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Bulk water characteristics

The sorption of water by excipients derived from cellulose and starch has been considered by numerous workers, with at least three thermodynamic states having been identified [82]. Water may be directly and tightly bound at a 1 1 stoichiometry per anhydroglucose unit, unrestricted water having properties almost equivalent to bulk water, or water having properties intermediate between these two extremes. The water sorption characteristics of potato starch and microcrystalline cellulose have been determined, and comparison of these is found in Fig. 11. While starch freely adsorbs water at essentially all relative humidity values, microcrystalline cellulose only does so at elevated humidity values. These trends have been interpreted in terms of the degree of available cellulosic hydroxy groups on the surfaces, and as a function of the amount of amorphous material present [83]. [Pg.30]

Biofilm Characteristics and Interactions with the Bulk Water Phase... [Pg.56]

When designing sewer networks, particularly gravity sewers, reaeration is the major process that should be focused on to reduce sulfide formation and the formation of organic odorous substances (cf. Section 4.4). A number of hydraulic and systems characteristics can be managed to increase the reaeration rate and avoid or reduce sulfide-related problems. The hydraulic mean depth, the hydraulic radius, the wastewater flow velocity and the slope of the sewer pipe are, in this respect, important factors that are dealt with in Section 4.4. It should be stressed that it is not necessarily the objective to avoid sulfide formation (in the sewer biofilm), but the sulfide that occurs in the bulk water phase should be at a low concentration level. Therefore, the DO concentration in the bulk water phase should not be lower than about 0.2-0.5 g02 m-3, sufficiently high to oxidize sulfide before a considerable amount is emitted to the sewer atmosphere. [Pg.150]

One of the most important characteristics of micelles is their ability to enclose all kinds of substances. Capture of these compounds in micelles is generally driven by hydrophobic, electrostatic and hydrogen-bonding interactions. The dynamics of solubilization into micelles are similar to those observed for entrance and exit of individual surfactant molecules, but the micelle-bound substrate will experience a reaction environment different from bulk water, leading to kinetic medium effects308. Hence, micelles are able to catalyse or inhibit reactions. The catalytic effect on unimolecular reactions can be attributed exclusively to the local medium effect. For more complicated bimolecular or higher-order reactions, the rate of the reaction is affected by an additional parameter the local concentrations of the reacting species in or at the micelle. [Pg.1080]

Vapor (Gas) Irritant Characteristics — Since MSDSs often provide non-qualifying statements, the most appropriate of five statements listed below is given. (Source National Academy of Sciences, Committee on Hazardous Materials, "Evaluation of the Hazard of Bulk Water Transportation of Industrial Chemicals, A Tentative Guide," Washington, D.C., 1970.)... [Pg.5]

Some characteristics and attributes of the molecule of H-,0 and of bulk water... [Pg.17]

As a result many different functioning structures may appear within the transient architecture of liquid water. This makes it possible for liquid water to perform in several roles. Water is thus comparable to a supramolecular assembly, and indeed it has been postulated to act as a template for macromolecular systems (e.g. nucleic acids) which have evolved and have breathed life into non-purposive molecular assemblies. In Table 1 we compare some characteristics and attributes of bulk water and the molecule of H2O. [Pg.17]

In a theoretical model, we considered the dynamics of bound water molecules and when they become free by translational and rotational motions. Two coupled reaction-diffusion equations were solved. The two rate constants, kbf and kjb, were introduced to describe the transition from bound (to the surface) to free (from the surface) and the reverse, respectively. We also took into account the effect of the bulk water re-entry into the layer—a feedback mechanism—and the role of orientational order and surface inhomogeneity on the observed decay characteristics. With this in mind, the expressions for the change in density with time were written defining the feedback as follows ... [Pg.15]

Kasai and Jones (270) applied MAS to the study of water in zeolites A, X, Y, mordenite, ZSM-5, and silicalite. They found that although the signals were sometimes quite broad, their chemical shifts were characteristic of the zeolite (Fig. 59). They interpret this as the effect of the disruption of hydrogen bonding of bulk water by the zeolitic framework and of the interaction of water molecules with framework oxygens. An inverse relationship was found between the chemical shift and the Si/Al ratio. The chemical shift of water in silicalite is quite different from that in ZSM-5 and does not fit this... [Pg.302]

Cory and Garroway [13] introduced the NMR pulsed gradient stimulated echo method to study compartments which are too small to be observed by conventional NMR imaging. They showed so-called proton displacement profiles of bulk water and dimethyl sulfoxide. The displacements are due to free diffusion and are Gaussian shaped. The profile of water in yeast cells showed restricted diffusion with a characteristic cell width of approximately 5 /xm. [Pg.160]

H2O] is the molarity of water in the protein solution, Tij,r and Tiw are the relaxation times for protons in the hydration spheres of the protein and in the bulk water, [Pr] is the protein concentration in mol/1, n the number of waters bound to each protein molecule, and rvr the residence time for water protons on the protein molecule. In writing Eq. (19) it was assumed for simplicity that there is only one type of hydration site with characteristic rpr and Tipr- It is seen that the relaxation enhancement through the presence of the protein is... [Pg.111]

Fig. 6.15. Multiplex stimulated Raman loss microspectroscopy of 20-pm polystyrene beads dispersed in water. A Raman spectra retrieved from SRL spectra of an individual bead and of bulk water at locations indicated by circles and squares, respectively, in the images. B Reconstructed Raman images of the beads representing the density maps of three characteristic Raman resonances at 1003 cm-1, 2904 cm-1, and 3066 cm-1 of polystyrene (Courtesy of Evelyn Ploetz et al., after [21])... Fig. 6.15. Multiplex stimulated Raman loss microspectroscopy of 20-pm polystyrene beads dispersed in water. A Raman spectra retrieved from SRL spectra of an individual bead and of bulk water at locations indicated by circles and squares, respectively, in the images. B Reconstructed Raman images of the beads representing the density maps of three characteristic Raman resonances at 1003 cm-1, 2904 cm-1, and 3066 cm-1 of polystyrene (Courtesy of Evelyn Ploetz et al., after [21])...
An important performance characteristic of passive samplers that operate in the TWA regime is the diffusion barrier that is inserted between the sampled medium and the sorption phase. This barrier is intended to control the rate of mass transfer of analyte molecules to the sorption phase. It is also used to define the selectivity of the sampler and prevent certain classes (e.g., polar or nonpolar compounds) of analytes, molecular sizes, or species from being sequestered. The resistance to mass transfer in a passive sampler is, however, seldom caused by a single barrier (e.g., a polymeric membrane), but equals the sum of the resistances posed by the individual media (e.g., aqueous boundary layer, biofilm, and membrane) through which analyte diffuses from the bulk water phase to the sorption phase.19 The individual resistances are equal to the reciprocal value of their respective mass transfer coefficients and are additive. They are directly proportional to the thickness of the barrier... [Pg.45]

The size and characteristics of soft-core reverse micelles are critically dependent upon the water content of the solution. The water present tends to accumulate with the soft-core to form an isolated pool which may exhibit unique properties. At a low ratio of water to surfactant (Wo < 10) the activity of the water is greatly diminished as compared with that of bulk water. The quantity of water... [Pg.77]

Wide variety of experimental techniques and data remain insufficient to explain characteristics even of pure water. The fraction of water modified by the particles surface in dispersions is very small and its properties differ only slightly from that of bulk water. This brings about additional complexity to the study of the properties of nanocarbon hydration layers. [Pg.572]

Measurements of the dynamic properties of the surface water, particularly NMR measurements, have shown that the characteristic time of the water motion is slower than the bulk water value by a factor of less than 100. The motion is anisotropic. There is litde or no irrotadonally bound water. Study of a protein labeled covalently with a nitroxide spin probe (Polnaszek and Bryant, 1984a,b) has shown that the diffusion constant of the surface water is about 5-fold below the bulk water value. The NMR results are in agreement with measurements of dielectric relaxation of water in protein powders (Harvey and Hoekstra, 1972). [Pg.128]


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See also in sourсe #XX -- [ Pg.3 , Pg.7 , Pg.8 , Pg.9 ]




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Bulk characteristics

Bulk water

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