Time-scale calculus was introduced in 1988 by the German mathematician Stefan Hilger.[1] However, similar ideas have been used before and go back at least to the introduction of the Riemann–Stieltjes integral, which unifies sums and integrals.
Dynamic equations
Many results concerning differential equations carry over quite easily to corresponding results for difference equations, while other results seem to be completely different from their continuous counterparts.[2] The study of dynamic equations on time scales reveals such discrepancies, and helps avoid proving results twice—once for differential equations and once again for difference equations. The general idea is to prove a result for a dynamic equation where the domain of the unknown function is a so-called time scale (also known as a time-set), which may be an arbitrary closed subset of the reals. In this way, results apply not only to the set of real numbers or set of integers but to more general time scales such as a Cantor set.
The three most popular examples of calculus on time scales are differential calculus, difference calculus, and quantum calculus. Dynamic equations on a time scale have a potential for applications such as in population dynamics. For example, they can model insect populations that evolve continuously while in season, die out in winter while their eggs are incubating or dormant, and then hatch in a new season, giving rise to a non-overlapping population.
Formal definitions
A time scale (or measure chain) is a closed subset of the real line. The common notation for a general time scale is .
The two most commonly encountered examples of time scales are the real numbers and the discrete time scale .
A single point in a time scale is defined as:
Operations on time scales
The forward jump and backward jump operators represent the closest point in the time scale on the right and left of a given point , respectively. Formally:
(forward shift/jump operator)
(backward shift/jump operator)
The graininess is the distance from a point to the closest point on the right and is given by:
For a right-dense , and .
For a left-dense ,
Classification of points
For any , is:
left dense if
right dense if
left scattered if
right scattered if
dense if both left dense and right dense
isolated if both left scattered and right scattered
As illustrated by the figure at right:
Point is dense
Point is left dense and right scattered
Point is isolated
Point is left scattered and right dense
Continuity
Continuity of a time scale is redefined as equivalent to density. A time scale is said to be right-continuous at point if it is right dense at point . Similarly, a time scale is said to be left-continuous at point if it is left dense at point .
Derivative
Take a function:
(where R could be any Banach space, but is set to the real line for simplicity).
Definition: The delta derivative (also Hilger derivative) exists if and only if:
For every there exists a neighborhood of such that:
The delta integral is defined as the antiderivative with respect to the delta derivative. If has a continuous derivative one sets
Laplace transform and z-transform
A Laplace transform can be defined for functions on time scales, which uses the same table of transforms for any arbitrary time scale. This transform can be used to solve dynamic equations on time scales. If the time scale is the non-negative integers then the transform is equal[2] to a modified Z-transform:
Associated with every time scale is a natural measure[8][9] defined via
where denotes Lebesgue measure and is the backward shift operator defined on . The delta integral turns out to be the usual Lebesgue–Stieltjes integral with respect to this measure
^Davis, John M.; Gravagne, Ian A.; Marks, Robert J. II (2010). "Bilateral Laplace Transforms on Time Scales: Convergence, Convolution, and the Characterization of Stationary Stochastic Time Series". Circuits, Systems and Signal Processing. 29 (6): 1141–1165. doi:10.1007/s00034-010-9196-2. S2CID16404013.
^Bastos, Nuno R. O.; Mozyrska, Dorota; Torres, Delfim F. M. (2011). "Fractional Derivatives and Integrals on Time Scales via the Inverse Generalized Laplace Transform". International Journal of Mathematics & Computation. 11 (J11): 1–9. arXiv:1012.1555. Bibcode:2010arXiv1012.1555B.