on the localisation in the superimposed soundfield - Hauptmikrofon ...
on the localisation in the superimposed soundfield - Hauptmikrofon ...
on the localisation in the superimposed soundfield - Hauptmikrofon ...
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
14<br />
3. It has to be ruled out that <strong>the</strong> suppressi<strong>on</strong> of sound colourati<strong>on</strong> can be expla<strong>in</strong>ed by<br />
means of some k<strong>in</strong>d of an averag<strong>in</strong>g process that <strong>the</strong> hear<strong>in</strong>g system carries out <strong>on</strong><br />
<strong>the</strong> spectra result<strong>in</strong>g at <strong>the</strong> left and right ears. Figure 5 shows <strong>the</strong> mean values of<br />
<strong>the</strong>se spectra. The resultant fluctuati<strong>on</strong>s <strong>in</strong> <strong>the</strong> amplitude spectrum would be clearly<br />
detectable.<br />
4. In <strong>the</strong> case of time-based stereoph<strong>on</strong>y, <strong>the</strong> ear signals’ spectral characteristics are<br />
very different from <strong>the</strong> <strong>on</strong>es of a real sound source that, like <strong>the</strong> phantom source,<br />
moves between 0° and 30°. This is evident from compar<strong>in</strong>g <strong>the</strong> measurements<br />
shown <strong>in</strong> Figure 6. This figure displays <strong>the</strong> spectral modificati<strong>on</strong>s that result if<br />
Loudspeaker B is moved from Ω B = 30° to <strong>the</strong> centre, Ω B = 0°. As <strong>the</strong> listen<strong>in</strong>g test<br />
to be reported <strong>in</strong> Secti<strong>on</strong> 2.2.2 will show, <strong>the</strong>se deviati<strong>on</strong>s cause perceivable sound<br />
colourati<strong>on</strong> <strong>in</strong> <strong>the</strong> case of m<strong>on</strong>aural listen<strong>in</strong>g.<br />
left ear<br />
right ear<br />
Figure 6:<br />
Changes <strong>in</strong> <strong>the</strong> ear signals’ spectra as a functi<strong>on</strong> of <strong>the</strong> angle of <strong>in</strong>cidence<br />
Ω B , relative to Ω B = 30°.<br />
5. As for <strong>the</strong> distance and elevati<strong>on</strong> of <strong>the</strong> phantom source, <strong>on</strong>e can see from Figure 4<br />
that <strong>the</strong> auditory system has to <strong>in</strong>terpret <strong>the</strong> signals as be<strong>in</strong>g “l<strong>in</strong>early distorted”,<br />
because no real sound source can produce such <strong>in</strong>teraural spectral differences. The