Cap 17 Hidratos

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    4

    74

    G

    as

    Hy

    drate Formatlon

    Gas hydr

    a

    tes behave

    a

    s s

    olution

    s o

    f

    gases in crystalline solids rather

    than

    a

    s ch

    e

    mical

    c

    ompoun

    ds

    Th

    e main fram

    ew

    ork o

    f

    the hydrate

    c

    ryst

    a

    l

    is formed with w

    ate

    r

    molec

    ul

    e

    s . The hydr

    ocarbo

    n

    mo

    le

    cules o

    cc

    upy void

    spa

    c

    e

    s

    w i

    thin the l

    a

    tti

    c

    e o

    f

    water mo

    lecule

    s .

    Hydrate

    formati

    on is physical

    ra

    the

    r

    than

    c

    h

    em

    ical in nature. Appar

    -

    e

    ntly, no strong chemical bonds

    ar

    e formed between the hy

    droc

    arbon

    a

    nd

    wa

    ter

    molecule

    s.

    A

    c

    tually

    ,

    th

    e

    h

    y

    d

    roc

    arbon

    mole

    c

    ule

    s ar

    e

    fr

    ee to ro

    ta

    t

    e

    w ith

    in

    th

    e void

    spaces

    .

    Toe

    wa

    ter

    fr

    ame

    w

    ork

    s

    eem

    s

    ice

    -

    like be

    ca

    use o

    f

    comparable

    h

    eats

    of

    forrnation.

    H

    oweve

    r,

    the crysta

    l l

    attice is somew

    h

    at different t

    h

    an

    ic

    e

    s

    ince an ice l

    a

    ttice

    pro

    vide

    s

    no space for

    e

    ven the

    s

    m

    al

    lest

    hydrocar

    bon

    mol

    ec

    ule

    Two types

    of

    hydrate crystal lattice

    s

    are know

    n.

    Each contains void

    space

    s of

    two differe

    nt

    size

    s .

    One lattice has voids s

    i

    zed to accept small

    molecules su

    ch

    as methane and l

    ar

    ge

    r

    m

    o

    l

    e

    cul

    es such as propane

    a

    t a

    r

    a

    tio

    o

    f

    ab

    o

    ut

    tw

    o

    s

    mall

    m

    olecules

    to

    on

    e

    l

    ar

    ge

    m

    olecule

    The

    oth

    e

    r

    lattice accepts methane mol

    e

    cules and medium-sized m olec

    ule

    s--such as

    ethan

    e

    -at

    a ratio o

    f

    about three mediums to one small.

    Although gas hy

    drat

    es

    a

    ppear to

    be

    solid solutions rather th

    a

    n

    chemical compounds

    ,

    a specific number o

    f

    water mole

    c

    ules is associated

    H

    ydrocarbon gas and liquid w

    ater

    c

    omb

    i

    n

    e to fo

    nn

    solid

    s

    resembling

    wet snow at

    temperatures

    so

    me

    what

    abo

    ve the temperature

    at

    w

    h

    ich

    wate

    r

    solid

    ifi

    es. The

    s

    e

    soli

    ds are called They are one of a

    form

    of

    cornplexes

    know

    n as Th

    i

    s phenomenon particul

    ar

    ly

    interests those in the

    petrol

    eum industry because

    th

    ese s

    olid

    s

    ca

    n form at

    te

    m

    peratures and pressures n

    ormal

    ly

    enco

    untered in producing

    an

    d

    tran

    sporting n

    a

    tura

    l

    gases.

    Gas Hydrates

    17

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    Conditions For Gas Hydrate Formation

    The most important consid

    e

    ration in hydrate formation is that liquid

    water must be present for hydrate to form Even with liquid water present

    a

    metastable equilibrium

    c

    an

    e

    xist b

    e

    tween water and gas at conditions of

    with each gas

    mol

    ecule. This dueto the framework o

    f

    the crystal. The

    ratio depends primarily on the size

    of

    the gas molecule.

    Figure 17-1 shows a number of gase

    s

    which form hydrate

    s

    , along

    with the maximum length of each molecule in angstrom units and the

    approximate ratio

    of

    water molecules to ga

    s m

    o

    le

    cules in the resulting

    crystals. Not only the size o

    f

    the ga

    s m

    olecule but also its isomeric

    configuration control whether or not hydrate will form. For example, iso-

    butane readily fo

    r

    ros hydrate, but the

    longe

    r n-butane

    m

    olecule forros

    hydra

    te only at temperature

    s s

    lightly above the

    fre

    ezing point

    of

    water.

    Yet, in the presence

    of

    other g

    as

    es with smaller molecules

    ,

    the n-butane

    molecules readily enter the h

    ydra

    te. This

    indic

    ates that n-butane mole-

    cules occupy the larger

    v

    oids the crystal lattice once h

    y

    drate formation

    begins.

    Fig. 17-1.

    Handbook of Natural

    Eng

    i

    neering

    u

    '4

    '-

    :~~#'$'.#

    .#

    i ' -~ 1

    -7//#/

    $#////#n'#/#/#r.

    Dl1

    C

    M

    t1

    1

    U\8 i

    (t ,He.

    bo

    C.

    l flll

    . ,~

    . .

    . . . . . .

    475

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    pressure and temperature for which

    hy

    drate forrn

    a

    tion could occur. But,

    once seed crystals are forme

    d

    ,

    hy

    dration

    occur

    s rea

    dil

    y.

    Seed crystals be gin to forrn at

    temperatur

    es

    3 t

    o

    O

    F

    lower than the

    hydrate-forming

    temperat

    ures dis

    cuss

    ed late

    r

    in

    t

    his chapter

    .

    Or, at a

    given temperature

    ,

    seed cry

    s

    tals start forming at 300 or more psi above

    hydrate-forming

    pressure.

    However

    ,

    dust or rust particles may act like

    seed crystals in initiating

    h

    ydrate formation

    .

    A portian

    of

    the ph

    as

    e diagram for a mixture of water and a light

    hydrocarbon is given in

    Fi

    g

    ur

    e 1

    7

    -2. The line Q C separates the region

    in which liquid water and

    h

    y

    drocarbon

    g

    as

    ex

    is

    t from the region in which

    liquid water and hydrocarbon liquid exist. None

    of

    the phases is pure; ali

    contain slight amounts

    of

    the other substance ac

    cordin

    g to their mutual

    solubility.

    Line Q C is parallel to and slightly

    abov

    e the vapor-pressure line for

    the pure hydrocarbon. The dashed Ii ne to the left

    of

    point Q is simply an

    extension

    of

    the vapor-pressure Iine

    of

    the

    hy

    drocarbon. Point C is the

    three-phase critica point at which the

    properti

    es of the hydrocarbon gas

    and liquid merge to form a

    s

    in

    g

    le

    hydro

    carbon phase in equilibrium with

    liquid water.

    The line Q1 Q 2 separates the area in

    whi

    ch liquid water and hydrocar-

    bon gas exist from the

    are

    a in w

    hi

    ch liquid water and

    hy

    drate e

    x

    ist. This

    line represents the conditions at w

    hi

    ch

    gas

    and liquid water combine to

    form hydrate.

    Fig.

    H y

    iNnpefl;iu

    e

    PETROLEUM FLUIDS

    76

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    Fig. 17-3.

    Handbook

    of Natural Eng

    ineerng

    20

    100

    60

    200

    i

    800

    2000

    4000

    1 0 ,000

    8000

    6000

    80 90

    0 40 .50 60 70

    _/

    , , , .

    /

    - ~

    1

    1

    :..,

    -

    ..-

    : . . . - -

    1

    , 1

    /

    ..,,/ , , .

    --

    1

    /

    - -

    ' ' -

    r

    - -

    /

    -

    40

    Point

    Q

    2

    i

    s a quadruple

    poin

    t. At Q 2, four phases are in

    equil i

    brium:

    Iiquid water, hydrocarbon liquid,

    hy

    dr

    o

    carbon gas, and solid h

    yd

    rate.

    To

    e

    almo

    st

    v

    ertical line

    extendin

    g

    fr

    o

    m point

    separate

    s

    th

    e

    ar

    e

    a

    o

    f

    liquid water and hydrocarbon Iiquid from the area of liquid water

    a

    nd

    hy

    d

    ra

    te

    .

    Q which occurs at approximately 32F, is also a quadruple

    p

    oi

    n

    t

    re

    presenting the point at whi

    c

    h ice

    ,

    hydrate, liquid water, and hyd

    roc

    ar-

    b

    o

    n gas

    ex

    ist in equilibrium. The vertical line extending from point

    separates the area far hydrate and liquid

    wat

    er from the area far hy

    dra

    te

    and ice.

    T

    he

    lin

    e

    of

    major intere

    st

    on

    this

    phase diagram is the Ii

    n

    e Q

    Q

    w

    hi

    c

    h

    r

    e

    p

    r

    esents the equilibrium

    betw

    ee

    n

    h

    y

    drocarbon

    ga

    s

    ,

    liquid

    water

    ,

    and hydrate.

    4

    77

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    Bureau of

    Min

    es

    M

    on

    ograph

    8

    lO

    1

    00

    '

    1

    000

    IOO

    1

    500

    'lY

    /

    -

    V

    , , ,

    V :

    /

    # .

    ~

    1 1 ~

    'o'

    -7

    ,

    ,o

    . .

    Figure

    17

    -3 shows the ~ lines for the five h

    y

    d

    r

    ate-forming

    hydrocarbon cons

    t

    ituents of natural

    gas

    . Portio

    n

    s of the

    vapor-pressur

    e

    lines of the hydrocarbons and parts

    of

    the vertical li

    n

    es from Q and Q

    also are shown

    .

    Pressures and

    tempe

    ra

    tures along

    the~

    line for each

    hydrocarbon indicate c

    on

    ditions for which

    h

    ydra

    t

    e

    formatio

    n occurs

    fo

    r

    mixtures of that hydrocarbon with li

    qu

    id water. Methane forms

    hy

    drate

    at much higher

    temperature

    s than the larger hydrocarbons. However

    ,

    the

    pressure required for hydrate formation becomes significantly lower as

    m o

    l

    ecular size

    in

    creases

    .

    Figure

    17

    -

    4

    gives a

    compariso

    n of the hy

    drate-f

    ormation

    lines

    of

    methane and propane w i

    t

    h the hydrate-formation lines for mixtures of

    th

    es

    e two

    h

    y

    drocarb

    o

    ns.

    3

    Note

    th

    at

    v

    ery sm al

    l

    quantities

    o

    f the larger

    hydrocarbon in the

    mixtur

    e

    s

    c

    au

    s

    e large

    re

    ducti

    o

    ns

    i

    n the

    pre

    ssure

    s

    required to initiate hydrate forma

    ti

    on .

    A mixture of

    4 0

    %

    m eth

    ane and

    60

    % propane forms

    hy

    drate at

    pressures nearly as low as pure propane, but hydr

    at

    e

    form

    s

    a

    t much

    higher temp

    e

    ratures

    t

    han for pure propane. Thus, mixtures of methane

    and l

    ar

    ger hydrocarbons retain the high

    h

    ydr

    ate-forming tempe

    ratur

    es

    o

    f

    meth

    a

    ne and approach the

    low

    er hy

    drate-f

    orming

    pres

    sures of th

    e

    larger

    molecules .

    This fact

    i

    s confirmed

    b

    y the data

    giv

    en in Figure

    17-5

    1

    This

    fi

    g

    ure

    shows

    th

    e

    h

    ydrate-forming

    c

    ond

    iti

    ons fo r s

    ev

    eral n

    a

    tural g

    a

    ses

    al

    ong

    PETROLEUM FLUIDS

    78

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    with the hydrate-

    for

    m

    ati

    on line fo

    r

    met

    hane .

    Toe pr

    e

    ssures at which

    hydrate formation occurs are

    s

    ignificantly low

    e

    r for the natural gases

    than for me

    than

    e.

    Th

    e natural gases w ith high

    e

    r specific gravitie

    s

    (that

    is , gases with more o

    f

    the

    heav

    ier hydro

    c

    arbons) form hydra

    tes

    at much

    lower pres

    s

    ure

    s

    than the lighter gases.

    The data are incomplete at the higher

    te

    mperatures, but appar

    e

    ntly all

    the gases form hy

    dra

    tes at

    temp

    eratures som e

    w

    hat

    a

    bov

    e

    70F.

    Figure

    17-6

    was

    d

    e

    v

    e

    l

    o

    p

    ed

    fro

    m

    th

    e

    da

    ta of

    Fi

    g

    ure

    1

    7

    -5

    .

    4

    Fig

    ure

    1

    7

    -6 is

    a correl

    a

    tion of hy

    d

    rate

    -formin

    g

    co

    ndition

    s

    fo

    r

    natural gases

    with various

    s

    pecific

    gra

    v

    ities, Th

    is

    fig

    ure can be used to estmate the

    condition

    s

    under which hy

    d

    r

    a

    tes

    w ill

    fo

    rm

    Toe

    re sul

    ting hydrate

    formation

    conditions m

    u

    s

    t u

    s

    ed with

    cau ti

    on be

    caus

    e

    th

    ere

    is

    a great

    discrepancy bet

    w

    een the

    li

    m

    it

    ed publi

    sh

    ed d

    a

    ta

    a

    nd the

    c

    orr

    e

    lation

    shown in Figure

    1

    7

    -6. To

    e

    differe

    nces

    hy

    drate-

    forming

    pr

    ess

    ures

    Fig.

    17-5.

    A

    Hendbook

    of Natural Gas Engneering

    40

    90

    00 60 70

    Temperoture, deg F

    30

    2

    00

    40

    0

    300

    600

    ~

    1

    000

    ~ 800

    a.

    0

    20

    0

    0

    ; ;

    c..

    4000

    3000

    ~ I J V

    V

    ~

    I

    ~

    I

    / ~

    /

    / /J

    /

    V

    ~ ~

    f

    V

    ~

    ~

    ~

    ~

    10,000

    8000

    6

    000

  • 7/25/2019 Cap 17 Hidratos

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    EXAMPLE

    17

    -1:

    7

    between

    th

    e

    avail

    able data

    an

    d the co

    rre

    lation in

    Fi

    g

    ur

    e 1 7

    -

    6

    ran

    ge from

    about

    1

    0% at the higher specific grav

    iti

    es to as

    mu

    ch as 35% at

    th

    e low er

    specific g

    rav

    itie

    s.

    G i

    ve

    n a

    va

    lu

    e of

    pr

    ess

    ure,

    th

    e

    erro

    r

    i

    n

    th

    e

    estmate of

    hydrate-formi

    ng

    temp

    erature

    co

    uld be 5F or

    m

    o

    re .

    Figure

    17 -6

    is for sweet gases.

    T

    he pr

    ese

    nce

    of

    hydrogen

    s

    ulfide and

    carbon dioxide

    shift

    s

    th

    e

    lin

    es to

    th

    e

    righ

    t. Thi

    s results i

    n an

    in

    crease in

    the hydrate temper

    a

    ture for a given pr

    e

    ssure or a d

    ec

    r

    ea

    se in hydrate

    pressure for a given t

    e

    mpera

    ture

    .

    Trans.,

    160,

    80

    0 60 70

    f

    4000

    1/)

    (L

    00

    J

    '/ji

    0

    0

    //J

    c

    7

    , , , , , ,

    ,,,

    --

    00

    ,r)"

    / /

    ~7 /

    ///

    0

    0

    C7m'

    - -

    h

    oc

    5 :

    q ; / /

    W

    o

    ~/

    ~/

    6

    tL

    - =

    -

    --- --

    1----------

    ~--

    1-------~

    --

    4

    8

    o

    1 . 1 . . .

    iJJ

    a:

    ~ 3

    a: 2

    iJJ

    o:

    P

    ET

    ROL

    E

    U

    M FLUIDS

    8

  • 7/25/2019 Cap 17 Hidratos

    8/15

    H andbook of Natural Gas Enginee

    r

    ing

    .ot

    o

    ~14

    18

    1//

    J

    lj

    2

    J I

    J

    ~ : : ;

    8

    6

    '

    4

    }

    < t

    V

    01~

    V

    20

    lnhibitionof

    Gas Hydrate Formation

    The p

    re se

    nce of dissolved

    so

    lids in the water reduces the te

    mperatur

    e

    s

    at which

    n

    atu

    ra

    l gases forro

    h

    ydrates. Figure

    1

    7-7 gives values to reduce

    th

    e

    t

    em

    perat

    ur

    es estimated from Figure

    1

    7

    -6

    to account for the e

    ff

    ect

    o

    f

    d isso

    l

    v

    ed

    so l

    i

    ds

    in the

    wat

    e

    r

    .

    The water which condenses from na

    tural

    gas at surface conditions is

    p

    ure w ater. Often an inhibitor is

    a

    dded to

    thi

    s

    wa

    ter to lower the hydrate-

    Yes .

    Figure

    17-6

    indicates th

    at a

    O

    .

    7 specific

    gravi

    ty

    ga

    s

    form

    s

    hydrates at temperatures

    b

    elow

    5

    6F at a pressure of 500 psia if

    liquid water is present.

    4

    81

  • 7/25/2019 Cap 17 Hidratos

    9/15

    The pres

    en

    ce of liquid hydrocarbons with a hydrocarbon gas

    al

    so

    lowers hydrate-forming

    temperature s

    .

    Fi

    gure

    17-9

    indicates this de-

    pression

    hy

    drate-forming

    temperatures

    . The figure

    repre

    sents a ga

    s

    with specific gravity less than 0.6 and is probably not

    suffici

    entl

    y

    Prob

    abl

    y not. The diethylene

    gly

    col reduces the

    hydrate-formin

    g

    temperature by about

    12F

    to about 44"F . See Figure

    17-8.

    EXAMPLE 17-2:

    formin

    g temperature. The effectivene

    s

    s of two inhibitors is

    sh

    own in

    Figur

    e 1

    7-8.

    Methanol is

    obviousl

    y the better inhibitor,

    but

    di

    ethy

    lene

    glycol,

    H O (

    C 2H

    40)

    2H, often is

    us

    ed because the volatility of

    m

    ethanol

    cau

    ses high methanol loss to the ga

    s

    .

    Mono. 8,

    Chem

    .

    Eng. Prog. 52,

    324.)

    Uqu l d .

    30 40

    0

    0

    : .

    aol - - - - -- -- - - -- , 1-+- - - - l - - - - -+ -- - 4

    :;

    s1----1----- '

    r

    -+---+----+-:r-i

    f al-----+

    ~--+---

    ',':---+------OO

    3000

    1

    . . . . . . .

    e o o o

    -

    1

    \

    . . .

    1

    I O O O

    _\

    o 1

    1'l 7 /

    1

    /

    I

    )

    ~

    I

    I

    J ;..,

    lOOO

    ///

    /

    ir

    . . . - -

    . , , . . . . , . .

    V

    /

    2000

    r

    . . . . . . .

    IS

    1

    ./

    ~

    _ J 9 . .

    -

    //

    V

    l

  • 7/25/2019 Cap 17 Hidratos

    14/15

    so li

    ds). At w hat tempe

    ra

    ture

    s

    i

    s

    hy

    dr

    ate fo

    rm

    a tion

    poss

    ible?

    17 -9.

    The

    gather

    ing

    sys

    tem o

    f E

    xercise

    1

    7-8

    must

    be protected from

    hydrate fo rmat

    io

    n to a temperature o

    f

    40

    "F . Me

    thanol

    w

    ill be

    added to

    th

    e liquid

    w

    ater.

    W hat conce

    n

    tr

    ation m

    ust

    the methanol

    reach to inhibit

    hy

    dra te

    fo

    rmation?

    17-10. What concentration

    o

    f di

    e

    th

    y len

    e glycol is

    r

    equired to in

    h

    ibit

    hydrate

    fo r

    mation

    t

    o 40

    F

    E

    x

    e

    rc

    i

    s

    e

    17

    -

    8?

    17-11. Tubin

    gh

    ead con

    ditio

    ns of a dry gas well are

    2 6

    00 psia and

    l lO F. The gas

    h

    as s

    peci

    fic gravity of

    0

    .600. Sorne water

    conden

    ses

    fro

    m the

    g

    as during

    p

    rod

    u

    ction. Gas pressure is

    reduc

    ed thro

    ug

    h a choke to 1 200 psia.

    I

    s

    there a

    po

    ssibility of

    hydrate formation?

    Fig. 17-13.

    Trans.

    160,

    1 0

    ee _

    . . . . . . .

    /

    6

    ...J

    : :

    4

    3-

    -

    2

    1 . : : :

    ./

    - - - . , . /

    487

  • 7/25/2019 Cap 17 Hidratos

    15/15

    References

    Katz, D

    .

    L., et

    McGraw-Hill Book

    C

    o., Inc

    .

    , New

    Yo

    rk C ity (1 95 9)

    .

    2. Scauzillo, F.R.:

    Inhibi

    t

    ing H ydr

    a

    te Fo

    rmations

    in Hydrocarbon

    Gases,

    (A ug . 1 956) 3 2 4

    -

    2 8.

    3. Deaton,

    W .M.

    and Fr

    os

    t

    ,

    E.M .

    ,

    Jr.:

    Monograph

    Series,

    USBM, (194 6) 8 .

    17

    -

    12.

    A

    0 .

    7

    0

    s

    p

    ec

    ifi

    c

    g

    ra

    v

    i

    ty gas

    i

    s e

    x

    p

    a

    n

    ded

    throu

    g

    h

    a c

    h

    o

    ke.

    Upstream conditions are 3000

    p

    sia and

    15 0

    F.

    What is the

    lowest pre ss

    ur

    e

    t

    o w

    h

    ich the gas

    c

    an be e

    x

    panded prior t

    o

    onset

    of

    hy

    drate

    fo

    rmati

    on

    ? W

    h

    at is t

    h

    e temperature at this

    p

    ressure?

    Fig. 17-14.

    Trans.

    1

    60

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    : :

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    '

    '

    1

    1 1

    ~ \

    . .

    l

    1

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    1

    1

    1 1 ~ 1

    :

    1 '

    ::

    1

    '

    1

    1

    4

    000

    J

    I

    EMPERAiU~F

    / I J

    1

    . ,

    1

    J

    ~

    V

    I

    ,

    ,, I

    J

    J

    '0

    zooo

    "

    '

    I

    J /

    "'

    - -

    V

    I

    /

    e---'

    I I

    1

    1 70

    -

    1

    }

    I I

    160

    -

    -

    /

    , // I

    /0

    - - -

    oo

    - -

    -

    0

    s:

    :.--

    2

    :.--

    _ _ _ .

    7

    "

    -

    /

    ~

    80

    V

    : : 1 ~

    /

    60

    se

    _ _ . ,

    '

    PET

    ROLEUM

    FLU

    IDS88