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Stability of solutions to PDEs through the numerical evaluation of the Evans function

Department of Mathematics Stability of solutions to PDEs through the numerical evaluation of the Evans function S. Lafortune College of Charleston Collaborators: J. Lega, S. Madrid-Jaramillo, S. Balasuriya, and J. Hornibrook Plan of Talk Toy example: KdV First Model : Kirchhoff rods.

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Stability of solutions to PDEs through the numerical evaluation of the Evans function

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  1. \ Department of Mathematics Stability of solutions to PDEs through the numerical evaluation of the Evans function S. Lafortune College of Charleston Collaborators: J. Lega, S. Madrid-Jaramillo, S. Balasuriya, and J. Hornibrook

  2. Plan of Talk • Toy example: KdV • First Model: Kirchhoff rods. • Existence: analytic • Stability: Evans Function (numerical) • Second model: Combustion • Existence and Stability: Numerical

  3. Toy example: KdV • KdV • Model for shallow water:

  4. Toy example: KdV • KdV • Traveling solution

  5. Toy example: KdV • Solution

  6. Toy example: KdV • Solution: Perturbed

  7. Toy example: KdV • Solution: Perturbation mode

  8. Toy example: KdV • Solution: Perturbation mode

  9. Toy example: KdV • Solution: Perturbation mode

  10. Toy example: KdV • Eqn for perturbation Plug in Into KdV First order in w

  11. Toy example: KdV • Eigenvalue problem where The solution is unstable if there is an eigenvalue on the right side of the complex plane

  12. Toy example: KdV • Eigenvalue problem turned into a dynamical system The solution is unstable this system has a bounded solution For  positive

  13. Model: Kirchhoff Rods • Elastic rods • One-dimensional elastic structure that offers resistance to bending and torsion. A rod can be twisted and/or bent. • A description of a rod is obtained by specifying • Ribbon geometry • Mechanics • Elasticity Ref: Antman‘s book(‘95)

  14. Coiling Bifurcation • Amplitude equations: For the inextensible, unshearable model. • A: Amplitude of deformation • B: Amplitude of twist • A and B are coupled. Ref: Goriely and Tabor (‘96, ‘97, ‘98)

  15. Pulse Solutions: Existence • Form of solutions

  16. Coiling Bifurcation: Pulses

  17. Coiling Bifurcation: Pulses Ref: Numerics by Lega and Goriely (‘00)

  18. Evans Function • Perturb Solution

  19. Evans Function

  20. Evans Function • The asymptotic matrix • Eigenvalues and eigenvectors known explicitly • 3-dim stable space

  21. Evans Function

  22. Evans Function

  23. Evans Function

  24. Evans Function

  25. Evans Function: Numerical Study Values of E() on a closed contour

  26. Evans Function: Numerical Study Evans function on the real axis

  27. Evans Function: Numerical Study • For each value of , find numerically 3 solutions converging at +∞ and 3 solutions at -∞ • Calculate the determinant of the initial conditions • Calculate E() on the boundary of a closed box • Number of zeros in the box is given by

  28. Evans Function: Analytical Results • Solve the linearization at the origin using symmetries • Expand the solutions of the linearization in  • Get the first nonzero derivative of E() • Instability result using the behavior of the Evans function as  approaches 

  29. Evans Function: Analytical Results

  30. Hamiltonian Formulation • Recall • Hamiltonian structure

  31. Hamiltonian Formulation: Strategy • Hamiltonian system: • Noether Theorem: • Lagrange multiplier problem: Ref: Grillakis, Shatah and Strauss (’87 and ‘90)

  32. Hamiltonian Formulation: Strategy • ‘‘Infinite-dimensional Hessian’’ • Only one negative eigenvalue • Continuous spectrum positive, bounded away from zero • One-dimensional Kernel Ref: Grillakis, Shatah and Strauss (’87 and ‘90)

  33. Stability Condition Ref: Grillakis, Shatah and Strauss (’87 and ‘90)

  34. Infinite-dimensional Hessian Fundamental step: ‘‘Infinite-dimensional Hessian’’ • 2-dim Kernel generated by generators of Lie algebra

  35. Infinite-dimensional Hessian • One negative eigenvalue Reduction of the operator, symmetry arguments and Sturm-Liouville theory • But: continuous spectrum touches the origin • Theorems of Grillakis, Shatah, Strauss extended to include this fact  Spectral stability only

  36. Theorems

  37. Spectral Stability Criterion

  38. Conclusions • Study of amplitude equations: coupled Klein-Gordon equations • Explicit conditions for stability of pulses • Numerical Evans

  39. Beyond • This technique can be applied to generalizations with tension mode and extensibility (work in progress with Tabor and Goriely) • Use same technique for Kirchhoff

  40. Evans Function • The Evans function vanishes on the point spectrum of a linear operator. • Stability results for the FitzHugh-Nagumo equations, the generalized KDV, Benjamin-Bona-Mahoey equation, the Boussinesq, the MKDV, the complex Ginzburg-Landau equation. • Our point of view: Evans function defined as a determinant

  41. Evans Function • Consider a Linear ODE • A value of λ is an eigenvalue if there exists a solution φ such that • φis an eigenvector

  42. Evans Function

  43. Evans Function

  44. Evans Function

  45. Evans Function

  46. Evans Function

  47. Evans Function: Numerical Study Values of E(λ) on a closed contour

  48. Evans Function: Numerical Study Evans function on the real axis

  49. Conclusions • Hamiltonian methodgave a stability criterion • The Evans function method gave precise info on the mechanism by which instabilities appear • The numerical method presented here can be applied to other cases. It presents several advantages w/r to other more traditional methods

  50. Evans Function: Numerical Study • For each value of , find numerically 3 solutions converging at +∞ and 3 solutions at -∞ • Calculate the determinant of the initial conditions • Calculate E() on the boundary of a closed box • Number of zeros in the box is given by

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