Recordings from auditory-nerve fibers in the anesthetized frog revealed that addition of broadband noise results in a reduction in the ability of a fiber to phase lock to a continuous pure tone. In particular, our results suggest that: (i) there is a threshold below which masking noise has little or no effect on vector strength (VS); then with increasing masking noise level, VS appears to decrease monotonically for all test frequencies (TFs); (ii) there exist subpopulations of auditory-nerve fibers in the frog for which the deterioration of phase locking to tones in wideband noise depends critically on the relationship of the TF to the fiber's CF. Specifically, in one subpopulation (43% of the fibers studied), the rate of VS decrease with increasing levels of masking noise is greater for CF tones than it is for TFs greater than CF. The net result is a "crossing" of the VS versus masking noise functions (e.g., Fig. 6); (iii) there exists a small subpopulation of amphibian papillar (a.p.) fibers for which the rate of VS decrease with increasing levels of masking noise is less for TFs less than CF than it is for CF tones (e.g., Fig. 5); (iv) there is a pronounced noise-induced phase lead for TFs greater than CF, whereas, for stimulus tones at or below CF, the preferred firing phase is nearly noise-level independent; (v) the remainder of the sample consists of fibers in which the VS-falloff rates appear to be test-frequency independent; (vi) addition of wideband masking noise to a CF tone, and increasing the CF-tone level in the absence of noise, produced (qualitatively) similar effects on the preferred firing phase of auditory-nerve fibers (e.g., Figs. 1 and 7). Thus amphibian auditory-nerve fibers appear to be energy detectors, i.e., exhibit phase shifts corresponding to the total energy within the filter passband defined by the frequency-threshold curve.
The decay kinetics of Cl−2, produced by photolysis of chloride ions, has been studied using a flash photolysis technique with conductometric detection. Flash photolysis of Cl− ions in acid solutions eventually yields H2O2, Cl2, HClO and H2. A mechanism is proposed (Fig. 6) consistent with the experimental observations.
Because there is no simple, general method for measuring solubilities of nonvolatile solutes in a polymer, this work presents a thermodynamic framework for estimating such solubilities from infinite‐dilution distribution‐coefficient data for aqueous solutions of the solute in equilibrium with the polymer. The experimental infinite‐dilution distribution coefficient is related to that calculated from a molecular‐thermodynamic model (Flory–Huggins). The three binary Flory parameters are obtained from water–solute and water–polymer data, and from the solute's distribution coefficient. Solubilities of 19 nonvolatile aromatic solutes were estimated in three polymers: ethyl‐vinyl acetate copolymer (EVAc) with 33 (EVAc33), 45 (EVAc45) wt. % vinyl acetate content, and poly(vinyl acetate) (PVAc) at 25°C, where most of the solutes are solids. For some of these systems, predicted solubilities are compared with new experimental results. The calculations reported here may be useful for various applications, including the design of membrane processes or drug‐delivery systems, and for packaging technology for foods, chemicals, and pharmaceuticals.
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