Actual velocity of jet at vena contracta to the theoretical velocity
Loss of head in the orifice to the head of water available at the exit of the orifice
Loss of head in the orifice to the head of water available at the exit of the orifice
Area of jet at vena-contracta to the area of orifice
D. Area of jet at vena-contracta to the area of orifice
Less than 2000
Between 2000 and 2800
More than 2800
None of these
Below the center of gravity
Below the center of buoyancy
Above the center of buoyancy
Above the center of gravity
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
Sum
Difference
Arithmetic mean
Geometric mean
Width of channel at the top is equal to twice the width at the bottom
Depth of channel is equal to the width at the bottom
The sloping side is equal to half the width at the top
The sloping side is equal to the width at the bottom
(v₁ - v₂)²/g
(v₁² - v₂²)/g
(v₁ - v₂)²/2g
(v₁² - v₂²)/2g
wH
wH/2
wH2/2
wH2/3
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
Velocity of flow in an open channel
Depth of flow in an open channel
Hydraulic jump
Depth of channel
The liquid particles at all sections have the same velocities
The liquid particles at different sections have different velocities
The quantity of liquid flowing per second is constant
Each liquid particle has a definite path
The area is horizontal
The area is vertical
The area is inclined
All of the above
Pressure in pipes, channels etc.
Atmospheric pressure
Very low pressure
Difference of pressure between two points
v²/2g
0.5v²/2g
0.375v²/2g
0.75v²/2g
0.375
0.5
0.707
0.855
Up-thrust
Buoyancy
Center of pressure
All the above are correct
Gauge pressure
Absolute pressure
Positive gauge pressure
Vacuum pressure
Pressure
Flow
Shape
Volume
Atmospheric pressure
Pressure in pipes and channels
Pressure in Venturimeter
Difference of pressures between two points in a pipe
N-m/s
N-s/m2
m2/s
N-m
Cohesion
Adhesion
Viscosity
Surface tension
Straight line
Parabolic curve
Hyperbolic curve
Elliptical
19.24 kPa
29.24 kPa
39.24 kPa
49.24 kPa
Supersonics, as with projectile and jet propulsion
Full immersion or completely enclosed flow, as with pipes, aircraft wings, nozzles etc.
Simultaneous motion through two fluids where there is a surface of discontinuity, gravity forces, and wave making effect, as with ship's hulls
All of the above
Actual velocity of jet at vena contracta to the theoretical velocity
Loss of head in the orifice to the head of water available at the exit of the orifice
Loss of head in the orifice to the head of water available at the exit of the orifice
Area of jet at vena-contracta to the area of orifice
Higher
Lower
Same
Higher/lower depending on temperature
15.3 m
25.3 m
35.3 m
45.3 m
The center of gravity of the body and the metacentre
The center of gravity of the body and the center of buoyancy
The center of gravity of the body and the center of pressure
Center of buoyancy and metacentre
400 kg/cm²
4000 kg/cm²
40 × 10⁵ kg/cm²
40 × 10⁶ kg/cm²
Weight of the liquid displaced
Pressure with which the liquid is displaced
Viscosity of the liquid
Compressibility of the liquid
Half the depth
Half the breadth
Twice the depth
Twice the breadth