polimerisation reactor
DESCRIPTION
ReactorTRANSCRIPT
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7.5. POLYMERISATION REACTOR
The methyl methacrylate (MMA) polymerisation takes place in a CSTR (see
Figure 27), using azo-iso-butyronitrile (AIBN) as initiator and toluene as sol-
vent. The reaction is exothermic, and a cooling jacket is used to remove the heat
of reaction (Silva et al. 2001).
The reaction mechanism ofMMA free radical polymerisation consists of the
following steps:
Initiation:
I!k0 2RRM!kI P1
Propagation:
Pi M!kp
Pi1
Monomer transfer:
Pi M!kfm
Pi DiAddition termination:
Pi Pj!ktc DijDisproportionation termination:
Pi Pj!ktd
Di Djwhere I, P, M, R and D refer to initiator, polymer, monomer, radicals and dead
polymer respectively.
[(Figure_7)TD$FIG]
FIGURE 27 Polymerisation reactor.
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7.5.1. Modelling Objective
The objective here is to develop a dynamic model so that the transient responses
of the compositions and the temperatures during the operation of the polymer-
isation reactor can be studied; existence of multiple solutions can be identified;
and closed-loop simulations performed by adding an appropriate control model.
7.5.2. Model Description
7.5.2.1 Model Assumptions
* The contents of the reactor are perfectly mixed.* Constant density and heat capacity of the reaction mixture.* Density and heat capacity of the cooling fluid stay constant.* Uniform cooling of fluid temperature.* The reactions only happen inside the reactor.* There is no gel effect (the conversion of monomer is low, and the proportion
of solvent in the reaction mixture is very high).* Constant volume of the reactor.* Polymerisation reactions occur according to the free radical mechanism.
7.5.2.2 Model Description
Based on the above assumptions, the mathematical model of the MMA poly-
merisation is given below.
Mass balance:
dCm
dt kp kfm
CmP0 F Cmin Cm
V42
dCI
dt kICI
FICIin FCI
V43
dD0
dt 0:5ktc ktd P20 kfmCmP0
FD0
V44
dD1
dt Mm kp kfm
CmP0 FD1
V45
Energy balance:
dT
dt DH kpCm
rCPP0 UA
rCPVT Tj F Tin T
V46
dTj
dt FCW TW0 Tj
V0
UArWCPWV0
T Tj 47
Chapter | 7 Models for Dynamic Applications 207
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Defined (constitutive) relations:
P0 2f *CIkI
ktd ktc
s48
kr AreEr=RT ; r p; f m; I; td; tc 49Defined polymer average molecular weight (Pm):
Pm D1=D0 50The percentage monomer conversion (X):
X Cmin Cm=Cmin*100 51
7.5.3. Model Analysis
The above mathematical model consists of a total of 14 equations out of which 6
are ODEs and 8 are algebraic equations (AEs). The 6 state (dependent) variables
for the 6 ODEs are: Cm, CI, T, D0, D1, Tj. The 8 algebraic (unknown) variables
for the 8 AEs are: k, P0, Pm, X (note that k is a vector of 5 variables). The rest of
the variables must be specified. Table 22 lists the variables that need to be
specified together with their specified values. Table 23 shows the incidence
matrix, which is not ordered in a lower tridiagonal form but it can easily be seen
that the algebraic equations have a lower tridiagonal form.
Based on the incidence matrix given in Table 23, the calculation procedure is
as follows: at any time, t, the values of the state (dependent) variables are known
TABLE 22 List of Specified Variables and their Given Values
F = 1.0 m3/h Mm = 100.12 kg/kgmol
FI = 0.0032 m3/h f* = 0.58
FCW = 0.1588 m3/h R = 8.314 kJ/kgmol K)
Cmin = 6.4678 kgmol/m3 -DH = 57800 kJ/kgmol
CIin = 8.0 kgmol/m3 Ep = 1.8283 104 kJ/kgmol
Tin = 350 K EI = 1.2877 105 kJ/kgmolTW0 = 293.2 K Efm = 7.4478 104 kJ/kgmolU = 720 kJ/(hkm2) Etc = 2.9442 103 kJ/kgmolA = 2.0 m2 Etd = 2.9442 103 kJ/kgmolV = 0.1 m3 Ap = 1.77 109 m3/(kgmoh)V0 = 0.02 m
3 AI = 3.792 1018 1/hr = 866 kg/m3 Afm = 1.0067 1015 m3/(kgmoh)rW = 1000 kg/m
3 Atc = 3.8283 1010 m3/(kgmoh)Cp =2.0 kJ/(kgK) Atd = 3.1457 1011 m3/(kgmoh)CpW = 4.2 kJ/(kgK)
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and so the AEs (Eq. 49 and then 48) are solved. Using these variables and the
known variables, the right-hand sides (RHSs) of ODES (Eqs. 4247) are deter-
mined, and based on these, new values of the dependent variables are obtained.
Equations 50-51 are used to calculate the polymer averagemolecular weight and
the percentage conversion at any time.
7.5.4. Numerical Solution
The model equations have been solved through ICAS-MoT (Sales-Cruz, 2006).
The calculated steady-state values for the state variables are given in Table 24. It
can be noted that this reactor has multiple steady states, which can be obtained
TABLE 23 Incidence Matrix (note that Eq 49 is actually five equations for the
vector k). The shaded Cells Indicate the ODEs and their Corresponding
Dependent Variables
Eq\Variable k P0 Cm CI D0 DI T Tj Pm X
Eq. 49 * *
Eq. 48 * * *
Eq. 42 * * *
Eq. 43 * *
Eq. 44 * * * *
Eq. 45 * * * *
Eq. 46 * * * * *
Eq. 47 * *
Eq. 50 * * *
Eq. 51 * *
TABLE 24 Calculated Steady-State Values for the MMA Polymerisation
Reactor
State 1 State 2 State 3
Cm, kgmol/m3 5.9651 5.8897 2.3636
CI, kgmol/m3 0.0249 0.0247 1.7661 10-04
T, K 351.41 353.40 436.20
D0, kgmol/m3 0.0020 0.0025 0.4213
D1, kgmol/m3 50.329 57.881 410.91
Tj, K 332.99 334.34 390.93
X, % 7.8 8.9 63.5
PM, kg/kgmol 25000 23000 975
Chapter | 7 Models for Dynamic Applications 209
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by starting the dynamic simulation runs from different initial conditions but
keeping all the known variables at the listed values of Table 22. This is an
example of output multiplicity. The transient responses for the 6 state variables
are shown in Figures 28a-f. These results are obtained for the following initial
conditions of the state variables: Cm = 0 ; CI = 0.5 ;T = 200 ; D0 = 0 ; D1 = 0; Tj=0. This corresponds to steady state 1 in Table 24.
[(Figure_8b)TD$FIG]
FIGURE 28b Transient response of Cm (y-axis) versus time (x-axis).
[(Figure_8a)TD$FIG]
FIGURE 28a Transient response of CI (y-axis) versus time (x-axis).
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[(Figure_8d)TD$FIG]
FIGURE 28d Transient response of DI (y-axis) versus time (x-axis).
[(Figure_8c)TD$FIG]
FIGURE 28c Transient response of D0 (y-axis) versus time (x-axis).
[(Figure_8e)TD$FIG]
FIGURE 28e Transient response of T (y-axis) versus time (x-axis).
Chapter | 7 Models for Dynamic Applications 211
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The model equations as implemented in ICAS-MoTare given in Appendix 1
(see chapter-7-5-poly-reactor.mot file).
Discussion: Try to obtain all the three steady states and evaluate their
stability through calculating the eigenvalues. Add the gel-effect to evaluate
the changes in the transient responses. A more detailed polymerisation reactor
model is given by Lopez-Arenas et al. (2006) try to implement this model.
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[(Figure_8f)TD$FIG]
FIGURE 28f Transient response of Tj (y-axis) versus time (x-axis).
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