Rie Tajiria,
Aki Mihataa,
Kazuya Yamamotoa and
Jun-ichi Kadokawa*ab
aGraduate School of Science and Engineering, Kagoshima University, 1-21-40 Korimoto, Kagoshima 890-0065, Japan. E-mail: kadokawa@eng.kagoshima-u.ac.jp; Fax: +81-99-285-3253; Tel: +81-99-285-7743
bResearch Center for Environmentally Friendly Materials Engineering, Muroran Institute of Technology, 27-1 Mizumoto-cho, Muroran, Hokkaido 050-8585, Japan
First published on 18th December 2013
In this study, we found that a chitin gel was facilely obtained by stirring a mixture of chitin with a highly concentrated CaBr2·2H2O/methanol solution at room temperature. We also examined the conversion of the resulting gel into a porous chitin by a regeneration technique. When the mixtures of chitin (0.9–3.5% (w/v)) with 3.85 mol L−1 CaBr2·2H2O/methanol solution were stirred at room temperature, chitin was gradually swollen, leading to a gelling form after 48 h. The mixtures of chitin (1.8% (w/v)) with CaBr2·2H2O/methanol solutions in different concentrations also turned into a gelling form by the same procedure. The dynamic viscoelastic measurement of the resulting chitin gels supported their gelling state. Then, porous chitins were efficiently prepared by removing methanol from the gels under reduced pressure, followed by washing with water and lyophilization. The α-chitin crystalline structure of the porous chitin was confirmed by powder X-ray diffraction measurement. The morphology of the porous chitins was evaluated by the SEM measurement. Consequently, it was found that the porosities were depending on contents of chitin in the gels. Furthermore, the mechanical properties of the porous chitins were investigated by compressive testing, which were affected by the pore sizes of the materials. On the other hand, the amounts of CaBr2·2H2O in the gels did not strongly affect the porosities and mechanical properties of the porous chitins.
On the other hand, in the previous study, we found that an ionic liquid, 1-allyl-3-methylimidazolium bromide (AMIMBr), dissolved or swelled chitin to form weak gel-like materials (ion gels).11,12 Furthermore, we also reported that self-assembled chitin nanofibers with ca. 20–60 nm in width and several hundred nm in length were facilely produced by regeneration from the ion gels using methanol, followed by sonication.13 Interestingly, nanofibers with higher aspect ratios were produced by the regeneration using CaBr2·2H2O/methanol solution with moderate concentrations (relatively low concentrations) compared with those regenerated using a sole methanol.14 This result indicated that CaBr2·2H2O/methanol solution affected the regeneration process of chitin from the ion gel, inspiring us its specific affinity for chitin.
On the basis of the above background, in this study, we found that gelation simply took place when a mixture of chitin with a highly concentrated CaBr2·2H2O/methanol solution was only stirred at room temperature. Because chitin has not been swollen by stirring a mixture of the aforementioned CaCl2·2H2O/methanol solution at room temperature, it can be noted that a highly concentrated CaBr2·2H2O/methanol solution exhibits specific behavior for chitin. The dynamic viscoelastic measurement was conducted to characterize the present gels prepared under the various conditions. Moreover, we also performed the conversion of the chitin gels into porous chitins by regeneration technique. Porous chitins have previously been produced by the appropriate regeneration approaches mostly via multiple steps through several days from chitin solutions with the aforementioned calcium chloride solvent and the other solvent systems.15–18 Moreover, these studies have not mostly revealed the precise dependence of porous morphologies on the procedures and conditions. Our method reported herein provides the quite facile procedure for the gelation and relatively regulated porositization of chitin prior to the previous methods. The present approaches, therefore, have potentials for further practical applications in the various research fields in the future.
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Scheme 1 Procedure for preparation of chitin gels with CaBr2·2H2O/methanol media and their conversion into porous chitins. |
Then, we also prepared the 1.8% (w/v) chitin gels with 3.49, 3.65, and 3.85 mol L−1 CaBr2·2H2O/methanol media. Because the total volumes of the media were adjusted to consistence in these gels, the amounts of CaBr2·2H2O for chitin were different depending on the concentrations of the media. The experimental procedure was conducted as the aforementioned, resulting in totally gelling form. However, CaBr2·2H2O/methanol media in lower concentrations did not afford total gelation. The dynamic viscoelastic data of the resulting gels in Fig. 2 showed that the G′ values were always larger than the G′′ values, supporting the gelling state of the samples. However, the gel with the lower CaBr2·2H2O concentration such as that with 3.49 mol L−1 CaBr2·2H2O/methanol media exhibited the weak-gel nature because of the smaller difference of the G′ and G′′ values (Fig. 2(a)) compared with the other gels (Fig. 2(b) and (c)). The above rheological results indicated that gel behaviors were affected by both the contents of chitin and the amounts of CaBr2·2H2O in the gels.
The crystalline structure of the regenerated chitin was confirmed by the XRD measurement. The XRD profile of the regenerated material obtained from the 1.8% (w/v) chitin gel with 3.85 mol L−1 CaBr2·2H2O/methanol media mainly showed six diffraction peaks at around 9.5°, 13.0°, 19.4°, 21.0°, 23.8°, and 26.5° (Fig. 3(b)), which were assignable to 020, 021, 110, 120, 130, and 013 planes, respectively.21 This diffraction pattern typically corresponds to the crystalline structure of α-chitin and was in good agreement with that of an original chitin powder (Fig. 3(a)). This result indicated the α-chitin crystalline structure was reconstructed during the aforementioned regeneration procedure. Furthermore, the XRD result in Fig 3(b) did not observe the crystalline peaks due to a CaBr2·2H2O powder as shown in Fig. 3(c), suggesting the absence of inorganic salts in the regenerated material. The absence of the salts was also supported by the SEM-EDX spectrum of the same material because signals assignable to Ca and Br elements were not detected.
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Fig. 3 XRD profiles of commercial chitin powder (a), porous chitin obtained from 1.8% (w/v) chitin gel with 3.85 mol L−1 CaBr2·2H2O/methanol media (b), and CaBr2·2H2O powder (c). |
The porosities of the regenerated materials were confirmed by the SEM measurement. Fig. 4(a)–(d) shows the SEM images of the four materials with same magnification obtained from the 0.9, 1.8, 2.4, and 3.5% (w/v) chitin gels with 3.85 mol L−1 CaBr2·2H2O/methanol media. The SEM pictures of the former two samples showed the porous morphologies, whereas such morphologies were not observed in the SEM images of the latter two samples. Furthermore, the pore sizes in Fig. 4(b) were relatively smaller than those in Fig. 4(a). When the SEM images of the latter two samples were taken with more magnification, the porous morphologies were obtained with decreasing the pore sizes in the order of Fig. 4(c′) to (d′). These SEM results supported that porous chitins were produced by the aforementioned regeneration procedure from the chitin gels with CaBr2·2H2O/methanol media. The observations also indicated the contents of chitin in the gels strongly affected the pore sizes of the porous chitins and the gels in the lower contents of chitin gave the larger pores via the regeneration procedure. Because looser network structure should form in the gel with lower content of chitin (e.g., 0.9% (w/v)) due to voluminously swollen chitin chains, the larger pores were formed by the above regeneration procedure, which was suitably performed as the network structure was maintained.
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Fig. 4 SEM images of porous chitins obtained from 0.9, 1.8, 2.4, and 3.5% (w/v) chitin gels with 3.85 mol L−1 CaBr2·2H2O/methanol media ((a), (b), (c) and (c′), and (d) and (d′), respectively). |
The SEM measurement of the regenerated chitin samples produced from the 1.8% (w/v) gels with 3.49–3.85 mol L−1 CaBr2·2H2O/methanol media was also performed. As shown in the SEM images of these samples with same magnification (Fig. 5), the pore sizes were not largely different. These results suggested that the amounts of CaBr2·2H2O in the gels did not strongly affect the porous morphologies. This is probably because that the network structures of the chitin chains were mainly regulated by the chitin contents in the gels, which were responsible for the porosity of the regenerated chitin materials.
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Fig. 5 SEM images of porous chitins obtained from 1.8% (w/v) chitin gels with 3.49, 3.65, and 3.85 mol L−1 CaBr2·2H2O/methanol media ((a), (b), and (c), respectively). |
The mechanical properties of the porous chitins were evaluated by compressive testing as one of the necessity properties for practical materials. Fig. 6 shows the stress–strain curves of the four porous chitins obtained from the 0.9, 1.8, 2.4, and 3.5% (w/v) chitin gels with 3.85 mol L−1 CaBr2·2H2O/methanol media. The results indicated that the materials prepared from the gels with the lower contents of chitin exhibited the more elastic properties with the larger fracture strain values, owing to the larger pore sizes. On the other hand, the stress–strain curves of the porous chitins resulted from the 1.8% (w/v) gels with 3.49–3.85 mol L−1 CaBr2·2H2O/methanol media (Fig. 7) showed almost the same profiles because of their similar porosities.
Because of the porous morphologies, the porous chitins exhibited water absorbent ability by immersing them in water. For example the porous chitin resulted from the 0.9% (w/v) chitin gel with 3.85 mol L−1 CaBr2·2H2O/methanol media absorbed 42.5 times its own weight in water.
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