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Monotonic function, mean value

Diffusion within the catalyst particle can be accounted for by using an effectiveness factor, tj, but x should no longer be defined to make k(x) linear in x. Rather, it would be sensible to make tjk linear in x. Of course, straightening out the monotone dependence on x of one parameter, distorts the distribution, as in equation (4), and it may be better to think of the Damkohler number as a function of x. We can alway write it as Da.u>(x), where a>(x) has a mean value of 1. [Pg.218]

As was shown at the end of Section 6.1, for the Dirichlet problem, G > 0. Hence for any monotonically decreasing /(/ ), the mean value (/) decreases with increasing R. This statement does not depend on the sign of the monotonic function, as was noted in [98] for the ls-Dirichlet problem. This statement holds for the lowest state with any given angular momentum in a spherically symmetric problem. For example, the monotonically decreasing r 3) data for the Dirichlet problem are presented in [101] for 2p states in the sphere of enlarged radius R. [Pg.61]

This situation is depicted in Figure 3 for the Is state of the hydrogen atom. Note that one may not insist on monotone density or mean values when the external potential has the form W(r - Rq) and rj = Rq. This may be formally explained as follows when IT is a smooth function (or an approximation to it) for the derivative on Ro there are at least two solutions for Equation (6.12) and conservation of the sign for the function G is not guaranteed (see... [Pg.62]

One further example. The problems in RD for increasing dimension D (or angular momentum l) for the lowest state of a given symmetry may be described by an additional external potential q(q + 1 )r 2, where q — t + (D - 3)/2. For small r values, one concludes that G > 0, and hence, for larger D (or larger l) the wavefunctions near the origin decrease and so does any mean value of the monotonically decreasing function /(/ ). [Pg.63]

Staphylococcus aureus strains are more hydrophobic than Staphylococcus epidermidis strains. The greater surface hydrophobicity of Staphylococcus aureus, along with the reduced negative surface charge on these bacteria, correlated with its increased resistance to pDMAEMA (Spearman s correlation coefficient >0.90). (Spearman s correlation coefficient is a non-parametric measure of statistical dependence between two variables and assesses how well the relationship between two variables can be described using a monotonic function. If there are no repeated data values, a perfect Spearman correlation of +1 or -1 occurs when each of the variables is a perfect monotone function of the other.) Although the Staphylococcus aureus isolates are more hydrophobic, as determined by mean values, some individual isolates had bacterial adhesion to hydrocarbons values similar to those of Staphylococcus epidermidis strains [23]. [Pg.7]

The difficulty is to know the monotonicity of the operands. This requires the computation of the derivatives of each subfunction involved in the expression of the function being studied, which needs a large amount of work. Alt and Lamote (2001) have proposed the idea of random interval arithmetic which is obtained by choosing standard or inner interval operations randomly with the same probability at each step of the computation. It is assumed that the distribution of the centres and radii of the evaluated intervals is normal. The mean values and the standard deviations of the centers and radii of the evaluated intervals computed using random interval arithmetic are used to evaluate an approximate range of the function ... [Pg.991]

Up till now we have dealt with (fuzzy) set-theoretic operations. Really it is more important in computational chemistry to compute with numbers, in particular with fuzzy numbers. For our purposes a fuzzy number is an element of the real axis E that has to satisfy the following conditions (i) there is only one xq, the mean value of A, with ix(xo) = I, (ii) /z is piecewise continuous, and (iii) /z(x) < /z(xo) is monotonically increasing and /z(x) > ix xo) is monotonically decreasing. The extension of the principle to fuzzy points, fuzzified functions and fuzzy functions is explained by Bandemer and Otto in a chemical context. A further extension of fuzzy numbers are flat fuzzy numbers that can model a fuzzy interval, e.g., by a trapezoidal membership function. [Pg.1092]

Accuracy of the difference scheme is 0(Af + Ar2), which could be reduced to 0(At2 4- Ar2) by means of the symmetrical difference scheme. In practice schemes with monotonously increasing spatial and temporal steps are usually used for these purposes [1, 9-11]. As r 1, Ar is small but increases with r whereas At increment is limited by the condition that the relative change of gm at any step should not exceed a given small value. Unlike the case of immobile particle reaction, the calculation of the functionals J[Z], (5.1.37) and (5.1.38), requires one-dimensional integration only which is not time-consuming. [Pg.249]

The function rt - fi(Pi, Vt) is known as an equation of state. Note that the latter provides us with a means of determining r through measurements of P and V. However, the function fi is arbitrary, in the sense that any single-valued function which increases or decreases monotonically with r can be used it does not matter what system is utilized for the specification of the empirical temperature. One can turn this looseness into an advantage in the following manner For the different systems i — 1, 2,. .. the various quantities flt f2,... [Pg.11]


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See also in sourсe #XX -- [ Pg.60 , Pg.61 ]




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Mean value

Monotone function

Monotonic

Monotonic functions

Value functions

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