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Thesis - Instituto de Telecomunicações

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70 CHAPTER 4. SIGNAL PROCESSING AND FEATURE EXTRACTION4.2.2 Electro<strong>de</strong>rmal Mo<strong>de</strong>lsVisual Event Detection The initial methods used by the researchers for the interpretationof the EDA signal were based on visual <strong>de</strong>tection of skin conductance responses, withthe observer manually annotating the time instants of the start of the events.In [98] the authors apply a preprocessing step prior to visual inspection, normalizing thesignal according to the recommendations of the EDA committee [72] and then smoothingthe speed of change, i.e., the second or<strong>de</strong>r <strong>de</strong>rivative, to reduce signal noise. After thisprocessing step, the extracted information shows the existence of an event after a particularstimulus.The sympathetic skin response signal is also evaluated following a qualitative mo<strong>de</strong>l in[134, 233]. The signal is visually scanned to find SCR events; these events are classified asp-waves, if the first peak of the wave is positive, or as n-waves, if it is negative.Visual-based SCR event <strong>de</strong>tection, that we call the qualitative approach, is strongly conditionedby the experience of the human scorer, and the mo<strong>de</strong>ling problems listed above aredifficult to solve via visual inspection. Furthermore, the signal obtained in the sympatheticskin response has the peaks and valleys substantially altered by the filtering procedure andas such, different conclusions can be reached by using different filtering conditions in thepre-processing step. Therefore, without a common well-<strong>de</strong>fined filtering setup, no reliableconclusions can be obtained. There is also no physiologic basis for the separation betweenthe two types of waves referred to above.Simple Mo<strong>de</strong>l The first computational mo<strong>de</strong>l applied to the EDA signal was based onthe i<strong>de</strong>ntification of the valleys and peaks of the signal [25, 211]. The mo<strong>de</strong>l assumes theexistence of two zones in a SCR: a <strong>de</strong>creasing part before t α , the activation instant, and acrescent zone between t α and t β (the maximum instant). The i<strong>de</strong>ntification of these zones,and of these transition instants, is based on the computation of signal <strong>de</strong>rivatives andcorresponding zero crossings, as summarized in expressions 4.16 to 4.20, that are processedin sequence. The pre-event zone (t < t α ) is characterized by negative first <strong>de</strong>rivative values(equation 4.16). The activation instant (t α ) corresponds to a null signal first or<strong>de</strong>r <strong>de</strong>rivativeand positive second or<strong>de</strong>r <strong>de</strong>rivative (eq. 4.17). Along the rise zone, that occurs betweent α and t β - the local maximum amplitu<strong>de</strong> instant, the signal first <strong>de</strong>rivative is positive

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