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13-1$
Solutions)for)Chapter)13)–)Unsteady)State)Non–isothermal)
Reactor)Design)
)
P13-1)(a))Example)13-1)
(i)$The$reaction$runs$away$at$T0$=$282.2$K$
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(ii)$$
(1)$Runaway$occurs$at$Ta1$=$292$K$
(2)$As$Ta1$increases,$the$maxima$of$the$Qr$versus$t,$and$Qg$versus$T$curves$occur$at$shorter$times.$This$is$
$
(iv)$$
If$the$heat$of$mixing$had$been$neglected,$the$shape$of$the$graphs$would$have$been$as$follows:$
)
(v)$$
The$new$T0$of$20$˚F$(497$˚R)$gives$a$new$δHRn$and$T.$With$T=497+89.8X$the$polymath$program$of$
13-2$
P13-1)(a)$Continued$
(vi)$
Calculated values of DEQ variables$$
d(T)/d(t) = (Qr – (-36309) * (–ra) * V) / NiCpi
k = 0.000273 * exp(16306 * ((1 / 535) – (1 / T)))
Qg = (–36309) * (–ra) * V
13-3$
P13-1)(a)$Continued$
$
P13-1)(b))Example)13-2)
(i)$No$explosion$would$occur$for$NA0$<$8.9$kmol.$Similarly,$no$explosion$would$have$occurred$for$NB0$<$
32.2$kmol$
$
13-4$
P13-1)(b)$Continued$
(v)$
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P13-1)(c))Example)13-3)
(i)$1650$lbmol/hr$
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(ii)$No,$it$is$not$possible.$
13-5$
P13-1)(c)$Continued$
Ordinary Differential Equations
Calculated values of DEQ variables
13-6$
P13-1)(c)$Continued$
Differential equations
d(Ca)/d(t) = 1/tau*(Ca0–Ca)+ra
d(Cb)/d(t) = 1/tau*(Cb0–Cb)+rb
d(Cc)/d(t) = 1/tau*(0–Cc)+rc
d(Cm)/d(t) = 1/tau*(Cm0–Cm)
k = 16.96e12*exp(–32400/1.987/(T+460))
ThetaCp = 35+Fb0/Fa0*18+Fm0/Fa0*19.5
v0 = Fa0/0.923+Fb0/3.45+Fm0/1.54
Ta2 = T–(T–Ta1)*exp(–UA/(18*mc))
NCp = Na*35+Nb*18+Nc*46+Nm*19.5
13-7$
P13-1)(c)$Continued$
(v)$See$polymath$program$p13–1cv.pol$
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(vi)$
$
13-8$
P13-1)(c)$Continued$
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$
$
$
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(vii)$No$solution$will$be$provided$
13-9$
P13–1)(c)$Continued$
(ix)$Time$to$reach$steady$state$increases$with$increase$in$tank$volume.$When$the$tank$volume$is$at$its$
minimum,$practical$stability$limit$is$not$exceeded$for$any$of$the$three$sets$of$initial$conditions.$However,$
as$we$increase$the$volume,$it$is$observed$that$for$Ti$=$340$K$and$CAi$=$1.4$M,$the$practical$stability$is$
P13-1)(d))Example)13-4$
(i)$The$maximum$in$CC$increases$with$an$increase$in$CB0.$
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P13-1)(e))Example)13-5$
(i)$One$of$the$possible$combinations$is$CA0$=$8$mol/dm3$and$𝑣!=$240$dm3/h.$
$
13–10$
P13-1)(e)$Continued$
$
We$can$see$from$the$graph$that$NA$and$NB$become$constant$at$large$times.$
(vi)$See$polymath$program$P13–1evi.pol$
$
Ordinary Differential Equations
Calculated values of DEQ variables
d(Ca)/d(t) = ra+(Cao–Ca)*vo/V
d(T)/d(t) = (35000*(298–T)–Cao*vo*30*(T–305)+((–6500)*(–k1a*Ca)+(8000)*(–
k2b*Cb))*V)/((Ca*30+Cb*60+Cc*20)*V+100*35)
13–11$
P13-1)(e)$Continued$
Explicit equations
k1a = 1.25*exp((9500/1.987)*(1/320–1/T))
k2b = 0.08*exp((7000/1.987)*(1/290–1/T))
$
We$find$that$after$running$the$code$for$a$final$time$of$10$hours,$we$get$NA$=$290.8397$mol$and$NB$=$
915.6613$mol.$$
𝐶
!!𝑣!
𝑘!!
=4∗
240
3.2881
=291.962 𝑚𝑜𝑙$
$
P13-1)(f))Example)13-6)
(i)$The$pressure$shoots$up$when$the$volumetric$flow$rate$is$3976$dm3.$
(v)$Individualized$solution$
(vi)$Individualized$solution$
(vii)$The$transition$to$runaway$occurs$over$a$very$small$range$of$Ua.$If$U$a$value$is$changed$such$that$Ua$is$
13–12$
P13-1)(f)$Continued$
But$the$cooling$starts$only$for$T>455K$
Thus$Ua$=$2.77$×$106$J/hr/K,$T>$455K$
$$$$$$$$$$$$$$$=$0$for$T<$455K$
$
Calculated values of DEQ variables$$
change in concentration of cyclomethylpentadiene$$
change in concentration of diglyme$$
d(P)/d(t)$=$SW1*((FD–Fvent)*0.082*T/VH)$$
d(T)/d(t)$=$SW1*((V0*(r1A*DHRx1A+r2S*DHRx2S)–SW1*UA*(T–373.15))/SumNCp)$+$SW1*Sw2*4/60$$
13–13$
P13-1)(f)$Continued$
Explicit equations
k1A$=$A1A*exp(–E1A/(8.31*T))$$
rate constant reaction 1$$
k2S$=$A2S*exp(–E2S/(8.31*T))$$
rate constant reaction 2$$
SW1$=$if$(T>600$or$P>45)$then$(0)$else$(1)$$
mol/dm3/hour (first order in sodium and cyclomethylpentadiene)$$
mol/dm3/hour (first order in diglyme)$$
FD$=$(–0.5*r1A–3*r2S)*V0$$
Fvent$=$if$(FD<11400)$then$(FD)$else(if$(P<28.2)$then$((P–1)*Cv1)$else$($(P–1)*(Cv1$+Cv2)))$$
UA$=$if$T>$455$then$(2.77e6)$else$(0)$$
Sw2$=$if$((T>300)$and$(T<422))$then$(1)$else$(0)$$
13–14$
P13-1)(f)$Continued$
$ $
$
(ix)$Solving$the$equations$with$Ua$=$0$for$the$entirety$of$the$process,$we$get$that$the$temperature$
reaches$at$0.94$hours$while$the$system$reaches$runaway$at$3.649$hours.$This$implies$the$maximum$time$
$
$
(x)$Individualized$solution$
)
P13-1)(g)$Example)RE13-1)
Using$the$code$from$Example$PRS$13.5,$we$can$determine$the$value$of$kc$for$which$the$reactor$will$fall$to$
the$lower$steady–state$and$when$it$becomes$unstable.$The$following$two$graphs$show$those$points$
13–15$
P13-1)(g)$Continued$
$
P13-1)(h))Example)RE13-2$
Using$the$code$from$Example$PRS$13.5,$we$can$change$the$value$of$kc$and$τ1$and$find$values$that$
$
$
P13-1)(i))No$solution$will$be$given$
$
P13–1)(j))Individualized$solution$
$
)
13–16$
P13-2)
After$the$feed$was$shut$off,$$$
)
$
)
See$Polymath$program$P13-2.pol$
Calculated values of DEQ variables
d(T)/d(t) = –dH * k / Cpa
k = (0.307/60)* exp(44498 * (1 / 970 – 1 / T))
13–17$
P13-2$Continued$
As$can$be$seen$from$the$above$plots,$temperature$shoots$at$time$t)=)3.16)mins)
Since$NA$doesn’t$come$in$the$temperature$equation,$there$will$not$be$any$effect$of$feed$present$in$the$
$
)
13–18$
P13-3)(a))
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$
$
$
$
13–19$
P13-3)(a)$Continued$
See$Polymath$program$P13-3-a.pol$
Calculated values of DEQ variables
d(T)/d(t) = ((6000*(–ra*V))–(Fbo*15*(T–323)))/(15*Na+15*Nb+30*Nc)
Fbo = if(t<50)then(10)else(0)
k = .01*exp((10000/1.987)*(1/300–1/T))
V = if(t<50)then(50+(vo*t))else(100)