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Open AccessFeature PaperArticle
On Asymptotic Series for Generalized Airy, Circular, and Hyperbolic Functions
by
Luiz M. B. C. Campos
Luiz M. B. C. Campos 1,†
and
Manuel J. S. Silva
Manuel J. S. Silva 1,2,*,†
1
CCTAE, IDMEC, LAETA, Instituto Superior Técnico, Universidade de Lisboa, Av. Rovisco Pais 1, 1049-001 Lisboa, Portugal
2
Atlântica, Instituto Universitário, Fábrica da Pólvora de Barcarena, 2730-036 Barcarena, Portugal
*
Author to whom correspondence should be addressed.
†
These authors contributed equally to this work.
Submission received: 2 November 2025
/
Revised: 15 December 2025
/
Accepted: 18 December 2025
/
Published: 23 December 2025
Abstract
The paper concerns the solution of the ordinary differential equation , which may be designated the generalized Airy equation, since the original Airy equation corresponds to the particular case with the + sign. The solutions may be designated generalized circular (hyperbolic) sines and cosines for the + (−) sign, since the particular case corresponds to the elementary circular (hyperbolic) sines and cosines. There are 3 cases of solution of the generalized Airy equation, depending on the parameter m: (I) for m a non-negative integer, the coefficient is an analytic function, and the solutions are also analytic series; (II) for m complex other than an integer, the coefficient has a branch point at the origin, and the solutions also have a branch point multiplied by an analytic series; (III) for m a negative integer, the coefficient has a pole of order m, and the generalized Airy equation is singular. Case III has four subcases: (III-A) for , the coefficient is a simple pole, and the solutions are Frobenius–Fuchs series of two kinds; (III-B) for , the coefficient is a double pole, and the solutions are a combination of elementary functions, namely exponential, logarithmic, and circular (hyperbolic) sine and cosine for the + (−) sign; (III-C,D) for , the coefficient is a pole of multiplicity , and the generalized Airy differential equation has an irregular singularity of degree at the origin. In the sub-cases (III-C,D), the solutions can be obtained by inversion as asymptotic series of descending powers specified by (III-C) Frobenius–Fuchs series of two kinds for a triple pole ; (III-D) for higher-order poles by generalized circular (hyperbolic) sines and cosines of . It is shown that in all cases the ascending and descending series are absolutely and uniformly convergent with the n-th term decaying like . This enables the use of a few terms of the series to obtain tables and plot graphs of the solutions of the generalized Airy differential equation as generalized circular and hyperbolic sines and cosines for several values of the parameter m. As a physical application, it is shown that the generalized circular (hyperbolic) cosines and sines specify the motion of a linear oscillator with natural frequency a power of time in the oscillatory (monotonic) case when the origin is an attractor (repeller).
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MDPI and ACS Style
Campos, L.M.B.C.; Silva, M.J.S.
On Asymptotic Series for Generalized Airy, Circular, and Hyperbolic Functions. Mathematics 2026, 14, 52.
https://doi.org/10.3390/math14010052
AMA Style
Campos LMBC, Silva MJS.
On Asymptotic Series for Generalized Airy, Circular, and Hyperbolic Functions. Mathematics. 2026; 14(1):52.
https://doi.org/10.3390/math14010052
Chicago/Turabian Style
Campos, Luiz M. B. C., and Manuel J. S. Silva.
2026. "On Asymptotic Series for Generalized Airy, Circular, and Hyperbolic Functions" Mathematics 14, no. 1: 52.
https://doi.org/10.3390/math14010052
APA Style
Campos, L. M. B. C., & Silva, M. J. S.
(2026). On Asymptotic Series for Generalized Airy, Circular, and Hyperbolic Functions. Mathematics, 14(1), 52.
https://doi.org/10.3390/math14010052
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