Differintegral
Previous topic: fractional calculus | Next topic: initialization of the differintegrals
In mathematics, the combined differentiation/integration operator used in fractional calculus is called the differintegral, and it has a few different forms which are all equivalent, provided that they are initialized (used) properly.
It is noted:
-
and is most generally defined as:
By far, the three most common forms are:
This is the simplest and easiest to use, and consequently it is the most often used.
We first introduce the Riemann-Liouville fractional integral, which is a straight-forward generalization of the Cauchy formula for repeated integration:
This gives us integration to an arbitrary order. To get differentation to an arbitrary order, we simply integrate to arbitrary order n-q, and differentiate the result to integer order n. (We choose n and q so that n is the smallest positive integer greater than or equal to q (that is, the ceiling of q)):
Thus, we have differentiated n-(n-q)=q times. The RL differintegral is thus defined as(the constant is brought to the front):
- definition
- When we are taking the differintegral at the upper bound (t), it is usually written:
- definition
- And when we are assuming that the lower bound is zero, it is usually written:
- definition
- That is, we are taking the differintegral of f(t) with respect to t.
- see for more info: Riemann-Liouville differintegral.
- The Grunwald-Letnikov differintegral(GL). -This has an interesting form. It may provide some geometric insight into fractional calculus if we can develop a good intepretation of it. This also poses fewer restrictions on the function being differintegrated. It is a generalization of the infinite Riemann Sum which defines integer-order integration in calculus. It uses the Binomial coefficient (generalized by the gamma function to arbitrary domain), commonly used in the branch of mathematics called counting.:
- definition
- see for more info: Grunwald-Letnikov differintegral.
- The Weyl differintegral. -This is very similar to the Riemann-Louiville differintegral. The most important difference is that its upper bound is infinity.
see for more info: Weyl differintegral.
Any function can be defined in a space isomorphic to a space which it has been shown to be defined in. We therefore define the differintegral via its behavior in certain transformed spaces corresponding to some common transformations.
- The Fourier Transform. -Firstly, we define differintegration in Fourier space (using the continuous Fourier transform, here denoted F). In Fourier space, differentation transforms into a simple translation:
This easily generalizes to:
- definition
- Note, however, that there are no bounds of differintegration.
- The Laplace Transform. Under the Laplace transform, (denoted here by L), differentation transforms to a simple translation:
Generalizing to arbitrary order and solving for Dqf(t), one obtains:
- definition
- Again, there are no bounds of differintegration.
History
"An Introduction to the Fractional Calculus and Fractional Differential Equations"
- by Kenneth S. Miller, Bertram Ross (Editor)
- Hardcover: 384 pages ; Dimensions (in inches): 1.00 x 9.75 x 6.50
- Publisher: John Wiley & Sons; 1 edition (May 19, 1993)
- ASIN: 0471588849
"The Fractional Calculus; Theory and Applications of Differentiation and Integration to Arbitrary Order (Mathematics in Science and Engineering, V)"
- by Keith B. Oldham, Jerome Spanier
- Hardcover
- Publisher: Academic Press; (November 1974)
- ASIN: 0125255500
"Fractional Differential Equations. An Introduction to Fractional Derivatives, Fractional Differential Equations, Some Methods of Their Solution and Some of Their Applications." (Mathematics in Science and Engineering, vol. 198)
- by Igor Podlubny
- Hardcover
- Publisher: Academic Press; (October 1998)
- ISBN: 0125588402