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Energetics, surface

For a flat fcc(001) siuface as standard, Zi = 4, Z2 = 5.73, and z, 3 = 12, and correspondingly, the bond contraction coefficient of Ci = 0.88, C2 = 0.92, and C, 3 = 1. Table 16.2 lists the effective CNs for other surfaces. For metals such as Au, Ag, and Cu, m = 1 for carbon, m — 2.56 and for Si, m — 4.88. For other alloys and compounds, the m may vary. Averaging the sum over the top two atomic layers, one can obtain the mean energy density per unit area within the two atomic layers and the mean energy remain per discrete atom in the top two atomic layers at T 0 K. With the given bond energy for Cu (4.39 eV/atom), Diamond [Pg.322]


Heterogeneous Ideal Adsorbed S olution TheoTy (HIAST). This IAS theory has been extended to the case of adsorbent surface energetic heterogeneity and is shown to provide improved predictions over lAST (12). [Pg.274]

Given the importance of surface and interfacial energies in determining the interfacial adhesion between materials, and the unreliability of the contact angle methods to predict the surface energetics of solids, it has become necessary to develop a new class of theoretical and experimental tools to measure the surface and interfacial energetics of solids. Thia new class of methods is based on the recent developments in the theories of contact mechanics, particularly the JKR theory. [Pg.99]

Various workers have used these equations extensively to understand the surface energetics of polymeric solids. [Pg.518]

About 51 percent of solar energy incident at the top of the atmosphere reaches Earth s surface. Energetic solar ultraviolet radiation affects the chemistry of the atmosphere, especially the stratosphere where, through a series of photochemical reactions, it is responsible for the creation of ozone (O,). Ozone in the stratosphere absorbs most of the short-wave solar ultraviolet (UV) radiation, and some long-wave infrared radiation. Water vapor and carbon dioxide in the troposphere also absorb infrared radiation. [Pg.86]

For example, the increment in maximum stress over the neat polymer is 100% and 53% in the case of the unmodified- and the modified-clay-fiUed samples, respectively. The extraordinary results obtained with the unmodified clays were explained with the help of thermodynamics and surface energetics. They explained it as follows. [Pg.39]

Surface energetics and thermodynamic driving force thus define the energy barrier for nucleation as shown in Fig. 2.13b. For heterogeneous nucleation,... [Pg.63]

In fact, it has been previously observed that measured diameters of dendrimer molecules by AFM are much larger than the theoretical values, which indicates that the dendrimers spread out and flatten on the surface [25, 26], Three major factors could account for this deformation. First, the unique architecture and chemical structure of PAMAM dendrimers result in macromolecules that are not solid balls, but instead are relatively open and hence soft materials. It is expected that the rigidity will increase substantially with increasing generation number [9]. Therefore, when deposited on solid substrates, they tend to deform to different degrees as a result of the interplay between their inherent rigidity and surface energetics from the interaction between the dendrimer molecules and the mica surface. Secondly, amine-terminated PAMAM dendrimers possess a... [Pg.300]

While direct, this method is the most difficult experimentally due to the diminutive nature of fiber diameters and the uncertainty involved with contact angle measurements and hysteresis. The value i ) can also be measured on flat sheets of the fiber material but due to fabric finishes and different surface properties incurred during manufacture, the surface energetics of the sheet and fiber may be very dissimilar. Therefore, the value of co8i i was determined in the following manner from detergency data. The Kubelka-Munk Equation (12-13),... [Pg.248]

The characteristics of particulate filled polymers are determined by the properties of their components, composition, structure and interactions [2]. These four factors are equally important and their effects are interconnected. The specific surface area of the filler, for example, determines the size of the contact surface between the filler and the polymer, thus the amount of the interphase formed. Surface energetics influence structure, and also the effect of composition on properties, as well as the mode of deformation. A relevant discussion of adhesion and interaction in particulate filled polymers cannot be carried out without defining the role of all factors which influence the properties of the composite and the interrelation among them. [Pg.112]

Although a number of filler characteristics influence composite properties, particle size, specific surface area, and surface energetics must again be mentioned here. All three also influence interfacial interactions. In the case of large particles and weak adhesion, the separation of the matrix/ filler interface is easy, debonding takes place under the effect of a small external load. Small particles form aggregates which cause a deterioration in the mechanical properties of the composites. Specific surface area, which depends on the particle size distribution of the filler, determines the size of the contact surface between the polymer and the filler. The size of this surface plays a crucial role in interfacial interactions and the formation of the interphase. [Pg.116]

The difference between IGC and conventional analytical gas-solid chromatography is the adsorption of a known adsorptive mobile phase (vapour) on an unknown adsorbent stationary phase (solid state sample). Depending on experiment setup, IGC can be used at finite or infinite dilution concentrations of the adsorptive mobile phase. The latter method is excellent for the determination of surface energetics and heat of sorption of particulate materials [3]. With IGC at finite dilution, it is possible to measure sorption isotherms for the determination of surface area and porosity [4], The benefits of using dynamic techniques are faster equilibrium times at ambient temperatures. [Pg.633]

The interphase is the volume of material in which the properties of one substance gradually change into the propeities of another. The intetphase is useful for describing the properties of an adhesive bond. The interface, contained within the interphase, is the plane of contact between the surface of one material and the surface of another. F.xcepl in certain special cases, the interface is imaginary. It is useful in describing surface energetics. [Pg.32]

Surface Energetics and Wettability Theory. The surface energetics and wettability theory of adhesion is concerned with the effect of intermolecular and interatomic forces on the surface energies of the adhesive and the adherend and the interfacial energy between the two. [Pg.32]

PVF films may alter the electrochemical response of semiconductor electrodes in useful ways. For example, for potentials more positive than —0.8 V (SCE) only reductions are possible with single crystal or polycrystalline Ti02 in contact with a ferrocene solution (acetonitrile). However, with plasma coated with PVF, ferrocene sites are oxidized in a potential region where n-Ti02 is considered blocked to electron transfer.70 Here two factors are involved obviously the coating of the electrode with an electroactive species, but also alteration of the surface energetics of the semiconductor. [Pg.21]

Mechanical activity at the surface such as load, speed, and variations in surface energetics, play a role in surface chemistry. For example, if a clean metal surface is exposed to materials such as oxygen, chlorine, and sulfur, an interaction goes on. There is no activation energy necessary to achieve the reaction of the species with the metal surface to form surface compounds. [Pg.177]

Kaltenecker-Commercon JM,Ward TC (1993) Water resistance of poly(imide siloxane) adhesives an IGC surface energetics study. J Adhes 42 1,113... [Pg.103]

Grimsey IM, et al. 1999. Interpretation of the differences in the surface energetics of two optical forms of mannitol by inverse gas chromatography and molecular modelling. Int. J. Pharm. 191 43-50. [Pg.325]

The surface energetics that control wetting are largely related to the general chemical composition of the epoxy polymer molecule. However, the surface tension of an epoxy... [Pg.50]

Solvents can also be used to reduce the surface tension of the adhesive formulation. The surface tensions of common solvents are shown in Table 3.5. Of course, when using solvents, one needs to make sure that they evaporate from the bond line before cure. Solvent solutions do not change the equilibrium surface energetics of the system. They only provide lower viscosity so that wetting is established at a faster rate. [Pg.57]

Schonhorn, H., and Sharpe, L., Surface Energetics, Adhesion, and Adhesive Joints II, Journal of Polymer Science PartB Polymer Letters, vol. 2, no. 7, 1964, p. 719. [Pg.110]


See other pages where Energetics, surface is mentioned: [Pg.953]    [Pg.229]    [Pg.287]    [Pg.42]    [Pg.100]    [Pg.350]    [Pg.34]    [Pg.35]    [Pg.96]    [Pg.104]    [Pg.112]    [Pg.143]    [Pg.154]    [Pg.540]    [Pg.226]    [Pg.245]    [Pg.207]    [Pg.23]    [Pg.251]    [Pg.100]    [Pg.159]    [Pg.323]    [Pg.1435]    [Pg.380]    [Pg.255]    [Pg.165]    [Pg.105]    [Pg.151]   
See also in sourсe #XX -- [ Pg.9 ]

See also in sourсe #XX -- [ Pg.18 ]

See also in sourсe #XX -- [ Pg.31 ]




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