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Liquid constrained

Simon, S.L., Park, J.Y., McKenna, G.B. Enthalpy recovery of a glass-forming liquid constrained in a nanoporous matrix negative pressure effects. Eur. Phys. J. E 8, 209-216 (2002)... [Pg.296]

An approximate treatment of the phenomenon of capillary rise is easily made in terms of the Young-Laplace equation. If the liquid completely wets the wall of the capillary, the liquids surface is thereby constrained to lie parallel to the wall at the region of contact and the surface must be concave in shape. The... [Pg.10]

Other SFA studies complicate the picture. Chan and Horn [107] and Horn and Israelachvili [108] could explain anomalous viscosities in thin layers if the first layer or two of molecules were immobile and the remaining intervening liquid were of normal viscosity. Other inteipretations are possible and the hydrodynamics not clear, since as Granick points out [109] the measurements average over a wide range of surface separations, thus confusing the definition of a layer thickness. McKenna and co-workers [110] point out that compliance effects can introduce serious corrections in constrained geometry systems. [Pg.246]

If 7 = 0, AT = 0, regardless of particle size. This is not expected, however, since chains emerging from a crystal face either make a highly constrained about-face and reenter the crystal or meander off into the liquid from a highly constrained attachment to the solid. In either case, a free-energy contribution is inescapable. [Pg.215]

Operated in this manner, the shell-and-tube type is a flooded evaporator (see Figure 7.3) and has oil drainage pots if using ammonia, or a mixture bleed system if the refrigerant is one of the halocarbons. The speed of the liquid within the tubes should be about 1 m/ s or more, to promote internal turbulence for good heat transfer. End cover baffles will constrain the flow to a number of passes, as with the shell-and-tube condenser. (See Section 6.4.)... [Pg.86]

Evaporators of this general type with dry expansion circuits will have the refrigerant within the tubes, in order to maintain a suitable continuous velocity for oil transport, and the liquid in the shell. These can be made as shell-and-tube, with the refrigerant constrained to a number of passes, or maybe shell-and-coil (see Figure 7.4). In both these configurations, baffles are needed on the water side to improve the turbulence, and the tubes maybe finned on the outside. Internal swirl strips or wires will help to keep liquid refrigerant in contact with the tube wall. [Pg.86]

The melting of ice is the reverse of the freezing of water. Energy becomes more constrained as it is transferred from the air in the room to the melting ice. At the same time, the molecules in the ice cube become less constrained, because they are free to move about in the liquid phase. Melting disperses matter but constrains energy. [Pg.979]

The substance in the more constrained phase has the lower entropy. For substances that are otherwise similar, liquid S gas. ... [Pg.995]

Phase changes, which convert a substance from one phase to another, have characteristic thermodynamic properties Any change from a more constrained phase to a less constrained phase increases both the enthalpy and the entropy of the substance. Recall from our description of phase changes in Chapter 11 that enthalpy increases because energy must be provided to overcome the intermolecular forces that hold the molecules in the more constrained phase. Entropy increases because the molecules are more dispersed in the less constrained phase. Thus, when a solid melts or sublimes or a liquid vaporizes, both A H and A S are positive. Figure 14-18 summarizes these features. [Pg.1020]

Figure 14.3 Vapor-liquid equilibrium data and calculated values for the carbon dioxide-n-hexane system. Calculations were done using interaction parameters from implicit and constrained least squares (LS) estimation, x and y are the mote fractions in the liquid and vapor phase respectively [reprinted from the Canadian Journal of Chemical Engineering with permission]... Figure 14.3 Vapor-liquid equilibrium data and calculated values for the carbon dioxide-n-hexane system. Calculations were done using interaction parameters from implicit and constrained least squares (LS) estimation, x and y are the mote fractions in the liquid and vapor phase respectively [reprinted from the Canadian Journal of Chemical Engineering with permission]...
Therefore, although the stability function was found to be positive at all the experimental conditions it becomes negative at mole fractions between 0 and the first measured data point. Obviously, if there were additional data available in this region, the simplified constrained LS method that was followed above would have yielded interaction parameters that do not result in prediction of false liquid phase splitting. [Pg.254]

The study of how fluids interact with porous solids is itself an important area of research [6], The introduction of wall forces and the competition between fluid-fluid and fluid-wall forces, leads to interesting surface-driven phase changes, and the departure of the physical behavior of a fluid from the normal equation of state is often profound [6-9]. Studies of gas-liquid phase equilibria in restricted geometries provide information on finite-size effects and surface forces, as well as the thermodynamic behavior of constrained fluids (i.e., shifts in phase coexistence curves). Furthermore, improved understanding of changes in phase transitions and associated critical points in confined systems allow for material science studies of pore structure variables, such as pore size, surface area/chemistry and connectivity [6, 23-25],... [Pg.305]

One extremely powerful feature of heterogeneous distillation is the ability to cross distillation boundaries. It was noted previously that distillation boundaries divide the compositions into two regions that cannot be accessed from each other. Decanters allow distillation boundaries to be crossed, as illustrated in Figure 12.32. The feed to the decanter at F is on one side of the distillation boundary. This splits in the decanter to two-liquid phases E and R. These two-liquid phases are now on opposite sides of the distillation boundary. Phase splitting in this way is not constrained by a distillation boundary, and exploiting a two-phase separation in this way is an extremely effective way to cross distillation boundaries. [Pg.251]

Traditionally, the production of LABs has been practiced commercially using either Lewis acid catalysts, or liquid hydrofluoric acid (HF).2 The HF catalysis typically gives 2-phenylalkane selectivities of only 17-18%. More recently, UOP/CEPSA have announced the DetalR process for LAB production that is reported to employ a solid acid catalyst.3 Within the same time frame, a number of papers and patents have been published describing LAB synthesis using a range of solid acid (sterically constrained) catalysts, including acidic clays,4 sulfated oxides,5 plus a variety of acidic zeolite structures.6"9 Many of these solid acids provide improved 2-phenylalkane selectivities. [Pg.328]


See other pages where Liquid constrained is mentioned: [Pg.573]    [Pg.11]    [Pg.279]    [Pg.573]    [Pg.11]    [Pg.279]    [Pg.104]    [Pg.1744]    [Pg.2409]    [Pg.145]    [Pg.479]    [Pg.738]    [Pg.123]    [Pg.395]    [Pg.441]    [Pg.386]    [Pg.89]    [Pg.125]    [Pg.12]    [Pg.975]    [Pg.978]    [Pg.981]    [Pg.996]    [Pg.1004]    [Pg.35]    [Pg.115]    [Pg.231]    [Pg.91]    [Pg.226]    [Pg.565]    [Pg.950]    [Pg.237]    [Pg.247]    [Pg.250]    [Pg.1317]    [Pg.254]    [Pg.380]    [Pg.88]    [Pg.469]    [Pg.12]   
See also in sourсe #XX -- [ Pg.495 ]

See also in sourсe #XX -- [ Pg.495 ]

See also in sourсe #XX -- [ Pg.495 ]




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Constrained flow at the outlet of a liquid pipeline

Constrained pressure at the inlet to a liquid pipeline

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