Page 98 - Mathematical Techniques of Fractional Order Systems
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86  Mathematical Techniques of Fractional Order Systems


            Remark 2: As explained in detail in Casagrande et al. (2017), the introduc-
            tion of the auxiliary term is necessary to make the number of unknowns in
                                                            a
            (3.22) equal to the number of equations. If the poles of Y ðwÞ are fixed, this
                                                           Σ
                                              a
            result is obtained when the orders of Y ðwÞ and UðsÞ are equal, i.e., the
                                              Σ
                                        a
            degree of the denominator of Y ðwÞ coincides with the degree n u of the
                                        Σ
            denominator of UðwÞ. The solution is then obtained by equating the coeffi-
                                                                   r
            cients of the equal powers of w at the numerators of the product W ðwÞUðwÞ
                           ν
                                   a
            and of Y U ðwÞ 1 Y ðwÞ 1 Y ðwÞ, respectively. The problem turns out to be
                                  Σ
                           Σ
            linear.
                                    a
            Remark 3: If the poles of Y ðwÞ are located far to the left of the imaginary
                                    Σ
            axis, this additional term does not alter appreciably the transient dynamics
            of the system while it leaves unchanged the input component.
            Remark 4: Due to the introduction of the auxiliary term, the order r of
                                                        ν
              r
            W ðwÞ is greater than the order ν of the function Y ðwÞ approximating the
                                                        Σ
            original system component Y Σ ðwÞ. However, since usually ν{n, the order
            r 5 ν 1 n u is still much smaller than n for the canonical inputs (n u # 2 for
            steps, ramps and sinusoids).
               Procedure 3.5.1 is schematically represented in Fig. 3.3. It has been
            applied to several benchmark examples with considerable success; three of
            them are illustrated in the next section.


























            FIGURE 3.3 Basic flow chart of Procedure 3.5.1.
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