Chapter 11 Turbulent Flow
• Shear stress in turbulent flow
where,
μ = dynamic coefficient of viscosity (fluid characteristic)
h = eddy viscosity coefficient (flow characteristic)
Hydrodynamically smooth : (k/d) < 0.25
Boundary in transition :0.25 < (k/d)< 6.0
Hydrodynamically Rough :(k/d) > 6.0
(a) Prandtl’s universal velocity distribution equation :
where
shear or friction velocity.
y = distance from pipe wall
R = radius of pipe.
(b) Karman - Prandtl Velocity distribution equation :
(i) Hydro Dynamically Smooth pipe
(ii) Hydro Dynamically Rough pipe
where
V* = shear velocity
y = distance from pipe wall
k = average height of roughness
v = kinematic viscosity.
(c) Velocity distribution in terms of mean velocity
The above equation is for both rough and smooth pipes.
(a) Friction factor ‘f’ for laminar flow :
f = (64/Re) where Re = Reynolds number
(b) Friction factor ‘f’ for transition flow :
There exists no specific relationship between f and Re for transition flow in pipes.
(c) Friction factor (f) for turbulent flow in smooth pipes :
(d) Friction factor (f) for turbulent flow in rough pipes
This equation shows that for rough pipes friction factor depends only on R/K (Relative smoothness) and not on Reynolds number (Re)
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1. What is turbulent flow in civil engineering? |
2. How is turbulent flow different from laminar flow? |
3. What factors affect turbulent flow in civil engineering? |
4. How is turbulent flow measured in civil engineering? |
5. What are the applications of understanding turbulent flow in civil engineering? |
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