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Peculiar function

The peculiar function of the science of safety in achieving this aim is the acquisition and summarization of knowledge regarding the conditions and design of safety in handling technical systems, as well as regarding the various possibilities of protection from their inherent dangers and to... [Pg.1]

Consider a partial molar value J(. In a uniform solution, that value is a function of the variables temperature and composition. If we examine a mole of the overall solution, taking as composition variables the molar fractions x it is always possible to decompose that fimetion into the sum of two functions such that one depends only on the temperature (we ignore the influence of pressure on a liquid solution) - this is the peculiar function... [Pg.194]

Function ana Process Cycle Industrial furnaces are enclosures in which process material is heated, dried, melted, and/or reac ted. Melting is considered a special category because of the peculiar difficulties that may be associated with a sohd feed, a hot hquid produc t, and a two-phase mixture in between it is customaiy, therefore, to classify furnaces as heating or melting. [Pg.2403]

The values in Figures 2-11 and 2-12 are not entirely typical of all composite materials. For example, follow the hints in Exercise 2.6.7 to demonstrate that E can actually exceed both E., and E2 for some orthotropic laminae. Similarly, E, can be shown to be smaller than both E. and E2 (note that for boron-epoxy in Figure 2-12 E, is slightly smaller than E2 in the neighborhood of 6 = 60°). These results were summarized by Jones [2-6] as a simple theorem the extremum (largest and smallest) material properties do not necessarily occur in principal material coordinates. The moduli Gxy xy xyx exhibit similar peculiarities within the scope of Equation (2.97). Nothing should, therefore, be taken for granted with a new composite material its moduli as a function of 6 must be examined to truly understand its character. [Pg.81]

TT-Electron materials, which are defined as those having extended Jt-electron clouds in the solid state, have various peculiar properties such as high electron mobility and chemical/biological activities. We have developed a set of techniques for synthesizing carbonaceous K-electron materials, especially crystalline graphite and carbon nanotubes, at temperatures below 1000°C. We have also revealed new types of physical or chemical interactions between Jt-electron materials and various other materials. The unique interactions found in various Jt-electron materials, especially carbon nanotubes, will lay the foundation for developing novel functional, electronic devices in the next generation. [Pg.153]

It is evident that, under certain conditions, an unusual shape of q]/ r) functions may be expected. This is a result of the blocking term contribution. Some rearrangement of terms is necessary for the case where kj = kq, but no peculiar behavior is observed under these conditions. It is worth emphasizing that our result for q]l(r) generalizes the expression obtained by Bratko and Chakraborty for infinite dilution of fluid particles [35]. The q]/ r) functions coincide with their result for p 0. [Pg.339]

From such information even the inexperienced estimator can establish an approximation of the costs, provided he adequately visualizes the work functions and steps involved. From the same type of work reference, the experienced estimator can develop a realistic cost, usually expressed with certain contingencies to allow for unknown factors and changing conditions. The professional estimator wall normally develop cost charts and tables peculiar to the nature of his responsibilities and requirements of his employer. [Pg.47]

The use of Polya s Theorem in a specialized context such as the above, has led to the extension of the theorem along certain useful lines. One such derivation pertains to the situation where the boxes are not all filled from the same store of figures. More specifically, the boxes are partitioned into a number of subsets, and there is a store of figures peculiar to each subset. To make sense of this we must assume that no two boxes in different subsets are in the same orbit of the group in question. A simple extension of Polya s Theorem enables us to tackle problems of this type. Instead of the cycle index being a function of a single family of variables, the 5j, we have other families of variables, one for each subset. An example from chemical enumeration will make this clear. [Pg.125]

Though due to the fact that it is difficult to interprete amplitude dependence of the elastic modulus and to unreliable extrapolation to zero amplitude, the treatment of the data of dynamic measurements requires a special caution, nevertheless simplicity of dynamic measurements calls attention. Therefore it is important to find an adequate interpretation of the obtained results. Even if we think that we have managed to measure correctly the dependences G ( ) and G"( ), as we have spoken above, the treatment of a peculiar behavior of the G (to) dependence in the region of low frequencies (Fig. 5) as a yield stress is debatable. But since such an unusual behavior of dynamic functions is observed, a molecular mechanism corresponding to it must be established. [Pg.94]

Early work on 14-3-3 proteins placed researchers in a peculiar position of trying to define the precise function of 14-3-3s. This came from the large number of, and apparently diverse type of targets proteins. Continued work has brought more and more insights and it is... [Pg.1026]

By means of the experimental methods briefly referred to in 9 a large number of specific-heat measurements have been made at very low temperatures. In Fig. 91 we haye the atomic heats of some metals, and of the diamond, represented as functions of the temperature. The peculiar shape of the curves will. be at once apparent. At a more or less low temperature, the atomic heat decreases with extraordinary rapidity, then apparently approaches tangentially the value zero in the vicinity of T = 0. The thin curves represent the atomic heats calculated from the equation ... [Pg.526]

This contrasts with relation (5.16), which led to a non-physical conservation law for J. Eqs. (5.28) and Eq. (5.30) make it possible to calculate in the high-temperature limit the relaxation of both rotational energy and momentum, avoiding any difficulties peculiar to EFA. In the next section we will find their equilibrium correlation functions and determine corresponding correlation times. [Pg.163]

A preliminaiy characterization of a new iron—sulfur protein isolated from Desulfovibrio vulgaris Hildenborough was reported in 1989 124). The protein contained approximately 6 iron and 6 inorganic sulfur atoms per molecule. The FPR spectrum of the dithionite reduced protein exhibited an S = signal similar to what was found for synthetic compounds with a [6Fe-6S] core (prismane core). No other FPR signals were reported at this time, and based on the observed similarity it was suggested that this peculiar iron-sulfur protein contained a [6Fe-6S] cluster. Because it had no known function, the pro-... [Pg.378]

The complete formula for the Taylor series expansion attached to a n-variable function f (x) in the neighbourhood of the point x, possess the following peculiar simple structure when using NSS s ... [Pg.235]


See other pages where Peculiar function is mentioned: [Pg.155]    [Pg.155]    [Pg.400]    [Pg.1097]    [Pg.236]    [Pg.25]    [Pg.78]    [Pg.21]    [Pg.150]    [Pg.54]    [Pg.286]    [Pg.155]    [Pg.155]    [Pg.400]    [Pg.1097]    [Pg.236]    [Pg.25]    [Pg.78]    [Pg.21]    [Pg.150]    [Pg.54]    [Pg.286]    [Pg.451]    [Pg.60]    [Pg.170]    [Pg.45]    [Pg.692]    [Pg.299]    [Pg.36]    [Pg.45]    [Pg.725]    [Pg.53]    [Pg.37]    [Pg.44]    [Pg.161]    [Pg.196]    [Pg.193]    [Pg.233]    [Pg.281]    [Pg.144]    [Pg.45]    [Pg.138]    [Pg.39]    [Pg.214]    [Pg.282]    [Pg.341]   
See also in sourсe #XX -- [ Pg.192 ]




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