5 - Pump-pipeline System Analyses Design

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    Pump Pipeline

    Analyses & Design

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    1 - Introduction

    This chapter : analysis & design of pipe systemincorporating rotodynamic pumps

    Pump selection CE concerned with: Design of river abstraction

    Borehole supplies from g/w & surface water

    Foulwater drainage from low-lying land

    3 categories of rotodynamic pumps (according to shapeof impellers): Centrifugal (radial flow)

    Mixed flow Propeller (axial flow

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    Specific Speed (Ns):

    (1)

    where Q: discharge

    H: total head

    N: rotational speed (rev/min) Expression interpreted as speed in rev/min

    Total head generated by a pump is also called the manometrichead (Hm) since it is the difference in pressure head recorded

    by pressure gauges connected to the delivery and inlet pipeson either side of the pump, provided that the pipes are of samediameter.

    4/3H

    QNNs

    Pump type Ns range

    Centrifugal

    Mixed flow

    Axial flow

    Up to 2600

    2600 to 5000

    5000 to 10 000

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    2 Head terms in pumping

    Static suction lift Vertical distance fr water level in source of tank to centerline ofpump

    If pump lower than source tank, static suction lift is -ve

    Static discharge head Vertical distance fr centerline of pump to w/l in discharge tank

    Total static head Static suction lift + static discharge head

    Total dynamic head (TDH) Static head + friction loss + minor losses a.k.a total head

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    Figure 1 Head terms in pumping

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    3 System head curve For any piping system, the friction loss, hf and the

    minor loss, hm can be expressed in terms of the flowthrough the system.

    (2)

    or,

    (3)

    Plot of eq (3) between Hp versus Q, is known as thesystem head curve.

    The curve represents behavior of the piping system,important in selection of a pump.

    g

    kV

    gD

    LVZHp

    22

    22

    4

    2

    5

    2

    81.0DKQ

    DLQ

    gZHp

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    Figure 2 Typical system head curve

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    4 Pump Characteristics Curve

    For a given pump at a given speed, there are definite relationshipsamong the pump discharge capacity, head, power, and efficiency.

    Relations are derived from actual tests on a given pump or similarunit and are usually depicted graphically by the pump characteristicsor performance curves, comprising the following:

    Pumping head versus discharge Power input (P) versus discharge

    Efficiency () versus discharge

    Energy imparted to fluid is gQHm, & pump efficiency may be

    derived as

    (4)P

    gQHm

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    General shape of curves varies with size, speed &

    design of particular pump Important feature : increase in head reduces capacity

    At given speed, pump is rated at the head and Q, whichgives max efficiency, referred as best efficiency point (A)

    Figure 3 Pump Characteristic Curve

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    5 Single Pump & Pipeline System Primary requirement : to determine a suitable pump and

    pipe combination for the required design discharge.

    Fig 4 : pump must generate total head equal to Hst plus

    the pipeline head losses at Q. Manometric head is defined as rise in total head across

    pump.

    (5)

    with:

    Thus, (6)

    g

    V

    g

    P

    g

    V

    g

    PH ssddm

    22

    22

    g

    VhZ

    g

    Ph

    g

    VZ

    g

    P dld

    d

    ls

    ss

    2;

    2

    2

    2

    2

    1

    lsldstm hhHH

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    Fig 4 Simple pumping main

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    Discharge is a function of both pump andpipeline.

    For a given system, head-discharge

    characteristic curves for the pump may besuperimposed on that for the pipeline (Fig 5).

    Point of intersection of the two characteristics

    curves locates one possible combination of headand discharge for the system under steady flowconditions.

    The intersection point is referred to as theoperating point.

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    Figure 5 Pump and pipeline characteristics curves

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    Example 1Calculate the steady discharge of water between the tanks

    in the system shown in Figure below and the power

    consumption. Pipe diameter (Ds = Dd) = 200 mm; Length =

    2000 m; k = 0.03 mm (uPVC). Losses in valves, bends plus

    the velocity head amount to 6.2 V2/2g. Static lift = 10.0 m.

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    Example 1

    Pump characteristics

    The efficiencies given are the overall efficiencies of the

    pump and motor combined.

    Discharge

    (l/s)

    0 10 20 30 40 50

    Total Head(m)

    25 23.2 20.8 16.5 12.4 7.3

    Efficiency

    (%)

    - 45 65 71 65 45

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    6 Multiple Pump SystemsA. Pumps in parallel

    Pumping stations frequently contain several pumps in parallelarrangement. (Fig 6a). Any number of the pumps can be

    operated simultaneously

    Objective: deliver a range of discharges. Common feature of

    sewage pumping stations where inflow rate varies. By automatic switching according to the level in the suction well,

    any number of the pumps can be brought into operation.

    Fig 6 (a) Pumps operating in parallel

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    In predicting H vs Q curve for parallel operation, it isassumed that head across each pump is the same.

    Thus, at any arbitrary head, individual pump dischargesare added (Fig 6b).

    (7)pnppnp nQQHH

    6 (b) Characteristic curves foridentical pumps operating in

    parallel

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    B. Pumps in Series Basis of multistage and borehole pumps; the discharge from the

    first pump (or stage) is delivered to the inlet of the second pump,

    and so on.

    Same discharge passes through each pump receiving a pressureboost in doing so.

    All the pump in series system must be operating simultaneously.

    (8)pnppnp QQnHH

    Figure 7

    Pumps operating

    in series

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    7 Variable speed pump operation By using variable speed motors, Q of single

    pump can be varied to suit operating

    requirements of the system. Using dimensionless analysis and dynamic

    similarity criteria, it can be shown that if the

    pump delivers a discharge Q1 at manometrichead H1 when running at speed N1; thecorresponding values when the pump is runningat speed N2 are given by:

    (9)2

    1

    212

    1

    212 )()(

    N

    NHH

    N

    NQQ

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    In constructing the characteristic curve for speed N2,several pairs of values of Q1, H1 from the curve for N1

    can be obtained and transformed into homologous pointsQ2, H2 on the N2 curve. (Fig 8).

    Figure 8 Effect of speed

    change on pump

    characteristics

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    Example 2

    A centrifugal pump delivers 30 liters ofwater per second against a head of 12

    metres and running at 1200 r.p.m. requires

    6 kW power. Determine the discharge,head of the pump and power required, if

    the pump runs at 1500 r.p.m.

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    8 Suction lift limitations Cavitation : phenomenon consists of local vaporization of

    a liquid

    Occurs when absolute pressure falls to the vapourpressure of the liquid at the operating temperature

    Can occur at the inlet to a pump and on the impellerblades, particularly if the pump is mounted above the

    level in the suction well. Cavitation causes physical damage, reduction in

    discharge and noise.

    To avoid: pressure head at inlet should not fall below a

    certain minimum which is influenced by the furtherreduction in pressure within the pump impeller. (Fig 9)

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    If Ps represents the pressure at inlet, then is

    the absolute head at the pump inlet above the vapour

    pressure (Pv) and is known as the net positive suctionhead (NPSH).

    Figure 9 Head conditions in suction pipe

    g

    pp vs

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    NPSH = (10)

    Where Pa : ambient atmospheric pressure; hs : suction lift;

    hls : total head loss in suction pipe; Vs : velocity head in suction pipe; :density of liquid.

    Value of NPSH can be obtained from the pump manufacturer;values must not be exceeded to avoid cavitation.

    Thoma introduced a cavitation number:

    (11)

    In recent years electro-submersible pumps in the smallto medium size range have been widely used. Theyeliminates the need for suction pipes; problems ofcavitation and cooling are avoided.

    g

    Vhh

    g

    pp

    g

    pp sfss

    vavs

    2

    2

    mH

    NPSH

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    9 Installation of Centrifugal Pumps

    Pump is installed between two valves for easy removal in case ofmaintenance.

    On suction side, a combined bellmouth entry and strainer are necessary,

    together with a non-return valve to ensure self-priming. On delivery side, a second non-return valve is necessary to prevent

    damage from possible surge pressures.

    In addition, an air valve and flow meter (venturi type) are desirable.

    Figure 10 Typical centrifugal

    pump installation