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Pore volume scattering

Characterization. When siHca gel is used as an adsorbent, the pore stmcture determines the gel adsorption capacity. Pores are characterized by specific surface area, specific pore volume (total volume of pores per gram of solid), average pore diameter, pore size distribution, and the degree to which entrance to larger pores is restricted by smaller pores. These parameters are derived from measuring vapor adsorption isotherms, mercury intmsion, low angle x-ray scattering, electron microscopy, gas permeabiHty, ion or molecule exclusion, or the volume of imbibed Hquid (1). [Pg.491]

N2 adsorption-desorption isotherms revealed that MCs had hi surface area (>1200 m /g) and large pore volume (>1.0 cm /g). From SAXS patterns of the prepared materials, it was confirmed that pores of SBA-15 and CMK-3 retained highly ordered 2-dimensional hexagonal type arrangement [5], while MCM-48 had 3-dimensional cubic type pore structure. It should be noted that a new scattering peak of (110) appeared in the CMK-1 after the removal of MCM-48 template. Furthermore, the pore size of CMK-1 and the wall thickness of MCM-48 were found to be 2.4 nm and 1.3 nm, respectively. This result demonstrates that a systematic transformation of pore structure occurred during the replication process from MCM-48 to CMK-1 [6]. [Pg.610]

After attachment of surface ligands the pore size decreased as expected. In addition to small-angle X-ray scattering and transmission electron microscopy, which are used to obtain information about structural ordering, nitrogen adsorption provides important information about solids under study such as BET surface area, pore size, pore volume, microporosity and surface heterogeneity. Pore size analysis for OMMs is especially crucial and it was performed by the KJS method,48 which was elaborated especially for ordered mesostructures. Table 1 presents adsorption parameters for the materials under study and provides details about calculations. [Pg.330]

The severe computational burden associated with assembling and carrying out adsorption calculations on disordered model microstructures for porous solids, such as those discussed in Sections ILA and II.B, has until recently limited the development of pore volume characterization methods in this direction. While the reahsm of these models is highly appealing, their application to experimental isotherm or scattering data for interpretation of adsorbent pore structure remains cumbersome due to the structural complexity of the models and the computational resources that must be brought to bear in their utilization. Consequently, approximate pore structure models, based upon simple pore shapes such as shts or cylinders, have been retained in popular use for pore volume characterization. [Pg.219]

Vollet D R, Scalar J P, Donatti D A et al (2(X)8) A thermoporometry and small-angle x-ray scattering study of wet silica sonogels as the pore volume fraction is varied. Journal of Physics-Condensed Matter 20 1-7... [Pg.498]


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