Solving nonlinear singular differential equations

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SUMMARY

This discussion focuses on solving nonlinear singular differential equations, specifically the Lane-Emden equation. The key method involves selecting initial values that allow trajectories to navigate through the vector field without encountering singularities. The conversation highlights the importance of classifying singularities into attractors, repellers, and intersecting trajectories to handle them effectively. Additionally, the robustness of numerical solutions is emphasized, particularly how variations in initial values affect the trajectories.

PREREQUISITES
  • Understanding of nonlinear differential equations, specifically the Lane-Emden equation.
  • Familiarity with boundary value problems and initial conditions.
  • Knowledge of vector fields and their representation in differential equations.
  • Basic numerical methods for solving differential equations.
NEXT STEPS
  • Research techniques for classifying singularities in differential equations.
  • Learn about numerical methods for solving nonlinear differential equations, focusing on stability and robustness.
  • Explore the concept of vector fields in the context of ordinary differential equations (ODEs).
  • Investigate the implications of varying initial conditions on the solutions of differential equations.
USEFUL FOR

Mathematicians, physicists, and engineers working with nonlinear differential equations, as well as students studying advanced differential equations and numerical methods.

wasi-uz-zaman
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TL;DR
how to tackle singularity in the differential equations
hi, i am going through differential equations which are nonlinear and singular - like Lane-Emden equation etc.
my question is how to tackle singularity - while coding.
regards
 
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What method are you using to solve these equations?

If you solve <br /> \frac{1}{r^{n-1}} \frac{d}{dr}\left(r^{n-1}\frac{d\theta}{dr}\right) = -\theta^m for n = 2 or 3 subject to \theta(0) =1 and \theta&#039;(0) = 0 then there is no difficulty: The singular point is at the origin, but you aren't enforcing the ODE there because \theta and \theta&#039; are fixed by the boundary conditions.
 
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I like to think of the solutions of an ODE as a vector field. @pasmith's answer means to avoid singularities by choosing initial values, i.e. trajectories which lead you through the field without encountering singularities.

If you still consider the entire field, then there are certain types of singularities: attractors, repellers, or intersecting trajectories, maybe even isolated points. Such a classification allows handling different types of singularities differently. It's always the same: what is the situation and what is the goal?

If you approach it numerically, then you have to consider how robust a solution is. This means if you vary the initial values, how much do the trajectories vary? Again a matter of the given situation and goal.
 
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Yes, I remember the idea of solutions as a vector field being a revelation for me. I was fortunate that this notion was introduced in my initial ODE course.
 
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