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Components increasing densities

Hybrid sol-gel films, in contrast to pnre inoiganic films, combine the properties of organic polymeric material with the properties of ceramic. The inorganic components mostly contribute to the increase of scratch resistance, durability and adhesion to the metal substrate. The organic component increases density. [Pg.222]

P/MForging. Even after conventional repressing of a P/M component, it is stiU difficult to increase density above 95%. However, hiU density in a P/M part improves its properties. Hot isostatic pressing in autoclaves works weU, especiaUy for titanium and superaUoy components, but the capital equipment is expensive and production rates are slow. [Pg.184]

Method Density gradient. Rate-zonal. The rate-zonal method is one of six addressed by SpinPro. The other methods are differential, differential-flotation, discontinuous, isopycnic, and 2-step isopycnic. These methods differ dramatically in their set up, principles of operation, and expected results. The rate-zonal method is described here briefly so that the recommendations to follow can be appreciated. Prior to the run in a rate-zonal method, a gradient material is introduced to the rotor tubes in steps of increasing density from the top to the bottom of the tube. The sample to be separated is layered, as a thin band, on the top of the gradient. As the run begins, each component in the sample moves toward the bottom of the tube. Some components sediment faster than others. This fact is the basis for the separation. If the run parameters are appropriate, the components will form separate bands within the gradient. At the conclusion of the run, the band representing the component of interest can be removed from the tube. [Pg.304]

Table 9.3 shows the measured detonation velocities and densities of various types of energetic explosive materials based on the data in Refs. [9-11]. The detonation velocity at the CJ point is computed by means of Eq. (9.7). The detonation velocity increases with increasing density, as does the heat of explosion. Ammonium ni-trate(AN) is an oxidizer-rich material and its adiabatic flame temperature is low compared with that of other materials. Thus, the detonation velocity is low and hence the detonation pressure at the CJ point is low compared with that of other energetic materials. However, when AN particles are mixed with a fuel component, the detonation velocity increases. On the other hand, when HMX or RDX is mixed with a fuel component, the detonation velocity decreases because HMX and RDX are stoichiometrically balanced materials and the incorporation of fuel components decreases their adiabatic flame temperatures. [Pg.260]

With increasing density, N-body interactions with N = 3, 4,. .. may have a discernible effect on the total intensities as well as on the shape of the absorption profile. One may expect a ternary component, and at higher densities perhaps four-body, etc., spectral components that are superimposed with the binary spectrum. At the highest densities (e.g., liquids and pressurized fluids) every monomer may be assumed in permanent interaction with a substantial number of near neighbors. At intermediate densities, that is well below liquid densities, one may be... [Pg.67]

In the framework of the impact approximation of pressure broadening, the shape of an ordinary, allowed line is a Lorentzian. At low gas densities the profile would be sharp. With increasing pressure, the peak decreases linearly with density and the Lorentzian broadens in such a way that the area under the curve remains constant. This is more or less what we see in Fig. 3.36 at low enough density. Above a certain density, the l i(0) line shows an anomalous dispersion shape and finally turns upside down. The asymmetry of the profile increases with increasing density [258, 264, 345]. Besides the Ri(j) lines, we see of course also a purely collision-induced background, which arises from the other induced dipole components which do not interfere with the allowed lines its intensity varies as density squared in the low-density limit. In the Qi(j) lines, the intercollisional dip of absorption is clearly seen at low densities, it may be thought to arise from three-body collisional processes. The spectral moments and the integrated absorption coefficient thus show terms of a linear, quadratic and cubic density dependence,... [Pg.353]

Collision-induced lines , and the induced far wings of allowed lines, are usually very diffuse, typically of a width of Aco 1/Af 1012 Hz reflecting the short duration (At p/vtms 10-12 s) of intermolecular interactions, just as was seen in the case of collision-induced absorption above. In the low-density limit, induced intensities vary as the square of the gas density, which reflects the supermolecular origin. With increasing density, cubic and higher components have been identified. [Pg.368]

Collision-induced absorption is a well developed science. It is also ubiquitous, a common spectroscopy of neutral, dense matter. It is of a supermolecular nature. Near the low-density limit, molecular pairs determine the processes that lead to the collision-induced interactions of electromagnetic radiation with matter. Collision-induced absorption by non-polar fluids is particularly striking, but induced absorption is to be expected universally, regardless of the nature of the interacting atoms or molecules. With increasing density, ternary absorption components exist which are important especially at the higher temperatures. Emission and stimulated emission by binary and higher complexes have also... [Pg.375]

A disadvantage of simple interpretive methods is that the model to which the retention data (or other data) are fit must be fairly accurate. In other words, an interpretive approach may fail if one or more sample components exhibits anomalous retention. Although rare in SFC, such retention behavior is observed occasionally and is difficult to predict intuitively. Note, however, that by anomalous retention we do not mean behavior that is merely unusual, e.g., retention that decreases smoothly with increasing density (at constant temperature). Retention that varies in a regular (continuous) manner, even if unusual, can usually be modeled with a high degree of accuracy (vide infra). [Pg.327]

Decreasing particle or grain size also decreases Df. This effect is seen in both Figure 21.9 and 21.10. The effect of initial density on Df is not the same in all explosives, nor at all densities. For most single-component HEs, such as RDX, HMX, TNT, etc., the Df decreases with increasing density. This trend continues... [Pg.284]

Cholesterol and triacylglycerols are transported in body fluids in the form of lipoprotein particles. Each particle consists of a core of hydrophobic lipids surrounded by a shell of more polar lipids and apoproteins. The protein components of these macromolecular aggregates have two roles they solubilize hydrophobic lipids and contain cell-targeting signals. Lipoprotein particles are classified according to increasing density (Table 26.1) chylomicrons, chylomicron remnants, very low density lipoproteins (VLDL), intermediate-density lipoproteins (IDL), low-density lipoproteins (LDL), and high-density lipoproteins (HDL). Ten principal apoproteins have been isolated and characterized. They are synthesized and secreted by the liver and the intestine. [Pg.1078]

One of the major uses of acid oil from soapstock and the distillates from physical refining is in the manufacture of animal feeds. The fatty components increase the caloric density of the feed. [Pg.784]


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See also in sourсe #XX -- [ Pg.19 ]




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Density component

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