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The main experimental facts

1 - The main experimental facts a) Pressure-temperature diagram [Pg.188]

The following facts can be remarked upon about Diagram 2, by fixing the initial temperature T at 600 K for example, and by increasing the pressure gradually  [Pg.188]

To sum up, the T -p diagram of propane shows three main zones, one of slow reaction, one of cool flames and one of autoignition, the same is also found for the heavier hydrocarbons, as well as for a large variety of organic substances (ethers, aldehydes, alcohols...). [Pg.189]

The precise experimental definition of a delay depends on the reactor being used and on the properties it is possible to measure. Thus, for a batch reactor, the recording of the pressure increase as a function of time allows the time for which the global rate d(Ap)/dt is at a maximum, to be determined. The intersection of the tangent to the curve Ap(t) at this point with the horizontal Ap = 0 gives the value of the delay. [Pg.189]

The preceding experimental data can be classed as macroscopic others exist which are equally interesting like the speed of a premixed laminar flame. It is possible to take this into account using globalized mechanisms. [Pg.191]


Abstract—A review is given of the main experimental facts concerning the modification of rXH vibration bands by hydrogen bonding, and of the various explanations advanced in the literature for the low frequencies, and the broad and (sometimes) smooth contours observed for these bands under conditions of strong hydrogen bonding. [Pg.85]

According to Fugita [45] the main experimental facts that have to be explained... [Pg.13]

The kinetic model, which can explain the origin of these two relaxation processes and can describe the dependence of the corresponding relaxation times on the concentration, has been proposed by Aniansson and Wall [114, 115, 119]. This model allows to explain the main experimental facts and is generally accepted nowadays. At the same time, subsequent studies allowed for the determination of the application limits of this theory [116-118, 128]. Because the model of Aniansson and Wall is frequently used also for the analysis of dynamic surface properties of micellar solutions [93, 96-103, 133-138], it will be considered below in details. [Pg.449]

Only a few measurements of the effect of pressure on the rates of radical polymerizations have been reported, but the general principles are well enough established that some information about mechanism can be obtained. The main experimental facts of many radical polymerizations can be accounted for in terms of the following reaction scheme (for a recent account see Bamford et al., 1958). [Pg.155]

We have briefly reviewed above the 1-D instabilities which have been predicted theoretically. With the synthesis of new series of molecular materials during these last twenty years, the experimentalists discovered most of these phase transitions which are specific of low-dimensional systems. Following a chronological order, we will next review the main experimental facts ... [Pg.57]

As will be evident from the brief survey of the main experimental facts relating to the stability of lyophobic colloids, to be given in the present section, this opinion is in complete accordance with colloid chemical evidence. [Pg.6]

The parameters K and a are evaluated from the intercept and slope, respectively, of the double-logarithmic plots of [tj] against M determined for a series of samples that differ only in their molar mass. The main experimental facts that have to be explained theoretically are as follows [4] ... [Pg.305]

Abidor IG, Arakelyan VB, Chemomoidik LV, Chizmadzhev Y, Pastushenko VF, Tarasevich MR (1979) Electric breakdown of bilayer lipid membranes. I the main experimental facts and their qualitative discussion. Bioelectrochem Bioenerg 6 37-52... [Pg.782]

We have shown that the effect of stirring on bistable chemical systems in a C.S.T.R. can be understood without any fluctuation process. Inhomogeneities originate in the local character of the feed. Even a simple reaction-diffusion scheme can qualitatively account for the main experimental facts, in particular the shift of the transition point kg to lower values of flow when the stirring rate is decreased. [Pg.176]

The main experimental elfects are accounted for with this model. Some approximations have been made a higher-level calculation is needed which takes into account the fact that the charge distribution of the trapped electron may extend outside the cavity into the liquid. A significant unknown is the value of the quasi-free mobility in low mobility liquids. In principle, Hall mobility measurements (see Sec. 6.3) could provide an answer but so far have not. Berlin et al. [144] estimated a value of = 27 cm /Vs for hexane. Recently, terahertz (THz) time-domain spectroscopy has been utilized which is sensitive to the transport of quasi-free electrons [161]. For hexane, this technique gave a value of qf = 470 cm /Vs. Mozumder [162] introduced the modification that motion of the electron in the quasi-free state may be in part ballistic that is, there is very little scattering of the electron while in the quasi-free state. [Pg.198]

Tbe main experimental facts are listed below, and are illustrated for some typical cases in fig. 1. In order to emphasize the true breadth of the rXH bands this figure has been drawn with a linear and uniform frequency scale throughout. [Pg.87]

A mechanism which explains these main experimental facts is the following. Methyl ethyl ketone is taken as the typical example. [Pg.105]

A model having predictions that are consistent with the aforementioned experimental facts is the Coupling Model (CM) [21-26]. Complex many-body relaxation is necessitated by intermolecular interactions and constraints. The effects of the latter on structural relaxation are the main thrust of the model. The dispersion of structural relaxation times is a consequence of this cooperative dynamics, a conclusion that follows from the presence of fast and slow molecules (or chain segments) interchanging their roles at times on the order of the structural relaxation time Ta [27-29]. The dispersion of the structural relaxation can usually be described by the Kohlrausch-William-Watts (KWW) [30,31] stretched exponential function,... [Pg.501]

The main conclusion from the above experimental facts and theoretical concepts to be emphasized is that the hydration energy or the hydrophobicity (hydrophilicity) of a solute depends upon the chemical composition of a given aqueous medium. It seems reasonable to assume that this dependence plays a regulating role in living systems and therefore it should be taken into account while studying the hydropobicity of biological molecules. [Pg.177]

The main reason why ligand-field models are important is the qualitative experimental fact that hundreds of compounds containing a transition metal ion with a partially filled d ov f shell have ground states and lower excited states whose symmetries can be predicted on the basis of a first-order perturbation model (using a basis set of I functions, 1 — 2 or 3) once the geometries of the molecules are known 1—4). [Pg.69]

The above-mentioned experimental observations encapsulate the main empirical facts established in a large number of studies on EOD. Several of these observations present features that have been analyzed in some detail as described in the following section. [Pg.320]

The above experimental facts show in the main, parallel chemical and stereochemical behavior for mono- and bifunctional silanes. The relative ease of displacement is ... [Pg.89]

Replicate experiments. Finally, we examine the impact of replicating experiments. The main reason one replicates an experiment is to obtain a direct measure of the experimental reproducibility. By replication we are confronted with the simple experimental fact that no matter how much care we take and how much effort we exert, the. results of two experiments are never exactly the same. The differences among replicated experiments g.tve us a direct quantitative m.easure of the experimental error or noise.. These errors are partly due to our Inability to measure accurately the outputs of interest, but they are also due to pur inability to control comp.letely the experimental environment. The... [Pg.283]

Abstract. A model of the conformational transitions of the nucleic acid molecule during the water adsorption-desorption cycle is proposed. The nucleic acid-water system is considered as an open system. The model describes the transitions between three main conformations of wet nucleic acid samples A-, B- and unordered forms. The analysis of kinetic equations shows the non-trivial bifurcation behaviour of the system which leads to the multistability. This fact allows one to explain the hysteresis phenomena observed experimentally in the nucleic acid-water system. The problem of self-organization in the nucleic acid-water system is of great importance for revealing physical mechanisms of the functioning of nucleic acids and for many specific practical fields. [Pg.116]

Although the partial rate factors for the alkylbenzenes vary somewhat with the experimental conditions, the main facts of the situation are perfectly clear ... [Pg.163]

The chloromethylation of thiophene has come somewhat into discredit, partly because of the lachrymatory nature of 2-thenyl chloride, partly because this reaction is highly dependent on the conditions used. Formalin in concentrated hydrochloric acid has been used for chloromethylation, as has the anhydrous system, formaldehyde and hydrogen chloride." The use of a-chloromethyl methylether has also been recommended. The sensitivity of chloromethylation to the experimental conditions is illustrated by the fact that addition of zinc chloride gives di-(2-thienyl)methane as the main product and... [Pg.39]

The second main application of the orbital model lies with ab initio calculations in chemistry (Szabo and Ostlund [1982]). The basic problem is to calculate the energy of an atom, for example, from first principles, without recourse to any experimental facts. The procedure consists in solving the time independent Schrodinger for the atom in question, but unfortunately only... [Pg.28]


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