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Complementary phase

All the above results, which are true but not desired, can be avoided by using a complementary phase increment... [Pg.15]

Table 1. Comparison between the results by two PIPs, one with a phase increment of A(p = 234 and the other with a complementary phase increment of Atp= —126°. For both PIPs, the time increment Ar = 50 is and RF field strength f = 1.235 kHz. The phase includes a UPS = — (Ay>/2) and a 180° if Xn < 0... Table 1. Comparison between the results by two PIPs, one with a phase increment of A(p = 234 and the other with a complementary phase increment of Atp= —126°. For both PIPs, the time increment Ar = 50 is and RF field strength f = 1.235 kHz. The phase includes a UPS = — (Ay>/2) and a 180° if Xn < 0...
In the early days of sleep research, sleep and wakefulness were considered as entirely separate entities and were studied in isolation from one another. All-night sleep was examined in its entirety and minutely dissected with total disregard for either the prior or following hours of wakefulness. Sleep researchers later began to consider these two complementary phases of the daily cycle of existence as mutually interactive. The most obvious interaction between sleep and wakefulness, other than their sequential occurrence in each succeeding 24-hr period, is the predictable fluctuation in daytime alertness as a function of the amount of nocturnal sleep. In other words, the more we sleep, the more we are alert and the less we sleep, the more we are sleepy in the daytime. [Pg.556]

Uziely B, Jeffers S, Isacson R, Kutsch K, Wei-Tsao D, Yehoshua Z, Libson E, Muggia EM, Gabizon A. Liposomal doxorubicin antitumor activity and unique toxi-cities during two complementary phase I studies. J Clin Oncol 1995 13(7) 1777-85. [Pg.259]

The Del matrix destroys the coherence created by E and the resultant 7(r) is r-independent. In contrast, as shown below, the D+ and D matrices preserve the coherences created by E, and the resultant I t) signals are r dependent. D+, the structure of which resembles that of E, produces a phased up signal that has maximum intensity at r = 0. In contrast, D produces a complementary, phased out minimum intensity signal at r = 0. For D, ... [Pg.641]

Uziely, B., Jeffers, S., Isacson, R., Kutsch, K., Wei-Tsao, D., Yehoshua, Z., Libson, E., Muggia, F. M. and Gabizon, A., Liposomal doxorubicin, antitumoiu- activity and unique toxicities during two complementary phase I studies, J. Clin. Oncol, 13,1777,1995. [Pg.253]

Habgood, M., Deij, M. A., Mazurek, J., Price, S. L., and ter Horst, J. H. 2010. Carbamazepine co-crystallization with pyridine carboxamides Rationalization by complementary phase diagrams and crystal energy landscapes. Cryst. Growth Des. 10 903. [Pg.183]

In addition to the CB-DM, the literature has cited the P-hydroxypropylated cyclodextrin (in the racemic form of hydroxypropyl) (CB-RSP) as the best complementary phase for this type of mechanism where steric bulk as well as hydrogen bonding can play a role in enantioseparation for any fused ring structure. The third most cited phase in this area is the P-acetylated cyclodextrin (CB-AC). More detailed description of these later two phases is given below. [Pg.64]

In a first phase, the diagram for processing oil fractions features the addition of complementary units that enable the production of unleaded gasoline such as ... [Pg.408]

As a final point, it should again be emphasized that many of the quantities that are measured experimentally, such as relaxation rates, coherences and time-dependent spectral features, are complementary to the thennal rate constant. Their infomiation content in temis of the underlying microscopic interactions may only be indirectly related to the value of the rate constant. A better theoretical link is clearly needed between experimentally measured properties and the connnon set of microscopic interactions, if any, that also affect the more traditional solution phase chemical kinetics. [Pg.891]

The dangling bonds of a Si surface abstract one F atom from an incident F2 molecule while the complementary F atom is scattered back into the gas phase [20]. This abstractive mechanism leads to F adsorjDtion at single sites rather than at adjacent pairs of sites, as observed directly by scanning tunnelling microscopy [21]. Br atoms adsorb only to Ga atoms in the second layer of GaAs(001)-(2 x 4) where empty dangling bonds on the Ga atoms can be filled by electrons from the Br atoms [22]. [Pg.2930]

Bubble columns in series have been used to establish the same effective mix of plug-flow and back-mixing behavior required for Hquid-phase oxidation of cyclohexane, as obtained with staged reactors in series. WeU-mixed behavior has been established with both Hquid and air recycle. The choice of one bubble column reactor was motivated by the need to minimize sticky by-products that accumulated on the walls (93). Here, high air rate also increased conversion by eliminating reaction water from the reactor, thus illustrating that the choice of a reactor system need not always be based on compromise, and solutions to production and maintenance problems are complementary. Unlike the Hquid in most bubble columns, Hquid in this reactor was intentionally weU mixed. [Pg.524]

Liquid chromatography is complementary to gas chromatography because samples that cannot be easily handled in the gas phase, such as nonvolatile compounds or thermally unstable ones, eg, many natural products, pharmaceuticals, and biomacromolecules, are separable by partitioning between a Hquid mobile phase and a stationary phase, often at ambient temperature. Developments in the technology of Ic have led to many separations, done by gc in the past, to be carried out by Hquid chromatography. [Pg.109]

Other excellent methods of phase identification include TEM and electron diffraction. These may be more useful for low-Z materials, ultrathin films, and for characterizing small areas, including individual grains. For multiphase films with incomplete texture, these methods and XRD are complementary, since in commonly used geometries, they probe atomic planes perpendicular and parallel to the thin film surface, respectively. [Pg.206]

The distribution coefficient is an equilibrium constant and, therefore, is subject to the usual thermodynamic treatment of equilibrium systems. By expressing the distribution coefficient in terms of the standard free energy of solute exchange between the phases, the nature of the distribution can be understood and the influence of temperature on the coefficient revealed. However, the distribution of a solute between two phases can also be considered at the molecular level. It is clear that if a solute is distributed more extensively in one phase than the other, then the interactive forces that occur between the solute molecules and the molecules of that phase will be greater than the complementary forces between the solute molecules and those of the other phase. Thus, distribution can be considered to be as a result of differential molecular forces and the magnitude and nature of those intermolecular forces will determine the magnitude of the respective distribution coefficients. Both these explanations of solute distribution will be considered in this chapter, but the classical thermodynamic explanation of distribution will be treated first. [Pg.47]

The final section of the volume contains three complementary review articles on carbon nanoparticles. The first by Y. Saito reviews the state of knowledge about carbon cages encapsulating metal and carbide phases. The structure of onion-like graphite particles, the spherical analog of the cylindrical carbon nanotubes, is reviewed by D. Ugarte, the dominant researcher in this area. The volume concludes with a review of metal-coated fullerenes by T. P. Martin and co-workers, who pioneered studies on this topic. [Pg.193]

FIGURE 12.19 Steps in the thermal denaturation and renaturation ofDNA. The nucle-ation phase of the reaction is a second-order process depending on sequence alignment of the two strands. This process takes place slowly because it takes time for complementary sequences to encounter one another in solution and then align themselves in register. Once the sequences are aligned, the strands zipper up quickly. [Pg.373]

This technique provides quantitative information about tautomeric equilibria in the gas phase. The results are often complementary to those obtained by mass spectrometry (Section VII,E). In principle, gas-phase proton affinities, as determined by ICR, should provide quantitative data on tautomeric equilibria. The problem is the need to correct the measured values for the model compounds, generally methyl derivatives, by the so-called N-, 0-, or S-methylation effect. Since the difference in stability between tautomers is generally not too large (otherwise determination of the most stable tautomer is trivial) and since the methylation effects are difficult to calculate, the result is that proton affinity measurements allow only semi-quantitative estimates of individual tautomer stabilities. This is a problem similar to but more severe than that encountered in the method using solution basicities (76AHCS1, p. 20). [Pg.52]

The principle of 2-D TLC separation is illustrated schematically in Figure 8.4. The multiplicative law for 2-D peak capacity emphasizes the tremendous increase in resolving power which can be achieved in theory, this method has a separating capacity of n, where n is the one-dimensional peak capacity (9). If this peak capacity is to be achieved, the selectivity of the mobile phases used in the two different directions must be complementary. [Pg.174]


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See also in sourсe #XX -- [ Pg.64 ]




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