Steady flow
Unsteady flow
Laminar flow
Turbulent flow
C. Laminar flow
μπ²NR/60t
μπ²NR²/60t
μπ²NR³/60t
μπ²NR⁴/60t
wH/2
wH
wH2/2
wH2/4
Remains constant
Increases
Decreases
Depends upon mass of liquid
Specific weight
Mass density
Specific gravity
None of these
Inertia
Gravity
Viscous
None of these
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
Linearly
First slowly and then steeply
First steeply and then gradually
Unpredictable
1.84 (L - 0.1nH)H3/2
1.84 (L - nH)H2
1.84 (L - 0.1nH)H5/2
1.84 (L - nH)H3
Minimum
Maximum
Zero
Could be any value
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)
Less than 2000
Between 2000 and 2800
More than 2800
None of these
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
Linear
Parabolic
Hyperbolic
Inverse type
400 kg/cm²
4000 kg/cm²
40 × 10⁵ kg/cm²
40 × 10⁶ kg/cm²
Less than 2000
Between 2000 and 2800
More than 2800
None of these
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
p/sinα
2p/sinα
p/2sinα
2p/sin (α/2)
9.81 kN/m3
9.81 × 103 N/m3
9.81 × 10-6 N/mm3
Any one of these
Pressure head
Velocity head
Pressure head + velocity head
Pressure head - velocity head
Specific gravity = gravity × density
Dynamic viscosity = kinematic viscosity × density
Gravity = specific gravity × density
Kinematic viscosity = dynamic viscosity × density
Cannot be compressed
Occupy definite volume
Are not affected by change in pressure and temperature
None of the above
Viscosity
Osmosis
Surface tension
Cohesion
The head loss for all the pipes is same
The total discharge is equal to the sum of discharges in the various pipes
The total head loss is the sum of head losses in the various pipes
Both (A) and (B)
Steady uniform
Non-steady non-uniform
Non-steady uniform
Steady non-uniform
Cylindrical shape
Convergent shape
Divergent shape
Convergent-divergent shape
Neutral equilibrium
Stable equilibrium
Unstable equilibrium
None of these
N/mm2
N/m2
Head of liquid
All of these
Cannot be subjected to shear forces
Always expands until it fills any container
Has the same shear stress at a point regardless of its motion
Cannot remain at rest under action of any shear force
Pressure, velocity and temperature
Shear stress and rate of shear strain
Shear stress and velocity
Rate of shear strain and temperature
Remain unaffected
Increases
Decreases
None of these