10.2 thermo probset

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    University of San Carlos

    Nasipit, Talamban, Cebu City 6000

    Department of Chemical Engineering

    CHE !!N

    Assignment on Low Pressure Vapor-Liquid Equilibria in Non-ideal Mixtures

    Submitte" by#

    Duterte, $an %ommel T&

    Submitte" to#

    Engr& 'uis (& Cabatingan

    )nstructor

    September !, *0!+

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    10.2-1

    iven#

    ethyl bromi"e -!. / nheptane -*. mi1ture at 202&!+ (

    P1

    vap= 0.7569 bar , P2

    vap= 0.0773 bar

    regular solution parameters

    3'-cm24mol. 5 -cal4cm2.!4*

    ethyl bromi"e + 7&8

    nheptane !7 &

    %e9uire"#

    a. Composition of the vapor in e9uilibrium :ith a li9ui" containing &*2 mol ; ethyl bromi"e at

    202&!+ ( an" 0&+2 bar, assuming the solution is i"eal

    b. 3apor composition in part a assuming the solution is regular

    c. 3apor composition in part a using the UN)

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    values are use" to calculate the van 'aar an" F parameters& These parameters are then use" to

    calculate the activity coefficients at the ne: composition -1!@ 0&*2 an" @ 0&+2 bar., an"

    the mo"ifie" %aoult>s 'a: use" to calculate the ne: vapor compositions&

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    vapor pressure "ata

    Species Temperature -C. vap-bar.

    Iater!08&+ !&077

    !00&6 !&02+*

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    ethanol -!. / benGene -*. mi1ture at +C

    e1perimental "ata

    x1 y1 -bar.

    0 0 0&*828

    0&02 0&!86+ 0&26!20&08* 0&*78+ 0&28+2

    0&*!72 0&220 0&077

    0&2!! 0&26*+ 0&!*

    0&!+0 0&27* 0&!*7

    0&+!88 0&06+ 0&!00

    0&+*7 0&!0! 0&082

    0&6!++ 0&22 0&0*7

    0&07 0&+! 0&278!

    0&7!0* 0&++6 0&26!+

    0&8!82 0&07 0&2026

    0&8+8! 0&7*0! 0&*!!

    !&00 !&00 0&*2*!%e9uire"#

    repare an 1y an" 1 "iagram for the system assuming, separately,

    a. the mi1ture is i"eal

    b. the mi1ture is regular

    c. the mi1ture is "escribe" by the UN)

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    The "iagrams can no: be constructe", as sho:n in s Chemical Engineers> Han"booK to calculate

    the ethanol vapor pressure at T!@ +C an" T*@ 6C,vap @ !&7+ K$4mol& This is use"

    to calculate the solubility parameter for ethanol, :hich is calculate" to be !*&66 -cal4cm 2.!4*& )n

    summary,

    3'-cm24mol. 5 -cal4cm2.!4*

    Ethanol +7&28 !*&66

    PenGene 78 8&*

    The volume fractions can then be calculate" from

    ( =x ( V (

    x1 V1+ x2 V2

    The activity coefficients are calculate" from

    1 = e

    V1 22

    ( 1- 2)2

    RT

    2 = e

    V2 12

    ( 1 - 2)2

    RT

    The e9uilibrium pressure an" vapor composition is calculate" using the mo"ifie" %aoult>s 'a:#

    Pe = x11 P1vap

    + x22 P2vap

    y ( =x ( ( P (vap

    Pe

    The follo:ing table summariGes the calculate" values&

    Table *& 3alues obtaine" using the regular solution mo"el

    A! A* B! B* 1! e9 y!0 ! 2&02+2 ! 0&00 0&*828 0

    6

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    0&068 0&82*! *&6*2 !&007 0&!0 0&2*+ 0&!760

    0&!08 0&7+8! *&*682 !&02* 0&*0 0&27+ 0&20*2

    0&*!8+ 0&70+ !&8668 !&078 0&20 0&260* 0&2702

    0&202 0&68+ !&!!6 !&!686 0&0 0&26+* 0&2+*

    0&286* 0&6027 !&88! !&20* 0&+0 0&26+6 0&+7

    0&860 0&+00 !&2*+7 !&+!6 0&60 0&26*8 0&+077

    0&608 0&28+! !&!782 !&7+ 0&0 0&2+0 0&+!2

    0&*! 0&*+8 !&077* *&*76 0&70 0&27 0&+760

    0&7++* 0&!7 !&0*26 2&6 0&80 0&2!+! 0&67+

    ! 0 ! +&2* !&00 0&*2*! !

    The "iagrams can no: be constructe", as sho:n in

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    2'I

    = e

    &

    (1+& x2#x1)

    2

    =n" the vapor composition is then

    y1 =x

    1

    1

    'IP

    1

    vap

    P

    The follo:ing table summariGes the calculate" values&

    Table & 3alues obtaine" using the van 'aar mo"el

    1! 1* B! B* e9 y!

    0&00 !&00 &+760 ! 0&*828 0

    0&!0 0&80 &6*67 !&0*+8 0&27 0&*72+

    0&*0 0&70 2&!0* !&!002 0&0* 0&2+6

    0&20 0&0 *&*+0 !&**2 0&076 0&27!

    0&0 0&60 !&+** !&00+ 0&086 0&28!

    0&+0 0&+0 !&*7 !&6!0 0&076 0&0870&60 0&0 !&*6 !&8+80 0&00 0&200

    0&0 0&20 !&!* *&226 0&28*0 0&66!

    0&70 0&*0 !&0+06 *&808+ 0&266! 0&+2*8

    0&80 0&!0 !&0!!7 2&+87+ 0&2!! 0&666+

    !&00 0&00 ! &707 0&*2*! !

    The "iagrams can no: be constructe", as sho:n in

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    0.00 0.10 0.20 0.30 0.40 0.50 0.60 0.70 0.80 0.90 1.000.2

    0.22

    0.24

    0.26

    0.28

    0.3

    0.32

    0.34

    0.36

    0.38

    0.4

    0.42

    Ide

    al mixture model UNIFAC mixture model van aar model

    !e"ular mixture model #x$erimental data

    x#t%&

    () *ar

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    $% 1=

    (1+ x 1 x2 )2

    $% 2=

    (1+ x2

    x 1 )2

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    b. Determine the enthalpy an" entropy changes on mi1ing :hen ! mole of benGene an" * moles of

    cyclohe1ane are mi1e" at T @ 200 ( an" constant pressure

    c. iven the follo:ing vapor pressure "ata at T @ 2*0 (, P1vap= 0&2*02 bar an" P2

    vap=

    0&2*!7 bar, "etermine the bubble point pressure of the li9ui" in part -b. at T @ 2*0 (, an" the

    composition of the vapor in e9uilibrium :ith that li9ui"

    Solution#

    a. ex

    = x11ex

    + x22ex

    = x1 RT$%1 + x2 RT$%2

    1

    ex= RT $% 1 an" 2

    ex= RT $% 2

    ex

    = x1 x2=(11+2 )(2

    1 + 2 )= 1 2 ( 1+ 2 )-2

    ex

    = 1 2 ( 1+2 )-1

    1ex

    =;

    ex

    ; 1= 12(1 + 2 )

    -2+ 2 (1 + 2 )

    -1= (21 + 2

    1 2

    ( 1+ 2 )2 )= x22

    2ex=

    Nex

    N2

    =A N1N2(N1+N2 )2+A N1 (N1+N2 )

    1=A ( N1N1+N2

    N1N2

    (N1+N2 )2 )=A x12

    Since 1ex

    = RT $% 1 ,

    1 =e1

    ex

    RT = ex2

    2

    RT =e(1- x1)

    2

    RT

    Similarly,

    2 =e

    2ex

    RT = e

    x12

    RT =e

    (1- x2)2

    RT

    b.x1=

    1

    3 an"x2=

    2

    3

    %ecall,

    (x = (x +T

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    P= x11P1vap

    + x22 P2vap

    =0.3557 bar

    y1 =x11 P1

    vap

    Pb?bb$e= 0.3662

    y2 =x22 P2vap

    Pb?bb$e= 0.6338

    =ns:er4s#

    a. The activity coefficients of the benGene an" cyclohe1ane can be "escribe" by

    1 = e

    ( 1-x 1 )2

    RT a% 2= e

    ( 1-x2)2

    RT , respectively&

    b. Ihen ! mole of benGene an" * moles of cyclohe1ane are mi1e" at T @ 200 ( an" constant

    pressure,

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    & =(1+ x1 $% 1BC(

    x2 $% 2BC( )

    2

    $% 2BC(

    = 1.0800

    Since the final li9ui" compositions are yet to be foun" an" they are nee"e" to calculate the final activity

    coefficients -:hich are use" to calculate the final vapor compositions., a trialan"error solution is use"&

    The follo:ing e9uations must be satisfie" in or"er to fin" the vapor an" li9ui" compositions#

    x1+ x2 = 1) y1+ y2= 1

    1BCD

    = e

    #

    (1+#x 1&x2)

    2

    ) 2BCD

    = e

    &

    (1+ &x2#x1)

    2

    593.425x11 = y1P) 416.5845 x22 = y2 P

    P= x11P1vap

    + x22 P2vap

    = trial value of 1!an" 1*is use" to calculate 1BCD

    an" 2BCD & The activity coefficients are use" to

    calculate the total e9uilibrium pressure, then the vapor compositions& The calculation is repeate" until

    x (= y (=1 an" x (=y ( & Using the icrosoft E1cel Solver function, the aGeotropic vapor an"li9ui" compositions are foun" to be 1!@ y!@ 0&6+22 an" 1*@ y*@ 0&26 at +0C an" 62&8 mm Hg&

    =ns:er4s# The aGeotropic composition of a methyl acetate / methanol mi1ture at +0C is 1 =@ y=@

    0&6+22 an" 1eH@ yeH@ 0&26 at a pressure of 62&8 mm Hg&

    10.2-2$

    iven#

    PenGene -!. / polyisobutylene -*. mi1ture at !0C

    Data on physical properties

    benGene polyisobutylene

    olecular :eight, g4mol 70 000

    !0 -monomeric.

    olar volume, cm24mol 77&*6 !2!&8 -monomeric.

    3apour pressure, bar0&!*66 -at *87&!+ (.

    0&*28* -at 2!*&+ (.=ssume" to be negligible

    Data for the activity of benGene in )P as a function of the mass ratio of benGene to )P

    E /PIE aE=xEE

    0&722! 0&87!!

    0&++2 0&8+8+

    0&*8! 0&7277

    %e9uire"#

    a. Using the "ata in )llustration !0&*, compare the pre"ictions of the

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    an" are 0&++, 0&2+66 an" 0&**+, respectively& The benGene mole fractions -in terms of the

    :eight fraction. are then calculate" as

    xE =

    HE

    78

    H E

    78 +

    HPIE

    40000

    an" are 0&88, 0&886+ an" 0&8822, respectively& The

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    b. The partial pressures of benGene are sho:n in table 6&

    10.2-$%

    iven#

    Component ! an" * mi1ture in vapourli9ui" e9uilibrium

    =t 80C an" !&7+0+ bar, a vapour of composition y! @ 0&26 coe1ists :ith a li9ui" ofcomposition 1!@ 0&

    3apour pressures are given by

    $:@10 P(vap

    = (E(

    T

    for pressure in bar an" T in (, :here =!@ &!*+, P!@ !+00, =*@ +&000 an" P*@ !+0

    %e9uire"#

    a. Determine the van 'aar parameters of the system using the given "ata

    b. Determine :hether the mi1ture has an aGeotrope at 80C an", if so, "etermine its composition an"

    i"entify :hether it is a ma1imum or minimumpressure aGeotropec. btain 1y an" 1y "iagrams for the system at 80C

    ". =n e9uimolar mi1ture of species ! an" * initially at very lo: pressure is compresse" at a constant

    80C& =t :hat pressure "oes the first "rop of li9ui" form, an" :hat is its compositionQ =t :hat

    pressure "oes the last bubble of vapour "isappear, an" :hat :as its compositionQ

    Solution#

    a.

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    0&0 !&!+8* *&!*6 !&672 0&+2!

    0&70 !&0677 *&!!! !&6668 0&+06+

    0&80 !&0!0 2&+82+ !&80 0&6*2

    !&00 ! &8++0 0&87 !

    The highlighte" ro: is the aGeotropic pointJ the mi1ture forms an aGeotrope at appro1imately

    0&2 mole fraction of species ! at 80C an" a pressure of !&7+!2 bar& The mi1ture is a ma1imum

    pressure aGeotrope since the activity coefficients of both species are greater than !&0, an" there

    are positive "eviations from %aoult>s 'a:&

    c. Using the values summariGe" in the previous table, the 1y an" 1y "iagrams can be

    constructe"&

    0.00 0.20 0.40 0.60 0.80 1.000

    0.2

    0.4

    0.6

    0.8

    1

    x1

    '1

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    b. The mi1ture forms an aGeotrope at appro1imately 0&2 mole fraction of species ! at 80C an" a

    pressure of !&7+!2 bar& The mi1ture is a ma1imum pressure aGeotrope since the activity

    coefficients of both species are greater than !&0, an" there are positive "eviations from %aoult>s

    'a:&

    c. See figures an" +&

    ". The pressure at :hich the first "rop of li9ui" forms is appro1imately !&6 bar, an" this "rop has acomposition 1!@ 0&70& The last bubble of vapor "isappears at !&7 bar, an" the bubble ha" a

    composition of y!@ 0&0&

    10.2-$

    iven#

    Iater -!. / !,"io1ane -*. mi1ture at 2*2&!+ (

    3aporli9ui" e9uilibrium "ata

    -mm Hg. 1! y!!*0&8 0&0000 0&0000

    !0&7+ 0&0+60 0&!8*0

    !+!&!6 0&080 0&*670

    !+8&! 0&!00 0&2+0

    !6&+ 0&*!60 0&2720

    !6+&6+ 0&*870 0&020

    !6&78 0&2660 0&*+0

    !6& 0&00 0&20

    !6&8 0&60 0&60

    !6&8+ 0&70 0&+!0

    !66&7 0&+280 0&++0

    !6+&7 0&6*80 0&660

    !60&7* 0&80 0&8+0

    !++&! 0&7!!0 0&+20!*&6 0&7800 0&600

    !!&6 0&860 0&8+0

    8*&+! !&0000 !&0000

    %e9uire"#

    a. =ctivity coefficients at each of the reporte" compositions

    b. =re these "ata thermo"ynamically consistentQ

    c. lot of e1cess ibbs energy as a function of composition

    Solution#

    a. The van 'aar mo"el :ill be use" to calculate the activity coefficients&

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    &!1-x1

    1+# x1

    1'I

    = e

    #

    ( )2

    &!1-x11+

    2'I

    = e

    &

    (# x1)2

    The results are summariGe" in the follo:ing table&

    Table 7& =ctivity coefficients of the :ater"io1ane system

    1! B! B*0&0000 +&76* !

    0&0+60 &60 !&00

    0&080 &!662 !&0!*

    0&!00 2&*+7 !&0+20&*!60 2&08 !&0+*

    0&*870 *&8+ !&!+!8

    0&2660 *&!08 !&*2*

    0&00 !&72+ !&28+

    0&60 !&7!27 !&28*6

    0&70 !&6762 !&72

    0&+280 !&+*72 !&6

    0&6*80 !&2*6 *&00*

    0&80 !&!2 *&786

    0&7!!0 !&070 2&!02

    0&7800 !&0*2 &++**

    0&860 !&00*+ 6&*627

    !&0000 ! &*680

    b.

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    0.00 0.10 0.20 0.30 0.40 0.50 0.60 0.70 0.80 0.90 1.00+2

    +1.5

    +1

    +0.5

    0

    0.5

    1

    1.5

    2

    2.5

    x1

    ln ,2-,1