cre ii -28

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    L -28 Diffusion Effects in Spherical Pellet

    Prof. K.K.Pant

    Department of Chemical EngineeringIIT Delhi.

    [email protected]

    mailto:[email protected]:[email protected]
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    1storder Reaction in Spherical Pellet

    What about n-th order ?

    022

    2

    nA

    e

    nAA CDk

    drdC

    rdrCd

    02 1

    2

    2

    A

    e

    AAC

    D

    k

    dr

    dC

    rdr

    Cd

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    Dimensionless Form of the Equation

    Dimensionless symbol are normally introduced to

    Reduce complexity in equation

    Simplify operation of calculation

    Scale-up the reactor

    Let = CA/CAs and =r/R

    dCA/dr= (dCA/d)(d/dr)= (d/d)(dCA/d )x(d/dr)

    => dCA/dr = (d/d)(CAS/R)d

    2

    CA/dr

    2

    = d/dr(dCA/dr)= (d

    2/d

    2

    )(CAS/R

    2

    )WhenCA=CAsat r=R, => =1 and =1

    CA=finite at r=0, => =finite and =0

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    Dimensionless eq.1storder

    for n-th order ?

    02

    2

    2

    n

    A

    e

    nAA CD

    k

    dr

    dC

    rdr

    Cd

    02 1

    2

    2

    A

    e

    AAC

    D

    k

    dr

    dC

    rdr

    Cd 2

    2

    12

    20

    d d

    d d

    22

    2

    20

    n

    n

    d d

    d d

    Thiele

    Module

    Thiele

    Module

    eDRk 21

    e

    n

    Asn

    D

    CRk 12

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    Thiele Modulus, n

    2 n-1 n

    2 n As n Asn

    e e As

    k R C k RC "a" surface reaction rate = = =D D [(C -0)/R] "a" diffusion rate

    If n is largeinternal diffusion limits the

    overall rate

    If n is smallthe surface reaction limits the

    overall rate

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    6

    Define y= => = y/

    d /d = 1/ (dy/d )y/2d2 /d 2 = 1/d2y/d2 - 2/2dy/d + 2y/ 3

    d2y/d 2 - 2y=0 Solutiony= A Cosh + B Sinh

    A=0 as must be finite at the centre

    (B. C =0, cos h 1; 1/ , and Sin h 0.

    A 1

    As 1

    C sinh 1 = =C sinh

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    The total rate of consumption Of A inside a pellet

    Evaluated at the surface conditions

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    Internal Effectiveness Factor

    As s

    Actual overall rate of reaction =

    Rate of reaction that would result if entire

    interior surface were exposed to the externalpellet surface conditions C ,T

    ' "

    A A A

    ' "

    As As As

    -r -r -r = = =

    -r -r -r

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    For STRONG PORE DIFFUSION

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    Internal Effectiveness Factor

    1 12

    1

    3

    = coth -1

    Internal effectivenessFactor, is: ranged 01

    for a first-orderreaction in a spherical

    catalyst pellet

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    12

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    Calculation of Catalytic Effectiveness FactorCatalytic Effectiveness Factor:

    where

    - Thiele Modulus

    1storder reaction rate:

    Spherical Pellet

    Cylindrical Pellet

    Slab Pellet

    )313(1

    Coth

    DekSaR p /3

    DekSaR

    p/2

    DekSaL p /

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    How can the rate of reaction be increased?

    Decrease the radius of the pellet.

    increase the temperature.

    Increase the concentration

    Increase the internal surface area

    For large value of Thiele modulus, the effectiveness factor (for n>1

    efffectiveness factor decrease with increase concentration at the

    external surface of the pellet

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    For nthorder reaction

    = ( 2/n+1 )1/23/

    = R( k CASn-1/ De)1/2

    OR

    2= R2kSap CASn-1/De

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    Uses the measured values of the rate of reaction to

    determine if Internal diffusion controls the rate.

    Weisz-Prater Parameter CWP2= 3( Coth -1)

    2 = (observed rate/rate cal. at CAS) x (rate

    calculated at CAS) / diffusion Rate)

    = (-rA(obs)/ -rAs

    2= -rASSapR2/De CAs = -rAS pR

    2/De CAs

    WeiszPrater Criterion for internal diffusion

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    CWP= (-rA(obs)/ -rAs )(-rASpR2/De CAS)

    CWP = (-rA(obs) (pR2/De CAS)

    These are measured or known terms.

    if CWP > 1, Internal diffusion limits the rate.

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    Falsified Kinetics Measurement of the apparentreaction order

    and activation energy results primarily wheninternal diffusion limitations are present.

    This becomes serious if the catalyst pelletshape and size between lab (apparent) andreal reactor (true) regime were Too different.

    Smaller catalyst pelletreduces the diffusion

    limitationhigher activation energy moretemperature sensitive

    RUNAWAY REACTION CONDITIONS!!!!

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    Falsified Kinetics

    With the same rate of production, reaction order

    and activation energy to be measured

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    Determination of apparent order of reaction

    For large value of Thiele modulus

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    21

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    Apparent order of reaction n = (ntrue+1 )/2

    N i th l ll t E b l

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    Non isothermal pellet Energy balance

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    24

    Non isothermal pellet effectiveness factor

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    25

    Overall effectiveness factor (Both internal and external

    diffusion are important

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    26

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    Slove for Cas, Conc at pellet

    Surface

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    Overall rate in terms of

    bulk concentration

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    Rate of reaction, -rA

    = (Actual overall rate of reaction) divided by(rate that would result if the entire surface

    were exposed to the bulk conditions, CAb,Ts)

    "

    1 a b c c

    " " "A Ab 1 Ab

    ' " "

    A A b A a b 1 Ab a b

    =1+k S /k a

    -r = (-r ) = k C

    -r = -r = -r S = k C S

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    Mass transfer and reaction in a

    packed bed

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    'AzA b

    AbAz AB Ab

    2'Ab Ab

    AB A b2

    dW- +r = 0

    dz

    where

    dCW = -D +C U and

    dz

    U = superficial velocity

    hence

    d C dCD -U +r = 0

    dz dz

    Mole balance in flux form, where Acis

    constant and FA= AcWAz =ACU CA

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    Mass Balance in a Packed bed (Mass Transfer

    control)

    FAzFAZ+Z - (-rA) a Ac z = 0

    A= surface area per unit volume, U superfecial

    velocity.

    U dCA/ dz = - kcCA ac

    . CA= CA0exp (- kcac z/U)

    Or ln (1-X) = ( -kc az/U)

    0.0)()( iSGiccGiG CCakdz

    dCU

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    Catalytic Fixed-Bed Reactor - Design Model

    Mass Balance around the catalyst

    Gas-Phase component mass balance (Plug Flow model)

    Gas-Phase component mass balance (Dispersion model)

    Energy Model

    inetSGicc RiCCak )()()(

    0.0)()( iSGiccGi

    G CCakdz

    dCU

    0.0)()(2

    2

    iSGiccGiGGiG CCakdz

    dCU

    zd

    CdiD

    )()( TaTUAjHRjdzdTCpU RGGG

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    Overall Rate with in the pellet (-rA= (rAb)

    For first order reaction : (-rAb;= (rAb)Sa= ksSa CAb

    =>(-rA)= (rAb) = Sabk CAb

    2

    2

    0s b bAb Ab Ad C dC

    Da U k SaCdz dz

    Neglecting Axial Dispersion

    ( )s aAb

    AbdC k S

    Cdz U

    => CAb= CAb0 exp(- Sa bks Z/U)

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    Axial diffusion, can be neglected when

    FAis very large

    so

    Finally, the conversion for

    1storder reaction in PBR is

    '

    0 p A b p

    a 0 Ab

    U d -r d>>

    D U C

    2Ab

    a 2

    d CDdz

    "

    Ab b aAb

    dC k S= - C

    dz U

    Remember the

    forced

    convection in

    binary external

    diffusion, JAisalso neglected

    b a-( k"S L)/UAb

    Ab0

    CX =1- =1- e

    C

    Mass transfer and reaction in a packed bed

    cont.

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    Determination of limiting situation from

    reaction data

    Type ofLimitation

    Variation of Reaction Rate with:

    Velocity

    Particle

    Size TemperatureExternaldiffusion

    U (dp)-3/2

    Rate= kcac CA

    Linear

    InternalDiffusion

    Independent (dp)-1 Exponential

    SurfaceDiffusion

    Independent

    Independent

    Exponential