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Material phase

Revised material for Section 5 includes the material on surface tension, viscosity, dielectric constant, and dipole moment for organic compounds. In order to include more data at several temperatures, the material has been divided into two separate tables. Material on surface tension and viscosity constitute the first table with 715 entries included is the temperature range of the liquid phase. Material on dielectric constant and dipole... [Pg.1283]

Ferroelectric Ceramic—Polymer Composites. The motivation for the development of composite ferroelectric materials arose from the need for a combination of desirable properties that often caimot be obtained in single-phase materials. For example, in an electromechanical transducer, the piezoelectric sensitivity might be maximized and the density minimized to obtain a good acoustic matching with water, and the transducer made mechanically flexible to conform to a curved surface (see COMPOSITE MATERIALS, CERAMiC-MATRix). [Pg.206]

Phase Materials. Phase holograms can be recorded in a large variety of materials, the most popular of which are dichromated gelatin, photopolymers, thermoplastic materials, and photorefractive crystals. Dichromated gelatin and some photopolymers require wet processing, and thermoplastic materials require heat processing. Photorefractive crystals are unique in that they are considered to be real-time materials and require no after-exposure processing. [Pg.160]

In many of the thin coatings on cemented carbide, either single or multiple coatings of single phase materials, such as TiC, are used. It would appear that extending the use of soHd solutions of multicarbides of W, Ti, and Ta or Nb for coatings may further enhance the performance of the coated carbides. It would not be difficult to accomplish this either by CVD or PVD techniques. [Pg.221]

IP, isolated pure MI, matrix isolated GP, data from pure gas phase material CE, chemical evidence for existence TH, theoretical calculation XR, X-ray structure MW, microwave structure UV ultraviolet spectrum. [Pg.3]

A pure gas A diffuses into a liquid film where it reacts with B from the liquid phase. Material balances on the two participants are ... [Pg.2108]

Shock-recovery experiments by Gray [10] were conducted to assess directly if the strain-path reversal inherent to the shock contains a traditional microstructurally controlled Bauschinger effect for a shock-loaded two-phase material. Two samples of a polycrystalline Al-4 wt.% Cu alloy were shock loaded to 5.0 GPa and soft recovered in the same shock assembly to assure identical shock-loading conditions. The samples had two microstructural... [Pg.206]

This reaction is carried out in tall fluidized beds of high L/dt ratio. Pressures up to 200 kPa are used at temperatures around 300°C. The copper catalyst is deposited onto the surface of the silicon metal particles. The product is a vapor-phase material and the particulate silicon is gradually consumed. As the particle diameter decreases the minimum fluidization velocity decreases also. While the linear velocity decreases, the mass velocity of the fluid increases with conversion. Therefore, the leftover small particles with the copper catalyst and some debris leave the reactor at the top exit. [Pg.183]

Condensation is the result of collisions between a gaseous molecule and an existing aerosol droplet when supersaturation exists. Condensation occurs at much lower values of supersaturation than nucleation. Thus, when particles already exist in sufficient quantities, condensation will be the dominant process occurring to relieve the supersaturated condition of the vapor-phase material. [Pg.145]

The conventionally covalently cross-linked rubbers and plastics cannot dissolve without chemical change. They will, however, swell in solvents of similar solubility parameter, the degree of swelling decreasing with increase in cross-link density. The solution properties of the thermoelastomers which are two-phase materials are much more complex, depending on whether or not the rubber phase and the resin domains are dissolved by the solvent. [Pg.87]

Following the success in blending rubbery materials into polystyrene, styrene-acrylonitrile and PVC materials to produce tough thermoplastics the concept has been used to produce high-impact PMMA-type moulding compounds. These are two-phase materials in which the glassy phase consists of poly(methyl methacrylate) and the rubbery phase an acrylate polymer, usually poly(butyl acrylate Commercial materials of the type include Diakon MX (ICI), Oroglas... [Pg.413]

There is also growing interest in multi-phase systems in which hard phase materials are dispersed in softer polyether diols. Such hard phase materials include polyureas, rigid polyurethanes and urea melamine formaldehyde condensates. Some of these materials yield high-resilience foams with load deflection characteristics claimed to be more satisfactory for cushioning as well as in some cases improving heat resistance and flame retardancy. [Pg.808]

What was recognised from the beginning was that colloidal solutions are two-phase materials. [Pg.42]

Figure 10,2.. Schematic of the microstructure of a nanostructured single-phase material (after... Figure 10,2.. Schematic of the microstructure of a nanostructured single-phase material (after...
Alhedai et al also examined the exclusion properties of a reversed phase material The stationary phase chosen was a Cg hydrocarbon bonded to the silica, and the mobile phase chosen was 2-octane. As the solutes, solvent and stationary phase were all dispersive (hydrophobic in character) and both the stationary phase and the mobile phase contained Cg interacting moieties, the solute would experience the same interactions in both phases. Thus, any differential retention would be solely due to exclusion and not due to molecular interactions. This could be confirmed by carrying out the experiments at two different temperatures. If any interactive mechanism was present that caused retention, then different retention volumes would be obtained for the same solute at different temperatures. Solutes ranging from n-hexane to n hexatriacontane were chromatographed at 30°C and 50°C respectively. The results obtained are shown in Figure 8. [Pg.42]

The first attempts employing two Cjg columns showed that the selectivity was not high enough, although this improved when the first column was substituted by a 5 p.m GFF n internal surface rcversed-phase material. This is known as a restricted-access-material (RAM) column which, since it restricts some compounds because of their size and includes rcversed-phase interaction and ionic exchange, is very useful for analysing herbicides in samples with high contents of humic and fulvic acids (54). [Pg.353]

Indeed, the self-consistent model averages the stresses and strains in either phase of a two-phase material, and it determines them, by solving separate problems, whose superposition yields the final configuration of the model 7). [Pg.174]

The ionic or polar substances can be seperated without any reaction on specially treated chromatographic columns and detected refractometrically. This is necessary because alkyl sulfosuccinates show only small absorption in the UV-visible region no sensitive photometric detection can be obtained. Separation problems can arise when common steel columns filled with reverse phase material (or sometimes silica gel) are used. This problem can be solved by adding a suitable counterion (e.g., tetrabutylammonium) to the mobile phase ( ion pair chromatography ). This way it is possible to get good separation performance. For an explanation of separation mechanism see Ref. 65-67. A broad review of the whole method and its possibilities in use is given in an excellent monograph [68]. [Pg.516]

There is currently considerable interest in processing polymeric composite materials filled with nanosized rigid particles. This class of material called "nanocomposites" describes two-phase materials where one of the phases has at least one dimension lower than 100 nm [13]. Because the building blocks of nanocomposites are of nanoscale, they have an enormous interface area. Due to this there are a lot of interfaces between two intermixed phases compared to usual microcomposites. In addition to this, the mean distance between the particles is also smaller due to their small size which favors filler-filler interactions [14]. Nanomaterials not only include metallic, bimetallic and metal oxide but also polymeric nanoparticles as well as advanced materials like carbon nanotubes and dendrimers. However considering environmetal hazards, research has been focused on various means which form the basis of green nanotechnology. [Pg.119]

The horizontal portion of the plot in Figure 23.6 represents the equilibrium mass uptake—the amount absorbed at equilibrium whose magnitude is influenced by the solubility parameter 8 (Section 23.4.3.1). In reality, coefficient D quite often varies with concentration, so that the overall plot takes on a sigmoid shape (see Section 23.4.4.3), although a horizontal portion is still usually achieved eventually if it is not, the elastomer is possibly a two-phase material (a blend), with one phase much slower at absorbing the incoming liquid. [Pg.640]

Sixteen solid-phase materials were tested on a laboratory scale and the antho-cyanin and sugar content of collected fractions were determined. Among these, reverse-phase silica gels and macroreticular non-ionic acrylic polymer adsorbents such as Serdolit PAD IV or Amberlite XAD-7 turned out to be most suitable. SPE was used to investigate these materials on an enlarged scale, improving elution gradient and column purification. Amberlite XAD-7 was successfully applied in a middle-scale separation. ... [Pg.313]


See other pages where Material phase is mentioned: [Pg.451]    [Pg.159]    [Pg.196]    [Pg.474]    [Pg.222]    [Pg.545]    [Pg.558]    [Pg.1665]    [Pg.1689]    [Pg.2152]    [Pg.2167]    [Pg.2382]    [Pg.55]    [Pg.206]    [Pg.448]    [Pg.314]    [Pg.202]    [Pg.175]    [Pg.102]    [Pg.94]    [Pg.654]    [Pg.136]    [Pg.517]    [Pg.517]    [Pg.3]    [Pg.402]    [Pg.142]    [Pg.314]    [Pg.380]   
See also in sourсe #XX -- [ Pg.18 ]

See also in sourсe #XX -- [ Pg.147 , Pg.156 , Pg.189 , Pg.191 ]




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Ab Initio Molecular-Dynamics Simulations of Doped Phase-Change Materials

Assessment Phase Material Balance Calculations

Assumptions for stacking of material phases in fiber direction

Basics in Phase Morphologies of Multicomponent Polymer-Based Materials

Binary-phase materials

Block copolymers phase-separated materials

Bonded phase Base materials

Bonded phase materials

Bonded stationary phases silica, base material

CMP for phase change materials

Catalytic phase material

Chiral nematic phase materials forming

Composite materials phases

Considerations for Phase 2 Material and Beyond

Design of Well-Defined Active Sites on Crystalline Materials for Liquid-Phase Oxidations

Electronic materials—phase diagram and crystal growth of GaAs

Emulsion phase material balances

Encapsulated phase change material

Encapsulation Shells for Phase Change Materials

Encapsulation phase change material

Functional Properties of Phase Change Materials from Atomistic Simulations

General assumptions for the stacking of material phases

Granular material, phases

High-performance liquid chromatography reversed-phase materials

Inorganic phase change materials

Liquid crystal materials lyotropic nematic phases

Liquid crystal materials nematic phases

Liquid crystal materials other lyotropic phases

Liquid crystal materials smectic phases

Liquid phase sintering of refractory materials

Material characteristics phases

Material characterization methods quantitative phase analysis

Membrane material selection inorganic phase

Membrane material selection polymer phase

Metal containing materials, cubic phases

Microcapsules phase change materials

Mobile phase material balance equation

Multicomponent polymer materials, phase

Normal-phase HPLC material after

Organic Polymer-based Stationary Phase Materials

Organic Stationary Phase Materials

Other Stationary Phase Materials

Phase Change Materials (PCMs)

Phase Change Materials and Their Basic Properties

Phase change materials

Phase change materials characteristics

Phase change materials chemical properties

Phase change materials classification

Phase change materials coating methods

Phase change materials micro-encapsulation

Phase change materials nano-encapsulation

Phase change materials nanoparticle-enhancement

Phase change materials organic

Phase change materials paraffin-based

Phase change materials physical properties

Phase change materials salt hydrate

Phase change materials textile applications

Phase change materials thermal properties

Phase changing materials

Phase diagram materials microstructure

Phase stability, nanostructured materials

Phase-transition calibration materials

Phases, of materials

Preparation, Testing, and Selectivity of Stationary Phase Materials

Protective clothing phase change materials

Pure Phase Encode Magnetic Resonance Imaging of Concrete Building Materials

Retention silica-based reversed-phase materials

Retention time reversed-phase materials

Reversed-phase HPLC materials

Reversed-phase Materials

Reversed-phase packing materials, silica-based

Selectivity of Stationary Phase Materials

Shape memory polymers phase change materials

Silica Gel-based Stationary Phase Materials

Silica-based Reversed-phase Materials

Single-phase polymer materials

Soft materials phases

Sohd-liquid phase change materials

Solid Core versus Fully Porous Phase Materials

Solid-liquid phase change materials

Solid-phase materials

Solid-phase separation materials for

Stacking of material phases in the axial directions

Stacking of material phases with respect to normal modes

Stacking of material phases with respect to shear modes

Stationary phase material balance

Stationary phases materials

Stationary phases phase materials

Synthesis of bonded phase materials

The Prototype Phase Change Material Ge2Sb2Te5 Amorphous Structure and Crystallization

Thermoregulating phase change materials

Two-phase material

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