Stabilization Problems of Unforeseen Difficulty The IHP Coron - - PowerPoint PPT Presentation

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Stabilization Problems of Unforeseen Difficulty The IHP Coron - - PowerPoint PPT Presentation

Stabilization Problems of Unforeseen Difficulty The IHP Coron Conference on Nonlinear Partial Differential Equations and Applications June 21 , 2016 Roger Brockett John A. Paulson School of Engineering and Applied Science Harvard


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Stabilization Problems of Unforeseen Difficulty The IHP Coron Conference on Nonlinear Partial Differential Equations and Applications June 21 , 2016

Roger Brockett John A. Paulson School of Engineering and Applied Science Harvard University

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We are here to honor Jean-Michel Let the festivities continue with a little WHOOP DE DOO on feedback stabilization!

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A little dictum from many years ago

As a fourth year college student I took a course called “Scientific Writing”. For the most part this consisted of submitting essays and receiving criticism in response However the professor did insist on one general principle. It takes the form of something like a contract between the author and the reader and I will try to observe it today. Here it is:

Never overestimate the prior knowledge

  • f the reader and never underestimate

the reader’s willingness to follow a logical

  • argument. Shall I explain whoop de doo?
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Sufficient conditions for the existence of a continuous, autonomous, stabilizing control

There are several versions depending on the type of feedback allowed and the type of stability of interest. Here we discuss the existence and construction of continuous, time invariant feedback control giving rise to (local) asymptotic stability. This is the only problem I intend to talk about!

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Notation

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Many questions, and a few answers

  • 1. Is there an algorithmic approach to finding a stabilizing control ?
  • 2. Can known topological conditions such as, the index of a fixed point,
  • etc. be extended in the direction of the Routh-Hurwitz test?
  • 3. Can the connection with optimal regulation be made more useful?
  • 4. Does there exist a useful classification in terms of normal forms?
  • 5. What is the best rate of convergence in a given setting, 1/t, etc. ?
  • 6. Assuming asymptotic stability, polynomial Liapunov functions exist

but what is the lowest degree possible?

  • 7. Is there a way to make simulation decisive for convergence to 0, even

for a single trajectory?

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Some (now quite old) background

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We do not wish to discuss linear or near linear cases

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Restrict attention to the critical cases The control version of “critical”

Critical cases for ODEs in the Russian literature of the 1950s

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I will assume u(0)=0; this is not quite standard

After choosing the constant we still have the problem of finding u.

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“Obvious” possibilities for attacking the problem

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Does Routh-Hurwitz help in this setting?

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13

.8 to

  • .8
  • .5 to .5

period about 3.3 make coefficients positive

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3 to

  • 3
  • 2 to 2
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15

  • 15 to 15

15 to

  • 15
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None of these work!

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Optimal Regulation and Factorization

Finding an invariant submanifold for the flow, which contains 0.

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Difficulties

Surprisingly (?), the optimal control is not continuous even though the description looks quite friendly.

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Smooth solutions of the regulator problem

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Organizing for a war of attrition

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Focus on a more specific class of problems

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How hard is it to find a suitable Liapunov function?

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The multiplicity one case follows a known pattern

Recall the Lur’e problem in feedback stability

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The higher multiplicity situation

The third order system requires two nonlinear terms but we will provide a “non Liapunov” aproach later.

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Standard forms: The invariants of matrix pairs

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Standard forms: B of rank one

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What does the KYP lemma tell us?

No restriction on the order but multiplicity <3

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Stability preserving enlargements (SPE)

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The Lemma in pictures

r(x) nonnegative x y

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Proof of Lemma part I

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Proof of Lemma part II

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Applying the lemma

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Applying the lemma

Building on the fact that the control u = x( ˙ x + x) stabilizes the null solution of ¨ x + ux = 0 we see that d

dt + x2

(¨ x + ( ˙ x + x)x2 = 0) = 0 has a asymptotically stable null solution and takes the form x(3) + 2x2¨ x + (2x ˙ x + 3x2 + x4) ˙ x + x5 = 0 Theorem: for any k ≥ 2 the null solution of x(k) + ux = 0 can be stabilized by a polynomial feedback Law.

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Summary

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Power law solutions provide insight on scale

Example of a homogenous equation of weight = -2.

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A numerical solution of

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Observe that one can give this an algebraic flavor

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Recall the index calculation

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Many questions, and a few answers

  • 1. Is there an algorithmic approach to finding a stabilizing control ?
  • 2. Can known topological conditions such as, the index of a fixed point,
  • etc. be extended in the direction of the Routh-Hurwitz test?
  • 3. Can the connection with optimal regulation be made more useful?
  • 4. Does there exist a useful classification in terms of normal forms?
  • 5. What is the best rate of convergence in a given setting, 1/t, etc. ?
  • 6. Assuming asymptotic stability, polynomial Liapunov functions exist

but what is the lowest degree possible?

  • 7. Is there a way to make simulation decisive for convergence to 0, even

for a single trajectory?

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Jean-Michel Congratulations on your many achievements! Best wishes for the years ahead!