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Fractional Calculus - Gauge-institute.org

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GAUGE-INSTITUTE<strong>Gauge</strong> Institute Journal<strong>Fractional</strong> <strong>Calculus</strong>The Fundamental Theorem of the <strong>Fractional</strong> <strong>Calculus</strong>, andthe Meaning of <strong>Fractional</strong> DerivativesH. Vic DannonAbstract: Since the beginning of the 18 th century, attempts weremade to generalize the Arithmetic Means Derivative, and obtain aGeneralized Arithmetic Means <strong>Calculus</strong>.As early as 1812, Lacroix [Lac] observed that for n = 1... m,nd m m! m−nΓ ( m + 1) m−nx = x =x ,ndx ( m −n)! Γ( m − n + 1)and by formal substitution ofn =12, obtained [Ross]1/2dΓ (1 + 1) 1−1/21x = x =( dx) Γ(1 − + 1) π /21/2 12x.In 1832, Liouville [Liou] used the Euler Gamma Integral formulau=∞−aa−1−xuΓ () ax = ∫ u e duu=0Differentiating both sides to an order ν , he obtained


Assuminghe hadνu=∞ν−aa−1d −νdxu=0dΓ () a x = u e( dx )ν ∫ ( )dνν( dx)νe−xuν−xu= ( −u)e , (3)u=∞d − a ν a+ ν−1Γ () a x = ( −1)u eν ∫( dx)u=0ν= ( −1) Γ ( a + ν)x− +xu du.− xu du( a ν ) ,and concluded [Ross] thatdνν( dx)x−aν= ( −1)Γ ( a + ν)xΓ()a−( a+ν)Many years later, the meaning of <strong>Fractional</strong> Derivatives is stillunclear.The common perception is that the <strong>Fractional</strong> Derivative Methodrepresents a new kind of <strong>Calculus</strong>, such as the Product <strong>Calculus</strong>,that is based on the Geometric Mean [Dan1],But so far, the <strong>Fractional</strong> Derivative Method has been developedonly as a refinement of the Arithmetic Means <strong>Calculus</strong>, and is nota new kind of <strong>Calculus</strong>, such as the Product <strong>Calculus</strong> is.Here, We interpret the <strong>Fractional</strong> Derivative in the context of theArithmetic Means <strong>Calculus</strong> in which it was presented.We notethat it can be similarly developed, and interpreted in the Product<strong>Calculus</strong>.


We proceed with the simplest fraction q =1. The <strong>Fractional</strong>integral2and the derivative−12f−1D212d≡ f ,−( dx)12 121df( dx) 2≡ Df.

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