Comparison of configurations of a four-column simulated moving bed
Comparison of configurations of a four-column simulated moving bed
Comparison of configurations of a four-column simulated moving bed
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<strong>Comparison</strong> <strong>of</strong> <strong>configurations</strong> <strong>of</strong> a <strong>four</strong>-<strong>column</strong><br />
<strong>simulated</strong> <strong>moving</strong> <strong>bed</strong> process by multi-objective<br />
optimization<br />
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Yoshiaki Kawajiri* and Lorenz T. Biegler<br />
Dept. <strong>of</strong> Chemical Engineering, Carnegie Mellon University, 5000 Forbes Ave.,<br />
Pittsburgh, PA, 15213<br />
*Corresponding author, Phone:(412) 268-2238, Fax: (412) 268-7139, E-mail:<br />
kawajiri@cmu.edu<br />
June 21, 2007<br />
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Abstract<br />
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Configurations <strong>of</strong> a <strong>four</strong>-<strong>column</strong> <strong>simulated</strong> <strong>moving</strong> <strong>bed</strong> chromatographic<br />
process are investigated by multi-objective optimization. Various existing <strong>column</strong><br />
<strong>configurations</strong> are compared through a multi-objective optimization problem.<br />
Furthermore, an approach based on an SMB superstructure is applied to<br />
find novel <strong>configurations</strong> which have been found to outperform the standard<br />
SMB configuration. An efficient numerical optimization technique is applied to<br />
the mathematical model <strong>of</strong> the SMB process. It has been confirmed that although<br />
the optimal configuration highly depends on the purity requirement, the<br />
superstructure approach is able to find the most efficient configuration without<br />
exploring various existing <strong>configurations</strong>.<br />
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1 Introduction<br />
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Chromatographic separation processes have been applied to many products for large-<br />
scale production. The most widely used operation mode is batch elution using a single
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<strong>column</strong>, where the feed mixture is loaded periodically and eluted with desorbent. In<br />
this mode, the purified products are collected at the end <strong>of</strong> the <strong>column</strong>. On the other<br />
hand, in the continuous mode, the feed can be continuously supplied and products<br />
can be continuously withdrawn. The representative system is the <strong>simulated</strong> <strong>moving</strong><br />
<strong>bed</strong> (SMB) process, where multiple <strong>column</strong>s are connected in a cycle, as shown in<br />
Figure 1. SMB mimics the countercurrent operation by intermittently switching the<br />
<strong>four</strong> streams, desorbent, extract, feed, and raffinate, in the direction <strong>of</strong> the liquid<br />
flow. Because <strong>of</strong> this continuous and pseudo-countercurrent operation mode, SMB<br />
has the potential to increase the productivity and reduce the desorbent consumption.<br />
However, numerical treatment <strong>of</strong> SMB processes comes with great difficulty because<br />
<strong>of</strong> the complex operation.<br />
In order to find efficient designs and operating parameters, various mathematical<br />
programming techniques have been applied to SMB. Dünnebier et al. (2000) and<br />
Toumi et al. (2002) have reported applications <strong>of</strong> sequential quadratic programming<br />
(SQP), a Newton-based nonlinear programming technique. In our previous study, we<br />
reported successful results <strong>of</strong> the full-discretization approach using an interior-point<br />
method for SMB processes (Kawajiri and Biegler, 2006d).<br />
In recent years, many modifications to the standard SMB have been attempted<br />
to further improve the performance. Fig.2(b) shows the Three-zone configuration<br />
(Ruthven and Ching, 1989; Ching et al., 1992), where the circulation from the right<br />
end to the left is cut and all liquid is withdrawn as the raffinate stream. Fig.2(c)<br />
shows the Three-zone configuration with purging, where the <strong>column</strong> at the left end<br />
is isolated and the components in the <strong>column</strong> are purged into the extract stream.<br />
As a result, the number <strong>of</strong> design alternatives for multi-<strong>column</strong> processes increases<br />
rapidly. However, only a few studies consider the <strong>column</strong> configuration <strong>of</strong> SMB.<br />
Zhang et al. (2002) used a genetic algorithm in their multi-objective optimization
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formulation. They investigated <strong>configurations</strong> <strong>of</strong> SMB with five <strong>column</strong>s. Ziomek<br />
et al. (2006) explored many different <strong>configurations</strong> <strong>of</strong> five identical <strong>column</strong>s. For<br />
this problem, we previously reported a superstructure based approach to find the<br />
optimal zone configuration and operation (Kawajiri and Biegler, 2006b). Although<br />
many novel <strong>configurations</strong> and operations have been found in previous studies, a<br />
systematic comparison <strong>of</strong> <strong>configurations</strong> has never been considered.<br />
In this work, we investigate extensively <strong>configurations</strong> <strong>of</strong> a <strong>four</strong>-<strong>column</strong> SMB.<br />
Various existing <strong>column</strong> <strong>configurations</strong> are compared through a multi-objective optimization<br />
study to analyze the trade-<strong>of</strong>f <strong>of</strong> throughput and desorbent consumption.<br />
The mathematical model is fully discretized and incorporated within a large-scale nonlinear<br />
programming (NLP) problem, which is solved using an interior-point solver,<br />
IPOPT (Wächter and Biegler, 2005). The superstructure approach, which em<strong>bed</strong>s<br />
many possible <strong>configurations</strong> such as Three-zone and standard SMB, is employed. A<br />
discussion <strong>of</strong> the standard and nonstandard <strong>column</strong> <strong>configurations</strong> is given in Section<br />
2. In Section 3, the mathematical model and superstructure approach are presented.<br />
Finally, standard and nonstandard <strong>configurations</strong> are compared with the superstructure<br />
approach in Section 4.<br />
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2 SMB <strong>column</strong> <strong>configurations</strong><br />
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In the standard SMB configuration, the <strong>column</strong> are connected in a cycle as shown<br />
in Figure 1. It is important to note that in a <strong>four</strong>-<strong>column</strong> process, there is only one<br />
standard configuration, where one <strong>column</strong> comes between every inlet/outlet streams.<br />
On the other hand, there are numerous non-standard <strong>configurations</strong>. One representative<br />
example is Three-zone (Figure 2(a)), where the circulation is cut <strong>of</strong>f and all<br />
liquid is withdrawn in the raffinate stream. This configuration consumes more des-
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orbent than the standard SMB configuration, since there is no recycle stream from<br />
the rightmost <strong>column</strong> to the leftmost <strong>column</strong>. Moreover, in Three-zone with purging<br />
(Figure 2(b)), the leftmost <strong>column</strong> is isolated and all components in the <strong>column</strong> are<br />
purged into the extract stream. This configuration is efficient if there is a component<br />
which has a high affinity to the adsorbent (slow <strong>moving</strong> component).<br />
Furthermore, in our previous study (Kawajiri and Biegler, 2006a), the F-shaped<br />
configuration was extracted from the SMB superstructure as the optimal <strong>column</strong><br />
configuration (Figure 2 (d)). This configuration has been found to have the highest<br />
throughput over other SMB <strong>configurations</strong> in our case studies <strong>of</strong> linear and nonlinear<br />
isotherms, but at the expense <strong>of</strong> higher desorbent consumption. This novel structure<br />
was an interesting finding; the desorbent stream is located downstream <strong>of</strong> the raffinate<br />
stream, and the recycle stream is cut <strong>of</strong>f. An analysis <strong>of</strong> this configuration is given in<br />
Section 4.<br />
It is also important to note that operations which involve multiple <strong>configurations</strong><br />
are possible. For instance, the operation <strong>of</strong> the Varicol system has multiple standard<br />
SMB <strong>configurations</strong> in one step. This feature can be generalized to operations<br />
which have multiple non-standard <strong>configurations</strong>. For this problem, we proposed a<br />
superstructure-based approach where the dynamic optimal configuration is obtained<br />
as a solution <strong>of</strong> an optimal control problem Kawajiri and Biegler (2006c). However,<br />
such dynamic <strong>configurations</strong> can be hard to implement in large-scale processes, since<br />
frequent changes <strong>of</strong> flow rates may lead to pressure instability. Therefore, investigations<br />
<strong>of</strong> operations <strong>of</strong> “static <strong>column</strong> configuration,” where the flow rates are kept<br />
constant in a step, also have significant importance.<br />
In the following section, we formulate a multi-objective optimization problem to<br />
compare the above-mentioned <strong>configurations</strong>. In this study, we only consider <strong>configurations</strong><br />
<strong>of</strong> <strong>four</strong>-<strong>column</strong> SMB. Discussion <strong>of</strong> SMBs with higher numbers <strong>of</strong> <strong>column</strong>s
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can be found in our previous studies Kawajiri and Biegler (2006b).<br />
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3 Mathematical Modeling and Problem Formula-<br />
tion<br />
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3.1 Modeling <strong>of</strong> Chromatographic Column<br />
For the modeling <strong>of</strong> each chromatographic <strong>column</strong>, the linear driving force (LDF)<br />
model is employed, as in our previous study (Kawajiri and Biegler, 2006d). Here<br />
both axial dispersion and diffusion into adsorbent particles, which cause band broadening,<br />
are lumped into a mass transfer coefficient. The validity <strong>of</strong> such an assumption<br />
can be found elsewhere (for example, Dünnebier and Klatt (2000); van Deemter et al.<br />
(1956); Golshan-Shirazi and Guiochon (2003)). The mass balance equations in the<br />
liquid and solid phases are given by:<br />
∂C j i (x, t)<br />
ǫ b<br />
∂t<br />
(1 − ǫ b ) ∂qj i (x, t)<br />
∂t<br />
+ (1 − ǫ b ) ∂qj i (x, t)<br />
∂t<br />
+ u j ∂Cj i (x, t)<br />
= 0 (1)<br />
∂x<br />
= K appl i (C j i (x, t) − Cj,eq i (x, t)) (2)<br />
The equilibrium between the liquid and solid phase is given by the linear isotherm:<br />
q j i (x, t) = f(Cj,eq i (x, t)) (3)<br />
Here ǫ b is the void fraction, C j i (x, t) is the concentration in the liquid phase <strong>of</strong> com-<br />
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ponent i in <strong>column</strong> j, q j i is the concentration in the solid phase, u j 105<br />
is the superficial<br />
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liquid velocity in the jth <strong>column</strong>, C j,eq<br />
i (x, t) is the equilibrium concentration in the<br />
liquid phase, q j,eq<br />
i<br />
is the equilibrium concentration in the solid phase, andK appl i is the
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liquid-phase based mass transfer coefficient, respectively. The subscripts i correspond<br />
to chemical components, superscript j is the <strong>column</strong> index, N c is the total number <strong>of</strong><br />
components, and N Column is the number <strong>of</strong> <strong>column</strong>s.<br />
At the CSS, the concentration pr<strong>of</strong>iles at the end <strong>of</strong> a cycle must be identical to<br />
those at the beginning <strong>of</strong> the cycle. The dynamics <strong>of</strong> the concentration pr<strong>of</strong>iles in<br />
the whole cycle need to be considered. However, the problem size can be reduced by<br />
taking advantage <strong>of</strong> the symmetry <strong>of</strong> the SMB operation. By enforcing the following<br />
constraints, the pr<strong>of</strong>iles at the end <strong>of</strong> the next step are required to be identical to those<br />
at the beginning <strong>of</strong> the current step, thus shifting the entire pr<strong>of</strong>iles downstream:<br />
C j i (x, 0) = Cj+1 i (x, t step ), j = 1, ..., N Column − 1 (4)<br />
q j i (x, 0) = qj+1 i (x, t step ), j = 1, ..., N Column − 1 (5)<br />
C N Column<br />
i (x, 0) = C 1 i (x, t step) (6)<br />
q N Column<br />
i (x, 0) = q 1 i (x, t step) (7)<br />
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3.2 Column <strong>configurations</strong> and SMB superstructure<br />
In this section, the <strong>configurations</strong> shown in Figure 2 are discussed. Note that these<br />
<strong>configurations</strong> can be extracted from the SMB superstructure shown in Figure 3.<br />
Referring to this figure, the following stream and <strong>column</strong> velocities are defined:<br />
u j , u j R , uj E , uj D , uj F ≥ 0, j = 1..N Column (8)<br />
where u j R , uj E<br />
are velocities <strong>of</strong> raffinate and extract withdrawn from jth <strong>column</strong>, and<br />
u j D and uj F<br />
are velocities <strong>of</strong> desorbent and feed supplied to jth <strong>column</strong>. Note that all<br />
velocities remain constant within each step. Furthermore, the volume and component
alance equations between the j − 1 th and j th <strong>column</strong>s are given by:<br />
u j−1 − u j−1<br />
E<br />
u N Column<br />
− u N Column<br />
E<br />
− uj−1 R + uj D + uj F = uj , j = 2, . . .N Column (9)<br />
− u N Column<br />
R<br />
+ u 1 D + u1 F = u1 (10)<br />
C j−1<br />
i (L, t)(u j−1 − u j−1<br />
E<br />
− uj−1 R ) + C F,iu j F = Cj i (0, t)uj , j = 2, . . .N Column<br />
(11)<br />
C N Column<br />
i (L, t)(u N Column<br />
− u N Column<br />
E<br />
− u N Column<br />
R<br />
) + C F,i u 1 F = C1 i (0, t)u1 (12)<br />
where C F,i is the concentration <strong>of</strong> component i in the feed. Further, in order to prevent<br />
draining the desorbent and feed into the product streams without going through a<br />
<strong>column</strong>, the following constraint is implemented:<br />
u j − u j D − uj F ≥ 0 j = 1, . . .,N Column (13)<br />
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If (13) is inactive, then the liquid from a <strong>column</strong> is transported to the next <strong>column</strong>.<br />
Otherwise, the circulation loop is cut open and all liquid is withdrawn in either or<br />
both <strong>of</strong> the product streams. We previously reported that this constraint is necessary<br />
not only to prevent undesirable operating parameters, but to ensure the robustness <strong>of</strong><br />
optimization (Kawajiri and Biegler, 2006a,c). Note that this superstructure em<strong>bed</strong>s a<br />
number <strong>of</strong> different non-standard <strong>configurations</strong> such as Three-zone, Three-zone with<br />
purging, and the standard SMB. Those <strong>configurations</strong> can be extracted by enforcing<br />
the flow constraints in Table 1.
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3.3 Optimization problem formulation<br />
In this study, we investigate the trade-<strong>of</strong>f <strong>of</strong> throughput maximization and desorbent<br />
minimization with fixed purity and recovery requirements by solving the following<br />
multi-objective optimization problem:<br />
(MOO) max ū F :=<br />
min ū D :=<br />
N Column<br />
∑<br />
j<br />
N Column<br />
∑<br />
j<br />
subject to : (1) − (13)<br />
(Extract Product Purity) =<br />
u j F<br />
(14)<br />
u j D<br />
(15)<br />
(Extract Product Recovery) =<br />
N Column ∑<br />
t step<br />
∫<br />
j=1 0<br />
N Column ∑ ∑Nc<br />
j=1<br />
N Column ∑<br />
i=1<br />
u j E (t)Cj E,Prod (t)dt<br />
t step<br />
∫<br />
0<br />
t step<br />
∫<br />
j=1 0<br />
N Column t<br />
∑ step<br />
∫<br />
j=1<br />
0<br />
u j E (t)Cj E,i (t)dt ≥ Pur min<br />
u j E (t)Cj E,Prod (t)dt<br />
(16)<br />
u j F (t)Cj F,Prod (t)dt ≥ Rec min<br />
(17)<br />
u l ≤ u j ≤ u u (18)<br />
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where t step is the valve switching interval, or step time, Pur min and Rec min are the<br />
purity and recovery requirements <strong>of</strong> the desired product which should be recovered<br />
in the extract stream, respectively. The desired product is denoted by the index<br />
Prod. u u and u l are the upper and lower bounds on the zone velocities, respectively.<br />
In addition, to examine the performance <strong>of</strong> the individual <strong>configurations</strong> shown in<br />
Figure 2, the constraints shown in Table 1 are enforced.
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3.4 Solution strategy<br />
The problem formulated in the previous section is a nonlinear multi-objective optimization<br />
problem. There have been many solution methods proposed for this type <strong>of</strong><br />
problem. For SMB optimization, Hakanen et al. (in press,s) used an interactive multiobjective<br />
optimization approach for SMB optimization with <strong>four</strong> objective functions,<br />
throughput, desorbent consumption, purity, and recovery. Their approach is useful<br />
when the number <strong>of</strong> objective function is large. Zhang et al. (2002) used a genetic<br />
algorithm for the zone configuration problem for a five-<strong>column</strong> SMB. In this study,<br />
however, the ǫ-constrained method based on a Newton-based numerical optimization<br />
approach is employed since there are only two objective functions. In this method,<br />
parameter ǫ p and the two objective functions <strong>of</strong> MOO (14)-(15) are reformulated into<br />
the following:<br />
maxū F (19)<br />
subject to : ū D ≤ ǫ p (20)<br />
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By changing the value <strong>of</strong> ǫ p and solving the above single-objective optimization problem<br />
repeatedly, the whole Pareto curve can be approximated. Although more computationally<br />
expensive than the interactive approach in Hakanen et al. (in press),<br />
this method allows us to compare the performance <strong>of</strong> different SMB <strong>configurations</strong><br />
by examining the entire Pareto curves.<br />
The resulting set <strong>of</strong> single-objective optimization problems is handled by the approach<br />
where the partial differential algebraic equations (PDAEs) are fully discretized<br />
both in the spatial and temporal domains using centered finite difference and Radau<br />
collocation on finite elements, respectively. Our previous study has found that this<br />
full-discretization approach significantly reduces the computational effort (Kawajiri
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and Biegler, 2006d). It is important to note that although the resulting NLP problem<br />
is large, the linear system to be solved in each iteration, i.e., the linearized Karush-<br />
Kuhn-Tucker (KKT) conditions, has a sparse structure and can be solved very quickly.<br />
To satisfy this requirement, we choose IPOPT, an interior-point solver with a filter<br />
line search method which exploits the sparse structure <strong>of</strong> linearized KKT conditions.<br />
Details <strong>of</strong> IPOPT can be found in Wächter and Biegler (2005).<br />
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4 Case study<br />
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4.1 <strong>Comparison</strong> <strong>of</strong> different <strong>configurations</strong><br />
For the numerical case study we consider the separation <strong>of</strong> fructose and glucose. The<br />
parameters in Hashimoto et al. (1983), where the equilibrium is linear, i.e.,<br />
q j i (x, t) = K iC j,eq<br />
i (x, t) (21)<br />
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are used in this study and are given in Table 2. Throughout this study, the number<br />
<strong>of</strong> finite elements in the temporal domain N FET and collocation points N COL are set<br />
to 5 and 3 respectively, and the number <strong>of</strong> finite elements N Column is set to 40 per<br />
<strong>column</strong>. Details <strong>of</strong> the accuracy <strong>of</strong> the discretization method and choice <strong>of</strong> numbers <strong>of</strong><br />
finite elements were determined in Kawajiri and Biegler (2006d). This optimization<br />
problem is implemented within the AMPL modeling environment (Fourer et al., 1992).<br />
It should be also noted that because the optimization problem is non-convex, our<br />
approach does not guarantee finding the global optimum. Therefore, we use several<br />
different starting points in order to avoid local optimal solutions. The starting points<br />
are obtained in the following manner: an initialization problem is solved where all operating<br />
parameters (u j ,u j R ,uj E ,uj F ,uj D ,t step) are fixed in a standard SMB configuration.
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Note that this initialization yields a set <strong>of</strong> linear equations which has no degrees <strong>of</strong><br />
freedom. It should also be noted that such a starting point satisfies all constraints <strong>of</strong><br />
the optimization problem except the purity and recovery requirements (16)-(17). Furthermore,<br />
multiple starting points can be easily obtained by changing the operating<br />
parameters arbitrarily and resolving the initialization problem.<br />
First, the throughput maximization problem (ǫ p = ∞ in (20)) is solved for each<br />
configuration. The result is summarized in Table 3. In all cases, the computational<br />
time takes only a few CPU minutes, which demonstrates the efficiency <strong>of</strong> our numerical<br />
optimization technique.<br />
The propagation <strong>of</strong> concentration pr<strong>of</strong>iles <strong>of</strong> the throughput maximization problem<br />
are compared in Figure 4. In the standard SMB configuration, concentrations <strong>of</strong> both<br />
<strong>of</strong> the faster and slower components are nearly zero at the right and left ends <strong>of</strong> the<br />
<strong>column</strong> train (Figure 4a). In other words, the faster component should not catch<br />
up with the slower component in order to achieve the purity and recovery demands.<br />
The optimizer finds such an operation because <strong>of</strong> the following reasons: Before the<br />
faster component reaches x = 8.0 in the rightmost <strong>column</strong>, switching must occur<br />
(the inlet and outlet streams are switched in the direction <strong>of</strong> the liquid flow) to<br />
avoid contaminating Zone I (leftmost <strong>column</strong>) by the faster component. At the same<br />
moment <strong>of</strong> switching, the concentration <strong>of</strong> the slower component at x = 0 must<br />
be nearly zero to avoid contaminating Zone IV (rightmost <strong>column</strong>) by the slower<br />
component. This “zone contamination” in Zones I/IV would lead to contamination<br />
<strong>of</strong> extract/raffinate by the faster/slower component.<br />
On the other hand, in the optimal concentration pr<strong>of</strong>iles <strong>of</strong> the Three-zone configuration<br />
shown in Figure 4b, the concentration <strong>of</strong> the faster component at the right<br />
end (x = 8.0) is significantly higher. However, this would not lead to contamination<br />
<strong>of</strong> the extract, since the recycle stream from x = 8.0 to x = 0 is cut <strong>of</strong>f. Therefore the
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internal concentration pr<strong>of</strong>iles can be higher, which leads to the higher throughput.<br />
It should be also noted that the desorbent consumption is higher because the recycle<br />
stream is cut <strong>of</strong>f.<br />
The throughput <strong>of</strong> the Three-zone with purging has the lowest throughput; this<br />
is because the leftmost <strong>column</strong>, where purging takes place, does not contribute to the<br />
separation effectively, as the concentrations remain nearly zero all the time (Figure<br />
4c). We note that this conclusion may not hold in cases where the Henry constant<br />
<strong>of</strong> the slower component K 2 is large and re<strong>moving</strong> the slower component from Zone<br />
I requires a higher amount <strong>of</strong> desorbent.<br />
Finally, note that the throughput <strong>of</strong> the F-shaped configuration is the highest.<br />
The propagation <strong>of</strong> the concentration pr<strong>of</strong>iles in the F-shaped configuration is shown<br />
in Figure 4d. This configuration allows such a situation where the slower component<br />
is “left behind” by the switching, and remains in the rightmost <strong>column</strong>. The resulting<br />
slower component left in the rightmost <strong>column</strong> is collected in the extract stream. This<br />
leads to further increase <strong>of</strong> throughput, since the concentration in the leftmost <strong>column</strong><br />
can be significantly higher.<br />
We note that the above comparison <strong>of</strong> <strong>configurations</strong> cannot be generalized to<br />
other systems, and it is not easy to determine the configuration that attains the<br />
highest throughput a priori (We will see this in the following case study where we<br />
consider different values <strong>of</strong> Pur min ). Here, an alternative approach is to use the SMB<br />
superstructure, which em<strong>bed</strong>s all possible <strong>configurations</strong> and extracts the optimal<br />
configuration. For Pur min = 95%, the optimal configuration extracted from the superstructure<br />
turns out to be the F-shaped configuration (Table 3). This configuration<br />
and optimal operating parameters can be found simultaneously in 2.87 CPU minutes.<br />
These <strong>configurations</strong> can be compared by changing ǫ p . Figure 5(a) shows the<br />
Pareto sets <strong>of</strong> different <strong>configurations</strong> with Pur min = 0.95. The solid line shows the
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Pareto set <strong>of</strong> the optimal solution <strong>of</strong> the superstructure formulation. As can be seen<br />
in the figure, it overlaps that <strong>of</strong> the standard SMB when the desorbent consumption is<br />
low. On the other hand, the part <strong>of</strong> the higher desorbent consumption overlaps that <strong>of</strong><br />
the F-shaped configuration. Also note that the Pareto curves <strong>of</strong> other <strong>configurations</strong>,<br />
Three-zone and Three-zone with purging, are below that <strong>of</strong> the superstructure. In<br />
the region <strong>of</strong> 1.5 ≤ ū D ≤ 3.0, however, none <strong>of</strong> the fixed <strong>configurations</strong> achieves the<br />
throughput <strong>of</strong> the superstructure solution; this optimal configuration is similar to the<br />
F-shaped configuration (Figure 6(a)) except that it has a recycle stream from x = 8<br />
to x = 0 in order to reduce desorbent consumption.<br />
Finally, the multi-objective optimization problem is solved for different values <strong>of</strong><br />
Pur min . In all cases, Pareto curve <strong>of</strong> the superstructure optimization becomes higher<br />
than those <strong>of</strong> other <strong>configurations</strong>. When Pur min = 0.90 (Figure 5b), the Pareto<br />
curves show a similar trend to those <strong>of</strong> Pur min = 0.95. The optimal configuration at<br />
ū D = 3.0 is shown in Figure 6 (b). However, when Pur min is decreased to 0.85 (Figure<br />
5c), the highest throughput is achieved by the Three-zone configuration at the expense<br />
<strong>of</strong> higher desorbent consumption. The optimal configuration and concentration pr<strong>of</strong>iles<br />
at ū D = 7.0 are shown in Figure 6(c). Finally, in the case <strong>of</strong> Pur min = 0.80, the<br />
F-shaped configuration never reaches the Pareto curve <strong>of</strong> the superstructure (Figure<br />
5d). Instead, the Three-zone with purging has the highest throughput at the highest<br />
desorbent consumption; this is closely followed by the Three-zone configuration with<br />
lower desorbent consumption. The optimal configuration at ū D = 5.0, shown in Figure<br />
6(d), is again similar to the F-shaped configuration, but the feed is supplied at<br />
x = 2.0 and the liquid is recycled from x = 8 to x = 0.<br />
From this multi-objective optimization study, we conclude that the optimal configuration<br />
is highly dependent on the purity specification, although the standard SMB<br />
configuration generally has good trade-<strong>of</strong>fs when desorbent consumption should be
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kept low. Nevertheless, our optimization approach using the SMB superstructure is<br />
able to find the most efficient configuration without exploring various <strong>configurations</strong>.<br />
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5 Conclusions and Future Work<br />
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Standard and nonstandard <strong>configurations</strong> <strong>of</strong> <strong>four</strong>-<strong>column</strong> SMB, under optimal operating<br />
conditions, have been compared through a case study. The optimal configuration<br />
is different depending on the purity requirement, throughput, and desorbent consumption.<br />
Here, we determined that although the standard SMB configuration has<br />
good trade-<strong>of</strong>fs when desorbent consumption is low, optimal configuration is highly<br />
dependent on the purity requirement. Nevertheless, our multi-objective optimization<br />
scheme using an SMB superstructure is able to find the optimal configuration<br />
efficiently without exploring various existing <strong>configurations</strong>. Also, our numerical optimization<br />
technique has been found to be efficient and reliable.<br />
Our future work will further extend our optimization approach to find optimal<br />
operating schemes for multi-component separations, where more than two components<br />
are fractionated into multiple streams. As our superstructure formulations em<strong>bed</strong> a<br />
number <strong>of</strong> both standard and nonstandard operating schemes, we aim to develop<br />
further efficient designs and operating schemes.<br />
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Acknowledgment<br />
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Funding from the National Science Foundation under Grant CTS-0314647 is gratefully<br />
acknowledged.
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Figure 1: Schematic diagram <strong>of</strong> 4 <strong>column</strong> SMB<br />
Figure 2: Examples <strong>of</strong> <strong>configurations</strong>: (a) standard SMB, (b) Three-zone (c) Threezone<br />
with purging (d) F-shaped.
Figure 3: SMB superstructure
Figure 4: <strong>Comparison</strong> <strong>of</strong> concentration pr<strong>of</strong>iles. Vertical dotted lines show the ports
Figure 5: Pareto curves
Figure 6: Configurations in Figure 5
Table 1: Configuration constraints<br />
Standard SMB 3-zone 3-zone purging F-Shaped<br />
u j D = 0, j ≠ 1 uj D = 0, j ≠ 1 uj D = 0, j ≠ 1, 2 uj D = 0, j ≠ 1<br />
u j F = 0, j ≠ 3 uj F = 0, j ≠ 3 uj F = 0, j ≠ 3 uj F = 0, j ≠ 3<br />
u j E = 0, j ≠ 1 uj E = 0, j ≠ 1 uj E = 0, j ≠ 1 uj E = 0, j ≠ 4<br />
u j R = 0, j ≠ 3 uj R = 0, j ≠ 4 uj R = 0, j ≠ 4 uj R = 0, j ≠ 3<br />
u 4 = u 4 R u 4 = u 4 R , u1 = u 1 E u 4 = u 4 E<br />
Table 2: Parameters <strong>of</strong> Fructose / glucose separation<br />
parameter value parameter value<br />
ǫ b 0.389 L [m] 2.0<br />
K 1 0.518 K appl 1 [1/s] 6.84 × 10 −3<br />
K 2 0.743 K appl 2 [1/s] 6.84 × 10 −3<br />
C F,1 [%] 50.0 C F,2 [%] 50.0<br />
u l [m/h] 0.0 u u [m/h] 8.0<br />
N Column 4 Rec min [%] 80.0<br />
N FET 5 N COL 3<br />
N FEX 40<br />
Table 3: Statistics <strong>of</strong> throughput maximization problem for Pur min = 0.95<br />
Objective function Φ Standard SMB 3-zone 3-zone purging F-Shaped Superstructure<br />
ū F [m/h] 0.410 0.521 0.344 0.737 0.737<br />
ū D [m/h] 1.199 4.836 2.083 4.669 4.669<br />
Extract purity [%] 95.0 95.0 95.0 95.0 95.0<br />
Extract recovery [%] 80.0 80.0 80.0 80.0 80.0<br />
Number <strong>of</strong> iterations 39 44 48 57 54<br />
CPU time [min] 1.76 1.65 1.87 3.12 2.87