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Distribution points

Figure 8-10. C raphical representation of/dcciu) versus u for (-t-)-3 and (-)-3 sampled at 75 evenly distributed points between -0.03 A and + 0.03 e A b Hydrogen atoins not bonded to chiral carbon atoms were not considered. Figure 8-10. C raphical representation of/dcciu) versus u for (-t-)-3 and (-)-3 sampled at 75 evenly distributed points between -0.03 A and + 0.03 e A b Hydrogen atoins not bonded to chiral carbon atoms were not considered.
Commercially pure (< 99.997%) helium is shipped directiy from helium-purification plants located near the natural-gas supply to bulk users and secondary distribution points throughout the world. Commercially pure argon is produced at many large air-separation plants and is transported to bulk users up to several hundred kilometers away by tmck, by railcar, and occasionally by dedicated gas pipeline (see Pipelines). Normally, only cmde grades of neon, krypton, and xenon are produced at air-separation plants. These are shipped to a central purification faciUty from which the pure materials, as well as smaller quantities and special grades of helium and argon, are then distributed. Radon is not distributed commercially. [Pg.12]

Identify the likely variations in load and p.f. during a 24-hour period. Maintain a minimum fixed kVAr permanently connected in the system, at the distribution point for the likely constant loads. For the rest, the banks may be selected so that only one or two are sufficient to control the whole system for the desired p.f. level or system regulation. This will also limit operations of the banks to only three or four a day and less than a thousand during a year, as recommended in Section 26.1(2). Control may now be carried out ... [Pg.768]

Consequently, consider an infinite one-dimensional line or rod along which fractures occur randomly with an average frequency of Nq per unit length as illustrated in Fig. 8.19. Randomly distributed points on an infinite line obey Poisson statistics and the probability of finding n fractures in a length, /, is given by... [Pg.297]

Leakage may require an increase in the fan power in order to ensure that the required design air distribution to all distribution points is achieved (See Table 9.12). [Pg.790]

Geometric uniformity of distribution points across the cross-section of the tower. [Pg.268]

The urea distribution network in Europe, around year 2006, would be limited to one distribution point for a 500 km radius area (heavy-duty vehicles compatibility - data to be checked and actualized), and would not allow a co-fueling strategy whose interests are the simultaneous fuel/urea filling up at the service-station and the minimization of the urea tank volume. Today, it is difficult to anticipate the consequences of EuroV. [Pg.230]

Some Common Interdependence of Relaxation Times. Consider an arbitrary disposition of the initial distribution point xo and the boundary point d [see Fig. 3(c,d)]. We may take into account two decision intervals I = [—oo, d] and h = [d, +oo] and define two probabilities ... [Pg.409]

FIGURE 2.8 Covariance matrices X for different distributions of two-dimensional data. In the main diagonal ofX are the variances ol x, and x2, respectively. For each covariance matrix 200 bivariate normally distributed points have been simulated. [Pg.54]

In trifluoroacetic acid [0.4 M TBABF4 (tetrabutyl ammonium tetrafluoroborate)] unbranched alkanes are oxidized in fair to good yields to the corresponding triflu-oroacetates (Table 2) [16]. As mechanism, a 2e-oxidation and deprotonation to an intermediate carbenium ion, that undergoes solvolysis is proposed. The isomer distribution points to a fairly unselective CH oxidation at the methylene groups. Branched hydrocarbons are preferentially oxidized at the tertiary CH bond [17]. [Pg.129]

Ceynowa performed electron microscopic studies of 60—80 nm thick microtomed Nafion 125 membranes that were converted, for the purpose of affecting electron density contrast, to the Pb2+ form, and all of the excess cations and co-ions were removed. It is the heavy metal that provides electron density contrast between the phase in which it resides and the surrounding phase. These membranes were then exposed to ethanol and 1,2-epoxypropane, although these solvents would not have remained in the samples under the vacuum in the microscope column. The micrographs consisted of uniformly distributed points that were presumed to be ion clusters that were 3—6 nm in diameter. [Pg.316]

The so-called static dephasing regime (SDR) predicts a linear dependence of I/T2 on the magnetic moment of the particles in solution (22, 25). This regime describes the transverse relaxation of homogeneously distributed static protons in the presence of static, randomly distributed point dipoles. The free induction decay rate, I/T2, is then proportional to the part of the sample magnetization due to the dipoles (p), M = rap, where ra is the concentration... [Pg.268]

The third approach is the introduction of another type of radiation quality high-LET radiation. Clinical experience with neutrons has demonstrated that high-LET radiations are superior to low-LET radiations for some tumor types or sites. Fast neutrons were indeed the first high-LET radiations to be applied clinically (see Sec. 4.1). Although in the first studies they were applied in suboptimal conditions from a technical or dose distributions point of view, their advantage for some types of tumors is well established, particularly for slowly growing, well-differentiated tumors. Randomized trials have indeed shown their superiority over conventional photons for salivary gland tumors and prostatic adenocarcinomas. [Pg.780]

In the case of irregularly distributed points a direction can be determined by an angle P with a tolerance of A F (opening angle) the corresponding distance is again l Al. [Pg.117]

Recently, Sokalski et al. presented distributed point charge models (PCM) for some small molecules, which were derived from cumulative atomic multipole moments (CAM Ms) or from cumulative multicenter multipole moments (CMMMs) [89,90] (see Sect. 3.2). For this method the starting point can be any atomic charge system. In their procedure only analytical formulas are used,... [Pg.60]


See other pages where Distribution points is mentioned: [Pg.392]    [Pg.45]    [Pg.187]    [Pg.685]    [Pg.768]    [Pg.78]    [Pg.364]    [Pg.948]    [Pg.268]    [Pg.268]    [Pg.1339]    [Pg.309]    [Pg.389]    [Pg.276]    [Pg.127]    [Pg.205]    [Pg.53]    [Pg.109]    [Pg.274]    [Pg.187]    [Pg.110]    [Pg.424]    [Pg.739]    [Pg.320]    [Pg.45]    [Pg.53]    [Pg.740]    [Pg.74]    [Pg.75]    [Pg.80]    [Pg.193]    [Pg.737]    [Pg.118]    [Pg.62]    [Pg.317]    [Pg.23]   
See also in sourсe #XX -- [ Pg.352 ]




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Boiling Point Distribution of Liquid Fraction

Boiling point distribution

Boiling point distributions, liquid products

Boiling-point distribution cracking

Bond critical point properties and electron density distributions

Catalytic boiling-point distribution

Charge Density Distribution Point-Like

Computational point distribution

Critical points of molecular charge distributions

Difference point distributed feed columns

Distributions by Boiling Point

Electron density distribution critical point

Fuels boiling point distributions

Melt crystallization melting points, distributions

Nuclear charge distribution point

Percentage Points, --Distribution

Percentage points, F-distribution

Percentage points, Student’s t-distribution

Percentage points, chi-square distribution

Point Analysis Providing Morphology, Texture and Strata Distribution

Point Source Diffusion Formulas Based on a Gaussian Distribution

Point distribution schemes

Point-pair distance distribution

Points of Molecular Charge Distributions

Random point distribution

Randomly distributed branching point

Systems with Randomly Distributed Branching Points

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