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5-41$
P5–24)Continued$
$
$
)
$
P5–25))$
δ=0“,”ε=0
∴p=1− αW
( )
1 2
$
Mole$Balance/Design$Equation$
$
5-42$
P5-25)Continued$
Rate$Law$
$
)
$
P5–26)Individualized$solution$
)
$
6-1$
Solutions)for)Chapter)6)–)Isothermal)Reactor)Design-)Molar)
Flow)rates)
)
P6–1)(a))Example)6–1))
(i)$The$conversion$increases$with$an$increase$in$both$E$and$T.$This$is$because$the$rate$constant$is$higher$
for$higher$E$and$T.$
Ordinary Differential Equations
Calculated values of DEQ variables
k = 0.29*exp(E/1.987*(1/500–1/T))
Total number of equations
Number of differential equations
Number of explicit equations
Truncation error tolerance. eps
)
(iii)$See$Polymath$program$P6-1-aiii.pol.$
Ordinary Differential Equations
Calculated values of DEQ variables
k = 0.29*exp(E/1.987*(1/500–1/T))
ra = –k*(Ca^2 – Cb^2*Cc/Kc)
Total number of equations
Number of differential equations
Number of explicit equations
Truncation error tolerance. eps
6-4$
$
(iv)$
𝑝=1− ∝!𝑉
!
!$
$
See$Polymath$program$P6-1-aiv.pol$
Ordinary Differential Equations
Calculated values of DEQ variables
k = 0.29*exp(E/1.987*(1/500–1/T))
Total number of equations
Number of differential equations
Number of explicit equations
Truncation error tolerance. eps
6-6$
$
$
P6–1)(b))Example)6–2)$
(i)$The$conversion$increases$with$increase$in$KC,$k,$CT0,$and$kc.$This$is$because$in$each$of$the$cases,$the$
(iii)$Individualized$solution$
(iv)$RB$is$maximum$when$KC,$k,$CT0,$and$kc$are$at$their$maximum$values$
(v)$Individualized$solution$
(vi)$See$Polymath$program$P6-1-b.pol.$
Ordinary Differential Equations
Calculated values of DEQ variables
6-7$
Differential equations
d(Fb)/d(V) = –ra–kc*Cto*(Fb/Ft)*p
ra = –k*Cto*((Fa/Ft)*p – Cto/Kc*(Fb/Ft)*(Fc/Ft)*p*p)
Total number of equations
Number of differential equations
Number of explicit equations
Truncation error tolerance. eps
$
The$conversion$goes$up$from$60%$to$66.6%$
(vii)$Individualized$solution$
$
(viii)$Individualized$solution$
$
6-8$
P6–1)(c))Example)6–2)$
See$Polymath$program$P6-1-c.pol$
Ordinary Differential Equations
Calculated values of DEQ variables
d(Fb)/d(V) = –ra–kc*Cto*(Fb/Ft)*p
Total number of equations
Number of differential equations
Number of explicit equations
Truncation error tolerance. eps
$
$
P6–1)(d))Example)6–3))
See$Polymath$program$P6-1-d.pol$
Ordinary Differential Equations
Calculated values of DEQ variables
d(Cb)/d(t) = ra+ (Cbo–Cb)*vo/V
ra = –k*(Ca*Cb – Cc*Cd/Kc)
X = (Cao*Vo–Ca*V)/(Cao*Vo)
Total number of equations
Number of differential equations
Number of explicit equations
Truncation error tolerance. eps
$
On$comparison$with$the$solution$obtained$from$the$irreversible$case,$we$find$that$the$conversion$after$t$
=$500$s$drops$down$from$99.9%$to$about$36%.$This$is$an$expected$result$as$the$reverse$reaction$also$
takes$place.$
$
P6–1)(e))Example)6-4$
P6–1)(f))Example)6-5)
Individualized$solution$
$
)
P6–2)The$key$for$decoding$the$algorithm$to$arrive$at$a$numerical$score$for$the$Interaction$Computer$
Games$(ICGs)$is$given$at$the$front$of$this$Solutions$Manual.$
)
P6-3$
Polymath$
d(Cb) / d(t) = rb
Cb(0) = 2
d(Ca) / d(t) = ra
Ca(0) = 2
6-11$
P6-3)Continued$
At$50$mins:$X$=$0.82$
At$100$mins:$X$=$0.9$
For$reactor$1:$
$
$
$
For$reactor$2:$
$
Therefore$the$design$equation$and$concentration$profiles$are$the$same$as$in$part$a)$for$the$two$reactors.$
As$they$have$the$same$concentration$profile$at$any$time,$the$conversions$are$the$same$for$the$two$
reactors$as$in$part$a).$$
At$10$mins:$X$=$0.47,$Ca$=$Cb$=$1.06$mol/dm3,$Cc$=$0.94$mol/dm3.$
At$50$mins:$X$=$0.82$
$
6-12$
P6–4)(a)$
$
P6–4)(b)$
$$$$ $
)
P6-5)
$
$
6-13$
P6-5)Continued$
$
Using$Polymath$to$solve$the$differential$equation$gives$a$volume$of$290$dm3$
See$Polymath$program$P6-5-c.pol.$
PFR$with$pressure$drop:$Alter$the$Polymath$equations$from$part$(c).$
See$Polymath$program$P6-5-c-pressure.pol.$
$
$
$
P6–5)continued$
Calculated)values)of)the)DEQ)variables$
Variable initial value minimal value maximal value final value$
v 0 0 500 500 $
ODE)Report)(STIFF)$
Differential equations as entered by the user$
[1] d(x)/d(v) = –r/fo$
Explicit equations as entered by the user$
[1] Kc = .025$
[2] alfa = 0.001$
[3] Cao = 0.3$