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Entire cross point region

Keywords— Cross point, entire cross point region, ideal cross point region, bit plane decomposition, entropy coding. [Pg.186]

These cross-point regions A(n) are called the entire cross-point regions (ECRs) to distinguish them from the ideal cross point regions (ICRs) in Definition 2.2. [Pg.186]

Observe that the CSTR locus is contained entirely within the region generated by the PFR, and hence a CSTR from the feed does not serve to expand the region of achievable points further. From Chapter 4, it is known that PFR trajectories cannot cross. Hence, running PFRs from the CSTR locus will not expand the region—any PFR trajectory extended from points on the CSTR locus in Figure 5.3 are contained... [Pg.112]

Infrared data in the 1575-400 cm region (1218 points/spec-trum) from LTAs from 50 coals (large data set) were used as input data to both PLS and PCR routines. This is the same spe- tral region used in the classical least-squares analysis of the small data set. Calibrations were developed for the eight ASTM ash fusion temperatures and the four major ash elements as oxides (determined by ICP-AES). The program uses PLSl models, in which only one variable at a time is modeled. Cross-validation was used to select the optimum number of factors in the model. In this technique, a subset of the data (in this case five spectra) is omitted from the calibration, but predictions are made for it. The sum-of-squares residuals are computed from those samples left out. A new subset is then omitted, the first set is included in the new calibration, and additional residual errors are tallied. This process is repeated until predictions have been made and the errors summed for all 50 samples (in this case, 10 calibrations are made). This entire set of... [Pg.55]

E.xample problems are included to highlight the need to estimate the entire set of products that can be reached for a given feed when using a particular type of separation unit. We show that readily computed distillation curves and pinch point cur es allow us to identify the entire reachable region for simple and e.xtractive distillation for ternary mixtures. This analysis proves that finite reflux often permits increased separation we can compute exactly how far we can cross so-called distillation boundaries. For extractive distillation, we illustrate how to find minimum. solvent rates, minimum reflux ratios, and, interestingly, ma.xinnim reflux ratios. [Pg.64]

If the feed is Fi, a point lying between D and P, then the pinch curve through D lies entirely to one side of the point F and curves back to cross at P. The corresponding distillation curve lies even farther away to the same side (the pinch point curve turns more sharply than the distillation curve). The reachable region for D excludes all points between D and P. Thus the points between F and P are unreachable by the top part of the column. As D could move to be coincident with F, points beyond F are not excluded. [Pg.147]

The phase behavior of a pure substance may be depicted schematically on a pressure-temperature diagram as shown in Figure 1.1. The curve OC, the vapor pressure curve, separates the vapor and liquid phases. At any point on this curve, the two phases can coexist at equilibrium, both phases having the same temperature and pressure. Phase transition takes place as the curve is crossed along any path. Figure 1.1 shows two possible paths at constant pressure (path AB) and at constant temperature (path DE). At the critical point, C, the properties of the two phases are indistinguishable and no phase transition takes place. In the entire region above the critical temperature or above the critical pressure, only one phase can exist. [Pg.11]


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