Differintegral#Basic formal properties

{{redirect-distinguish|Fractional integration|Autoregressive fractionally integrated moving average}}

{{Calculus|expanded=Specialized calculi}}

In fractional calculus, an area of mathematical analysis, the differintegral is a combined differentiation/integration operator. Applied to a function ƒ, the q-differintegral of f, here denoted by

:\mathbb{D}^q f

is the fractional derivative (if q > 0) or fractional integral (if q < 0). If q = 0, then the q-th differintegral of a function is the function itself. In the context of fractional integration and differentiation, there are several definitions of the differintegral.

Standard definitions

The four most common forms are:

{}^{RL}_a\mathbb{D}^q_tf(t) & = \frac{d^qf(t)}{d(t-a)^q} \\

& =\frac{1}{\Gamma(n-q)} \frac{d^n}{dt^n} \int_{a}^t (t-\tau)^{n-q-1}f(\tau)d\tau

\end{align}

  • The Grunwald–Letnikov differintegral{{pb}}The Grunwald–Letnikov differintegral is a direct generalization of the definition of a derivative. It is more difficult to use than the Riemann–Liouville differintegral, but can sometimes be used to solve problems that the Riemann–Liouville cannot. \begin{align}

{}^{GL}_a\mathbb{D}^q_tf(t) & = \frac{d^qf(t)}{d(t-a)^q} \\

& =\lim_{N \to \infty}\left[\frac{t-a}{N}\right]^{-q}\sum_{j=0}^{N-1}(-1)^j{q \choose j}f\left(t-j\left[\frac{t-a}{N}\right]\right)

\end{align}

  • The Weyl differintegral{{pb}} This is formally similar to the Riemann–Liouville differintegral, but applies to periodic functions, with integral zero over a period.
  • The Caputo differintegral{{pb}}In opposite to the Riemann-Liouville differintegral, Caputo derivative of a constant f(t) is equal to zero. Moreover, a form of the Laplace transform allows to simply evaluate the initial conditions by computing finite, integer-order derivatives at point a. \begin{align}

{}^{C}_a\mathbb{D}^q_tf(t) & = \frac{d^qf(t)}{d(t-a)^q} \\

& =\frac{1}{\Gamma(n-q)} \int_{a}^t \frac{f^{(n)}(\tau)}{(t-\tau)^{q-n+1}}d\tau

\end{align}

Definitions via transforms

The definitions of fractional derivatives given by Liouville, Fourier, and Grunwald and Letnikov coincide.{{cite book |url=https://books.google.com/books?id=mPXzp1f7ycMC&pg=PA11 |first=Richard |last=Herrmann|title=Fractional Calculus: An Introduction for Physicists |year=2011 |isbn=9789814551076 }} They can be represented via Laplace, Fourier transforms or via Newton series expansion.

Recall the continuous Fourier transform, here denoted \mathcal{F}:

F(\omega) = \mathcal{F}\{f(t)\} = \frac{1}{\sqrt{2\pi}}\int_{-\infty}^\infty f(t) e^{- i\omega t}\,dt

Using the continuous Fourier transform, in Fourier space, differentiation transforms into a multiplication:

\mathcal{F}\left[\frac{df(t)}{dt}\right] = i \omega \mathcal{F}[f(t)]

So,

\frac{d^nf(t)}{dt^n} = \mathcal{F}^{-1}\left\{(i \omega)^n\mathcal{F}[f(t)]\right\}

which generalizes to

\mathbb{D}^qf(t) = \mathcal{F}^{-1}\left\{(i \omega)^q\mathcal{F}[f(t)]\right\}.

Under the bilateral Laplace transform, here denoted by \mathcal{L} and defined as \mathcal{L}[f(t)] =\int_{-\infty}^\infty e^{-st} f(t)\, dt, differentiation transforms into a multiplication

\mathcal{L}\left[\frac{df(t)}{dt}\right] = s\mathcal{L}[f(t)].

Generalizing to arbitrary order and solving for \mathbb{D}^qf(t), one obtains

\mathbb{D}^qf(t)=\mathcal{L}^{-1}\left\{s^q\mathcal{L}[f(t)]\right\}.

Representation via Newton series is the Newton interpolation over consecutive integer orders:

\mathbb{D}^qf(t) =\sum_{m=0}^{\infty} \binom {q}m \sum_{k=0}^m\binom mk(-1)^{m-k}f^{(k)}(x).

For fractional derivative definitions described in this section, the following identities hold:

:\mathbb{D}^q(t^n)=\frac{\Gamma(n+1)}{\Gamma(n+1-q)}t^{n-q}

:\mathbb{D}^q(\sin(t))=\sin \left( t+\frac{q\pi}{2} \right)

:\mathbb{D}^q(e^{at})=a^q e^{at}See {{cite book |page=16 |url=https://books.google.com/books?id=mPXzp1f7ycMC&pg=PA11 |first=Richard |last=Herrmann|title=Fractional Calculus: An Introduction for Physicists | year=2011 |isbn=9789814551076 }}

Basic formal properties

  • Linearity rules \mathbb{D}^q(f+g) = \mathbb{D}^q(f)+\mathbb{D}^q(g)

\mathbb{D}^q(af) = a\mathbb{D}^q(f)

  • Zero rule \mathbb{D}^0 f = f
  • Product rule \mathbb{D}^q_t(fg) = \sum_{j=0}^{\infty} {q \choose j}\mathbb{D}^j_t(f)\mathbb{D}^{q-j}_t(g)

In general, composition (or semigroup) rule is a desirable property, but is hard to achieve mathematically and hence is not always completely satisfied by each proposed operator;See {{cite book |page=75 |chapter=2. Fractional Integrals and Fractional Derivatives §2.1 Property 2.4 |chapter-url=https://books.google.com/books?id=uxANOU0H8IUC&pg=PA75 |first1=A. A. |last1=Kilbas |first2=H. M. |last2=Srivastava |first3=J. J. |last3=Trujillo |title=Theory and Applications of Fractional Differential Equations |publisher=Elsevier |year=2006 |isbn=9780444518323 }} this forms part of the decision making process on which one to choose:

  • \mathbb{D}^a\mathbb{D}^{b}f = \mathbb{D}^{a+b}f (ideally)
  • \mathbb{D}^a\mathbb{D}^{b}f \neq \mathbb{D}^{a+b}f (in practice)

See also

References

{{Reflist}}

{{refbegin}}

  • {{cite book |first=Kenneth S. |last=Miller |editor-first=Bertram |editor-last=Ross |title=An Introduction to the Fractional Calculus and Fractional Differential Equations |publisher=Wiley |year=1993 |isbn=0-471-58884-9 }}
  • {{cite book |first1=Keith B. |last1=Oldham |first2=Jerome |last2=Spanier |title=The Fractional Calculus; Theory and Applications of Differentiation and Integration to Arbitrary Order |publisher=Academic Press |series=Mathematics in Science and Engineering |volume=V |year=1974 |isbn=0-12-525550-0 }}
  • {{cite book |first=Igor |last=Podlubny |title=Fractional Differential Equations. An Introduction to Fractional Derivatives, Fractional Differential Equations, Some Methods of Their Solution and Some of Their Applications |publisher=Academic Press |series=Mathematics in Science and Engineering |volume=198 |year=1998 |isbn=0-12-558840-2 }}
  • {{cite book |editor-first=A. |editor-last=Carpinteri |editor2-first=F. |editor2-last=Mainardi |title=Fractals and Fractional Calculus in Continuum Mechanics |publisher=Springer-Verlag |year=1998 |isbn=3-211-82913-X }}
  • {{cite book |first=F. |last=Mainardi |title=Fractional Calculus and Waves in Linear Viscoelasticity: An Introduction to Mathematical Models |publisher=Imperial College Press |year=2010 |isbn=978-1-84816-329-4 |url=http://www.worldscibooks.com/mathematics/p614.html |archive-url=https://web.archive.org/web/20120519174508/http://www.worldscibooks.com/mathematics/p614.html |url-status=dead |archive-date=2012-05-19 }}
  • {{cite book |first=V.E. |last=Tarasov |title=Fractional Dynamics: Applications of Fractional Calculus to Dynamics of Particles, Fields and Media |publisher=Springer |year=2010 |isbn=978-3-642-14003-7 |url=https://www.springer.com/physics/complexity/book/978-3-642-14003-7|series=Nonlinear Physical Science }}
  • {{cite book |first=V.V. |last=Uchaikin |title=Fractional Derivatives for Physicists and Engineers |publisher=Springer |year=2012 |isbn=978-3-642-33910-3 |url=https://www.springer.com/physics/theoretical,+mathematical+%26+computational+physics/book/978-3-642-33910-3|series=Nonlinear Physical Science |bibcode=2013fdpe.book.....U }}
  • {{cite book |first1=Bruce J. |last1=West |first2=Mauro |last2=Bologna |first3=Paolo |last3=Grigolini |title=Physics of Fractal Operators |publisher=Springer Verlag |year=2003 |isbn=0-387-95554-2 |url=https://books.google.com/books?id=EgyTpQZOga0C&pg=PR7}}

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