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Further stabilization and exact observability results for voltage-actuated piezoelectric beams with magnetic effects

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Abstract

It is well known that magnetic energy of the piezoelectric beam is relatively small, and it does not change the overall dynamics. Therefore, the models, relying on electrostatic or quasi-static approaches, completely ignore the magnetic energy stored/produced in the beam. A single piezoelectric beam model without the magnetic effects is known to be exactly observable and exponentially stabilizable in the energy space. However, the model with the magnetic effects is proved to be not exactly observable/exponentially stabilizable in the energy space for almost all choices of material parameters. Moreover, even strong stability is not achievable for many values of the material parameters. In this paper, it is shown that the uncontrolled system is exactly observable in a space larger than the energy space. Then, by using a \(B^*\)-type feedback controller, explicit polynomial decay estimates are obtained for more regular initial data. Unlike the classical counterparts, this choice of feedback corresponds to the current flowing through the electrodes, and it matches better with the physics of the model. The results obtained in this manuscript have direct implications on the controllability/stabilizability of smart structures such as elastic beams/plates with piezoelectric patches and the active constrained layer (ACL) damped beams/plates.

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References

  1. Alabau F, Cannarsa P, Komornik V (2002) Indirect internal stabilization of weakly coupled evolution equations. J Evol Equ 2–2:127–150

    Article  MathSciNet  Google Scholar 

  2. Alabau-Boussouira F, Lautaud M (2012) Indirect stabilization of locally coupled wave-type systems. ESAIM COCV 18–2:548–582

    Article  Google Scholar 

  3. Alabau-Boussouira F (2003) A two-level energy method for indirect boundary observability and controllability of weakly coupled hyperbolic systems SIAM. J Control Optim 42–3:871–906

    Article  MathSciNet  Google Scholar 

  4. Ammar-Khodja F, Benabdallah A, Gonzlez-Burgos M, de Teresa L (2011) Recent results on the controllability of linear coupled parabolic problems: a survey. Math Control Relat Fields 1–3:267–306

    Article  Google Scholar 

  5. Ammar Khodja F, Benabdallah A, Gonzlez-Burgos M, de Teresa L (2013) A new relation between the condensation index of complex sequences and the null controllability of parabolic systems. C R Math Acad Sci Paris 351(19–20):743–746

    Article  MATH  MathSciNet  Google Scholar 

  6. Ammari K, Tucsnak M (2001) Stabilization of second order evolution equations by a class of unbounded feedbacks. ESAIM COCV 6:361–386

    Article  MATH  MathSciNet  Google Scholar 

  7. Avdonin S, Moran W (2001) Ingham-type inequalities and Riesz bases of divided differences. Int J Appl Math Comput Sci 11–4:803–820

    MathSciNet  Google Scholar 

  8. Avdonin S, Moran W (2002) Riesz bases of exponentials and divided differences. St Petersburg Math J 13–3:339–351

    Google Scholar 

  9. Baiocchi C, Komornik V, Loreti P (2002) Ingham-Beurling type theorems with weakened gap conditions. Acta Math Hungar 97:55–95

    Article  MATH  MathSciNet  Google Scholar 

  10. Banks HT, Smith RC, Wang Y (1996) Smart material structures: Modelling. Estimation and Control, Mason, Paris 1996

  11. Baz A (1996) Active Constrained Layer Damping, US Patent # 5,485,053

  12. Bégout P, Soria F (2007) A generalized interpolation inequality and its application to the stabilization of damped equations. J Differ Equ 240–2:324–356

    Article  Google Scholar 

  13. Bernik VI, Dodson MM (1999) Metric Diophantine Approximation on Manifolds. Cambridge University Press, Cambridge

    Book  MATH  Google Scholar 

  14. Cassels JW (1966) An Introduction to Diophantine Approximation. Cambridge University Press, Cambridge

    Google Scholar 

  15. Castro C, Zuazua E (1998) Boundary controllability of a hybrid system consisting in two flexible beams connected by a point mass. SIAM J Control Optim 36–5:1576–1595

    Article  MathSciNet  Google Scholar 

  16. Dager R, Zuazua E (2006) Wave propagation, Observation and Control in 1-d Flexible Multi-structures, Springer

  17. Destuynder PH, Legrain I, Castel L, Richard N (1992) Theoretical, numerical and experimental discussion of the use of piezoelectric devices for control-structure interaction. Eur J Mech A Solids 11:181–213

    MathSciNet  Google Scholar 

  18. Hansen SW (2004) Several Related Models for Multilayer Sandwich Plates. Math Models Methods Appl Sci 14–8:1103–1132

    Article  Google Scholar 

  19. Hansen SW, Özer AÖ (2010) Exact boundary controllability of an abstract Mead-Marcus Sandwich beam model. In: The Proceedings of 49th IEEE Conf. on Decision & Control, Atlanta, USA, pp 2578–2583

  20. Jaffard S, Tucsnak M (1997) Regularity of plate equations with control concentrated in interior curves. Proc R Soc Edinb Sect A 127:1005–1025

    Article  MATH  MathSciNet  Google Scholar 

  21. Jaffard S, Tucsnak M, Zuazua E (1998) Singular internal stabilization of the wave equation. J Differ Equ 145–1:184–215

    Article  MathSciNet  Google Scholar 

  22. Kapitonov B, Miara B, Menzala GP (2007) Boundary observation and exact control of a quasi-electrostatic piezoelectric system in multilayered media. SIAM J Control Optim 46–3:1080–1097

    Article  MathSciNet  Google Scholar 

  23. Komornik V, Loreti P (2005) Fourier Series in Control Theory. Springer, New York

    MATH  Google Scholar 

  24. Lions JL (1988) Exact Controllability, stabilization and perturbations for distributed parameter systems. SIAM Rev 30–1:1–68

    Article  Google Scholar 

  25. Luca F, de Teresa L (2013) Control of coupled parabolic systems and Diophantine approximations. SEMA J 61:1–17

    Article  MATH  Google Scholar 

  26. Miller SJ, Takloo-Bighash R (2006) An Invitation to Modern Number Theory. Princeton University Press, Princeton

    MATH  Google Scholar 

  27. Morris KA, Özer AÖ (2014) Comparison of stabilization of current-actuated and voltage-actuated piezoelectric beams. In: The Proceedings of 53rd IEEE Conference on Decision & Control, Los Angeles, USA, pp 571–576

  28. Morris KA, Özer AÖ (2013) Strong stabilization of piezoelectric beams with magnetic effects. In: The Proceedings of 52nd IEEE Conference on Decision & Control, Firenze, Italy, pp 3014–3019

  29. Morris KA, Özer AÖ (2014) Modeling and stabilizability of voltage-actuated piezoelectric beams with magnetic effects. SIAM J Control Optim 52–4:2371–2398

    Article  Google Scholar 

  30. Özer AÖ, Hansen SW (2014) Exact boundary controllability results for a multilayer Rao-Nakra sandwich beam. SIAM J Control Optim 52–2:1314–1337

    Article  Google Scholar 

  31. Özer AÖ, Hansen SW (2013) Uniform stabilization of a multi-layer Rao-Nakra sandwich beam. Evol Equ Control Theory 2–4:195–210

    Google Scholar 

  32. Özer AÖ, Morris KA (2014) Modeling an elastic beam with piezoelectric patches by including magnetic effects. In: The Proceedings of the American Control Conference, Portland, USA, pp 1045–1050

  33. Rogacheva N (1994) The Theory of Piezoelectric Shells and Plates. CRC Press, Boca Raton

    Google Scholar 

  34. Russell DL (1986) The DirichletNeumann boundary control problem associated with Maxwells equations in a cylindrical region. SIAM J Control Optim 24:199–229

    Article  MATH  MathSciNet  Google Scholar 

  35. Scott WT (1940) Approximation to real irrationals by certain classes of rational fractions. Bull Am Math Soc 46:124–129

    Article  Google Scholar 

  36. Smith RC (2005) Smart Material Systems: Model Development. SIAM, Philadelphia

  37. Tiersten HF (1969) Linear piezoelectric plate vibrations. Plenum Press, New York

    Book  Google Scholar 

  38. Triebel H (1978) Interpolation Theory, Function Spaces. Differential Operators, North-Holland, Amsterdam

  39. Tucsnak M (1996) Regularity and exact controllability for a beam with piezoelectric actuator. SIAM J Control Optim 34:922–930

    Article  MATH  MathSciNet  Google Scholar 

  40. Tucsnak M (1996) Control of plate vibrations by means of piezoelectric actuators. Discret Contin Dyn Syst 2:281–293

    Article  MATH  MathSciNet  Google Scholar 

  41. Tucsnak M, Weiss G (2001) Simultaneous controllability in sharp time for two elastic strings. ESAIM Control Optim Calc Var 6:259–273

    Article  MATH  MathSciNet  Google Scholar 

  42. Tucsnak M, Weiss G (2009) Observation and Control for Operator Semigroups. Birkhuser Verlag, Basel

    Book  MATH  Google Scholar 

  43. Tzou HS (1993) Piezoelectric shells, Solid Mechanics and Its applications 19. Kluwer Academic, The Netherlands

    Google Scholar 

  44. Ulrich D (1980) Divided Differences and Systems of Nonharmonic Fourier Series. Proc Am Math Soc 80(1):47–57

    Article  MathSciNet  Google Scholar 

  45. Yang J (2005) An Introduction to the Theory of Piezoelectricity. Springer, New York

    MATH  Google Scholar 

  46. Yang J (2006) A review of a few topics in piezoelectricity. Appl Mech Rev 59:335–345

    Article  Google Scholar 

Download references

Acknowledgments

I would like to thank to Prof. Kirsten Morris and Prof. Sergei Avdonin for the fruitful discussions and suggestions to finalize this paper.

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Correspondence to Ahmet Özkan Özer.

Appendix: Some results in number theory

Appendix: Some results in number theory

In this section, we briefly mention some fundamental results of Diophantine’s approximation. The theorem of Khintchine (Theorem 8) plays an important role to determine the Lebesgue measure of sets investigated in this paper.

Let \(f:\mathbb {N}\rightarrow \mathbb {R}^+\) be called an approximation function if

$$\begin{aligned} \mathop {\lim }\limits _{\tilde{q} \rightarrow \infty } f(\tilde{q})=0. \end{aligned}$$

A real number \(\zeta \) is \(f\)-approximable if \(\zeta \) satisfies

$$\begin{aligned} \left| ~\zeta -\frac{\tilde{p}}{\tilde{q}}~\right| <f(\tilde{q}) \end{aligned}$$
(63)

for infinitely many rational numbers \(\frac{\tilde{p}}{\tilde{q}}.\) Let \(P(f)\) be the set of all \(f\)-approximable numbers. We recall the following theorem to find the measure of sets of type \(P(f).\)

Theorem 8

(Khintchine’s theorem) [13, Page4] Let \(\mu \) be the Lebesgue measure. Then

$$\begin{aligned} \mu (P(f))=\left\{ \begin{array}{l@{\quad }l} 0, \quad &{} \mathrm{{if}} \quad \sum \limits _{\tilde{q}\in \mathbb {N}} {\tilde{q} f(\tilde{q})}<\infty , \\ \mathrm{{full}}, \quad &{} \mathrm{if} \quad \tilde{q} f(\tilde{q}) \quad \mathrm{{is\, nonincreasing\, and}} ~ \sum \limits _{\tilde{q}\in \mathbb {N}} {\tilde{q} f(\tilde{q})}=\infty . \end{array} \right. \end{aligned}$$
(64)

Dirichlet’s theorem [14] states that every irrational number can be approximated to the order 2. The following theorem from [35] is a special case of Dirichlet’s theorem:

Theorem 9

Let \(\zeta \in \mathbb {R}-\mathbb {Q}.\) Then there exists a constant \(C\ge 1,\) and increasing sequences of coprime odd integers \(\{\tilde{p}_j\},\{\tilde{q}_j\}\) satisfying the asymptotic relation

$$\begin{aligned} \left| ~\zeta - \frac{\tilde{p}_j}{\tilde{q}_j}~\right| \le \frac{C}{{\tilde{q}_j}^{2}},\quad j\rightarrow \infty . \end{aligned}$$
(65)

It obvious by Theorem 8 that the set \( \mathbb {R}-\mathbb {Q}\) is uncountable and it has a full Lebesgue measure.

Definition 5

A real number \(\zeta \) is a Liouville’s number if for every \(m\in \mathbb {N}\) there exists \(\frac{\tilde{p}_m}{\tilde{q}_m}\) with \(p_m, q_m \in \mathbb {Z}\) such that

$$\begin{aligned} \left| ~\zeta -\frac{\tilde{p}_m}{\tilde{q}_m}~\right| <\frac{1}{\tilde{q}_m^m}. \end{aligned}$$

It is proved that any Liouville’s number is transcendental. Theorem 8 implies that the set of Liouville’s numbers is of Lebesgue measure zero.

Definition 6

A real number \(\zeta \) is an algebraic number if it is a root of a polynomial equation

$$\begin{aligned} a_n x^n+ a_{n-1}x^{n-1}+ \cdots + a_1 x + a_0=0 \end{aligned}$$

with each \(a_i \in \mathbb {Z},\) and at least one of \(a_i\) is non-zero. A number which is not algebraic is called transcendental.

Now we give the following results of Diophantine’s approximations:

Theorem 10

There exists a set \(\tilde{\mathbb {Q}}\) such that if \(\zeta \in \mathbb {R}-\tilde{\mathbb {Q}},\) then for every \(\varepsilon >0\) there are infinitely many \(\frac{\tilde{p}}{\tilde{q}}\in \mathbb {Q}\) and a constant \(C_\zeta >0\) such that

$$\begin{aligned} \left| ~\zeta -\frac{\tilde{p}}{\tilde{q}}~\right| \ge \frac{C_\zeta }{\tilde{q}^{2+\varepsilon }}. \end{aligned}$$
(66)

Moroever, \(\mu (\tilde{\mathbb {Q}})=0.\)

Proof

We know that the irrational algebraic numbers belong to \(\tilde{\mathbb {Q}}\) by Roth’s theorem (Page 103, [14]). Therefore \(\tilde{\mathbb {Q}}\) is not empty. We proceed to the second part of the lemma. The first part of the theorem implies that if \(\zeta \in \tilde{\mathbb Q}\) then for all \(C_\zeta >0,\) the inequality \(\left| ~\zeta -\frac{\tilde{p}}{\tilde{q}}~\right| < \frac{C_\zeta }{\tilde{q}^{2+\varepsilon }}\) holds for some \(\frac{\tilde{p}}{\tilde{q}}\in \mathbb {Q}.\) Now define the set

$$\begin{aligned} \tilde{\mathbb Q}_{\varepsilon }=\left\{ \zeta \in \mathbb {R}~:~ \left| ~~\zeta -\frac{\tilde{p}}{\tilde{q}}~\right| < \frac{C_\zeta }{\tilde{q}^{2+\varepsilon }} ~ {\text {for infinitely many}} \frac{\tilde{p}}{\tilde{q}}\in \mathbb {Q} \right\} . \end{aligned}$$

By the notation of Theorem 8, choose \(f(\tilde{q})=\frac{C_\zeta }{\tilde{q}^{2+\varepsilon }}\) so that \(\tilde{q} f(\tilde{q})\) is nonincreasing and \(\sum \nolimits _{\tilde{q}\in \mathbb {N}}\frac{C_\zeta }{\tilde{q}^{1+\varepsilon }}<\infty .\) By Theorem 8, \(\mu (\tilde{\mathbb Q}_{\varepsilon })=0. \) Now we prove \(\tilde{\mathbb {Q}}\subset \tilde{\mathbb Q}_{\varepsilon }\) by contradiction. Assume that \(\zeta \notin \tilde{\mathbb Q}_{\varepsilon }\), i.e., there are finitely many rationals \(\left\{ \frac{p_i}{q_i}\right\} _{i=1,\ldots , N}\) such that

$$\begin{aligned} \left| ~\zeta -\frac{p_i}{q_i}~\right| < \frac{C_\zeta }{q_i^{2+\varepsilon }} ~~\mathrm{{for}}~~ i=1,\ldots , N, ~~\mathrm{{and}}~~\left| ~\zeta -\frac{\tilde{p}}{\tilde{q}}\right| \ge \frac{C_\zeta }{q^{2+\varepsilon }} ~~ \mathrm{{for}} ~~ \frac{\tilde{p}}{\tilde{q}}\notin \bigcup \limits _{i = 1}^N {\left\{ \frac{\tilde{p}_i}{\tilde{q}_i}\right\} }. \end{aligned}$$

The last inequality implies that \(\zeta \in \mathbb {R}-\mathbb {Q}.\) This implies that the set \(\mathbb {R}-\tilde{\mathbb {Q}}\) has a full Lebesgue measure. \(\square \)

Now define the set \(\tilde{\tilde{\mathbb {Q}}}\) by

$$\begin{aligned} \tilde{\tilde{\mathbb {Q}}}=\left\{ \zeta \in \mathbb {R}~:~ \exists C>0, ~~ \left| ~\zeta -\frac{\tilde{p}}{\tilde{q}}~\right| \ge \frac{C}{\tilde{q}^{2}} {\text { for infinitely many}} ~\frac{\tilde{p}}{\tilde{q}}\in \mathbb {Q} \right\} . \end{aligned}$$
(67)

If we consider numbers \(\zeta \in \mathbb {R}\) whose the partial quotients satisfy \(|a_k|<C(\zeta )\) for all \(k\in \mathbb {N}\) in its continued fraction expansion

$$\begin{aligned} \zeta =[a_0; a_1, a_2, \ldots ]=a_0+\frac{1}{a_1+\frac{1}{a_2+ \ddots }}, \end{aligned}$$

then \(\zeta \in \tilde{\tilde{\mathbb {Q}}}.\) By Liouville’s theorem (Page 128, [26]), \(\tilde{\tilde{\mathbb {Q}}}\) also contains all quadratic irrational numbers (the roots of an algebraic polynomial of degree \(2\)). Therefore the set is uncountable.

Lemma 6

The set \(\tilde{\tilde{\mathbb {Q}}}\) has a Lebesgue measure zero.

Proof

Define the set \(F_m\) by

$$\begin{aligned} F_m=\left\{ \zeta \in \mathbb {R}~:~ \left| ~\zeta -\frac{\tilde{p}}{\tilde{q}}~\right| < \frac{C}{m\tilde{q}^{2}} ~ {\text { for infinitely many}}~\frac{\tilde{p}}{\tilde{q}}\in \mathbb {Q} \right\} . \end{aligned}$$

Then \(F_m\) has a full Lebesgue measure by Theorem 8, i.e., \(f(\tilde{q})=\frac{C}{m\tilde{q}^2},\) and \(\sum \nolimits _{\tilde{q}\in \mathbb {N}} {\tilde{q} f(\tilde{q})}=\infty .\) Now consider the set \(\bigcap \nolimits _{m\in \mathbb {N}} F_m.\) This set is the countable intersection of sets \(F_m,\) and each \(F_m\) has full Lebesgue measure. Therefore \(\mu \left( \bigcap \nolimits _{m\in \mathbb {N}} F_m\right) \) has full Lebesgue measure. Since \(\tilde{\tilde{\mathbb {Q}}}=\mathbb {R}-\bigcap \nolimits _{m\in \mathbb {N}} F_m,\) then \(\mu (\tilde{\tilde{\mathbb {Q}}})=0\). \(\square \)

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Özer, A.Ö. Further stabilization and exact observability results for voltage-actuated piezoelectric beams with magnetic effects. Math. Control Signals Syst. 27, 219–244 (2015). https://doi.org/10.1007/s00498-015-0139-0

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