2.89 kN
8.29 kN
9.28 kN
28.9 kN
B. 8.29 kN
p = T × r
p = T/r
p = T/2r
p = 2T/r
0° C
0° K
4° C
20° C
wH/2
wH
wH2/2
wH2/4
Same as
Lower than
Higher than
None of these
Metres² per sec
kg-sec/metre
Newton-sec per metre²
Newton-sec per meter
Higher surface tension
Lower surface tension
Surface tension is no criterion
High density and viscosity
Remain unaffected
Increases
Decreases
None of these
Neutral
Stable
Unstable
None of these
1000 kg
4000 kg
2000 kg
8000 kg
Centre of pressure
Centre of gravity
Centre of buoyancy
Metacentre
Mass of liquid displaced
Viscosity of the liquid
Pressure of the liquid displaced
Depth of immersion
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 plane
Constant
Variable
Zero
Zero under limiting conditions
Sinθ
1/Sinθ
Cosθ
1/Cosθ
Surface tension
Cohesion of the liquid
Adhesion of the liquid molecules and the molecules on the surface of a solid
All of the above
At the inlet
At the outlet
At the summit
At any point between inlet and outlet
The nature of the liquid and the solid
The material which exists above the free surface of the liquid
Both of die above
Any one of the above
Gauge pressure + atmospheric pressure
Gauge pressure - atmospheric pressure
Atmospheric pressure - gauge pressure
Gauge pressure - vacuum pressure
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 plane
(bd²/12) + x
(d²/12 x) + x
b²/12 + x
d²/12 + x
It has low vapour pressure
It is clearly visible
It has low surface tension
It can provide longer column due to low density
Directly proportional to its distance from the centre
Inversely proportional to its distance from the centre
Directly proportional to its (distance)2 from the centre
Inversely proportional to its (distance)2 from the centre
More
Less
Same
More or less depending on size of glass tube
Cc × Cv
Cc × Cr
Cv × Cr
Cc/Cr
2 metres of water column
3 metres of water column
3.5 metres of water column
4 m of water column
Equal
Directly proportional
Inversely proportional
None of these
14π R1/2/15Cd × a √(2g)
14π R3/2/15Cd × a √(2g)
14π R5/2/15Cd × a √(2g)
14π R7/2/15Cd × a √(2g)
Centre of gravity
Centre of pressure
Metacentre
Centre of buoyancy
Reynold's number
Froude's number
Weber's number
Mach number
Water surface
Center of pressure
Center of gravity
Center of buoyancy