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Surface Melting

In the case of a pure crystalline substance, this change occurs at constant temperature. The normal freezing point is the temperature at which the solid and liquid are in equilibrium at 1 atm (760 torr, or 101.3 kPa) pressure. [Pg.328]

Melting, the reverse of freezing, also occurs at constant temperature. As a solid melts, it continuously absorbs energy as heat, as represented by the following equation. [Pg.328]

For pure crystalline solids, the melting point and freezing point are the same. At equilibrium, melting and freezing proceed at equal rates. The following general equilibrium equation can be used to represent these states. [Pg.328]

At normal atmospheric pressure, the temperature of a system containing ice and liquid water wiU remain at 0.°C as long as both ice and water are present, no matter what the surrounding temperature. Adding energy in the form of heat to such a system shifts the equilibrium to the right. That shift increases the proportion of liquid water and decreases that of ice. Only after aU the ice has melted will the addition of energy increase the temperature of the system. [Pg.328]

At sufficiently low temperature and pressure conditions, a liquid caimot exist. Under such conditions, a solid substance exists in equilibrium with its vapor instead of its liquid, as represented by the following equation. [Pg.328]


Kofman R ef a/1989 Solid-liquid transition of metallic clusters occurrence of surface melting Physica A 157 631 Kofman R ef al 1994 Surface melting enhanced by curvature effects Surf. Sc/. 303 231... [Pg.2923]

Wang Z L ef a/1998 Shape transformations and surface melting of cubic and tetrahedral platinum nanocrystals J. Phys. Chem. B 102 6145... [Pg.2923]

In bulk coating processes, bulk materials are joined to the substrate either by a surface melt process or by attachment of the soHd material. An example of the latter is the appHcation of heat-resistant tiles of sHica-type material to the aluminum alloy skin of a space shuttle vehicle, enabling the vehicle to withstand the reentry heat. [Pg.46]

Pontikis, V. (1993) Crystal surfaces melting and roughening, in Supplementary Volume 3 of the Encyclopedia of Materials Science and Engineering, ed. Cahn, R.W. (Pergamon press, Oxford), p. 1587. [Pg.421]

More recently, simulation studies focused on surface melting [198] and on the molecular-scale growth kinetics and its anisotropy at ice-water interfaces [199-204]. Essmann and Geiger [202] compared the simulated structure of vapor-deposited amorphous ice with neutron scattering data and found that the simulated structure is between the structures of high and low density amorphous ice. Nada and Furukawa [204] observed different growth mechanisms for different surfaces, namely layer-by-layer growth kinetics for the basal face and what the authors call a collected-molecule process for the prismatic system. [Pg.376]

J. P. van der Eerden, A. Roos, J. M. van der Veer. Surface roughening versus surface melting on Lennard-Jones crystal surfaces. J Cryst Growth 99 11, 1990. [Pg.917]

Y. Furukawa, H. Nada. Anisotropic surface melting of an ice crystal and its relationship to growth forms. J Phys Chem B 707 6167, 1997. [Pg.924]

At the same time, many lattice dynamics models have been constructed from force-constant models or ab-initio methods. Recently, the technique of molecular dynamics (MD) simulation has been widely used" " to study vibrations, surface melting, roughening and disordering. In particular, it has been demonstrated " " " that the presence of adatoms modifies drastically the vibrational properties of surfaces. Lately, the dynamical properties of Cu adatoms on Cu(lOO) " and Cu(lll) faces have been calculated using MD simulations and a many-body potential based on the tight-binding (TB) second-moment aproximation (SMA). " ... [Pg.151]

T.L. Boggs et al, AIAA J 8 (2), 370-72 (1970) CA 72, 113371 (1970) Scanning electron microscopy is used to study the surface structure of solid proplnts, prepd from AP (1) and polyurethane or caiboxylated polybutadiene. Polyurethane proplnts are self-extinguish-ing at high pressure due to the flow of molten binder over I crystals. I crystals formed a thin surface melt with gas liberation in the molten phase... [Pg.947]

CSMP [Cupola surface melting process] A process for vitrifying residues from the incineration of municipal wastes. Offered by ML Entsoigungs und Eneigieanlagen. [Pg.75]

Unlike supercooling of liquids, superheating of crystalline solids is difficult due to nucleation of the liquid at surfaces. However, by suppressing surface melting, superheating to temperatures well above the equilibrium melting temperature has... [Pg.129]

Finally, if the temperature increases, becomes larger until the crystal melts. The Lindemann criterion predicts that melting sets in when becomes about 0.25 a2, where a is the interatomic distance of the metal. Because the mean squared displacements of surface atoms is higher we expect that the surface melts at lower temperatures than the bulk does [2]. Indeed, evidence has been presented that the (110) surface of lead starts to melt at 560 K whereas the bulk melting temperature is about 600 K [13]. [Pg.299]

Disordering on surfaces Layers on materials Vapour deposition, laser surface melting, ion beam modification... [Pg.51]

Disclosed is a crossUnked ethylenic polymer foam structure of an ethylenic polymer material of a crosslinked, substantially linear ethylenic polymer. The ethylenic polymer in an uncrossUnked state has (a) a melt flow ratio greater than or equal to 5.63 (b) a molecular weight distribution defined by a given equation and (c) a critical shear rate at onset of surface melt fracture of at least 50% greater than the critical shear rate at the onset of surface melt fracture of a linear ethylenic polymer having about the same melt flow ratio and molecular weight distribution. Further disclosed is a process for making the above foam structure. [Pg.94]

The polymer material contains a linear ethylenic polymer having a melt flow ratio, 11012, of 5.63 or above, a MWD, Mw/Mn, defined by the equation Mw/Mn less than or equal to (I10/I2)-4.63 and a critical shear rate at onset of surface melt fracture of at least 50% greater than that of a linear olefin polymer having about the same 12 and Mw/ Mn. The foam structures have toughness and elasticity similar to those formed from conventional LLDPE without the poor dimensional stability and foam quality associated with those structures and foam quality similar... [Pg.99]

The polymer is a linear ethylenic polymer having a melt flow rate of 5.63, a specified MWD and a critical shear rate at onset of surface melt fracture of at least 50% greater than that at the onset of surface melt fracture of a linear... [Pg.99]

The ethylenic polymer has, in the uncrosslinked state, specified melt flow ratio, MWD and critical shear rate at the onset of surface melt fracture. [Pg.103]

The stability of the Au, cluster compound is of course supplied at least in part by the ligand shell, and this complicates a direct comparison of the above theoretical predictions for imaginary bare Au,. But experimentally, the presence of an MES spectrum consisting of a superposition of distinct lines of the natural linewidth for gold from four different structural sites also constitutes proof that gold core of the Au, cluster is, at least on the time scale of the MES measurements (i.e. 0.1 ps < t < 10 ps) [112,113], a solid up to temperatures of at least 30 K. Surface melting on this time scale can also be refuted for Au, for the same reason. The same has also been observed by MES on the water soluble compound Au, [46],... [Pg.13]

These contact angles can be related to the physical state of the surface. The 100 facet is better wetted than the 111 one because the 100 surface is partly premelted. But, the liquid-like disordered monolayer is too thin to have the properties of the macroscopic liquid, and this "adsorbed liquid layer" coexists with a non-wetting macroscopic liquid. This so-called "incomplete surface melting" has also been observed on a pure single crystal of ice. ... [Pg.55]

M. Elbaum, S.G. Lipson and J.G. Dash, Optical Study of Surface Melting on Ice, J. Crystal Growth,... [Pg.58]

J.C. Heyraud, J.J. Metois and J.M. Bermond, Surface Melting and Equilibrium Shape the Case ofPb on... [Pg.58]

A. Pavlovska, K. Faulianand E. Bauer, Surface Roughening and Surface Melting in the High Temperature... [Pg.58]

An interesting result of this effect occurs for falling ice spheres. When the surface melts, and therefore becomes smooth, flow can pass from supercritical to subcritical and the terminal velocity is suddenly reduced (W6). [Pg.245]

The sorbitol solution produced from hydrogenation is purified in two steps [4]. The first involves passing the solution through an ion-exchange resin bed to remove gluconate and other ions. In the second step, the solution is treated with activated carbon to remove trace organic impurities. The commercial 70% sorbitol solution is obtained by evaporation of the water under vacuum. The solid is prepared by dehydration until a water-free melt is obtained which is cooled and seeded. The crystals are removed continuously from the surface (melt crystallization). The solid is sold as flakes, granules, pellet, and powder forms in a variety of particle size distributions. [Pg.465]

Binh, V. T., and Garcia, N. (1991). Atomic metallic ion emission, field surface melting, and scanning tunneling microscopy tips. J. Phys. I. 1, 605-612. [Pg.385]


See other pages where Surface Melting is mentioned: [Pg.270]    [Pg.271]    [Pg.281]    [Pg.2913]    [Pg.344]    [Pg.336]    [Pg.147]    [Pg.46]    [Pg.249]    [Pg.149]    [Pg.938]    [Pg.938]    [Pg.273]    [Pg.282]    [Pg.215]    [Pg.350]    [Pg.99]    [Pg.320]    [Pg.41]    [Pg.55]    [Pg.58]    [Pg.58]   
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Adsorption behavior, solid surface polymer melts

Affective interactions, solid surface polymer melts

Bulk polymers, solid surface melts, properties

Crystalline polymers surface melting

Free melt surface

Laser surface melting

Laser surface melting schematic

Melt agglomeration surface plasticity

Melt glass surface area

Melting temperature, nanoparticles surfaces

Melting temperature, nanoparticles surfaces relating

Melts, surface-induced phases

Molecular models, solid surface polymer melts

Nucleation and Surface Melting of Ice

Oxide melts surface tension

Polymer melt surface

Polymer melt surface density profile

Polymer melt surface roughness

Polymers melts at solid surfaces

Reversing, table surface melting

Solid surface polymer melts chain conformations

Solid surface polymer melts polymeric liquids

Solid surface polymer melts simple liquids

Solid surface polymer melts systems

Surface Crystallization and Melting

Surface Forces in Polymer Solutions and Melts

Surface energy of liquids and melts

Surface melt glass

Surface melting tension energy

Surface phenomena melting

Surface silicate melts

Surface-Induced Phases in Melts

Surface-melted phase

The surface of a simple polymer melt

Thermal surface melting

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