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Liquid water models

Fate and exposure analyses. The multimedia transport and transformation model is a dynamic model that can be used to assess time-varying concentrations of contaminants that are placed in soil layers at a time-zero concentration or contaminants released continuously to air, soil, or water. This model is used for determining the distribution of a chemical in the environmental compartments. An overview of the partitioning among the liquid, solid and/or gas phases of individual compartments is presented in Fig. 7. The exposure model encompasses... [Pg.60]

Pohorille, A. Benjamin, I., Structure and energetics of model amphiphilic molecules at the water liquid-vapor interface. A molecular dynamic study, J. Phys. Chem. 1993, 97, 2664-2670... [Pg.73]

Reviews on water structure models include Mishima and Stanley (1998), Wallqvist and Mountain (1999), and Ludwig (2001). Mishima and Stanley (1998) concentrated their review on three relatively recent water structure hypotheses (1) the stability limit hypothesis (Speedy, 1982), (2) the singularity-free hypothesis (Sastry et al., 1996), and (3) the liquid-liquid phase transition hypothesis (Poole et al., 1992). [Pg.19]

The superheated-liquid model introduced earlier to explain LNG-water RPTs was not considered applicable for smelt-water explosions since the very large temperature difference between the smelt and water would, it... [Pg.109]

Thus, it would appear that overpressures experienced in the air from LNG RPTs for spills less than about 30 are not particularly large unless one is very close to the spill site. Overpressures in the water are much larger, as shown in Table X from transducer measurements about 0.7 m from the surface. In fact, in one instance, the overpressure in the water exceeded the critical pressure of the LNG this would not have been expected from the superheated liquid model. [Pg.141]

In this article, we suggest that a modified superheated-liquid model could explain many facts, but the basic premise of the model has never been established in clearly delineated experiments. The simple superheated-liquid model, developed for LNG and water explosions (see Section III), assumes the cold liquid is prevented from boiling on the hot liquid surface and may heat to its limit-of-superheat temperature. At this temperature, homogeneous nucleation results with significant local vaporization in a few microseconds. Such a mechanism has been rejected for molten metal-water interactions since the temperatures of most molten metals studied are above the critical point of water. In such cases, it would be expected that a steam film would encapsulate the water to... [Pg.160]

To prove or disprove such a modified superheated-liquid model, experiments are necessary to delineate the rates and products of reaction between molten metals and water in a high-temperature environment with and without substrates which could participate in the reaction. [Pg.161]

Weber and Newman do the averaging by using a capillary framework. They assume that the two transport modes (diffusive for a vapor-equilibrated membrane and hydraulic for a liquid-equilibrated one) are assumed to occur in parallel and are switched between in a continuous fashion using the fraction of channels that are expanded by the liquid water. Their model is macroscopic but takes into account microscopic effects such as the channel-size distribution and the surface energy of the pores. Furthermore, they showed excellent agreement with experimental data from various sources and different operating conditions for values of the net water flux per proton flux through the membrane. [Pg.456]

Relaxation dispersion data for water on Cab-O-Sil, which is a monodis-perse silica fine particulate, are shown in Fig. 2 (45). The data are analyzed in terms of the model summarized schematically in Fig. 3. The y process characterizes the high frequency local motions of the liquid in the surface phase and defines the high field relaxation dispersion. There is little field dependence because the local motions are rapid. The p process defines the power-law region of the relaxation dispersion in this model and characterizes the molecular reorientations mediated by translational displacements on the length scale of the order of the monomer size, or the particle size. The a process represents averaging of molecular orientations by translational displacements on the order of the particle cluster size, which is limited to the long time or low frequency end by exchange with bulk or free water. This model has been discussed in a number of contexts and extended studies have been conducted (34,41,43). [Pg.299]

In light of the discussion of hydrogen bonds between water molecules, one can expect some degree of association of molecules in liquid water. Many models for the structure of water have been proposed, but we discuss only one. [Pg.11]

Uniformist, Average Models. We divide the current water structure models into two major categories. The first treats water essentially as an unstructured liquid while the second admits the simultaneous existence of at least two states of water—i.e., the structural models which Frank has termed the mixture models. ... [Pg.90]

Tmskett and Dill (2002) proposed a two-dimensional water-like model to interpret the thermodynamics of supercooled water. This model is consistent with model (1) for liquid water. Cage-like and dense fluid configurations correspond to transient structured and unstructured regions, observed in molecular simulations of water (Errington and Debenedetti, 2001). Truskett and Dill s model provides a microscopic theory for the global phase behavior of water, which predicts the liquid-phase anomalies and expansion upon freezing. [Pg.119]

Gel Permeation Chromatography (GPC) GPC of all samples were recorded with a Waters Associates Model 244 high-pressure liquid chromatograph using a dilute solution (0.02% in tetrahydrofuran and a flow rate of 5 ml/min). The chromatograph was connected with four microstyragel columns in series (pore size 10 , 10 ,... [Pg.157]

The structure of liquid water has been studied both by Monte Carlo [355] and molecular dynamics [356]. In these calculations, hydrogen-bond potentials based on the water dimer model are unsatisfactory, and the simulations have to include the increased binding energy due to cooperativity to give acceptable thermodynamical results [357]. [Pg.93]

Figure 8.7 - along the saturation curve of liquid water for model... [Pg.189]


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