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    PRESENTED BY:

    1NAVIER'S-STOKES EQUATION

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    ` Fora fluid of constant density and constant

    viscosity we used equationof motion known as

    Naviers-stokes equation.` In vector form:

    gVP

    Dt

    DV!

    2V

    2NAVIER'S-STOKES EQUATION

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    ` Considera volume element,now the momentun

    balance onthe element as

    ` Rate of accumulation = (rate of momentum in)-(rate of momentum out)+(forces actingonthe

    system)

    ` eqn-(1)

    ` The velocityof fluid In cartesian form

    kwjviuV !

    3NAVIER'S-STOKES EQUATION

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    ` Considerthe fluid flowsthoughthe six facesofthe

    element.First we considered that

    ` The fluid flowingthroughthe x-direction:

    ` Momentum enters at x =

    ` Momentum leaves at x+x =

    ` Similarly fory-direction:

    `

    Momentum enters aty =` Momentum leaves aty+y =

    zyuux

    (()(V

    zyuuxx ((()(V

    zxuu y (()(V

    zxuuyy

    (((

    )(V

    4NAVIER'S-STOKES EQUATION

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    ` Forz-direction:

    ` Momentum enters at z =` Momentum leaves at z+z =

    ` Now the net convective flow throughthe element:

    eqn-(2)

    yxuuz

    (()(V

    yxuuzz

    ((()(V

    ])()[(

    ])()[(])()[(

    zzz

    yyyxxx

    uuuuyx

    uuuuzxuuuuzy

    (

    ((

    ((

    ((((

    5NAVIER'S-STOKES EQUATION

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    ` Now the normal stress actingonthe element:

    `

    ` Normal Stress actingonthe x-face:

    ` Normal stress at x =

    ` Normal stress at x+x =

    ` Similarlynormal stress actingony-face:

    ` Normal stress aty =

    `

    Normal stress aty+y =

    zyxxx

    (()(X

    zyxxxx

    (((

    X

    zxyyx

    ((X

    zxyyyx (((X

    6NAVIER'S-STOKES EQUATION

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    ` Forthe z-face:

    ` Normal stress at z =` Normal stress at z+z =

    ` The netnormal stress actingonthe element:

    `

    eqn-(3)

    ` The shearstressresult from the deformationof

    the volume element.

    yxz

    zxX

    yxzzzx

    X

    ][

    ][][

    zzzxzzx

    yyyyxxxxxxxx

    yx

    yxzxzy

    (

    ((

    ((

    ((((

    7NAVIER'S-STOKES EQUATION

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    ` The fores arise due tothe system is fluid pressure

    p and the gravitational force perunit massg.

    ` The resultantofthe forces inthe x-direction:

    ` eqn-(4)` Finallythe rate of accumulationof x momentum

    withinthe element isx yz (u/ t)

    ` Substitute all the above expression inthe equationno. 1 and resulting equation divide

    zyxgppzyxxxx

    V

    8NAVIER'S-STOKES EQUATION

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    ` byxyz.takingthe limit asx,y, and z

    appoachesto zerogivesthe x componentofthe

    equationof motion:

    ` eqn-(5)

    xzxyxxxg

    x

    p

    ttt

    wu

    t

    vu

    t

    uu

    t

    u

    t

    VXXX

    VVVV

    x

    x

    x

    x

    x

    x

    x

    x

    x

    x

    x

    x

    x

    x!

    x

    x

    )(

    )(

    9NAVIER'S-STOKES EQUATION

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    ` The equation isrearranged withthe help of

    equationof continuitytogive:

    `

    eqn-(6)` Similarequation may be derived forthe y and z

    components. Addingthe three equation vectorially

    gives

    ` eqn-(7)

    xzxyxxx gzyxt

    p

    Dt

    DuVXXXV

    x

    x

    x

    x

    x

    x

    x

    x! )(

    gpDt

    DV VXV ! ][

    10NAVIER'S-STOKES EQUATION

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    ` The stress at any point is dependsonthe velocity

    gradient and the rheological propertiesofthe fluids.Forthe newtonian fluids,the x-direction component

    ofthe stresstensorare

    ` eqn-(8)

    eqn-(9)

    eqn-(10)

    z

    w

    y

    v

    x

    uV

    x

    v

    y

    u

    Vx

    u

    yxxy

    xx

    x

    x

    x

    x

    x

    x!

    x

    x

    x

    x!!

    x

    x!

    )(

    ))(3

    2(2

    QXX

    OQQX

    11NAVIER'S-STOKES EQUATION

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    ` Where k= bulk viscosity

    ` The general equationof motion fora newtonian

    fluid with varying and viscosity are exemplified by

    the following equation forthe x direction:

    `

    ` eqn(11)

    xg

    z

    u

    x

    w

    zx

    v

    y

    u

    y

    Vx

    u

    x

    p

    Dt

    Du

    VQ

    OQQV

    xx

    xx

    xx

    xx

    xx

    xx

    xx

    xx

    !

    ][][

    ])3

    2(2[

    12NAVIER'S-STOKES EQUATION

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    z

    y

    gVz

    w

    z

    z

    v

    y

    w

    yz

    v

    x

    w

    xz

    p

    Dt

    Dw

    gz

    v

    y

    w

    z

    Vy

    v

    y

    y

    u

    x

    v

    xy

    p

    Dt

    Dv

    VOQQ

    QQV

    VQ

    OQQ

    QV

    xx

    xx

    x

    x

    x

    x

    x

    x

    x

    x

    x

    x

    x

    x

    x

    x!

    xx

    xx

    xx

    xx

    xx

    xx

    xx

    xx

    xx

    !

    ]3

    22[

    ][][

    ][

    ]3

    22[

    ][

    13NAVIER'S-STOKES EQUATION

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    ` Fora fluid of constant density and constant viscosity

    the equations (5) becomes

    `

    ` eqn(14)

    ` eqn(15)

    xx

    xx

    xx

    xx

    z

    uw

    y

    uv

    x

    uu

    t

    uV

    xg

    x

    p

    z

    u

    y

    u

    x

    u VQ xx

    xx

    xx

    xx! )(

    2

    2

    2

    2

    2

    2

    x

    x

    x

    x

    x

    x

    x

    x

    z

    u

    w

    u

    v

    u

    ut

    u

    V

    gp

    z

    uuuVQ

    x

    x

    x

    x

    x

    x

    x

    x!

    2

    2

    2

    2

    2

    2

    14NAVIER'S-STOKES EQUATION

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    x

    x

    x

    x

    x

    x

    x

    x

    z

    uw

    y

    uv

    x

    uu

    t

    wV

    zg

    z

    p

    z

    w

    y

    w

    x

    wVQ

    x

    x

    x

    x

    x

    x

    x

    x!

    2

    2

    2

    2

    2

    2

    gVpDt

    DVVQV ! 2

    15NAVIER'S-STOKES EQUATION

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    ` Unitoperationof chemical engineering-MacCabe

    smith and harriott

    NAVIER'S-STOKES EQUATION 16