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Oscillations, Waves, and Interactions - GWDG

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356 R. Pottel, J. Haller <strong>and</strong> U. Kaatze<br />

Figure 21. Ultrasonic excess absorption spectrum for a solution of 0.8 mol/l ZnCl2 in water<br />

at 25 ◦ C. The subdivision of the spectrum into three Debye relaxation terms is indicated by<br />

dashed lines. The full line represents the sum of these terms [30].<br />

louin scattering study of zinc chloride hydrated melts [97]. Three terms with discrete<br />

relaxation time are necessary to represent the experimental spectra adequately<br />

(Fig. 21). Consistency of the dependencies of relaxation parameters upon the salt<br />

concentration, however, requires even four Debye relaxation terms.<br />

As a four-Debye-term model comprises too many unknown parameters the spectra<br />

have been evaluated assuming a reduced reaction scheme<br />

Zn 2+ + 4Cl − ⇀↽ (Zn 2+ ) ∗ + 4Cl − ⇀↽ (ZnCl) + + 3Cl −<br />

⇀↽ ZnCl2 + 2Cl − ⇀↽ (ZnCl3) − + Cl −<br />

⇀↽ (ZnCl4) 2−<br />

in which (Zn 2+ ) ∗ is assumed an activated zinc ion, e.g. an ion with one hydration<br />

molecule less than Zn 2+ . Relating the rate constants <strong>and</strong> reaction volumes of the<br />

coupled equilibrium to one another the number of unknown parameters in the regression<br />

analysis of the ultrasonic spectra has been reduced so that reliable rate constants<br />

<strong>and</strong> reaction volumes followed from the fitting procedures [30].<br />

Alternatively, the multitude of proposed ion complex structures (Fig. 19) <strong>and</strong> the<br />

finding of precritical behaviour for concentrated zinc chloride aqueous solutions [98]<br />

has suggested the idea of rapidly fluctuating diffuse ion clusters rather than of stoichiometrically<br />

defined species [31]. The Romanov-Solov’ev model of noncritical concentration<br />

fluctuations [99–101] has been implemented. But, even if an additional<br />

Debye relaxation is taken into account, this model did not satisfactorily apply to the<br />

spectra at all concentrations. However, a superior analytical description of the experimental<br />

excess absorption spectra is reached with the Dissado-Hill (“DH”) relaxation<br />

spectral function with only four unknown parameters (Fig. 22). This function has<br />

been originally derived for a uniform representation of a diversity of dielectric spec-<br />

(20)

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