Hydraulics of Water Distribution Systems

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    The cornerstone of any healthy population is access to safe drinking water.

    The population growth in developing countries almost entirely wiped out thegains. In fact, nearly as many people lack those services.

    INTRODUCTION

    Developing Country Needs for Urban and Rural Water Supply,1990 and 2000

    Population not served

    (millions) in 1990

    Expected Population

    Increase 1990-2000(millions)

    Total Additional

    PopulationRequiring

    Service 2000

    (millions)

    Urban 243 570 813

    Rural 989 312 1301

    Total 1232 882 2114

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    Shaft of water holder at the Acropolis at Athens, Greece. (Photograph by L. W. Mays).

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    Water distribution pipe in Ephesus, Turkey. (Photographs by L. W. Mays).

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    Reference

    Z2

    Z1

    g

    P

    1

    g

    P

    2

    g

    V

    2

    22

    g

    V

    2

    21

    E

    Energy, Piezometric and pressure Head

    EEE 21

    Eg

    V

    g

    PZ

    g

    V

    g

    PZ

    22

    22

    2

    2

    1211

    Bernoulli equation states that for constant flow, an energy balance between twopipes cross section can be written as: or expressed in developed

    form, per unit weight (in MWC):

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    Elevation Head: this is an amount of flow potential energy in one cross section

    defined by the elevation. This correspond to Z in cross section

    Pressure Head :this is an amount of the flow potential energy in one cross

    section defined by the water pressure.

    Piezometric Head : this is the sum of elevation and pressure head in

    one cross section.

    Velocity Head : this is an amount of flow kinetic energy in one cross section

    defined by the water velocity.

    gP

    g

    PZ

    gV2

    2

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    Energy Losses

    (Head losses)

    Major Losses Minor losses

    The roughnessof the pipe The propertiesof the fluid

    The mean

    velocity, V The pipediameter, D The pipelength, L

    Head (Energy) Losses

    When a fluid is flowing through a pipe, the fluid experiences some resistancedue to which some of energy (head) of fluid is lost.

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    Compound Pipe flow

    The system is called compound pipe flow:When two or more pipes withdifferent diameters are connected together head to tail (in series) or connected

    to two common nodes (in parallel)

    A. Flow Through Pipes in Series

    pipes of different lengths and different diameters connected end to end

    (in series) to form a pipeline

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    Discharge: Thedischarge through each pipe is the same

    Head loss: The difference in liquid surface levels is equal to the sum of the

    total head loss in the pipes:

    332211 VAVAVAQ

    HL total = HL1 + HL2 + HL3

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    B. Flow Through Parallel Pipes:

    If a main pipe divides into two or more

    branches and again join together

    downstream to form a single pipe,then the branched pipes are said

    to be connected in parallel

    (compound pipes).

    Points A and B are called nodes.

    Q1, L1, D1, f1

    Q2

    , L2

    , D2

    , f2

    Q3, L3, D3, f3

    3

    1

    321

    i

    iQQQQQ

    g

    V

    D

    Lf

    g

    V

    D

    Lf

    g

    V

    D

    Lf

    222

    2

    3

    3

    3

    3

    2

    2

    2

    2

    2

    2

    1

    1

    1

    1

    321 fffL hhhh

    Discharge:

    Head loss: the head loss for each branch is the same

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    Example

    Four pipes connected in parallel as shown. The following details are given:

    Pipe L

    (m) D

    (mm) f

    1 200 200 0.020

    2 300 250 0.018

    3 150 300 0.015

    4 100 200 0.020

    If ZA

    = 150 m , ZB

    = 144m,determine the discharge in eachpipe ( assume PA=PB= Patm)

    Q1

    Q4

    Q3

    Q2Q QA B

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    Solution

    ZA- ZB = hf= hf1 = hf2= hf3=hf4 (neglect minor losses)

    150 -144 = 6 hfi =

    But Vi = =

    g

    V

    D

    Lf i

    i

    ii

    2

    2

    i

    i

    A

    Q2

    4iD

    Qi

    22

    28

    6igD

    QLf ii

    Substitute for Pipe 1, 2, 3 and 4

    Q = 0.0762 + 0.1146+ 0.28 + 0.1078 = 0.579 m3/s

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    MODERN WATER DISTRIBUTION SYSTEMS

    All water transport and distribution system and devices have to satisfy the followingcriteria:

    a) To be constructed and/or manufactured of materials that are not harmful for

    human being life.

    b) To be resistant to mechanical; and chemical attacks possible in distribution

    system

    c) To be constructed and manufactured of durable materials.

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    Urban water distribution is composed of three major components:

    distribution piping

    distribution storage

    pumping stations

    These components can be further divided into subcomponents, which can in

    turn be divided into sub-subcomponents.

    The pumping station component consists of structural, electrical, piping, and

    pumping unit subcomponents.

    The pumping unit can be further divided into sub-subcomponents:

    pump, driver, controls, power transmission, piping and valves.

    The exact definition of components, subcomponents, and sub-

    subcomponents is somewhat fluid and depends on the level of detail of the

    required analysis and, to a somewhat greater extent, the level of detail of

    available data.

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    Water Distribution System

    Pumping Station Distribution PipingDistribution Storage

    ElectricalStructural Pumping Piping Tanks Pipes Valve Pipes Valve

    pump driver Power transmission controls

    Hierarchical relationship of Components, Subcomponent, and sub-subcomponent.(Cullinane, 1989)

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    Pipes

    Pipe sections or links are the most abundant elements in the network.

    These sections are constant in diameter and may contain fittings and otherappurtenances, such as valves, storage facilities, and pumps.

    Pipes are the largest capital investment in a distribution system.

    Pipes used in water supply are made of various materials. They can be

    categorized in three large groups:

    Rigid (iron, prestressed concrete, asbestos cement)

    Semi-rigid (steel, ductile iron)

    Flexible (PVC, PE, HDPE, glass reinforced plastic)

    System Components

    Transmission: This is the basic part of water transport and distribution system

    that represents a large proportion of investment.

    It consists of various types of pipes, joints, fittings and connections, thatoperate together with miscellaneous control equipment.

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    Trunk main: To transport water from the source to the distribution area. (usually

    above 400mm to few meters).

    Secondary main: To link main distribution pipes with the service reservoir or

    /and with the trunk distribution mains.

    Distribution Main: carry water from the secondary main to the smaller

    consumers. These are in particular pipes laid in the roads and streets of urban

    areas with diameters in principal 100-200mm.

    Service pipe: To bring water from distribution main directly to a public dwelling.

    In case of domestic supplies service pipes are generally less than 25mmdiameter.

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    Water distribution network pipelines classification

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    Design Criteria

    Are the design limitations required to get the most efficient andeconomical water-distribution network.

    Velocity Pressure

    Pipe Sizes

    Head Losses Design PeriodAverage Water Consumption

    The design criteria for water distribution system can be divided in non-

    hydraulic and hydraulic design consideration.

    One of the non-hydraulic criteria can be the ability to isolate part of the

    system especially during emergency operation.

    Hydraulic design criteria are primarily related to the flow and pressure in the

    network. Moreover, criteria for minimum and maximum pipe capacities, flow

    velocities, pressure fluctuations and pressure gradients are relevant factors.

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    Velocity

    Not be lower than 0.6 m/s to prevent sedimentation

    Not be more than 2 m/s to prevent erosion and high head losses.

    Commonly used values are 1 - 1.5 m/sec.

    Diameter (mm) Velocity ( m/sec )

    100 0.9

    150 1.21

    250 1.52

    400 1.82

    Design Criteria ( Velocity )

    Source: Standards Handbook

    Diameter (mm) Head losses ( m/km )

    100 7.7

    150 4.8

    200 3.4

    250 2.6

    300 2.1

    350 1.7

    400 1.7

    Design Criteria ( Head Losses )

    Source: Water Supply ( 4th Edition )

    Instead of pressure gradient, the velocity can also be used as a design criterion

    (both parameters are correlated by friction loss calculations).

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    Pressure in municipal distribution systems ranges from 150-300

    kPa in residential districts with structures of four stories or lessand 400-500 kPa in commercial districts.

    Also, for fire hydrants the pressure should not be less than 150kPa (15 m of water).

    In general for any node in the network the pressure should not beless than 25 m of water.

    Moreover, the maximum pressure should be limited to 70 m ofwater

    Pressure

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    The pressure criterion can be formulated as a min. /max. In general 5 mwc above

    the highest tap is sufficient. For urban areas this means min. 20-25 mwc above

    street level. In case of high building, internal posting system has to be installed.

    As mentioned in the Standard Handbook, in multi-storied structures the following

    pressures are satisfactory.

    No. of Floors Pressure Required ( kg / cm2 = 0.98 bar)

    Up to and below 3 stories 23 - 6 2.1 - 4.2

    6 - 10 4.2 - 5.27

    Above 10 5.27 - 7

    Design Criteria ( Pressure )

    Source : Standards Handbook

    Maximum pressure limitations are required to reduce the additional

    cost of the pipe, strengthening necessary due to the high pressure.

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    Pipe sizes

    Lines which provide only domestic flow may be as small as 100 mm (4 in) butshould not exceed 400 m in length (if dead-ended) or 600 m if connected to

    the system at both ends.

    Lines as small as 50-75 mm (2-3 in) are sometimes used in smallcommunities with length not to exceed 100 m (if dead-ended) or 200 m ifconnected at both ends.

    The size of the small distribution mains is seldom less than 150 mm (6 in) withcross mains located at intervals not more than 180 m.

    In high-value districts the minimum size is 200 mm (8 in) with cross-mains atthe same maximum spacing. Major streets are provided with lines not lessthan 305 mm (12 in) in diameter.

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    General requirement for pipe network

    1. Mains should be divided into sections and valves should be provided so that

    any section may be taken out of operation for repair.

    2. Dead ends are to be avoided. If a dead-end is must, a hydrant should be

    provided for cleaning.

    3. Air valves at summits and drains at the lowest point between summits should

    be installed.

    4. Mains should follow the general contour of the ground.

    5. The minimum cover under roadway should be 90cm and under paths 75 cm.

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    Network Layout

    Estimate pipe sizes on the basis of water demand and local code requirements.

    The pipes are then drawn on a digital map (using AutoCAD, for example) startingfrom the water source.

    All the components (pipes, valves, fire hydrants) of the water network should beshown on the lines.

    Hydraulic Analysis

    After completing allpreliminary studies and layout drawing of the network, one of

    the methods of hydraulic analysis is used to

    Size the pipes and

    Assign the pressures and velocities required.

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    Hydraulic Analysis of Water Networks

    The solution to the problem is based on the same basic hydraulic principles that

    govern simple and compound pipes that were discussed previously.

    The following are the most common methods used to analyze the Grid-system

    networks:

    1. Hardy Cross method.

    2. Sections method.

    3. Circle method.

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    Hardy Cross Method

    This method is applicable to closed-loop pipe networks

    (a complex set of pipes in parallel).

    It depends on the idea of head balance method

    Was originally devised by professor Hardy Cross.

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    Assumptions / Steps of this method:

    1. Assume that the water is withdrawn from nodes only; not directly from pipes.

    2. The discharge, Q, entering the system will have (+) value, and the discharge, Q,leaving the system will have (-) value.

    3. Usually neglect minor losses since these will be small with respect to those inlong pipes, i.e.; or could be included as equivalent lengths in each pipe.

    4. Assume flows for each individual pipe in the network.

    5. At any junction (node), as done for pipes in parallel,

    outin QQ Q

    0or

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    6. Around any loop in the grid, the sum of head losses must equal to zero:

    Conventionally, clockwise flows in a loop are considered (+) and

    produce positive head losses; counterclockwise flows are then (-) andproduce negative head losses.

    This fact is called the head balance of each loop, and this can be validonly if the assumed Qfor each pipe, within the loop, is correct.

    hfloop 0

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    The probability of initially guessing all flow rates correctly is virtually null.

    Therefore, to balance the head around each loop, a flow rate correction ( )

    for each loop in the network should be computed, and hence some iteration

    scheme is needed.

    7. After finding the discharge correction, (one for each loop) , theassumed discharges Q0are adjusted and another iteration is

    carried out until all corrections (values of ) become zero ornegligible. At this point the condition of :

    is satisfied.

    hfloop

    0 0.

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    Note that if Hazen Williams (which is generally used in this

    method) is used to find the head losses, then

    h k Qf 185.

    h

    h

    Q

    f

    f185.

    If Darcy-Wiesbach is used to find the head losses, then

    h k Qf 2

    h

    h

    Q

    f

    f2

    85.1

    87.47.10

    HW

    fC

    Q

    D

    Lh

    gV

    DLfhf

    2)(

    2

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    Hardy Cross Method

    The figure below represents a simplified pipe network.

    Flows for the area have been disaggregated to the nodes, and amajor fire flow has been added at node G.

    The water enters the system at node A.

    Pipe diameters and lengths are shown on the figure.

    Find the flow rate of water in each pipe using the Hazen-

    Williams equation with CHW= 100.

    Carry out calculations until the corrections are less then 0.2m3/min.

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