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Hoy’s system

TABLE 7.11 The equations to be used in Hoy s system (1985) for estimation of the solubility parameter and its components. See text for significance of symbols ... [Pg.217]

TABLE 7.12 Values of increments in Hoy s System (1985), for the molar attraction function ... [Pg.220]

Hoy s system for estimation of the solubility parameter and its components, 217 Huggins... [Pg.995]

Solubility Parameter I Component Group Contributions Solubility Parameter IP Component Group Contributions Eguatlons to be Used for Hoy s System... [Pg.2151]

In this work we have attempted to model the available experimental data for CaO Cu2+ using a variety of parameter sets taken from the literature. We conclude that only O Brien s multimode model [7], for which hw 216 cm 1 and jX/hoy 8, can satisfactorily account for all the data. These systems are particularly attractive to both the theoretician and experimentalist fascinated by Jahn-Teller funny business in that the states pertaining to j = 1/2 and 3/2 span just a few wave numbers. We have demonstrated how a number of modem physical techniques can be employed to elucidate further the low-lying vibronic structure. In particular it should be possible to obtain a direct measure of the tunnelling splitting from a high-held, high-frequency EPR experiment. [Pg.479]

Glick, R. Hoying, J. Cerullo, L. Perlman, S. Phenylpropa- 64. nolamine an over the counter drug causing central nervous system vasculitis and intra cerebral Hemorrhage. Case reports and review. Neurosurgery 1987, 20, 969-974. [Pg.2430]

Figure 7. Volume data jor systems with t < 22 s plotted according to Hoy-land s diffusion equation [10],... Figure 7. Volume data jor systems with t < 22 s plotted according to Hoy-land s diffusion equation [10],...

See other pages where Hoy’s system is mentioned: [Pg.217]    [Pg.2163]    [Pg.2163]    [Pg.217]    [Pg.2163]    [Pg.2163]    [Pg.610]    [Pg.212]    [Pg.200]    [Pg.432]    [Pg.464]    [Pg.730]    [Pg.136]    [Pg.142]    [Pg.628]   
See also in sourсe #XX -- [ Pg.687 , Pg.688 ]




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