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Phase I—Safety study, 10-100 subjects, open label... [Pg.204]

Subject Open Enrollment for Medical and Dental Insurance... [Pg.239]

Figure 6.4. Scatter diagram of the results of two groups of subjects (open and filled spheres) in a three-dimensional measurement space. The groups differ in location. The difference between the groups can be fully described only by considering all three variables simultaneously. Figure 6.4. Scatter diagram of the results of two groups of subjects (open and filled spheres) in a three-dimensional measurement space. The groups differ in location. The difference between the groups can be fully described only by considering all three variables simultaneously.
FIGURE 47.2 A trajectory plot showing the direction of change of a safety biomarker for individual subjects. Open circles represent the basehne safety biomarker values, filled triangles are the safety biomarker values at end of treatment, and the dotted fines show the trends from baseline values of the safety biomarker. [Pg.1180]

Fig. 2. Dose-response effects of insulin on glucose disposal (Rd) and HGP in T2D patients with fasting hyperinsuh-naemia (closed symbols) and in age- and weight-matched control subjects (open symbols). p < 0.05 [9]. Fig. 2. Dose-response effects of insulin on glucose disposal (Rd) and HGP in T2D patients with fasting hyperinsuh-naemia (closed symbols) and in age- and weight-matched control subjects (open symbols). p < 0.05 [9].
The activation of TLC plates is a subject open to dispute. Hahn-Deinstrop (1993) recommends heating silica gel and alumina layers at 120°C for 30 min... [Pg.26]

For a long time, the wheels were mainly tested with dye penetration. This test procedure can make defects which are open to the surface of the material visible for the tester. It is, however, common knowledge that the test results vary greatly depending on the subjective view of the individual tester. [Pg.306]

The ultrasonic array characterization purpose is a current subject of interest for presumably many UT teams. We hope that this paper will open a discussion, leading to a new standard. [Pg.826]

With tlie development of femtosecond laser teclmology it has become possible to observe in resonance energy transfer some apparent manifestations of tire coupling between nuclear and electronic motions. For example in photosyntlietic preparations such as light-harvesting antennae and reaction centres [32, 46, 47 and 49] such observations are believed to result eitlier from oscillations between tire coupled excitonic levels of dimers (generally multimers), or tire nuclear motions of tire cliromophores. This is a subject tliat is still very much open to debate, and for extensive discussion we refer tire reader for example to [46, 47, 50, 51 and 55]. A simplified view of tire subject can nonetlieless be obtained from tire following semiclassical picture. [Pg.3027]

Another example of the role played by a nonradiative relaxation pathway is found in the photochemistry of octatetraene. Here, the fluorescence lifetime is found to decrease dramatically with increasing temperature [175]. This can be assigned to the opening up of an efficient nonradiative pathway back to the ground state [6]. In recent years, nonradiative relaxation pathways have been frequently implicated in organic photochemistry, and a number of articles published on this subject [4-8]. [Pg.276]

The book opens with a chapter on the theory underlying the technique of the chief operations of practical organic chemistry it is considered that a proper understanding of these operations cannot be achieved without a knowledge of the appropriate theoretical principles. Chapter II is devoted to a detailed discussion of experimental technique the inclusion of this subject in one chapter leads to economy of space, par ticularly in the description of advanced preparations. It is not expected that the student will employ even the major proportion of the operations described, but a knowledge of their existence is thought desirable for the advanced student so that he may apply them when occasion demands. [Pg.1193]

When a sound wave comes in contact with a soHd stmcture, such as a wall between two spaces, some of the sound energy is transmitted from the vibrating air particles into the stmcture causing it to vibrate. The vibrating stmcture, in turn, transmits some of its vibrational energy into the air particles immediately adjacent on the opposite side, thereby radiating sound to the adjacent space. For an incomplete barrier, such as a fence or open-plan office screen, sound also diffracts over the top and around the ends of the barrier. The subject of this section is confined to complete barriers that provide complete physical separation of two adjacent spaces. Procedures for estimating the acoustical performance of partial barriers can be found in References 5 and 7. [Pg.315]


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