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Material mass density

Stability requirements for the existence of these alternative conformational states at Tg allowed us also to estimate the strength of their coupling to the regular lattice vibrations, which is determined by Tg, the material mass density, and the speed of sound. This enabled us to understand the universality of the phonon scattering at the low temperatures. [Pg.193]

Material Mass Density Osglw ) Specific Weight (kN/m )... [Pg.507]

Density of ambient air, mass/voliime p.3 Initial density of released material, mass/voliime... [Pg.2340]

When trying to understand and to manipulate matter and materials, chemistry does not start by looking at the natural world in all its complexity. Rather, it seeks to establish what have been termed exemplar phenomena ideal or simplified examples that are capable of investigation with the tools available at the time (Gilbert, Borrlter, Elmer, 2000). This level consists of representatiorrs of the empirical properties of solids, liquids (taken to include solutions, especially aqueous solutiorts), colloids, gases and aerosols. These properties are perceptible in chemistry laboratories and in everyday life and are therefore able to be meastrred. Examples of such properties are mass, density, concentration, pH, temperatrrre and osmotic presstrre. [Pg.5]

Electron Density. Continuing the preceding considerations, calibration to absolute intensity means normalization to the scattering of a single electron , Ie that can be expressed in electron units, [e.u.]. Inevitably a calibration to absolute units involves also a normalization with respect to the irradiated volume V. Thus, for the field of materials science a suitable dimension of the absolute intensity is [I/V] = e.u./nm3 - The intensity measured in the detector is originating from a material with an average electron density of 400 electrons per nanometers cubed . The electron density itself is easily computed from mass density and chemical composition of the material (cf. Sect. 2.2.1). [Pg.102]

What is the mass of a sphere of material of density 7500 kg/m3 whose terminal velocity in a large deep tank of water is 0.6 m/s ... [Pg.34]

In this liquid phase reaction, it may be assumed that the mass density of the liquid is unaffected by the reaction, allowing the material balance for the tubular reactor to be applied on a volume basis (Section 1.7.1, Volume 3) with plug flow. [Pg.263]

Role of Bombardment in Pattern Transfer Regime. Gokan et al. [18] measured the relative 02 RIE rates of a series of polymers and found that the RIE rates scaled inversely with the mass density of carbon as in their IBE study (several materials deviated from the correlation). The relative RIE rates [18] varied by a factor of 3 and do not show the large variations characteristic of the radical-induced mechanism [10]. These results strongly suggest a bombardment-induced mechanism, but one can not directly apply the IBE results to RIE conditions because IBE neutral-to-ion flux ratios are orders of magnitude lower than under RIE conditions. [Pg.215]

Here, v is the velocity vector field, p is the mass density of the fluid, D/Dt = S/Sf + V V is the material derivative, Vp is the gradient of the pressure, r[j is the shear viscosity, and F is the external force acting on the fluid volume. The right-hand side of Eq. (1) is a momentum balance between the internal pressure and viscous stress and the external forces on the fluid body. Any excess momentum contributes to the material acceleration of the fluid volume, on the left-hand side. [Pg.63]

Shown in Figure 3 is the model fitting of the sorption data for the HA and its esters. The mass densities of the materials (Table 5) have been used to convert the concentration to volume fraction. As shown, the model is able to satisfactorily interpolate the experimental data. The estimated parameters of the model are reported in Table 6. [Pg.181]

Measurement of the physieal properties of feed and produet phases (e.g., mass densities, viseosities, surfaee tensions, and wettability) and their dependenee on temperature on typieal equipment materials Qualitative examination of the mass transfer intensity of a single droplet (kicking drop)... [Pg.412]

The phase of a material is a function of its temperature. In the solid phase, the atoms or molecules only vibrate about fixed positions. In the liquid phase, these submicroscopic particles are able to tumble over one another. In the gaseous phase, the atoms or molecules have enough kinetic energy to be separated from one another by relatively large distances. Finally, this chapter introduced density, which is the ratio of a materials mass to its volume. Materials are often characterized by their densities. [Pg.28]

Density is the ratio of a materials mass to volume. As the mass stays the same and the volume decreases, the density of the material increases. [Pg.681]

Physical properties are termed either intensive or extensive. Intensive properties are independent of the quantity of material present. Density, specific volume, and compressibility factor are examples. Properties such as volume and mass are termed extensive their values are determined by the total quantity of matter present. [Pg.46]

The mass density of material, p, is the amount of mass of the material per unit volume (i.e., kg m-3). For component i, the mass density, pt, is therefore... [Pg.587]

In the treatment which follows, it will be assumed that the mass density of the reaction mixture is constant throughout a series of stirred tanks. Thus, if the volumetric feed rate is v, then in the steady state, the rate of outflow from each tank will also be v. Material balances may then be written on a volume basis, and this considerably simplifies the treatment. In practice, the constancy of the density of the mixture is a reasonable assumption for liquids, and any correction which may need to be applied is likely to be small. [Pg.44]


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Material densities

Particle mass material density

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