Does not change
Decreases
Increases
None of these
B. Decreases
Pressure head
Velocity head
Pressure head + velocity head
Pressure head - velocity head
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
Less than
More than
Equal to
None of these
Meta centre should be above e.g.
Centre of buoyancy and e.g. must lie on same vertical plane
A righting couple should be formed
All of the above
ω.r/2g
ω².r²/2g
ω.r/4g
ω².r²/4g
At the Centroid
Above the Centroid
Below the Centroid
At metacentre
Decreases
Increases
Remain same
None of these
Dissolved air
Dissolved salt
Suspended matter
All of the above
Specific weight
Specific mass
Specific gravity
Specific density
10 m/sec
25 m/sec
2 m/sec
50 m/sec
Centre of pressure
Centre of gravity
Centre of buoyancy
Metacentre
Real fluid
Ideal fluid
Newtonian fluid
Non-Newtonian fluid
Steady flow
Turbulent flow
Vortex flow
Uniform flow
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
Unity
Greater than unity
Greater than 2
Greater than 4
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
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
Cc × Cv
Cc × Cr
Cv × Cr
Cc/Cr
1
5
7
6
Mass
Momentum
Energy
Work
flv²/2gd
flv²/gd
3flv²/2gd
4flv²/2gd
Horizontal line
Inclined line with flow upwards
Inclined line with flow downwards
Any direction and in any location
The pressure below the nappe is atmospheric
The pressure below the nappe is negative
The pressure above the nappe is atmospheric
The pressure above the nappe is negative
Gas law
Boyle's law
Charles law
Pascal's law
Less than 2000
Between 2000 and 4000
More than 4000
Less than 4000
wH
wH/2
wH2/2
wH2/3
Z + p/w + v²/2g = constant
Z + p/w - v²/2g = constant
Z - p/w + v²/2g = constant
Z - p/w - v²/2g = constant
2gH
H × √(2g)
2g × √H
√(2gh)
(v₁ - v₂)²/g
(v₁² - v₂²)/g
(v₁ - v₂)²/2g
(v₁² - v₂²)/2g
Cd × a × √(2gH)
Cd × a × √(2g) × H3/2
Cd × a × √(2g) × H2
Cd × a × √(2g) × H5/2