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Monolithic silsesquioxane materials with well-defined pore structure

Published online by Cambridge University Press:  01 December 2014

Kazuyoshi Kanamori*
Affiliation:
Department of Chemistry, Graduate School of Science, Kyoto University, Kitashirakawa, Sakyo-ku, Kyoto 606-8502, Japan
*
a) Address all correspondence to this author. e-mail: kanamori@kuchem.kyoto-u.ac.jp

Abstract

In this article, monolithic porous silsesquioxane materials, which are derived by sol–gel from trialkoxysilanes with substituent groups such as trimethoxysilane (HTMS), methyltrimethoxysilane (MTMS), and vinyltrimethoxysilane (VTMS), are reviewed with a special emphasis on our recent works. Careful controls over fundamental synthetic parameters such as pH, amounts of water and solvent, and kind of solvent and additives play a crucial role in the formation of monolithic gels based on random polysiloxane networks. Crystalline/amorphous precipitation is otherwise observed when the formation of isolated species including polyhedral oligomeric silsesquioxanes dominates or if phase separation of the hydrophobic networks in aqueous media is not adequately controlled. In the successfully controlled system, pore size can be varied from a few tens of nanometers to a few tens of micrometers; porous materials such as transparent aerogels and hierarchically porous monoliths have been explored. In addition, unique properties derived from trialkoxysilanes such as reactivity of the pore surface and flexible mechanical properties are demonstrated. Possibilities in the silsesquioxane materials with controlled pore structures are discussed.

Information

Type
Invited Feature Papers
Copyright
Copyright © Materials Research Society 2014 
Figure 0

FIG. 1. Typical molecular-level structure of silsesquioxanes derived from trialkoxysilanes: (a) random network structure necessary for the monolith formation, (b) perfect cage structure, and (c) partial cage structure.

Figure 1

FIG. 2. Examples of multiphase structural formations in the sol–gel system. (a) Aggregation of colloids leads to a gel, which can be converted to an aerogel after an adequate drying process (usually supercritical drying). Note that nanometer-sized colloids are exaggerated in the figure. (b) Structural formation via spinodal decomposition, which can be induced during concurrent sol–gel transition to yield a gel with controlled macropores in the micrometer scale.

Figure 2

FIG. 3. (a) A reaction scheme for the HSQ monoliths with controlled macropores. (b) Typical macroporous co-continuous structures and appearance of a rod-shaped HSQ monolith (starting compositions: HTMS 2.1 mL, 50 mM nitric acid 2.5 mL, methanol 2.5 mL and PEO (Mn = 35,000) 150 mg (HY150) and 210 mg (HY210)). (c) Macropore distributions of the two samples characterized by mercury intrusion porosimetry. (d) Nitrogen adsorption–desorption isotherms and the Barrett-Joyner-Halenda (BJH) mesopore size distributions of the two samples.

Figure 3

FIG. 4. (a) A cartoon showing the reduction of noble metal ions in the macroporous HSQ, resulting in the (alloy) nanoparticle formation in the monolith. (b) XRD patterns of Au–Pd alloy embedded monoliths with different Au/Pd ratios. The gradual change in the diffraction angles suggests the formation of alloys. (c) 29Si single pulse solid-state NMR spectra of the original HSQ and Pd@HSQ. (d) A TEM image of the Pd nanoparticles embedded in the HSQ.

Figure 4

FIG. 5. (a) Reaction of the HSQ pore surface with alcohols under the presence of a Lewis acid (zinc(II) 2-ethylhexanoate in this case). The dehydrogenative addition of an alcohol in anhydrous solvent is followed by oxidation-condensation of Si–H species in aqueous solvent. (b) An example of two-step modification of the HSQ pore surface; the addition of azidopropanol is followed by the CuAAC click reaction.

Figure 5

FIG. 6. Relationship between macroscopic morphology and starting composition in (a) MTMS, (b) VTMS, and (c) VTMS–TMOS sol–gel systems with FA and 1 M nitric acid.

Figure 6

FIG. 7. (a) A reaction scheme for MSQ aerogels/xerogels in an acid-base two-step sol–gel system under the presence of surfactant. (b) The typical “spring-back” behavior observed during uniaxial compression on an optimized MSQ aerogel sample.

Figure 7

FIG. 8. (a) An example of a successfully obtained MSQ “xerogel” tile with large area by ambient pressure drying. (b) Thermal conductivity of a MSQ xerogel, a standard silica aerogel, and nitrogen gas (filled in the measurement space) versus pressure measured by the guarded hot plate method.

Figure 8

FIG. 9. MSQ gels prepared with different amounts of Pluronic F127 in the acid-base two-step system. The resultant gel becomes more transparent with increasing amount of F127, due to more effective suppression of phase separation. At appropriate F127 concentrations, hierarchically porous MSQ gels with well-defined co-continuous macropores and mesopores in the skeletons are obtained. Starting composition: MTMS 5 mL, 5 mM acetic acid 6 mL, urea 0.5 g, and F127.

Figure 9

FIG. 10. (a) The MSQ–CNF composite aerogel with the lowest bulk density (0.02 g cm−3), showing bendability. (b) Relationship between bulk density and thermal conductivity of MSQ–CNF composite aerogels. Typical value ranges of other insulating materials are also shown.

Figure 10

FIG. 11. Precursors and multifunctionality of the marshmallow-like gels. Superhydrophobicity and low-temperature flexibility are consequent properties derived from PDMS-like crosslinked networks. The pore surface of vinyl-functionalized marshmallow gels can be derivatized by, for example, the thiol-ene reaction to give superamphiphobicity. See the text and Ref. 93 for details.