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
A. Varies as the square of the radial distance
Surface tension
Viscosity
Friction
Cohesion
Remains horizontal
Becomes curved
Falls on the front end
Falls on the back end
Gauge pressure
Absolute pressure
Positive gauge pressure
Vacuum pressure
Orifice
Notch
Weir
Dam
51 cm
50 cm
52 cm
52.2 cm
Q = Cd × bH₁ × √(2gh)
Q = Cd × bH2 × √(2gh)
Q = Cd × b (H2 - H1) × √(2gh)
Q = Cd × bH × √(2gh)
Viscosity
Osmosis
Surface tension
Cohesion
Surface tension
Compressibility
Capillarity
Viscosity
Inertia force
Viscous force
Gravity force
Pressure force
Absolute pressure
Velocity of fluid
Flow
Rotation
Pascal's law
Dalton's law of partial pressure
Newton's law of viscosity
Avogadro's hypothesis
Dissolved air
Dissolved salt
Suspended matter
All of the above
Avoid the tendency of breaking away the stream of liquid
To minimise frictional losses
Both (A) and (B)
None of these
Same as
Less than
More than
None of these
Bourdon tube
Pirani Gauge
Micro-manometer
Lonisation gauge
Actual velocity of jet at vena contracta to the theoretical velocity
Area of jet at vena contracta to the area of orifice
Actual discharge through an orifice to the theoretical discharge
None of the above
At the centre of gravity
Above the centre of gravity
Below be centre of gravity
Could be above or below e.g. depending on density of body and liquid
Kinematic viscosity in C. G. S. units
Kinematic viscosity in M. K. S. units
Dynamic viscosity in M. K. S. units
Dynamic viscosity in S. I. units
Weir
Notch
Orifice
None of these
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
Specific viscosity
Viscosity index
Kinematic viscosity
Coefficient of viscosity
Planes of the body are completely smooth
Space around the body is completely filled with the fluid
Fluid particles do not exert any influence on one another
All of the above
Moving
Viscous
Viscous and static
Viscous and moving
Remains constant
Increases
Decreases
Depends upon mass of liquid
The weight of the body
More than the weight of the body
Less than the weight of the body
Weight of the fluid displaced by the body
0.62
0.76
0.84
0.97
0.1 N-s/m2
1 N-s/m2
10 N-s/m2
100 N-s/m2
p = T × r
p = T/r
p = T/2r
p = 2T/r
μ π³ N² R² /1800 t
μ π³ N² R⁴ /1800 t
μ π³ N² R² /3600 t
μ π³ N² R⁴ /3600 t
Frictional force
Viscosity
Surface friction
All of the above