10.2 thermo probset
TRANSCRIPT
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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