Is.11625.1986 Penstock Design

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    Disclosure to Promote the Right To Information

    Whereas the Parliament of India has set out to provide a practical regime of right to

    information for citizens to secure access to information under the control of public authorities,in order to promote transparency and accountability in the working of every public authority,

    and whereas the attached publication of the Bureau of Indian Standards is of particular interest

    to the public, particularly disadvantaged communities and those engaged in the pursuit of

    education and knowledge, the attached public safety standard is made available to promote the

    timely dissemination of this information in an accurate manner to the public.

    !"#$% '(%)

    !"# $ %& #' (")* &" +#,-.Satyanarayan Gangaram Pitroda

    Invent a New India Using Knowledge

    /0)"1 &2 324 #' 5 *)6Jawaharlal Nehru

    Step Out From the Old to the New

    7"#1&"8+9&"), 7:1&"8+9&")Mazdoor Kisan Shakti Sangathan

    The Right to Information, The Right to Live

    !"# %& ;

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    ( Reaffirmed 2001 )

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    IS : 11625 1986

    I ndian Standard

    CRITERIA FOR

    HYDRAULIC DESIGN OF PENSTOCKS

    Water Conductor Systems Sectional Committee, BDC 58

    Chairman

    SHRIP.M. MANE

    39, Shivaji Co-operative Housing So Q, Pune

    Members

    Rsjmmxting

    CEIEB ENUINEER

    DIRECTOR Alternate)

    Mukerian Hyde1 Project Design, Chandigarh

    CEIEF ENGINEER (HP)

    Tamil Nadu Electricity Board, Coimhatore

    SUPERINTENDINQ ENGINEER

    Alternate)

    ENQINEER ( GENERAL )

    Public Works Department, Government of Tamil

    Nadu, Madras

    CHIEF ENGINEER ( IRRITATION )

    (

    Alternate )

    CEIEF ENQINEER ( CIVIL Drss~oxs )

    Karnataka Power Corporation Limited, Bangalore

    SHRI P. R. MALLIKARJUNA ( Alternate )

    CHIEF ENQINEER

    Bhakra Beas Management Board, Chandigarh

    SHRI SUNDERSHAN KUMAIL (

    Altwnate)

    f. Sr~;ra~~~~~~~ ( IRRITATION

    Public Works and Electricity Department,

    Government of Karnataka, Mysore

    SUPERINTENDING ENQINEER ( Alternate )

    SHRI C. ETTY DARWIN

    In personal capacity (

    P. 0. Muttada,

    TTVandTum

    DIRECTOR

    Central Soils and Materials Research Station,

    New Delhi

    DEPUTY DIRECTOR ( A&ernate )

    DIRECTOR ( HCD-I )

    Central Water Commission, New Delhi

    DEPUTY DIRECTOR ( HCD-I ) ( Alternate )

    DR A. K. DUBE

    Central Mining Research Station Unit, Roorkee

    DR J. L. JETHWA ( Alternate)

    DR B.PANT

    Water Resources Development Training Centre,

    Roorkee

    SHRI J. P. GUPTA

    Power House Designs, Irrigation Department,

    Roorkee

    SHRI A. P. GUPTA (

    Alternate )

    SHRI M.V.S.IYENaAR

    Hmdustan Construction Co Ltd, New Delhi

    SHRI M. G. KHAN Alternate)

    ( Continued on page 2 )

    0 Copyright 1986

    INDIAN STANDARDS INSTITUTION

    This publication is protected under the

    Indian Cofiyright Act (

    XIV of 1957 ) and

    reproduction in whole or in part by any means except with written permissionof the

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    IS:11625 1986

    ( Continued.from page 1 )

    MtWltWS Representing

    1

    OINT DI,~E~TOR

    R~J~A~CK Research Designs and Standards Organization,

    I (GE-II)

    SHRI

    P. N.

    KIIAR

    Lucknow

    National Hydroelectro Power Corporation Ltd,

    New Delhi

    SHRI A. K. MEHTA National Projects Construction

    Corporation

    Limited, New Delhi

    SHI~I S. C. R,\LI ( Alternate )

    Mnxmx ( CIVIL ) Kerala State Electricity Board, Trivandrum

    SHIU G. PANT Geological Survey of India, New Delhi

    SHRI N. K. MANUW~L ( Alternate )

    SHXI A. R. RAI~HUR In personal capacity ( 147, Garodianagar, Bombay )

    SHRI Y. KA~A KIUSHNA RAO Andhra Pradesh State

    Electricity

    Board,

    Hyderabad

    SUPERIRTFNUING ENGINEER

    (

    DESIGN ANU PLANNING ) ( Alternate )

    SHRI G.

    V. SATHI~YE Central Designs Organization, Nasik

    DR H. R. SHAI HA* CentralElectricity Authority, New Delhi

    SHRI s. c. SEN Assam State Electricity Board, Guwahati

    SHRI N. I

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    IS : 11625 - 1986

    I ndian St andard

    CRITERIA FOR

    HYDRAULIC DESIGN OF PENSTOCKS

    0. FOREWORD

    0.1 This Indian Standard was adopted by the Indian Standards Institu-

    tion on 28 February 1986, after the draft finalized by the Water

    Conductor System Sectional Committee had been approved by the Civil

    Engineering Division Council.

    0.2 The water is taken from the forebary to the power station through

    the penstocks. These may be pressure conduits or shafts. The penstocks

    shall carry water to the turbines with the least possible loss of head con-

    sistent with the overall economy of the project. For successful operation,

    the size of the pipe for a given discharge may vary between wide limits,

    but there is usually one size that will make for the greatest economy and

    design. Hence the diameter of the penstocks isdetermined from the con-

    sideration of economy and is checked to see that the acceptable ve ocities

    are not exceeded.

    1. SCOPE

    1.1 This standard covers the criteria for hydraulic design of penstocks.

    2. GENERAL

    2.1

    The hydraulic design of penstocks covers hydraulic design of intake

    for penstocks, hydraulic losses in penstock, pressure rise or pressure drop

    due to turbine or pump operations and ascertaining most economic

    diameter of penstock on the basis of available data.

    3. HYDRAULIC DESIGN OF INTAKE FOR PENSTOCK

    3.1 The hydraulic design of the main components of intake shall be in

    accordance with IS

    :

    9761-1981.

    *Criteria for hydraulic design of hydropower intakes.

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    IS : 11625 - 1986

    4. HYDRAULIC LOSSES IN PENSTOCK

    4.1 The hydraulic losses in the penstock comprise the following:

    a) Head loss at trash rack,

    b) Head loss at intake entrance,

    c) Friction losses, and

    d) Other losses as at bends, bifurcations, transitions, valves, etc.

    These head losses are expressed in terms of coefficient to be applied

    to the velocity head at the section in question.

    4.2

    Head Loss at Trash Rack

    4.2;1 The head loss through trash rack (ht) may be expressed by the

    formula given below:

    ht = k,+

    where

    ht trash rack head loss,

    kt = loss

    coefficient,

    u = actual velocity through rack opening, and

    P

    3

    acceleration due to gravity.

    The loss corfficient kt shall be calculated in accordance with IS : 4880

    Part 3 )-1976*.

    4.3 Head Loss at Intake Entrance

    4.3.1 The magnitude of head loss at entrance depends upon the shape

    of intake mouth. For bell mouth shape shown in Fig. 1, losses-are given by

    the following formula:

    h, = k,

    where

    h, =

    head loss at entrance,

    k, =

    loss coefficient at entrance,

    u =f velocity at entrance, and

    g i= acceleration due to gravity.

    4.3.2 The value of loss coefficient

    k,

    shall be in accordance with

    IS

    :

    4880 ( Part 3 )-1976*.

    *Code of practice for design of tlmncls conveying water : Part 3 Hydraulic design

    ( jirsl rmkkm ).

    4

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    IS : 11625 1986

    Friction Losses

    4.4.1

    Head loss due to friction in pipes may be estimated from the

    given in 4.4.1.1 to 4.4.1.2.

    444.1.1

    Darcy-Waisbach formula:

    hl = fLv_

    2C P

    where

    hf

    friction head loss in pipe in m;

    f =

    loss coeficient depending upon type, conditions of the

    pipe and Reynolds number which may be obtained from

    Fig. 2;

    L = length of pipe in m;

    t -= velocity through pipe in m/set; and

    I) = diameter of pipe.

    4.4.1.2 Mannings formula may be used in case of fully rough tur-

    bulent flow.

    Mannings formula

    ~ = Ral3 S/z

    n

    where

    R = hydraulic radius

    area

    ( .

    rttedseter

    -) in m;

    S = slope of energy gradient; and

    n

    ;

    roughness coefficient, shall vary from 0.012 to 0.014 for

    concrete pipes and for steel pipes the valve of n shall vary

    from 0.008 to 0*012.

    4.5 Other Losses

    4.5.1 In a penstock other losses include losses due to bends, expansion

    or contraction, obstruction caused by valve passage and losses in penstock

    branches and wyes.

    4.5.2 Rend Loss .-

    The bend loss excluding friction loss for a circular

    conduit depends U~OLI the shape of bend, deflection angle and ratio of

    radius of bend to diameter of pipe. The bend loss may be calculated from

    the following formula:

    h,, =

    kb

    2.9

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    h3:11625 1986

    where

    hb = head loss due to bend,

    kb = bend loss coefficient which may be obtained from Fig. ~3 for

    various R/D ratios and deflection angles, and

    v = velocity in pipe.

    4.5.3 Loss Due to Expansion and Contraction

    4.5.3.1

    Head loss due to gradual expansion

    h,,

    may be estimated

    from the formula:

    where

    VI = velocity at upstream end in m/set;

    V, = ve1ocit.y at downstream end in m/set, and

    k,, - loss coefficient depending upon the cone angle and shall

    be in accordance with IS : 2951 (Part 2) - 1965*.

    Fro. IA

    BELL MOUTH DETAILS - Contd

    Recommendations for estimation of flow of liquids

    in

    closed conduits

    :

    Part 2

    Head loss in valves and fittings.

    6

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    I

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    0.20

    i---

    v

    V- VELOCITY

    D= DIAMETER

    = KINEMATIC VISCOSITY

    0 1

    LOSS OF COEFFICIENTS

    PIPE BENDS OF sMOOTl

    R,=225,000= %I

    O. l L

    I PIJ I I Yk

    I I

    t

    I /./ I I /-I I/ I

    Oat2

    I /,I I L -

    I_/ I

    I

    kb

    IW,I

    I A I

    O-08

    I

    I 1, I

    I I

    I

    I

    I I

    I I I I I

    I I

    1

    0 5 10 15 20 2S 30 35 LO0 45 50 55 60 65 70 75 80 85 90

    B

    I

    DEFLECTION ANGLE,A+

    FIG.

    3

    Loss COEFFICIENTS FOZ PIPE BENIX

    OF SMOOTHNTERIOR

    5

    8

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    IS:11625 - f986

    4.5.3.2 Head loss in reducer piece h, may he estimated by the

    following formula:

    where

    k =

    v =

    v =

    loss coefficient for contraction,

    velocity in normal section, and

    velocity at the contraction section.

    The value of k shall be in accordance with IS : 4880 ( Part 3 )-

    1976*.

    4.5.?;3 When a diffuser follows immediately after a bend without a

    straight length in-between, the loss in the diffuser will be more than that

    given in 4.5.3.2. It is recommended to provide a straight length equal to

    the diameter of the pipe between the bend and the diffuser.

    4.5.4 Losses in Valve Passages

    4.5.4.1 Valves are usually installed at two places in the penstocks of

    a hydro power station -

    one at the upstream end and the other at the

    downstream end immediately ~ahend of the turbine. The former called as

    control or penstock valve is usually a butterfly valve and the latter known

    as inlet valve is either butterfly valve or a spherical valve. These valves

    remain either in fully closed or open position. Under fully opened position

    the losses through spherical valves are negligible. The value of loss

    coefficient for butterfly valve may be obtained from Fig. 4.

    4.5.5

    Losses i n Penst ock Branches and Wl es

    4.5.5.1

    A penstock bifurcation into two is termed as a wye and when

    more than two, it is termed as manifold.

    4.5.5.2 The hydraulic losses at wyes are governed by angle of bifur-

    cation, ratio of cross-sectional area, +ype and shape of bifurcation.

    4.5.5.3 Various types of wyes and branches generally adopted are:

    a) Wyeslbranches with sharp transition,

    b) Wyeslbranches with conical transition, and

    c) Wyeslbranches with rounded corners.

    *Code of practice for design of tunnels conveying water: Part 3 Hydraulic design

    first revision ).

    10

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    IS : 11625 - 1986

    1.0

    0.9

    0- B

    0.7

    0.6

    0.5

    0.4

    0.3

    0.2

    0.1

    0

    Q

    AREA

    A0

    Ag= REFERENCE AREA

    FOR V2/2,,

    L REDUCED

    AREA, AR

    0 40

    80

    120

    160

    200

    VALVE DIAMETER (cm1

    FIG.

    4

    GENERAL TREND OF VALVE Loss COEFFICIENT

    OF PASSAGE FOR BUTTERFLY VALVES

    4.5.5.4 Figure 5 gives the head loss-coefficient

    sharp, rounded and conical transitions.

    5.

    PRESSURE RISE AND PRESSURE DROP

    AND RESTRICTION

    for branches with

    5.1 The criteria to be adopted for the calculation of pressure rise and

    pressure drop, and method of computations are covered in the Indian

    Standard Code of practice for design of water hammer in water conductor

    systems (

    under Preparation

    ) .

    6. ECOINOMIC DIAMETER OF PENSTOCK

    6.1 The economic diameter of penstock is the diameter for which the

    annual cost, which includes the cost of power lost due to friction and

    charges for amortization of construction cost, maintenance, operation, etc,

    is the minimum.

    6.2 The economic diameter is calculated by evaluating annual power loss

    and annual cost for maintcn;mce and equating first derivative with respect

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    CYLINDRICAL

    SHARP EDGE

    SHARP FnGF

    J

    r

    DEFLN \\\

    ii . k?x\kOUh

    CJ/O FOR DblD =0~58(MUNICH1

    Vb/v

    - 01

    .

    -.-.--.~~~

    MUNICH MODEL TEST

    HI

    ---_----Z--

    0 000 F

    &

    r; jui

    2

    0.1 1.0 vb/ Y 10.0

    90 DEFLECTION

    SO DEFLECTION

    45 DEFLECTION

    FIG.

    5

    Loss AT PIPE

    JUNCTIONS WITH DIVIDING FLOW

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    IS:11625 - 1986

    D to zero and is given by the following equation based on Mannifigs

    The derivation of the formula is given at Appendix A.

    DWs =

    2.36 x 106 x Qs x ne x e t , x

    C,

    c

    l-39 C, + O-6 C, + 21 Hc;a(;, + )

    . 1

    p

    where

    Cc = unit cost of concrete lining in Rupees/ma;

    C, = unit cost of excavation in RupeesIms;

    C, = cost of 1 kWh of energy in Rupees;

    C, = cost of steel in Rupees/kg;

    D =

    diameter of the penstock;

    e = overall efficiency of plant;

    et = joint efficiency of penstock;

    H

    - head on penstock including water hammer in m;

    i = percentage by which steel in penstock is overweight due to

    ~provision of stiffeners, corrosion allowance, etc;

    ;

    = Rugosity coefficient in Mannings formula;

    = ratio of annual fixed operation and maintenance charges

    to construction cost of penstock;

    pI = annual load factor; and

    Q = discharge through penstock in ms/s.

    APPENDIX A

    Clause 6.2 )

    tiI)ERIVATION OF THE FORMULA FOR CALCULATING

    THE ECONOMIC DIAMETER OF PENSTOCKS

    -l. COST OF POWER LOST

    1.1 Head Loss in Penstock/Metre Length - Head loss due to fric-

    ion is given by Manning? formula:

    va ne

    his.------=

    10.29 Q n2

    R4/3

    jp/3

    Annual cost of power lost E,) = 9.804 x Q x hf x e p, x 8 7606,

    E

    f

    = O-88 x 106 Q3 n e p f cp

    DI 6 / 3

    13

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    IS t 11625 1986

    A-2. ANNUAL CHARGES ON CAPITAL COST

    A-2.1 Cost of Excavation -

    The cost due to excavation for laying the

    penstock is calculated considering the tunnel diameter to be

    0.33

    D in

    excess of penstock diameter total cost/unit length of penstock is given by:

    ___ D +

    0.33

    D ) x C,

    i

    =

    1.39

    D= C,

    NOTE -

    033 D to be varied between 0.2 D to 0.33 D depending on the c&me-

    ter of penstock such that the excavated diameter is not greater than the

    penstock

    diameter by about 90 cm.

    A-2.2 Cost of Concrete Lining -

    Cost of concrete lining in penstock

    has been calculated taking thickness of lining as 0.165 D. Thus cost of con-

    crete lining is given by:

    7c (

    D +

    0,165

    D ) x

    0.165

    D x C,

    =

    0.6 02 C,

    NOTE -

    0165

    D

    to be varied between 0.1

    D

    to 0165

    D

    depending

    on the dia-

    meter of penstock such that concrete lining thickness is not greater than 30 cm.

    A-2.3 Cost of Steel in Penstock

    Pd 0.1

    HD

    Steel lining thickness t = 2ae = -__

    a 1

    2 ba ej

    x

    Dt

    (1 + 2) 7 850 x Cs

    Penstock cost = _--~-__---

    2 ua x 9.81 x ej

    = 120.93 HD2 x C, (1 + ;)

    @a X el

    A-2.4 Annual Charges on Capital Cost - The annual cost of penstock

    is expressed by:

    [D2 (1.39 C, + 0.6 C, + 120.93 HC, 1 + i)] x /J

    E, _ _______ ______

    ___-~---

    ba ej

    A-3. ECONOMIC DIAMETER

    A-3.1 Total Annual Cost E) = E, + E,

    Economical diameter is obtained by:

    8 (E, 4 E,)

    SD

    _ o

    2*36x 106x Q3x112x efif XC,

    02213 = _~_

    ._____~

    1.39 C, + 0.6 C, + 12 yx$+ ) ] x p

    a

    14

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    fS:11625-1986

    ( Continued from page 2 )

    Members Representing

    SHR~ N. C. JAIN

    Irrigation Department, Government of Uttar

    Pradesh, Lucknow

    R ZAEAR MEHDI Bharat Heavy Electricals Ltd, Bhopal

    SHRI J. L. KHOSA ( Alternate )

    SHRI C. GANESA PILLAI

    Kerala State Electricity Board, Trivandrum

    SHRI A.-R. R~QRAVAN

    Tamilnadu Electricity Board, Madras

    SHRI T.

    RAMASWAXY

    Indian Hume Pipe Co Ltd, Bombay

    SHRI

    B. RAMASWAMY (

    Alternate )

    DR H. R. SHARMA

    Central Electricity Authority, New Delhi

    SHRI B. THOMAS

    Central Water &kPower Research Station, Pune

    HRI R. VIJAYAN

    In personal capacity [ 351136 (2) Kamaldoth Lane,

    Cochin ]

    SHRI N. G. KURUP ( Alternate )

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    INTERNATIONAL SYSTEM OF UNITS SI UNITS)

    Ease Units

    Quantity

    -Length

    Mass

    Time

    Electric current

    Thermodynamic

    temperature

    Luminous intensity

    Amount of substance

    Supplementary Units

    Qoanfity

    Plane angle

    Solid angle

    Derived Units

    Quant i ty

    Force

    Energy

    Power

    Flux

    Flux density

    Frequency

    Electric conductance

    Electromotive force

    Pressure stress

    Unit

    metre

    kilogram

    second

    ampere

    kelvin

    candela

    mole

    Unit

    radian

    steradian

    Unif

    newton

    joule

    watt

    weber

    tesla

    hertz

    siemens

    volt

    Pascal

    Sym bo l

    m

    kg

    :

    K

    cd

    mol

    Sym bo l

    rad

    sr

    Sym bo l

    N

    Wb

    T

    t-fz

    S

    V

    Pa

    Oepni t lon

    1 N = 1 kg.m/ss

    1 J = 1 N.m

    I W = %J/s

    1 Wb = 1 V.s

    1 T = 1 Wb/ms

    1 Hz = 1 c/s (s-1)

    1 S = 1 A V

    I V = 1 W/A

    1 Pa - 1 N/ms