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Thesis - Instituto de Telecomunicações

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4.2. ELECTRODERMAL ACTIVITY 75the process based on linear systems theory [97]. Taking the SCR signal as the impulsiveresponse of a system with transfer function H(s), with the impulsive input representing thetriggering stimulus of the SCR (see figure 4.5), we tried to i<strong>de</strong>ntify the transfer functionthat would provi<strong>de</strong> the <strong>de</strong>sired observed SCR behavior. Given that SC ′ = 0 at t o , andtaking, for simplicity, t o = 0, a single pole mo<strong>de</strong>l, with multiplicity n higher than one,seemed plausible. We therefore looked for transfer functions of the formH(s) =α(s + b) n . (4.27)Figure 4.5: Proposed SCR mo<strong>de</strong>l.With this mo<strong>de</strong>l we assume that the overlapping of EDA events is a linear operation,and that SCL is a constant ad<strong>de</strong>d to the signal. In the next sections we <strong>de</strong>rive the completemo<strong>de</strong>l, and also provi<strong>de</strong> the mechanism to use this isolated mo<strong>de</strong>l to find overlapping eventsand compute the tonic level (SCL) of the entire signal with multiple SCR events.EDA Mo<strong>de</strong>lAccording to our proposal, an isolated SCR is mo<strong>de</strong>led as the output of a linear systemwith transfer function H(s) given by equation 4.27, to an impulsive-type input, representingthe triggering stimulus of the SCR. The i<strong>de</strong>ntification of the mo<strong>de</strong>l or<strong>de</strong>r, n, is based onmatching the corresponding impulsive response h(t), given by the inverse Laplace transform( )h(t) =L −1 α(s + b) n= αtn−1 e −bt(n − 1)! u(t) =atk e −bt u(t) =f(t)u(t), (4.28)with the observed morphological signal features, <strong>de</strong>tailed in the previous section, inparticular the evenly spaced temporal marks t o to t 4 . In the previous equation, u(t) refersto the unitary step function (presented in equation 4.22), k = n − 1 and a = α k! .

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