Yasufumi
Fuse
a,
Yusuke
Ide
b and
Makoto
Ogawa
*ab
aGraduate School of Creative Science and Engineering, Waseda University, 1-6-1 Shinjyuku-ku, Nishiwaseda, Tokyo, 169-8050, Japan
bDepartment of Earth Sciences, Waseda University, 1-6-1 Shinjyuku-ku, Nishiwaseda, Tokyo, 169-8050, Japan
First published on 24th February 2010
A layered titanate-epoxy nanocomposite was synthesized by the reaction of a layered titanate modified with glycidyl and octadecyl groups and an epoxy resin followed by curing. The nanocomposite exhibited durability toward UV light compared with the pristine epoxy resin. Moreover, the refractive index (at 598 nm) of the nanocomposite was controlled in the rage of 1.51–1.53 by the added amount (0.00–0.04 mass%) of the organically modified titanate.
In this article, the successful synthesis of a layered titanate-polymer nanocomposite and the two useful properties of the nanocomposite are reported. Epoxy resin, which is one of the most commonly used engineering thermosetting plastics, was chosen as a polymer to be modified by embedding the titanate. The resulting layered titanate-epoxy nanocomposite exhibited UV light-durability, which was due to the effective absorption of UV light by the hybridized layered titanate, since layered titanates are semiconductors with the band gap energy corresponding to UV light.6 Moreover, the refractive index of the nanocomposite was controlled due to the higher refractive index of layered titanates (∼2.0 at 600 nm7) than that of epoxy resin. Although physicochemical properties of clay-polymer nanocomposites, such as improved mechanical and gas barrier ones and reduced flammability, have been reported,4 to our knowledge, the present report is the first example of the UV light durability and controlled refractive index of a layered solid-based nanocomposite. The present results suggest the merits of layered titanates as fillers for functionalizing polymers multiply.
For synthesizing the nanocomposite, a layered titanate, K0.59Ti1.66Li0.34O3.78,8 was modified with silane coupling reagents,9 glycidylpropyltrimethoxysilane and octadecyltrimethoxysilane, to swell in an epoxy resin. It has been reported that the surface modification of interlayer hydroxyl groups of layered alkali silicates with polymerizable silyl groups and subsequent copolymerization of the attached silyl groups with monomers resulted in the swelling of the layered solids in the corresponding polymers.10 We expect, in this study, that the intercalation of an epoxy resin and subsequent copolymerization of the epoxy resin with the attached glycidyl groups are facilitated by the expansion of the interlayer space with the co-attached alkyl groups.
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Fig. 1 XRD patterns of (a) K0.59Ti1.66Li0.34O3.78, (b) C12N+-TLO, (c) (b) reacted with GTMS, (d) C18TMS-GTMS-TLO, and (e) GTMS-TLO. |
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Fig. 2 Infrared spectra of (a) C18TMS-GTMS-TLO and (b) GTMS-TLO. |
The organic derivative of K0.59Ti1.66Li0.34O3.78 modified only with GTMS (GTMS-TLO) was also prepared, as a reference to discuss the cooperative effect of the two organosilyl groups on the swelling in an epoxy resin. The basal spacing of C12N+-TLO (2.7 nm) decreased to 2.6 nm after the reaction with GTMS (Fig. 1e), which decrease was due to the smaller molecular length of GTMS (1.5 nm × 0.5 nm × 0.5 nm) than that (1.9 × 0.4 nm × 0.4 nm) of C12N+. In addition to the XRD result, the infrared spectrum of GTMS-TLO (Fig. 2b), which shows Si–O–Ti absorption band (952 cm−1), reveals the successful attachment of GTMS onto K0.59Ti1.66Li0.34O3.78. From the basal spacing (3.2 nm and 2.6 nm, respectively) and composition (ca 0.7 groups per Ti1.66Li0.34O3.78) of C18TMS-GTMS-TLO and GTMS-TLO, taking the molecular size of C18TMS (2.6 nm × 0.5 nm × 0.5 nm) and GTMS into consideration, the attached silyl groups are thought to take an identical arrangement (interdigitated monolayer) in the two silylated derivatives. Accordingly, larger basal spacing (3.2 nm) of C18TMS-GTMS-TLO than that (2.6 nm) of GTMS-TLO is explained by the presence of C18TMS.
The composition of the obtained organic derivatives of K0.59Ti1.66Li0.34O3.78 is shown in Table 1. It should be noted here that the surface coverage with organosilyl groups is similar for C18TMS-GTMS-TLO and GTMS-TLO (0.74 and 0.70 groups per Ti1.66Li0.34O3.78, respectively). Based on the composition and the available surface area of K0.59Ti1.66Li0.34O3.78, 0.23 nm2 per Ti1.66Li0.34O3.78 unit cell (= 2ac = 2 × 0.38 nm × 0.30 nm, where a and c are the lattice parameters of the titanate14), the distance between the adjacent organosilyl groups was calculated to be 0.57 nm (= (0.23/0.7)1/2) (equivalent to 3.0 groups per nm2 (= 0.7/0.23)). In the light of the bottom area of the two organosilyl groups (0.5 nm × 0.5 nm) if their molecular shape is rectangular parallelepipeds, the organosilyl groups are thought to cover the interlayer surface of K0.59Ti1.66Li0.34O3.78 almost fully so that an epoxy resin can interact neither with surface titanol groups nor silanol groups formed by the hydrolysis of the remained methoxy groups of the attached C18TMS and GTMS. The surface coverage with organosilyl groups and the amount of interlayer hydroxy groups have been found to affect the adsorptive property of the organosilyl derivatives of layered solids.11,13,15 In the case of the present C18TMS-GTMS-TLO and GTMS-TLO, the surface coverage with organosilyl groups is similar and the presence of titanol and silanol groups is negligible as described above. Therefore, it is possible to discuss the cooperative effect of glycidyl and alkyl groups on the intercalation of an epoxy resin and subsequent copolymerization of the epoxy resin with the attached glycidyl groups.
The reaction of C18TMS-GTMS-TLO with an epoxy resin followed by curing resulted in the formation of the composite with texture homogeneity (Fig. 3 (I) c) and transparency in visible light wavelength region comparable to that of the pristine epoxy resin (Fig. 4 c). On the other hand, particles with several tens of μm, which is the aggregates of GTMS-TLO particles with a diameter of 1–2 μm (Fig. 3 (II) b), were observed in the GTMS-TLO-epoxy composite (Fig. 3 (I) b). The TEM image (Fig. 5) of the composite synthesized from C18TMS-GTMS-TLO showed that the titanate sheets with the thickness of ca. 1–5 nm and the diameter of several hundreds of nm were dispersed in the polymer. These results indicate the cooperative effect of the attached GTMS and C18TMS on the swelling of K0.59Ti1.66Li0.34O3.78 in the epoxy resin; the intercalation of an epoxy resin and copolymerization of the epoxy resin with the attached GTMS are facilitated by the expansion of the interlayer space with the attachment of C18TMS (Fig. 1 d and e).
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Fig. 3 (I) Photographs of (a) epoxy resin and the composite with (b) GTMS-TLO and (c) C18TMS-GTMS-TLO; (II) SEM images of (a) GTMS-TLO and (b) C18TMS-GTMS-TLO. |
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Fig. 4 Transmittance spectra of (a) epoxy resin and the composite with (b) GTMS-TLO and (c) C18TMS-GTMS-TLO and UV-vis absorption spectrum of a suspension of C18TMS-GTMS-TLO in benzene (1 mass%). |
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Fig. 5 A TEM image of the C18TMS-GTMS-TLO-epoxy nanocomposite. The inset shows the magnified TEM image. |
The UV-Vis absorption spectrum of a colloidal suspension of C18TMS-GTMS-TLO (1.0 mass%) was shown in Fig. 4. An absorption peak was observed at around 280 nm, which was shifted to a shorter wavelength region from an absorption edge (350 nm) of K0.59Ti1.66Li0.34O3.78. Similar absorption peaks have been observed for the aqueous16 or organic13 suspensions of layered titanates and was due to the absorption of swelled titanate sheets.16 In the UV-Vis absorption spectra of the layered titanate-epoxy composites, the absorption onset of the epoxy resin was at around 450 nm, so that the location of the absorption due to the titanate sheets is not seen owing to the overlapping. The titanate sheets were shown to be dispersed in C18TMS-GTMS-TLO-epoxy nanocomposite as described above. The integral (2.4) of the absorption band at UV light wavelength region of the C18TMS-GTMS-TLO suspension, which correlates to the oscillator strength of the titanate sheets, is higher than that (0.013) of epoxy resin,17 suggesting that the titanate sheets absorb UV light preferentially to prevent UV light-degrading of the nanocomposite. The UV-light durability of the present materials was investigated using an ultra-high pressure mercury lamp as UV light source.
Fig. 6 depicts the variation in the transmission spectrum of the pristine epoxy resin with UV-light irradiation time. The transmittance at around 400 nm gradually decreased (Fig. 7 ○), as a result of the decomposition of organic groups in the epoxy resin to be yellow-colored (the pristine epoxy resin prepared in this study is originally pale yellow-colored). The GTMS-TLO-epoxy mixture, in which K0.59Ti1.66Li0.34O3.78 did not swell, was degraded similarly (Fig. 7 ◇). On the other hand, the degradation of the C18TMS-GTMS-TLO-epoxy nanocomposite was remarkably suppressed (Fig. 7 □). The titanate sheets were thought to absorb UV light efficiently to prevent the epoxy matrix from degrading. It has been reported that epoxy encapsulant around light emitting diode is UV light-degraded to discolor followed by the decrease in the light output intensity.18 The effect of the photocatalytic decomposition of organic substance by the titanate induced by UV light on the present photo-degradation of the epoxy resin is not clear at present.
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Fig. 6 Variation in transmittance spectra of epoxy resin with UV light irradiaiton time; inset shows the expanded verion of the figure at the wavelength region from 430 to 370 nm. |
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Fig. 7 Variation in transmittance at 400 nm as a function of UV light irradiation time of (○) epoxy resin and the composite of epoxy resin with (◇) GTMS-TLO and (□) C18TMS-GTMS-TLO. |
Another noticeable property of the C18TMS-GTMS-TLO-epoxy nanocomposite was the controlled refractive index. The control of refractive indices of organic polymers by hybridizing molecular titania (domain size of several to several tens of nm) has widely been investigated.19,20 In this study, as depicted in Fig. 8, the refractive index of epoxy resin was successfully controlled with the added amount (mass%) of the titanate. There is a linear relationship between the refractive indices of the nanocomposite and the C18TMS-GTMS-TLO concentration, suggesting again that the titanate sheets are homogeneously dispersed in epoxy resin and also implying that the refractive index variation reflects only the change of the amount of the titanate embedded in epoxy resin since the filler size does not vary depending on the loaded amount. Layered titanates with different particle size are available,8,14 therefore, the present result motivates us to investigate the effect of the aspect ratio (diameter/thickness) of the titanate sheets on the refractive index of nanocomposites. The gas barrier properties of clay-polymer nanocomposites have been demonstrated to correlate with the aspect ratio of the silicate layers.21
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Fig. 8 Variation in refractive index of C18TMS-GTMS-TLO-epoxy nanocomposite with the weight concentration of the titania. |
Fig. 9 shows the variation in the refractive index of the present nanocomposite with the titania volume fraction22 together with that of the reported molecular titania (a domain size of ca. 100 nm)-based epoxy nanocomposite.20 It is worth mentioning that to increase the refractive index of epoxy resin the present system needs a much smaller amount of titania than the previously reported system. We believe that the ultrathin sheet morphology of the present filler plays an important role in the observed effect.
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Fig. 9 Refractive index variation of (●) C18TMS-GTMS-TLO-epoxy nanocomposite and (□) the reported titania-based epoxy nanocomposite20 with the volume fraction of titania. Inset: an expanded version of the figure. |
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