Differintegral

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

𝔻qf

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 legitimate definitions of the differintegral.

Standard definitions

The four most common forms are:

  • The Riemann–Liouville differintegral
    This is the simplest and easiest to use, and consequently it is the most often used. It is a generalization of the Cauchy formula for repeated integration to arbitrary order. Here, n=q. aRL𝔻tqf(t)=dqf(t)d(ta)q=1Γ(nq)dndtnat(tτ)nq1f(τ)dτ
  • The Grunwald–Letnikov differintegral
    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. aGL𝔻tqf(t)=dqf(t)d(ta)q=limN[taN]qj=0N1(1)j(qj)f(tj[taN])
  • The Weyl differintegral
    This is formally similar to the Riemann–Liouville differintegral, but applies to periodic functions, with integral zero over a period.
  • The Caputo differintegral
    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. aC𝔻tqf(t)=dqf(t)d(ta)q=1Γ(nq)atf(n)(τ)(tτ)qn+1dτ

Definitions via transforms

The definitions of fractional derivatives given by Liouville, Fourier, and Grunwald and Letnikov coincide.[1] They can be represented via Laplace, Fourier transforms or via Newton series expansion.

Recall the continuous Fourier transform, here denoted : F(ω)={f(t)}=12πf(t)eiωtdt

Using the continuous Fourier transform, in Fourier space, differentiation transforms into a multiplication: [df(t)dt]=iω[f(t)]

So, dnf(t)dtn=1{(iω)n[f(t)]} which generalizes to 𝔻qf(t)=1{(iω)q[f(t)]}.

Under the bilateral Laplace transform, here denoted by and defined as [f(t)]=estf(t)dt, differentiation transforms into a multiplication [df(t)dt]=s[f(t)].

Generalizing to arbitrary order and solving for 𝔻qf(t), one obtains 𝔻qf(t)=1{sq[f(t)]}.

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

𝔻qf(t)=m=0(qm)k=0m(mk)(1)mkf(k)(x).

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

𝔻q(tn)=Γ(n+1)Γ(n+1q)tnq
𝔻q(sin(t))=sin(t+qπ2)
𝔻q(eat)=aqeat[2]

Basic formal properties

  • Linearity rules 𝔻q(f+g)=𝔻q(f)+𝔻q(g)

𝔻q(af)=a𝔻q(f)

  • Zero rule 𝔻0f=f
  • Product rule 𝔻tq(fg)=j=0(qj)𝔻tj(f)𝔻tqj(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;[3] this forms part of the decision making process on which one to choose:

  • 𝔻a𝔻bf=𝔻a+bf (ideally)
  • 𝔻a𝔻bf𝔻a+bf (in practice)

See also

References