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Oscillations, Waves, and Interactions - GWDG

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374 U. Kaatze <strong>and</strong> R. Behrends<br />

Figure 5. Sonic excess attenuation spectra for aqueous solutions of D-fructose at 25 ◦ C [44].<br />

The saccharide concentrations are △, 0.5 mol/l; �, 0.7 mol/l; ◦, 1 mol/l; ⋄, 1.5 mol/l. The<br />

lines represent a relaxation spectral function with three Debye-type relaxation terms <strong>and</strong><br />

with parameter values from a nonlinear fitting procedure.<br />

Basically ourdays principles of measurement are the same as in early acoustical relaxation<br />

studies [43]. More sophisticated liquid spectrometry is enabled by a higher<br />

precision of the cell constructions, by advanced electronics, <strong>and</strong> by computer controlled<br />

measuring routines. Mechanical stability offers a 10 nm resolution in the cell<br />

length, which is m<strong>and</strong>atory for measurements in the GHz region where the wavelength<br />

is on the order of 300 nm <strong>and</strong> where the extraordinary large attenuation coefficient<br />

allows for small variations in the sample length only [42]. Modern electronics enable<br />

progressive measurement routines, scanning the complete transfer function of resonators<br />

to properly consider effects from higher order modes <strong>and</strong> running routinely<br />

calibrations in the variable-path-length method. Automatic measuring procedures<br />

finally facilitate multiple measurements for the reduction of statistical errors. Examples<br />

of broadb<strong>and</strong> attenuation spectra are shown in Fig. 5.<br />

2.3 Sound velocity dispersion<br />

According to the Kramers-Kronig relations acoustical attenuation originating from<br />

relaxation processes is associated with a dispersion in the sound velocity c, which<br />

could be also utilized for liquid spectrometry. Normally, however, the dispersion in<br />

c is small <strong>and</strong> it is notoriously difficult to reach, in a significant frequency range, a<br />

sufficiently high accuracy in the sound velocity measurements. But since the sound<br />

velocity follows as a byproduct from the attenuation coefficient spectrometry, it can<br />

be used to consider the dispersion corresponding with large sonic absorption. Figure 6<br />

shows the dispersion in c that is related to the formation of ion complexes in an<br />

aqueous solution of zinc chloride [45]. The total dispersion step of that system<br />

amounts to c(∞) − c(0) = 0.01 · c(0) which should not be neglected in the evaluation<br />

procedures.

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