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Free water molecules

The mass balance equations express conservation of mass in terms of the components in the basis. The mass of each chemical component is distributed among the species and minerals that make up the system. The water component, for example, is present in free water molecules of the solvent and as the water required to make... [Pg.42]

The H NMR derivative spectra of natural clinoptilolite sample CT and two modified clinoptilolite samples CT ODA 2 and CT ODA 5 are at Fig. 4. The NMR signal arose from hydrogen in OH groups of water that are placed along the clinoptilolite channel walls, from the CH3, CH2 and —NH3+ groups that are in the ODA chains and also from free water molecules that are always present in natural clinoptilolites. [Pg.17]

The behavior of metal ions in reversed micelles may be more interesting, since the reversed micelle provides less solvated metal ions in its core (Sunamoto and Hamada, 1978). Through kinetic studies on the hydrolysis of the p-nitrophenyl ester of norleucine in reversed micelles of Aerosol OT and CC14 which solubilize aqueous cupric nitrate, Sunamoto et al. (1978) observed the formation of naked copper(II) ion this easily formed a complex with the substrate ester (formation constant kc = 108—109). The complexed substrate was rapidly hydrolyzed by free water molecules acting as effective nucleophiles. [Pg.481]

Figure 5-11 shows a simple model of the compact double layer on metal electrodes. The electrode interface adsorbs water molecules to form the first mono-molecular adsorption layer about 0.2 nm thick next, the second adsorption layer is formed consisting of water molecules and hydrated ions these two layers constitute a compact electric double layer about 0.3 to 0.5 nm thick. Since adsorbed water molecules in the compact layer are partially bound with the electrode interface, the permittivity of the compact layer becomes smaller than that of free water molecules in aqueous solution, being in the range from 5 to 6 compared with 80 of bulk water in the relative scale of dielectric constant. In general, water molecules are adsorbed as monomers on the surface of metals on which the affinity for adsorption of water is great (e.g. d-metals) whereas, water molecules are adsorbed as clusters in addition to monomers on the surface of metals on which the affinity for adsorption of water is relatively small (e.g. sp-metals). [Pg.132]

Fig. 5-11. A simple model of an interfacial compact double layer on metal electrodes H20,j = adsorbed water molecule H20. = water molecule coordinated with ions H20 . = free water molecule ih = hydrated ions. [From Bockiis-Devanathan-Muller, 1963.]... Fig. 5-11. A simple model of an interfacial compact double layer on metal electrodes H20,j = adsorbed water molecule H20. = water molecule coordinated with ions H20 . = free water molecule ih = hydrated ions. [From Bockiis-Devanathan-Muller, 1963.]...
Serine hydroxymethyl transferase catalyzes the decarboxylation reaction of a-amino-a-methylmalonic acid to give (J )-a-aminopropionic acid with retention of configuration [1]. The reaction of methylmalonyl-CoA catalyzed by malonyl-coenzyme A decarboxylase also proceeds with perfect retention of configuration, but the notation of the absolute configuration is reversed in accordance with the CIP-priority rule [2]. Of course, water is a good proton source and, if it comes in contact with these reactants, the product of decarboxylation should be a one-to-one mixture of the two enantiomers. Thus, the stereoselectivity of the reaction indicates that the reaction environment is highly hydro-phobic, so that no free water molecule attacks the intermediate. Even if some water molecules are present in the active site of the enzyme, they are entirely under the control of the enzyme. If this type of reaction can be realized using synthetic substrates, a new method will be developed for the preparation of optically active carboxylic acids that have a chiral center at the a-position. [Pg.3]

Figure 10.4 Normal modes of vibration of the free water molecule. Figure 10.4 Normal modes of vibration of the free water molecule.
In the second item above, the presence of bound and free water molecules was noted. Both bound ions and ionic surfactant groups are hydrated to about the same extent in the micelle as would be observed for the independent ions. The dehydration of these ionic species is an endothermic process, and this would contribute significantly to the AH of micellization if ion dehydration occurred. In the next section we discuss the thermodynamics of micellization, but it can be noted for now that there is no evidence of a dehydration contribution to the AH of micelle formation. The extent of micellar hydration can be estimated from viscosity... [Pg.363]

This bimodal dynamics of hydration water is intriguing. A model based on dynamic equilibrium between quasi-bound and free water molecules on the surface of biomolecules (or self-assembly) predicts that the orientational relaxation at a macromolecular surface should indeed be biexponential, with a fast time component (few ps) nearly equal to that of the free water while the long time component is equal to the inverse of the rate of bound to free transition [4], In order to gain an in depth understanding of hydration dynamics, we have carried out detailed atomistic molecular dynamics (MD) simulation studies of water dynamics at the surface of an anionic micelle of cesium perfluorooctanoate (CsPFO), a cationic micelle of cetyl trimethy-lainmonium bromide (CTAB), and also at the surface of a small protein (enterotoxin) using classical, non-polarizable force fields. In particular we have studied the hydrogen bond lifetime dynamics, rotational and dielectric relaxation, translational diffusion and vibrational dynamics of the surface water molecules. In this article we discuss the water dynamics at the surface of CsPFO and of enterotoxin. [Pg.214]

Fig. 5 (a) Power spectrum of oxygen atoms of bound and free water molecules, (b) Power spectrum of hydrogen atoms of different kinds of water molecules. [Pg.217]

These atoms were found to lie in the same plane as the other atoms of the molecule. The dimensions O—H = 0.95 A and angle H—O—H — 108° are essentially the same as those of the free water molecule. This is the result that would be expected not for a single bond between the oxygen atom and the copper atom, which would make the Cu-—O—H angles about 105°, but rather for a double bond or for singlet-bond double-bond resonance. [Pg.159]

An ionization reaction often decreases the entropy of a solution, instead of increasing it as one might at first expect, because clustering of water molecules around the ions can result in a net decrease in the number of free water molecules. [Pg.35]

The free water molecule was assumed to lie in the yz plane with its C2 axis pointing along the z-direction and with d(O-H) = 95.7 pm and ZHOH = 104.57°. A perfect agreement with experimental values is obtained for the asymmetry parameter and an antishielding factor (1 - yoo) = 22.7 is required for matching the coupling constant Cq. As for corundum, changing atomic radii alters only the y value. [Pg.284]

Table VIII. Absolute O NMR shielding tensors (values in ppm) for the free water molecule (AEE = 56.1 eV) and a crystalline tungstate K2W04 (AEE = t ) assuming that <(a0/r)3> = 5.0 + q(O). Parametrization for K1WOd was r t(W) =... Table VIII. Absolute O NMR shielding tensors (values in ppm) for the free water molecule (AEE = 56.1 eV) and a crystalline tungstate K2W04 (AEE = t ) assuming that <(a0/r)3> = 5.0 + q(O). Parametrization for K1WOd was r t(W) =...
Interactions between water and the polar head groups of lipid molecules are necessary for the formation of lamellar phases however, it appears that there is no free water associated with the 13 nm trilaminar units. This is supported by the observation that this periodicity does not increase with increasing stratum corneum water content.22 There is likely water hydrogen bonded to the polar regions of the lamellae. In contrast, the minor short periodicity swells from 5.8 to 6.6 nm as the water content of stratum corneum increases from 12 to 50%.23 This suggests that the lipid lamellae are simple individual bilayers and free water molecules can exist between adjacent bilayers, thus causing the increase in the lamellar spacing. [Pg.25]

Salt induced peptide formation [108] is based on a dehydrating activity of concentrated NaCl solutions in which free water molecules are less available, which drives the equilibrium towards peptide formation. This change in the thermodynamic barrier is coupled to a decrease of the kinetic barrier owing to the addition of a Cu(II) salt catalyst. A complex of copper with two amino acid ligands 14 has been proposed to be responsible for the catalytic process. In this way, the reaction between two amino acid ligands leading to peptide bond formation can take place intramolecularly ... [Pg.86]


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