ρ ω2 r2
2ρ ω2 r2
ρ ω2 r2/2
ρ ω2 r2/4
C. ρ ω2 r2/2
Higher
Lower
Same
Higher/lower depending on temperature
Red wood
Say bolt
Engler
Orsat
Velocity of flow in an open channel
Depth of flow in an open channel
Hydraulic jump
Depth of channel
Buoyancy, gravity
Buoyancy, pressure
Buoyancy, inertial
Inertial, gravity
Inversely proportional to H3/2
Directly proportional to H3/2
Inversely proportional to H5/2
Directly proportional to H5/2
0° C
0° K
4° C
20° C
Sill or crest
Nappe or vein
Orifice
None of these
Directly
Inversely
Both A and B
None of these
0.3 to 0.45
0.50 to 0.75
0.75 to 0.95
0.95 to 1.0
To control the pressure variations due to rapid changes in the pipe line flow
To eliminate water hammer possibilities
To regulate flow of water to turbines by providing necessary retarding head of water
All of the above
Cylindrical shape
Convergent shape
Divergent shape
Convergent-divergent shape
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
Rectangular
Triangular
Trapezoidal
Circular
Parallel to central axis flow
Parallel to outer surface of pipe
Of equal velocity in a flow
Along which the pressure drop is uniform
Pressure
Distance
Density
Flow
Velocity of liquid
Pressure of liquid
Area of mouthpiece
Length of mouthpiece
Pressure in pipes, channels etc.
Atmospheric pressure
Very low pressure
Difference of pressure between two points
v₁²/2g
v₂²/2g
0.5 v₁²/2g
0.375 v₂²/2g
Ratio of inertial force to force due to viscosity
Ratio of inertial force to force due to gravitation
Ratio of inertial force to force due to surface tension
All the four ratios of inertial force to force due to viscosity, gravitation, surface tension, and elasticity
Effects
Does not effect
Both A and B
None of these
At C.G. of body
At center of pressure
Vertically upwards
At metacentre
(bd²/12) + x
(d²/12 x) + x
b²/12 + x
d²/12 + x
Are viscous
Possess surface tension
Are compressible
Possess all the above properties
Newton-sec/m
Newton-m/sec
Newton/m
Newton
Resistance to shear stress is small
Fluid pressure is zero
Linear deformation is small
Only normal stresses can exist
Vertical upward force through e.g. of body and center line of body
Buoyant force and the center line of body
Midpoint between e.g. and center of buoyancy
All of the above
Less than
More than
Equal to
None of these
Real fluid
Ideal fluid
Newtonian fluid
Non-Newtonian fluid
Equal to
Less than
More than
None of these
N-m/s2
N-s/m2
Poise
Stoke