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Graph limitations

X = x(K) per site and demand that it be strictly negative (even for the infinite graph limit). The Euler relation then devolves ° to... [Pg.327]

The calibration graph for the probe using a strength machine, has been shown in Fig. 7 It can be observed that the dependence of indications of the device of Wirotest type on the loading is linear within the proportionality limit scope. After unloading the indications do not return to zero, but show own stress caused in effect of plastic deformation of the tested sample... [Pg.387]

The graph of Figure 6.8 illustrates the effect of increasing voltage on the electric current between two electrodes immersed in a gas. The circuit is completed by an external resistance, used to limit the current flow. As shown in Figure 6.8, the discharge can be considered in regions, which are described below. [Pg.39]

Following this procedure urea can be determined with a linear calibration graph from 0.143 p.g-ml To 1.43 p.g-ml and a detection limit of 0.04 p.g-ml based on 3o criterion. Results show precision, as well as a satisfactory analytical recovery. The selectivity of the kinetic method itself is improved due to the great specificity that urease has for urea. There were no significant interferences in urea determination among the various substances tested. Method was applied for the determination of urea in semm. [Pg.371]

To overcome the limitations of the database search methods, conformational search methods were developed [95,96,109]. There are many such methods, exploiting different protein representations, objective function tenns, and optimization or enumeration algorithms. The search algorithms include the minimum perturbation method [97], molecular dynamics simulations [92,110,111], genetic algorithms [112], Monte Carlo and simulated annealing [113,114], multiple copy simultaneous search [115-117], self-consistent field optimization [118], and an enumeration based on the graph theory [119]. [Pg.286]

It is evident that an approximate — 1.5cr shift ean be determined from the data and so the Cpi value is more suitable as a model. Using the graph on Figure 6, whieh shows the relationship Cp, (at 1.5cr shift) and parts-per-million (ppm) failure at the nearest limit, the likely annual failure rate of the produet ean be ealeulated. The figure has been eonstrueted using the Standard Normal Distribution (SND) for various limits. The number of eomponents that would fall out of toleranee at the nearest limit, is potentially 30 000 ppm at = 0.62, that is, 750 eomponents of the 25 000 manufaetured per annum. Of eourse, aetion in the form of a proeess eap-ability study would prevent further out of toleranee eomponents from being produeed and avoid this failure rate in the future and a target Cp = 1.33 would be aimed for. [Pg.294]

These MUST be taken from Shaft A to Shaft B , then from Shaft B to Shaft A (s of these measurements is compared with the limit calculated from the graph. [Pg.611]

The author has curve-fit the Erbar/Maddox curves since readability for the graph is limited. For simplicity, let ... [Pg.53]

To evaluate the fibrillation behavior of dispersed TLCP domains according to the - 5 relation discussed previously, different - 5 graphs were calculated by eliminating the thickness variable x. The result is reported in Fig. 18. It is obvious that all the points obtained are found to be relatively close to the critical curve by Taylor. The Taylor-limit is also shown in the figure with a solid curve. One finds that all the values calculated on sample 1 are completely above the limit, while all those determined on sample 4 are completely below the limit. The other two samples, 2 and 3, have the We - 5 relation just over the limit. [Pg.695]

Table 6.2 Number of nodes Ht, C = 0,.. . 4 in the minimal deterministic state transition graph (DSTG) representing the regular language r2t[0, where 0 is an elementary fc = 2, r = 1 CA rule Amax is the maximal eigenvalue of the adjacency matrix for the minimal DSTG and determines the entropy of the limit set in the infinite time limit (see text), Values are taken from Table 1 in [wolf84a. ... Table 6.2 Number of nodes Ht, C = 0,.. . 4 in the minimal deterministic state transition graph (DSTG) representing the regular language r2t[0, where 0 is an elementary fc = 2, r = 1 CA rule Amax is the maximal eigenvalue of the adjacency matrix for the minimal DSTG and determines the entropy of the limit set in the infinite time limit (see text), Values are taken from Table 1 in [wolf84a. ...
Figure 6.15 also shows a graph of / against m2. Note that this plot has a non-zero slope and it becomes linear as m2—>0. Therefore, the limiting law... [Pg.295]

Figure 6.14 Graph of vapor fugacity /against. v, for. Vjl-TO +. y2HC1. The various curves are as follows . vapor fugacity of H Ot , vapor fugacity of HC1 . total vapor fugacity (H2O + HC1). The dashed line gives the Raoult s law limiting values for the vapor fugacity of H20. Figure 6.14 Graph of vapor fugacity /against. v, for. Vjl-TO +. y2HC1. The various curves are as follows . vapor fugacity of H Ot , vapor fugacity of HC1 . total vapor fugacity (H2O + HC1). The dashed line gives the Raoult s law limiting values for the vapor fugacity of H20.

See other pages where Graph limitations is mentioned: [Pg.491]    [Pg.578]    [Pg.1426]    [Pg.1659]    [Pg.39]    [Pg.35]    [Pg.710]    [Pg.19]    [Pg.148]    [Pg.416]    [Pg.226]    [Pg.1336]    [Pg.87]    [Pg.548]    [Pg.386]    [Pg.421]    [Pg.610]    [Pg.41]    [Pg.491]    [Pg.1116]    [Pg.1294]    [Pg.79]    [Pg.98]    [Pg.158]    [Pg.86]    [Pg.138]    [Pg.136]    [Pg.310]    [Pg.232]    [Pg.35]    [Pg.692]    [Pg.30]    [Pg.240]    [Pg.565]    [Pg.753]    [Pg.48]    [Pg.54]    [Pg.273]    [Pg.279]   
See also in sourсe #XX -- [ Pg.40 , Pg.324 ]




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