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Confinement medium liquid

From the above examples it is clear that reaction cavity provided by an organized or confining medium has unique features that mimics some of the features of proteins. While crystals and zeolites provide reaction cavities that are inflexible, there is a whole spectrum of organized and confined media (e.g., micelles, host-guest complexes, monolayers and bilayers, liquid crystals etc.,) that allow different degrees of freedom to the reactant molecules. These systems demonstrate clever usage of favorable entropy that is so important in natural systems. One should keep in mind... [Pg.563]

Experimental verification of all the above hypotheses has not been possible because, as mentioned above, liquid water cannot be supercooled without crystallization below 232 K, while amorphous ice cannot be superheated above 155 K. So, nobody has been able to find the LDL, except in a confined medium. However, the properties of water are expected to differ in a confined medium from those in the bulk. [Pg.337]

In condensed matter physics, the effects of disorder, defects, and impurities are relevant for many materials properties hence their understanding is of utmost importance. The effects of randomness and disorder can be dramatic and have been investigated for a variety of systems covering a wide field of complex phenomena [109]. Examples include the pinning of an Abrikosov flux vortex lattice by impurities in superconductors [110], disorder in Ising magnets [111], superfluid transitions of He in a porous medium [112], and phase transitions in randomly confined smectic liquid crystals [113, 114]. [Pg.209]

Note that in both Equations 9.43 and 9.44 the terms reflecting the influence of curvature-initiated excess pressure in a confined medium, that is, the terms in the second set of round brackets, might be expressed through the parameters of solid/ wall and liquid/wall interfaces (cf. Equations 9.40 and 9.42). Further simplification of the analysis may then be achieved by neglecting the difference between Vt(L) and Vt(s) where Vt is the molar volume in the k-th sublayer of liquid or solid boundary phase. From Equation 9.44 we will obtain ... [Pg.174]

While the properties of the fast dynamic mode related to intrapore orientational fluctuations of the director field are quite well understood, the origin of various slow dynamic processes is for the moment still far from being resolved. The observed characteristics of the slow mode are typically very specific for a selected system and strongly depend on the morphology and composition of the confining medium. The slow process usually exhibits a profound non-exponetial relaxation, which is attributed to the structural randomness of the material. Further studies in confined liquid crystal media with well-resolved morphological details are needed to elucidate the nature of different slow modes. [Pg.156]

The earliest SFA experiments consisted of bringing the two mica sheets into contact m a controlled atmosphere (figure Bl.20.61 or (confined) liquid medium [14, 27, 73, 74 and 75]. Later, a variety of surfactant layers [76, 77], polymer surfaces [5, 9, fO, L3, 78], poly electrolytes [79], novel materials [ ] or... [Pg.1738]

It has been proposed recently [28] that static friction may result from the molecules of a third medium, such as adsorbed monolayers or liquid lubricant confined between the surfaces. The confined molecules can easily adjust or rearrange themselves to form localized structures that are conformal to both adjacent surfaces, so that they stay at the energy minimum. A finite lateral force is required to initiate motion because the energy barrier created by the substrate-medium system has to be overcome, which gives rise to a static friction depending on the interfacial substances. The model is consistent with the results of computer simulations [29], meanwhile it successfully explains the sensitivity of friction to surface film or contamination. [Pg.182]

Gas mobility depends on the permeability of the porous medium. In the presence of foam gas mobility is the mobility of the continuous gas phase through the free channels and the mobility of the confined gas along with the liquid. Formally the relative permeability of each phase (liquid or gas) can be expressed by Darcy s equation. [Pg.723]

Kinetic studies on the sulfur dioxide insertion have been few and most have utilized liquid SO2 as the reaction medium. The most exhaustive investigation in neat SO2 was conducted on the systems CpFe(CO)2R and various (R Cp)Fe(CO)2R (77, 74, 75) studied cursorily were CpMo(CO)3R, CpRu(CO)2R, RMn(CO)5, and RRe(CO)5 71, 76). Kinetic studies in organic solvents have been confined to a few CpFe(CO)2R complexes 71, 77). Of the many SO2 reactions of the main group metal-carbon systems, only those involving some MesSnR aryl and benzyl compounds were examined kinetically 51, 52, 99). [Pg.38]

A porous medium affects a liquid mixture not only by mere confinement to volumes of nanoscopic dimensions [91] but also by the energetic preference of the solid substrate for molecules of one of the components of the mixture [92, 93]. This selectivity causes an enrichment of the component in the proximity of the pore walls. For sufficiently wide pores, the decay length of the resulting concentration profile corresponds to the correlation length of concentration fluctuations [94]. In narrow pores, on the other hand, when the mean pore width D is less than concentration profiles near the pore walls overlap, thereby causing enhanced adsorption. [Pg.160]


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