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P12-1)(c))Continued$
Case$4:$Countercurrent$conditions$
We$need$to$enter$Ta$(V$=0)$values$such$that$at$V=Vf,$Taf$=$1000K,$1175K$and$1350K$respectively$
12–22$
P12-1)(f))Continued$
Calculated values of NLE variables
f(X) = X–(403.3*(T–535)+92.9*(T–545))/(36400+7*(T–528)) = 0
f(T) = X–tau*k/(1+tau*k) = 0
$
(iii)$See$Polymath$program$P12-1-f-3.pol.$
$
Calculated values of NLE variables
P12-1)(f))Continued$
Nonlinear equations
f(X) = X–(403.3*(T–535)+92.9*(T–545))/(36400+7*(T–528)) = 0
f(T) = X–tau*k/(1+tau*k) = 0
$
(iv)$See$Polymath$program$P12-1-f-4.pol.$
Change$CP$=$29$and$–ΔH$=$38700$
Polymath)Results$
NLES)Solution)$
$
NLES)Report)(safenewt)$
Nonlinear$equations$$
$[1]$f(X)$=$X–(397.3*(T–535)+92.9*(T–545))/(38700+7*(T–528))$=$0$
(v)$Modify$the$polymath$code$to$incorporate$area$as$shown$in$polymath$program$P12-1-5.pol$
f(X)=X–(403.3*(T–535)+(U*area*(T–545)/Fao))/(36400+7*(T–528))
$
Change$the$area$in$the$above$program$to$get$the$values$of$conversion$corresponding$to$the$value$of$the$
12–24$
P12-1)(f))Continued$
$
$
P12–1)(g)
(i)$0.178$mol/L$
(ii)$Ua$=$10,460$J/m3s$C$
(iii)$See$Polymath$program$P12-1-g.pol.$
Calculated)values)of)DEQ)variables$$
$
Differential)equations$$
d(T)/d(V)$=$(4000*(373–T)+(–r1a)*20000+(–r2a)*60000)/(90*Fa+90*Fb+180*Fc)$$
d(y)/d(V)$=$–alpha/(2*y)*(Ft/Fto)*(T/To)$$
12–25$
P12-1)(g))Continued$
Explicit)equations$$
k1a$=$10*exp(4000*(1/300–1/T))$$
k2a$=$0.09*exp(9000*(1/300–1/T))$$
Ca$=$Cto*(Fa/Ft)*(To/T)*y$$
Cb$=$Cto*(Fb/Ft)*(To/T)*y$$
Cc$=$Cto*(Fc/Ft)*(To/T)*y$$
$
$
$
(iv)$In$the$Polymath$program$of$part$(f)$(iii),$rate$equation$will$be$changed$as$–$$
$$$$$$$r1a$=$–k1a*(Ca–Cb/Kc)$
12–26$
P12-1)(g))Continued$
$
$
$
(v)$The$selectivity$would$increase$with$an$increase$in$Ua,$and$vice$versa.$
$
P12-1)(h)$
(i)$The$maximum$temperature$that$can$be$kept$is$440$K.$
(ii)$235$K$<$T0$<$355$K$
P12-1)(i)$
(i)$Flow$rate$will$be$close$to$zero.$
(ii)$E2$
12–27$
P12-1)(i))Continued$
Calculated)values)of)DEQ)variables$$
$
Differential$equations$$
d(T)/d(V)$=$(Qg$-$Qr)$/$sumFiCpi$$
d(Ta)/d(V)$=$Ua$*$(T$-$Ta)$/$m$/$Cpco$$
12–28$
P12-1)(i))Continued$
Explicit$equations$$
k2c$=$2$*$exp((E2$/$R)$*$(1$/$300$-$1$/$T))$$
Ca$=$Cto$*$(Fa$/$Ft)$*$(To$/$T)$*$y$$
Cc$=$Cto$*$(Fc$/$Ft)$*$(To$/$T)$*$y$$
r2c$=$–k2c$*$Ca$^$2$*$Cc$^$3$$
Cb$=$Cto$*$(Fb$/$Ft)$*$(To$/$T)$*$y$$
k1a$=$40$*$exp((E1$/$R)$*$(1$/$300$-$1$/$T))$$
r1a$=$–k1a$*$Ca$*$Cb$^$2$$
sumFiCpi$=$Cpa$*$Fa$+$Cpb$*$Fb$+$Cpc$*$Fc$+$Cpd$*$Fd$$
Qg$=$r1b$*$DH1b$+$r2a$*$DH2a$$
$
$
Addition)of)Inerts:$
The$adding$of$inerts$will$decrease$the$peak$in$the$reactor$temperature.$By$trial$and$error,$an$inert$flow$
rate$of$6.2$mol/min$is$seen$to$be$sufficient$to$keep$the$reactor$temperature$below$700K.$
12–29$
P12-1)(i))Continued$
Calculated$values$of$DEQ$variables$$
$
Differential$equations$$
d(T)/d(V)$=$(Qg$-$Qr)$/$sumFiCpi$$
d(Ta)/d(V)$=$Ua$*$(T$-$Ta)$/$m$/$Cpco$$
12–30$
P12-1)(i))Continued$
Explicit$equations$$
k2c$=$2$*$exp((E2$/$R)$*$(1$/$300$-$1$/$T))$$
Ca$=$Cto$*$(Fa$/$Ft)$*$(To$/$T)$*$y$$
Cc$=$Cto$*$(Fc$/$Ft)$*$(To$/$T)$*$y$$
r2c$=$–k2c$*$Ca$^$2$*$Cc$^$3$$
Cb$=$Cto$*$(Fb$/$Ft)$*$(To$/$T)$*$y$$
k1a$=$40$*$exp((E1$/$R)$*$(1$/$300$-$1$/$T))$$
r1a$=$–k1a$*$Ca$*$Cb$^$2$$
Qg$=$r1b$*$DH1b$+$r2a$*$DH2a$$
sumFiCpi$=$Cpa$*$Fa$+$Cpb$*$Fb$+$Cpc$*$Fc$+$Cpd$*$Fd$+$Cpi$*$Fi$$
12–31$
P12-1)(i))Continued$
(viii)$The$only$way$to$make$more$of$species$D$is$to$increase$E2.$
$
(ix)$No$solution$will$be$provided$
$
(x)$The$molar$flow$rate$of$C$does$not$go$through$a$maximum$because$the$activation$energy$of$the$
second$reaction$is$higher$than$that$of$the$first$reaction,$and$the$specific$rate$constant$is$higher$for$the$
Differential equations
d(T)/d(V) = (Qg–Qr)/sumFiCpi
d(Ta)/d(V) = Ua*(T–Ta)/m/Cpco
k2c = 2*exp((E2/R)*(1/300–1/T))
p = (1 – alpha_rho*V)^0.5
Ca = Cto*(Fa/Ft)*(To/T)*p
k1a = 40*exp ((E1/R)*(1/300–1/T))
Cb = Cto*(Fb/Ft)*(To/T)*p
Cc = Cto*(Fc/Ft)*(To/T)*p
sumFiCpi = Cpa*Fa+Cpb*Fb+Cpc*Fc+Cpd*Fd
$$
P12-1)(j))No$solution$will$be$given$
P12-1)(k))No$solution$will$be$given$
P12-1)(l))No$solution$will$be$given$
$
$
P12–2)(a)))
(i)$The$axial$temperature$profile$is$virtually$unaffected$by$change$in$heat$transfer$coefficient.$The$
maximum$of$the$radial$temperature$profile$decreases$with$an$increase$in$heat$transfer$coefficient.$This$
is$an$expected$result$as$more$heat$is$exchanged$with$an$increase$in$heat$transfer$coefficient.$$
$
$
P12–3))
(a)$FA0$
(b)$CT0$
$
NH 4NO3
( )
→2H2O g
( )
+N2O g
( )
A
( )
→2W g
( )
+B g
( )
ln k2
k1
=E
R
T2−T
1
T2T
1
#
$
%
&
‘
( =ln 2.912
0.307
#
$
% &
‘
( =E
R
50
( )
970
( )
1020
( )
k=0.307exp E
R
1
970 −1
T
#
$
% &
‘
(
)
*
+
,
–
.
XMB =−r
AV
FA0
=
kM
V⋅V
FA0
=kM
FA0
FA0HA0+FW0HW0−FAHAg
( )
−FWHWg
( )
−FBHBg
( )
=0
FA0HA0+FA0ΘWHW0−FA01−X
( )
HAg
( )
−FA0ΘW+2FA0X
( )
HWg
( )
−FA0XHBg
( )
=0
HAg,T
( )
=HA,T
( )
+ΔHVap
ΔHRx =2HWg
( )
+HBg
( )
−HA
( )
HA0−HAg
( )
+ΘWHW0−HWg
( )
( )
−2HWg
( )
+HBg
( )
−HA
( )
ΔHRx
− ΔHVap
%
&
‘
‘
(
)
*
*
X=0
HA,T
( )
−HA0
( )
CPAT−660
( )
+1−X
( )
ΔHVap +ΘWHS500°F
( )
−HW200°F
( )
+CPST−500
( )
[ ]
=−ΔHRx X
XE=CPT−660
( )
+ΘWHS500°F
( )
−HW200°F
( )
+CPST−500
( )
[ ]
−ΔHRx
ΘW=F
W
FA
=0.17
( )
18
( )
0.83
( )
80
( )
=0.9103
CPA=0.38 BTU
lb°R×80 lb
mol =30.4 BTU
lbmol°R
CPS=0.47 BTU
lb°R×18 lb
mol =8.46 BTU
lbmol°R
ΔHRx =−336 BTU
lb ×80 lb
mol =−26,880 BTU
lbmol
H200°F
( )
=168 BTU
lb =2,916 BTU
lbmol
HW500°F
( )
=1,202 BTU
lb =21,636 BTU
lbmol
12–35$
P12–5)continued$
$
$
$
P12–6))
~
Pio
Btu
C
lb mole F
! “
# $
°
% &
,lb
MW
lb mol
! “
# $
% &
20, 000
R
Btu
H
lb mol A
Δ=
,
Energy$balance$with$work$term$included$is:$
[ ]
0
0
0
10
1, 1, 1
10
( )
S
A R i Pi o
A
B
A B AF
A
Q W X H C T T
F
FX
F
Q UA Ts T
θ
θ θ
−− Δ =∑ −
= = = = =
=−
12–36$
P12–6)continued$
Substituting$into$energy$balance,$
[ ]
{ }
[ ]
0 0 0
0 0 0
0
0
0
( )
( )
( )
63525
199
S S A R AF A pA pB
S S A R A pA pB
S S A R
A pA pB
s
UA T T W F H X F C C T T
UA T T W F H F C C UA T T
UA T T W F H
T T F C C UA
Btu
Whr
T F
! “
− − − Δ = + −
% &
! “
⇒ − − − Δ = + + −
% &
− − − Δ
= + ! “
+ +
% &
−=
∴= °
$
$
$
P12-7)(a))
$
Since$the$feed$is$equimolar,$CA0$=$CB0$=$0$.1$mol/dm3$
CA$=$CA0(1-X)$
T=T0+X[−ΔHR(T0)]
φ
i
CP
i
∑+XΔ
CP
ΔCP=CpC −CpB −CpA =30 −15−15 =0
$=$-$41000$-$(-15000$)$-$(–20000)$=$–6000$cal/mol$A$
15 15 30
i i pA B pB
cal
C C C mol K
θ θ
= + = + =
∑
6000
300 300 200
30
X
T X= + = +
2 2 2
0(1 ) .01 (1 )
A A
r k C X k X−=−=−
0
0
PFR A
A
A
CSTR
A
dX
V F
r
F X
V
r
=−
=−
∫
FA0$=$CA0v0$=$(.1)(2)$=$0.2$mols/dm3$
k$=$.01*exp((10000$/$2)$*$(1$/$300$-$1$/$T))$
See$Polymath$program$P12-7-a.pol.$
Calculated)values)of)NLE)variables)$
12–37$
P12–7)(a))continued$
1$$
f(T)$=$T-$300$-$200$*$X$=$0$$
f(X)$=$X$+$V*ra/Fa0$=$0$$
k$=$0.01*exp((10000$/$2)$*$(1$/$300$-$1$/$T))$$
ra$=$–k$*$(Ca0$^$2)$*$((1$-$X)$^$2)$$
$
For)500)dm3)CSTR,)X)=)0.92$
P12–7)(b))Constant)heat)exchanger)temperature)Ta$
When$heat$exchanger$is$added,$the$energy$balance$can$be$written$as$
$
So$with$ =$0$,$$$$,$$$$=$–6000$cal/mol$
$
Where$Ua$=$20$cal/m3/s/K,$Ta$=$450$K$
See$Polymath$program$P12-7-b.pol.$
Calculated)values)of)the)DEQ)variables$
12–38$
P12–7)(b))continued$
ODE)Report)(RKF45)$
Differential$equations$as$entered$by$the$user$
$[1]$d(X)/d(V)$=$–ra$/$Fa0$
$Explicit$equations$as$entered$by$the$user$
$[1]$k$=$.01$*$exp((10000$/$1.987)$*$(1$/$300$-$1$/$T))$
$[2]$Kc$=$10$*$exp(–6000$/$1.987$*$(1$/$450$-$1$/$T))$
$
$
12–39$
P12–7)(b))continued$
$
$
$
P12–7)(c)$
For$a$co–current$heat$exchanger,$
CpC$=$1cal/g/K,$Ta1=450$K,$
12–40$
P12–7)(c))continued$
Calculated)values)of)the)DEQ)variables$
$
ODE)Report)(RKF45)$
Differential$equations$as$entered$by$the$user$
$[1]$d(X)/d(V)$=$–ra$/$Fa0$
$[1]$k$=$.01$*$exp((10000$/$1.987)$*$(1$/$300$-$1$/$T))$
$[12]$Cpc$=$1$
$
$