Page 663 - Mathematical Techniques of Fractional Order Systems
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634  Mathematical Techniques of Fractional Order Systems


            21.3.1.2 Definition of Riemann Liouville
            The derivative in the sense of Riemann Liouville is based on the first primi-
            tive or integral of a function f(t), is defined as Eq. (21.5):

                                       1    d  n  ð t  fðνÞ
                              p
                           α D fðtÞ 5        n       p2n11 dν         ð21:5Þ
                              t
                                    Γðn 2 pÞ dt  α ðt2νÞ
            where Γ(.) the Euler’s Gamma function is defined for all nA@ and pA[n-1,
            n[ as:
                                         ð 1N
                                   Γ nðÞ 5   t n21 2t                 ð21:6Þ
                                                 e dt
                                           0

            21.3.1.3 Definition of Caputo
            The definition of the fractional derivative of f(t) in the sense of Caputo incor-
            porates the initial conditions of the function to be treated, as well as its inte-
            ger derivatives, the derivative of a function f(t) in the Caputo sense is
            defined by the following relation (21.7):
                                                   n
                                              t
                                                  d fðνÞ
                                        1
                                             ð
                             c  p                  dt n  dν
                             α D fðtÞ 5             p2n11             ð21:7Þ
                               t
                                     Γðp 2 nÞ  α ðt2νÞ
            where Γ(.) the Gamma function, n is the smallest integer larger than the frac-
            tional order p and pA]0, 1].
            21.3.2 The n-Dimensional Fractional Order Chaotic System
            The n-dimensional fractional order chaotic system is defined as following
            relation (21.8):
                                      P
                                   α D X t 5 fðX t ; X 0 ; ΘÞ         ð21:8Þ
                                      t
                                       n
                                   0
            where X t 5 ðx 1t ; x 2t ; ...; x nt Þ Aℜ is the n-dimensional state vector of the
            original system; X 0 is the initial state of the system, P 5 ðp 1 ; p 2 ; ...; p n Þ Aℜ n
                                                                       0
            is a set of fractional order of the original system verifying that for all i 5 1,
                                  n
            2,..., n 0 , p i # 1, f: ℜ -ℜ n  is the linear or nonlinear function and
                                m
            Θ 5 ðθ 1 ; θ 2 ; ...; θ m Þ Aℜ is the n-dimensional vector value of original sys-
                            0
            tem parameters.
            21.3.3 The General Numerical Solution of the Fractional
            Differential Equation and Stability
            A remarkable property that distinguishes a fractional order derivation from an
            integer derivation is that a noninteger derivation assumes a global character in
            contrast to an integer derivation. It turns out that the fractional order derivative
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