Methods for Solving Non-Linear Second Order Systems of Differential Equations

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Discussion Overview

The discussion revolves around methods for solving a system of non-linear second order differential equations, specifically related to geodesic equations in hyperbolic space. Participants explore various approaches to find solutions, including integrating factors and trial solutions, while expressing uncertainty about the complexity of the equations involved.

Discussion Character

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

Main Points Raised

  • One participant presents a system of equations and suggests a potential solution related to geodesics in hyperbolic space.
  • Another participant successfully solves one of the equations using integrating factor methods and derives a new equation to solve.
  • Some participants discuss the implications of the proposed solution and suggest differentiating it to verify if it satisfies the original system.
  • A proposed solution of the form y(λ) = ±iαC sec(αλ + β) is introduced, with a suggestion to verify it through substitution.
  • Multiple participants mention alternative methods for solving the equations, indicating that there may be various approaches to reach a solution.
  • One participant expresses difficulty in following the final steps of the proposed methods, indicating a lack of clarity on how to proceed with integrating factors.
  • Another participant notes that if the relationship between x and y is the primary interest, a simpler method may be applicable.

Areas of Agreement / Disagreement

Participants express various methods and approaches to solving the equations, but there is no consensus on a single solution or method. Uncertainty remains regarding the best approach to take and the complexity of the equations involved.

Contextual Notes

Some participants highlight the non-linear nature of the equations and the challenges it presents, while others suggest that certain methods may simplify the problem. There are references to specific forms of the equations that may influence the choice of method.

Who May Find This Useful

Readers interested in differential equations, particularly in the context of physics and geometry, may find the exploration of various solution methods and the discussion of non-linear systems relevant.

LAHLH
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Hi,

could anyone tell me what methods I would need to solve this system:

[tex]y\frac{d^2 y}{d\lambda^2}+\left(\frac{dx}{d\lambda}\right)^2-\left(\frac{dy}{d\lambda}\right)^2=0[/tex]

[tex]\frac{y}{2}\frac{d^2x}{d \lambda ^2}-\left(\frac{dx}{d\lambda}\right)\left(\frac{dy}{d\lambda}\right)=0[/tex]

I believe the solution is [tex](x-x_0)^2+y^2=l^2[/tex]

I think (unless I've made a mistake anyway) that these are the geodesic equations for H^2, so the solutions are semicircles in the upper half plane (cf Sean Carroll). I'm not sure how to solve these however despite him saying "it is straightforward to show...", because they seem to be non linear and second order.

Thanks
 
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I've managed to solve the second equation using integrating factor methods.

If we write [tex]u=\frac{dx}{d\lambda}[/tex] then the second equation is:

[tex]\frac{du}{d\lambda}+\left[-\frac{2}{y}\left(\frac{dy}{d\lambda}\right)\right] u=0[/tex]

So now this is of the form [tex]u' (\lambda)+P(\lambda) u(\lambda) =0[/tex] and we can use int factors. Which we can find as [tex]M(\lambda)=exp\left[\int -\frac{2}{y}\left(\frac{dy}{d\lambda}\right) d\lambda\right]=\frac{1}{y^2}[/tex]

So multiplying our equation by this leads to:

[tex]\frac{1}{y^2}\frac{du}{d\lambda}-\frac{2}{y^3}\left(\frac{dy}{d\lambda}\right) u=0[/tex]

or

[tex]\frac{d}{d\lambda} \left[\frac{1}{y^2} u\right] =0[/tex]

from which we find [tex]u=\frac{1}{C} y^2[/tex]

So now we have [tex]\frac{dx}{d\lambda}=\frac{1}{C} y^2[/tex] we can plug this in equation one to obtain:

[tex]\frac{d^2 y}{d\lambda^2}-\frac{1}{y}\left(\frac{dy}{d\lambda}\right)^2+\frac{y^3}{C^2}=0[/tex]

So now I just need to solve this second order non linear equation.
 
LAHLH said:
I'm not sure how to solve these however despite him saying "it is straightforward to show...", because they seem to be non linear and second order.

Thanks

You sure that doesn't mean, "it is straightforward to show that this solution solves the system?"

If so, then you can take the solution:

[tex](x-x_0)^2+y^2=a^2[/tex]

differentiate once and twice, solve for x' and x'', back-substitute into the second equation, then by using the first equation show the second equation is zero and thereby show the solution satisfies the second equation. And I assume you can do likewise for the first and therefore show it's pretty straightforward to show that solution satisfies the system.
 
jackmell said:
You sure that doesn't mean, "it is straightforward to show that this solution solves the system?"

If so, then you can take the solution:

[tex](x-x_0)^2+y^2=a^2[/tex]

differentiate once and twice, solve for x' and x'', back-substitute into the second equation, then by using the first equation show the second equation is zero and thereby show the solution satisfies the second equation. And I assume you can do likewise for the first and therefore show it's pretty straightforward to show that solution satisfies the system.

you are probably correct that he did mean just do this I suppose. I guess now I've come this far I'd like to solve it explicitely however. I think it should be do able despite it being non linear, as their is no lambda factors, y'' is just a function of y' and y
 
Your second-order equation

[tex]y^{\prime \prime} - \frac{y^{\prime 2}}{y} + \frac{y^3}{C^2} = 0[/tex]

probably has many solutions, but there is a simple solution of the form

[tex]y(\lambda) = \pm i \alpha C \sec{(\alpha \lambda + \beta)}[/tex]

where [tex]\alpha[/tex] and [tex]\beta[/tex] are constants. You can show this very easily by substitution of a trial solution of the form

[tex]y(\lambda) = A \sec{(\alpha \lambda + \beta)}[/tex].
 
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Another way to solve it. Simpler on my opinion.
The first part is presented in attachment.
The ODE obtained isn't very difficult to be solved. I have not enough time this evening to write it up. Next part for tomorrow.
 

Attachments

  • EDOsystem-First part.JPG
    EDOsystem-First part.JPG
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JJacquelin said:
Another way to solve it. Simpler on my opinion.
The first part is presented in attachment.
The ODE obtained isn't very difficult to be solved. I have not enough time this evening to write it up. Next part for tomorrow.

Man that is so slick. :)

So then we get:

[tex]yy''+c^2y^4-\left(y'\right)^2=0[/tex]

Don't know what Jacquelin has in mind but I would then let p=y' and obtain:

[tex]yp\frac{dp}{dy}+c^2y^4-p^2=0[/tex]

or:

[tex](c^2y^4-p^2)dy+(yp)dp=0[/tex]

for which I think an integrating factor is [itex]\frac{1}{y^3}[/tex] which will then make the equation exact and we can solve it using that method.[/itex]
 
The method proposed by jackmell would probably solve the EDO.
My method is not exactly the same, but the result is obtained anyway.
 

Attachments

  • ODEsystem-Second part.JPG
    ODEsystem-Second part.JPG
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If we are not interested to explicitly know x and y as function of lambda, but if we only are interested to know the relationship between x and y, then a much simpler method is possible :
 

Attachments

  • EDOsystem-third part.JPG
    EDOsystem-third part.JPG
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  • #10
These are great thanks a lot. I must be being stupid, and I follow both your arguments upto the last line, but I can't quite see how to solve your final equations with integrating factors, e.g. for [tex]\frac{d^2h}{dx^2}+\frac{1}{h}\left(\frac{dh}{dx}\right)^2+\frac{1}{h}=0[/tex] how does one procede?

I assumed from here you would need to make a substitution [tex]p=h'[/tex] which leads me to [tex]h''=\frac{dh}{dx}=\frac{dp}{dh}\frac{dh}{dx}=pp'[/tex] so
[tex]pp'h+p^2+1=0[/tex] but this isn't the standard form I'm used to for finding integrating factors.

EDIT: actually is it just seperable?
 
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  • #11
Just note that h*h''+(h')² = (h*h')'
(h*h')' = -1
h*h' = -x+x_0
etc.

In fact, what is done in my preceeding post is only to eliminate lambda from the two primary ODE.
 

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