Fractal derivative

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In applied mathematics and mathematical analysis, the fractal derivative or Hausdorff derivative is a non-Newtonian generalization of the derivative dealing with the measurement of fractals, defined in fractal geometry. Fractal derivatives were created for the study of anomalous diffusion, by which traditional approaches fail to factor in the fractal nature of the media. A fractal measure t is scaled according to t^α. Such a derivative is local, in contrast to the similarly applied fractional derivative.

Physical background[]

Porous media, aquifers, turbulence, and other media usually exhibit fractal properties. Classical diffusion or dispersion laws based on random walks in free space (essentially the same result variously known as Fick's laws of diffusion, Darcy's law, and Fourier's law) are not applicable to fractal media. To address this, concepts such as distance and velocity must be redefined for fractal media; in particular, scales for space and time are to be transformed according to (x^β, t^α). Elementary physical concepts such as velocity are redefined as follows for (x^β, t^α):

${\displaystyle v'={\frac {dx'}{dt'}}={\frac {dx^{\beta }}{dt^{\alpha }}}\,,\quad \alpha ,\beta >0}$,

where S^α,β represents the fractal spacetime with scaling indices α and β. The traditional definition of velocity makes no sense in the non-differentiable fractal spacetime.

Definition[]

Based on above discussion, the concept of the fractal derivative of a function u(t) with respect to a fractal measure t has been introduced as follows:

${\displaystyle {\frac {\partial f(t)}{\partial t^{\alpha }}}=\lim _{t_{1}\rightarrow t}{\frac {f(t_{1})-f(t)}{t_{1}^{\alpha }-t^{\alpha }}}\,,\quad \alpha >0}$,

A more general definition is given by

${\displaystyle {\frac {\partial ^{\beta }f(t)}{\partial t^{\alpha }}}=\lim _{t_{1}\rightarrow t}{\frac {f^{\beta }(t_{1})-f^{\beta }(t)}{t_{1}^{\alpha }-t^{\alpha }}}\,,\quad \alpha >0,\beta >0}$.

Motivation[]

The derivatives of a function f can be defined in terms of the coefficients a_k in the Taylor series expansion:

${\displaystyle f(x)=\sum _{k=1}^{\infty }a_{k}\cdot (x-x_{0})^{k}=\sum _{k=1}^{\infty }{1 \over k!}{d^{k}f \over dx^{k}}(x_{0})\cdot (x-x_{0})^{k}=f(x_{0})+f'(x_{0})\cdot (x-x_{0})+o(x-x_{0})}$

From this approach one can directly obtain:

${\displaystyle f'(x_{0})={f(x)-f(x_{0})-o(x-x_{0}) \over x-x_{0}}=\lim _{x\to x_{0}}{f(x)-f(x_{0}) \over x-x_{0}}}$

This can be generalized approximating f with functions (x^α-(x₀)^α)^k:

${\displaystyle f(x)=\sum _{k=1}^{\infty }b_{k}\cdot (x^{\alpha }-x_{0}^{\alpha })^{k}=f(x_{0})+b_{1}\cdot (x^{\alpha }-x_{0}^{\alpha })+o(x^{\alpha }-x_{0}^{\alpha })}$

note: the lowest order coefficient still has to be b₀=f(x₀), since it's still the constant approximation of the function f at x₀.

Again one can directly obtain:

${\displaystyle b_{1}=\lim _{x\to x_{0}}{f(x)-f(x_{0}) \over x^{\alpha }-x_{0}^{\alpha }}{\overset {\underset {\mathrm {def} }{}}{=}}{df \over dx^{\alpha }}(x_{0})}$

Properties[]

Expansion coefficients[]

Just like in the Taylor series expansion, the coefficients b_k can be expressed in terms of the fractal derivatives of order k of f:

${\displaystyle b_{k}={1 \over k!}{\biggl (}{d \over dx^{\alpha }}{\biggr )}^{k}f(x=x_{0})}$

Proof idea: assuming ${\textstyle ({d \over dx^{\alpha }})^{k}f(x=x_{0})}$ exists, b_k can be written as ${\textstyle b_{k}=a_{k}\cdot ({d \over dx^{\alpha }})^{k}f(x=x_{0})}$

one can now use ${\textstyle f(x)=(x^{\alpha }-x_{0}^{\alpha })^{n}\Rightarrow ({d \over dx^{\alpha }})^{k}f(x=x_{0})=n!\delta _{n}^{k}}$ and since ${\textstyle b_{n}{\overset {\underset {\mathrm {!} }{}}{=}}1\Rightarrow a_{n}={1 \over n!}}$

Connection with Derivative[]

If for a given function f both the derivative Df and the fractal derivative D_αf exists, one can find an analog to the chain rule:

${\displaystyle {df \over dx^{\alpha }}={df \over dx}{dx \over dx^{\alpha }}={1 \over \alpha }x^{1-\alpha }{df \over dx}}$

The last step is motivated by the Implicit function theorem which, under appropriate conditions, gives us dx/dx^α = (dx^α/dx)⁻¹

Similarly for the more general definition:

${\displaystyle {d^{\beta }f \over d^{\alpha }x}={d(f^{\beta }) \over d^{\alpha }x}={1 \over \alpha }x^{1-\alpha }\beta f^{\beta -1}(x)f'(x)}$

Fractal derivative for function f(t) = t, with derivative order is α ∈ (0,1]

Application in anomalous diffusion[]

As an alternative modeling approach to the classical Fick's second law, the fractal derivative is used to derive a linear anomalous transport-diffusion equation underlying anomalous diffusion process,

${\displaystyle {\frac {du(x,t)}{dt^{\alpha }}}=D{\frac {\partial }{\partial x^{\beta }}}\left({\frac {\partial u(x,t)}{\partial x^{\beta }}}\right),-\infty <x<+\infty \,,\quad (1)}$

${\displaystyle u(x,0)=\delta (x).}$

where 0 < α < 2, 0 < β < 1, and δ(x) is the Dirac delta function.

In order to obtain the fundamental solution, we apply the transformation of variables

${\displaystyle t'=t^{\alpha }\,,\quad x'=x^{\beta }.}$

then the equation (1) becomes the normal diffusion form equation, the solution of (1) has the stretched Gaussian form:

${\displaystyle u(x,t)={\frac {1}{2{\sqrt {\pi t^{\alpha }}}}}e^{-{\frac {x^{2\beta }}{4t^{\alpha }}}}}$

The mean squared displacement of above fractal derivative diffusion equation has the asymptote:

${\displaystyle \left\langle x^{2}(t)\right\rangle \propto t^{(3\alpha -\alpha \beta )/2\beta }.}$

Fractal-fractional calculus[]

The fractal derivative is connected to the classical derivative if the first derivative of the function under investigation exists. In this case,

${\displaystyle {\frac {\partial f(t)}{\partial t^{\alpha }}}=\lim _{t_{1}\rightarrow t}{\frac {f(t_{1})-f(t)}{t_{1}^{\alpha }-t^{\alpha }}}\ ={\frac {df(t)}{dt}}{\frac {1}{\alpha t^{\alpha -1}}},\quad \alpha >0}$.

However, due to the differentiability property of an integral, fractional derivatives are differentiable, thus the following new concept was introduced

The following differential operators were introduced and applied very recently.^[1] Supposing that y(t) be continuous and fractal differentiable on (a, b) with order β, several definitions of a fractal–fractional derivative of y(t) hold with order α in the Riemann–Liouville sense:^[1]

• Having power law type kernel:

${\displaystyle ^{FFP}D_{0,t}^{\alpha ,\beta }{\Big (}y(t){\Big )}={\dfrac {1}{\Gamma (m-\alpha )}}{\dfrac {d}{dt^{\beta }}}\int _{0}^{t}(t-s)^{m-\alpha -1}y(s)ds}$

• Having exponentially decaying type kernel:

${\displaystyle ^{FFE}D_{0,t}^{\alpha ,\beta }{\Big (}y(t){\Big )}={\dfrac {M(\alpha )}{1-\alpha }}{\dfrac {d}{dt^{\beta }}}\int _{0}^{t}\exp {\Big (}-{\dfrac {\alpha }{1-\alpha }}(t-s){\Big )}y(s)ds}$,

• Having generalized Mittag-Leffler type kernel:

${\displaystyle {}_{a}^{FFM}D_{t}^{\alpha }f(t)={\frac {AB(\alpha )}{1-\alpha }}{\frac {d}{dt^{\beta }}}\int _{a}^{t}f(\tau )E_{\alpha }\left(-\alpha {\frac {\left(t-\tau \right)^{\alpha }}{1-\alpha }}\right)\,d\tau \,.}$

The above differential operators each have an associated fractal-fractional integral operator, as follows:^[1]

• Power law type kernel:

${\displaystyle ^{FFP}J_{0,t}^{\alpha ,\beta }{\Big (}y(t){\Big )}={\dfrac {\beta }{\Gamma (\alpha )}}\int _{0}^{t}(t-s)^{\alpha -1}s^{\beta -1}y(s)ds}$

• Exponentially decaying type kernel:

${\displaystyle ^{FFE}J_{0,t}^{\alpha ,\beta }{\Big (}y(t){\Big )}={\dfrac {\alpha \beta }{M(\alpha )}}\int _{0}^{t}s^{\alpha -1}y(s)ds+{\dfrac {\beta (1-\alpha )t^{\beta -1}y(t)}{M(\alpha )}}}$.

• Generalized Mittag-Leffler type kernel:

${\displaystyle ^{FFM}J_{0,t}^{\alpha ,\beta }{\Big (}y(t){\Big )}={\dfrac {\alpha \beta }{AB(\alpha )}}\int _{0}^{t}s^{\alpha -1}y(s)(t-s)^{\alpha -1}ds+{\dfrac {\beta (1-\alpha )t^{\beta -1}y(t)}{AB(\alpha )}}}$. FFM is refereed to fractal-fractional with the generalized Mittag-Leffler kernel.

See also[]

• Fractional calculus
• Fractional-order system
• Multifractal system

References[]

External links[]

• Power Law & Fractional Dynamics
• Non-Newtonian calculus website