Control under constraints of reaction-diffusion equations · 2021. 2. 10. · Control under...

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Control under constraints of reaction-diffusion equations Domènec Ruiz-Balet Universidad Autónoma de Madrid, 28049 Madrid, Spain Fundación Deusto, University of Deusto, 48007 Bilbao, Basque Country, Spain. Erlangen, Janurary 21 st 2020

Transcript of Control under constraints of reaction-diffusion equations · 2021. 2. 10. · Control under...

Page 1: Control under constraints of reaction-diffusion equations · 2021. 2. 10. · Control under constraints of reaction-diffusion equations Domènec Ruiz-Balet Universidad Autónoma de

Control under constraints of reaction-diffusionequations

Domènec Ruiz-Balet

Universidad Autónoma de Madrid, 28049 Madrid, SpainFundación Deusto, University of Deusto, 48007 Bilbao, Basque

Country, Spain.Erlangen, Janurary 21st 2020

Page 2: Control under constraints of reaction-diffusion equations · 2021. 2. 10. · Control under constraints of reaction-diffusion equations Domènec Ruiz-Balet Universidad Autónoma de

IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Introduction

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

The models

Homogeneous bistable reaction-diffusion:ut −∆u = f (u) (x , t) ∈ Ω× (0,T )

u = a(x , t) (x , t) ∈ ∂Ω× (0,T )

0 ≤ u(x ,0) ≤ 1

Bistable reaction-diffusion with heterogeneous drift:ut −∆u +∇b(x)∇u = f (u) (x , t) ∈ Ω× (0,T )

u = a(x , t) (x , t) ∈ ∂Ω× (0,T )

0 ≤ u(x ,0) ≤ 1

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

0 1

0

The typical example is:

f (s) = s(1− s)(s − θ)

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Applications

Reaction-diffusion equations typically model the evolution ofquantities that are nonnegative or bounded by above and below,for example:

TemperatureConcentrations of chemicalsProportions

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Control problem

ut −∆u = f (u) (x , t) ∈ Ω× (0,T )

u = a(x , t) (x , t) ∈ ∂Ω× (0,T )

u(x ,0) = u0

(1)

Main GoalLet f be bistable, and consider 0 ≤ u0 ≤ 1 there exists a T > 0such that equation (1) is controllable towards the constantsteady states 0,θ and 1 in a way that the trajectory fulfills for all(x , t) ∈ Ω× [0,T ] that 0 ≤ u(x , t) ≤ 1?

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

Page 7: Control under constraints of reaction-diffusion equations · 2021. 2. 10. · Control under constraints of reaction-diffusion equations Domènec Ruiz-Balet Universidad Autónoma de

IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Negative result: Barriers

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Barriers

The comparison principle ensures that if a solution to theproblem

−∆v = f (v) x ∈ Ω

v = 0 x ∈ ∂Ω

1 > v > 0 x ∈ Ω

(2)

exists1 and our initial data u0 is above v then for anya ∈ L∞(Ω, [0,1]) the solution of the parabolic problem will stayabove v .

1P.L. Lions, On the existence of positive solutions of semilinear ellipticequations, SIAM Rev. 24 (1982), no. 4, 441–467

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

Page 9: Control under constraints of reaction-diffusion equations · 2021. 2. 10. · Control under constraints of reaction-diffusion equations Domènec Ruiz-Balet Universidad Autónoma de

IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Barriers

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Existence of barriers

After a space rescaling one can rewrite the elliptic equation

−vxx = L2f (v) x ∈ (0,1)

v(0) = v(1) = 01 > v > 0 x ∈ (0,1)

The associated functional is:

J : H10 ((0,1)) −→ R

J(v) =

∫ 1

0

12

v2x − L2F (v)dx

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

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Heterogeneous driftsReferences

Nonexistence of barriers

If λ is small, a barrier cannot exist:

λ1

∫ 1

0v2 ≤

∫ 1

0v2

x = λ

∫ 1

0vf (v) ≤ λ

∫ 1

0v2‖g‖∞

where f (v) = vg(v). Choose λ small enough so that:

λ1

∫ 1

0v2 > λ

∫ 1

0v2‖g‖∞

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

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Heterogeneous driftsReferences

Visual representation

J : Vh −→ R

J(v) =

∫ 1

0

12

v2x − λF (v)dx

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Nonexistence of barriers II

Nonexistence of barriers for reaching 1

Let F (1) ≥ 0, for any λ > 0 there exists a unique solution (v ≡ 1)to the problem:

−vxx = λf (v) x ∈ (0,1)

0 ≤ v ≤ 1 x ∈ (0,1)

v(0) = v(1) = 1(3)

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Visual representation

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Control towards θ

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

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Heterogeneous driftsReferences

Staircase method

TheoremLet v0 and v1 be pathconnected. If T is largeenough, ∃a ∈ L∞ suchthat the problem (1)with initial datum v0 andcontrol a admits uniquesolution verifyingv(T , ·) = v1 s.t. itstrajectory is admissible. b

b b b

b

b

γ(0)

γ(s1)γ(s2)

γ(s3)

γ(s4)

γ(1)

22D. Pighin and E. Zuazua, Controllability under positivity constraints of

semilinear heat equations, Math. Control Relat. Fields 8 (2018), 935.Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Continuous Path

S :=

v ∈ H1(0,L) such that v satisfies (4)

−uxx = f (u)

u(0) = a1, u(L) = a2

0 ≤ u ≤ 1(4)

The construction of the path involves to find a map

γ : [0,1]→ S

fulfillingγ(0) = 0γ(1) = θγ is continuous with respect to the L∞ topology.

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Phase portrait

Assume F (1) > 0. Observe that the one dimensional ellipticequation can be written as an ODE3

ddx

(uux

)=

(ux−f (u)

)

3C. Pouchol, E. Trélat, and E. Zuazua, Phase portrait control for 1dmonostable and bistable reaction–diffusion equations, Nonlinearity 32 (2019),no. 3, 884–909

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

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Heterogeneous driftsReferences

Invariant region

ddx

(uux

)=

(ux−f (u)

),

(u(0) = sθux (0) = 0

)

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Traveling waves

When F (1) = 0 the traveling waves are stationary and theyenclose an invariant region.

For F (1) > 0 they give a natural control towards thestationary solution 1.

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Multi-D

ut − µ∆u = f (u) (x , t) ∈ Ω× (0,T )

u = a(x , t) (x , t) ∈ ∂Ω× (0,T )

0 ≤ u(x ,0) ≤ 1(5)

Ω

BR

−urr − N−1

r ur = 1µ f (u) r ∈ (0,R)

u(0) = aur (0) = 0

44D. Ruiz-Balet and E. Zuazua, Control under constraints for

multi-dimensional reaction-diffusion monostable and bistable equations,Preprint (2019)

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

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Heterogeneous driftsReferences

ddr

(uur

)=

(ur−f (u)

)−(

0N−1

r ur

)E(u,ur ) =

12

u2r + F (u)

ddr

E = −N − 1r

u2r < 0

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

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Heterogeneous driftsReferences

Theorem (Theorem 1.2 in (4))

Let f be bistable. Let Ω ⊂ RN be a C2-regular domain ofmeasure 1. If F (1) > 0, ∃T ∈ (0,+∞], and ∃A ⊂ L∞(Ω; [0,1])s.t. the solution of the system (5) can be controlled by means ofa function a ∈ L∞(∂Ω× [0,T ], [0,1])

in infinite time to w ≡ 0:for any initial data u0 iff µ > µ∗(Ω, f ),for any µ > 0 if u0 ∈ A,

in finite time to w ≡ θ:for any initial data u0 iff µ > µ∗(Ω, f ),for any µ > 0 if u0 ∈ A,

in infinite time to w ≡ 1 for any admissible initial data u0 andfor any µ > 0.

Furthermore µ∗(Ω, f ) > 0.Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Heterogeneous drifts

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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Heterogeneous driftsReferences

The model

Consider a distribution of population N > 0. Consider that thepopulation is divided between two traits. We model the evolutionof the proportion of one trait by5:

ut −∆u − ∇N(x)N(x) ∇u = f (u) (x , t) ∈ Ω× (0,T )

u = a(x , t) (x , t) ∈ ∂Ω× (0,T )

0 ≤ u(x ,0) ≤ 1

we will also use the notation ∇b(x) = ∇N(x)N(x)

5I. Mazari, D. Ruiz-Balet, and E. Zuazua, Constrained control of bistablereaction-diffusion equations: Gene- flow and spatially heterogeneous models,Preprint (2019)

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

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Heterogeneous driftsReferences

Two examples

For N(x) = e−x2σ , ut − uxx + 2x

σ ux = f (u)

For N(x) = ex2σ , ut − uxx − 2x

σ ux = f (u)

-10 -5 0 5 10-0.5

0

0.5

1

-5 0 5-0.5

0

0.5

1

1.5

2

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

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Firsts Barriers

Nontrivial solutions with 0 boundary also exist:

-6 -4 -2 0 2 4 6

x

0

1u

Non trivial solution

Figure: ∇b(x) = 2 xσ .

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

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Heterogeneous driftsReferences

Differential inequality

When can we ensure controllability?The multi-dimensional case shows us that the important factis to have a conservative or dissivative ODE dynamics.If we set a radial drift that makes the ODE dynamicsdissipative, would be enough to guarantee the constructionof the path.Theorem 3 in (5) ensures the existence of a continuous pathwhenever the drift is radial and fulfills:

N ′(r) ≥ −N − 12r

N(r) (6)

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

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Heterogeneous driftsReferences

Upper barriers

QuestionWhat happens if the differential inequality (6) is not satisfied?

Take N(x) = e−x2σ . We observed that an upper barrier can exist

(Theorem 4 in (5)). −uxx + 2 x

σux = f (u)

u(−L) = u(L) = 1(7)

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

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Heterogeneous driftsReferences

Shooting method

This steady state cannot correspond to a global energeticminima hence a shooting method is employed.

0 1

u

-1

-0.8

-0.6

-0.4

-0.2

0

0.2

0.4

0.6

0.8

1

ux

Trajectory for a=0.10

-8 -6 -4 -2 0 2 4 6 8

x

0

1

u

Non trivial solution

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

Emergence of a barrier

In the following numerical simulation one can observe how theparabolic trajectory finds the barrier found before.

-5 0 5

space

0

1

stat

e

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

Page 33: Control under constraints of reaction-diffusion equations · 2021. 2. 10. · Control under constraints of reaction-diffusion equations Domènec Ruiz-Balet Universidad Autónoma de

IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

References

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

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IntroductionNegative result: Barriers

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Heterogeneous driftsReferences

1 P.L. Lions, On the existence of positive solutions ofsemilinear elliptic equations, SIAM Rev. 24 (1982), no. 4,441–467

2 D. Pighin and E. Zuazua, Controllability under positivityconstraints of semilinear heat equations, Math. ControlRelat. Fields 8 (2018), 935.

3 C. Pouchol, E. Trélat, and E. Zuazua, Phase portrait controlfor 1d monostable and bistable reaction–diffusion equations,Nonlinearity 32 (2019), no. 3, 884–909

4 D. Ruiz-Balet and E. Zuazua, Control under constraints formulti-dimensional reaction-diffusion monostable andbistable equations, Preprint (2019)

5 I. Mazari, D. Ruiz-Balet, and E. Zuazua, Constrained controlof bistable reaction-diffusion equations: Gene- flow andspatially heterogeneous models, Preprint (2019)

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations

Page 35: Control under constraints of reaction-diffusion equations · 2021. 2. 10. · Control under constraints of reaction-diffusion equations Domènec Ruiz-Balet Universidad Autónoma de

IntroductionNegative result: Barriers

Control towards θ

Heterogeneous driftsReferences

THANK YOU FOR YOUR ATTENTION!

This project has received funding from the European ResearchCouncil (ERC) under the European Union’s Horizon 2020 re-search and innovation program (grant agreement No 694126-DYCON).

Domènec Ruiz-Balet Control under constraints of reaction-diffusion equations