Differential Eqns. (checking an answer + some questions)

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Homework Help Overview

The discussion revolves around a second-degree differential equation, specifically \( y^{\prime \prime} = xy \). The original poster presents a series solution approach using power series and seeks validation of their method and results.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to derive a recursion relation for the coefficients of a power series solution and questions the elegance of the denominators in their expressions. Other participants provide insights into the relationship of the problem to Airy functions and discuss the implications of specific coefficient values.

Discussion Status

Participants are actively engaging with the original poster's solution, offering clarifications and corrections regarding the nature of the functions involved. There is a productive exchange of ideas, but no explicit consensus has been reached on the final form of the solution.

Contextual Notes

Some participants note the complexity of the series and the potential for misinterpretation regarding the relationships between the functions discussed. The original poster's assumptions about the coefficients \( c_0 \) and \( c_1 \) are also under consideration.

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Any help is highly appreciated.

Thank you

Problem

[tex]y^{\prime \prime} = xy[/tex]

My Solution

If

[tex]y = \sum _{n=0} ^{\infty} c_n x^n \Longrightarrow xy = \sum _{n=0} ^{\infty} c_n x^{n+1} = \sum _{n=1} ^{\infty} c_{n-1} x^n[/tex]

and

[tex]y^{\prime \prime} = \sum _{n=2} ^{\infty} \left( n-1 \right) n c_n x^{n-2} = \sum _{n=0} ^{\infty} \left( n+1 \right) \left( n+2 \right) c_{n+2} x^{n}[/tex]

Then

[tex]\sum _{n=0} ^{\infty} \left( n+1 \right) \left( n+2 \right) c_{n+2} x^{n} = \sum _{n=1} ^{\infty} c_{n-1} x^n[/tex]

Hence, we may find the recursion relation

[tex]c_{n+2} = \frac{c_{n-1}}{\left( n+1 \right) \left( n+2 \right)} \qquad n=1,2,3,\ldots[/tex]

and so we have:

[tex]c_0[/tex]

[tex]c_1[/tex]

[tex]c_2[/tex]

[tex]c_3 = \frac{c_0}{2\cdot 3}[/tex]

[tex]c_4 = \frac{c_1}{3\cdot 4}[/tex]

[tex]c_5 = \frac{c_2}{4\cdot 5}[/tex]

[tex]c_6 = \frac{c_3}{5\cdot 6} = \frac{c_0}{2\cdot 3\cdot 5\cdot 6}[/tex]

[tex]c_7 = \frac{c_4}{6\cdot 7} = \frac{c_1}{3\cdot 4\cdot 6\cdot 7}[/tex]

[tex]c_8 = \frac{c_5}{7\cdot 8} = \frac{c_2}{4\cdot 5\cdot 7\cdot 8}[/tex]

[tex]\vdots[/tex]

Well, since this is a second-degree differential equation, we must have [tex]c_2 = 0[/tex]. It also follows that

[tex]c_{3n} = \frac{c_0}{2\cdot 3\cdot 5\cdot 6\cdot \cdots \cdot \left( 3n -1 \right) \left( 3n \right)} \qquad n=1,2,3,\ldots[/tex]

and

[tex]c_{3n+1} = \frac{c_1}{3\cdot 4\cdot 6\cdot 7\cdot \cdots \cdot \left( 3n \right) \left( 3n +1 \right)} \qquad n=1,2,3,\ldots[/tex]

Therefore

[tex]y = c_0 + c_1 x + c_0 \sum_{n=1} ^{\infty} \left[ \frac{x^{3n}}{2\cdot 3\cdot 5\cdot 6\cdot \cdots \cdot \left( 3n -1 \right) \left( 3n \right)} \right] + c_1 \sum_{n=1} ^{\infty} \left[ \frac{x^{3n+1}}{3\cdot 4\cdot 6\cdot 7\cdot \cdots \cdot \left( 3n \right) \left( 3n +1 \right)} \right][/tex]

Questions

1. Have I got it right? :smile:

2. If so, can I write the denominators in a more elegant way? I mean:

[tex]2\cdot 3\cdot 5\cdot 6\cdot \cdots \cdot \left( 3n -1 \right) \left( 3n \right) = \left[ 3\cdot 6\cdot 9\cdot \cdots \cdot \left( 3n \right) \right] \left[ 2\cdot 5\cdot 8\cdot \cdots \cdot \left( 3n-1 \right) \right] = n!3^n \times ( ? )[/tex]

and

[tex]3\cdot 4\cdot 6\cdot 7\cdot \cdots \cdot \left( 3n \right) \left( 3n +1 \right) = \left[ 3\cdot 6\cdot 9\cdot \cdots \cdot \left( 3n \right) \right] \left[ 4\cdot 7\cdot 10\cdot \cdots \cdot \left( 3n+1 \right) \right] = n!3^n \times ( ? )[/tex]

where [tex]( ? )[/tex] represents the other factor which I haven't been able to figure out so far.
 
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You essentially have it! With a little reworking you can put it into the standard form of the Airy functions (your equation is Airy's DE which describes waves traveling in a medium with a linear variation in density or water waves with linear variation of the depth, e.g.).

It's a bit much to LaTeX so you can just look here for details: http://functions.wolfram.com/BesselAiryStruveFunctions/AiryAi/06/01/01/
 
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Thanks for your input. I've just checked out that website. The formulas there are a bit scary, but then I looked up a problem in my calc book about the Airy function. It looks simpler:

[tex]A(x) = 1 + \frac{x^3}{2\cdot 3} + \frac{x^6}{2\cdot 3\cdot 5\cdot 6} + \frac{x^9}{2\cdot 3\cdot 5\cdot 6\cdot 8\cdot 9} +\cdots[/tex]

Anyway, it seems to me that I get to [tex]A(x)[/tex] from

[tex]y = c_0 + c_1 x + c_0 \sum_{n=1} ^{\infty} \left[ \frac{x^{3n}}{2\cdot 3\cdot 5\cdot 6\cdot \cdots \cdot \left( 3n -1 \right) \left( 3n \right)} \right] + c_1 \sum_{n=1} ^{\infty} \left[ \frac{x^{3n+1}}{3\cdot 4\cdot 6\cdot 7\cdot \cdots \cdot \left( 3n \right) \left( 3n +1 \right)} \right][/tex]

if I let [tex]c_0 = 1[/tex] and [tex]c_1 = 0[/tex].

Regards
 
That works! By the way, the functions are usually indicated as Ai(x) and Bi(x) [not A(x) and B(x)] with Ai(x) going to 0 as x -> infinity while Bi(x) diverges in that limit.
 
Let me see how that works...

We get [tex]A_i (x)[/tex] if [tex]c_0 = 1[/tex] and [tex]c_1 = 0[/tex]. Conversely, [tex]B_i (x)[/tex] is obtained if [tex]c_0 = 0[/tex] and [tex]c_1 = 1[/tex].
 
Actually, no. The Ai and Bi are combinations of the two infinite series you wrote. One of those grows and the other one decays as x -> +infinity. I misspoke (miswrote) eariler when I compared your A(x) with Ai(x) - they are not the same.
 

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