Next Article in Journal
Effects of the Substrate on Interfacial Polymerization: Tuning the Hydrophobicity via Polyelectrolyte Deposition
Next Article in Special Issue
P84/ZCC Hollow Fiber Mixed Matrix Membrane with PDMS Coating to Enhance Air Separation Performance
Previous Article in Journal
Bovine Hemoglobin Enzymatic Hydrolysis by a New Ecoefficient Process—Part I: Feasibility of Electrodialysis with Bipolar Membrane and Production of Neokyotorphin (α137-141)
Previous Article in Special Issue
Dimensional Nanofillers in Mixed Matrix Membranes for Pervaporation Separations: A Review
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Hydrogen Selective SiCH Inorganic–Organic Hybrid/γ-Al2O3 Composite Membranes

1
Department of Life Science and Applied Chemistry, Graduate School of Engineering, Nagoya Institute of Technology, Gokiso-cho, Showa-ku, Nagoya 466-8555, Japan
2
Institut für Materialwissenschaft, Technische Universität Darmstadt, Otto-Berndt-Str. 3, 64287 Darmstadt, Germany
3
CNRS, IRCER, UMR 7315, University of Limoges, F-87000 Limoges, France
*
Author to whom correspondence should be addressed.
Submission received: 28 August 2020 / Revised: 21 September 2020 / Accepted: 24 September 2020 / Published: 25 September 2020

Abstract

:
Solar hydrogen production via the photoelectrochemical water-splitting reaction is attractive as one of the environmental-friendly approaches for producing H2. Since the reaction simultaneously generates H2 and O2, this method requires immediate H2 recovery from the syngas including O2 under high-humidity conditions around 50 °C. In this study, a supported mesoporous γ-Al2O3 membrane was modified with allyl-hydrido-polycarbosilane as a preceramic polymer and subsequently heat-treated in Ar to deliver a ternary SiCH organic–inorganic hybrid/γ-Al2O3 composite membrane. Relations between the polymer/hybrid conversion temperature, hydrophobicity, and H2 affinity of the polymer-derived SiCH hybrids were studied to functionalize the composite membranes as H2-selective under saturated water vapor partial pressure at 50 °C. As a result, the composite membranes synthesized at temperatures as low as 300–500 °C showed a H2 permeance of 1.0–4.3 × 10−7 mol m−2 s−1 Pa−1 with a H2/N2 selectivity of 6.0–11.3 under a mixed H2-N2 (2:1) feed gas flow. Further modification by the 120 °C-melt impregnation of low molecular weight polycarbosilane successfully improved the H2-permselectivity of the 500 °C-synthesized composite membrane by maintaining the H2 permeance combined with improved H2/N2 selectivity as 3.5 × 10−7 mol m−2 s−1 Pa−1 with 36. These results revealed a great potential of the polymer-derived SiCH hybrids as novel hydrophobic membranes for purification of solar hydrogen.

Graphical Abstract

1. Introduction

Hydrogen (H2) is an attractive energy carrier because of its high energy yield of 120 J g−1. This value is about 2.8 times higher than hydrocarbon fuels [1]. Moreover, the combustion product is water and thus completely clean in a carbon dioxide (CO2)-neutral manner.
In addition to the current hydrogen production by the steam reforming of naphtha and methane, hydrogen can be produced using several resources including hydropower, nuclear energy and renewable energy sources like biomass, wind, geothermal and solar. Among them, hydrogen production via photoelectrochemical (PEC) water-splitting has received increased attention as an environmental-friendly and low-cost solar-to-hydrogen pathway because of its potential for high conversion efficiency at low operating temperatures using cost-effective semiconductor-based photoreaction catalysts [2,3,4]. The solar hydrogen production systems are expected to be used in terms of global-warming prevention and a stable supply of energy. Therefore, in Japan, the research and development of these systems have been promoted by the Ministry of Economy, Trade and Industry (METI). For example, as an ongoing New Energy and Industrial Technology Develop Organization (NEDO) R&D project, the “Artificial Photosynthesis” Project has been conducted by the Japan Technological Research Association of Artificial Photosynthetic Chemical Process (ARPChem) [5,6]. This project is composed of three research teams: the Solar Hydrogen Team for water photo-splitting catalysts, the Hydrogen Separation Team for gas separation membranes and the Synthetic Catalyst Team for CO2 hydrogenation catalysts. All teams are concentrating in materials research and development. These teams also have their missions for future planning and designing industrial photocatalytic plants, gas separation systems with safety measures against explosion, and catalytic synthesis plants, respectively [5,6].
The PEC reaction simultaneously generates H2 and oxygen (O2) by an oxidation–reduction reaction of water under sunlight in the presence of semiconducting catalysts
2 H 2 O     2 H 2   +   O 2
Since H2 and O2 react in a large range of H2 concentration of 4–95% [7], this hydrogen production system requires an efficient separation technology for purifying H2 from the syngas containing O2.
There are several candidate technologies for H2 purification such as cryogenic distillation, PSA (pressure swing adsorption) and membrane separation. Among them, membrane separation shows some advantages including energy efficiency and simple separation schemes suitable for establish safe operation process for purification of solar H2.
However, under the given operating conditions [5,6,8], it is difficult to apply conventional H2-selective membranes, which require higher operation temperatures, approximately above 90, 180 and 350 °C for polymer [9], silica [10,11,12] and metal membranes [13,14,15], respectively. There are also technical issues such as water-induced swelling for polymer membranes, lower H2 permeance for supported liquid membranes [16,17,18] and gas permeability degradation for intrinsically hydrophilic silica-based membranes [8,19,20].
Recently, increasing attention has been directed to organic–inorganic hybrid materials as promising functional materials in various fields such as optics, electronics and energy. Synergistic properties of hybrid materials can be achieved by harmonizing advantageous properties of an organic component, such as solubility, plasticity and hydrophobicity, with those of an inorganic component such as high strength and thermal and/or chemical stability [21,22]. The polymer-derived ceramics (PDCs) route [23,24] appears to be an efficient approach for the synthesis of novel organic–inorganic hybrids categorized as Class II hybrids according to the classification given by Sanchez [25], where the organic and inorganic components are linked together by strong chemical bonds, by polymerization and thermal or chemical cross-linking of silicon-based polymers. Moreover, this process can provide a means to vary the specific properties of the silicon-based polymers such as solubility and viscosity, which provides the versatility in shaping capabilities including the formation of surface coatings and membranes similar to those successfully achieved with hydrocarbon-based polymers. In the topic of PDCs, polycarbosilanes (PCSs) are well known as precursors for silicon carbide (SiC)-based ceramics [26,27]. Their synthesis by the Kumada rearrangement of polydimethylsilane (PDS) has been reported by Yajima et al. [26]. Since polymer-derived amorphous silicon (oxy)carbide (SiC and SiCO) show excellent thermal and chemical stabilities [28,29], PDS [30], PCSs [31,32,33,34,35,36,37] and PCS derivatives such as allyl-hydro-polycarbosilane (AHPCS) [38,39,40,41,42] have been applied as precursors of microporous amorphous SiOC [30,31,32,33,34] and SiC [29,35,36,37,38,39,40,41,42] membranes to investigate their gas permeation properties mainly at high temperatures, T ≥ 200 °C. PCSs are also appropriate as functional Class II hybrids: The silicon-carbon (Si-C) backbone endows several attractive properties of PCSs such as high flexibility and excellent thermal, chemical and electrical stabilities [43,44,45]. The hydrocarbon groups attached to the Si-C backbone provide room temperature stability in air and PCSs can be applied as an active binder for the formation of powder compact to fabricate polycrystalline SiC ceramics [46,47,48,49]. Moreover, in our previous study [50], PCSs were found to show an excellent hydrophobic property: gas permeations under highly humid condition at 50 °C of a hydrophilic mesoporous γ-Al2O3 membrane were successfully stabilized by modification with SiCH organic–inorganic hybrid via melt impregnation of PCS at 120 °C [50].
In this study, AHPCS was converted to highly cross-linked ternary SiCH organic–inorganic hybrids with enhanced thermal stability and hydrophobicity by heat treatment at temperatures as low as 300–500 °C in argon (Ar). Highly hydrophobic property of the AHPCS-derived SiCH hybrids was characterized by the water vapor adsorption–desorption isotherm measurement at 25 °C. Then, the SiCH organic–inorganic hybrid served to modify a mesoporous γ-Al2O3 membrane via dip-coating with AHPCS followed by the heat treatment of the composite at 300–500 °C in Ar.
Single gas permeances of helium (He), hydrogen (H2) and nitrogen (N2) under dry condition at 25–80 °C were measured to characterize the intrinsic low-temperature gas permeation properties of the SiCH organic–inorganic hybrid/γ-Al2O3 composite membrane. Then, as the primary accelerated degradation test for the suggested solar H2 purification condition of 10% humidity at 50 °C [5,6], the gas permeance measurements were performed under the saturated water vapor partial pressure at 50 °C. In this measurement, a H2-N2 mixed feed gas in the molar ratio 2:1 was used as a simulated syngas produced by the PEC reaction (Equation (1)) in which O2 (0.346 nm) [51] was replaced by inert N2 having a similar kinetic diameter (0.364 nm) [51] to avoid explosion accidents. Moreover, for some selected membrane samples and the supported mesoporous γ-Al2O3 membrane itself, cyclic gas permeation measurements were continuously performed under water vapor partial pressures ranging from 0 to 1.0 at 50 °C. Effect of the composite membrane synthesis temperature on the hydrophobicity and gas permeation properties under dry and wet conditions were discussed aiming to develop novel hydrophobic membranes for the purification of solar hydrogen at low temperatures around 50 °C.

2. Experimental Procedures

2.1. Preparation of the Supported Mesoporous γ-Al2O3 Membrane

Commercially available macroporous α-Al2O3 tubular support (6 mm outer diameter, 4 mm inner diameter and 60 mm length, Noritake Co., Ltd., Nagoya, Japan) was used. The α-Al2O3 support was composed of a fine outer surface layer (mean pore diameter, dp = 150 nm) and a core (dp = 700 nm). Total porosity of the tubular support was 40%. A mesoporous γ-Al2O3 membrane was fabricated by dip coating of a boehmite (γ-AlOOH) sol on the α-Al2O3 tubular support followed by heat treatment in air at 600 °C for 3 h according to a published procedure [50].

2.2. Modification of a Supported γ-Al2O3 Membrane with AHPCS-Derived Organic–Inorganic SiCH Hybrid

Commercially available AHPCS (SMP-10 was provided by Starfire Systems, Inc., Glenville, NY, USA. Anal. Found (wt %): Si, 54.8; C, 35.0; H, 8.3; O, 1.9. FT-IR (ATR/cm−1): ν (C−H) = 3076 (s), 3003 (s), 2958 (s), 2895 (s), 2850 (m), ν(Si−H) = 2123 (vs), δ(allyl) = 1629 (m), δ(CH2) = 1395 (m), δ(Si-CH3) = 1251 (s), δ(Si-CH2-Si) = 1049 (s), δ(Si-H) = 941.1 (s), δ(Si-C) = 854.3 (s), δ(SiCH3) = 770 (s); 1H NMR (300 MHz, CDCl3, δ/ppm): 0.05 (br, -Si-CH3), 0.4 (br, -Si-CH2-), 1.56–1.9 (br, -Si-CH2-CH=CH2), 3.4–3.84 (br, -SiH3C), 3.8–4.1 (br, -SiH2CH2), 4.85–5.05 (br, -Si-CH2-CH=CH2), 5.71–5.93 (br, Si-CH2-CH=CH2). As a precursor solution for modifying the supported γ-Al2O3 membrane, 1 wt % dry xylene (super dehydrated grade, 99.5% purity, Wako Pure Chemical Co., Ltd., Osaka, Japan) solution of as-received AHPCS was prepared under the inert atmosphere of Ar. By following the procedures described in our previous report [50], the AHPCS solution was dip-coated on the supported γ-Al2O3 membrane, then dried and heat-treated under flowing Ar at 300, 400 and 500 °C for 1 h at a heating/cooling rate of 100 °C h−1 to afford SiCH organic–inorganic hybrid-modified γ-Al2O3 membrane placed on the α-Al2O3 tubular support (SiCH hybrid/γ-Al2O3 composite membrane).
The 500 °C-heat treated membrane was further modified by the melt impregnation of a commercially available PCS at 120 °C under Ar atmosphere (Type L, Nippon Carbon Co., Ltd., Tokyo, Japan) according to the published procedure [50].

2.3. Characterizations

The molecular weight distribution curve of as-received AHPCS was measured at 40 °C by using gel permeation chromatography (GPC, Model ShodexGPC-104 equipped with two tandem columns (Model Shodex LF-404, Showa Denko K.K., Tokyo, Japan) and a refractive index detector (Model Shodex RI-74S, Showa Denko K.K., Tokyo, Japan). The columns were calibrated against polystyrene standards. Tetrahydrofuran (THF, 99.5% purity, Wako Pure Chemical Co., Ltd., Osaka, Japan) was used as the eluent and a flow rate was adjusted to 1.0 mL min−1.
The thermal decomposition and cross-linking behaviors of as-received AHPCS up to 1000 °C was studied by thermogravimetry combined with mass spectrometry (TG-MS) analyses (Model STA7200, Hitachi High Technologies Ltd., Tokyo, Japan/Model JMS-Q1500 GC, JEOL, Tokyo, Japan). The measurements were performed under He atmosphere with a heating rate of 10 °C min−1.
Powder samples of the heat-treated AHPCS were prepared under the same manner for the heat treatment of the supported mesoporous γ-Al2O3 membrane after dip-coating of the AHPCS solution.
Fourier transform (FT)-IR spectrum was recorded on the as-received AHPCS and AHPCS-derived powder samples by the potassium bromide (KBr) disk method (Model FT/IR-4200IF, JASCO Corp., Tokyo, Japan). Note that FT-IR spectrum was also recorded on the powder sample of 700 °C-heat treated AHPCS. Raman spectrum was recorded on as-received AHPCS and heat-treated AHPCS (Renishaw, inVia Reflex, New Mills, England).
Hydrophobicity of the heat-treated AHPCS powder samples was characterized by measuring the water vapor adsorption–desorption isotherms at 25 °C (Model BELSORP-aqua 3, MicrotracBEL Corp., Osaka, Japan). The powder samples were pretreated at 120 °C for 6 h under vacuum.
The cross-sectional structure and top surface of the SiCH hybrid/γ-Al2O3 composite membrane were observed by a scanning electron microscope (SEM, Model JSM-6360LV, JEOL Ltd., Tokyo, Japan). The distribution of the SiCH hybrid within the composite membrane was examined by the energy dispersive X-ray spectroscopic (EDS) analysis (Model JSM-6010LA mounted on SEM, JEOL Ltd., Tokyo, Japan).
Single gas permeances through the membrane samples under dry conditions were measured for He, H2 and N2 by the volumetric method at constant pressure. The setup of the equipment and procedure for the measurements was shown in our previous report [50]. The gas permeances at 25, 50 and 80 ˚C were measured in the size order of a kinetic diameter for He (0.26 nm), H2 (0.289 nm) and N2 (0.364 nm) [51]. The single gas permeance (Qi) was evaluated by using Equation (2),
Q i = V A ( p H p L )
where V (mol s−1) is the permeate molar flow rate, A (m2) is the membrane area and pH (Pa) and pL (Pa) are pressures of the gas feed side and the gas permeate side, respectively. In this study, the (pH − pL) in Equation (1) was fixed as 100 kPa.
The permselectivity (α) was evaluated by calculating the single gas permeance ratio of two different kinds of gases.
H2 and N2 gas permeances under dry and wet condition of the saturated water vapor partial pressure (p/p0 (H2O) = 1.0) were measured at 50 °C using a mixed feed gas with a 2:1 molar ratio of H2 and N2 as a simulated syngas produced by the PEC reaction. For some selected membranes and the supported mesoporous γ-Al2O3 membrane itself, cyclic gas permeation measurements were performed under various p/p0 (H2O) ranging from 0 to 1.0 at 50 °C.
The permeate gas composition was analyzed using a gas chromatograph (GC, Model CP-4900 Micro-GC, Varian medical systems Inc., Palo Alto, CA, USA) and Ar sweep gas (50 mL min−1). Each gas permeance of H2 and N2 was calculated using the analyzed composition and the measured mixed gas permeate molar flow rate. The water vapor permeance was evaluated using a gas chromatograph for the polar gas analysis (GC323, GL Sciences Inc., Tokyo, Japan) according to the published procedure [50].
The membrane performance under the H2-N2 (2:1) mixed feed gas flow at p/p0 (H2O) = 1.0 was assessed in terms of the separation factor (SF):
S F = Y A / Y B X A / X B
where Y and X are the mass fractions of permeate and feed, respectively and subscripts A and B denote H2 and N2, respectively.
To examine the hydrogen affinity of the AHPCS-derived SiCH organic–inorganic hybrids, the amount of H2 adsorption onto a thin film of the AHPCS-derived hybrid was measured using a quartz-crystal microbalance (QCM), which is one of the useful methods for detecting in-situ minute mass changes [52]. Commercially available quartz crystal unit (SEN-9E-H-10, Tamadevice Co., Ltd., Kawasaki, Japan) connected with a crystal oscillator circuit (Tamadevice Co. Ltd., Kawasaki, Japan), power supply (GPS-S, GW Instek, Texio Technology Co., Yokohama, Japan) and frequency counter (SC-7205A, UNIVERSALCOUNTER, Iwatsu Electric Co., Ltd., Tokyo, Japan) were used, and the measurement system shown in Figure 1 was set-up at our laboratory.
The sample film was formed on the quartz crystal unit surface using the dry xylene solution of as-received AHPCS under the same manner as mentioned for the 300 °C-synthesized membrane. The sample film on the quartz crystal unit was placed in a four-necked round-bottom glass flask. Then, the temperature inside the flask was precisely adjusted at 30 °C (±0.1 °C) by a styrofoam-covered mantle heater operated by the PID control. The sample film was exposed to He atmosphere maintained by a continuous He gas flow at 30 mL min−1. After 15 h, the frequency shift was measured for 90 ks to confirm that the He adsorption reached the equilibrium. Then, the weight change measurement under a H2 flow (30 mL min−1) was started by switching the feed gas from He to H2, and the weight change was monitored for an additional 90 ks. The measurement system was controlled by a standard PC with a software (Labview, National Instruments Corp., Austin, TX, USA) for recording the transition of the frequencies corresponding to the mass change.
Conversion from the measured frequency shift Δf (Hz) to the mass change Δm (g) was calculated using the Sauerbrey equation [53],
Δ f = 2 f 0 2 μ q   ρ q   Δ m A e
where, f0 is the frequency of the quartz crystal prior to a mass change (9.0 × 106 (Hz)), μq is the shear modulus of quartz (2.947 × 1013 (g m−1 s−2)), ρq is the density of quartz (2.648 (g cm−3)) and Ae is the electrode area (3.93 × 10−5 (m2)).

3. Results and Discussion

3.1. Heat Treatment Temperatures Selected for Highly Cross-Linked SiCH Organic–Inorganic Hybrid Synthesis

Chemical structure and molecular distribution of the AHPCS are shown in Figures S1 and S2, respectively, in the electric supplementary information (ESI). In this study, the SiCH hybrid polymer of AHPCS was converted into the highly cross-linked SiCH organic–inorganic hybrid as a component of the hydrogen separation membrane. The temperatures for thermal conversion of AHPCS to highly cross-linked SiCH hybrid in this study was selected as 300, 400 and 500 °C based on the results obtained by the TG-MS analyses (Figures S3 and S4 in ESI) as well as FT-IR and Raman spectroscopic analyses for the heat-treated AHPCSs (Figures S5 and S6 in ESI). The thermal behavior of AHPCS has been already studied by several research groups [42,54,55,56,57,58], and the results obtained in this study were well consistent with those previously reported: As shown in Figure S2, as-received AHPCS had a considerable amount of low molecular weight fraction below 1000. TG-MS analyses revealed the thermal decomposition of the low molecular weight fraction proceeded during the first weight loss at 100–300 °C and a second one from 350 to 500 °C by detecting gaseous species assigned to the fragments of carbosilane species (Figures S3 and S4). On the other hand, thermal cross-linking was observed up to 300 °C for the formation of ≡Si-CH2-CH2-CH2-Si≡ and/or ≡Si-CH(CH3)-CH2-Si≡ via hydrosilylation between ≡Si-H and ≡Si-CH2-CH=CH2 groups in AHPCS, which was identified by the disappearance of the FT-IR absorption band at 1629 cm−1 attributed to the C=C bond of the allyl group [55,56] associated with the decrease in the relative FT-IR band intensities assigned to ν(Si-H) at 2123 cm−1 and δ(Si-H) at 947 cm−1 [55,56] (Figure S5). At 400–700 °C, formation of ≡Si-Si≡ between Si-H and Si-CH3 groups [42] was suggested by detecting gaseous species at the m/z ratio of 15 assigned to methane (CH4; Figure S4b). Since the thermal decomposition and cross-linking contentiously proceeded at 300–500 °C, the quantity of organic groups and microporosity of the SiCH hybrid differed depending on the specific heat treatment temperature in this temperature range. On the other hand, the FT-IR spectrum for the 700 °C-heat treated AHPCS revealed that polymer/inorganic silicon carbide conversion almost completed (Figure S5). It should be noted that the samples heat-treated at 300–500 °C were identified as the ternary SiCH Class II hybrid without graphite-like carbon, since the Raman spectra of these samples exhibited several peaks due to the organic groups without those attributed to graphite-like carbon typically detected at 1347.5 and 1596.5 cm−1 assigned as D-band (for disordered graphite) and G-band (for the sp2 graphite network), respectively [59,60] (Figure S6). Based on these results, the heat treatment of AHPCS was achieved at 300, 400 and 500 °C for the synthesis of powder and membrane samples.

3.2. Hydrophobicity

The water vapor adsorption–desorption isotherms at 25 °C measured for the powder samples are shown in Figure 2. The AHPCS heat-treated at 300 and 400 °C generated a type III isotherm [61,62], which showed a weak interaction to water molecule. The maximum amount of the water adsorption ((Va(H2O)) of these samples was below 2 cm3(STP) g−1. The 500 °C-heat treated AHPCS also showed relatively high hydrophobicity, and the Va(H2O) remained at 6.3 cm3 (STP) g−1.
The Va(H2O) values evaluated for the AHPCS-derived SiCH were much lower than that of highly hydrophilic mesoporous γ-Al2O3 (297 cm3 (STP) g−1) characterized in our previous study [50].
On the other hand, the 700 °C-heat treated AHPCS presented a type V [61,62]-like isotherm with a large open loop of hysteresis at p/p0 (H2O) above 0.3, and the Va(H2O) reached 42.5 cm3 (STP) g−1. As shown in Figure S5, the thermal decomposition of the organic groups in AHPCS was almost completed at 700 °C, which led to the analyzed hydrophilic character.

3.3. Properties of SiCH Hybrid/γ-Al2O3 Composite Membrane

(1)
Structure of the composite membrane
As a typical observation, Figure 3a presents a cross-sectional SEM image of a supported γ-Al2O3 membrane after dip coating of the AHPCS xylene solution and subsequent heat treatment at 400 °C under flowing Ar. There was no additional layer on the γ-Al2O3 membrane surface. Then, an EDS analysis was performed on the modified membrane. As shown in Figure 3b, the line scan of the EDS mapping for Si derived form AHPCS was detected within the γ-Al2O3 membrane having approximately 2.5 μm thickness. Accordingly, the resulting composite membranes in this study were composed of γ-Al2O3 with mesopore channels infiltrated by the AHPCS-derived SiCH hybrid.
(2)
Gas permeation behaviors under dry condition
Arrhenius plots of He, H2 and N2 permeances evaluated for the SiCH hybrid/γ-Al2O3 composite membranes synthesized at 300, 400 and 500 °C are shown in Figure 4a–c, respectively. Despite the low permeation temperature of 25 °C, the composite membranes exhibited a relatively high H2 permeance of 1 × 10−7 to 4 × 10−6 mol m−2 s−1 Pa−1 with a H2/N2 permselectivity (α(H2/N2)) of 9.2–17, apparently higher than that of the theoretical one (3.73) based on the Knudsen’s diffusion.
The gas permeation behavior through each composite membrane was similar, and all the gas permeances increased linearly with the permeation temperature and thus followed the Arrhenius law. Since the gas permeations through the supported mesoporous γ-Al2O3 membrane exhibited a typical Knudsen’s diffusion characteristics in our previous study [50], the gas permeation behaviors observed for the present composite membranes suggested that all the gases permeated through the microporous SiCH hybrid, which filled in the mesopore channels of the γ-Al2O3, and the dominant mechanism for the gas permeations was activated diffusion. However, at all permeation temperatures from 25 to 80 °C, the composite membranes exhibited a unique α(H2/He) of 1.44–1.95, which was higher than the theoretical one (1.41) based on the Knudsen’s diffusion.
To highlight this unique gas permeation behavior, the gas permeances measured at 50 °C were characterized and are shown in Figure 5 by plotting the kinetic diameter dependence of the normalized gas (i) permeance relative to the He permeance (Qi/QHe), and compared with the ideal value (QK,i/QK,He) by the Knudsen model [63,64],
Q K , i Q K , He = M He M i            
where Mi and MHe are molecular weights of gas-i and He, respectively.
The apparent activation energies for He and H2 permeations were evaluated by the Arrhenius plot (Figure 4) and are listed in Table 1. The apparent activation energy (Ea) for He permeation was 20.3–1.4 kJ mol−1, while that for H2 permeation was 17.0–0.5 kJ mol−1.
The Ea values for both He and H2 permeations decreased with the composite membrane synthesis temperature. This tendency was well consistent with the result of TG-MS analyses (Figures S3 and S4) and the gas permeation behaviors (Figure 4): weight loss due to the volatilization of the low molecular weight fraction of as-received AHPCS contentiously proceeded at 300–500 °C (Figure S4), and resulting yields of the SiCH hybrid at 300, 400 and 500 °C were measured to be 87%, 83% and 76%, respectively (Figure S3), while all the gas permeances through the composite membrane increased with the synthesis temperature (Figure 4). Thus, the observed Ea values for He and H2 permeations could depend on the density of the AHPCS-derived SiCH organic–inorganic hybrid network. However, a unique point was that, regardless of the synthesis temperature, the Ea for H2 permeation was found to be smaller than that for He permeation, which was a clear contrast to those evaluated for the H2-selecitve microporous amorphous silica membranes [10,11,65,66,67]. Then, an attempt was made for study on the hydrogen affinity of the AHPCS-derived SiCH organic–inorganic hybrid: The amount of H2 adsorption on the AHPCS-derived SiCH film was measured by using a quartz-crystal microbalance (QCM). The SiCH sample film was formed on the quartz crystal unit surface by following the procedure for the composite membrane synthesis at 300 °C (effective film area corresponded to Ae in Equation (2), 3.93 × 10−5 m2). The sample film was exposed to He atmosphere under the strictly regulated isothermal condition at 30 °C (±0.1 °C) for more than 90 ks. After the He adsorption reached equilibrium, weight gain was monitored by exposing the sample film to H2 atmosphere under the same isothermal condition. As shown in Figure 6, the weight gain increased with H2 exposure time and reached 7.14 ng (1.82 × 10−4 g m−2) after the additional 88,130 s. Since the molecular weight of H2 (2.016) was approximately one-half of He (4.002), the weight gain measured under the H2 atmosphere revealed preferential adsorption of H2 relative to He, i.e., existence of H2 affinity of the AHPCS-derived SiCH organic–inorganic hybrid, which might contribute to the experimentally observed unique α(H2/He) > 1.41 and high H2 permeances (10−7–10−6 mol m−2 s−1 Pa−1 order at 25–80 °C).
(3)
Gas permeation behaviors under the wet condition
For study on the potential application to the solar hydrogen production system, the gas permeation measurement was performed on the composite membranes by using a mixed H2-N2 feed gas in the molar ratio 2:1 under dry and saturated water vapor partial pressure (p/p0 (H2O) = 1) at 50 °C. The results are summarized and shown in Figure 7. The composite membranes were found to be water vapor permeable and the permeance was measured to be 2.7–3.8 × 10−7 mol m−2 s−1 Pa−1.
The α(H2/N2) of the composite membranes was 6.0–11.3, and regardless of the synthesis temperature, there was no significant degradation under the highly humid condition at 50 °C. The 300 °C-synthesized composite membrane kept relatively high gas permeances. The retentions evaluated for the H2 and N2 permeances under the p/p0 (H2O) = 1 at 50 °C were 69 and 67%, respectively. However, with increasing synthesis temperature, the permeance retention of both H2 and N2 decreased, in other words, the hydrophobicity in terms of stable gas permeation property degraded with the synthesis temperature. This degradation tendency is consistent with the temperature dependence of the SiCH hybrid polymer/highly cross-linked SiCH hybrid conversion yield as described above, and thus is related to the quantity of organic groups remained in the SiCH hybrid and the microporosity or volume of the SiCH hybrid, which infiltrated the mesopore channels of the composite membrane.
Then, the 500 °C-synthesized composite membrane was further modified with polycarbosilane (PCS) by the 120 °C-melt impregnation established by our previous study [50]. As shown in Figure 7, under the dry condition at 50 °C, the PCS-modified composite membrane showed a relatively high H2 permeance of 8.4 × 10−7 mol m−2 s−1 Pa−1 with a significantly improved α(H2/N2) of 29.6. Moreover, under the p/p0 (H2O) = 1 at 50 °C, the PCS-modification successfully improved the membrane performance: H2 permeance and α(H2/N2) were measured to be 3.5 × 10−7 mol m−2 s−1 Pa−1 and 36, respectively.
Gas permeation properties under the wet condition at 50 °C of the composite membranes were also assessed by cyclic gas permeance measurements under p/p0(H2O) ranging from 0.1 to 1.0 and compared with those of the supported mesoporous γ-Al2O3 membrane itself. As shown in Figure 8a, H2 and N2 permeances through the supported mesoporous γ-Al2O3 membrane drastically decreased above p/p0(H2O) = 0.74. This degradation is due to the highly hydrophilic property of γ-Al2O3, which leads to the blockage of the gas permeable mesopore channels by adsorption and subsequent condensation of water molecules as the permeate [50]. On the other hand, the 300 °C-synthesized composite membrane exhibited stable gas permeations at all the p/p0(H2O) up to 1.0 (Figure 8b). A slight decrease in the gas permeances at p/p0(H2O) > 0.74 was due to the pressure-drop caused by the water vapor condensation within the mesopore channels of hydrophilic γ-Al2O3 partly remained without surface modification with the AHPCS-derived hydrophobic hybrid. The 500 °C-synthesized composite membrane also showed the decreasing tendency in gas permeances, however further modification with PCS successfully improved the membrane performance at the final gas permeation measurement under the saturated humidity at 50 °C: H2 permeance remained at 10−7 mol m−2 s−1 Pa−1 order with α(H2/N2) > 30 under (Figure 8c), and the resulting separation factor (SF) evaluated based on the gas permeation data shown in Table 2 was found as 26.
Moreover, the polymer-derived SiCH organic–inorganic hybrid investigated in this study showed sufficient stability under the present high humidity conditions at 50 °C: Figure 9 presents the top surface view of the 500 °C-synthesized composite membrane modified with PCS before and after the cyclic gas permeation measurements under p/p0(H2O) up to 1.0 at 50 °C. Compared with the surface of the as-synthesized mesoporous γ-Al2O3 membrane over an α-Al2O3 porous support (Figure 9a), the composite membrane exhibited a smooth surface (Figure 9b) and kept the surface without structural degradation after the cyclic gas permeation measurements (Figure 9c). These results revealed that, in addition to hydrogen permselectivity, the modification with the polymer-derived SiCH organic–inorganic hybrid investigated in this study greatly improved the hydrophobicity in terms of stable gas permeations under the saturated water vapor partial pressure at 50 °C.
The H2-permselectivities of the composite membrane measured in this study were briefly compared with those recently reported for other membranes composed of various materials systems, and their H2 permeation data with α(H2/X) (X = N2 (0.364 nm) [51] or O2 (0.346 nm) [51]) measured under the dry condition at T ≤ 50 °C are listed in Table 3 [18,68,69,70,71,72,73,74,75,76,77,78]. Among them, novel ultrathin (9 nm thickness) graphene oxide membrane formed on an anodic oxidized alumina support (#09) exhibited a H2 permeance of approximately 1 × 10−7 mol m−2 s−1 Pa−1 with α(H2/N2) of 900 at 20 °C [75,76]. The zeolite imidazolate framework (ZIF) nanosheet membrane (#08) also showed H2 permeance of 2.04 × 10−7 mol m−2 s−1 Pa−1 with high α(H2/N2) of 66.6 at 30 °C [73,74]. Among other practical membranes, SiO2-based organic–inorganic hybrid membrane (#03) showed the highest H2 permeance of 10−6 mol m−2 s−1 Pa−1 order, while the α(H2/N2) remained at 12 [68]. On the other hand, zeolite/CMC (carbon molecular sieve) composite membranes (#04, #05) showed a high α(H2/N2) of 61-100.2, however the H2 permeance at 30 °C was 10−9–10−8 mol m−2 s−1 Pa−1 order [69,70].
As shown in Figure 4 and Figure 5, in addition to the H2/N2 selectivity, the present composite membranes exhibited unique H2/He selectivity due to the H2 affinity of the AHPCS-derived highly cross-linked SiCH organic–inorganic hybrid in the composite membrane (Figure 6). This unique H2 preferential permeation property contributed to relatively high H2 permeance of 8.4 × 10−7 mol m−2 s−1 Pa−1 with α(H2/N2) of 29.6.
For the application of the purification of solar hydrogen, the long-term stability and robustness of H2-selecitve membranes under the humid condition at around 50 °C are practical issues for us to pursue. In this context, there are few reports as mentioned above, and Oyama et al. reported [18] their pioneering study on the stability of PFDA-based liquid membrane (#06 in Table 3) under the humid condition (10 mol%) at 30 °C as a simulated condition for the purification of solar hydrogen, and they confirmed its stability for up to 48 h. The stabilities of the composited membranes characterized by the primary accelerated degradation test (Figure 7, Figure 8 and Figure 9) were compatible with that of the supported liquid membrane (#06 in Table 3) [18]. Under the scheme of the current NEDO R&D “Artificial Photosynthesis” Project, we plan to conduct the long-term stability test for the composite membranes by using a H2-O2 (2:1) mixed feed gas as a simulated syngas at the project facility with safety measures against explosion.

4. Conclusions

In this study, AHPCS was converted to highly cross-linked ternary SiCH organic–inorganic hybrid compounds by heat treatment at 300–500 °C under Ar atmosphere. The water vapor adsorption–desorption isotherm measurement revealed that the AHPCS-derived highly cross-linked SiCH hybrids exhibited excellent hydrophobicity, and the maximum amount of water vapor adsorption at 25 °C was 1.5–6.3 cm3 (STP) g−1.
Aiming to develop H2-selective membranes for the application of the novel solar hydrogen production system, a supported mesoporous γ-Al2O3 membrane with a thickness of about 2.5 μm was modified with AHPCS xylene solution and subsequently heat-treated at 300–500 °C under Ar atmosphere. SEM observation revealed that the mesoporous channels of the γ-Al2O3 membrane were coated by the AHPCS-derived SiCH to afford a SiCH hybrid/γ-Al2O3 composite membrane. Even at a low temperature of 25 °C, the composite membranes exhibited a high H2 permeance of 1 × 10−7 to 4 × 10−6 mol m−2 s−1 Pa−1 and a α(H2/N2) of 9.2–17 together with a unique α(H2/He) of 1.44–1.95.
The apparent activation energy for the H2 permeation at 25–80 °C was 17.0–0.5 kJ mol−1 and found to be smaller than that for He (20.3–1.4 kJ mol−1). Moreover, the measurement of H2 adsorption on an AHPCS-derived SiCH film by using a QCM revealed preferential H2 adsorption at 30 °C. These results strongly indicate a significant H2 affinity of the AHPCS-derived SiCH organic–inorganic hybrid, which contributes to the experimentally observed unique α(H2/He) and the high H2 permeance at 25–80 °C.
As a simulated wet condition for the purification of solar hydrogen, the gas permeation measurement under saturated water vapor partial pressure at 50 °C was performed on the composite membranes by using a mixed H2-N2 feed gas in the molar ratio 2:1. The 300–500 °C synthesized composite membranes exhibited a relatively high H2 permeance of 1.0–4.3 × 10−7 mol m−2 s−1 Pa−1 with a α(H2/N2) of 6.0–11.3. Further modification by the 120 °C-melt impregnation of PCS successfully improved the H2-permselectivity of the 500 °C synthesized composite membrane by maintaining the H2 permeance combination with improved α(H2/N2) as 3.5 × 10−7 mol m−2 s−1 Pa−1 and 36. These results clearly revealed a promising potential of polymer-derived SiCH organic–inorganic hybrids to develop advanced H2 selective membranes applicable to novel solar hydrogen production systems.

Supplementary Materials

The following are available online at https://0-www-mdpi-com.brum.beds.ac.uk/2077-0375/10/10/258/s1, Figure S1: Structure of commercially available allyl-hydrido-polycarbosilane (AHPCS), Figure S2: Molecular weight distribution of as-received AHPCS, Figure S3: Thermal behavior of as-received AHPCS. (a) TG curve and total ion current chromatogram (TICC) under flowing He, and typical mass spectra recorded during (b) the first weight loss from100 to 250 °C and (c) the second weight loss from 350 to 500 °C, Figure S4: Continuous in-situ monitoring of gaseous species by mass spectrometry: (a) Fragments derived from low molecular weight fraction of as-received AHPCS during the first weight loss from 100 to 300 °C and the second one from 350 to 500 °C and (b) methane (CH4) at 400 to 700 °C. (c) Fragments suggested for gaseous spices derived from low molecular weight fraction of as-received AHPCS (Equation (1)), m/z = 42 ((CH2)3) from AHPCS after cross-linking via hydrosilylation between ≡Si-H and CH2=CH-CH2-Si≡ (Equations (2) and (3)) and m/z = 15 (CH4) due to the thermal crosslinking between ≡Si-H and ≡Si-CH3 groups to afford ≡Si-Si≡ above 350 °C (Equation (4)) [42], Figure S5: FT-IR spectra for as-received AHPCS and those after heat treatment at 300 to 700 °C in Ar, Figure S6: Raman spectra for as-received and those AHPCS after heat treatment at 300 to 500 °C in Ar. Spectra indicated the heat-treated samples were free from graphite-like carbon typically detected at 1347.5 and 1596.5 cm−1 attributed to the D-band (for disordered graphite) and G-band (for the sp2 graphite network), respectively [59,60].

Author Contributions

Conceptualization, M.K. (Miwako Kubo) and Y.I.; methodology, Y.D. and E.I.; investigation, R.M., M.K. (Misako Kojima) and K.N.; Formal analysis, S.H.; writing—original draft preparation, M.K. (Miwako Kubo) and Y.I.; writing—review and editing, S.B. and R.R.; visualization, supervision and funding acquisition, Y.I. All authors have read and agreed to the published version of the manuscript.

Funding

This work was in part supported by “Research Project for Future Development: Artificial Photosynthetic Chemical Process (ARPChem)” (METI/NEDO, Japan: 2012-2022). Samuel Bernard and Yuji Iwamoto would like to thank CNRS who financially supported present work via the International Research Project (IRP) ‘Ceramics materials for societal challenges’.

Conflicts of Interest

The authors declare no conflict of interest.

Nomenclature

Amembrane area, m2
Aeelectrode area, m2
Eaactivation energy, kJ mol−1
Dfmeasured frequency shift, Hz
f0frequency of quartz crystal prior to a mass change, Hz
Δmmass change, g
Mimolecular weights of gas-i, kg mol−1
p/p0 (H2O)relative pressure of water vapor, dimensionless
pHpressures of gas feed side, Pa
pLpressures of gas permeate side, Pa
Qipermeance of gas-i, mol m−2 s−1 Pa−1
QK,iKnudsen permeance of gas-i, mol m−2 s−1 Pa−1
Vpermeate molar flow rate, mol s−1
Va(H2O)maximum amount of water adsorption, cm3(STP) g−1

Greek Symbols

αpermselectivity, dimensionless
ρqshear modulus of quartz, g m−1 s−2
μqdensity of quartz, g cm−3

Abbreviations

AHPCSallyl-hydro-polycarbosilane
BTESE1,2-bis(triethoxysilyl)ethane
BTESMbis(triethoxysilyl)methane
CMScarbon molecular sieve
EAethanoanthracene
MOFmetal organic framework
PCSpolycarbosilane
PDCsPolymer-Derived Ceramics
PDSpolydimethylsilane
PECphotoelectrochemical
PFDA1H,1H,2H,2H-perfluorodecyl acrylate
PIMpolymers of intrinsic microporosity
QCMquartz-crystal microbalance
SFseparation factor
STPstandard temperature and pressure (273.15 K and 101.30 kPa)
THFtetrahydrofuran
TB6H,12H-5,11-methanodibenzo[b,f][1,5]diazocine (Tröger’s base)
Triptriptycene
ZIFzeolite imidazolate framework

References

  1. Ogden, J.M.; Williams, R.H.; Larson, E.D. Societal lifecycle costs of cars with alternative fuels/engines. Energy Policy 2004, 32, 7–27. [Google Scholar] [CrossRef]
  2. Maeda, K.; Domen, K. New non-oxide photocatalysts designed for overall water splitting under visible light. J. Phys. Chem. C 2007, 111, 7851–7861. [Google Scholar] [CrossRef]
  3. Wang, Q.; Hisatomi, T.; Jia, Q.; Tokudome, H.; Zhong, M.; Wang, C.; Pan, Z.; Takata, T.; Nakabayashi, M.; Shibata, N. Scalable water splitting on particulate photocatalyst sheets with a solar-to-hydrogen energy conversion efficiency exceeding 1%. Nat. Mater. 2016, 15, 611–615. [Google Scholar] [CrossRef] [PubMed]
  4. Goto, Y.; Hisatomi, T.; Wang, Q.; Higashi, T.; Ishikiriyama, K.; Maeda, T.; Sakata, Y.; Okunaka, S.; Tokudome, H.; Katayama, M.; et al. A Particulate Photocatalyst Water-Splitting Panel for Large-Scale Solar Hydrogen Generation. Joule 2018, 2, 509–520. [Google Scholar] [CrossRef] [Green Version]
  5. Yamada, T.; Domen, K. Development of Sunlight Driven Water Splitting Devices towards Future Artificial Photosynthetic Industry. ChemEngineering 2018, 2, 36. [Google Scholar] [CrossRef] [Green Version]
  6. Development of Basic Chemical Processes for Carbon Dioxide as Raw Material. Available online: www.nedo.go.jp/activities/EV_00296.html (accessed on 2 August 2020).
  7. Yagyu, S.; Matsui, H.; Matsuda, T.; Yasumoto, H. Studies of Explosive Characteristics of Hydrogen (1st Report); RIIS-RR-18-1; Ministry of Labour, the Research Institute of Industrial Safety, 1969. Available online: www.jniosh.johas.go.jp/publication/doc/rr/RR-18-1.pdf (accessed on 2 August 2020).
  8. Tanaka, K.; Sakata, Y. Present and Future Prospects of Hydrogen Production Process Constructed by the Combination of Photocatalytic H2O Splitting and Membrane Separation Process. Membrane 2011, 36, 113–121. [Google Scholar] [CrossRef]
  9. Oyama, S.T.; Stagg-Williams, S.M. Inorganic, Polymeric and Composite Membranes: Structure, Function and Other Correlations; Elsevier: Amsterdam, The Netherlands, 2011. [Google Scholar]
  10. Mise, Y.; Ahn, S.J.; Takagaki, A.; Kikuchi, R.; Oyama, S.T. Fabrication and evaluation of trimethylmethoxysilane (TMMOS)-derived membranes for gas separation. Membranes 2019, 9, 123. [Google Scholar] [CrossRef] [Green Version]
  11. Kato, H.; Lundin, S.-T.B.; Ahn, S.-J.; Takagaki, A.; Kikuchi, R.; Oyama, S.T. Gas Separation Silica Membranes Prepared by Chemical Vapor Deposition of Methyl-Substituted Silanes. Membranes 2019, 9, 144. [Google Scholar] [CrossRef] [Green Version]
  12. Ted Oyama, S.; Aono, H.; Takagaki, A.; Sugawara, T.; Kikuchi, R. Synthesis of silica membranes by chemical vapor deposition using a dimethyldimethoxysilane precursor. Membranes 2020, 10, 50. [Google Scholar] [CrossRef] [Green Version]
  13. Yun, S.; Ted Oyama, S. Correlations in palladium membranes for hydrogen separation: A review. J. Membr. Sci. 2011, 375, 28–45. [Google Scholar] [CrossRef]
  14. Liguori, S.; Iulianelli, A.; Dalena, F.; Pinacci, P.; Drago, F.; Broglia, M.; Huang, Y.; Basile, A. Performance and long-term stability of Pd/PSS and Pd/Al2O3 membranes for hydrogen separation. Membranes 2014, 4, 143–162. [Google Scholar] [CrossRef] [PubMed]
  15. Alique, D.; Martinez-Diaz, D.; Sanz, R.; Calles, J.A. Review of supported Pd-based membranes preparation by electroless plating for ultra-pure hydrogen production. Membranes 2018, 8, 5. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  16. Castro-Dominguez, B.; Leelachaikul, P.; Takagaki, A.; Sugawara, T.; Kikuchi, R.; Oyama, S.T. Supported perfluorotributylamine liquid membrane for H2/O2 separation. J. Memb. Sci. 2013, 448, 262–269. [Google Scholar] [CrossRef]
  17. Leelachaikul, P.; Castro-Dominguez, B.; Takagaki, A.; Sugawara, T.; Kikuchi, R.; Oyama, S.T. Perfluorooctanol-based liquid membranes for H2/O2 separation. Sep. Purif. Technol. 2014, 122, 431–439. [Google Scholar] [CrossRef]
  18. Yamaguchi, T.; Takagaki, A.; Sugawara, T.; Kikuchi, R.; Oyama, S.T. Supported fluorocarbon liquid membranes for hydrogen/oxygen separation. J. Membr. Sci. 2016, 520, 272–280. [Google Scholar] [CrossRef]
  19. Burneau, A.; Lepage, J.; Maurice, G. Porous silica-water interactions. I. Structural and dimensional changes induced by water adsorption. J. Non-Cryst. Solids 1997, 217, 1–10. [Google Scholar] [CrossRef]
  20. Tsuru, T.; Hino, T.; Yoshioka, T.; Asaeda, M. Permporometry characterization of microporous ceramic membranes. J. Membr. Sci. 2001, 186, 257–265. [Google Scholar] [CrossRef]
  21. Díaz, U.; Corma, A. Organic-Inorganic Hybrid Materials: Multi-Functional Solids for Multi-Step Reaction Processes. Chem.-A Eur. J. 2018, 24, 3944–3958. [Google Scholar] [CrossRef]
  22. Mir, S.H.; Nagahara, L.A.; Thundat, T.; Mokarian-Tabari, P.; Furukawa, H.; Khosla, A. Review—Organic-Inorganic Hybrid Functional Materials: An Integrated Platform for Applied Technologies. J. Electrochem. Soc. 2018, 165, B3137–B3156. [Google Scholar] [CrossRef]
  23. Bill, J.; Aldinger, F. Precursor-derived Covalent Ceramics. Adv. Mater. 1995, 7, 775–787. [Google Scholar] [CrossRef]
  24. Riedel, R. Advanced Ceramics from Inorganic Polymers. In Materials Science and Technology; Brook, R.J., Ed.; Wiley-VCH: Weinheim, Germany, 1996; Volume 17B, pp. 1–50. [Google Scholar]
  25. Judeinstein, P.; Sanchez, C. Hybrid organic–inorganic materials: A land of multidisciplinarity. J. Mater. Chem. 1996, 6, 511–525. [Google Scholar] [CrossRef]
  26. Yajima, S.; Hayashi, J.; Omori, M. Continuous silicon carbide fiber of high tensile strength. Chem. Lett. 1975, 4, 931–934. [Google Scholar] [CrossRef]
  27. Yajima, S.; Okamura, K.; Hayashi, J.; Omori, M. Synthesis of Continuous SiC Fibers with High Tensile Strength. J. Am. Ceram. Soc. 1976, 59, 324–327. [Google Scholar] [CrossRef]
  28. Colombo, P.; Mera, G.; Riedel, R.; Sorarù, G.D. Polymer-derived ceramics: 40 Years of research and innovation in advanced ceramics. J. Am. Ceram. Soc. 2010, 93, 1805–1837. [Google Scholar] [CrossRef]
  29. Hotza, D.; Di Luccio, M.; Wilhelm, M.; Iwamoto, Y.; Bernard, S.; Diniz da Costa, J.C. Silicon carbide filters and porous membranes: A review of processing, properties, performance and application. J. Membr. Sci. 2020, 610, 118193. [Google Scholar] [CrossRef]
  30. Lee, L.-L.; Tsai, D.-S. A Hydrogen-Permselective Silicon Oxycarbide Membrane Derived from Polydimethylsilane. J. Am. Ceram. Soc. 1999, 82, 2796–2800. [Google Scholar] [CrossRef]
  31. Shelekhin, A.B.; Grosgogeat, E.J.; Hwang, S.T. Gas separation properties of a new polymer/inorganic composite membrane. J. Membr. Sci. 1992, 66, 129–141. [Google Scholar] [CrossRef]
  32. Kusakabe, K.; Yan Li, Z.; Maeda, H.; Morooka, S. Preparation of supported composite membrane by pyrolysis of polycarbosilane for gas separation at high temperature. J. Membr. Sci. 1995, 103, 175–180. [Google Scholar] [CrossRef]
  33. Li, Z.; Kusakabe, K.; Morooka, S. Preparation of thermostable amorphous Si-C-O membrane and its application to gas separation at elevated temperature. J. Membr. Sci. 1996, 118, 159–168. [Google Scholar] [CrossRef]
  34. Li, Z.; Kusakabe, K.; Morooka, S. Pore Structure and Permeance of Amorphous Si-C-O Membranes with High Durability at Elevated Temperature. Sep. Sci. Technol. 1997, 32, 1233–1254. [Google Scholar] [CrossRef]
  35. Suda, H.; Yamauchi, H.; Uchimaru, Y.; Fujiwara, I.; Haraya, K. Preparation and gas permeation properties of silicon carbide-based inorganic membranes for hydrogen separation. Desalination 2006, 193, 252–255. [Google Scholar] [CrossRef]
  36. Nagano, T.; Sato, K.; Saitoh, T.; Iwamoto, Y. Gas permeation properties of amorphous SiC membranes synthesized from polycarbosilane without oxygen-curing process. J. Ceram. Soc. Jpn. 2006, 114, 533–538. [Google Scholar] [CrossRef] [Green Version]
  37. Takeyama, A.; Sugimoto, M.; Yoshikawa, M. Gas permeation property of SiC membrane using curing of polymer precursor film by electron beam irradiation in helium atmosphere. Mater. Trans. 2011, 52, 1276–1280. [Google Scholar] [CrossRef] [Green Version]
  38. Elyassi, B.; Deng, W.; Sahimi, M.; Tsotsis, T.T. On the use of porous and nonporous fillers in the fabrication of silicon carbide membranes. Ind. Eng. Chem. Res. 2013, 52, 10269–10275. [Google Scholar] [CrossRef]
  39. Dabir, S.; Deng, W.; Sahimi, M.; Tsotsis, T. Fabrication of silicon carbide membranes on highly permeable supports. J. Membr. Sci. 2017, 537, 239–247. [Google Scholar] [CrossRef]
  40. Ciora, R.J.; Fayyaz, B.; Liu, P.K.T.; Suwanmethanond, V.; Mallada, R.; Sahimi, M.; Tsotsis, T.T. Preparation and reactive applications of nanoporous silicon carbide membranes. Chem. Eng. Sci. 2004, 59, 4957–4965. [Google Scholar] [CrossRef]
  41. Sandra, F.; Ballestero, A.; NGuyen, V.L.; Tsampas, M.N.; Vernoux, P.; Balan, C.; Iwamoto, Y.; Demirci, U.B.; Miele, P.; Bernard, S. Silicon carbide-based membranes with high soot particle filtration efficiency, durability and catalytic activity for CO/HC oxidation and soot combustion. J. Membr. Sci. 2016, 501, 79–92. [Google Scholar] [CrossRef]
  42. Wang, Q.; Yokoji, M.; Nagasawa, H.; Yu, L.; Kanezashi, M.; Tsuru, T. Microstructure evolution and enhanced permeation of SiC membranes derived from allylhydridopolycarbosilane. J. Membr. Sci. 2020, 118392. [Google Scholar] [CrossRef]
  43. Interrante, L.V.; Shen, Q. Polycarbosilanes. In Silicon-Containing Polymers; Jones, R.G., Ando, W., Chojnowski, J., Eds.; Kluwer Academic Publisher: Dordrecht, The Netherlands, 2000; pp. 247–321. [Google Scholar]
  44. Matsumoto, K. Polycarbosilanes. In Encyclopedia of Polymer Science and Technology; Mark, H.F., Ed.; John Wiley & Sons: New York, NY, USA, 2003; Volume 7, pp. 426–438. [Google Scholar]
  45. Matsumoto, K.; Endo, T. Synthesis and ring-opening polymerization of functional silacyclobutane derivatives and their application to lithium ion batteries. Macromol. Symp. 2015, 349, 21–28. [Google Scholar] [CrossRef]
  46. Yajima, S.; Shishido, T.; Okamira, K. SiC Bodies Sintered with Three-Dimensional Cross-Linked Polycarbosilane. Am. Ceram. Soc. Bull. 1977, 56, 1060–1063. [Google Scholar]
  47. Kim, Y.-W.; Lee, J.-G. Effect of polycarbosilane addition on mechanical properties of hot-pressed silicon carbide. J. Mater. Sci. 1992, 27, 4746–4750. [Google Scholar] [CrossRef]
  48. Czubarow, P.; Seyferth, D. Application of poly(methylsilane) and Nicalon® polycarbosilane precursors as binders for metal/ceramic powders in preparation of functionally graded materials. J. Mater. Sci. 1997, 32, 2121–2130. [Google Scholar] [CrossRef]
  49. Sawai, Y.; Iwamoto, Y.; Okuzaki, S.; Yasutomi, Y.; Kikuta, K.; Hirano, S. Synthesis of Silicon Carbide Ceramics Using Chemically Modified Polycarbosilanes as a Compaction Binder. J. Am. Ceram. Soc. 1999, 82, 2121–2125. [Google Scholar] [CrossRef]
  50. Kubo, M.; Kojima, M.; Mano, R.; Daiko, Y.; Honda, S.; Iwamoto, Y. A hydrostable mesoporous γ-Al2O3 membrane modified with Si–C–H organic-inorganic hybrid derived from polycarbosilane. J. Membr. Sci. 2020, 598, 117799. [Google Scholar] [CrossRef]
  51. Breck, D.W. Zeolite Molecular Sieves: Structure, Chemistry, and Use; John Wiley & Sons: New York, NY, USA, 1974; ISBN 978-0471099857. [Google Scholar]
  52. Buttry, D.A.; Ward, M.D. Measurement of Interfaclal Processes at Electrode Surfaces with the Electrochemical Quartz Crystal Microbalance. Chem. Rev. 1992, 92, 1355–1379. [Google Scholar] [CrossRef]
  53. Sauerbrey, G. Verwendung von Schwingquarzen zur Wägung dünner Schichten und zur Mikrowägung. Zeitschrift Für Physik 1959, 155, 206–222. [Google Scholar] [CrossRef]
  54. Sreeja, R.; Swaminathan, B.; Painuly, A.; Sebastian, T.V.; Packirisamy, S. Allylhydridopolycarbosilane (AHPCS) as matrix resin for C/SiC ceramic matrix composites. Mater. Sci. Eng. B Solid-State Mater. Adv. Technol. 2010, 168, 204–207. [Google Scholar] [CrossRef]
  55. Kaur, S.; Riedel, R.; Ionescu, E. Pressureless fabrication of dense monolithic SiC ceramics from a polycarbosilane. J. Eur. Ceram. Soc. 2014, 34, 3571–3578. [Google Scholar] [CrossRef]
  56. Wen, Q.; Xu, Y.; Xu, B.; Fasel, C.; Guillon, O.; Buntkowsky, G.; Yu, Z.; Riedel, R.; Ionescu, E. Single-source-precursor synthesis of dense SiC/HfCxN1-x-based ultrahigh-temperature ceramic nanocomposites. Nanoscale 2014, 6, 13678–13689. [Google Scholar] [CrossRef]
  57. Proust, V.; Bechelany, M.C.; Ghisleni, R.; Beaufort, M.F.; Miele, P.; Bernard, S. Polymer-derived Si-C-Ti systems: From titanium nanoparticle-filled polycarbosilanes to dense monolithic multi-phase components with high hardness. J. Eur. Ceram. Soc. 2016, 36, 3671–3679. [Google Scholar] [CrossRef]
  58. Schmidt, M.; Durif, C.; Acosta, E.D.; Salameh, C.; Plaisantin, H.; Miele, P.; Backov, R.; Machado, R.; Gervais, C.; Alauzun, J.G.; et al. Molecular-Level Processing of Si-(B)-C Materials with Tailored Nano/Microstructures. Chem.-A Eur. J. 2017, 23, 17103–17117. [Google Scholar] [CrossRef] [PubMed]
  59. Ferrari, A.C.; Robertson, J. Interpretation of Raman spectra of disordered and amorphous carbon. Phys. Rev. B 2000, 61, 14095–14107. [Google Scholar] [CrossRef] [Green Version]
  60. Pimenta, M.A.; Dresselhaus, G.; Dresselhaus, M.S.; Cançado, L.G.; Jorio, A.; Saito, R. Studying disorder in graphite-based systems by Raman spectroscopy. Phys. Chem. Chem. Phys. 2007, 9, 1276–1291. [Google Scholar] [CrossRef] [PubMed]
  61. Sing, K.S.W.; Everett, D.H.; Haul, R.A.W.; Moscou, L.; Pierotti, R.A.; Rouquerol, J.; Siemienieska, T. Reporting physisorption data for gas/solid systems with special reference to the determination of surface area and porosity. Pure Appl. Chem. 1985, 57, 603–619. [Google Scholar] [CrossRef]
  62. Lowell, S.; Shields, J.E.; Thomas, M.A.; Thommes, M. Characterization of Porous Solids and Powders; Springer: Dordrecht, The Netherlands, 2004. [Google Scholar]
  63. Lee, H.R.; Kanezashi, M.; Shimomura, Y.; Yoshioka, T.; Tsuru, T. Evaluation and fabrication of pore-size-tuned silica membranes with tetraethoxydimethyl disiloxane for gas separation. AIChE J. 2011, 57, 2755–2765. [Google Scholar] [CrossRef]
  64. Yoshioka, T.; Kanezashi, M.; Tsuru, T. Micropore size estimation on gas separation membranes: A study in experimental and molecular dynamics. AIChE J. 2013, 59, 2179–2194. [Google Scholar] [CrossRef]
  65. Lee, D.; Zhang, L.; Oyama, S.T.; Niu, S.; Saraf, R.F. Synthesis, characterization, and gas permeation properties of a hydrogen permeable silica membrane supported on porous alumina. J. Membr. Sci. 2004, 231, 117–126. [Google Scholar] [CrossRef]
  66. Gu, Y.; Oyama, S.T. High Molecular Permeance in a Poreless Ceramic Membrane. Adv. Mater. 2007, 19, 1636–1640. [Google Scholar] [CrossRef]
  67. Ahn, S.J.; Yun, G.N.; Takagaki, A.; Kikuchi, R.; Oyama, S.T. Synthesis and characterization of hydrogen selective silica membranes prepared by chemical vapor deposition of vinyltriethoxysilane. J. Membr. Sci. 2018, 550, 1–8. [Google Scholar] [CrossRef]
  68. Ren, X.; Tsuru, T. Organosilica-based membranes in gas and liquid-phase separation. Membranes 2019, 9, 107. [Google Scholar] [CrossRef] [Green Version]
  69. Li, L.; Wang, C.; Wang, N.; Cao, Y.; Wang, T. The preparation and gas separation properties of zeolite/carbon hybrid membranes. J. Mater. Sci. 2015, 50, 2561–2570. [Google Scholar] [CrossRef]
  70. Li, L.; Xu, R.; Song, C.; Zhang, B.; Liu, Q.; Wang, T. A review on the progress in nanoparticle/C hybrid CMS membranes for gas separation. Membranes 2018, 8, 134. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  71. Zeynali, R.; Ghasemzadeh, K.; Sarand, A.B.; Kheiri, F.; Basile, A. Performance evaluation of graphene oxide (GO) nanocomposite membrane for hydrogen separation: Effect of dip coating sol concentration. Sep. Purif. Technol. 2018, 200, 169–176. [Google Scholar] [CrossRef]
  72. Nouri, M.; Ghasemzadeh, K.; Iulianelli, A. Theoretical evaluation of graphene membrane performance for hydrogen separation using molecular dynamic simulation. Membranes 2019, 9, 110. [Google Scholar] [CrossRef] [Green Version]
  73. Li, Y.; Lin, L.; Tu, M.; Nian, P.; Howarth, A.J.; Farha, O.K.; Qiu, J.; Zhang, X. Growth of ZnO self-converted 2D nanosheet zeolitic imidazolate framework membranes by an ammonia-assisted strategy. Nano Res. 2018, 11, 1850–1860. [Google Scholar] [CrossRef]
  74. Fang, M.; Montoro, C.; Semsarilar, M. Metal and covalent organic frameworks for membrane applications. Membranes 2020, 10, 107. [Google Scholar] [CrossRef] [PubMed]
  75. Li, H.; Song, Z.; Zhang, X.; Huang, Y.; Li, S.; Mao, Y.; Ploehn, H.J.; Bao, Y.; Yu, M. Ultrathin, molecular-sieving graphene oxide membranes for selective hydrogen separation. Science 2013, 342, 95–98. [Google Scholar] [CrossRef] [PubMed]
  76. Huang, L.; Lin, H. Engineering sub-nanometer channels in two-dimensional materials for membrane gas separation. Membranes 2018, 8, 100. [Google Scholar] [CrossRef] [Green Version]
  77. Lasseuguette, E.; Malpass-Evans, R.; Carta, M.; McKeown, N.B.; Ferrari, M.C. Temperature and pressure dependence of gas permeation in a microporous Tröger’s base polymer. Membranes 2018, 8, 132. [Google Scholar] [CrossRef] [Green Version]
  78. Malpass-Evans, R.; Rose, I.; Fuoco, A.; Bernardo, P.; Clarizia, G.; McKeown, N.B.; Jansen, J.C.; Carta, M. Effect of bridgehead methyl substituents on the gas permeability of Tröger’s-base derived polymers of intrinsic microporosity. Membranes 2020, 10, 62. [Google Scholar] [CrossRef] [Green Version]
Figure 1. Schematic diagram of the weight change measurement with the quartz crystal microbalance (QCM).
Figure 1. Schematic diagram of the weight change measurement with the quartz crystal microbalance (QCM).
Membranes 10 00258 g001
Figure 2. Water vapor adsorption–desorption isotherms at 25 °C for SiCH inorganic–organic hybrid powder samples synthesized by heat treatment of AHPCS at 300–700 °C in Ar.
Figure 2. Water vapor adsorption–desorption isotherms at 25 °C for SiCH inorganic–organic hybrid powder samples synthesized by heat treatment of AHPCS at 300–700 °C in Ar.
Membranes 10 00258 g002
Figure 3. (a) A typical cross-sectional SEM image of the γ-Al2O3 membrane on a microporous α-Al2O3 support after modification with AHPCS and subsequent heat treatment at 400 °C in Ar. (b) Line scan of EDS mapping for Si derived from AHPCS detected within the mesoporous γ-Al2O3 membrane having a thickness of approximately 2.5 μm.
Figure 3. (a) A typical cross-sectional SEM image of the γ-Al2O3 membrane on a microporous α-Al2O3 support after modification with AHPCS and subsequent heat treatment at 400 °C in Ar. (b) Line scan of EDS mapping for Si derived from AHPCS detected within the mesoporous γ-Al2O3 membrane having a thickness of approximately 2.5 μm.
Membranes 10 00258 g003
Figure 4. Gas permeation behaviors under dry condition of the supported mesoporous γ-Al2O3 membrane after modification with AHPCS and subsequent heat treatment under flowing Ar at (a) 300 °C, (b) 400 °C and (c) 500 °C.
Figure 4. Gas permeation behaviors under dry condition of the supported mesoporous γ-Al2O3 membrane after modification with AHPCS and subsequent heat treatment under flowing Ar at (a) 300 °C, (b) 400 °C and (c) 500 °C.
Membranes 10 00258 g004
Figure 5. Kinetic diameter dependence of normalized gas permeance based on He permeance (Qi/QHe) at 50 °C through the SiCH hybrid/γ-Al2O3 composite membrane synthesized at different temperatures of 300, 400 and 500 °C. Dotted line indicates predicted values by the Knudsen diffusion model based on He permeance.
Figure 5. Kinetic diameter dependence of normalized gas permeance based on He permeance (Qi/QHe) at 50 °C through the SiCH hybrid/γ-Al2O3 composite membrane synthesized at different temperatures of 300, 400 and 500 °C. Dotted line indicates predicted values by the Knudsen diffusion model based on He permeance.
Membranes 10 00258 g005
Figure 6. Weight gain measured at 30 °C for H2 adsorption to the sample film of the SiCH organic–inorganic hybrid prepared by 300 °C-heat treatment in Ar.
Figure 6. Weight gain measured at 30 °C for H2 adsorption to the sample film of the SiCH organic–inorganic hybrid prepared by 300 °C-heat treatment in Ar.
Membranes 10 00258 g006
Figure 7. Gas permeation properties under the dry (p/p0(H2O) = 0) and wet (p/p0(H2O) = 1) condition at 50 °C, and water vapor permeation properties at p/p0(H2O) = 1 at 50 °C evaluated for SiCH hybrid/γ-Al2O3 composite membranes synthesized at different temperatures of 300, 400 and 500 °C, and the 500 °C-synthesized membrane further modified with PCS by the melt impregnation at 120 °C [50].
Figure 7. Gas permeation properties under the dry (p/p0(H2O) = 0) and wet (p/p0(H2O) = 1) condition at 50 °C, and water vapor permeation properties at p/p0(H2O) = 1 at 50 °C evaluated for SiCH hybrid/γ-Al2O3 composite membranes synthesized at different temperatures of 300, 400 and 500 °C, and the 500 °C-synthesized membrane further modified with PCS by the melt impregnation at 120 °C [50].
Membranes 10 00258 g007
Figure 8. Results of cyclic gas permeation measurements at 50 °C under p/p0(H2O) = 0–1.0 using the H2-N2 (2:1) mixed feed gas evaluated for (a) a supported mesoporous γ-Al2O3 membrane, (b) a 300 °C-synthesized SiCH hybrid/γ-Al2O3 composite membrane and (c) a 500 °C-synthesized composite membrane further modified with PCS.
Figure 8. Results of cyclic gas permeation measurements at 50 °C under p/p0(H2O) = 0–1.0 using the H2-N2 (2:1) mixed feed gas evaluated for (a) a supported mesoporous γ-Al2O3 membrane, (b) a 300 °C-synthesized SiCH hybrid/γ-Al2O3 composite membrane and (c) a 500 °C-synthesized composite membrane further modified with PCS.
Membranes 10 00258 g008
Figure 9. SEM images of the top surface view of an (a) as-synthesized mesoporous γ-Al2O3 layer and 500 °C-synthesized membrane further modified with PCS (b) before and (c) after gas permeation measurements under p/p0(H2O) up to 1 at 50 °C.
Figure 9. SEM images of the top surface view of an (a) as-synthesized mesoporous γ-Al2O3 layer and 500 °C-synthesized membrane further modified with PCS (b) before and (c) after gas permeation measurements under p/p0(H2O) up to 1 at 50 °C.
Membranes 10 00258 g009
Table 1. Activation energies for He and H2 permeations through the supported mesoporous γ-Al2O3 membrane after modification with AHPCS and subsequent heat treatment at 300–500 °C.
Table 1. Activation energies for He and H2 permeations through the supported mesoporous γ-Al2O3 membrane after modification with AHPCS and subsequent heat treatment at 300–500 °C.
SiCH Hybrid/γ-Al2O3 Composite Membrane Synthesis Temp.Activation Energy (Ea)/kJ mol−1
HeH2
300 °C20.317.0
400 °C9.88.6
500 °C1.40.5
Table 2. Gas permeation data of 500 °C-synthesized membrane further modified with PCS measured at 50 °C under p/p0 (H2O) =1.0 using a H2-N2 (2:1) mixed feed gas.
Table 2. Gas permeation data of 500 °C-synthesized membrane further modified with PCS measured at 50 °C under p/p0 (H2O) =1.0 using a H2-N2 (2:1) mixed feed gas.
Feed SidePermeate SideSeparation Factor (SF)
Flow Rate, VF/× 10−5 mol s−1Flow Rate, V/× 10−5 mol s−1Flux, J/× 10−5 mol m−2 s−1
VF, H2VF, N2VH2VN2JH2JN2
14.77.42.20.0432971.856.626
Table 3. H2-permselectivities of composite membrane in this study and those of other membranes evaluated at T ≤ 50 °C under the dry condition.
Table 3. H2-permselectivities of composite membrane in this study and those of other membranes evaluated at T ≤ 50 °C under the dry condition.
No.MembranesTemp./°CH2 PermeanceH2/X SelectivityRef.
/mol m−2 s−1 Pa−1α(H2/X)X
#01500 °C modified with PCS, Dry508.4 × 10−729.6N2This study
Wet, p/p0(H2O) = 1.0503.5 × 10−736.1N2
#02SiO2-based organic–inorganic hybrid (BTESE)407.66 × 10−7−20N2[68]
#03SiO2-based organic–inorganic hybrid (BTESM)501.79 × 10−612N2
#04zeolite-β/CMS302.64 × 10−997N2[69,70]
301.95 × 10−867.3N2
#05zeolite-Y/CMS302.77 × 10−9100.2N2
301.96 × 10−861N2
#06PFDA-based liquid membrane302.4 × 10−910O2[18]
#07graphene nanosheetRT5.9 × 10−716.5N2[71,72]
#08ZIF nanosheet membrane302.04 × 10−766.55N2[73,74]
#09ultrathin graphene oxide20−1 × 10−7−900N2[75,76]
#10microporous polymer (PIM-EA(H2)-TB)30(1.7 × 10−12) *22N2[77]
#11microporous polymer (PIM-Trip(Me2)-TB)25(1.8 × 10−12) *21.4N2[78]
*: H2 permeability/mol m−1 s−1 Pa−1.

Share and Cite

MDPI and ACS Style

Kubo, M.; Mano, R.; Kojima, M.; Naniwa, K.; Daiko, Y.; Honda, S.; Ionescu, E.; Bernard, S.; Riedel, R.; Iwamoto, Y. Hydrogen Selective SiCH Inorganic–Organic Hybrid/γ-Al2O3 Composite Membranes. Membranes 2020, 10, 258. https://0-doi-org.brum.beds.ac.uk/10.3390/membranes10100258

AMA Style

Kubo M, Mano R, Kojima M, Naniwa K, Daiko Y, Honda S, Ionescu E, Bernard S, Riedel R, Iwamoto Y. Hydrogen Selective SiCH Inorganic–Organic Hybrid/γ-Al2O3 Composite Membranes. Membranes. 2020; 10(10):258. https://0-doi-org.brum.beds.ac.uk/10.3390/membranes10100258

Chicago/Turabian Style

Kubo, Miwako, Ryota Mano, Misako Kojima, Kenichi Naniwa, Yusuke Daiko, Sawao Honda, Emanuel Ionescu, Samuel Bernard, Ralf Riedel, and Yuji Iwamoto. 2020. "Hydrogen Selective SiCH Inorganic–Organic Hybrid/γ-Al2O3 Composite Membranes" Membranes 10, no. 10: 258. https://0-doi-org.brum.beds.ac.uk/10.3390/membranes10100258

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop