Water amd wastewater treatemt Hydraulics

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Presentation transcript:

Water amd wastewater treatemt Hydraulics

Hydraulics Objective Analysis of pipe flow system Head losses in pipes Flow measurements Small diameter gravity and vaccum sewers Introduction to tutorial questions

Pipe flow analysis E1 = E2 ± ΔE The Bernoulli’s Equation 1 2 E1 = E2 ± ΔE P1/ ρg + v21 /2g + Z1 = P2/ ρg + v22 /2g + Z2 ± ΔE

Bernoulli’s equation BE is used in analysis of pipe flow It states that total energy remains constant along a stream line (That is total head is constant) It uses certain assumptions Flow is steady Fluid is incompressible Valid at two points along a single streamline The hydraulic grade and the energy line are graphical presentations of the Bernoulli’s equation (BE)

Energy and hydrulic grade line Energy grade line E2 H1 v21 /2g H2 Hydraulic grade line v22/2g P1/ ρg P2/ ρg 1 2 V Water supply The HGL should never fall below the GL The HGL helps to calculate the pressure in pipes and select the pipe material Wastewater . HGL Analyze the system’s hydraulic grade line to determine if you can accommodate design flows in the drainage system without causing flooding at some location or causing flows to exit the system at locations where this is unacceptable. Z1 Z2 Reference level

Energies, Head 2 Z2 P2/ ρg v22/2g H2 E2 Reference level EGL HGL Energy Head (total) Piezometric head Pressure head Elevation head (potential)

Energies, Heads H2 Piezometric head HGL P2/ ρg Pressure head Velocity head neglected except well above 1 m/s (example: pumping stations) 2 Z2 Elevation head (potential) Reference level

Hydraulic gradient Slope of the hydraulic grade line

Hydraulic gradient Slope of the hydraulic grade line

Hydraulic losses Friction, minor ΔE results from a friction between the water and the pipe wall, and /or a turbulence developed by obstructions of the flow ΔE = hf + hm = Rf Qn (f) + Rm Qn (m) hf,m = Friction, Minor loss (respectively) Rf,m = Pipe resistance Q = Flow nf, m = exponents

Friction Losses Darcy- Weisbach λ = Friction factor (-) L = Pipe length (m) D = Pipe diameter (m) Q = Pipe flow (m3 /s) Or propotional to the kinetic energy

Friction factor Friction factor, λ is the most important parameter in the Darcy-weisbach equation Is the complex function of the Reynolds number and relative roughness Reynolds Number V = Flow velocity (m/s) D = Pipe diameter (m) = Kinematic viscosity (m2/s) Temperature, T(0 C)

Flow regime Laminar flow – Re falls under 2000 Transitional zone - Re falls between 2000 and 4000 Turbulent flow - Re above 4000 For Laminar flow λ = 64/ Re

Choice for rough pipes There are empirical formula and diagrams to determine friction factor (f) depending on the pipe roughness and Reynolds Number Moody diagram Colebrook-white equations etc.

The Moody diagram Department of Plant and Environmental Sciences

Absolute rougness

Friction losses Hazen –Williams Or L = Pipe length (m) C = Hazen-Williams factor D = Pipe diameter (m) Q = Pipe flow (m3 /s) R = Hydrualic Radius (flow area/wetted perimeter) S = Slope of energy grade line = hf /L

Hazen-Williams Factors

Friction losses Manning or L = Pipe length (m) n = mannings factor ( m-1/3 s) D = Pipe diameter (m) Q = Pipe flow (m3 /s) R = Hydrualic Radius (flow area/wetted perimeter) S = Slope of energy grade line = hf /L

Manning factor

The best formula ? Darcy-weisbach – the most accurate Hazen-williams- (straight forward and simpler (friction coefficient not function of diameter or velocity), suitable for smooth pipes not attacked by corrosion) Mannings- straight forward, suitable for rough pipes, commonly applied for open channel flows

Difference between pressure flow and open channel flow EGL v21 /2g EGL Open channel flow (in large gravity sewer) v21 /2g HGL HGL Pressure flow

Minor losses Given by hf = k V2 /2g K determined experimentally for various fittings Values of K for various fittings: Valve ( fully open ) 2 Tee 0.2 – 2.0 Bend 1.2

Flow measurements in pipes Orifice plates Where C = discharge coefficient

Flow measurements in open channel flow Sharp crested weir L = Length of weir, m Cd = discharge coefficient

Small diameter sewer collection system Transport sewage to treatment or disposal point Size and length of sewer depends upon the type of sewerage system (centralised or decentralised) Need sufficient velocity to transport sewage

Small diameter sewer network Septic tank effluent gravity (STEG) Septic tank effluent pump (STEP) and pressure sewer with grinder pumps

Small diameter sewer network Vacuum sewer

Friction losses Hazen –Williams Hazen –Williams formula based on actual flow area- so inside pipe diameter is used. Hazen –Williams Or L = Pipe length (m) C = Hazen-Williams factor D = Pipe diameter (m) Q = Pipe flow (m3 /s) R = Hydrualic Radius (flow area/wetted perimeter) S = Slope of energy grade line = hf /L

Design and layout of collection system Information required Topography of the area Depth of soil Depth of water table Depth of freezing zone Amount (daily minimum, average and peak flow rates) Population growth rate source:nn

Excersise-Sewer collection system Prepare a profile Select a pipe size Calculate the velocity Calculate the pipe cross sectional area and determine the actual capacity Check for the surcharged condition source:nn

Friction Losses Hazen –Williams Or L = Pipe length (m) C = Hazen-Williams factor D = Pipe diameter (m) Q = Pipe flow (m3 /s) R = Hydrualic Radius (flow area/wetted perimeter) S = Slope of energy grade line = hf /L

Pipe selection Crites and Technobanoglous 1998)

Crites and Technobanoglous 1998)

Design of STEP sewer Design of STEP for a small community as shown in plan view below. The informations given are:

1.31English unit !!!!!!!! R = D/4

L Slope should be 0.5 to 1.5 % If too low -pipe is oversized Design flow/CA of pipe EGL/100 *L Plot EGL –begin from D/S

References Water supply and Sewerage – Terence J McGhee Chapter 3 (Page 24 – 61) (IHNALibrary catlog No. 628.1 MCG) Crites, R. and G. Technobanoglous (1998). Small and decentralized wastewater management systems, McGraw-Hill. (Chapter 6) Advanced Water Distribution Modelling and Management by Haestad and et al. (Chapter 2.3, 2.4, 2.5, 2.6) (IHNALibrary catlog No. 628.1)

THANK YOU