2.1. Applications of Inorganic Membrane Reactors
Thus far, membrane reactors have been tested and studied for different reaction systems, ranging from methane and biogas reforming to ammonia cracking [
17,
18] and to ethanol and methanol reforming [
19]. However, most of the work done on inorganic membrane reactors concerns hydrogen production, where hydrogen-selective membranes are used to selectively remove the product of a reaction.
Table 1 summarizes the various reactions considered for hydrogen production in membrane reactors.
Natural gas is a typical feedstock considered for hydrogen production in membrane reactors. This is a typical endothermic system where high temperatures (up to 1200 K) are required to activate the methane and convert to it hydrogen and CO. CO should then be converted into CO
2 in WGS reactors, which operate at relatively lower temperatures because of equilibrium constrains.
Figure 5 shows a conventional steam methane reforming (SMR) process for hydrogen production. In this process, due to the exo-endothermic nature of the reactions and the effect of pressure and temperature, several steps (vessels) of and heat exchangers are used to achieve high-purity hydrogen in an efficient way.
The application of hydrogen-permeable membranes for methane steam reforming is possibly the most studied application of membrane reactors. This is probably due to the ease of its demonstration, providing experimental proof that membrane reactors can achieve higher conversions (specifically at higher pressures) compared to equilibrium-limited conventional systems (
Figure 6).
In this case, the membrane reactor technology allows us to achieve the same conversions of a conventional system while working at much lower operating temperatures (550 °C for an MR compared to 850–900 °C for a conventional system). On top of it, as hydrogen is permeating through the membranes, the WGS reaction is shifted towards the products and a downstream separation is not required [
20].
In another study, Matsuka et al. [
21] performed membrane reactor tests in a packed-bed configuration using nickel-based catalysts coupled with different types of self-supported membranes: 25 and 50 μm-thick Pd
77Ag
23 and 100 μm-thick V and V
92Ni
8 layers coated on both sides with Pd by magnetron sputtering (1 μm). The best performance was observed for the Pd-coated vanadium membrane, obtaining a ~45% methane conversion at 400 °C while the permeation flux was 0.09 (mol m
−2 s
−1). This is due to higher diffusion rate of hydrogen molecules in vanadium compared to in palladium. However, and to enhance the hydrogen-splitting phenomenon, thin layers of Pd are still required.
Silva et al. [
22] demonstrated that methane steam reforming can be performed in a packed bed membrane reactor with an up to 47% hydrogen recovery at a 35% methane conversion (at 600 °C). Additionally, Gil et al. [
23] used a catalytic hollow-fiber membrane reactor where the Ni-based catalyst was supported on the hollow fiber’s walls, while the selective Pd-based layer was coated on the other side of the hollow-fiber wall. In this case, an up to 45% hydrogen recovery at a >50% conversion was obtained at 560 °C.
Similarly, Gallucci et al. [
24] have also showed the advantages of self-supported Pd-based membrane reactors compared to packed-bed reactors at temperatures higher than 350 °C, as reported in
Figure 7.
2.2. Inorganic Membrane Reactors Configurations
Recently, more interesting ultra-thin Pd-based membranes have been reported that would make the membrane reactor application even more interesting [
25]. By decreasing the thickness of the membrane, the amount of Pd per square meter of membrane decreases proportionally. Additionally, the hydrogen flux increases proportionally as well, so, consequently, the required membrane area for the same amount of separated hydrogen will be much lower. Since both the total required membrane area and the palladium per m
2 are proportionally decreased by decreasing the thickness, the cost benefit of decreasing the thickness is double. However, when the membranes become thinner, the diffusion resistance through the bulk of the membrane decreases. Thus, other mass transfer limitations can become more important and become limiting phenomena. In particular, mass transfer limitations in the gas phase, also known as concentration polarization, may become the limiting factor in the efficiency of the system [
26,
27,
28].
To circumvent concentration polarization, one can either decrease the gas phase pathway—i.e., using micro-channel reactors [
29]—or increase the mixing in the gas phase, for example using fluidized bed reactors. In both cases, the heat transfer rate is improved as well, which is beneficial for membrane reactors in any case. Both strategies have several advantages and have their own disadvantages, which will be discussed here.
The advantages of micro-reactors have been reported and discussed by several authors in recent publications [
29,
30,
31]. In a micro-channel membrane reactor, the distance between the catalyst bed (generally wash-coated on the channel wall) where hydrogen is produced and the membrane wall, where hydrogen is recovered, is in the microscale, and thus the mass and heat transfer limitations are negligible. The ratio between the membrane area and the catalyst bed is also increased, which allows achieving high recoveries, as this ratio is an essential parameter in membrane reactors [
32].
However, in a micro-channel reactor the production of hydrogen per module will be limited due to very limited amount of available catalyst [
33]. This can be solved by numbering up the microchannel modules; these can also integrate different reaction zones, such that the heat required from the reaction is supplied by either heating fluids or combustion reactions (see
Figure 8).
The integration of membranes in micro-channel modules has been extensively studied by Norwegian research organization SINTEF as well, where different strategies have been developed to improve the membrane stability at the high pressures required for membrane reactor operations [
34].
On the other hand, fluidized bed reactors are also used to decrease the mass transfer limitation, where mixing is induced by catalyst particles circulation inside the reactor [
35,
36]. As a direct consequence, the temperature profiles are also virtually uniform throughout the bed. An application of fluidized bed reactors for ultra-pure hydrogen production has been demonstrated by Helmi et al. [
37] (see
Figure 9), who reported stable operation and high-purity hydrogen production for a duration of 900 h. In this case, the fluidized bed membrane reactor system was operated with syngas composition coming from a reformer; the CO concentration in the permeate side was always below 10 ppm, thus producing in one step the hydrogen purity required by a low-temperature Proton Exchange Membrane (PEM) fuel cell.
Additionally, in our previous works [
32] we have reported fluidized bed membrane reactor configurations for ultra-pure hydrogen production with integrated CO
2 capture. The reactor is divided in two zones: in the first zone, using oxygen membranes and hydrogen membranes, while in the second zone using only Pd-based membranes (for both hydrogen separation and partially for heat integration). This concept is reported in
Figure 10.
The concept allows the complete conversion of the fuel into pure hydrogen and a stream of CO2 and steam, and pure CO2 can be easily achieved followed by a condensation step. However, to achieve this a very large membrane area is required (because of the shift of the remaining CO to CO2), and 1/3 of those expensive membranes are used for heat supply to the system.
In another work [
38], we have developed a new reactor concept combining membrane reactors and chemical looping concepts to obtain pure hydrogen production with integrated CO
2 capture.
Figure 11 schematically shows the newly developed Membrane Assisted Chemical Looping Reactor (MA-CLR) for hydrogen production via steam methane reforming.
The results have shown that the MA-CLR can be continuously operated at the lab scale [
39] while pure hydrogen is recovered by Pd-based membranes, and Ni-based particles are used as both oxygen carriers for the chemical looping system and as catalysts for the reforming reaction. If the system is scaled up and operated at higher pressures, the produced hydrogen cost will be even lower than the hydrogen produced via the conventional steam methane reforming process, while also avoiding a large part of the CO
2 emissions associated with hydrogen production [
40].
The MA-CLR concept requires two interconnected reactors, with solids circulating between them. This is a common configuration that has, however, only been used (at industrial level) at lower pressures. The high-pressure operation is thus one of the challenges to be solved for the large-scale implementation of this technology.
Membrane-assisted gas switching reforming is another concept which combines chemical looping and a membrane reactor for operation at high pressures. This concept foresees dynamically operated fluidized bed reactors where the solids are periodically oxidized and reduced (reforming stage). Thus, a series of reactors operate in parallel to achieve the steady-state production of pure hydrogen. This concept has been demonstrated experimentally at the lab scale [
41], and a full techno-economic analysis has been carried out [
42]. The results have shown that, although this is an interesting concept, the economics are worse than the MA-CLR proposed before. In addition, the membranes’ stability is significantly compromized due to the continuous oxidation/reduction cycles that they will experience.
Pure hydrogen production with CO
2 capture can also be obtained by integrating membrane reactors with a CO
2 sorbent, as reported by Madeira et al. [
43] (see
Figure 12). By combining the sorption of carbon dioxide on a solid sorbent (an exothermic reaction) and hydrogen recovery through membranes, a double shift effect is obtained (both products are removed from the reaction system). In this case, the reactor should be operated dynamically, which means that at least two units need to be operated in parallel to achieve continuous hydrogen production.
Wang et al. [
44] have used nickel-based hollow-fiber membranes for hydrogen permeation and the WGS reaction (see
Figure 13). The thin-wall nickel membranes have shown a very good stability in cyclic operation, as well as a very good membrane selectivity (at the expense of lower fluxes). Interestingly, the membranes showed a high stability in different gas atmospheres, including in the presence of H
2S (detrimental for Pd-based membranes) [
45].
Bhushan et al. [
46] have studied Tantalum-based membranes in membrane reactors for enhancing the HI decomposition reaction. This concept is experimentally demonstrated over a very thin (2.5 micron) supported Ta-based membrane. Additionally, in a modelling study reported by the authors, it was found that the HI conversion can be increased up to 95% in conditions in which the thermodynamic equilibrium of a conventional system is limited to 22% conversion. Again, the Ta-based membrane was effectively used in an environment where Pd-based membranes cannot be applied.
Another Ta-based membrane reactor has been proposed by Suk et al. [
47] for hydrogen production from ammonia decomposition. The authors used a Ta tube and coated it with a very thin Pd layer (to enhance hydrogen dissociation) and used it for an ammonia decomposition reaction. The membrane was proven to be very stable in conditions in which Pd-based membranes could suffer ammonia poisoning. The authors have shown its very good permeation properties and stable ultra-pure hydrogen production (with ammonia impurities of below 0.1 ppm). A similar reaction has been carried out by Lamb et al. [
48] using a V-based membrane. However, in this case a cascade of catalytic bed and membrane separation has been used rather than a membrane reactor.
2.3. New Trends and Applications of Inorganic Membrane Reactors
An interesting newly investigated application of metallic membranes is the propane dehydrogenation reaction. In this case, the product is not hydrogen but propylene. This reaction system is generally a dynamic process, because the catalyst should be periodically regenerated to remove the carbon deposited during the reaction. By removing hydrogen from the system, the equilibrium is shifted towards the product and similar yields can be achieved at lower temperatures, which in turn will reduce the carbon deposition and reduce the regeneration frequency. This concept has been studied in the literature by several authors [
49,
50,
51]. These studies have shown that conventional Pd membranes were quickly deactivated when used for propane dehydrogenation, probably due to the carbonaceous species formed on the surface due to the interaction with propylene. On the other hand, the membranes can be more resistant if protected with an intermediate porous layer that prevents the direct interaction of Pd with propylene, such as in the double-skin membranes recently proposed by Arratibel et al. [
52].
Another interesting recent application of inorganic membrane reactors is the oxidative coupling of methane, where currently research activities are mainly focused on using oxygen separation membranes in the reactor. A direct route for the production of ethylene from natural gas in a single step has been on the top position of the wish list of the chemical industry for a long time now. However, methane is a difficult molecule to activate, and a possible route for methane-to-ethylene reaction is the widely investigated oxidative coupling of methane (OCM), which involves the conversion of methane together with oxygen at a high temperature (>750 °C) into the desired product C
2H
4 (or C
2H
6). However, being a high temperature oxidative route, undesired by-products (CO and CO
2) are obtained through parallel and consecutive oxidation reactions. To simplify the problem, the main reactions involved in OCM are the following (although up to 14 reactions have been used to describe the system in the literature [
53]):
As with many partial oxidation reactions, the competition of many parallel and consecutive reactions results in the typical conversion-selectivity problem: high CH
4 conversions (i.e., feeding a relatively large amount of O
2) result in a relatively poor product selectivity, with a large yield of undesired combustion products such as COx. In addition, the highly reactive intermediate C
2H
4 may easily react to the unwanted and thermodynamically favored oxidation products at high O
2 concentrations [
54]. This is the main reason why the yield of higher hydrocarbons (C2+) is insufficient (<<30%) to make the OCM concept industrially feasible, which would require C2+ yields of above 30-35% [
55,
56]. Since the first OCM articles were published [
57], there have been many studies aiming at improving the C2 yield by working on new catalyst formulations, resulting in some of the most promising catalysts for OCM: Li/MgO [
1,
2], La
2O
3/CaO [
58], and Mn/Na
2WO
4/SiO
2 [
59]. Although the optimization of the catalyst and the development of various different reactor types has led to an improved performance of the process, a single-pass C2 yield above 30–35% has never been achieved yet (e.g., [
60]).
In addition, several reactor concepts have been proposed to achieve a higher product yield by recycling the reactants to the reactor and selectively separating the desired products of the primary reactions [
60,
61,
62]. Most of the new concepts are also looking at improving the heat management of the system.
One of most interesting concepts to carry out the OCM and to achieve an industrially feasible yield is the membrane reactor based on oxygen-selective membranes (also studied in the EU-funded MEMERE project). By using the oxygen separation membranes in the reactor, often perovskite-type membranes, a distributed oxygen feeding strategy is achieved, thus maintaining a low oxygen concentration along the reactor and favoring the C2+ production reactions. However, the reactions are highly exothermic and thus even the membrane reactor needs an optimized cooling system, which results in a very complicated reactor design [
63].
Godini et al. have worked on different configurations of membrane reactors for the OCM reaction [
64] and have reported a techno economic analysis of such a reactor system, showing higher conversions and yields than conventional reactors and thus better economics [
65]. Additionally, Vamvakeros et al. have reported the real-time characterization of a membrane reactor for the OCM reaction [
66]. Although the membrane reactor for OCM remains a very interesting concept, the sealing at the reactor temperature and the membrane stability in these conditions remain the main challenges that still need to be tackled [
67].
CO
2 valorization is another interesting application of inorganic membrane reactors, especially for methanol production from CO
2 and hydrogen [
11]. The methanol synthesis is indeed an equilibrium system that is best represented by the following set of reactions:
Either as a component of the syngas or as only source of carbon, CO
2 is always present in methanol production. The third reaction is indeed the typical example of CO
2 valorization into chemical building blocks. Among the different membrane reactors proposed for this reaction, zeolite membrane reactors have gained increasing interest during the last 20 years [
68]. Masuda and co-workers [
69] investigated a zeolite-based membrane reactor for increasing the selectivity of olefins during the methanol conversion. The membranes resulted in being defect-free and they successfully withdrew the olefins from the reaction zone during the methanol conversion. In this paper, a method for testing the durability of membranes under a sequence of thermal and mechanical shocks is reported. Their membrane showed a quite high durability, while the selectivity of olefins from methanol was increased up to 90% even at high methanol conversions. The same group [
70] further improved the use of ZSM-5 membranes for the methanol to olefins reaction.
In another study, Li et al. [
71] synthesized an Linde type A (LTA) zeolite membrane for improving the performances of the Fisher–Tropsch (FT) reaction. The use of a hydrophilic membrane during the FT reaction can allow the separation of water (a product of the reaction) for the permanent gases, resulting in an increase in the conversion per pass and, more importantly, avoiding the catalyst deactivation caused by the high amount of water present in the reaction system. The authors produced their LTA zeolite membrane with an in situ method improved with microwaves on a α-Al
2O
3 tubular support. They obtained very high perm-selectivities over a broad range of experimental conditions.
The use of membranes for the FT reaction was also suggested by Espinoza et al. [
72]. In this work, the possibility of water recovery from the reaction system is investigated, leading to increase in the catalyst lifetime and conversion by using different types of membranes, such as silicalite-1, Mordenite, and ZSM-5.
De Falco et al. [
73] simulated a zeolite membrane reactor for the production of Dimethyl ether (DME). The authors simulated the behavior of the reactor in different conditions, demonstrating once more that the zeolite membrane reactor can be used for DME as a CO
2 reuse route. They reported a conversion enhancement compared to a conventional reactor of more than 30% (see
Figure 14). These results should be, of course, confirmed by an experimental study.
In another effort, the efficient synthesis of the DME in a membrane reactor is experimentally demonstrated by Zhou et al. [
74] by using an FAU-LTA zeolite dual-layer membrane in a membrane reactor. The authors were able to boost the conversion of methanol up to >90% at a 100% DME selectivity in their membrane reactor.
Barbieri et al. [
75] performed a thermodynamic analysis of the CO
2 hydrogenation into methanol by using zeolite membranes with different values of methanol and steam permeation. As indicated in
Figure 15, the authors found a sharp increase in the carbon dioxide conversion while using the membrane reactors with respect to the conventional system. Additionally, the increase in the methanol permeation in the membrane (compared to water) resulted in a higher selectivity and methanol yield. The methanol yield (per pass) increased from 5.8% in a conventional system to up to 13.7% in the best membrane reactor.
The modeling study of Barbieri and co-workers heavily relies on the permeation rates of methanol and water in zeolite membranes. The more reliable the data available on this separation are, the better the modeling of membrane reactors can be. In this sense, Sawamura and co-workers [
76] studied the selective removal of water from a water-methanol-hydrogen mixture using a mordenite membrane. The membrane was prepared by the secondary growth method on the outer surface of an α-alumina commercial tube with an asymmetric structure.
The methanol production in zeolite membrane reactors has also been studied from an experimental point of view, as reported by [
77].
Figure 16 shows the behavior of CO
2 conversion versus temperature in terms of experimental results for both the traditional system and the membrane reactor at 20 bar and at two different H
2/CO
2 feed ratios. The membrane reactor generally outperforms the traditional system. However, for temperatures higher than 230 °C, the membrane reactor tends to converge with the traditional reactor. Two explanations can be given for this loss in performance. The first explanation is related to the thermal stability of the zeolite membrane. However, another possible explanation is the impossibility, at high temperatures, of methanol condensing inside the pores of the structure. Methanol has a critical temperature at 238 °C, so at T > 238 °C a behavior like a gas is expected. The critical temperature of water (374 °C) assures us that, in the range of temperature considered for experimental tests (200–263 °C), only methanol is expected to change phase from vapor to gas when passing 238 °C. Above 238 °C, due to this effect a weaker increase in the CO
2 conversion versus temperature is expected. In fact, at 255–263 °C both the membrane reactor and the traditional reactor show a similar CO
2 conversion.
Gorbe et al. [
68] have recently reported the permeation data of zeolite membranes for this reaction system. The authors have reported that a temperature gradient between the reaction side and the permeation side of the zeolite membrane can be effectively used to improve the water permeation through the membrane, and thus improve the methanol yield in a membrane reactor.
The previous sections have shown that there is quite an amount of works dealing with inorganic membrane reactors. However, despite the big amount of data showing that the membrane reactors have a superior performance compared to conventional reactors, still the scale-up of these reactors at the larger industrial scale is missing. A few examples of scale-up to pre-industrial scale have been attempted for hydrogen membrane reactors and for hydroformylation (see the MEMBER and MACBETH H2020 projects). The reason for such slow scale-up exercises is to be found in the lack of evidence of the long-term stability of the membranes in reactive conditions, as well as to the very large scale of these chemical pants. A real break-through application is required to push forward the implementation of inorganic membrane reactors. On the other hand, membrane reactors have already found their industrial application in biological systems where the scale of the plants is smaller and the cost of the membranes is much lower, which allows for pilot-plant application in the short term. In the next section, the status of membrane bioreactors will be reviewed and possible future directions will be discussed.