On Asymptotic Series for Generalized Airy, Circular, and Hyperbolic Functions

The paper concerns the solution of the ordinary differential equation y″±xmy=0, which may be designated the generalized Airy equation, since the original Airy equation corresponds to the particular case m=1 with the + sign. The solutions may be designated generalized circular (hyperbolic) sines and cosines for the + (−) sign, since the particular case m=0 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 xm is an analytic function, and the solutions are also analytic series; (II) for m complex other than an integer, the coefficient xm 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 xm has a pole of order m, and the generalized Airy equation is singular. Case III has four subcases: (III-A) for m=−1, the coefficient x−1 is a simple pole, and the solutions are Frobenius–Fuchs series of two kinds; (III-B) for m=−2, 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 m=−3,−4,…, the coefficient is a pole of multiplicity m, and the generalized Airy differential equation has an irregular singularity of degree m−2 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 m=−3; (III-D) for higher-order poles m=−4,−5,… by generalized circular (hyperbolic) sines and cosines of 1/x. It is shown that in all cases the ascending and descending series are absolutely and uniformly convergent with the n-th term decaying like On2. 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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Journal
Mathematics
Published
2025-12-23
DOI
https://doi.org/10.3390/math14010052
Primary Topic
Advanced Mathematical Theories
Type
article
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article

On Asymptotic Series for Generalized Airy, Circular, and Hyperbolic Functions

Luiz M. B. C. Campos, Manuel J. S. Silva
Mathematics
Advanced Mathematical Theories
article

On Asymptotic Series for Generalized Airy, Circular, and Hyperbolic Functions

Luiz M. B. C. Campos, Manuel J. S. Silva
article en

Abstract

The paper concerns the solution of the ordinary differential equation y″±xmy=0, which may be designated the generalized Airy equation, since the original Airy equation corresponds to the particular case m=1 with the + sign. The solutions may be designated generalized circular (hyperbolic) sines and cosines for the + (−) sign, since the particular case m=0 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 xm is an analytic function, and the solutions are also analytic series; (II) for m complex other than an integer, the coefficient xm 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 xm has a pole of order m, and the generalized Airy equation is singular. Case III has four subcases: (III-A) for m=−1, the coefficient x−1 is a simple pole, and the solutions are Frobenius–Fuchs series of two kinds; (III-B) for m=−2, 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 m=−3,−4,…, the coefficient is a pole of multiplicity m, and the generalized Airy differential equation has an irregular singularity of degree m−2 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 m=−3; (III-D) for higher-order poles m=−4,−5,… by generalized circular (hyperbolic) sines and cosines of 1/x. It is shown that in all cases the ascending and descending series are absolutely and uniformly convergent with the n-th term decaying like On2. 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).

MathematicsVol. 14(1)
University of Lisbon (PT), Atlântica Instituto Universitário (PT)
Openalex Percentile: Top 23%
Advanced Mathematical Theories
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