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Operators difference

Operational differences in the analytical methods used for determining the heating value of the volatile content. [Pg.515]

These circuits include components that carry out arithmetic operations, differ-... [Pg.114]

Chapter 11 analyzes the recently discovered mechanistic equivalence of electrochemical promotion and metal-support interactions on ionic and mixed conducting supports containing Zr02, Ce02 or Ti02. The analysis focuses on the functional identity and operational differences of promotion, electrochemical promotion and metal support interactions. [Pg.11]

Promotion, electrochemical promotion and metal-support interactions are three, at a first glance, independent phenomena which can affect catalyst activity and selectivity in a dramatic manner. In Chapter 5 we established the (functional) similarities and (operational) differences of promotion and electrochemical promotion. In this chapter we established again the functional similarities and only operational differences of electrochemical promotion and metal-support interactions on ionic and mixed conducting supports. It is therefore clear that promotion, electrochemical promotion and metal-support interactions on ion-conducting and mixed-conducting supports are three different facets of the same phenomenon. They are all three linked via the phenomenon of spillover-backspillover. And they are all three due to the same underlying cause The interaction of adsorbed reactants and intermediates with an effective double layer formed by promoting species at the metal/gas interface (Fig. 11.2). [Pg.509]

Consequently the proven functional identity of classical promotion, electrochemical promotion and metal-support interactions should not lead the reader to pessimistic conclusions regarding the practical usefulness of electrochemical promotion. Operational differences exist between the three phenomena and it is very difficult to imagine how one can use metal-support interactions with conventional supports to promote an electrophilic reaction or how one can use classical promotion to generate the strongest electronegative promoter, O2, on a catalyst surface. Furthermore there is no reason to expect that a metal-support-interaction-promoted catalyst is at its best electrochemically promoted state. Thus the experimental problem of inducing electrochemical promotion on fully-dispersed catalysts remains an important one, as discussed in the next Chapter. [Pg.510]

Having discussed the functional equivalence of classical promotion, electrochemical promotion and metal-support interactions on 02 -conducting and mixed electronic-ionic conducting supports, it is useful to also address and systematize their operational differences. This is attempted in Figure 11.15 The main operational difference is the promoter lifetime, Tpr, on the catalyst surface (Fig. 11.15). [Pg.510]

In addition to the extra hardware required for these experimental runs, the ARC was operated differently than under standard hazard evaluation conditions. Instead of heating, searching and waiting, the samples were heated to a specified temperature and were then maintained isothermally at that temperature for extended periods of time. Pressure and temperature data were then monitored and stored in the microcomputer at a rate of 1 Hz. It should be noted that the apparatus reverts back to normal operation (i.e., tracking an exotherm), if a heat rise rate greater than 0.02 °C/min is detected. [Pg.431]

In this chapter we study the stability with respect to the initial data and the right-hand side of two-layer and three-layer difference schemes that are treated as operator-difference schemes with operators in Hilbert space. Necessary and sufficient stability conditions are discovered and then the corresponding a priori estimates are obtained through such an analysis by means of the energy inequality method. A regularization method for the further development of various difference schemes of a desired quality (in accuracy and economy) in the class of stability schemes is well-established. Numerous concrete schemes for equations of parabolic and hyperbolic types are available as possible applications, bring out the indisputable merit of these methods and unveil their potential. [Pg.383]

Operator-difference schemes. We now consider a linear system 8h depending on a parameter h as a vector of some normed space equipped with the norm h. With regard to the linear system 8h, it is reasonable to introduce a collection of norms li 111,. II II/, m II ll m. .., thus causing... [Pg.384]

The notion of stability. The notion of stability for three-layer schemes is of our initial concern. By a two-layer scheme we mean a set of operator-difference equations (4) depending on the parameters h and t. We preassumed here that the operators A and B are given on the entire space Bh-... [Pg.388]

Approximation and convergence. The notions of approximation, convergence and accuracy for operator-difference schemes are introduced by analogy with the corresponding notions for the operator schemes A y — arising earlier in Chapter 2, Section 4. Only a few editorial changes will... [Pg.394]

Stability and convergence. No restrictions are made regarding the smoothness of the coefficients and the. solution in the further estimation of the accuracy of scheme (7)-(9). This can be done using various a priori estimates for the operator-difference three-layer scheme... [Pg.503]

Further development of some a priori estimate for a solution of the problem concerned is mostly based on an operator-difference analog of problem (37)-(38) such as... [Pg.557]

In this view, it seems reasonable to turn to operator-difference schemes... [Pg.712]

The two-layer operator-difference scheme we are interested in acquires the canonical form... [Pg.779]

Also, we consider the total approximation method as a constructive method for creating economical difference schemes for the multidimensional equations of mathematical physics. The notion of additive scheme is introduced as a system of operator difference equations that approximates the original differential equation in the total sense. Two quite general heuristic methods (proposed earlier by the author) for obtaining additive economical schemes are discussed in full details. The additive schemes require a new technique for investigating convergence and a new type of a priori estimates that take into account the definition of the property of approximation. [Pg.783]

Hence, the method of Mead and Truhlar [6] yields a single-valued nuclear wave function by adding a vector potential A to the kinetic energy operator. Different values of odd (or even) I yield physically equivalent results, since they yield (< )) that are identical to within an integer number of factors of exp(/< )). By analogy with electromagnetic vector potentials, one can say that different odd (or even) I are related by a gauge transformation [6, 7]. [Pg.19]

In the preceding section, we presented principles of spectroscopy over the entire electromagnetic spectrum. The most important spectroscopic methods are those in the visible spectral region where food colorants can be perceived by the human eye. Human perception and the physical analysis of food colorants operate differently. The human perception with which we shall deal in Section 1.5 is difficult to normalize. However, the intention to standardize human color perception based on the abilities of most individuals led to a variety of protocols that regulate in detail how, with physical methods, human color perception can be simulated. In any case, a sophisticated instrumental set up is required. We present certain details related to optical spectroscopy here. For practical purposes, one must discriminate between measurements in the absorbance mode and those in the reflection mode. The latter mode is more important for direct measurement of colorants in food samples. To characterize pure or extracted food colorants the absorption mode should be used. [Pg.14]

Figure 6.18 Galvanic cell operationally differing from an electrolytic cell (two methods of representation are shown). Figure 6.18 Galvanic cell operationally differing from an electrolytic cell (two methods of representation are shown).
The closeness of agreement between independent results obtained with the same method on identical test material but under different conditions (different operators, different apparatus, different laboratories, and/or after different intervals of time). The measure of reproducibility is the standard deviation qualified with the term reproducibility as reproducibility standard deviation. In some contexts reproducibility may be defined as the value below which the absolute difference between two single test results on identical material obtained under the above conditions may be expected to lie with a specified probability. Note that a complete statement of reproducibility requires specification of the experimental conditions which differ. [Pg.80]

Recently, Chiron introduced the System 340 platform that automates incubation, washing, reading, data processing, and report generation. It is anticipated that automation will dramatically reduce operator-to-operator differences while decreasing labor requirements. In one laboratory the average coefficient of variation was reduced 43% and the hands-on labor was reduced 39% with the automated... [Pg.211]


See other pages where Operators difference is mentioned: [Pg.469]    [Pg.194]    [Pg.177]    [Pg.34]    [Pg.167]    [Pg.180]    [Pg.308]    [Pg.42]    [Pg.542]    [Pg.88]    [Pg.162]    [Pg.91]    [Pg.542]    [Pg.118]    [Pg.383]    [Pg.385]    [Pg.387]    [Pg.389]    [Pg.391]    [Pg.393]    [Pg.395]    [Pg.562]    [Pg.779]    [Pg.782]    [Pg.74]    [Pg.65]    [Pg.51]    [Pg.510]   
See also in sourсe #XX -- [ Pg.170 ]




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Central difference operator

Central difference operator averaged

Cluster operator different

Difference approximation of elementary differential operators

Difference of two operators

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Difference schemes as operator equations General formulations

Different reflectron operational modes

Dipole difference operator, definition

Energy difference operator

Finite differences operators

Forward difference operator

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Operator-difference scheme

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