Math 2.0

Ordinary differential equations Complex domain and special equations Example

Airy equation

Example

The Airy equation is y′′−z y=0.y'' - z\, y = 0. Its coefficients are polynomials, so every point of ℂ\C is an ordinary point, and all solutions are entire functions. A power series solution y=∑k≥0akzky = \sum_{k \ge 0} a_k z^k gives 2a2=02 a_2 = 0 and (k+2)(k+1) ak+2=ak−1for k≥1.(k + 2)(k + 1)\, a_{k+2} = a_{k-1} \quad \text{for } k \ge 1. With a0=1a_0 = 1 and a1=0a_1 = 0 one gets y1=1+z36+z6180+⋯y_1 = 1 + \frac{z^3}{6} + \frac{z^6}{180} + \cdots. With a0=0a_0 = 0 and a1=1a_1 = 1 one gets y2=z+z412+z7504+⋯y_2 = z + \frac{z^4}{12} + \frac{z^7}{504} + \cdots. They are linearly independent, since their Wronskian at 00 is y1(0)y2′(0)−y1′(0)y2(0)=1y_1(0) y_2'(0) - y_1'(0) y_2(0) = 1.

Remarks

The standard solutions are the Airy functions Ai⁡\operatorname{Ai} and Bi⁡\operatorname{Bi}, which are fixed linear combinations of y1y_1 and y2y_2. For real x→+∞x \to +\infty, Ai⁡(x)\operatorname{Ai}(x) decays like exp⁡(−23x3/2)\exp\left( -\frac{2}{3} x^{3/2} \right) up to a power of xx, and Bi⁡(x)\operatorname{Bi}(x) grows like exp⁡(23x3/2)\exp\left( \frac{2}{3} x^{3/2} \right). For x→−∞x \to -\infty, both oscillate with an amplitude that decays like ∣x∣−1/4\abs{x}^{-1/4}. The point ∞\infty is an irregular singular point, and Ai⁡\operatorname{Ai} is the classical example of the Stokes phenomenon.

Further reading

  1. Web https://en.wikipedia.org/wiki/Airy_function
About this page
TagPNESAD6R5T
URIm2://PNESAD6R5T
Kindexample
WritingW0 stub
MSC34B30, 33C10, 34M03
IllustratesOrdinary point and singular point, Power series solution
Changed2 November 2026

Markdown · JSON · Edit on GitHub

What this page needs for W1

  • an inventory row: the row of the inventory that the node accounts for (0 of 1)
  • a source with a locator (0 of 1)

The writing levels say how complete the text of a page is. They do not measure its truth.

What links here

No page links to this page yet.