WATER DISTRIBUTION NETWORKS

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WATER DISTRIBUTION NETWORKS CE 370 1 Components of Water Supply System 2 1

Water Distribution System Water distribution systems are designed to adequately satisfy the water requirements for a combinations of the following demands: Domestic Commercial Industrial Fire-fighting The system should be capable of meeting the demands at all times and at satisfactory pressure 3 Water Distribution System The main elements of the distribution system are: Pipe systems Pumping stations Storage facilities Fire hydrants House service connections Meters Other appurtenances 4 2

System Configurations Distribution systems may be classified as: Branching systems Grid systems A combination of the above two systems The configuration of the system is dictated by: Street patterns Topography Degree and type of development of the area Location of the treatment and storage works. 5 6 3

System Configurations Branching vs. grid systems: A grid system is usually preferred over a branching system, since it can furnish a supply to any point from at least two directions The branching system has dead ends, therefore, does not permit supply from more than one direction. Should be avoided where possible. In locations where sharp changes in topography occur (hilly or mountainous areas), it is common practice to divide the distribution system into two or more service areas. 7 Basic System Requirements Pressure: Pressure should be great enough to adequately meet consumer and fire-fighting needs. Pressure should not be excessive: Cost consideration Leakage and maintenance increase Capacity: The capacity is determined on the bases of local water needs plus fire-fighting demand. Pipe sizes should be selected to avoid high velocities: Pipe sizes should selected based on flow velocity of 3-5 fps Where fire-fighting is required, minimum pipe diameter is 6 in. 8 4

Hydraulic Design The design flowrate is based on the maximum of the following two rates: Maximum day demand plus fire demand Maximum hourly rate Analysis of distribution system: Distribution system have series of pipes of different diameters. In order to simplify the analysis, skeletonizing is used. Skeletonizing is the replacement of a series of pipes of varying diameters with one equivalent pipe or replacing a system of pipes with one equivalent pipe. 9 Skeletonization 10 5

Hydraulic Design Example: Consider the piping system shown in the figure, replace (a) pipes BC and CD with an equivalent 12-in. pipe and (b) the system from B to D with an equivalent 20-in. pipe. Solution: a) for pipes in series: 1. assume any value for Q through BCD (8 cfs) 2. from nomograph with Q = 8 cfs and dia = 18-in, read head loss for BC = 6.1ft/1000ft 3. from nomograph with Q = 8 cfs and dia = 16-in, read head loss for CD = 11ft/1000ft 4. total head loss BD = (6.1/1000)*200+(11/1000)*500 = 6.72ft 11 200 ft - 18 in. C 500 ft - 16 in. A B A D E Z 900 ft - 12 in. 12 6

Nomograph for Hazen Williams equation 13 Hydraulic Design 5. the total head loss for 12-in equivalent pipe at 8 cfs is 45ft/1000ft (from nomograph) 6. head loss BCD = head loss BD, therefore; 6.72ft = L eq * (45/1000) L eq = 6.72 * (1000/45) = 149 ft b) for pipes in parallel: 1. assume any value of head loss between BD (h L =5 ft) 2. for the equivalent pipe (L = 149 ft), head loss per 1000ft is; h L = (5/149)*1000 = 33.5ft/1000ft Diameter of equivalent pipe = 12-in Q eq = 6.8 cfs (from nomograph) 14 7

Hydraulic Design 3. for the 900 ft 12-in pipe: h L = (5/900)*1000 = 5.5ft/1000ft Q 900 = 2.6 cfs (from nomograph) 4. total flow = 6.9 + 2.6 = 9.4 cfs 5. for Q = 9.4 cfs and 20-in pipe: head loss = 4.8ft/1000ft (nomograph) 6. head loss 12-in pipe = head loss 20-in pipe 5 ft = L * (4.8ft/1000ft) L = 5 * (1000/4.8) = 1042 ft 15 Hydraulic Design Pipe networks: Pipe networks are composed of a number of constant-diameter pipe sections containing pumps and fittings. From next figure, following are defined: Node: end of each pipe section. (A, B, C, D, E, F, G, and H) Junction node: points where pipes meet and where flow may be introduces or withdrawn. (B, C, D, E, F, and G) Fixed-grade nodes: points where constant grade is maintained. (A and B) Loops: closed pipe circuits. (1 and 2) From above terminology, we can write the following eq. P = J + L + F 1 Where: P = # pipes, J = # Junction node, L = #loops, F = # fixed-grade nodes 16 8

Pipe Network 17 Hydraulic Design Loop equations: Hydraulic performance of pipe networks are based on mass continuity and energy conservation. Continuity of mass: ΣQ in - ΣQ out = Q e (J number of equations) Q in = inflow into node Q out = outflow from node Q e = external flow into the system or withdrawal Conservation of energy: Σh L = ΣE p (L number of equations) h L = head loss; E p = pump head For fixed-grade nodes, the following can be written: E = Σh L - ΣE p (F-1 equations) 18 9

Hydraulic Design Loop equations: (continue) Frictional losses in pipes: h LP = K P Q n Where; K P = constant incorporating pipe size, its roughness, and units used n = an exponent The Hazen-Williams formula for head loss is given as: h LP = K P Q 1.85 Minor losses: These losses are due fittings, valves, meters, or other insertions that affect the flow. They are expressed as: h LM = K M Q 2 Where; K M = minor loss constant 19 Hydraulic Design Node equations: When considering nodes, the principle relationship used is the continuity equation: Q in -Q out = Q e The discharge in pipe ab can be expressed in terms of grade (head) as the following: h L = KQ n h Lab = h a h b = K ab Q n Or Q ab Q ab = {(h a -h b )/K ab } 1/n a b Q e 20 10

Hydraulic Design Node equations: If pump exist in the line, then junction nodes are specified at the inlet and outlet. for continuity: Q ab = Q cd {(h a -h b )/K ab } 1/n = {(h c -h d )/K cd } 1/n h a -h b = (K ab /K cd ) (h c h d ) The head change across pump is: h c h b = P(Q) P(Q) = is the head developed by the pump = (550 hp)/(γq) hp = horsepower, γ = weight of water, Q = flow 21 Distribution Reservoirs Definition: Distribution reservoirs provide service storage to meet the widely fluctuating demands often imposed on the distribution system, to accommodate fire-fighting and emergency requirements, and to equalize operating pressure. Types of reservoirs: Surface reservoir Usually lined with concrete, gunite, asphalt, or membrane. They may be covered or uncovered, but usually covered to prevent contamination. Standpipes or elevated tanks Normally employed where the construction of a surface reservoir would not provide sufficient head. Stand pipes are tall cylindrical tanks whose storage volume includes an upper portion (useful storage) and a lower portion (supporting storage). 22 11

Surface Reservoir 23 Standpipes 24 12

Elevated tanks 25 Distribution Reservoirs Location Distribution reservoirs should be located strategically for maximum benefits. Normally the reservoir should be near the center of use. For large areas, a number of reservoirs may be located at key locations A central location decreases the friction losses by reducing the distance to the serviced area. Storage function To provide head required head. To provide excess demand such as: fire-fighting: should be sufficient to provide flow for 10-12 hours. emergency demands: to sustain the demand during failure of the supply system and times of maintenance. To provide equalization storage. 26 13

27 Pumping Introduction Pumping is an important part of the transportation and distribution system. Requirements vary from small units (few gallons per minute) to large units (several hundred cubic feet per second) Two kinds of pumping equipments are mainly used; centrifugal and displacement pumps. Types of pumps Low-lift pumps: used to lift water from a source to the treatment plant High-service pumps: used to discharge water under pressure to the distribution system Booster pumps: used to increase pressure in the distribution system. Recirculation pumps: used within a treatment plant. Well pumps: used to left water from wells. 28 14

Centrifugal pumps Used to lift and transport water Widely used in water and wastewater applications due to: Simplicity of installation and operation. Compactness. Low cost compared to others. Operate under variety of conditions How do they operate: On the principle of centrifugal force; force of pushing outwards. The impeller driven at high speed throws water into the casing Water is channeled through a nozzle to the discharge piping 29 30 15

31 Centrifugal pumps Pumping head The pump operates against a certain head called Total Dynamic Head (TDH). TDH is composed of the following: The difference in elevation between the pump centerline and the elevation to which the water is to be raised. The difference in elevation between the level of the suction pool and the pump centerline The friction losses Velocity head TDH = H L + H F + H V Where; H L = total static head H F = total friction head H V = velocity head (V 2 /2g) 32 16

33 Centrifugal pumps Power The theoretical horsepower required may be found by using the following equation: hp = QγH/550 Where; Q = discharge, cfs γ = specific weight of water, 62.4 lb/ft 3 H = total dynamic head, ft The actual hp required is obtained by dividing the theoretical hp by the efficiency of the pump. 34 17

Centrifugal pumps System head The system head is represented by a plot of TDH vs. discharge for the system being studied. The plot is used to help in selecting the pumping unit. The system head curve will vary with flow since H F and H V are both a function of discharge. Since the static head H L may vary as a result of fluctuating water levels, it is necessary to plot system head curves covering the range of variations in static head. 35 36 18

Centrifugal pumps Pump characteristics Each pump has its own characteristics relative to power requirements, efficiency, and head developed as a function of rate of flow. These relationships are usually given as a set of pump characteristic curves for a specified speed. Pump characteristic curves are used in conjunction with system-head curves to select suitable pumping equipment for a particular installation. As the flow of the centrifugal pump increases, the head will fall. At maximum efficiency, the discharge is known as normal or rated discharge. To change the flow, the practical and efficient approach is to provide two or more pumps in parallel so that the flow may be carried at close to the peak efficiency. The normal range of efficiency is between 50-85%. 37 38 19

39 Centrifugal pumps Selection of pumping units Normally the engineer is given the system-head characteristics curve and is required to find a pump or pumps to deliver the required flow. The system-head curve is plotted with the pump characteristics curve. The operating point is located at the intersection of the system-head curve and the pump characteristics curve. This point gives the head and flow at which the pump will be operating. A pump should be selected so that the operating point is also as close as possible to peak efficiency. Pumps connected in series; the total head equals the sum of the heads added by each pump (discharge stay constant). Pumps connected in parallel; the total discharge is the sum of the discharges of each pump at a given head (head stay constant). 40 20

21 41