Solving Nonlinear First Order Differential Equations | Methods and Techniques

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Discussion Overview

The discussion focuses on methods and techniques for solving a specific first-order nonlinear differential equation of the form y' + ay^2 = bx. Participants explore various approaches, including substitutions and transformations, while addressing the complexities involved in finding solutions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant, danmag, questions the solvability of the equation, suggesting it may not be solvable due to its nonlinear nature.
  • Another participant identifies the equation as a Riccati differential equation and suggests a substitution v = 1/y to facilitate solving it.
  • A different participant elaborates on the Riccati form and proposes converting it to a second-order ODE using the substitution y = u'/Ru, mentioning potential solution methods like power series or Airy functions.
  • Further complexity is introduced by another participant who raises questions about the relationship between power-series solutions and Airy functions, as well as the process for solving an initial value problem (IVP) related to the Riccati equation.
  • One participant discusses reducing the equation to a different form and applying the Fourier Transform, leading to a solution involving an integral that may be simplified using Euler's formula.

Areas of Agreement / Disagreement

Participants express differing views on the solvability and methods for tackling the equation, with no consensus reached on a definitive approach or solution. The discussion remains unresolved with multiple competing ideas presented.

Contextual Notes

Participants mention various methods and transformations, but the discussion includes unresolved mathematical steps and dependencies on specific assumptions or definitions related to the differential equation.

danmag
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Hi,
As far as I know this is a first order, nonlinear diff eqn with both dependent and dependent variables...so it is not solvable??

y'+ay^2 = bx

If anybody knows if there is a method to solving it, please let me know.

Thanks,
danmag
:confused:
 
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I think this is a Ricatti diff eqn. Its like the Bernouilli equation, but with nonhomogenous parts (its a bit of a pain if I recall right, you need to do some guessing).

But anyway make the substitution v = 1/y and go from there.
 
As Haelfix mentioned, it's a Riccati equation of the form:

[tex]y^{'}+Q(x)y+R(x)y^2=P(x)[/tex]

So use the standard approach:

[tex]y=\frac{u^{'}}{Ru}[/tex]

to convert it to a second-order ODE with variable coefficients. This then can be solved via power series or just bust it up directly with Airy functions (equal . . . nevermind).:rolleyes:
 
Know what, this turned out to be a quagmire. But very interesting nevertheless. For example:

1. What is the relationship between the power-series solution of the reduced Riccati equation:

[tex]u^{''}-abxu=0[/tex]

and the solution expressed in terms of Airy functions?

(not easy)

2. Using the solutions above, how then does one proceed to solve an IVP for the original Riccati equation:

[tex]y^{'}+ay^{2}=bx,\quad y(0)=a[/tex]

(just barely)

3. What is the relationship between the Airy function expressed in terms of a hypergeometric series and the integral expression for the Airy function:

[tex]Ai(x)=\frac{1}{3^{2/3}\Gamma(2/3)} F_1(2/3,z^3/9)-\frac{z}{3^{1/3}\Gamma(1/3)}F_1(4/3,z^3/9)[/tex]

[tex]Ai(x)=\frac{1}{\pi}\int_0^{\infty}Cos[t^3/3+xt]dt[/tex]

(not even close)

See . . . quagmire.
 
Last edited:
More complex contours:

So I reduce the equation down to:

[tex]u^{''}-axy=0[/tex]

Now, consider the Fourier Transform of u(x):

[tex]g(\xi)=\mathcal{F}\left\{u\right\}=<br /> \frac{1}{\sqrt{2\pi}}\int_{-\infty}^{\infty}u(x)e^{-i\xi x}dx[/tex]

So I'll take the Fourier transform of the DE and noting:

[tex]\mathcal{F}\left\{xu(x)\right\}=i\frac{dg}{d\xi}[/tex]

I obtain:

[tex]-\xi^2 g-ia\frac{dg}{d\xi}=0[/tex]

That's a piece of cake to solve and yields:

[tex]g(\xi)=Ce^{i(\xi^3/(3ai)}[/tex]

Now, inverting the transform:

[tex]u(x)=\frac{C}{\sqrt{2\pi}}\int_{-\infty}^{\infty} e^{i(\xi^3/(3a)+\xi x)}d\xi[/tex]

That's close. :smile: Looks like I can just split up the integral via Euler's formula to get a Cos and iSin. That might be all there is to it but need to check . . .
 
Last edited:

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