1. Introduction
In the chemical industry, high-efficiency reactions and separation processes are needed to reduce greenhouse gas emissions. Reactive separation processes have attracted considerable attention given their high levels of efficiency [
1]. Reactive distillation is one such reactive separation technology. Reactive distillation offers advantages such as energy and capital savings, increased reaction conversion, high selectivity, and utilization of the reaction heat [
2]. Therefore, reactive distillation processes have been examined for application to esterification and etherification reactions [
3,
4,
5,
6].
The design and operability of a reactive distillation process become more difficult than those of a conventional distillation or reaction process because of the interactions between the reaction and the separation. Multiple steady states exist in a reactive distillation process because of these interactions. Through experiments, Mohl et al. confirmed the existence of multiple steady states when using a pilot-scale reactive distillation column for
tert-amyl methyl ether (TAME) synthesis [
7]. Some researchers empirically confirmed the existence of multiple steady states in a reactive distillation process. Jacobs and Krishina and Nijhuis et al. reported on the existence of multiple steady states observed in the simulation of a reactive distillation for the synthesis of methyl
tert-butyl ether (MTBE) using a steady-state equilibrium stage model [
8,
9]. Baur et al. performed bifurcation analysis for TAME synthesis in a reactive distillation using the reaction kinetics methods for pseudo-homogeneous and heterogeneous models [
10]. They reported that multiple steady states can be captured by simulation for two different reaction kinetics methods. Wang et al. analyzed the product purity attained with MTBE synthesis in a reactive distillation column and observed multiple steady states [
11]. Ramzan et al. simulated a reactive distillation column for ethyl
tert-butyl ether synthesis and again detected multiple steady states [
12]. Cárdenas-Guerra et al. found multiple steady states in the reactive distillation process for the deep hydrodesulfurization of diesel [
2]. Meanwhile, Jairnel-Leal et al. analyzed the operating conditions and parameter sensitivity of multiple steady states in a reactive distillation for TAME and MTBE syntheses [
13]. They found that the feed thermal condition has a major influence on the occurrence of multiple steady states.
Our research group considers that the process performance of a reactive distillation can be improved through the multiple steady-state condition, and process design and analysis are performed. The effects of the operating conditions in the multiple steady states on the performance of a reactive distillation column used for TAME synthesis were evaluated [
14]. The reaction conversion in the upper branch in the multiple steady states was the highest and increased with the reflux ratio. In addition, the energy-saving performance of reactive distillation consisting of one reactive distillation column and two recovery distillation columns for the multiple steady states was examined [
15]. The energy consumption for TAME synthesis with multiple steady states became lower than that in the case in which multiple steady states did not exist because of the improvement in the reaction conversion and the reduction in the reboiler duties of the recovery columns. However, the factor leading to an improvement in the reaction conversion has not been clarified. If the factors leading to an improvement in the reaction conversion can be clarified, this may lead to an improvement in the process performance of a reactive distillation column without the multiple steady-state conditions.
The present work investigated the factors leading to an improvement in the reaction conversion for operation in the multiple steady states. This study focused on the profile of the reactive distillation column used for TAME synthesis. In our previous study, the multiple steady states did not exist for a reflux ratio of 1, but did exist for a reflux ratio of 2. The column profiles of the steady-state solutions for reflux ratios of 1 and 2 were compared. A simulation model of the reactive distillation column with an intermediate condenser at the top of the reactive section was developed to manipulate the internal flow rate of the reactive distillation column. The effect of the intermediate condenser duty on the amount of TAME product and the reboiler duty of the reactive distillation column was clarified. Furthermore, a simulation model of the reactive distillation column with an intermediate condenser and an intermediate reboiler was developed. The effects of the intermediate cooling and heating on the amount of TAME product and the reboiler duty of the reactive distillation were evaluated. Furthermore, the variation in the process performance of the reactive distillation column when the internal vapor liquid flow rate was manipulated was discussed.
3. Simulation Results and Discussion
3.1. Process Characteristics
Our previous study reported the condition in which multiple steady states exist, as shown in Figure 3 of previous work [
15]. For a reflux ratio of 1, multiple steady states did not exist, but were observed at a reflux ratio of 2 for a reboiler duty between 12.25 and 12.12 MW. This study focused on four steady-state solutions.
Table 2 summarizes the simulation results for each steady-state solution. Three solutions with reboiler duty values in the middle of the range were selected for the multiple steady states. The MeOH conversion (
εMeOH) as the reactant was calculated using the MeOH flow rate in the feed (
FMeOH), distillate (
DMeOH), and bottom (
BMeOH):
The MeOH conversions in the steady-state solutions in the multiple steady states became higher than those in steady state 1. This result indicates that the reaction conversion in the multiple steady states can be improved.
This section discusses the factors leading to the reaction conversion improvement in terms of the column profiles.
Figure 2,
Figure 3,
Figure 4 and
Figure 5 show the column profiles for the temperature, vapor, and liquid flow rates, mole fraction, and generated TAME amounts, respectively. From the temperature profile, in the stripping section, the temperature in the 1st stage for steady states 1 and 4 reached 398.4 K, which is the boiling point of TAME. The TAME and MeOH mixture was obtained as shown in
Figure 4; hence, the temperatures in the 1st stage for steady states 2 and 3 were 362.7 and 367.4 K, respectively. However, the temperatures in the reactive sections were nearly the same in each of the four steady states; thus, the temperature in the reactive distillation column has little effect on the MeOH conversion.
The vapor and liquid flow rate profiles showed that the vapor and liquid flow rates in steady states 2–4 were larger than that in steady state 1 because the reflux ratio in steady states 2–4 were higher than that in steady state 1. Large vapor and liquid flow rates promoted separation. Therefore, the vapor–liquid flow rate contributed to an increase in the MeOH conversion.
The composition profiles and the generated TAME amount profile showed little change in the mole fractions of MeOH, 2M1B, and 2M2B in the rectifying and reactive sections in steady state 1. The reactants were distilled from the distillate stream; hence, the generated TAME amounts became small. In contrast, in steady states 2–4, the mole fraction of MeOH in the reactive section decreased along with the stage number because MeOH was consumed by TAME synthesis around the bottom of the reactive section. In the stripping section, TAME was not separated from MeOH, and MeOH was discharged from the bottom stream in steady states 3 and 4. By contrast, high-purity TAME was obtained in steady state 5. For these column profiles, the internal vapor–liquid flow rate must be controlled, and the discharge of reactants must be prevented to increase the reaction conversion.
3.2. Effect of an Intermediate Condenser
Based on the abovementioned results, the small MeOH conversion in steady state 1 was caused by the small internal flow rate and the reactant discharge from the top of the reactive section. The internal flow rate may be increased, such that the MeOH discharge is reduced, by condensing the vapors from the top of the reactive section. Thus, a simulation model of the reactive distillation with an intermediate condenser at the 28th stage (top of the reactive section) was developed (
Figure 1b). The effect of the intermediate condenser duty on the column profiles was then evaluated. The intermediate condenser duty was changed from 0 to −5 MW. The reboiler duty was adjusted such that the TAME mole fraction in the bottom stream reached 1.00.
Figure 6 shows the effect of the intermediate condenser duty on the bottom flow rate and reboiler duty. The bottom flow rate increased with an increase in the intermediate condenser duty, indicating that the MeOH conversion increased because the TAME mole fraction in the bottom stream was 1.00.
Figure 7 presents the vapor–liquid flow rate and the composition profiles for an intermediate condenser duty of −3.0 MW. In this case, the internal flow rate was larger than that in steady state 1. The composition profile was such that the mole fraction of MeOH decreased along with the stage number in the reactive section, leading to an improvement in the reaction performance. However, in the stripping section, the mole fraction of MeOH was higher than that in steady state 3. The MeOH conversion may increase if the amount of MeOH discharged from the bottom of the reactive section decreases.
3.3. Effects of the Intermediate Condenser and the Intermediate Reboiler
This study also examined liquid vaporization from the bottom of the reactive section with the intermediate reboiler to reduce the amount of MeOH discharged from the bottom of the reactive section. A simulation model for the reactive distillation column with an intermediate reboiler and condenser was developed (
Figure 1c).
Figure 8 shows the effects of the intermediate condenser and reboiler duty on the bottom flow rate and reboiler duty. The reboiler duty was adjusted such that the TAME mole fraction in the bottom stream reached 1.00. The effect of the intermediate reboiler duty on the bottom flow rate was similar to that in
Figure 6. The degree of MeOH conversion also cannot increase beyond the results attained with reactive distillation when using an intermediate condenser. However, the reboiler duty can be reduced with the addition of the intermediate reboiler presumably because the separation of TAME and MeOH occurs as a result of introducing the intermediate reboiler.
Finally, the energy consumption for each reactive distillation column is discussed. A comparison was made with the energy consumption when TAME was produced at a rate of 72 kmol/h from the bottom-out stream. The energy consumptions in steady state 4 of the reactive distillation column with one intermediate condenser and of the reactive distillation column with one intermediate condenser and reboiler were 612, 628, and 637 kJ/mol. The present study did not attempt to optimize either the locations of the intermediate condenser and reboiler or the energy input. Further energy savings could possibly be achieved by optimizing these locations and the input energy.
4. Conclusions
The present study clarified the factors leading to an improvement in the reaction conversion during operation in multiple steady states for the reactive distillation column used for TAME synthesis. The column profiles for reflux ratios of 1 (no multiple steady state) and 2 (multiple steady states) were compared. The comparison of the column profiles for four steady-state solutions clearly showed that the internal vapor and liquid flow rates in the reactive distillation column affected the reaction conversion. An intermediate condenser was introduced at the top of the reactive section to control the liquid flow rate in the reactive distillation column. The effect of the intermediate condenser duty on the TAME production was evaluated, with the amount of TAME product increasing from 55.2 to 72.1 kmol/h as a result of operating the intermediate condenser between 0 and −5 MW. The liquid vaporization from the bottom of the reactive section with the intermediate reboiler was also examined. As a result, the amount of TAME product cannot increase beyond the amounts produced by reactive distillation using an intermediate condenser, but the reboiler duty can be reduced through the addition of the intermediate reboiler. These results indicate that the liquid and vapor flow rates in the reactive distillation column influence the reaction and separation performances, respectively.
In the future, we will investigate the attainment of optimal vapor–liquid flow rates with small input energy. The temperature difference between the top and the bottom of the reactive section was 2.9 K (
Figure 2). Heat integration between the intermediate condenser and the intermediate reboiler through the application of the heat-pump technology may be effective [
17,
18,
19].