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Density material property

Physical or material properties density p, diffusivity D and kinematic viscosity v The corresponding dimensional matrix can be written as... [Pg.184]

As mentioned earlier, necessary for the description of the fluid flow is the knowledge of the material properties density and viscosity. Thus for the complex rheology of the ceramic material additionally the preparatory work of designation of the parameters rjB and To (7) is required. If in addition the formation of phase separation at the wall by a wall slip boundary condition is to be included, the rheological measurement of the parameters Ts and k is indispensable. [Pg.412]

Material properties (density, viscosity, consistence, fluidity, interfadal tension in liquids with fluid particles)... [Pg.156]

Measuring devices measure with the help of sensors in several parts of the plant material properties (density, viscosity, composition etc.) or process parameters (pressure, temperature, flow, level, number of revolutions, valve positions etc.). [Pg.207]

Material properties Density q, specific heat capacity Cp corresponding to the specific enthalpy h of the material and latent energies like melting Ah, condensation Aha and evaporation Ahy. [Pg.21]

Material properties Density (ASTM C 642), moisture content (ASTM C 642), shrinkage (ASTM C 596, C 426), dynamic modulus (ASTM C 215), modulus of elasticity (ASTM C 464)... [Pg.182]

Flow distribution and pressure losses for any arrangement of fuel plates and cooling gaps are determined by iterative hydraulic calculation. Using total mass flow and channel dimensions, the local pressure is determined to calculate local saturation temperature as a criterion for the onset of boiling. Hydraulic calculations are linked to the heat transfer module. To take into account the variation of material properties (density, viscosity, conductivity, and heat capacity) with the local pressure and temperature, the hydraulic and heat transfer modules are linked through outer iteration. [Pg.8]

Elstner M, Porezag D, Jungnickel G, Eisner J, Flaugk M, Frauenheim Th, Suhai S and Seifert G 1998 Self-consistent-charge density-functional tight-binding method for simulations of complex materials properties Phys. Rev. B 58 7260... [Pg.2229]

Material properties can be further classified into fundamental properties and derived properties. Fundamental properties are a direct consequence of the molecular structure, such as van der Waals volume, cohesive energy, and heat capacity. Derived properties are not readily identified with a certain aspect of molecular structure. Glass transition temperature, density, solubility, and bulk modulus would be considered derived properties. The way in which fundamental properties are obtained from a simulation is often readily apparent. The way in which derived properties are computed is often an empirically determined combination of fundamental properties. Such empirical methods can give more erratic results, reliable for one class of compounds but not for another. [Pg.311]

The insulating properties of polyethylene compare favourably with those of any other dielectric material. As it is a non-polar material, properties such as power factor and dielectric constant are almost independent of temperature and frequency. Dielectric constant is linearly dependent on density and a reduction of density on heating leads to a small reduction in dielectric constant. Some typical data are given in Table 10.6. [Pg.226]

Throne has reported that the relationship between foam modulus and density can be generalised to other properties such as tensile strength, fatigue strength, creep properties as well as shear and compression modulus. Thus if X is the general material property then... [Pg.68]

Luft and Tsuo have presented a qualitative summary of the effects of various plasma parameters on the properties of the deposited a-Si H [6]. These generalized trends are very useful in designing deposition systems. It should be borne in mind, however, that for each individual deposition system the optimum conditions for obtaining device quality material have to be determined by empirical fine tuning. The most important external controls that are available for tuning the deposition processs are the power (or power density), the total pressure, the gas flow(s), and the substrate temperature. In the following the effects of each parameter on material properties will be discussed. [Pg.108]

Summarizing the results, it is clear that most of the material properties are not strongly dependent on frequency in the range of 30 to 80 MHz. The effect of power density is much more important. The material deposited at the lowest power... [Pg.143]

Other material properties that are of general interest to the polymer chemist are shown in Table 3. Linear toluene swell is indicative of cross-link density in the material. The vinyl-phenyl modified rubber showed the lowest degree of swell. This is due to additional cross-links introduced by the vinyl groups during synthesis. The unmodified rubber was found to swell considerably in toluene and was found to dissolve partially in the solvent. [Pg.107]

Gelatine explosives, initiated by commercial detonators, will normally fire at the low velocity of detonation initially, although this may well build up quite quickly into the high velocity. For some applications a high velocity of detonation is essential. This can be ensured by the addition of barium sulphate, or other material with density exceeding 2-8, in a fine form. Such additives have the property of ensuring rapid transition to the high velocity of detonation. This is, for example, of particular importance when the explosive is to be fired under a hydrostatic head, as in submarine work. [Pg.53]

In order to enable these fluctuations to occur, the network chains are assumed to be "phantom" in nature i.e. their material properties are dismissed and they act only to exert forces on the junctions to which they are attached. With common networks having tetrafunctional junctions, the results of the two approaches differ by a factor of two. Identical results are only obtained from both theories, when the functionality is infinite. From a practical viewpoint, however, a value of about 20 for f can already be equated to infinity because crosslink densities can hardly be obtained with an accuracy better than 10%. [Pg.310]


See other pages where Density material property is mentioned: [Pg.365]    [Pg.370]    [Pg.461]    [Pg.192]    [Pg.456]    [Pg.361]    [Pg.365]    [Pg.370]    [Pg.461]    [Pg.192]    [Pg.456]    [Pg.361]    [Pg.315]    [Pg.328]    [Pg.2]    [Pg.231]    [Pg.119]    [Pg.435]    [Pg.8]    [Pg.311]    [Pg.27]    [Pg.616]    [Pg.148]    [Pg.446]    [Pg.180]    [Pg.54]    [Pg.3]    [Pg.863]    [Pg.141]    [Pg.128]    [Pg.175]    [Pg.58]    [Pg.164]    [Pg.372]    [Pg.119]    [Pg.133]    [Pg.282]    [Pg.307]    [Pg.198]    [Pg.388]   
See also in sourсe #XX -- [ Pg.18 ]

See also in sourсe #XX -- [ Pg.504 , Pg.506 ]




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Material densities

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