above
Centre of gravity
Centre of pressure
Metacentre
Centre of buoyancy
It is incompressible
It has uniform viscosity
It has zero viscosity
It is at rest