The adsorption of water in two mesoporous silica materials with cylindrical pores of uniform diameter, MCM-41 and SBA-15, was studied by 1H MAS (MAS=magic angle spinning) and static solid-state NMR spectroscopy. All observed hydrogen atoms are either surface -SiOH groups or hydrogen-bonded water molecules. Unlike MCM-41, some strongly bound water molecules exist at the inner surfaces of SBA-15 that are assigned to surface defects. At higher filling levels, a further difference between MCM-41 and SBA-15 is observed. Water molecules in MCM-41 exhibit a bimodal line distribution of chemical shifts, with one peak at the position of inner-bulk water, and the second peak at the position of water molecules in fast exchange with surface -SiOH groups. In SBA-15, a single line is observed that shifts continuously as the pore filling is increased. This result is attributed to a different pore-filling mechanism for the two silica materials. In MCM-41, due to its small pore diameter (3.3 nm), pore filling by pore condensation (axial-pore-filling mode) occurs at a low relative pressure, corresponding roughly to a single adsorbed monolayer. For SBA-15, owing to its larger pore diameter (8 nm), a gradual increase in the thickness of the adsorbed layer (radial-pore-filling mode) prevails until pore condensation takes place at a higher level of pore filling.
The hydrogen bond interaction of pyridine with the silanol groups of the inner surfaces of MCM-41 and SBA-15 ordered mesoporous silica has been studied by a combination of solid-state NMR techniques. The pore diameters were varied between 3 and 4 nm for MCM-41 and between 7 and 9 nm for SBA-15. 1H MAS experiments performed under magic angle spinning (MAS) conditions in the absence and the presence of pyridine-d 5 reveal that the large majority of silanol groups are located in the inner surfaces, isolated from each other but able to form hydrogen bonds with pyridine. On the other hand, low- and room-temperature 15N CPMAS and MAS experiments (CP ≡ cross-polarization) performed on pyridine-15 N show that at low concentrations all pyridine molecules are involved in hydrogen bonds with the surface silanol groups. In the presence of an excess of pyridine, a non-hydrogen-bonded pyridine phase is observed at 120 K in the slow hydrogen bond exchange regime and associates with an inner core phase. From these measurements, the number of pyridine molecules bound to the inner surfaces corresponding to the number of silanol groups could be determined to be n OH ≈ 3 nm-2 for MCM-41 and ≈3.7 nm-2 for SBA-15. At room temperature and low concentrations, the pyridine molecules jump rapidly between the hydrogen-bonded sites. In the presence of an excess of pyridine, the hydrogen-bonded binding sites are depleted as compared to low temperatures, leading to smaller apparent numbers n OH. Using a correlation established previously between the 15N and 1H chemical shifts and the NHO hydrogen bond geometries, as well as with the acidity of the proton donors, the distances in the pyridine−hydroxyl pairs were found to be about r HN = 1.68 Å, r OH = 1.01 Å, and r ON = 2.69 Å. This geometry corresponds in the organic solid state to acids exhibiting in water a pK a of about 4. Room-temperature 15N experiments on static samples of pyridine-15 N in MCM-41 at low coverage show a residual 15N chemical shift anisotropy, indicating that the jumps of pyridine between different different silanol hydrogen bond sites is accompanied by an anisotropic reorientational diffusion. A quantitative analysis reveals that in this regime the rotation of pyridine around the molecular C 2 axis is suppressed even at room temperature, and that the angle between the Si−O axes and the OH axes of the isolated silanol groups is about 47°. These results are corroborated by 2H NMR experiments performed on pyridine-4-d 1. In contrast, in the case of SBA-15 with the larger pore diameters, the hydrogen bond jumps of pyridine are associated with an isotropic rotational diffusion, indicating a high degree of roughness of the inner surfaces. This finding is correlated with the finding by 29Si CPMAS of a substantial amount of Si(OH)2 groups in SBA-15, in contrast to the MCM-41 materials. The Si(OH)2 groups are associated with surface defects, exhibiting not only silanol groups pointing into the pore center but also silanol groups pointing into other directions of space including t...
Benzene-d 6 confined in the hexagonal ordered cylindrical pores of mesoporous silica SBA-15 (pore diameter 8.0 nm) was studied by low-temperature 2H-solid-state NMR spectroscopy in the temperature range between 236 and 19 K and compared to bulk benzene-d 6. The solid-state spectra of the bulk benzene-d 6 exhibit quadrupolar Pake patterns at high and low temperatures, and in the intermediate temperature regime the typical line shape changes caused by rotational jumps around the 6-fold axis. At all temperatures the benzene molecules are characterized by a single rotational correlation time. For benzene-d 6 confined in SBA-15, however, these exchange dominated line shapes are not found. At all temperatures below the freezing point the spectra of benzene in the silica show the coexistence of two states with temperature-dependent intensity ratios. This behavior is the result of a Gaussian distributions of activation energies for the rotational jumps inside the pores. For the solid I−solid II (fast 6-fold jump to slow 6-fold jump) transition the center of the distribution is at 40 K (6.0 kJ/mol) with a width of 19.5 K (2.9 kJ/mol). For the liquid−solid I (liquidlike to fast 6-fold jump) transition the center of the distribution is at 204 K (30.6 kJ/mol) and the width is 15 K (2.2 kJ/mol). From the pore volume and the filling factor, a thickness of four molecular layers of this surface phase is estimated.
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