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Column B : Measured turn rates as a function of calculated filter output.
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The plot of Papp vs. calculated Log Poctanol (Fig. 8) showed that compounds predicted to move by passive permeation either paracellularly or transcellularly (sucrose, naloxone, propranolol, diazepam) had Papp that was a linear function of calculated Log Poctanol, with R=0.96.
Lines represent calculated values after Eq. (12) with the data in Figs. 8 and 9. b Electric losses as a function of frequency calculated after AC-conductivity through DNA molecule for different temperature humps (H2).
Lines represent calculated values after Eq. (2) with the data in Figs. 8 and 9. e Electric losses as a function of frequency calculated after AC-conductivity through DNA molecule for different temperature humps (H5).
Lines represent calculated values after Eq. (12) with the data in Figs. 8 and 9. d Electric losses as a function of frequency calculated after AC-conductivity through DNA molecule for different temperature humps (H4).
Lines represent calculated values after Eq. (12) with the data in Figs. 8 and 9. c Electric losses as a function of frequency calculated after AC-conductivity through DNA molecule for different temperature humps (H3).
One can better see the effect of frequency on H1 at lower frequencies in next figure Fig. 17 a Electric losses as a function of frequency calculated after AC-conductivity through DNA molecule for different temperature humps (H1).
Fig. 5. Extinction curves (extinction per hydrogen nucleus as a function of wavelength) calculated for Models A D (upper panel).
Figure 7 shows the gradient f of −U dissipation (or U total) as a function of a calculated by Eq. (12).
a Moment rate ({dot{m}}_{mathrm{s}}) (solid) as a function of time, calculated according to (106), compared with the observed moment rate (dashed) reported by Wei et al.
Figure 4 shows the linewidth of the exciton transition as a function of temperature calculated from Lorentzian fits to the exciton peak.
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