Cauchy’s formula for repeated integration is shown to be valid for the function
R(t) = (q)tq1Eq;q((q)tq)
where and q are given positive constants with q 2 (0; 1), is the Gamma function, and Eq;q is a Mittag-
Leffler function. The function R is important in the study of Volterra integral equations because it is the
unique continuous solution of the so-called resolvent equation
R(t) = tq1
Z t
0
(t s)q1R(s) ds
on the interval (0;1). This solution, commonly called the resolvent, is used to derive a formula for the
unique continuous solution of the Riemann-Liouville fractional relaxation equation
Dqx(t) = ax(t) + g(t) (a > 0)
on the interval [0;1) when g is a given polynomial. This formula is used to solve a generalization of the
equation of motion of a falling body. The last example shows that the solution of a fractional relaxation
equation may be quite elementary despite the complexity of the resolvent.
Cauchy’s formula for repeated integration fractional differential equations Mittag-Leffler functions relaxation equations resolvents Riemann-Liouville operators Volterra integral equations
Birincil Dil | İngilizce |
---|---|
Konular | Matematik |
Bölüm | Articles |
Yazarlar | |
Yayımlanma Tarihi | 25 Mart 2018 |
Yayımlandığı Sayı | Yıl 2018 Cilt: 2 Sayı: 1 |