Naofumi Naga*ab,
Shun Fujiokab,
Daisuke Inoseb,
Kumkum Ahmedc,
Hassan Nagehd and
Tamaki Nakanode
aDepartment of Applied Chemistry, College of Engineering, Shibaura Institute of Technology, 3-7-5 Toyosu, Koto-ku, Tokyo 135-8548, Japan
bGraduate School of Engineering and Science, Shibaura Institute of Technology, 3-7-5 Toyosu, Koto-ku, Tokyo 135-8548, Japan
cSIT Research Laboratpries, Shibaura Institute of Technology, 3-7-5 Toyosu, Koto-ku, Tokyo 135-8548, Japan
dInstitute for Catalysis and Graduate School of Chemical Sciences and Engineering, Hokkaido University, N 21, W 10, Kita-ku, Sapporo 001-0021, Japan
eIntegrated Research Consortium on Chemical Sciences (IRCCA), Institute for Catalysis, Hokkaido University, N 21, W 10, Kita-ku, Sapporo 001-0021, Japan
First published on 23rd December 2019
Porous polymers have been synthesized by Michael addition reactions of multi-functional acrylate and diamine or dithiol compounds. Aza-Michael addition reaction of multi-functional acrylate, trimethylolpropane propoxylate triacrylate (TPT) and hexamethylene diamine (HDA) in dimethyl sulfoxide (DMSO) successfully yielded the porous polymer. The porous structure was characterized by connected globules or co-continuous structure, and could be controlled by the reaction conditions. Mechanical properties of the porous polymers were investigated by compression test. The porous polymers with co-continuous structure showed higher Young's modulus than those with connected globules. The porous polymer absorbed some organic solvents, especially CHCl3. The porous polymer as prepared in DMSO state showed coloring induced by Christiansen filter effect depending on the reaction time and observation temperature. The thio-Michael addition reaction of TPT and 1,6-hexanedithiol (HDT) in DMSO using different base catalysts also yielded the porous polymer. The porous structure could be controlled by the catalysts amount when the reaction was initiated by a photo-base generator as the base catalyst. The present reaction systems make it possible to synthesize the porous polymers with simple process without phase separator.
Previously, we have developed various gels, which are synthesized by addition reactions between multi-functional compounds and α,ω-bifunctional compounds in various solvents, for example, hydrosilylation reaction of multifunctional siloxane or silsesquioxane and α,ω-diolefin, thiol-ene reaction of multifunctional thiol and diacrylate, multifunctional vinyl siloxane or silsesquioxane and dithiol, azide-alkene reaction of multifunctional vinyl siloxane or silsesquioxane and diazide, and so on.6 This molecular design makes it possible to synthesize the gels with homogeneous, controlled mesh size, and designed molecular geometry network structures. In a series of the studies, we found that the reactions of multi-functional thiol and diisocyanate compounds in toluene induced phase separation, which yielded porous polymers without phase separator.6e We have been studying the affinity between the network structure and solvent in the gels synthesized by addition reactions between multi-functional compounds and α,ω-bifunctional compounds, and found Michael addition reactions of conventional multifunctional acrylate compound trimethylolpropane propoxylate triacrylate (TPT) with hexamethylene diamine (HDA) or 1,6-hexanedithiol (HDT) in dimethyl sulfoxide (DMSO) successfully yielded the porous polymers. These reaction systems make simplify the post-processing of the porous polymers. Here we report the effect of the polymerization conditions, polymerization temperature, monomer feed ratio, and monomer concentration, on the production state and structure of the TPT–HDA, -HDT polymers. The porous structure, space structure and size, can be precisely controlled by the reaction conditions. The mechanical property and absorption capacity of the porous polymer were quantitatively evaluated to study the effect of the porous structure on the features. We also report the coloration of the TPT–HDA porous polymer in DMSO, in the as prepared state, due to structural coloration, so called Christiansen filter effect. Transition of the color was observed depended on the observation temperatures (Scheme 1).
Scheme 1 Synthesis mechanism of gels and porous polymers by means of Michael addition reaction of multi-functional acrylate compound, TPT, and HDA, HDT in DMSO. |
Scanning electron microscopy (SEM) images of the porous polymers were obtained by a JEOL JSM-7610F microscope with an LEI detector at an acceleration voltage of 3.0 kV.
Surface area of the porous polymers were measured by nitrogen sorption using an Autosorb 6AG (Quantachrome), and determined by Brunauer–Emmett–Teller (BET) equation.
Mechanical properties of the porous polymers were investigated by compression test with an universal testing instrument, Tensilon RTE-1210 (ORIENTEC Co. LTD.). The test samples were cut to 1 cm cube, and pressed at a rate of 0.5 mm min−1 at room temperature. Young's modulus was determined from slope of the stress–strain curve acquired by the compression test in the elastic deformation region (at 10% of strain).
Differential scanning calorimetry (DSC) measurements of the porous polymers were conducted with a Rigaku DSC 8230. The transition temperature was determined on the 2nd heating process from −50 °C to 200 °C at a rate of 10 °C min.
UV-vis spectroscopy of the porous polymers prepared in DMSO was conducted with a SHIMADZU UV-1600PC, and the transmittance was recorded by 0.1 nm at a scan rate of 550 nm min−1.
Fig. 1 Production diagram of the TPT–HDA system, ○ porous polymer, △ gel, ◇ solution, monomer concentration: 20 wt%, overlap means co-existence of two types of polymers. |
Production diagram of the TPT–HDA system with the [TPT]/[HDA] feed ratio of 4/3 (mol mol−1) at 30–50 °C is illustrated in Fig. 2 to show the effect of monomer concentration. The reaction systems with 20 and 25 wt% of monomer concentrations yielded the porous polymers. By contrast, the reactions with 30 wt% of monomer concentration yielded the gels independent of the reaction temperatures. The increase of the monomer concentration would change the state from separated two-phase to single-phase.
Fig. 2 Production diagram of the TPT–HDA system, ○ porous polymer, △ gel, [TPT]/[HDA] = 4/3 (mol mol−1), solvent: DMSO, overlap means co-existence of two types of polymers. |
Reaction of TPT and HDA in DMSO was traced by FT-IR spectroscopy (ESI Fig. 1). Intensity of the absorption peaks at around 1650 cm−1, 810 cm−1, or 1410 cm−1 derived from vibration of primary or secondary amine, CC bending of acryloyl group, or CH2 bending of acryloyl group decreased after the reaction, indicating promotion of aza-Micahel reaction between acrylate and amine groups. Reaction conversions in TPT–HDA gel and porous polymer, [TPT]/[HDA] feed ratio of 4/3 (mol mol−1), evaluated from the peak intensity of the acrolyl groups in FT-IR spectra were 59% (monomer concentration: 20 wt% at 60 °C) and 64% (monomer concentration: 25 wt% at 45 °C), respectively. These results indicate that the reaction conversions are high enough to form the network structure independent of the production state.
SEM images of some resulting porous polymers, which were obtained in the reactions with [TPT]/[HDA] feed ratio of 4/3 (mol mol−1) are shown in Fig. 3. The reaction with 20 wt% of monomer concentration at 30 and 40 °C yielded the porous structure formed by aggregated globules of ∼5 μm diameter, as shown in Fig. 3(a) and (b). Continuous structure formed by broadly connected globules was observed in the porous polymer obtained in the corresponding reaction at 50 °C (Fig. 3 (c)). The reaction with 25 wt% of monomer concentration at 30 °C produced the porous structure formed by aggregated globules of ∼5 μm diameter (Fig. 3(d)). The porous structure formed by aggregated globules with relatively large, 50 μm, and small, 5–10 μm, sizes was observed in the porous polymer obtained in the corresponding reaction at 40 °C (Fig. 3(e)). Furthermore, the reaction at 45 °C yielded the porous polymer with co-continuous monolithic structure as shown in Fig. 3(f). Variation of the porous structures can be explained by spinodal decomposition during the network formation. When the reaction rate is high at high reaction temperature, the co-contentious monolithic structure is fixed at the early stage of the spinodal decomposition. In the case of the low temperature reactions, the secondary phase separation, which forms globules at later stage of the spinodal decomposition, should be induced during the reaction due to the low reaction rate. The similar results were reported in other reaction systems.7
Surface area of the porous polymers were relatively small, less than 2 m2 g−1, and could not be determined quantitatively by BET method. The small surface area of the porous polymers should be derived from the macroporous structure.
Mechanical properties of the TPT–HDA porous polymers were investigated by the compression test. The porous structure of the test samples was precisely controlled by the reaction temperatures ranged from 40–45 °C in the reactions of [TPT]/[HDA] = 4/3 (mol mol−1), monomer concentration: 25 wt% based on the results in Fig. 3 (ESI Fig. S2†). Fig. 4 shows stress–strain curves of the TPT–HDA porous polymers, and the results are summarized in Table 1. All the porous polymers were unbreakable by the compression test under 50 N. The glass transition temperature of a TPT–HDA porous polymer prepared from the reaction solution with 25 wt% monomer at 45 °C is −24.4 °C, and flexible feature in the compression test at room temperature is derived from amorphous phase of the porous polymer. The porous polymers with monolithic structure showed hard property, and the Young's modulus decreased with increasing of the size of co-continuous structure. Profiles of the stress–strain curves showed S-curve, indicating two steps deformation. The former or latter deformation should be derived from compression of contentious holes or pressed bulk. The soft feature of the porous polymers with large co-continuous structure should be caused by former deformation with low Young's modulus. The porous polymers formed by aggregated globules showed lower Young's modulus than that of the porous polymers formed by monolithic structure. Dissociation of the aggregation would be the driving force of the initial deformation of these porous polymers.
Reaction temperature [°C] | Young's modulusb [kPa] | Porous structure (SEM) | Sizec [mm] |
---|---|---|---|
a [TPT]/[HDA] = 4/3 (mol mol−1), monomer concentration in reaction solution: 25 wt%.b Not breakable under 50 N.c Average diameters of the globules or continuous holes of monolith determined by image processing. | |||
40 | 17.8 | Globule (Fig. 3(e)) | 18, 55 |
44 | 18.8 | Globule (Fig. S2(a)) | 13 |
44.5 | 52.4 | Monolith (Fig. S2(b)) | 19 |
45 | 80.9 | Monolith (Fig. 3(f)) | 5.7 |
The TPT–HDA porous polymer absorbs various organic solvents, chloroform, DMSO, dimethyl formamide, ethanol, and so on. The absorption of chloroform and DMSO was especially quick, and was completed within 10 min. The absorption of chloroform and DMSO was quantitatively investigated by TPT–HDA porous polymers formed by the aggregated globules or monolithic structure, prepared from the reaction solutions with 20 wt% or 25 wt%, respectively, at 45 °C (Table 2). Both the weight gain and volume gain in chloroform absorption were higher than those in DMSO. The calculated solubility parameters of the repeating unit of TPT–HDA porous polymers is 17.3 (MJ m−3)1/2.8 The solubility parameters of chloroform and DMSO are 19.0 and 29.7 (MJ m−3)1/2. Close solubility parameters between the polymer and solvent is an index of high miscibility. The values of the solubility parameters indicate that miscibility of the porous polymer with chloroform is much higher than that with DMSO, which should induce higher absorption of chloroform. Porous structure also affected the absorption capacity, and the polymer with aggregated globules showed larger weight gain than that with monolithic structure. By contrast, there was no difference in volume gain. One explanation of these results are that the porous polymer with aggregated globules would absorb the solvents not only in the vacant space and but inside of the globules.
Monomer concentration [wt%] | Solvent | Weight gain [wt%] | Volume gain [vol%] | Porous structure (SEM) |
---|---|---|---|---|
a [TPT]/[HDA] = 4/3 (mol mol−1), monomer concentration in reaction solution: 20 wt%, 25 wt%, reaction temperature: 45 °C, reaction time 48 h. | ||||
20 | CHCl3 | 1610 | 324 | Globule (Fig. 3(b)) |
25 | CHCl3 | 934 | 331 | Monolith (Fig. 3(f)) |
20 | DMSO | 519 | 135 | Globule (Fig. 3(b)) |
25 | DMSO | 298 | 140 | Monolith (Fig. 3(f)) |
The TPT–HDA porous polymers with chloroform were whitely clouded. By contrast, those with DMSO turned clear, and slightly colored under the white light (ESI Fig. S3 and S4†). The coloring feature of the TPT–HDA porous polymer in DMSO is derived from not absorption of light due to electron excitation (like dyes and pigments) but periodic microstructures, so called structural coloration. In the case of the present TPT–HDA system, the porous polymer size is much larger than the correlation of wavelength of the visible light. The diffusion reflection of irradiated visible light should would occur in the systems, and the systems appears white when the reflective indexes of polymer and solvent are different each other, as observed in TPT–HDA with chloroform. By contrast, when the reflective indexes of polymer and solvent are closed, the visible light transmits through the system, as observed in TPT–HDA with DMSO. We focused on the coloring behaviour of the porous polymers as prepared in DMSO. Effect of the reaction time on the coloring of the porous polymers was studied. Fig. 5 shows the TPT–HDA porous polymer as prepared in DMSO, [TPT]/[HDA] = 4/3 (mol mol−1), monomer concentration: 20 wt% (connected globules structure) or 25 wt% (monolithic structure). The porous polymers obtained with 24 h or 48 h reactions at 45 °C colored slightly purple or orange, respectively, independent of the monomer concentration. Reaction conversion would affect the color of the porous polymers. Effect of the observation temperatures on the coloring of TPT–HDA porous polymer, [TPT]/[HDA] = 4/3 (mol mol−1), monomer concentration: 25 wt%, are demonstrated in Fig. 6. The color changed from blue, purple, pink, orange, to yellow with increasing of the observation temperature from 5 °C to 60 °C on the heating process. The color did not change (stayed yellow) at the temperatures higher than 60 °C. The sample showed reverse color change on the cooling process. These transitions in the transmittance spectra are derived from Christiansen filter effect, as reported in some porous gels, dispersions, and colloids in solvents.9
Transmittance spectra of the TPT–HDA porous polymers, monomer concentration: 25 wt% prepared at 40 °C, are shown in Fig. 7. The reaction time to prepare the porous polymer affected profile of the transmittance spectra. The porous polymer obtained with 48 h reaction showed lower transmittance at long wave length, more than 600 nm, in comparison with the polymer obtained with 24 h reaction. The increase of the measured temperature decreased the transmittance at the long wave length accompanied by blue-shift of peak maxima of the transmittance peak, from 590 nm to 490 nm. The color of the TPT–HDA porous polymers in DMSO should be derived from both the reflected light and transmitted light. The broader perspective red-shift of the wave length of the visual aspect with increasing of the observation temperature should be derived from the decrease of the transmittance at long wave length of the reflected light. By contrast, the localized blue-shift of the visual aspect with increasing of the measured temperature should be derived from the blue-shift of the transmitted light. The combination of these transitions in both the reflected light and transmitted light via the TPT–HDA porous polymers in DMSO would cause the discontinuous wave length of the visual aspect.
Fig. 8 Production diagram of the TPT–HDT system, ○ porous polymer, △ gel, reaction temperature: room temp., reaction time: 48 h, overlap means co-existence of two types of polymers. |
The molecular structure of the porous polymers prepared by TEA, Pip, and PipHPP as the base catalysts was studied by FT-IR spectroscopy (ESI Fig. S5†). The absorption peak at around 2550 cm−1 derived from stretching of thiol group was almost disappeared, and intensity of the absorption peaks at 810 cm−1, or 1410 cm−1 derived from CC bending of acryloyl group, or CH2 bending of acryloyl group decreased in comparison with the spectrum of TPT, indicating almost complete promotion of Michael reaction between acrylate and thiol groups with all the catalysts.
Effect of the monomer concentration on the porous structure of the resulting porous polymers was precisely studied in the reactions with [TPT]/[HDT] feed ratio of 4/3 (mol mol−1). SEM images of some resulting porous polymers, which were obtained in the various monomer concentrations, are shown in Fig. 9. The monomer concentrations were sensitive to the porous structure. The reaction with 23 wt% of monomer concentration yielded the porous structure formed by aggregated globules about 1–5 μm diameter and deformed large continuous structure, as shown in Fig. 9(a). By contrast, co-continuous structure was observed in the porous polymers obtained in the corresponding reactions with 23.5, 24.5, and 25.5 wt% of monomer concentrations, as shown in Fig. 9(c)–(e), respectively. The increase of the monomer concentration decreased size of the co-continuous structure. The reaction with higher monomer concentration increased the reaction rate, and the co-contentious monolithic structure should be fixed at the early stage of the spinodal decomposition.
The SEM images of the porous polymers obtained from the reaction systems with [TPT]/[HDT] feed ratio of 2/3 (mol mol−1) and 25 wt% of monomer concentration using Pip as the base catalyst are shown in Fig. 10 (a) and (b). The porous polymers showed co-contentious structure with the isolated micro holes, as observed in the corresponding polymers obtained using TEA as the catalyst, as shown in Fig. 9(d). The increase of the Pip concentration decreased the size of the co-contentious structure. The increase of the reaction rate should fix the co-contentious monolithic structure at the early stage of the spinodal decomposition.
A photobase generator, PipHPP, produces Pip by irradiation of UV. The application of the photobase generator makes it possible to yield the porous polymers by UV irradiation. The SEM images of the porous polymers obtained from the reaction systems with [TPT]/[HDT] feed ratio of 2/3 (mol mol−1) and 25 wt% of monomer concentration are shown in Fig. 11(a)–(d). The porous polymers obtained from low PipHPP system showed the structure formed by broadly connected globules, as shown in Fig. 11(a). The reaction systems with higher PipHPP concentration yielded the porous polymers formed by mixed structure of the co-contentious and isolated distorted holes, as shown in Fig. 11(b) and (c). The increase of the reaction rate with increasing of the PipHPP concentration may induce precipitation of the resulting polymer, which would disturb the porous structure derived from phase separation.
Mechanical properties of the TPT–HDT monolithic porous polymers, where [TPT]/[HDT] = 2/3 (mol mol−1) and monomer concentration in reaction solution: 25 wt%, obtained with different catalysts, TEA, Pip, and PipHPP, were investigated. Fig. 12 shows the representative stress–strain curves of these polymers having co-continuous monolithic structure. All the porous polymers were unbreakable under the compressive load of 50 N and showed similar profiles in the stress–strain curves due to the same monomer concentration in the reaction solutions and similar porous structures. The values of the Young's modulus of the polymers are given in Table 3. The glass transition temperature of a TPT–HDT porous polymer prepared from the reaction solution with 25 wt% using Pip as the catalyst is −30.0 °C. The flexible feature, unbreakable and low Young's modulus, should be derived from amorphous phase of the porous polymer.
Catalyst (SEM Fig.) | Young's modulusb [kPa] | Solvent | Weight gain [wt%] | Volume gain [vol%] |
---|---|---|---|---|
a [TPT]/[HDT] = 2/3 (mol mol−1), solvent of reaction system: DMSO, monomer concentration in reaction solution: 25 wt%, catalyst concentration in reaction solution: [TEA] = 70.7 μmol mL−1, [Pip] = 1.66 μmol mL−1, [PipHPP] = 1.42 μmol mL−1, reaction temperature: r.t., reaction time: 48 h, porous structure: monolith.b Not breakable under 50 N. | ||||
TEA (9(d)) | 49.6 | CHCl3 | 2220 | 771 |
DMSO | 208 | 137 | ||
Pip (10(a)) | 53.4 | CHCl3 | 1930 | 832 |
DMSO | 238 | 124 | ||
PipHPP (11(b)) | 36.4 | CHCl3 | 2160 | 930 |
DMSO | 214 | 126 |
The absorption of chloroform and DMSO was quantitatively investigated by TPT–HDT porous polymers formed by the monolithic structure, prepared from the reaction solutions with 25 wt% of monomer concentration using different base catalysts. Theses porous polymers absorbed about 2000 wt% of chloroform and 200 wt% of DMSO. The TPT–HDT porous polymers absorbed much chloroform in comparison with the TPT–HDA porous polymers, as summarized in Table 3. One possibility to explain these results is the miscibility of the network structure of the porous polymers and solvents. The calculated solubility parameters of the repeating unit of TPT–HDA and TPT–HDT porous polymers are 17.3 and 16.4 (MJ m−3)1/2,8 and the solubility parameter of chloroform is 19.0 (MJ m−3)1/2. Close solubility parameters between the polymer and solvent would show high miscibility. If absorbance capacity of the porous polymer obeys this theory, the TPT–HDA porous polymer should absorb more chloroform than the TPT–HDT porous polymer. The contrary results to the theory would be derived from difference in the porous structure. Thickness of the framework of the TPT–HDA porous polymers, 1–3 μm as shown in Fig. 3(f), was smaller than that of the TPT–HDT porous polymers used in the experiment, 5–15 μm as shown in Fig. 9(d), and showed low absorbance capacity of chloroform with the TPT–HDA porous polymers.
The TPT–HDT porous polymers did not show Christiansen filter effect (ESI Fig. S6†). The small difference in chemical structure, NH or S, should make difference in refractive index between the TPT–HDA and TPT–HDT porous polymers.
As mentioned above, aza- and thio-Michael addition reactions of the multi-functional acrylate, TPT, with conventional diamine, HDA, or dithiol, HDT, in DMSO yielded the porous polymers in facile process. One of the merits of the both the present systems is that the porous polymers can be obtained without phase separator. This makes simplify the post-processing of the porous polymers. The reaction of TPT with HDA proceeds without catalyst. The reaction of TPT with HDT can be promoted by a photo-base catalyst. The photo initiated polymerization should make it possible to patter and 3D print of the TPT–HDT porous polymers. The reaction of the multi-functional molecules and bi-functional molecules in selected solvents must be useful method to develop the porous polymers induced by the phase separation during the polymerization. As the next step, we are developing new porous polymers by addition reaction of various multi-functional molecules with bi-functional molecules in conventional solvents. We are also trying to apply the present porous polymers for separation columns or catalyst supports. The coloring feature depended on the temperature of the TPT–HDA porous polymer in DMSO would be applicable to sensors. These results will be reported elsewhere.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c9ra09684a |
This journal is © The Royal Society of Chemistry 2020 |