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Graph value

The Bandwidth is essentially a normalized half confidence band. The confidence interval bandwidths for 9 data sets using inverse transformed data are given in Table X. The bandwidths are approximately the vertical widths of response from the line to either band. The best band was found for chlorpyrifos, 1.5%, at the minimum width (located at the mean value of the response) and 4.9% at the minimum or lowest point on the graph. Values for fenvalerate and chlorothalonil were slightly higher, 2.1-2.2% at the mean level. The width at the lowest amount for the former was smaller due to a lower scatter of its points. The same reason explains the difference between fenvalerate and Dataset B. Similarly, the lack of points in Dataset A produced a band that was twice as wide when compared to Dataset B. Dataset C gave a much wider band when compared to Dataset B. [Pg.153]

Clyne and Thrush s results showed that the intercepts of Figures 7-1 and 7-2 depend on the nature of the chaperone gas, but not on its concentration. Thus, k3 must be small compared to 4[M] for the conditions employed an upper limit of 10 sec-1 was predicted for k3. From the slopes of the graphs, values of kx + k2 could be deduced. These values are listed in Table 7-1 for various chaperone gases. [Pg.274]

Tabulate and graph values of coefficient of isothermal compressibility of this oil for the pressure ranges indicated. Does your graph look like Figure 8-5 ... [Pg.244]

In both graphs values of %Ca and %Cn are read from the values of nff and d ° these values are... [Pg.30]

Graph values of versus the Charton steric constant for the substituents C2H5-, H-, Me-, CH2Br-, CH2CI-, CH2I-, CH(Me)2-, Bu-, CCI3-, Ph-, CBr - and CEst. and values are found in tables in Appendix 3). [Pg.48]

It is interesting to note that the mix water naturally inhibited the gel formation and the formation water accelerated same. We had a pot life with the mix water of approximately one hundred minutes instead of a graph value of seventy minutes. We expected to pressure off on the holes because of the salt and temperature of the formation water. This condition did not seem to cause us any problems in the field. [Pg.427]

Figure 4 (left). Isotopic compositions of carbon flows, and of reactant C, at the C branch point. As shown by the graph, values of d vary with, a parameter eqnivalent to the fractional yield of D. The zero point of the S scale is arbitrarily set by the isotopic composition of the input carbon flow, <5,. [Pg.229]

The above solution has been implemented in the mathematical computer program Mathcad. The solution is readily calculated. The result for a=0.9 and = 0.85 is shown in Figure 1. The degree of saturation S(r,T) is shown as a function of the radius rlr, for a number of dimensionless times r. The top graph shows short times from T =0.002 to r= 0.216, and the bottom graph values from r = 0.216 to r=3. [Pg.338]

Figure 4 A one-dimensional visualization graphing values in selected-ion channels along a slice through co-eluted peaks. Figure 4 A one-dimensional visualization graphing values in selected-ion channels along a slice through co-eluted peaks.
Fig. 5.3.2. Distance at which 9/10 and 3/4 of the associated ions lie from a central ion = 3 A) against the Bjerrum distance /. The vertical bars denote the values of / for a (1 1) electrolyte in W = water, D = dimethylformamide, A = acetone, P = pyridine, C = < -dichIorobenzene. In the top of the graph values of Ka corresponding to some / values are given. Fig. 5.3.2. Distance at which 9/10 and 3/4 of the associated ions lie from a central ion = 3 A) against the Bjerrum distance /. The vertical bars denote the values of / for a (1 1) electrolyte in W = water, D = dimethylformamide, A = acetone, P = pyridine, C = < -dichIorobenzene. In the top of the graph values of Ka corresponding to some / values are given.
It is seen that equation (17) shows a linear relationship between the reciprocal of the corrected retention volume and the concentration of solvent in the mobile phase. Consequently, if retention data is measured over a range of solvent concentrations, employing the chiral agent itself as the solute, a linear relationship will be obtained by plotting (lA ) against (C ) and from the intercept and slope of the graph, values for... [Pg.75]

Recording the weight of sand used and the size of the crystaUizing dish will help to make the graph values more reproducible. [Pg.21]

FiG. C-12 Maximum aiiowabie ioad for thoroughly lubricated bearings. Reduce load to 10 percent of graph value for dry running. (Source Advance Carbon Products.)... [Pg.139]

In the annealed cylinder the presence of own compressive stress has been observed, which was disclosed as lack of indications changes in the initial stretching phase, and their value may be evaluated on the basis of extrapolating the graphs to the coordinate axis. [Pg.385]

Figure Bl.10.1. Poisson distribution for fi(left vertical axis). Cumulative Poisson distribution for fi= l(right vertical axis). The cumulative distribution is the sum of the values of the distribution from 0 to n, where n =, 2, 3, 4, 5 on this graph. Figure Bl.10.1. Poisson distribution for fi(left vertical axis). Cumulative Poisson distribution for fi= l(right vertical axis). The cumulative distribution is the sum of the values of the distribution from 0 to n, where n =, 2, 3, 4, 5 on this graph.
The complete reduction of zinc oxide is favoured by a small value of K. i.e. when log,u A, > log,o X,. Figure 3.5 shows plots of logio Xi, and logio X2 against 1/T where the two graphs intersect log)o X for the reduction process is zero and hence X = 1. [Pg.71]

The minimum number of cycles is given by the nullity or Frerejacque number ( ) according to Eq. (5). It is the difference between the number of nodes a = atoms) and the number of edges h = bonds). The value of 1 stands for the number of compounds considered (here, one compound). This minimum number corresponds to the munber of chords. These are defined as nodes that turn a cyclic graph or structure into an acyclic one. [Pg.55]

Quail titles, wli ich arc selected from lh e. Averages On ly coluiii n and added to the. Avg. graph column, will he written out and averaged, as described above, but will also be plotted on th e tn olccti lar dyu am ics graph. fo in spect the com pii ted average value, select th e quantity so that the outline appears around it and the average is displayed beside Value. [Pg.320]

Moli cii lar dynamics is csscn Lially a sLiidy of ih c evniiitioii in tim c of energetic and siniclnral molecular data. The data is often best represented as a graph of a molecular quantity as a function of iime. The values to be plotted can be any qnantity x that is being averaged over the trajectory, or the standard deviation. Dx. You can create as many as four simultaneous graphs at once. [Pg.323]

Many of the descriptors which can be calculated from the 2D structure rely upon the molecular graph representation because of the need for rapid calculations. Kier and Hall have developed a large number of topological indices, each of which characterises the molecular structure as a single number [Hall and Kier 1991]. Every non-hydrogen atom ir the molecule is characterised by two delta values, the simple delta Si and the valence delta SJ ... [Pg.687]

Averages or plotted values at regular time intervals. You specify an Average/Graph period in the Molecular Dynamics Averages dialog box. [Pg.80]


See other pages where Graph value is mentioned: [Pg.226]    [Pg.57]    [Pg.57]    [Pg.105]    [Pg.28]    [Pg.175]    [Pg.226]    [Pg.57]    [Pg.57]    [Pg.105]    [Pg.28]    [Pg.175]    [Pg.384]    [Pg.578]    [Pg.816]    [Pg.2524]    [Pg.2647]    [Pg.300]    [Pg.428]    [Pg.80]    [Pg.318]    [Pg.323]    [Pg.324]    [Pg.162]    [Pg.390]    [Pg.658]    [Pg.663]    [Pg.161]    [Pg.258]    [Pg.2]    [Pg.1267]    [Pg.318]    [Pg.323]    [Pg.323]   
See also in sourсe #XX -- [ Pg.6 , Pg.8 ]




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