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Fractional calculus GudangMovies21 Rebahinxxi LK21
Fractional calculus is a branch of mathematical analysis that studies the several different possibilities of defining real number powers or complex number powers of the differentiation operator
D
{\displaystyle D}
D
f
(
x
)
=
d
d
x
f
(
x
)
,
{\displaystyle Df(x)={\frac {d}{dx}}f(x)\,,}
and of the integration operator
J
{\displaystyle J}
J
f
(
x
)
=
∫
0
x
f
(
s
)
d
s
,
{\displaystyle Jf(x)=\int _{0}^{x}f(s)\,ds\,,}
and developing a calculus for such operators generalizing the classical one.
In this context, the term powers refers to iterative application of a linear operator
D
{\displaystyle D}
to a function
f
{\displaystyle f}
, that is, repeatedly composing
D
{\displaystyle D}
with itself, as in
D
n
(
f
)
=
(
D
∘
D
∘
D
∘
⋯
∘
D
⏟
n
)
(
f
)
=
D
(
D
(
D
(
⋯
D
⏟
n
(
f
)
⋯
)
)
)
.
{\displaystyle {\begin{aligned}D^{n}(f)&=(\underbrace {D\circ D\circ D\circ \cdots \circ D} _{n})(f)\\&=\underbrace {D(D(D(\cdots D} _{n}(f)\cdots ))).\end{aligned}}}
For example, one may ask for a meaningful interpretation of
D
=
D
1
2
{\displaystyle {\sqrt {D}}=D^{\scriptstyle {\frac {1}{2}}}}
as an analogue of the functional square root for the differentiation operator, that is, an expression for some linear operator that, when applied twice to any function, will have the same effect as differentiation. More generally, one can look at the question of defining a linear operator
D
a
{\displaystyle D^{a}}
for every real number
a
{\displaystyle a}
in such a way that, when
a
{\displaystyle a}
takes an integer value
n
∈
Z
{\displaystyle n\in \mathbb {Z} }
, it coincides with the usual
n
{\displaystyle n}
-fold differentiation
D
{\displaystyle D}
if
n
>
0
{\displaystyle n>0}
, and with the
n
{\displaystyle n}
-th power of
J
{\displaystyle J}
when
n
<
0
{\displaystyle n<0}
.
One of the motivations behind the introduction and study of these sorts of extensions of the differentiation operator
D
{\displaystyle D}
is that the sets of operator powers
{
D
a
∣
a
∈
R
}
{\displaystyle \{D^{a}\mid a\in \mathbb {R} \}}
defined in this way are continuous semigroups with parameter
a
{\displaystyle a}
, of which the original discrete semigroup of
{
D
n
∣
n
∈
Z
}
{\displaystyle \{D^{n}\mid n\in \mathbb {Z} \}}
for integer
n
{\displaystyle n}
is a denumerable subgroup: since continuous semigroups have a well developed mathematical theory, they can be applied to other branches of mathematics.
Fractional differential equations, also known as extraordinary differential equations, are a generalization of differential equations through the application of fractional calculus.
Historical notes
In applied mathematics and mathematical analysis, a fractional derivative is a derivative of any arbitrary order, real or complex. Its first appearance is in a letter written to Guillaume de l'Hôpital by Gottfried Wilhelm Leibniz in 1695. Around the same time, Leibniz wrote to one of the Bernoulli brothers describing the similarity between the binomial theorem and the Leibniz rule for the fractional derivative of a product of two functions.
Fractional calculus was introduced in one of Niels Henrik Abel's early papers where all the elements can be found: the idea of fractional-order integration and differentiation, the mutually inverse relationship between them, the understanding that fractional-order differentiation and integration can be considered as the same generalized operation, and the unified notation for differentiation and integration of arbitrary real order.
Independently, the foundations of the subject were laid by Liouville in a paper from 1832. Oliver Heaviside introduced the practical use of fractional differential operators in electrical transmission line analysis circa 1890. The theory and applications of fractional calculus expanded greatly over the 19th and 20th centuries, and numerous contributors have given different definitions for fractional derivatives and integrals.
Computing the fractional integral
Let f(x) be a function defined for x > 0. Form the definite integral from 0 to x. Call this
(
J
f
)
(
x
)
=
∫
0
x
f
(
t
)
d
t
.
{\displaystyle (Jf)(x)=\int _{0}^{x}f(t)\,dt\,.}
Repeating this process gives
(
J
2
f
)
(
x
)
=
∫
0
x
(
J
f
)
(
t
)
d
t
=
∫
0
x
(
∫
0
t
f
(
s
)
d
s
)
d
t
,
{\displaystyle {\begin{aligned}\left(J^{2}f\right)(x)&=\int _{0}^{x}(Jf)(t)\,dt\\&=\int _{0}^{x}\left(\int _{0}^{t}f(s)\,ds\right)dt\,,\end{aligned}}}
and this can be extended arbitrarily.
The Cauchy formula for repeated integration, namely
(
J
n
f
)
(
x
)
=
1
(
n
−
1
)
!
∫
0
x
(
x
−
t
)
n
−
1
f
(
t
)
d
t
,
{\displaystyle \left(J^{n}f\right)(x)={\frac {1}{(n-1)!}}\int _{0}^{x}\left(x-t\right)^{n-1}f(t)\,dt\,,}
leads in a straightforward way to a generalization for real n: using the gamma function to remove the discrete nature of the factorial function gives us a natural candidate for applications of the fractional integral operator as
(
J
α
f
)
(
x
)
=
1
Γ
(
α
)
∫
0
x
(
x
−
t
)
α
−
1
f
(
t
)
d
t
.
{\displaystyle \left(J^{\alpha }f\right)(x)={\frac {1}{\Gamma (\alpha )}}\int _{0}^{x}\left(x-t\right)^{\alpha -1}f(t)\,dt\,.}
This is in fact a well-defined operator.
It is straightforward to show that the J operator satisfies
(
J
α
)
(
J
β
f
)
(
x
)
=
(
J
β
)
(
J
α
f
)
(
x
)
=
(
J
α
+
β
f
)
(
x
)
=
1
Γ
(
α
+
β
)
∫
0
x
(
x
−
t
)
α
+
β
−
1
f
(
t
)
d
t
.
{\displaystyle {\begin{aligned}\left(J^{\alpha }\right)\left(J^{\beta }f\right)(x)&=\left(J^{\beta }\right)\left(J^{\alpha }f\right)(x)\\&=\left(J^{\alpha +\beta }f\right)(x)\\&={\frac {1}{\Gamma (\alpha +\beta )}}\int _{0}^{x}\left(x-t\right)^{\alpha +\beta -1}f(t)\,dt\,.\end{aligned}}}
This relationship is called the semigroup property of fractional differintegral operators.
= Riemann–Liouville fractional integral
=The classical form of fractional calculus is given by the Riemann–Liouville integral, which is essentially what has been described above. The theory of fractional integration for periodic functions (therefore including the "boundary condition" of repeating after a period) is given by the Weyl integral. It is defined on Fourier series, and requires the constant Fourier coefficient to vanish (thus, it applies to functions on the unit circle whose integrals evaluate to zero). The Riemann–Liouville integral exists in two forms, upper and lower. Considering the interval [a,b], the integrals are defined as
D
a
D
t
−
α
f
(
t
)
=
I
a
I
t
α
f
(
t
)
=
1
Γ
(
α
)
∫
a
t
(
t
−
τ
)
α
−
1
f
(
τ
)
d
τ
D
t
D
b
−
α
f
(
t
)
=
I
t
I
b
α
f
(
t
)
=
1
Γ
(
α
)
∫
t
b
(
τ
−
t
)
α
−
1
f
(
τ
)
d
τ
{\displaystyle {\begin{aligned}\sideset {_{a}}{_{t}^{-\alpha }}Df(t)&=\sideset {_{a}}{_{t}^{\alpha }}If(t)\\&={\frac {1}{\Gamma (\alpha )}}\int _{a}^{t}\left(t-\tau \right)^{\alpha -1}f(\tau )\,d\tau \\\sideset {_{t}}{_{b}^{-\alpha }}Df(t)&=\sideset {_{t}}{_{b}^{\alpha }}If(t)\\&={\frac {1}{\Gamma (\alpha )}}\int _{t}^{b}\left(\tau -t\right)^{\alpha -1}f(\tau )\,d\tau \end{aligned}}}
Where the former is valid for t > a and the latter is valid for t < b.
It has been suggested that the integral on the positive real axis (i.e.
a
=
0
{\displaystyle a=0}
) would be more appropriately named the Abel–Riemann integral, on the basis of history of discovery and use, and in the same vein the integral over the entire real line be named Liouville–Weyl integral.
By contrast the Grünwald–Letnikov derivative starts with the derivative instead of the integral.
= Hadamard fractional integral
=The Hadamard fractional integral was introduced by Jacques Hadamard and is given by the following formula,
D
a
D
t
−
α
f
(
t
)
=
1
Γ
(
α
)
∫
a
t
(
log
t
τ
)
α
−
1
f
(
τ
)
d
τ
τ
,
t
>
a
.
{\displaystyle \sideset {_{a}}{_{t}^{-\alpha }}{\mathbf {D} }f(t)={\frac {1}{\Gamma (\alpha )}}\int _{a}^{t}\left(\log {\frac {t}{\tau }}\right)^{\alpha -1}f(\tau ){\frac {d\tau }{\tau }},\qquad t>a\,.}
= Atangana–Baleanu fractional integral (AB fractional integral)
=The Atangana–Baleanu fractional integral of a continuous function is defined as:
I
A
a
AB
I
t
α
f
(
t
)
=
1
−
α
AB
(
α
)
f
(
t
)
+
α
AB
(
α
)
Γ
(
α
)
∫
a
t
(
t
−
τ
)
α
−
1
f
(
τ
)
d
τ
{\displaystyle \sideset {_{{\hphantom {A}}a}^{\operatorname {AB} }}{_{t}^{\alpha }}If(t)={\frac {1-\alpha }{\operatorname {AB} (\alpha )}}f(t)+{\frac {\alpha }{\operatorname {AB} (\alpha )\Gamma (\alpha )}}\int _{a}^{t}\left(t-\tau \right)^{\alpha -1}f(\tau )\,d\tau }
Fractional derivatives
Unfortunately, the comparable process for the derivative operator D is significantly more complex, but it can be shown that D is neither commutative nor additive in general.
Unlike classical Newtonian derivatives, fractional derivatives can be defined in a variety of different ways that often do not all lead to the same result even for smooth functions. Some of these are defined via a fractional integral. Because of the incompatibility of definitions, it is frequently necessary to be explicit about which definition is used.
= Riemann–Liouville fractional derivative
=The corresponding derivative is calculated using Lagrange's rule for differential operators. To find the αth order derivative, the nth order derivative of the integral of order (n − α) is computed, where n is the smallest integer greater than α (that is, n = ⌈α⌉). The Riemann–Liouville fractional derivative and integral has multiple applications such as in case of solutions to the equation in the case of multiple systems such as the tokamak systems, and Variable order fractional parameter. Similar to the definitions for the Riemann–Liouville integral, the derivative has upper and lower variants.
D
a
D
t
α
f
(
t
)
=
d
n
d
t
n
D
a
D
t
−
(
n
−
α
)
f
(
t
)
=
d
n
d
t
n
I
a
I
t
n
−
α
f
(
t
)
D
t
D
b
α
f
(
t
)
=
d
n
d
t
n
D
t
D
b
−
(
n
−
α
)
f
(
t
)
=
d
n
d
t
n
I
t
I
b
n
−
α
f
(
t
)
{\displaystyle {\begin{aligned}\sideset {_{a}}{_{t}^{\alpha }}Df(t)&={\frac {d^{n}}{dt^{n}}}\sideset {_{a}}{_{t}^{-(n-\alpha )}}Df(t)\\&={\frac {d^{n}}{dt^{n}}}\sideset {_{a}}{_{t}^{n-\alpha }}If(t)\\\sideset {_{t}}{_{b}^{\alpha }}Df(t)&={\frac {d^{n}}{dt^{n}}}\sideset {_{t}}{_{b}^{-(n-\alpha )}}Df(t)\\&={\frac {d^{n}}{dt^{n}}}\sideset {_{t}}{_{b}^{n-\alpha }}If(t)\end{aligned}}}
= Caputo fractional derivative
=Another option for computing fractional derivatives is the Caputo fractional derivative. It was introduced by Michele Caputo in his 1967 paper. In contrast to the Riemann–Liouville fractional derivative, when solving differential equations using Caputo's definition, it is not necessary to define the fractional order initial conditions. Caputo's definition is illustrated as follows, where again n = ⌈α⌉:
D
C
D
t
α
f
(
t
)
=
1
Γ
(
n
−
α
)
∫
0
t
f
(
n
)
(
τ
)
(
t
−
τ
)
α
+
1
−
n
d
τ
.
{\displaystyle \sideset {^{C}}{_{t}^{\alpha }}Df(t)={\frac {1}{\Gamma (n-\alpha )}}\int _{0}^{t}{\frac {f^{(n)}(\tau )}{\left(t-\tau \right)^{\alpha +1-n}}}\,d\tau .}
There is the Caputo fractional derivative defined as:
D
ν
f
(
t
)
=
1
Γ
(
n
−
ν
)
∫
0
t
(
t
−
u
)
(
n
−
ν
−
1
)
f
(
n
)
(
u
)
d
u
(
n
−
1
)
<
ν
<
n
{\displaystyle D^{\nu }f(t)={\frac {1}{\Gamma (n-\nu )}}\int _{0}^{t}(t-u)^{(n-\nu -1)}f^{(n)}(u)\,du\qquad (n-1)<\nu
which has the advantage that is zero when f(t) is constant and its Laplace Transform is expressed by means of the initial values of the function and its derivative. Moreover, there is the Caputo fractional derivative of distributed order defined as
D
a
b
D
n
u
f
(
t
)
=
∫
a
b
ϕ
(
ν
)
[
D
(
ν
)
f
(
t
)
]
d
ν
=
∫
a
b
[
ϕ
(
ν
)
Γ
(
1
−
ν
)
∫
0
t
(
t
−
u
)
−
ν
f
′
(
u
)
d
u
]
d
ν
{\displaystyle {\begin{aligned}\sideset {_{a}^{b}}{^{n}u}Df(t)&=\int _{a}^{b}\phi (\nu )\left[D^{(\nu )}f(t)\right]\,d\nu \\&=\int _{a}^{b}\left[{\frac {\phi (\nu )}{\Gamma (1-\nu )}}\int _{0}^{t}\left(t-u\right)^{-\nu }f'(u)\,du\right]\,d\nu \end{aligned}}}
where ϕ(ν) is a weight function and which is used to represent mathematically the presence of multiple memory formalisms.
= Caputo–Fabrizio fractional derivative
=In a paper of 2015, M. Caputo and M. Fabrizio presented a definition of fractional derivative with a non singular kernel, for a function
f
(
t
)
{\displaystyle f(t)}
of
C
1
{\displaystyle C^{1}}
given by:
D
C
a
CF
D
t
α
f
(
t
)
=
1
1
−
α
∫
a
t
f
′
(
τ
)
e
(
−
α
t
−
τ
1
−
α
)
d
τ
,
{\displaystyle \sideset {_{{\hphantom {C}}a}^{\text{CF}}}{_{t}^{\alpha }}Df(t)={\frac {1}{1-\alpha }}\int _{a}^{t}f'(\tau )\ e^{\left(-\alpha {\frac {t-\tau }{1-\alpha }}\right)}\ d\tau ,}
where
a
<
0
,
α
∈
(
0
,
1
]
{\displaystyle a<0,\alpha \in (0,1]}
.
= Atangana–Baleanu fractional derivative
=In 2016, Atangana and Baleanu suggested differential operators based on the generalized Mittag-Leffler function
E
α
{\displaystyle E_{\alpha }}
. The aim was to introduce fractional differential operators with non-singular nonlocal kernel. Their fractional differential operators are given below in Riemann–Liouville sense and Caputo sense respectively. For a function
f
(
t
)
{\displaystyle f(t)}
of
C
1
{\displaystyle C^{1}}
given by
D
A
B
a
ABC
D
t
α
f
(
t
)
=
AB
(
α
)
1
−
α
∫
a
t
f
′
(
τ
)
E
α
(
−
α
(
t
−
τ
)
α
1
−
α
)
d
τ
,
{\displaystyle \sideset {_{{\hphantom {AB}}a}^{\text{ABC}}}{_{t}^{\alpha }}Df(t)={\frac {\operatorname {AB} (\alpha )}{1-\alpha }}\int _{a}^{t}f'(\tau )E_{\alpha }\left(-\alpha {\frac {(t-\tau )^{\alpha }}{1-\alpha }}\right)d\tau ,}
If the function is continuous, the Atangana–Baleanu derivative in Riemann–Liouville sense is given by:
D
A
B
a
ABC
D
t
α
f
(
t
)
=
AB
(
α
)
1
−
α
d
d
t
∫
a
t
f
(
τ
)
E
α
(
−
α
(
t
−
τ
)
α
1
−
α
)
d
τ
,
{\displaystyle \sideset {_{{\hphantom {AB}}a}^{\text{ABC}}}{_{t}^{\alpha }}Df(t)={\frac {\operatorname {AB} (\alpha )}{1-\alpha }}{\frac {d}{dt}}\int _{a}^{t}f(\tau )E_{\alpha }\left(-\alpha {\frac {(t-\tau )^{\alpha }}{1-\alpha }}\right)d\tau ,}
The kernel used in Atangana–Baleanu fractional derivative has some properties of a cumulative distribution function. For example, for all
α
∈
(
0
,
1
]
{\displaystyle \alpha \in (0,1]}
, the function
E
α
{\displaystyle E_{\alpha }}
is increasing on the real line, converges to
0
{\displaystyle 0}
in
−
∞
{\displaystyle -\infty }
, and
E
α
(
0
)
=
1
{\displaystyle E_{\alpha }(0)=1}
. Therefore, we have that, the function
x
↦
1
−
E
α
(
−
x
α
)
{\displaystyle x\mapsto 1-E_{\alpha }(-x^{\alpha })}
is the cumulative distribution function of a probability measure on the positive real numbers. The distribution is therefore defined, and any of its multiples is called a Mittag-Leffler distribution of order
α
{\displaystyle \alpha }
. It is also very well-known that, all these probability distributions are absolutely continuous. In particular, the function Mittag-Leffler has a particular case
E
1
{\displaystyle E_{1}}
, which is the exponential function, the Mittag-Leffler distribution of order
1
{\displaystyle 1}
is therefore an exponential distribution. However, for
α
∈
(
0
,
1
)
{\displaystyle \alpha \in (0,1)}
, the Mittag-Leffler distributions are heavy-tailed. Their Laplace transform is given by:
E
(
e
−
λ
X
α
)
=
1
1
+
λ
α
,
{\displaystyle \mathbb {E} (e^{-\lambda X_{\alpha }})={\frac {1}{1+\lambda ^{\alpha }}},}
This directly implies that, for
α
∈
(
0
,
1
)
{\displaystyle \alpha \in (0,1)}
, the expectation is infinite. In addition, these distributions are geometric stable distributions.
= Riesz derivative
=The Riesz derivative is defined as
F
{
∂
α
u
∂
|
x
|
α
}
(
k
)
=
−
|
k
|
α
F
{
u
}
(
k
)
,
{\displaystyle {\mathcal {F}}\left\{{\frac {\partial ^{\alpha }u}{\partial \left|x\right|^{\alpha }}}\right\}(k)=-\left|k\right|^{\alpha }{\mathcal {F}}\{u\}(k),}
where
F
{\displaystyle {\mathcal {F}}}
denotes the Fourier transform.
= Conformable fractional derivative
=The conformable fractional derivative of a function
f
{\displaystyle f}
of order
α
{\displaystyle \alpha }
is given by
T
a
(
f
)
(
t
)
=
lim
ϵ
→
0
f
(
t
+
ϵ
t
1
−
α
)
−
f
(
t
)
ϵ
{\displaystyle T_{a}(f)(t)=\lim _{\epsilon \rightarrow 0}{\frac {f\left(t+\epsilon t^{1-\alpha }\right)-f(t)}{\epsilon }}}
Unlike other definitions of the fractional derivative, the conformable fractional derivative obeys the product and quotient rule has analogs to Rolle's theorem and the mean value theorem. However, this fractional derivative produces significantly different results compared to the Riemann-Liouville and Caputo fractional derivative. In 2020, Feng Gao and Chunmei Chi defined the improved Caputo-type conformable fractional derivative, which more closely approximates the behavior of the Caputo fractional derivative:
a
C
T
~
a
(
f
)
(
t
)
=
lim
ϵ
→
0
[
(
1
−
α
)
(
f
(
t
)
−
f
(
a
)
)
+
α
f
(
t
+
ϵ
(
t
−
a
)
1
−
α
)
−
f
(
t
)
ϵ
]
{\displaystyle _{a}^{C}{\widetilde {T}}_{a}(f)(t)=\lim _{\epsilon \rightarrow 0}\left[(1-\alpha )(f(t)-f(a))+\alpha {\frac {f\left(t+\epsilon (t-a)^{1-\alpha }\right)-f(t)}{\epsilon }}\right]}
where
a
{\displaystyle a}
and
t
{\displaystyle t}
are real numbers and
a
<
t
{\displaystyle a
.They also defined the improved Riemann-Liouville-type conformable fractional derivative to similarly approximate the Riemann-Liouville fractional derivative:
a
R
L
T
~
a
(
f
)
(
t
)
=
lim
ϵ
→
0
[
(
1
−
α
)
f
(
t
)
+
α
f
(
t
+
ϵ
(
t
−
a
)
1
−
α
)
−
f
(
t
)
ϵ
]
{\displaystyle _{a}^{RL}{\widetilde {T}}_{a}(f)(t)=\lim _{\epsilon \rightarrow 0}\left[(1-\alpha )f(t)+\alpha {\frac {f\left(t+\epsilon (t-a)^{1-\alpha }\right)-f(t)}{\epsilon }}\right]}
where
a
{\displaystyle a}
and
t
{\displaystyle t}
are real numbers and
a
<
t
{\displaystyle a
. Both improved conformable fractional derivatives have analogs to Rolle's theorem and the interior extremum theorem.
= Other types
=Classical fractional derivatives include:
Grünwald–Letnikov derivative
Sonin–Letnikov derivative
Liouville derivative
Caputo derivative
Hadamard derivative
Marchaud derivative
Riesz derivative
Miller–Ross derivative
Weyl derivative
Erdélyi–Kober derivative
F
α
{\displaystyle F^{\alpha }}
-derivative
New fractional derivatives include:
Coimbra derivative
Katugampola derivative
Hilfer derivative
Davidson derivative
Chen derivative
Caputo Fabrizio derivative
Atangana–Baleanu derivative
Coimbra derivative
The Coimbra derivative is used for physical modeling: A number of applications in both mechanics and optics can be found in the works by Coimbra and collaborators, as well as additional applications to physical problems and numerical implementations studied in a number of works by other authors
For
q
(
t
)
<
1
{\displaystyle q(t)<1}
a
C
D
q
(
t
)
f
(
t
)
=
1
Γ
[
1
−
q
(
t
)
]
∫
0
+
t
(
t
−
τ
)
−
q
(
t
)
d
f
(
τ
)
d
τ
d
τ
+
(
f
(
0
+
)
−
f
(
0
−
)
)
t
−
q
(
t
)
Γ
(
1
−
q
(
t
)
)
,
{\displaystyle {\begin{aligned}^{\mathbb {C} }_{a}\mathbb {D} ^{q(t)}f(t)={\frac {1}{\Gamma [1-q(t)]}}\int _{0^{+}}^{t}(t-\tau )^{-q(t)}{\frac {d\,f(\tau )}{d\tau }}d\tau \,+\,{\frac {(f(0^{+})-f(0^{-}))\,t^{-q(t)}}{\Gamma (1-q(t))}},\end{aligned}}}
where the lower limit
a
{\displaystyle a}
can be taken as either
0
−
{\displaystyle 0^{-}}
or
−
∞
{\displaystyle -\infty }
as long as
f
(
t
)
{\displaystyle f(t)}
is identically zero from or
−
∞
{\displaystyle -\infty }
to
0
−
{\displaystyle 0^{-}}
. Note that this operator returns the correct fractional derivatives for all values of
t
{\displaystyle t}
and can be applied to either the dependent function itself
f
(
t
)
{\displaystyle f(t)}
with a variable order of the form
q
(
f
(
t
)
)
{\displaystyle q(f(t))}
or to the independent variable with a variable order of the form
q
(
t
)
{\displaystyle q(t)}
.
[
1
]
{\displaystyle ^{[1]}}
The Coimbra derivative can be generalized to any order, leading to the Coimbra Generalized Order Differintegration Operator (GODO)
For
q
(
t
)
<
m
{\displaystyle q(t)
−
∞
C
D
q
(
t
)
f
(
t
)
=
1
Γ
[
m
−
q
(
t
)
]
∫
0
+
t
(
t
−
τ
)
m
−
1
−
q
(
t
)
d
m
f
(
τ
)
d
τ
m
d
τ
+
∑
n
=
0
m
−
1
(
d
n
f
(
t
)
d
t
n
|
0
+
−
d
n
f
(
t
)
d
t
n
|
0
−
)
t
n
−
q
(
t
)
Γ
[
n
+
1
−
q
(
t
)
]
,
{\displaystyle {\begin{aligned}^{\mathbb {\quad C} }_{\,\,-\infty }\mathbb {D} ^{q(t)}f(t)={\frac {1}{\Gamma [m-q(t)]}}\int _{0^{+}}^{t}(t-\tau )^{m-1-q(t)}{\frac {d^{m}f(\tau )}{d\tau ^{m}}}d\tau \,+\,\sum _{n=0}^{m-1}{\frac {({\frac {d^{n}f(t)}{dt^{n}}}|_{0^{+}}-{\frac {d^{n}f(t)}{dt^{n}}}|_{0^{-}})\,t^{n-q(t)}}{\Gamma [n+1-q(t)]}},\end{aligned}}}
where
m
{\displaystyle m}
is an integer larger than the larger value of
q
(
t
)
{\displaystyle q(t)}
for all values of
t
{\displaystyle t}
. Note that the second (summation) term on the right side of the definition above can be expressed as
1
Γ
[
m
−
q
(
t
)
]
∑
n
=
0
m
−
1
{
[
d
n
f
(
t
)
d
t
n
|
0
+
−
d
n
f
(
t
)
d
t
n
|
0
−
]
t
n
−
q
(
t
)
∏
j
=
n
+
1
m
−
1
[
j
−
q
(
t
)
]
}
{\displaystyle {\begin{aligned}{\frac {1}{\Gamma [m-q(t)]}}\sum _{n=0}^{m-1}\{[{\frac {d^{n}\!f(t)}{dt^{n}}}|_{0^{+}}-{\frac {d^{n}\!f(t)}{dt^{n}}}|_{0^{-}}]\,t^{n-q(t)}\prod _{j=n+1}^{m-1}[j-q(t)]\}\end{aligned}}}
so to keep the denominator on the positive branch of the Gamma (
Γ
{\displaystyle \Gamma }
) function and for ease of numerical calculation.
= Nature of the fractional derivative
=The
a
{\displaystyle a}
-th derivative of a function
f
{\displaystyle f}
at a point
x
{\displaystyle x}
is a local property only when
a
{\displaystyle a}
is an integer; this is not the case for non-integer power derivatives. In other words, a non-integer fractional derivative of
f
{\displaystyle f}
at
x
=
c
{\displaystyle x=c}
depends on all values of
f
{\displaystyle f}
, even those far away from
c
{\displaystyle c}
. Therefore, it is expected that the fractional derivative operation involves some sort of boundary conditions, involving information on the function further out.
The fractional derivative of a function of order
a
{\displaystyle a}
is nowadays often defined by means of the Fourier or Mellin integral transforms.
Generalizations
= Erdélyi–Kober operator
=The Erdélyi–Kober operator is an integral operator introduced by Arthur Erdélyi (1940). and Hermann Kober (1940) and is given by
x
−
ν
−
α
+
1
Γ
(
α
)
∫
0
x
(
t
−
x
)
α
−
1
t
−
α
−
ν
f
(
t
)
d
t
,
{\displaystyle {\frac {x^{-\nu -\alpha +1}}{\Gamma (\alpha )}}\int _{0}^{x}\left(t-x\right)^{\alpha -1}t^{-\alpha -\nu }f(t)\,dt\,,}
which generalizes the Riemann–Liouville fractional integral and the Weyl integral.
Functional calculus
In the context of functional analysis, functions f(D) more general than powers are studied in the functional calculus of spectral theory. The theory of pseudo-differential operators also allows one to consider powers of D. The operators arising are examples of singular integral operators; and the generalisation of the classical theory to higher dimensions is called the theory of Riesz potentials. So there are a number of contemporary theories available, within which fractional calculus can be discussed. See also Erdélyi–Kober operator, important in special function theory (Kober 1940), (Erdélyi 1950–1951).
Applications
= Fractional conservation of mass
=As described by Wheatcraft and Meerschaert (2008), a fractional conservation of mass equation is needed to model fluid flow when the control volume is not large enough compared to the scale of heterogeneity and when the flux within the control volume is non-linear. In the referenced paper, the fractional conservation of mass equation for fluid flow is:
−
ρ
(
∇
α
⋅
u
→
)
=
Γ
(
α
+
1
)
Δ
x
1
−
α
ρ
(
β
s
+
ϕ
β
w
)
∂
p
∂
t
{\displaystyle -\rho \left(\nabla ^{\alpha }\cdot {\vec {u}}\right)=\Gamma (\alpha +1)\Delta x^{1-\alpha }\rho \left(\beta _{s}+\phi \beta _{w}\right){\frac {\partial p}{\partial t}}}
= Electrochemical analysis
=When studying the redox behavior of a substrate in solution, a voltage is applied at an electrode surface to force electron transfer between electrode and substrate. The resulting electron transfer is measured as a current. The current depends upon the concentration of substrate at the electrode surface. As substrate is consumed, fresh substrate diffuses to the electrode as described by Fick's laws of diffusion. Taking the Laplace transform of Fick's second law yields an ordinary second-order differential equation (here in dimensionless form):
d
2
d
x
2
C
(
x
,
s
)
=
s
C
(
x
,
s
)
{\displaystyle {\frac {d^{2}}{dx^{2}}}C(x,s)=sC(x,s)}
whose solution C(x,s) contains a one-half power dependence on s. Taking the derivative of C(x,s) and then the inverse Laplace transform yields the following relationship:
d
d
x
C
(
x
,
t
)
=
d
1
2
d
t
1
2
C
(
x
,
t
)
{\displaystyle {\frac {d}{dx}}C(x,t)={\frac {d^{\scriptstyle {\frac {1}{2}}}}{dt^{\scriptstyle {\frac {1}{2}}}}}C(x,t)}
which relates the concentration of substrate at the electrode surface to the current. This relationship is applied in electrochemical kinetics to elucidate mechanistic behavior. For example, it has been used to study the rate of dimerization of substrates upon electrochemical reduction.
= Groundwater flow problem
=In 2013–2014 Atangana et al. described some groundwater flow problems using the concept of a derivative with fractional order. In these works, the classical Darcy law is generalized by regarding the water flow as a function of a non-integer order derivative of the piezometric head. This generalized law and the law of conservation of mass are then used to derive a new equation for groundwater flow.
= Fractional advection dispersion equation
=This equation has been shown useful for modeling contaminant flow in heterogenous porous media.
Atangana and Kilicman extended the fractional advection dispersion equation to a variable order equation. In their work, the hydrodynamic dispersion equation was generalized using the concept of a variational order derivative. The modified equation was numerically solved via the Crank–Nicolson method. The stability and convergence in numerical simulations showed that the modified equation is more reliable in predicting the movement of pollution in deformable aquifers than equations with constant fractional and integer derivatives
= Time-space fractional diffusion equation models
=Anomalous diffusion processes in complex media can be well characterized by using fractional-order diffusion equation models. The time derivative term corresponds to long-time heavy tail decay and the spatial derivative for diffusion nonlocality. The time-space fractional diffusion governing equation can be written as
∂
α
u
∂
t
α
=
−
K
(
−
Δ
)
β
u
.
{\displaystyle {\frac {\partial ^{\alpha }u}{\partial t^{\alpha }}}=-K(-\Delta )^{\beta }u.}
A simple extension of the fractional derivative is the variable-order fractional derivative, α and β are changed into α(x, t) and β(x, t). Its applications in anomalous diffusion modeling can be found in the reference.
= Structural damping models
=Fractional derivatives are used to model viscoelastic damping in certain types of materials like polymers.
= PID controllers
=Generalizing PID controllers to use fractional orders can increase their degree of freedom. The new equation relating the control variable u(t) in terms of a measured error value e(t) can be written as
u
(
t
)
=
K
p
e
(
t
)
+
K
i
D
t
−
α
e
(
t
)
+
K
d
D
t
β
e
(
t
)
{\displaystyle u(t)=K_{\mathrm {p} }e(t)+K_{\mathrm {i} }D_{t}^{-\alpha }e(t)+K_{\mathrm {d} }D_{t}^{\beta }e(t)}
where α and β are positive fractional orders and Kp, Ki, and Kd, all non-negative, denote the coefficients for the proportional, integral, and derivative terms, respectively (sometimes denoted P, I, and D).
= Acoustic wave equations for complex media
=The propagation of acoustical waves in complex media, such as in biological tissue, commonly implies attenuation obeying a frequency power-law. This kind of phenomenon may be described using a causal wave equation which incorporates fractional time derivatives:
∇
2
u
−
1
c
0
2
∂
2
u
∂
t
2
+
τ
σ
α
∂
α
∂
t
α
∇
2
u
−
τ
ϵ
β
c
0
2
∂
β
+
2
u
∂
t
β
+
2
=
0
.
{\displaystyle \nabla ^{2}u-{\dfrac {1}{c_{0}^{2}}}{\frac {\partial ^{2}u}{\partial t^{2}}}+\tau _{\sigma }^{\alpha }{\dfrac {\partial ^{\alpha }}{\partial t^{\alpha }}}\nabla ^{2}u-{\dfrac {\tau _{\epsilon }^{\beta }}{c_{0}^{2}}}{\dfrac {\partial ^{\beta +2}u}{\partial t^{\beta +2}}}=0\,.}
See also Holm & Näsholm (2011) and the references therein. Such models are linked to the commonly recognized hypothesis that multiple relaxation phenomena give rise to the attenuation measured in complex media. This link is further described in Näsholm & Holm (2011b) and in the survey paper, as well as the Acoustic attenuation article. See Holm & Nasholm (2013) for a paper which compares fractional wave equations which model power-law attenuation. This book on power-law attenuation also covers the topic in more detail.
Pandey and Holm gave a physical meaning to fractional differential equations by deriving them from physical principles and interpreting the fractional-order in terms of the parameters of the acoustical media, example in fluid-saturated granular unconsolidated marine sediments. Interestingly, Pandey and Holm derived Lomnitz's law in seismology and Nutting's law in non-Newtonian rheology using the framework of fractional calculus. Nutting's law was used to model the wave propagation in marine sediments using fractional derivatives.
= Fractional Schrödinger equation in quantum theory
=The fractional Schrödinger equation, a fundamental equation of fractional quantum mechanics, has the following form:
i
ℏ
∂
ψ
(
r
,
t
)
∂
t
=
D
α
(
−
ℏ
2
Δ
)
α
2
ψ
(
r
,
t
)
+
V
(
r
,
t
)
ψ
(
r
,
t
)
.
{\displaystyle i\hbar {\frac {\partial \psi (\mathbf {r} ,t)}{\partial t}}=D_{\alpha }\left(-\hbar ^{2}\Delta \right)^{\frac {\alpha }{2}}\psi (\mathbf {r} ,t)+V(\mathbf {r} ,t)\psi (\mathbf {r} ,t)\,.}
where the solution of the equation is the wavefunction ψ(r, t) – the quantum mechanical probability amplitude for the particle to have a given position vector r at any given time t, and ħ is the reduced Planck constant. The potential energy function V(r, t) depends on the system.
Further,
Δ
=
∂
2
∂
r
2
{\textstyle \Delta ={\frac {\partial ^{2}}{\partial \mathbf {r} ^{2}}}}
is the Laplace operator, and Dα is a scale constant with physical dimension [Dα] = J1 − α·mα·s−α = kg1 − α·m2 − α·sα − 2, (at α = 2,
D
2
=
1
2
m
{\textstyle D_{2}={\frac {1}{2m}}}
for a particle of mass m), and the operator (−ħ2Δ)α/2 is the 3-dimensional fractional quantum Riesz derivative defined by
(
−
ℏ
2
Δ
)
α
2
ψ
(
r
,
t
)
=
1
(
2
π
ℏ
)
3
∫
d
3
p
e
i
ℏ
p
⋅
r
|
p
|
α
φ
(
p
,
t
)
.
{\displaystyle (-\hbar ^{2}\Delta )^{\frac {\alpha }{2}}\psi (\mathbf {r} ,t)={\frac {1}{(2\pi \hbar )^{3}}}\int d^{3}pe^{{\frac {i}{\hbar }}\mathbf {p} \cdot \mathbf {r} }|\mathbf {p} |^{\alpha }\varphi (\mathbf {p} ,t)\,.}
The index α in the fractional Schrödinger equation is the Lévy index, 1 < α ≤ 2.
Variable-order fractional Schrödinger equation
As a natural generalization of the fractional Schrödinger equation, the variable-order fractional Schrödinger equation has been exploited to study fractional quantum phenomena:
i
ℏ
∂
ψ
α
(
r
)
(
r
,
t
)
∂
t
α
(
r
)
=
(
−
ℏ
2
Δ
)
β
(
t
)
2
ψ
(
r
,
t
)
+
V
(
r
,
t
)
ψ
(
r
,
t
)
,
{\displaystyle i\hbar {\frac {\partial \psi ^{\alpha (\mathbf {r} )}(\mathbf {r} ,t)}{\partial t^{\alpha (\mathbf {r} )}}}=\left(-\hbar ^{2}\Delta \right)^{\frac {\beta (t)}{2}}\psi (\mathbf {r} ,t)+V(\mathbf {r} ,t)\psi (\mathbf {r} ,t),}
where
Δ
=
∂
2
∂
r
2
{\textstyle \Delta ={\frac {\partial ^{2}}{\partial \mathbf {r} ^{2}}}}
is the Laplace operator and the operator (−ħ2Δ)β(t)/2 is the variable-order fractional quantum Riesz derivative.
See also
Acoustic attenuation
Autoregressive fractionally integrated moving average
Initialized fractional calculus
Nonlocal operator
= Other fractional theories
=Fractional-order system
Fractional Fourier transform
Prabhakar function
Notes
References
Further reading
= Articles regarding the history of fractional calculus
=Debnath, L. (2004). "A brief historical introduction to fractional calculus". International Journal of Mathematical Education in Science and Technology. 35 (4): 487–501. doi:10.1080/00207390410001686571. S2CID 122198977.
= Books
=Miller, Kenneth S.; Ross, Bertram, eds. (1993). An Introduction to the Fractional Calculus and Fractional Differential Equations. John Wiley & Sons. ISBN 978-0-471-58884-9.
Samko, S.; Kilbas, A.A.; Marichev, O. (1993). Fractional Integrals and Derivatives: Theory and Applications. Taylor & Francis Books. ISBN 978-2-88124-864-1.
Carpinteri, A.; Mainardi, F., eds. (1998). Fractals and Fractional Calculus in Continuum Mechanics. Springer-Verlag Telos. ISBN 978-3-211-82913-4.
Igor Podlubny (27 October 1998). Fractional Differential Equations: An Introduction to Fractional Derivatives, Fractional Differential Equations, to Methods of Their Solution and Some of Their Applications. Elsevier. ISBN 978-0-08-053198-4.
Tarasov, V.E. (2010). Fractional Dynamics: Applications of Fractional Calculus to Dynamics of Particles, Fields and Media. Nonlinear Physical Science. Springer. doi:10.1007/978-3-642-14003-7. ISBN 978-3-642-14003-7.
Li, Changpin; Cai, Min (2019). Theory and Numerical Approximations of Fractional Integrals and Derivatives. SIAM. doi:10.1137/1.9781611975888. ISBN 978-1-61197-587-1.
External links
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Fractional calculus - Wikipedia
Fractional calculus is a branch of mathematical analysis that studies the several different possibilities of defining real number powers or complex number powers of the differentiation operator = (), and of the integration operator J {\displaystyle J} [ Note 1 ] J f ( x ) = ∫ 0 x f ( s ) d s , {\displaystyle Jf(x)=\int _{0}^{x}f(s)\,ds\,,}
A Compact Introduction to Fractional Calculus arXiv:2301 ...
Jan 3, 2023 · theorem of calculus — Fundamental Theorem of Fractional Calculus (FTFC) for the 1 cases of the Riemann-Liouville,Liouville, Caputo, Weyl and Riesz derivatives.
MDPI - Publisher of Open Access Journals
PDF-1.7 %âãÏÓ 1238 0 obj >>>/Metadata 1235 0 R/Outlines 1296 0 R/PageLabels 1209 0 R/Pages 1211 0 R/Type/Catalog>> endobj 1235 0 obj >stream 2018-08-28T12:31:17+08: ...
FRACTIONAL CALCULUS AND SPECIAL FUNCTIONS
Fractional calculus is the eld of mathematical analysis which deals with the investigation and applications of integrals and derivatives of arbitrary order. The term fractional is a misnomer, but it is retained following the prevailing use. The fractional calculus may be considered an old and yet novel topic. It is an old topic
Introduction to Fractional Calculus with Brief Historical ...
Jan 1, 2014 · The Fractional Calculus (FC) is a generalization of classical calculus concerned with operations of integration and differentiation of non-integer (fractional) order. The concept of fractional...
What is Fractional Calculus? - Ohio State University
about fractional calculus is that most reasonable de nitions for the derivative or integral may be taken as the starting point of the development of the theory. All of these de nitions are either equivalent or intimately related.
Fractional Calculus and Some Problems - Rutgers University
After that, many famous mathematicians, like J. Fourier, N. H. Abel, J. Liouville, B. Riemann and others, contributed to the development of the Fractional Calculus. The theory of derivatives and integrals of arbitrary order took more or less nished form by the end of the XIX century.