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Liquid-like

Al-Obaidi A H R, Rigby S J, Hegarty J N M, Bell S E J and McGarvey J J 1996 Direct formation of silver and gold metal liquid-like films (MELLFS) from thiols and sols without organic solvents SERS and AFM studies ICORS 96 XVth Int. Conf on Raman Spectroscopy ed S A Asher and P B Stein (New York Wiley) pp 590-1... [Pg.1232]

Rare-gas clusters can be produced easily using supersonic expansion. They are attractive to study theoretically because the interaction potentials are relatively simple and dominated by the van der Waals interactions. The Lennard-Jones pair potential describes the stmctures of the rare-gas clusters well and predicts magic clusters with icosahedral stmctures [139, 140]. The first five icosahedral clusters occur at 13, 55, 147, 309 and 561 atoms and are observed in experiments of Ar, Kr and Xe clusters [1411. Small helium clusters are difficult to produce because of the extremely weak interactions between helium atoms. Due to the large zero-point energy, bulk helium is a quantum fluid and does not solidify under standard pressure. Large helium clusters, which are liquid-like, have been produced and studied by Toennies and coworkers [142]. Recent experiments have provided evidence of... [Pg.2400]

Flard spherocylinders (cylinders witli hemispherical end caps) were studied using computer simulations [118]. In addition to a nematic phase, such particles also display a smectic-A phase, in which tire particles are arranged in liquid-like layers. To observe tliis transition, ratlier monodisperse particles are needed. The smectic-A phase was indeed observed in suspensions of TMV particles [17]. [Pg.2689]

Finally, the molecules in all layers above the first are postulated to have the same partition function 9, as in the bulk liquid, so that 9, = 9, j,j for i > 1. This is of course equivalent to the BET assumption of liquid-like properties for these higher layers. [Pg.45]

In general there are two factors capable of bringing about the reduction in chemical potential of the adsorbate, which is responsible for capillary condensation the proximity of the solid surface on the one hand (adsorption effect) and the curvature of the liquid meniscus on the other (Kelvin effect). From considerations advanced in Chapter 1 the adsorption effect should be limited to a distance of a few molecular diameters from the surface of the solid. Only at distances in excess of this would the film acquire the completely liquid-like properties which would enable its angle of contact with the bulk liquid to become zero thinner films would differ in structure from the bulk liquid and should therefore display a finite angle of contact with it. [Pg.123]

Some liquids like caustic soda can crystallize with additional heat. [Pg.189]

With its support system pressurized above the seal chamber pressure, this double seal functions well with toxic and dangerous liquids (like the back-to-back dual seal). If the support system is pressurized at / the seal chamber pressure, this seal can handle higher pressures where a single seal would fail. If the support system should be non pressurized... [Pg.197]

In a separate study using the JKR technique, Chaudhury and Owen [48,49] attempted to understand the correlation between the contact adhesion hysteresis and the phase state of the monolayers films. In these studies, Chaudhury and Owen prepared self-assembled layers of hydrolyzed hexadecyltrichlorosilane (HTS) on oxidized PDMS surfaces at varying degrees of coverage by vapor phase adsorption. The phase state of the monolayers changes from crystalline (solidlike) to amoiphous (liquid-like) as the surface coverage (0s) decreases. It was found that contact adhesion hysteresis was the highest for the most closely packed... [Pg.102]

Fig. 12. Schematic representation of solid-like (crystalline), amorphous solid, and liquid-like surface layers (reproduced from [87], copyright American Chemical Society). Fig. 12. Schematic representation of solid-like (crystalline), amorphous solid, and liquid-like surface layers (reproduced from [87], copyright American Chemical Society).
Perlite and Solka-floc are finely divided powders manufactured from a volcanic mineral and from wood pulp respectively, which have filtration properties very similar to those of diatomite. Like diatomite, they are inert to a wide range of process liquids. Like diatomite, they are available in a range of particle-size distributions to give the desired clarity and flowrate in different applications. On a cost-of-use basis, they are as economical as, or more economical than, diatomite. [Pg.112]

The largest correlation times, and thus the slowest reorientational motion, were shown by the three C- Fl vectors of the aromatic ring, with values of between approximately 60 and 70 ps at 357 K, values expected for viscous liquids like ionic liquids. The activation energies are also in the typical range for viscous liquids. As can be seen from Table 4.5-1, the best fit was obtained for a combination of the Cole-Davidson with the Lipari-Szabo spectral density, with a distribution parame-... [Pg.171]

Fan turbine 6 blades 12 in., 45° Pitch Tank and liquids like above No baffles 0.67 22... [Pg.331]

Anchor impeller 22in. Diam. Tank and liquids like above 0.5 up to Nr, = 300 22... [Pg.331]

The ideal gas law offers a simple approach to the experimental determination of the molar mass of a gas. Indeed, this approach can be applied to volatile liquids like acetone (Example 5.4). All you need to know is the mass of a sample confined to a container of fixed volume at a particular temperature and pressure. [Pg.109]


See other pages where Liquid-like is mentioned: [Pg.640]    [Pg.595]    [Pg.830]    [Pg.1215]    [Pg.1744]    [Pg.2111]    [Pg.2271]    [Pg.2547]    [Pg.329]    [Pg.451]    [Pg.233]    [Pg.456]    [Pg.43]    [Pg.70]    [Pg.174]    [Pg.84]    [Pg.276]    [Pg.104]    [Pg.105]    [Pg.110]    [Pg.239]    [Pg.341]    [Pg.537]    [Pg.63]    [Pg.64]    [Pg.225]    [Pg.283]    [Pg.362]    [Pg.284]    [Pg.301]    [Pg.352]    [Pg.871]    [Pg.317]    [Pg.233]    [Pg.334]   
See also in sourсe #XX -- [ Pg.61 , Pg.433 ]




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Adsorption liquid-like

Amorphous liquid-like structure

Atomic environments liquid-like

Biocatalysts Based on Covalently Supported Ionic Liquid-Like Phases (SILLPs)

Correlations liquid-like

Crown liquid-like

Disordered systems liquid-like behavior

Ferroelectric crystals liquid-like behavior

How Do Correction Fluids like Liquid Paper and White-Out Work

Liquid crystals banana-like

Liquid crystals of disc-like molecules

Liquid crystals of rod-like molecules

Liquid-crystal-like superstructure

Liquid-like amorphous component

Liquid-like behavior

Liquid-like behaviour

Liquid-like clusters

Liquid-like clusters free energy

Liquid-like clusters model

Liquid-like complexes

Liquid-like domain

Liquid-like mobility

Liquid-like motion

Liquid-like order

Liquid-like pair correlation function

Liquid-like particles

Liquid-like phase

Liquid-like properties

Liquid-like rheology

Liquid-like root

Liquid-like state

Liquid-like viscous mechanism

Liquids solid-like models

Lodge rubber like liquids

Oligomers, liquid-like

Phase Transitions in Rod-Like Liquid Crystals

Phase structure liquid-like

Photooxidation in Solution and Liquid-like Surfaces of Organic Aerosols

Physical adsorption liquid like

Polyethylene liquid-like amorphous phase

Rod-Like Liquid Crystals Combining RH- and RF-Chains Monolayer Smectic Phases

Rod-Like Liquid Crystals with Fluorinated Chains

Rod-Like Liquid Crystals with Two Fluorinated Chains at Opposite Ends Layer Frustration

Rod-like liquid crystals

Rubber-like liquid

Star-like liquid crystals

Supercritical fluid liquid-like density

The Surface of Liquid Water Behaves Like an Elastic Film

Water liquid-like

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