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12–81$
P12–16)(i))continued$
See$Polymath$program$P12–16–i.pol.$
$
$
P12–16)(j)$
Lowing$T0$or$Ta$or$increasing$UA$will$help$keep$the$reaction$running$at$the$lower$steady$state.$
$
)
P12-17$
TC$=$Ta$=$T0$$=$330$K$
$
See$Polymath$program$P12–18.pol.$
Calculated)values)of)DEQ)variables$$
12–82$
P12–17)continued$
Differential)equations$$
k$=$0.001*exp((E/1.987)*(1/300–1/T))$$
Kc$=$5000000*exp((DHrx/1.987)*(1/300–1/T))$$
X$=$tau*k/(1+tau*k$+$tau*k/Kc)$$
$
$
$
From)the)plot,)the)maximum)conversion)achieved,)Xmax)=)0.86$
At$Xmax,$T$=$367.6$K$and$G(T)$=$36100$cal/mol$
Therefore,)UA)=)(2.84)(10)mol/h)(250)cal/mol/K))=)7,100))cal/h/K$
$
12–83$
P12-18)
Note$p$=$y$
Adiabatic)$
Ordinary$Differential$Equations$
Calculated)values)of)DEQ)variables$$
$
Differential)equations$$
d(y)/d(W)$=$–alpha/2/y*(1+epsilon*X)*T/T0$$
d(T)/d(W)$=$(ra*(DH+deltaCp*(T–298))$-$Ua*(T–Ta))/Fa0/Cp0$$
d(Ta)/d(W)$=$Ua*(T–Ta)/m/Cpc$$
Ca$=$Ca0*(1–X)/(1+epsilon*X)*T/T0*y$$
Kc$=$10000*exp(DH/8.314*(1/450–1/T))$$
Cc$=$Ca0*X/2/(1+epsilon*X)*T0/T*y$$
k$=$0.01*exp(8000/8.314*(1/450–1/T))$$
12–84$
P12-18$(continued)$
$
Now,)constant)temperature)Ta)=)300K)
$
Ordinary$Differential$Equations$
Calculated)values)of)DEQ)variables$$
)
Differential)equations$$
d(y)/d(W)$=$–alpha/2/y*(1+epsilon*X)*T/T0$$
d(T)/d(W)$=$(ra*(DH+deltaCp*(T–298))$-$Ua*(T–Ta))/Fa0/Cp0$$
d(Ta)/d(W)$=$Ua*(T–Ta)/m/Cpc$*0$$
12–85$
P12-18)continued$
Explicit)equations$$
Ca$=$Ca0*(1–X)/(1+epsilon*X)*T/T0*y$$
Kc$=$10000*exp(DH/8.314*(1/450–1/T))$$
Cc$=$Ca0*X/2/(1+epsilon*X)*T0/T*y$$
k$=$0.01*exp(8000/8.314*(1/450–1/T))$$
$
Now,)Co–current)heat)exchanger)
Ordinary$Differential$Equations$
Calculated)values)of)DEQ)variables$$
$
Differential)equations$$
d(y)/d(W)$=$–alpha/2/y*(1+epsilon*X)*T/T0$$
d(T)/d(W)$=$(ra*(DH+deltaCp*(T–298))$-$Ua*(T–Ta))/Fa0/Cp0$$
d(Ta)/d(W)$=$Ua*(T–Ta)/m/Cpc$$
Ca$=$Ca0*(1–X)/(1+epsilon*X)*T/T0*y$$
Kc$=$10000*exp(DH/8.314*(1/450–1/T))$$
Cc$=$Ca0*X/2/(1+epsilon*X)*T0/T*y$$
k$=$0.01*exp(8000/8.314*(1/450–1/T))$$
12–87$
P12-18)continued$
$
$
Now,)counter)–)current)heat)exchanger$
$
Ordinary$Differential$Equations$
Calculated)values)of)DEQ)variables$$
$
1$$
d(X)/d(W)$=$–ra/Fa0$$
d(y)/d(W)$=$–alpha/2/y*(1+epsilon*X)*T/T0$$
d(T)/d(W)$=$(ra*(DH+deltaCp*(T–298))$-$Ua*(T–Ta))/Fa0/Cp0$$
d(Ta)/d(W)$=$-$Ua*(T–Ta)/m/Cpc$$
Ca$=$Ca0*(1–X)/(1+epsilon*X)*T/T0*y$$
Kc$=$10000*exp(DH/8.314*(1/450–1/T))$$
Cc$=$Ca0*X/2/(1+epsilon*X)*T0/T*y$$
k$=$0.01*exp(8000/8.314*(1/450–1/T))$$
12–89$
P12-18)continued$
$
$
$
$
P12–19)
No$solution$will$be$given.$
$
)
P12–20)(a))Figure$1$matches$Figure$_C_$
)
12–90$
P12-21$
First$note$that$ΔCP$=$0$for$both$reactions.$This$means$that$ΔHRx(T)$=$ΔHRx°$for$both$reactions.$
Now$start$with$the$differential$energy$balance$for$a$PFR:$
dT
dV =Ua(Ta−T)+rij (ΔHRxij )
∑
FjCPj
∑=Ua(Ta−T)+r
1A(ΔH1A)+r
2B(ΔHRx2B)
FjCPj
∑
$
If$we$evaluate$this$differential$equation$at$its$maximum$we$get$
r
1A=−
Ua(Ta−T)−2k2DCBCC(ΔHRx 2B)
(ΔHRx1A)
043.0
50000
)5000)(5.0)(2.0)(4.0(2)500325(10
1−=
−
−−
−=
A
r
r
1A=−0.043 =−1
2
k1CCACB=−1
2
k1C(0.1)(0.2)
k1C(500) =k1C(400) exp E
R
1
400 −1
500
“
#
$%
&
‘
(
)
*
*
+
,
–
–
4.3 =0.043exp E
1.987
1
400 −1
500
“
#
$%
&
‘
(
)
*
*
+
,
–
–
$
$
Alternate)Solution:$
$
12–91$
P12–21)continued$
)
P12-22!
!$
12–93$
P12–23)(a))continued$
$
12–95$
P12–23)(b)$continued$
$
$