Regular particulates also emerge along the fibers in the water bulk and precipitate at the bottom of the beaker PS-341 mw (see Figure 1). We noticed that 10 to 14 days is a typical period for fiber growth over which the yield and pore order of fibers

increase markedly with time. The long time is due to quiescent conditions where species has to interdiffuse slowly in absence of any bulk movement. TBOS species diffuse from the silica layer into the water phase; surfactant micelles also diffuse in the water bulk to interact with silica species in the interfacial region. Water and alcohol (resulting from the hydrolysis) diffuse as well and evaporate at the interface. This was reported to influence the growth in this method [42]. SEM images in Figure 2 illustrate the typical fiber and co-existing particulate morphologies. The fibers can grow to a length scale of millimeters, but they break easily yielding average dimensions of 500-μm length × 25-μm diameter. Gyroids are examples of co-existing particulates having comparable diameters to fibers. They apparently start to grow within the water phase and precipitate when they become denser than the aqueous solution. A TEM image (Figure 2c) depicts the ordered pore structure of the fibers, which corresponds to a 2D hexagonal mesostructure of p6mm symmetry. The ordered pores extend along the fiber axis in a helical or circular

fashion as revealed by microscopy [39] and diffusional investigations [38, 40]. Such architecture is interesting in catalysis and this website controlled release applications. Ordered pore structure was further confirmed by XRD (Figure 3a). The pattern

displays a high intensity primary reflection at 2.37° of d spacing = 3.72 nm which confirms the hexagonal structure. Two additional secondary reflections are also observed verifying a long range order. The peaks appear in the low range of 2θ between 1.5° to 6° and are indexed as (100), (110), and (200) planes. Figure 2 Electron micrographs of MSF sample. Bacterial neuraminidase (a) SEM of fiber morphology, (b) SEM of some co-existing morphologies, and (c) TEM of fibers. Figure 3 XRD pattern (a) and N 2 ads/desorption isotherms (b) of mesoporous silica fibers. N2 sorption isotherms of MSF measured at 77 F are shown in Figure 3b. They have type IV responses typical to mesoporous materials with well-defined capillary condensation step at 0.3 p/po that is absent of any hysteresis. This indicates a uniform and narrow pore size distribution. Textural properties obtained from the XRD patterns (d spacing and lattice parameter a 0) and sorption isotherms (average pore size, surface area, and pore volume) for all samples are summarized in Table 2. The fibers have a BET surface area of 1,008 m2/g and a total pore NVP-BGJ398 volume of 0.64 cm3/g. The pore size, calculated from the desorption isotherm using the BJH theory was found to be 2.