Clean Technologies and Environmental Policy

, Volume 10, Issue 3, pp 245–254 | Cite as

New processes for recovery of acetic acid from waste water

  • Jignesh Gangadwala
  • Gabriel Radulescu
  • Achim Kienle
  • Frank Steyer
  • Kai Sundmacher
Open Access
Original Paper


This paper addresses an industrially important problem of acetic acid recovery from a waste water stream via reactive distillation. The presence of a three-phase regime on the column stages due to a liquid–liquid phase split between aqueous and organic phases is a typical characteristic of this process. A modern modeling approach is presented to detect the existence of potential phase splitting in this column. A good agreement of a phase splitting model with the literature data has been shown. A theoretical study for the recovery of acetic acid from its 30 wt% aqueous solution by esterification with n-butanol is presented. Alternate column structures were investigated and two structures rendering theoretically close to 100% conversion of acetic acid were identified. The dynamic simulations were performed on proposed structures to see transient responses wrt. to common process disturbances.


Phase splitting Homotopy continuation Reactive distillation Modeling and dynamic simulation Butyl acetate Esterification Acetic acid recovery 

List of symbols


Molar liquid holdup on tray


Jacobian matrix


Number of components


Reaction ratio




Volumetric liquid holdup on tray


Function vector to be solved to 0


Vapor sidedraw molar flowrate


External vapor feed molar flowrate


Liquid sidedraw molar flowrate


External liquid feed molar flowrate


Internal liquid molar flowrate




Saturation pressure in the vapor phase


Internal vapor molar flowrate

x, x1, x2

Mole fraction, liquid (global, phase 1, phase 2)


Mole fraction, vapor phase


Mole fraction in external liquid feed


Mole fraction in external vapor feed

Greek letters

Φ (or Fi)

Phase ratio

γ1, γ2

Activity coefficient (phase 1, phase 2)


Solution vector


Continuation parameter


Stoichiometric coefficient



Critical point of the miscibility gap


Value given by the Phase Splitting Algorithm


Reference state (starting point for continuation)


A, B, C

Example states in the phase diagram


Tray number


Component indices


Variable indices (in the solution vector)


Current step


The recovery of dilute acetic acid from its aqueous stream is a major concern for many petrochemical and fine chemical industries. Conventional distillation is highly uneconomical due to (a) the presence of a tangent pinch on the water end in the yx diagram, that means high reflux ratio or high number of column stages to get pure products; and (b) large amount of water to be vaporized from dilute acid stream, which is impractical due to the high latent heat of vaporization of water. Recently, more advanced concepts based on azeotropic and extractive distillation have been proposed (Chien et al. 2004; Demiral and Yildirim 2003). Another very promising option is reactive distillation, where acetic acid is reacted off with a suitable alcohol in order to produce a valuable ester product at the one end of the column and the aqueous stream free of organic impurities at the other end of the column. In particular, esterification with n-butanol was proposed for this purpose (Saha et al. 2000). In that work, however, by trial and error experiments a maximum of up to 58% acetic acid conversion was achieved with a 100% excess of butanol in feed. In the present paper, using a model based approach, it can be observed that conversion close to 100% is possible for such a process.

Figure 1 shows a typical RD column for the acetic acid recovery process. The interesting feature of this process is the potential phase split that can occur on many trays inside the column. To reliably predict the liquid–liquid phase split on the column trays in the course of a simulation run, an extra routine for the phase split calculations is required. The routine is based on homotopy continuation methods (Bausa and Marquardt 2000; Brüggemann et al. 2004; Steyer et al. 2005). The complexity introduced by the liquid–liquid phase split besides the existing complexity of a reaction–separation interaction makes the analysis of this process very challenging.
Fig. 1

A typical RD column for acid recovery: a double question mark indicates that many distinct arrangements are possible, for example, considering the feed tray(s), reflux stream(s), product stream, reaction zone, etc. Apart from that potential liquid–liquid phase split may occur on some column stages

The article is organized in the following way: first an appropriate model is presented that carries out the simultaneous phase split calculations for a reactive distillation column. Model results showing very good agreement with literature data are presented afterwards. The phase split routine is used to design a heterogeneously catalyzed reactive distillation column for the acetic acid recovery process. Steady state simulation results are presented for six alternate configurations generated based on physical insights. After the process screening based on the conversion levels, two process configurations are proposed. Next, dynamic simulation results are presented. At the end, conclusions and future directions are discussed.

Mathematical model

The classical approach treats the RD process as a pseudo-homogeneous system, where no phase splitting occurs in the liquid phase (Sundmacher and Kienle 2002; Taylor and Krishna 2000). However, for some systems, significant differences between states in the pseudo-homogeneous regime (no liquid phase splitting) and heterogeneous regime (with phase splitting) can be revealed (Bausa and Marquardt 2000; Brüggemann et al. 2004). As consequence, an appropriate model has to be used in order to better reflect the real system behavior. However, dynamic simulation of a (reactive) distillation column taking into account the potential appearance of a second liquid phase is a much more difficult task. The main challenge is to write a model, which switches between two model structures during the course of a simulation run. The switching is required when changes in the phase state on some trays occur. The model switching can be handled by considering that always there are two liquid phases present in the model and when the system leaves the heterogeneous regime, these two phases become identical having the same compositions. This way, there is no need to change the number of model equations when the system crosses the boundary between the homogeneous and heterogeneous region.

In this work, in order to improve the simulation robustness, a structural modeling approach was adopted, which consists of two sections:
  • the main model, relatively close to the “classical” RD model (without phase splitting), which calculates at each step the global composition in liquid (x) and vapor (y) phases, temperature (T), internal liquid (liq) and vapor (vap) streams flowrates, for all distillation stages (column trays and condenser + decanter);

  • the phase splitting algorithm, externally carried out in a separate procedure, called by the main model at each step, for all distillation stages; this algorithm gets from the main model the global compositions (x) and temperatures (T), together with some other parameters, giving back both liquid phases compositions (x1 and x2) and ratios (Φ).

Main model

The model assumptions are presented in the following. For a model validation section, a homogeneously catalyzed batch reactive distillation column model without energy balance; and for steady state and dynamic simulations, a continuous heterogeneously catalyzed reactive distillation column model with energy balances have been used. While the particular assumptions need to be presented for each specific case, the general ones are always valid:
  1. 1.

    All column trays and the decanter have constant liquid holdups.

  2. 2.

    The vapor holdup on trays is neglected.

  3. 3.

    The vapor and liquid phases are in equilibrium.

  4. 4.

    The reaction takes place only in the liquid phases.

  5. 5.

    The pressure drop along the column length was neglected.

Here as example, the simple case of kth regular tray inside the column (as shown in Fig. 2), for a homogeneously catalyzed process, with perfectly mixed reactants and catalyst, without considering the energy balance, is presented. The regular equations are:
Fig. 2

The kth tray inside RD column

Component material balance:
$$ \begin{aligned} {\rm HOLD}_k \frac{{{\rm d}x_{i,k}}} {{{\rm d}t}} & = {{\rm liq}_{k - 1}} \times x_{i,k - 1} + {{\rm vap}_{k + 1}} \times y_{i,k + 1} - {{\rm liq}_k} \times x_{i,k} - {{\rm vap}_k} \times y_{i,k} + {{\rm flzu}_k} \times {{\rm zflzu}_{i,k}} + {{\rm fgzu}_k} \times {{\rm zfgzu}_{i,k}} - {{\rm flab}_k} \times x_k - {{\rm fgab}_k} \times y_k + \nu _i \times \left[{\left({1 - \Phi _k} \right) \times R\left({x1_{1,k}, \ldots,x1_{{\rm NC},k}} \right) + \Phi _k \times R\left({x2_{1,k}, \ldots,x2_{{\rm NC},k}} \right)} \right] \times V_k \\ & \quad \quad i=1,\ldots,{\rm NC}-1. \\ \end{aligned} $$
It can be seen that a global reaction rate R is considered as the linear combination between the reaction rate in phase 1 and the reaction rate in phase 2, taking into account the phase split ratio Φ k . If the liquid phase splitting does not occur, then the compositions in both phases are equal and the reaction rates are identical. As remark, such a linear expression \([(1- \Phi_{k}) \times R(x1_{1,k},\ldots,x1_{{\rm NC},k}) + \Phi_{k} R(x2_{1,k},\ldots,x2_{{\rm NC},k})]\) can only be used when the uniform catalyst distribution in both liquid phases is considered.
Summation condition for global liquid phase compositions:
$${\sum\limits_{j = 1}^{\rm NC} {x_{{j,k}} = 1}}.$$
Compositions in liquid phase 1 (externally calculated):
$$x1_{{i,k}} = x1^{{\rm PSA}}_{{i,k}}, \quad i=1,\ldots,{\rm NC}.$$
In this equation, x1PSA k,i represents the phase 1 composition, externally determined with the “Phase Splitting Algorithm”. The same annotation, PSA, is attached for compositions in liquid phase 2 and phase ratio, also given by the same procedure:
Compositions in liquid phase 2(externally calculated):
$$x2_{{i,k}} = x2^{{\rm PSA}}_{{i,k}}, \quad i=1,\ldots,{\rm NC}.$$
Phase ratio (externally calculated):
$$\Phi _{k} = \Phi ^{{\rm PSA}}_{k}.$$
Phase equilibrium:
$$y_{{i,k}} \times p = {\rm psp}_{i} \times \gamma 1_{{i,k}} \times x1_{{i,k}}, \quad i=1,\ldots,{\rm NC}.$$
Summation condition for vapor phase compositions:
$${\sum\limits_{j = 1}^{\rm NC} {y_{{j,k}} = 1}}.$$
Total material balance for the liquid phase:
$$\begin{aligned}& 0 = {{\rm liq}_{{k - 1}}} - {{\rm liq}_{k}} + {{\rm flzu}_{k}} - {{\rm flab}_{k}} + {\sum\limits_{j = 1}^{\rm NC} {{\left[{\nu _{j} \times {\left[{{\left({1 - \Phi _{k}} \right)} \times R{\left({x1_{{1,k}}, \ldots,x1_{{\rm NC,k}}} \right)} + \Phi _{k} \times R{\left({x2_{{1,k}}, \ldots,x2_{{\rm NC,k}}} \right)}} \right]} \times V_{k}} \right].}}} \\ \end{aligned}$$
Total material balance for the vapor phase:
$${{\rm vap}_{k}} = {{\rm vap}_{{k + 1}}}.$$
The models for the column top (condenser + decanter) and bottom (including the reboiler) are also based on the “core” equations above, with usual changes available in the literature describing these slightly modified structures.

The model to be used later for steady state and dynamic simulations as said before is a heterogeneously catalyzed reactive disitllation column model with energy balances. This model has two major changes: (1) For the global reaction rate calulcation the phase split ratio has not to be taken into account and the assumption of a uniform catalyst distribution is not required. The reason for this is that the reaction rate is based on activities rather than mole fractions and that phase equilibrium implies equal activities in both liquid phases. (2) An energy balance replaces Eq. 9 and Eq. 8 has to be replaced by a total material balance for the liquid and vapor phases.

Phase splitting algorithm

As mentioned before, the phase splitting algorithm runs almost independently, checking at each step the state of all distillation stages and returning to the main model the phases compositions and ratios. Of course, before running, it takes some mandatory information from the main model, including overall compositions, stages temperatures and other needed parameters (i.e., for the vapor–liquid (–liquid) equilibrium calculation, also some algorithm “tuning parameters”—as starting points for the internal continuation algorithm, for instance—and so on).

The phase splitting algorithm used in this work was originally presented by Bausa and Marquardt (2000) and subsequently modified by Steyer et al. (2005). It is a hybrid method using a-priori knowledge of phase diagram properties in order to tune-up the computational algorithm. The flash calculation is decomposed in two steps: a preprocessing step and the computational one.

In the first step, all heterogeneous regions of the system’s phase diagram at the specified pressure and boiling temperature are divided into convex regions and, for each region, one reference state inside it, (x START, x1START, x2START, y START, ΦSTART, p START, T START), is stored—denoting here the overall composition, compositions in both liquid phases, vapor composition, phase ratio, pressure and temperature. Typically, this analyzing procedure may be carried out only once, before simulations and more, since the phase diagrams are investigated in an early phase of the process design, the information on the heterogeneous region(s) existence may be directly provided by user (at least for mixture with up to four components).

In the next step, homotopy continuation is carried out starting at the known solution (x START, x1START, x2START and ΦSTART) and ending at a desired two phase solution (x, x1, x2 and Φ) if it exists. The homotopy run can be parameterized by a continuation parameter λ in the following manner:
$$\bar{x}_{i} = \lambda \times x_{i} + (1 - \lambda) \times x^{{\rm START}}_{i} = \bar{x}_{i} (\lambda), \quad i=1,\ldots,{\rm NC}.$$
λ is changed from 0 to 1 when the continuation is performed. It can be observed that \(\bar{x}_{i} (0) = x^{{\rm START}}_{i}\) and \(\bar{x}_{i} (1) = x_{i}.\)

On its turn, the homotopy continuation algorithm is based on a repetitive two-step process. First one, the correction step, solves the following equations:

Mass balances (as constraints):
$$x1_{i} \times (1 - \Phi) + x2_{i} \times \Phi = \bar{x}_{i} (\lambda), \quad i=1,\ldots,{\rm NC},$$
Activity difference equations (as necessary conditions):
$$x1_{i} \times \gamma 1_{i} - x2_{i} \times \gamma 2_{i} = 0, \quad i=1,\ldots,{\rm NC},$$
and The summation equation (as constraint):
$$1 - {\sum\limits_{i = 1}^{\rm NC} {x1_{i} = 0}}\quad \left(\hbox{or } 1 - {\sum\limits_{i = 1}^{\rm NC} {x2_{i} = 0}}\right).$$
The above equations are written for the global composition \(\bar{x}\) at a particular value for λ. A remark regarding the annotations: no tray index “k” is provided, in order to increase the readability.
In the second step (predictor step), a solution θ to Eqs. (11)–(13) for a new value of λ is estimated using
$$\theta _{{m,s + 1}} = \theta _{{m,s}} + \Delta \theta _{m} = \theta _{{m,s}} + \frac{{\rm d}\theta _{m}}{{\rm d}\lambda}\Delta \lambda, \quad m=1,\ldots,2{\rm NC}+1,$$
θ m denoting an element of the solution vector. For the algorithm of Bausa and Marquardt (2000), θ contains 2NC mole fractions (x1 and x2) and one phase ratio (Φ).

The algorithm works by alternating prediction and correction steps while increasing λ from 0 to 1, effectively moving along the binodal surface in an effort to reach the desired x composition.

In systems with multiple binary pairs that exhibit phase splitting, multiple starting points for continuation have to be used in order to reach the correct solution (Bausa and Marquardt 2000). This is due to the fact that the straight line according to Eq. (10) connecting the starting point x START with the desired composition x might cross over a region of one-phase behavior between the two-phase starting and ending points. As Bausa and Marquardt show in their paper, this approach is very successful in finding the correct solution very quickly, with a high reliability.

However, their original implementation has a big drawback: the solution vector θ has 2NC + 1 components even if the system degree of freedom is NC!, increasing this way the computational time for the solver. This is why a modified method, developed by Steyer et al. (2005) was used. The method’s principle is to parameterize the solution vector θ by introducing so-called phase partitioning coefficients, reducing the system order to NC, as the quoted authors proved in their work.

The correction step is based on Newton iteration, where the following equation system has to be solved:
$$\theta _{{s + 1}} = \theta _{s} - J^{{- 1}} (f(\theta _{s})) \times f(\theta _{s}).$$
In this equation, J denotes the Jacobian matrix of the remaining equation system (after model reduction), denoted here as f. To avoid inverting the Jacobian matrix, the equivalent linear equation system has to be solved. Also, for a fast and reliable solution, the authors suggest that the Jacobian should be computed analytically since the equation system is highly non-linear due to the activity coefficient model.

Model validation

Due to the lack of comprehensive experimental data, the model is validated by reproducing the results of Brüggemann et al. (2004). Brüggemann et al. have studied a batch distillation process in the heterogeneous regime, taking as example the laboratory column for butanol esterification to butyl acetate, previously presented by Venimadhavan et al. (1999).

In particular, following operating scenarios were considered:
  1. 1.

    ternary non-reactive distillation (loading the column still pot with a mixture of 40% water, 20% butanol and 40% butyl acetate, with no catalyst load), at a constant reflux ratio (0.9);

  2. 2.

    reactive distillation (filling the still pot with a binary mixture of 51% butanol and 49% acetic acid), homogeneously catalyzed with sulfuric acid, at a constant reflux ratio (0.9);

  3. 3.

    reactive distillation (filling the still pot with a binary mixture of 51% butanol and 49% acetic acid), homogeneously catalyzed with sulfuric acid, at a variable-adaptive reflux ratio (0.9 and 0.99).

In order to reproduce those scenarios, the model presented in this work was adapted for a 33 stage batch column, including the condenser + decanter and the still pot (with internal reboiler). At top, the external reflux (from decanter) comes on the first column tray. The holdup on each tray is 0.001 kmol, the combined holdup of the condenser and decanter is 0.01 kmol and the initial holdup of the still pot is 2 kmol. Also, a constant vapor flowrate of 2 kmol/h from the reboiler is considered. To maintain the consistency with Brüggemann’s work, the thermodynamic data and reaction kinetics were taken from Venimadhavan et al. (1999).
All three operating strategies were investigated with our model implementation, but due to the lack of space only the results for the first one are here covered. Figures 3 and 4 depict the global composition in the decanter and the reboiler, respectively. On the left, the simulation time SIM_TIME is expressed in (s × 104), on the right, t is in (h). The right hand side picture is taken from Brüggemann et al. (2004).
Fig. 3

Comparison between our model results (left) and literature results (right),—global composition in decanter

Fig. 4

Comparison between our model results (left) and literature results (right)—global composition in still pot

For a homogeneously catalyzed RD column the phase split algorithm precisely detects the existence of two liquid phases. In the remainder, a heterogeneously catalyzed process will be considered.

Alternate designs for acetic acid recovery by RD column

The above-validated phase split routine is combined with a heterogeneously catalyzed continuous reactive distillation column model from Gangadwala et al. (2004) to design the acetic acid recovery process. In this section we present a few possible column configurations for the recovery process. Some of these configurations are based on the work by Saha et al. (2000). Configurations 1–6 shown in Fig. 5 are obtained by changing the locations of aqueous and organic reflux from the decanter. For example, configuration 1 has no aqueous reflux and a total organic reflux is positioned at the top; configuration 2 on the other hand has no organic reflux and a total aqueous reflux is positioned at the top; configuration 3 has a total organic reflux and partial aqueous reflux at the top; configuration 4 has a partial organic and aqueous reflux; configuration 5 has a total aqueous reflux positioned at the reboiler and a partial organic reflux positioned at the top; and finally configuration 6 has reflux features similar to configuration 5 but the feed is introduced into two parts, i.e., dilute acetic acid feed at the top of the reaction zone and the pure alcohol feed at the bottom of the reaction zone. Obviously many other process variations are viable. The intention, here, is not to cover all the possible configurations rather to show the challenge involved in fixing these discrete decision variables in such a process. Note that by changing the positions of the reflux streams, the complete reversions of the product streams are possible. For example, configuration 1 has an aqueous stream as distillate and an organic stream containing butanol and butyl acetate as bottoms. The reverse is true for configuration 6, where an aqueous stream is obtained at the bottom and an organic stream is obtained as distillate.
Fig. 5

Different process alternatives based on different combinations of design variables

Its required to test for all the design alternatives, whether they are feasible to achieve the desired process goal. The desired goal in this work is to achieve a very high conversion of acetic acid (>99%). Not all the configurations will lead to the high conversion of acetic acid to butyl acetate. In order to check whether the configurations 1–6 achieve 99% conversion, ideally all of them have to be tested with various sets of design parameters in the entire solution space. In fact, this can be seen as an optimization problem with conversion of acetic acid set as a constraint or as a cost function to be maximized. The phase split routine to be used for the phase split detection on the column stages, however, does not allow the use of standard optimization tools. It was therefore necessary to use a simulation environment for this purpose. Designing all the configurations with a simulation tool is a tedious procedure. Through simulations we carried out limited feasibility tests for configurations 1–6. It has been found that configurations 1 and 6 can achieve the above desired goal. However, for configurations 2–5 no feasible solution was found.

Characteristic simulation results of different configurations of Fig. 5 in a liquid–liquid phase split regime are presented in Table 2. The feed compositions and feed flow rate are shown in Table 1. The molar ratio of butanol to acetic acid in the feed was considered to be 2:1, as recommended by Saha et al. Though it will be interesting to study the effect of the molar ratio in the feed, this is beyond the scope of the paper and will be considered in a separate work. As can be seen from the Table 2, configurations 1 and 6 achieve 99% conversion, configuration 5 achieves 92% conversion and very little conversion levels are achieved by the other configurations. Due to numerical difficulties for configuration 4 no steady state solution could be obtained. The other configurational details like number of column stages, reaction zone locations, feed stage locations, catalyst loading and reboiler duty requirement are also presented in Table 2. Configurations 1 and 6 require nearly the same reboiler heat duty to achieve 99% conversion. The steady state composition profiles and profiles of the phase split ratio for configuration 1 and 6 can be seen from Figs. 6a–c and 8a–c, respectively, as a start point for the dynamic simulation results.
Fig. 6

Transient response for configuration 1 to a 5% increase in the feed flow rate: a BuAc profile b H2O profile c phase fraction and d AcH conversion. (Lightest gray line is a base case steady state with 99% AcH conversion; intermediate gray lines show transient states and darkest gray line shows a final steady state)

Table 1

Feed composition (mole fraction), BuOH:AcH is 2:1


Configurations 1–5

Configuration 6

Feed I

Feed II

Feed (kmol/h)












X BuAc












Table 2

Configurational details







AcH conversion (%)






Reboiler duty (kW)






Catalyst (kg/tray)






Reactive stages






Column stages






Feed tray location





9 and 21

Though configuration 1 and configuration 6 having very different column structures and reverse product streams, both are capable of providing close to 100% conversion of acetic acid. Configuration 1 yields 99% aqueous stream as a distillate and nearly a 50–50 mixture of butanol and butyl acetate as the bottoms. Downstream processing is required to separate the two organics. Configuration 6 yields a 98% water stream at the bottom and an organic stream containing 44% BuAc, 26% BuOH and 24% water is obtained as a distillate. Significant amount of side product di-butyl ether is also present in the distillate stream. Here again a downstream processing step is required to produce a high purity acetate stream.

Dynamic simulations for the proposed configurations

In this section, dynamic simulation results are presented for the base case steady states with 99% conversion for configurations 1 and 6. Process responses are determined for ±5% step disturbances of the feed flow rate and the AcH composition in the feed.

Configuration 1

The composition profiles show a very high sensitivity to the disturbances for configuration 1, as shown in Fig. 6. For instance, with an increase of 5% in feed flowrate, these profiles move like a traveling wave down in the stripping section leading to a serious drop in acetic acid conversion (from 99 to 38%, see Fig. 6d). The system moves toward a new steady state with totally different composition profiles in the reactive zone. As it can be seen in Fig. 6a and b, the non-reactive zone above the feed tray remains unaffected. Fig. 6c shows how the three-phase regime extends from a small region around the feed tray to about 75% of the reactive zone, without any effect in the upper part of the column.

A similar sensitivity was observed when feed flowrate was decreased by 5%. The composition waves moved in a rectifying zone and the three-phase regime observed to shrunken. At the new steady state conversion of acetic acid slightly increases as shown in Fig. 7a. Figures 7b and c show the transient responses of acetic acid conversion when acetic acid composition in feed was decreased and increased by 5 mole%, respectively.
Fig. 7

Transient response of acetic acid conversion for configuration 1: a 5% decrease in feed flow; b 5% decrease in acetic acid composition in feed and c 5% increase in acetic acid composition in feed

Configuration 6

For configuration 6, less sensitivity to disturbances is observed compared to configuration 1. For instance, for an increase of 5% of both feed flow rates, the composition profiles, Fig. 8a and b, did not differ significantly from the base case steady state profiles. The three-phase regime and conversion level also found to be stable to the disturbance as shown in Fig. 8c and d. The transient responses to the other disturbances, viz. decrease of 5% in acid feed and butanol feed; increase and decrease of 5 mole% acid composition in acid feed also shows stable conversion levels (see Fig. 9a–c).
Fig. 8

Transient response for configuration 6 to 5% increase of both feed flow rates: a BuAc profile b H2O profile c phase fraction and d AcH conversion. (Lightest gray line is a base case steady state with 99% AcH conversion; intermediate gray lines show transient states and darkest gray line shows a final steady state)

Fig. 9

Transient response of acetic acid conversion for configuration 1: a 5% decrease in both the feed flow rates; b 5% decrease in acetic acid composition in acid feed and c 5% increase in acetic acid composition in acid feed


This work presented new features characterizing a modern modeling approach for RD processes, which include phase splitting calculation. By adapting a rapid, robust and reliable algorithm based on a homotopy-continuation method, the new model implementation was first validated and then put into value for a specific application, i.e., acetic acid recovery from the waste water. Two promising reactive distillation column structures were identified giving close to 100% conversion of acetic acid to a valuable ester product. The intringuing process behavior was revealed for the proposed column structures through a series of dynamic simulation runs—expansion and contraction of the three-phase regime along the column length is one of these phenomena, for example.

Important future directions are: (1) experimental validation of the proposed model, (2) integration of a reliable phase split routine within the standard optimization tool to obtain an economically optimal design and (3) control of the desired steady state using some suitable control strategy.


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Copyright information

© Springer-Verlag 2007

Authors and Affiliations

  • Jignesh Gangadwala
    • 1
  • Gabriel Radulescu
    • 1
  • Achim Kienle
    • 1
    • 2
  • Frank Steyer
    • 1
  • Kai Sundmacher
    • 1
    • 2
  1. 1.Max-Planck-Institute für Dynamik Komplexer Technischer SystemeMagdeburgGermany
  2. 2.Otto-von-Guericke-UniversitaetMagdeburgGermany

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