Tutorial on Control and State Constrained Optimal Control Problems

Size: px
Start display at page:

Download "Tutorial on Control and State Constrained Optimal Control Problems"

Transcription

1 Tutorial on Control and State Constrained Optimal Control Problems To cite this version:. blems. SADCO Summer School Optimal Control, Sep 211, London, United Kingdom. <inria > HAL Id: inria Submitted on 6 Oct 211 HAL is a multi-disciplinary open access archive for the deposit and dissemination of scientific research documents, whether they are published or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

2 Tutorial on Control and State Constrained Optimal Control Problems Part 2 : Mixed Control-State Constraints University of Münster, Germany Institute of Computational and Applied Mathematics SADCO Summer School Imperial College London, September 5, 211

3 Outline 1 Optimal Control Problems with Control and State Constraints 2 Numrical Method: Discretize and Optimize 3 Theory of Optimal Control Problems with Mixed Control-State Constraints 4 Example: Rayleigh Problem with Different Constraints and Objectives 5 Example: Optimal Exploitation of Renewable Resources

4 Optimal Control Problem state x(t) R n, control u(t) R m. Dynamics and Boundary Conditions ẋ(t) = f (t, x(t),u(t)), a.e. t [,t f ], x(t) = x, ψ(x(t f )) = (ψ : R n R r ). Control and State Constraints c(x(t),u(t)), t t f, ( c : R n R m R k ) s(x(t)), t t f, ( s : R n R l ) Minimize tf J(u, x) = g(x(t f )) + f (t,x(t),u(t))dt

5 Discretization For simplicity consider a MAYER type problem with cost functional J(u, x) = g(x(t f )). This can achieved by considering the additional state variable x with ẋ = f (x,u), x () =. Then we have x (t f ) = tf f (t,x(t), u(t)). Choose an integer N N, a stepsize h and grid points t i : h = t f /N, t i : = ih, (i =,1,...,N). Approximation of control and state at grid points: u(t i ) u i R m, x(t i ) x i R n (i =,...,N)

6 Large-scale NLP using EULER s method Minimize J(u,x) = g(x N ) subject to x i+1 = x i + h f (t i,x i,u i ), i =,..,N 1, x = x, ψ(x N ) =, c(x i,u i ), i =,..,N, s(x i ), i =,..,N, Optimization variable for full discretization: z := (u,x 1,u 1,x 2,...,u N 1,x N,u N ) R N(m+n)+m

7 NLP Solvers AMPL : Programming language (Fourer, Gay, Kernighan) IPOPT : Interior point method (Andreas Wächter) LOQO : Interior point method (Vanderbei et al.) Other NLP solvers embedded in AMPL : cf. NEOS server NUDOCCCS : optimal control package (Christof Büskens) WORHP : SQP solver (Christof Büskens, Matthias Gerdts) Special feature: solvers provide LAGRANGE-multipliers as approximations of the adjoint variables.

8 Optimal Control Problem with Control-State Constraints State x(t) R n, Control u(t) R m. All functions are assumed to be suffciently smooth Dynamics and Boundary Conditions ẋ(t) = f (x(t),u(t)), a.e. t [,t f ], x() = x R n, ψ(x(t f )) = R k, ( = ϕ(x(), x(t f )) mixed boundary conditions ) Mixed Control-State Constraints α c(x(t),u(t)) β, t [, t f ], c : R n R m R Control bounds α u(t) β are included by c(x, u) = u. Minimize tf J(u,x) = g(x(t f )) + f (x(t),u) dt

9 Hamiltonian Hamiltonian H(x, λ, u) = λ f (x, u) + λ f (x, u) Augmented Hamiltonian λ R n (row vector) H(x, λ,µ, u) = H(x, λ, u) + µ c(x, u) = λ f (x, u) + λ f (x, u) + µ c(x, u), µ R. Let (u, x) L ([, T], R m ) W 1, ([, T], R n ) be a locally optimal pair of functions. Regularity assumption c u (x(t), u(t)) t J a J a := { t [, t f ] c(x(t), u(t)) = α or = β }

10 Minimum Principle of Pontryagin et al. and Hestenes Let (u, x) L ([, t f ], R m ) W 1, ([, t f ], R n ) be a locally optimal pair of functions that satisfies the regularity assumption. Then there exist an adjoint (costate) function λ W 1, ([, t f ], R n ) and a scalar λ, a multiplier function µ L ([, t f ], R), and a multiplier ρ R r associated to the boundary condition ψ(x(t f )) = that satisfy the following conditions for a.a. t [, t f ], where the argument (t) denotes evaluation along the trajectory (x(t), u(t), λ(t)) :

11 Minimum Principle of Pontraygin et al. and Hestenes (i) Adjoint ODE and transversality condition: λ(t) = H x (t) = (λ f + λ f ) x (t) µ(t) c x (t), λ(t f ) = (λ g + ρψ) x (x(t f )), (iia) Minimum Condition for Hamiltonian: H(x(t), λ(t),u(t)) = min { H(x(t), λ(t),u) α c(x(t),u) β } (iib) Local Minimum Condition for Augmented Hamiltonian: = H u (t) = (λ f + λ f ) u (t) + µ(t) c u (t) (iii) Sign of multiplier µ and complementarity condition: µ(t), if c(x(t),u(t)) = α ; µ(t), if c(x(t), u(t)) = β, µ(t) =, if α < c(x(t),u(t)) < β.

12 Evaluation of the Minimum Principle: boundary arc Boundary arc: Let [t 1,t 2 ], t 1 < t 2 < t f, be an interval with c(x(t), u(t)) = α or c(x(t), u(t)) = β t 1 t t 2. For simplicity assume a scalar control, i.e., m = 1. Due to the regularity condition c u (x(t),u(t)) there exists a smooth function u b (x) satisfying c(x,u b (x)) α ( β) x in a neighborhood of the trajectory. The control u b (x) is called the boundary control and yields the optimal control by the relation u(t) = u b (x(t)). It follows from the local minimum condition = H u = H u + µc u that the multiplier µ is given by µ = µ(x, λ) = H u (x, λ,u b (x))/c u (x,u b (x)).

13 Case I : Regular Hamiltonian, u is continuous CASE I : Consider optimal control problems which satisfy the Assumption: The Hamiltonian H(x, λ,u) is regular, i.e., it admits a unique minimum u. The strict Legendre condition holds: H uu (t) > t [,t f ]. (a) Then there exists a free control u = u free (x, λ) satisfying H u (x, λ,u free (x, λ)). (b) The optimal control u(t) is continuous in [,t f ]. Claim (b) follows from the continuity and regularity of H. The continuity of the control implies junctions conditions at junction points t k (k = 1, 2) with the boundary: u free (x(t k ), λ(t k )) = u b (x(t k )), µ(t k ) = (k = 1,2).

14 Rayleigh Problem with Quadratic Control The Rayleigh problem is a variant of the van der Pol Oszillator, where x 1 denotes the electric current. Control problem for the Rayleigh Equation Minimize J(x, u) = subject to t f (u 2 + x 2 1 ) dt (t f = 4.5) ẋ 1 = x 2, x 1 () = 5, ẋ 2 = x 1 + x 2 (1.4.14x 2 2 ) + 4u, x 2() = 5. Three types of constraints: Case (a) : no control constraints. Case (b) : control constraint 1 u(t) 1. Case (c) : mixed control-state constraint α u(t) + x 1 (t)/6, α = 1, 2

15 Case I (a) : Rayleigh problem, no constraint Normal Hamiltonian: H(x, λ,u) = u 2 + x λ 1 x 2 + λ 2 ( x 1 + x 2 (1.4.14x 2 2) + 4u) Adjoint Equations: λ 1 = H x1 = 2x 1 + λ 2 λ 1 (t f ) =, λ 2 = H x2 = λ 1 λ 2 (1.4.42x 2 2 ) λ 2(t f ) =, Minimum condition: = H u = 2u + 4λ 2 u = u free (x, λ) = 2λ 2. Shooting method for solving the boundary value problem for (x, λ): Determine unknown shooting vector s = λ() R 2 that satisfies the terminal condition λ(t f ) = : use Newton s method

16 Case I : Rayleigh problem without constraints x 1, x 2 state variables x 1, x (x 1,x 2 ) phaseportrait (x 1,x 2 ) u optimal control u lambda 1, lambda 2 adjoint variables lambda 1, lambda Note: Hamiltionian is regular, control u(t) is continuous (analytic).

17 Case I (b) : Rayleigh problem, constraint 1 u(t) 1 Hamiltonian H and adjoint equations are as in Case (a). The free control is given by u free (x, λ) = 2λ 2. Structure of optimal control: u(t) = 1 for t t 1 2λ 2 (t) for t 1 t t 2 1 for t 2 t t 3 2λ 2 (t) for t 3 t t f Junction conditions: Continuity of the control implies u(t k ) = 2λ 2 (t k ) = 1 1 1, k = 1,2,3. Shooting method for solving the boundary value problem for (x, λ): Determine shooting vector s = (λ(),t 1,t 2,t 3 ) R 2+3 that satisfies 2 terminal conditions λ(t f ) = and 3 junction conditions.

18 Rayleigh problem with control constraint u(t) 1 x 1, x state variables x 1, x (x 1,x 2 ) phaseportrait (x 1,x 2 ) u optimal control u lambda 1, lambda adjoint variables lambda 1, lambda Note: Hamiltonian is regular, control u(t) is continuous. Junction conditions: 2λ 2 (t k ) = 1 1 1, k = 1,2,3

19 Case I (c) : Rayleigh problem, 1 u + x 1 /6 Augmented (normal) Hamiltonian: H(x, λ,µ,u) = u 2 + x λ 1 x 2 +λ 2 ( x 1 + x 2 (1.4.14x 2 2 ) + 4u) + µ(u + x 1/6) Adjoint Equations: λ 1 = H x1 = 2x 1 + λ 2 µ/6, λ 1 (t f ) =, λ 2 = H x2 = λ 1 λ 2 (1.4.42x 2 2 ) λ 2(t f ) =, Free control : u free (x, λ) = 2λ 2. Boundary control : u b (x) = α x 1 /6 for α { 1,}. Multiplier : µ = µ(x, λ) = H u (x, λ,u b (x))/c u (x,u b (x)) = 2u b (x) + 4λ 2.

20 Case I (c) : Rayleigh problem, 1 u + x 1 /6 u optimal control u C(x,u) = u + x 1 /6 mixed constraint -1 <= u + x 1 /6 <= x 1, x state variables x 1, x mu multiplier for constraint -1 <= u + x 1 /6 <= Hamiltonian is regular, control u(t) is continuous. Junction conditions: 2λ(t k ) = α x 1 (t k )/6, α {, 1}.

21 Case I (c) : Rayleigh problem, structure of optimal control for mixed constraint 1 u + x 1 /6 mixed constraint -1 <= u + x 1 /6 <= C(x,u) = u + x 1 / u(t) = x 1 /6 for t t 1 2λ 2 (t) for t 1 t t 2 1 x 1 /6 for t 2 t t 3 2λ 2 (t) for t 3 t t 4 x 1 /6 for t 4 t t 5 2λ 2 (t) for t 5 t t f

22 Case II : control u appears linearly CASE II : Control appears linearly in the cost functional, dynamics and mixed control-state constraint. Let u be scalar. Dynamics and Boundary Conditions ẋ(t) = f 1 (x(t)) + f 2 (x(t)) u(t), a.e. t [,t f ], x() = x R n, ψ(x(t f )) = R k, Mixed Control-State Constraints α c 1 (x(t)) + c 2 (x(t)) u(t) β t [,t f ]. c 1, c 2 : R n R Minimize J(u, x) = g(x(t f )) + tf ( f 1 (x(t)) + f 2 (x(t) ) u(t)dt

23 Case II : Hamiltonian and switching function Normal Hamiltonian H(x, λ,u) = f 1 (x) + λf 1 (x) + [ f 2 (x) + λf 2 (x) ] u. Augmented Hamiltonian H(x, λ,µ,u) = H(x, λ,u) + µ(c 1 (x) + c 2 (x) u) The optimal control u(t) solves the minimization problem min { H(x(t), λ(t),u) α c 1 (x(t)) + c 2 (x(t)) u β } Define the switching function σ(x, λ) = H u (x, λ,u) = f 2 (x) + λf 2 (x), σ(t) = σ(x(t), λ(t)).

24 Case II : Hamiltonian The minimum condition is equivalent to the minimization problem min { σ(t) u) α c 1 (x(t)) + c 2 (x(t)) u β } We deduce the control law c 1 (x(t))+c 2 (x(t)) u(t) = α, if σ(t) c 2 (x(t)) > β, if σ(t) c 2 (x(t)) < undetermined if σ(t) The control u is called bang-bang in an interval I [, t f ], if σ(t) c 2 (x(t)) for all t I. The control u is called singular in an interval I sing [, t f ], if σ(t) c 2 (x(t)) for all t I sing. For the control constraint α u(t) β with c 1 (x) =, c 2 (x) = 1 we get the classical control law α, if σ(t) > u(t) = β, if σ(t) < undetermined, if σ(t)

25 Bang-Bang and Singular Controls

26 Case II : Rayleigh problem with 1 u(t) 1 Rayleigh problem with control appearing linearly Minimize J(x, u) = subject to t f (x x2 2 )dt (t f = 4.5) ẋ 1 = x 2, x 1 () = 5, ẋ 2 = x 1 + x 2 (1.4.14x 2 2 ) + 4u, x 2() = 5, 1 u(t) 1. Adjoint Equations: λ 1 = H x1 = 2x 1 + λ 2, λ 1 (t f ) =, λ 2 = H x2 = 2x 2 λ 1 λ 2 (1.4.42x 2 2 ), λ 2(t f ) =, The switching function σ(t) = H u (t) = 4λ 2 (t) gives the control law u(t) = sign (λ 2 (t)).

27 Case II : Rayleigh problem, 1 u(t) 1 u optimal control u x 1, x 2 state variables x 1, x u, lambda 2 / control u and (scaled) switching function lambda 1, lambda 2 adjoint variables lambda 1, lambda Control u(t) is bang-bang-singular. Switching conditions: λ(t 1 ) =, λ 2 (t) t [t 2,t f ].

28 Case II : Rayleigh problem, α u + x 1 /6 Minimize J(x, u) = subject to t f (x x2 2 )dt (t f = 4.5) ẋ 1 = x 2, x 1 () = 5, ẋ 2 = x 1 + x 2 (1.4.14x 2 2 ) + 4u, x 2() = 5, and the mixed control-state constraint Adjoint Equations: α u(t) + x 1 (t)/6 t t f. λ 1 = H x1 = 2x 1 + λ 2 µ/6, λ 1 (t f ) =, λ 2 = H x2 = 2x 2 λ 1 λ 2 (1.4.42x 2 2 ), λ 2(t f ) =,

29 Control law for α u + x 1 /6 The switching function is σ(t) = H u (t) = 4λ 2 (t). In view of c 2 (x) 1 we have the control law α <, if λ 2 (t) > u + x 1 /6 =, if λ 2 (t) < undetermined, if λ 2 (t)

30 Case II : Rayleigh problem, 1 u + x 1 /6 u optimal control u x 1, x 2 state variables x 1, x C(x,u) and (scaled) switching function 2 multiplier for constraint -1 <= u + x 1 /6 <=.5 1 u, lambda 2 / mu Note: constraint u(t) + x 1 (t)/6 is bang-bang.

31 Case II : Rayleigh problem, 2 u + x 1 /6 u optimal control u x 1, x 2 state variables x 1, x c(x,u), lambda 2 /1 c(x,u) and (scaled) switching function mu multiplier for constraint -1 <= u + x 1 /6 <= Note: constraint u(t) + x 1 (t)/6 is bang-singular-bang-singular.

32 Optimal Fishing, Clark, Clarke, Munro Colin W. Clark, Frank H. Clarke, Gordon R. Munro: The optimal exploutation of renewable resource stock: problem of irreversible investment, Econometric 47, pp (1979). State variables and control variables: x(t) : population biomass at time t [,t f ], renewable resource, e.g., fish, K(t) : amount of capital invested in the fishery, e.g., number of standardized fishing vessels available, E(t) : fishing effort (control), h(t) = E(t)x(t) is harvest rate, I(t) : investment rate (control),

33 Optimal Fishing: optimal control model Dynamics in [,t f ] ( here: a = 1, b = 5, γ = ) ẋ(t) = a x(t) (1 x(t)/b) E(t) x(t), x() = x, K(t) = I(t) γ K(t), K() = K. Mixed Control-State Constraint and Control Constraint E(t) K(t), I(t) I max, t [,t f ], Maximize benefit (parameters: r =.5, c E = 2, c I = 1.1 ) J(u,x) = tf exp( r t)(p E(t) x(t) c E E(t) c I I(t) )dt

34 Optimal Fishing: x =.5, K =.2, I max =.5 controls E, I and state variables.5*x, K 2 "E.dat" "I.dat" "K.dat" "x-scal.dat"

35 Optimal Fishing: x =.5, K =.6, I max =.5 controls E, I and state variables.5*x, K 2 "E.dat" "I.dat" "K.dat" "x-scal.dat" Fishing rate : E(t) =, E(t) = singular, E(t) = K(t). Investment rate : I(t) =, I(t) = I max, I(t) =.

36 Optimal Fishing: x =.2, K =.1, I max =.1 controls E, I and state variables.5*x, K 2 "E.dat" "I.dat" "K.dat" "x-scal.dat" Fishing rate : E(t) =, E(t) = K(t), E(t) singular, E(t) = K(t). Investment rate : 2 arcs with I(t) = I max.

37 Optimal Fishing: x = 1., K =.5, I max = controls E, I and state variables.5*x, K "E.dat" "I.dat" "K.dat" "x-scal.dat" Fishing rate : E(t) =, E(t) singular E(t) = K(t), Investment rate : 1 impulse with I(t) = I max.

Theory and Applications of Constrained Optimal Control Proble

Theory and Applications of Constrained Optimal Control Proble Theory and Applications of Constrained Optimal Control Problems with Delays PART 1 : Mixed Control State Constraints Helmut Maurer 1, Laurenz Göllmann 2 1 Institut für Numerische und Angewandte Mathematik,

More information

Tutorial on Control and State Constrained Optimal Control Pro. Control Problems and Applications Part 3 : Pure State Constraints

Tutorial on Control and State Constrained Optimal Control Pro. Control Problems and Applications Part 3 : Pure State Constraints Tutorial on Control and State Constrained Optimal Control Problems and Applications Part 3 : Pure State Constraints University of Münster Institute of Computational and Applied Mathematics SADCO Summer

More information

Methylation-associated PHOX2B gene silencing is a rare event in human neuroblastoma.

Methylation-associated PHOX2B gene silencing is a rare event in human neuroblastoma. Methylation-associated PHOX2B gene silencing is a rare event in human neuroblastoma. Loïc De Pontual, Delphine Trochet, Franck Bourdeaut, Sophie Thomas, Heather Etchevers, Agnes Chompret, Véronique Minard,

More information

Theory and Applications of Optimal Control Problems with Tim

Theory and Applications of Optimal Control Problems with Tim Theory and Applications of Optimal Control Problems with Time Delays University of Münster Applied Mathematics: Institute of Analysis and Numerics Université Pierre et Marie Curie, Paris, March 1, 217

More information

Linear Quadratic Zero-Sum Two-Person Differential Games

Linear Quadratic Zero-Sum Two-Person Differential Games Linear Quadratic Zero-Sum Two-Person Differential Games Pierre Bernhard To cite this version: Pierre Bernhard. Linear Quadratic Zero-Sum Two-Person Differential Games. Encyclopaedia of Systems and Control,

More information

Finite Volume for Fusion Simulations

Finite Volume for Fusion Simulations Finite Volume for Fusion Simulations Elise Estibals, Hervé Guillard, Afeintou Sangam To cite this version: Elise Estibals, Hervé Guillard, Afeintou Sangam. Finite Volume for Fusion Simulations. Jorek Meeting

More information

Thomas Lugand. To cite this version: HAL Id: tel

Thomas Lugand. To cite this version: HAL Id: tel Contribution à la Modélisation et à l Optimisation de la Machine Asynchrone Double Alimentation pour des Applications Hydrauliques de Pompage Turbinage Thomas Lugand To cite this version: Thomas Lugand.

More information

A new simple recursive algorithm for finding prime numbers using Rosser s theorem

A new simple recursive algorithm for finding prime numbers using Rosser s theorem A new simple recursive algorithm for finding prime numbers using Rosser s theorem Rédoane Daoudi To cite this version: Rédoane Daoudi. A new simple recursive algorithm for finding prime numbers using Rosser

More information

Easter bracelets for years

Easter bracelets for years Easter bracelets for 5700000 years Denis Roegel To cite this version: Denis Roegel. Easter bracelets for 5700000 years. [Research Report] 2014. HAL Id: hal-01009457 https://hal.inria.fr/hal-01009457

More information

Minimum-fuel trajectories for a hypersonic passenger aircraft under a temperature restriction for the thermal protection system

Minimum-fuel trajectories for a hypersonic passenger aircraft under a temperature restriction for the thermal protection system Minimum-fuel trajectories for a hypersonic passenger aircraft under a temperature restriction for the thermal protection system Hans-Josef Pesch To cite this version: Hans-Josef Pesch. Minimum-fuel trajectories

More information

L institution sportive : rêve et illusion

L institution sportive : rêve et illusion L institution sportive : rêve et illusion Hafsi Bedhioufi, Sida Ayachi, Imen Ben Amar To cite this version: Hafsi Bedhioufi, Sida Ayachi, Imen Ben Amar. L institution sportive : rêve et illusion. Revue

More information

Smart Bolometer: Toward Monolithic Bolometer with Smart Functions

Smart Bolometer: Toward Monolithic Bolometer with Smart Functions Smart Bolometer: Toward Monolithic Bolometer with Smart Functions Matthieu Denoual, Gilles Allègre, Patrick Attia, Olivier De Sagazan To cite this version: Matthieu Denoual, Gilles Allègre, Patrick Attia,

More information

Solution to Sylvester equation associated to linear descriptor systems

Solution to Sylvester equation associated to linear descriptor systems Solution to Sylvester equation associated to linear descriptor systems Mohamed Darouach To cite this version: Mohamed Darouach. Solution to Sylvester equation associated to linear descriptor systems. Systems

More information

Passerelle entre les arts : la sculpture sonore

Passerelle entre les arts : la sculpture sonore Passerelle entre les arts : la sculpture sonore Anaïs Rolez To cite this version: Anaïs Rolez. Passerelle entre les arts : la sculpture sonore. Article destiné à l origine à la Revue de l Institut National

More information

Case report on the article Water nanoelectrolysis: A simple model, Journal of Applied Physics (2017) 122,

Case report on the article Water nanoelectrolysis: A simple model, Journal of Applied Physics (2017) 122, Case report on the article Water nanoelectrolysis: A simple model, Journal of Applied Physics (2017) 122, 244902 Juan Olives, Zoubida Hammadi, Roger Morin, Laurent Lapena To cite this version: Juan Olives,

More information

Evolution of the cooperation and consequences of a decrease in plant diversity on the root symbiont diversity

Evolution of the cooperation and consequences of a decrease in plant diversity on the root symbiont diversity Evolution of the cooperation and consequences of a decrease in plant diversity on the root symbiont diversity Marie Duhamel To cite this version: Marie Duhamel. Evolution of the cooperation and consequences

More information

On size, radius and minimum degree

On size, radius and minimum degree On size, radius and minimum degree Simon Mukwembi To cite this version: Simon Mukwembi. On size, radius and minimum degree. Discrete Mathematics and Theoretical Computer Science, DMTCS, 2014, Vol. 16 no.

More information

Dispersion relation results for VCS at JLab

Dispersion relation results for VCS at JLab Dispersion relation results for VCS at JLab G. Laveissiere To cite this version: G. Laveissiere. Dispersion relation results for VCS at JLab. Compton Scattering from Low to High Momentum Transfer, Mar

More information

Can we reduce health inequalities? An analysis of the English strategy ( )

Can we reduce health inequalities? An analysis of the English strategy ( ) Can we reduce health inequalities? An analysis of the English strategy (1997-2010) Johan P Mackenbach To cite this version: Johan P Mackenbach. Can we reduce health inequalities? An analysis of the English

More information

Trajectory Optimization for Differential Flat Systems

Trajectory Optimization for Differential Flat Systems Trajectory Optimization for Differential Flat Systems Kahina Louadj, Benjamas Panomruttanarug, Alexre Carlos Brao-Ramos, Felix Antonio Claudio Mora-Camino To cite this version: Kahina Louadj, Benjamas

More information

The FLRW cosmological model revisited: relation of the local time with th e local curvature and consequences on the Heisenberg uncertainty principle

The FLRW cosmological model revisited: relation of the local time with th e local curvature and consequences on the Heisenberg uncertainty principle The FLRW cosmological model revisited: relation of the local time with th e local curvature and consequences on the Heisenberg uncertainty principle Nathalie Olivi-Tran, Paul M Gauthier To cite this version:

More information

From Unstructured 3D Point Clouds to Structured Knowledge - A Semantics Approach

From Unstructured 3D Point Clouds to Structured Knowledge - A Semantics Approach From Unstructured 3D Point Clouds to Structured Knowledge - A Semantics Approach Christophe Cruz, Helmi Ben Hmida, Frank Boochs, Christophe Nicolle To cite this version: Christophe Cruz, Helmi Ben Hmida,

More information

Completeness of the Tree System for Propositional Classical Logic

Completeness of the Tree System for Propositional Classical Logic Completeness of the Tree System for Propositional Classical Logic Shahid Rahman To cite this version: Shahid Rahman. Completeness of the Tree System for Propositional Classical Logic. Licence. France.

More information

Full-order observers for linear systems with unknown inputs

Full-order observers for linear systems with unknown inputs Full-order observers for linear systems with unknown inputs Mohamed Darouach, Michel Zasadzinski, Shi Jie Xu To cite this version: Mohamed Darouach, Michel Zasadzinski, Shi Jie Xu. Full-order observers

More information

Reduced Models (and control) of in-situ decontamination of large water resources

Reduced Models (and control) of in-situ decontamination of large water resources Reduced Models (and control) of in-situ decontamination of large water resources Antoine Rousseau, Alain Rapaport To cite this version: Antoine Rousseau, Alain Rapaport. Reduced Models (and control) of

More information

Exact Comparison of Quadratic Irrationals

Exact Comparison of Quadratic Irrationals Exact Comparison of Quadratic Irrationals Phuc Ngo To cite this version: Phuc Ngo. Exact Comparison of Quadratic Irrationals. [Research Report] LIGM. 20. HAL Id: hal-0069762 https://hal.archives-ouvertes.fr/hal-0069762

More information

A non-linear simulator written in C for orbital spacecraft rendezvous applications.

A non-linear simulator written in C for orbital spacecraft rendezvous applications. A non-linear simulator written in C for orbital spacecraft rendezvous applications. Paulo Ricardo Arantes Gilz To cite this version: Paulo Ricardo Arantes Gilz. A non-linear simulator written in C for

More information

A Simple Model for Cavitation with Non-condensable Gases

A Simple Model for Cavitation with Non-condensable Gases A Simple Model for Cavitation with Non-condensable Gases Mathieu Bachmann, Siegfried Müller, Philippe Helluy, Hélène Mathis To cite this version: Mathieu Bachmann, Siegfried Müller, Philippe Helluy, Hélène

More information

FORMAL TREATMENT OF RADIATION FIELD FLUCTUATIONS IN VACUUM

FORMAL TREATMENT OF RADIATION FIELD FLUCTUATIONS IN VACUUM FORMAL TREATMENT OF RADIATION FIELD FLUCTUATIONS IN VACUUM Frederic Schuller, Renaud Savalle, Michael Neumann-Spallart To cite this version: Frederic Schuller, Renaud Savalle, Michael Neumann-Spallart.

More information

Analysis of Boyer and Moore s MJRTY algorithm

Analysis of Boyer and Moore s MJRTY algorithm Analysis of Boyer and Moore s MJRTY algorithm Laurent Alonso, Edward M. Reingold To cite this version: Laurent Alonso, Edward M. Reingold. Analysis of Boyer and Moore s MJRTY algorithm. Information Processing

More information

On Newton-Raphson iteration for multiplicative inverses modulo prime powers

On Newton-Raphson iteration for multiplicative inverses modulo prime powers On Newton-Raphson iteration for multiplicative inverses modulo prime powers Jean-Guillaume Dumas To cite this version: Jean-Guillaume Dumas. On Newton-Raphson iteration for multiplicative inverses modulo

More information

Entropies and fractal dimensions

Entropies and fractal dimensions Entropies and fractal dimensions Amelia Carolina Sparavigna To cite this version: Amelia Carolina Sparavigna. Entropies and fractal dimensions. Philica, Philica, 2016. HAL Id: hal-01377975

More information

Norm Inequalities of Positive Semi-Definite Matrices

Norm Inequalities of Positive Semi-Definite Matrices Norm Inequalities of Positive Semi-Definite Matrices Antoine Mhanna To cite this version: Antoine Mhanna Norm Inequalities of Positive Semi-Definite Matrices 15 HAL Id: hal-11844 https://halinriafr/hal-11844v1

More information

On Symmetric Norm Inequalities And Hermitian Block-Matrices

On Symmetric Norm Inequalities And Hermitian Block-Matrices On Symmetric Norm Inequalities And Hermitian lock-matrices Antoine Mhanna To cite this version: Antoine Mhanna On Symmetric Norm Inequalities And Hermitian lock-matrices 015 HAL Id: hal-0131860

More information

Soundness of the System of Semantic Trees for Classical Logic based on Fitting and Smullyan

Soundness of the System of Semantic Trees for Classical Logic based on Fitting and Smullyan Soundness of the System of Semantic Trees for Classical Logic based on Fitting and Smullyan Shahid Rahman To cite this version: Shahid Rahman. Soundness of the System of Semantic Trees for Classical Logic

More information

A Simple Proof of P versus NP

A Simple Proof of P versus NP A Simple Proof of P versus NP Frank Vega To cite this version: Frank Vega. A Simple Proof of P versus NP. 2016. HAL Id: hal-01281254 https://hal.archives-ouvertes.fr/hal-01281254 Submitted

More information

b-chromatic number of cacti

b-chromatic number of cacti b-chromatic number of cacti Victor Campos, Claudia Linhares Sales, Frédéric Maffray, Ana Silva To cite this version: Victor Campos, Claudia Linhares Sales, Frédéric Maffray, Ana Silva. b-chromatic number

More information

Dissipative Systems Analysis and Control, Theory and Applications: Addendum/Erratum

Dissipative Systems Analysis and Control, Theory and Applications: Addendum/Erratum Dissipative Systems Analysis and Control, Theory and Applications: Addendum/Erratum Bernard Brogliato To cite this version: Bernard Brogliato. Dissipative Systems Analysis and Control, Theory and Applications:

More information

A Context free language associated with interval maps

A Context free language associated with interval maps A Context free language associated with interval maps M Archana, V Kannan To cite this version: M Archana, V Kannan. A Context free language associated with interval maps. Discrete Mathematics and Theoretical

More information

Some explanations about the IWLS algorithm to fit generalized linear models

Some explanations about the IWLS algorithm to fit generalized linear models Some explanations about the IWLS algorithm to fit generalized linear models Christophe Dutang To cite this version: Christophe Dutang. Some explanations about the IWLS algorithm to fit generalized linear

More information

Impulse response measurement of ultrasonic transducers

Impulse response measurement of ultrasonic transducers Impulse response measurement of ultrasonic transducers F. Kadlec To cite this version: F. Kadlec. Impulse response measurement of ultrasonic transducers. Journal de Physique IV Colloque, 1994, 04 (C5),

More information

Cutwidth and degeneracy of graphs

Cutwidth and degeneracy of graphs Cutwidth and degeneracy of graphs Benoit Kloeckner To cite this version: Benoit Kloeckner. Cutwidth and degeneracy of graphs. IF_PREPUB. 2009. HAL Id: hal-00408210 https://hal.archives-ouvertes.fr/hal-00408210v1

More information

Vibro-acoustic simulation of a car window

Vibro-acoustic simulation of a car window Vibro-acoustic simulation of a car window Christophe Barras To cite this version: Christophe Barras. Vibro-acoustic simulation of a car window. Société Française d Acoustique. Acoustics 12, Apr 12, Nantes,

More information

Theory and Applications of Optimal Control Problems with Time-Delays

Theory and Applications of Optimal Control Problems with Time-Delays Theory and Applications of Optimal Control Problems with Time-Delays University of Münster Institute of Computational and Applied Mathematics South Pacific Optimization Meeting (SPOM) Newcastle, CARMA,

More information

New estimates for the div-curl-grad operators and elliptic problems with L1-data in the half-space

New estimates for the div-curl-grad operators and elliptic problems with L1-data in the half-space New estimates for the div-curl-grad operators and elliptic problems with L1-data in the half-space Chérif Amrouche, Huy Hoang Nguyen To cite this version: Chérif Amrouche, Huy Hoang Nguyen. New estimates

More information

Posterior Covariance vs. Analysis Error Covariance in Data Assimilation

Posterior Covariance vs. Analysis Error Covariance in Data Assimilation Posterior Covariance vs. Analysis Error Covariance in Data Assimilation François-Xavier Le Dimet, Victor Shutyaev, Igor Gejadze To cite this version: François-Xavier Le Dimet, Victor Shutyaev, Igor Gejadze.

More information

On the longest path in a recursively partitionable graph

On the longest path in a recursively partitionable graph On the longest path in a recursively partitionable graph Julien Bensmail To cite this version: Julien Bensmail. On the longest path in a recursively partitionable graph. 2012. HAL Id:

More information

On path partitions of the divisor graph

On path partitions of the divisor graph On path partitions of the divisor graph Paul Melotti, Eric Saias To cite this version: Paul Melotti, Eric Saias On path partitions of the divisor graph 018 HAL Id: hal-0184801 https://halarchives-ouvertesfr/hal-0184801

More information

Axiom of infinity and construction of N

Axiom of infinity and construction of N Axiom of infinity and construction of N F Portal To cite this version: F Portal. Axiom of infinity and construction of N. 2015. HAL Id: hal-01162075 https://hal.archives-ouvertes.fr/hal-01162075 Submitted

More information

On Solving Aircraft Conflict Avoidance Using Deterministic Global Optimization (sbb) Codes

On Solving Aircraft Conflict Avoidance Using Deterministic Global Optimization (sbb) Codes On Solving Aircraft Conflict Avoidance Using Deterministic Global Optimization (sbb) Codes Sonia Cafieri, Frédéric Messine, Ahmed Touhami To cite this version: Sonia Cafieri, Frédéric Messine, Ahmed Touhami.

More information

Finite volume method for nonlinear transmission problems

Finite volume method for nonlinear transmission problems Finite volume method for nonlinear transmission problems Franck Boyer, Florence Hubert To cite this version: Franck Boyer, Florence Hubert. Finite volume method for nonlinear transmission problems. Proceedings

More information

Unbiased minimum variance estimation for systems with unknown exogenous inputs

Unbiased minimum variance estimation for systems with unknown exogenous inputs Unbiased minimum variance estimation for systems with unknown exogenous inputs Mohamed Darouach, Michel Zasadzinski To cite this version: Mohamed Darouach, Michel Zasadzinski. Unbiased minimum variance

More information

Numerical Modeling of Eddy Current Nondestructive Evaluation of Ferromagnetic Tubes via an Integral. Equation Approach

Numerical Modeling of Eddy Current Nondestructive Evaluation of Ferromagnetic Tubes via an Integral. Equation Approach Numerical Modeling of Eddy Current Nondestructive Evaluation of Ferromagnetic Tubes via an Integral Equation Approach Anastassios Skarlatos, Grégoire Pichenot, Dominique Lesselier, Marc Lambert, Bernard

More information

A new approach of the concept of prime number

A new approach of the concept of prime number A new approach of the concept of prime number Jamel Ghannouchi To cite this version: Jamel Ghannouchi. A new approach of the concept of prime number. 4 pages. 24. HAL Id: hal-3943 https://hal.archives-ouvertes.fr/hal-3943

More information

On infinite permutations

On infinite permutations On infinite permutations Dmitri G. Fon-Der-Flaass, Anna E. Frid To cite this version: Dmitri G. Fon-Der-Flaass, Anna E. Frid. On infinite permutations. Stefan Felsner. 2005 European Conference on Combinatorics,

More information

Sparse multivariate factorization by mean of a few bivariate factorizations

Sparse multivariate factorization by mean of a few bivariate factorizations Sparse multivariate factorization by mean of a few bivariate factorizations Bernard Parisse To cite this version: Bernard Parisse. Sparse multivariate factorization by mean of a few bivariate factorizations.

More information

Impedance Transmission Conditions for the Electric Potential across a Highly Conductive Casing

Impedance Transmission Conditions for the Electric Potential across a Highly Conductive Casing Impedance Transmission Conditions for the Electric Potential across a Highly Conductive Casing Hélène Barucq, Aralar Erdozain, David Pardo, Victor Péron To cite this version: Hélène Barucq, Aralar Erdozain,

More information

A Novel Aggregation Method based on Graph Matching for Algebraic MultiGrid Preconditioning of Sparse Linear Systems

A Novel Aggregation Method based on Graph Matching for Algebraic MultiGrid Preconditioning of Sparse Linear Systems A Novel Aggregation Method based on Graph Matching for Algebraic MultiGrid Preconditioning of Sparse Linear Systems Pasqua D Ambra, Alfredo Buttari, Daniela Di Serafino, Salvatore Filippone, Simone Gentile,

More information

Towards an active anechoic room

Towards an active anechoic room Towards an active anechoic room Dominique Habault, Philippe Herzog, Emmanuel Friot, Cédric Pinhède To cite this version: Dominique Habault, Philippe Herzog, Emmanuel Friot, Cédric Pinhède. Towards an active

More information

Quasi-periodic solutions of the 2D Euler equation

Quasi-periodic solutions of the 2D Euler equation Quasi-periodic solutions of the 2D Euler equation Nicolas Crouseilles, Erwan Faou To cite this version: Nicolas Crouseilles, Erwan Faou. Quasi-periodic solutions of the 2D Euler equation. Asymptotic Analysis,

More information

Two Dimensional Linear Phase Multiband Chebyshev FIR Filter

Two Dimensional Linear Phase Multiband Chebyshev FIR Filter Two Dimensional Linear Phase Multiband Chebyshev FIR Filter Vinay Kumar, Bhooshan Sunil To cite this version: Vinay Kumar, Bhooshan Sunil. Two Dimensional Linear Phase Multiband Chebyshev FIR Filter. Acta

More information

Characterization of Equilibrium Paths in a Two-Sector Economy with CES Production Functions and Sector-Specific Externality

Characterization of Equilibrium Paths in a Two-Sector Economy with CES Production Functions and Sector-Specific Externality Characterization of Equilibrium Paths in a Two-Sector Economy with CES Production Functions and Sector-Specific Externality Miki Matsuo, Kazuo Nishimura, Tomoya Sakagami, Alain Venditti To cite this version:

More information

Hook lengths and shifted parts of partitions

Hook lengths and shifted parts of partitions Hook lengths and shifted parts of partitions Guo-Niu Han To cite this version: Guo-Niu Han Hook lengths and shifted parts of partitions The Ramanujan Journal, 009, 9 p HAL Id: hal-00395690

More information

Fast Computation of Moore-Penrose Inverse Matrices

Fast Computation of Moore-Penrose Inverse Matrices Fast Computation of Moore-Penrose Inverse Matrices Pierre Courrieu To cite this version: Pierre Courrieu. Fast Computation of Moore-Penrose Inverse Matrices. Neural Information Processing - Letters and

More information

Understanding SVM (and associated kernel machines) through the development of a Matlab toolbox

Understanding SVM (and associated kernel machines) through the development of a Matlab toolbox Understanding SVM (and associated kernel machines) through the development of a Matlab toolbox Stephane Canu To cite this version: Stephane Canu. Understanding SVM (and associated kernel machines) through

More information

Near-Earth Asteroids Orbit Propagation with Gaia Observations

Near-Earth Asteroids Orbit Propagation with Gaia Observations Near-Earth Asteroids Orbit Propagation with Gaia Observations David Bancelin, Daniel Hestroffer, William Thuillot To cite this version: David Bancelin, Daniel Hestroffer, William Thuillot. Near-Earth Asteroids

More information

A note on the acyclic 3-choosability of some planar graphs

A note on the acyclic 3-choosability of some planar graphs A note on the acyclic 3-choosability of some planar graphs Hervé Hocquard, Mickael Montassier, André Raspaud To cite this version: Hervé Hocquard, Mickael Montassier, André Raspaud. A note on the acyclic

More information

On a series of Ramanujan

On a series of Ramanujan On a series of Ramanujan Olivier Oloa To cite this version: Olivier Oloa. On a series of Ramanujan. Gems in Experimental Mathematics, pp.35-3,, . HAL Id: hal-55866 https://hal.archives-ouvertes.fr/hal-55866

More information

SOLAR RADIATION ESTIMATION AND PREDICTION USING MEASURED AND PREDICTED AEROSOL OPTICAL DEPTH

SOLAR RADIATION ESTIMATION AND PREDICTION USING MEASURED AND PREDICTED AEROSOL OPTICAL DEPTH SOLAR RADIATION ESTIMATION AND PREDICTION USING MEASURED AND PREDICTED AEROSOL OPTICAL DEPTH Carlos M. Fernández-Peruchena, Martín Gastón, Maria V Guisado, Ana Bernardos, Íñigo Pagola, Lourdes Ramírez

More information

Particle-in-cell simulations of high energy electron production by intense laser pulses in underdense plasmas

Particle-in-cell simulations of high energy electron production by intense laser pulses in underdense plasmas Particle-in-cell simulations of high energy electron production by intense laser pulses in underdense plasmas Susumu Kato, Eisuke Miura, Mitsumori Tanimoto, Masahiro Adachi, Kazuyoshi Koyama To cite this

More information

The beam-gas method for luminosity measurement at LHCb

The beam-gas method for luminosity measurement at LHCb The beam-gas method for luminosity measurement at LHCb P. Hopchev To cite this version: P. Hopchev. The beam-gas method for luminosity measurement at LHCb. XLVth Rencontres de Moriond: Electroweak Interactions

More information

A proximal approach to the inversion of ill-conditioned matrices

A proximal approach to the inversion of ill-conditioned matrices A proximal approach to the inversion of ill-conditioned matrices Pierre Maréchal, Aude Rondepierre To cite this version: Pierre Maréchal, Aude Rondepierre. A proximal approach to the inversion of ill-conditioned

More information

Thermodynamic form of the equation of motion for perfect fluids of grade n

Thermodynamic form of the equation of motion for perfect fluids of grade n Thermodynamic form of the equation of motion for perfect fluids of grade n Henri Gouin To cite this version: Henri Gouin. Thermodynamic form of the equation of motion for perfect fluids of grade n. Comptes

More information

approximation results for the Traveling Salesman and related Problems

approximation results for the Traveling Salesman and related Problems approximation results for the Traveling Salesman and related Problems Jérôme Monnot To cite this version: Jérôme Monnot. approximation results for the Traveling Salesman and related Problems. Information

More information

A Study of the Regular Pentagon with a Classic Geometric Approach

A Study of the Regular Pentagon with a Classic Geometric Approach A Study of the Regular Pentagon with a Classic Geometric Approach Amelia Carolina Sparavigna, Mauro Maria Baldi To cite this version: Amelia Carolina Sparavigna, Mauro Maria Baldi. A Study of the Regular

More information

Stickelberger s congruences for absolute norms of relative discriminants

Stickelberger s congruences for absolute norms of relative discriminants Stickelberger s congruences for absolute norms of relative discriminants Georges Gras To cite this version: Georges Gras. Stickelberger s congruences for absolute norms of relative discriminants. Journal

More information

Finite element computation of leaky modes in straight and helical elastic waveguides

Finite element computation of leaky modes in straight and helical elastic waveguides Finite element computation of leaky modes in straight and helical elastic waveguides Khac-Long Nguyen, Fabien Treyssede, Christophe Hazard, Anne-Sophie Bonnet-Ben Dhia To cite this version: Khac-Long Nguyen,

More information

On Symmetric Norm Inequalities And Hermitian Block-Matrices

On Symmetric Norm Inequalities And Hermitian Block-Matrices On Symmetric Norm Inequalities And Hermitian lock-matrices Antoine Mhanna To cite this version: Antoine Mhanna On Symmetric Norm Inequalities And Hermitian lock-matrices 016 HAL Id: hal-0131860

More information

The Mahler measure of trinomials of height 1

The Mahler measure of trinomials of height 1 The Mahler measure of trinomials of height 1 Valérie Flammang To cite this version: Valérie Flammang. The Mahler measure of trinomials of height 1. Journal of the Australian Mathematical Society 14 9 pp.1-4.

More information

Extended-Kalman-Filter-like observers for continuous time systems with discrete time measurements

Extended-Kalman-Filter-like observers for continuous time systems with discrete time measurements Extended-Kalman-Filter-lie observers for continuous time systems with discrete time measurements Vincent Andrieu To cite this version: Vincent Andrieu. Extended-Kalman-Filter-lie observers for continuous

More information

Solving the neutron slowing down equation

Solving the neutron slowing down equation Solving the neutron slowing down equation Bertrand Mercier, Jinghan Peng To cite this version: Bertrand Mercier, Jinghan Peng. Solving the neutron slowing down equation. 2014. HAL Id: hal-01081772

More information

On the link between finite differences and derivatives of polynomials

On the link between finite differences and derivatives of polynomials On the lin between finite differences and derivatives of polynomials Kolosov Petro To cite this version: Kolosov Petro. On the lin between finite differences and derivatives of polynomials. 13 pages, 1

More information

The Windy Postman Problem on Series-Parallel Graphs

The Windy Postman Problem on Series-Parallel Graphs The Windy Postman Problem on Series-Parallel Graphs Francisco Javier Zaragoza Martínez To cite this version: Francisco Javier Zaragoza Martínez. The Windy Postman Problem on Series-Parallel Graphs. Stefan

More information

A remark on a theorem of A. E. Ingham.

A remark on a theorem of A. E. Ingham. A remark on a theorem of A. E. Ingham. K G Bhat, K Ramachandra To cite this version: K G Bhat, K Ramachandra. A remark on a theorem of A. E. Ingham.. Hardy-Ramanujan Journal, Hardy-Ramanujan Society, 2006,

More information

Numerical Optimal Control Overview. Moritz Diehl

Numerical Optimal Control Overview. Moritz Diehl Numerical Optimal Control Overview Moritz Diehl Simplified Optimal Control Problem in ODE path constraints h(x, u) 0 initial value x0 states x(t) terminal constraint r(x(t )) 0 controls u(t) 0 t T minimize

More information

Lower bound of the covering radius of binary irreducible Goppa codes

Lower bound of the covering radius of binary irreducible Goppa codes Lower bound of the covering radius of binary irreducible Goppa codes Sergey Bezzateev, Natalia Shekhunova To cite this version: Sergey Bezzateev, Natalia Shekhunova. Lower bound of the covering radius

More information

CHAPTER 3 THE MAXIMUM PRINCIPLE: MIXED INEQUALITY CONSTRAINTS. p. 1/73

CHAPTER 3 THE MAXIMUM PRINCIPLE: MIXED INEQUALITY CONSTRAINTS. p. 1/73 CHAPTER 3 THE MAXIMUM PRINCIPLE: MIXED INEQUALITY CONSTRAINTS p. 1/73 THE MAXIMUM PRINCIPLE: MIXED INEQUALITY CONSTRAINTS Mixed Inequality Constraints: Inequality constraints involving control and possibly

More information

Sound intensity as a function of sound insulation partition

Sound intensity as a function of sound insulation partition Sound intensity as a function of sound insulation partition S. Cvetkovic, R. Prascevic To cite this version: S. Cvetkovic, R. Prascevic. Sound intensity as a function of sound insulation partition. Journal

More information

On Politics and Argumentation

On Politics and Argumentation On Politics and Argumentation Maria Boritchev To cite this version: Maria Boritchev. On Politics and Argumentation. MALOTEC, Mar 2017, Nancy, France. 2017. HAL Id: hal-01666416 https://hal.archives-ouvertes.fr/hal-01666416

More information

Stochastic invariances and Lamperti transformations for Stochastic Processes

Stochastic invariances and Lamperti transformations for Stochastic Processes Stochastic invariances and Lamperti transformations for Stochastic Processes Pierre Borgnat, Pierre-Olivier Amblard, Patrick Flandrin To cite this version: Pierre Borgnat, Pierre-Olivier Amblard, Patrick

More information

Chebyshev polynomials, quadratic surds and a variation of Pascal s triangle

Chebyshev polynomials, quadratic surds and a variation of Pascal s triangle Chebyshev polynomials, quadratic surds and a variation of Pascal s triangle Roland Bacher To cite this version: Roland Bacher. Chebyshev polynomials, quadratic surds and a variation of Pascal s triangle.

More information

On Poincare-Wirtinger inequalities in spaces of functions of bounded variation

On Poincare-Wirtinger inequalities in spaces of functions of bounded variation On Poincare-Wirtinger inequalities in spaces of functions of bounded variation Maïtine Bergounioux To cite this version: Maïtine Bergounioux. On Poincare-Wirtinger inequalities in spaces of functions of

More information

Some tight polynomial-exponential lower bounds for an exponential function

Some tight polynomial-exponential lower bounds for an exponential function Some tight polynomial-exponential lower bounds for an exponential function Christophe Chesneau To cite this version: Christophe Chesneau. Some tight polynomial-exponential lower bounds for an exponential

More information

Multiple sensor fault detection in heat exchanger system

Multiple sensor fault detection in heat exchanger system Multiple sensor fault detection in heat exchanger system Abdel Aïtouche, Didier Maquin, Frédéric Busson To cite this version: Abdel Aïtouche, Didier Maquin, Frédéric Busson. Multiple sensor fault detection

More information

There are infinitely many twin primes 30n+11 and 30n+13, 30n+17 and 30n+19, 30n+29 and 30n+31

There are infinitely many twin primes 30n+11 and 30n+13, 30n+17 and 30n+19, 30n+29 and 30n+31 There are infinitely many twin primes 30n+11 and 30n+13, 30n+17 and 30n+19, 30n+29 and 30n+31 Sibiri Christian Bandre To cite this version: Sibiri Christian Bandre. There are infinitely many twin primes

More information

Symmetric Norm Inequalities And Positive Semi-Definite Block-Matrices

Symmetric Norm Inequalities And Positive Semi-Definite Block-Matrices Symmetric Norm Inequalities And Positive Semi-Definite lock-matrices Antoine Mhanna To cite this version: Antoine Mhanna Symmetric Norm Inequalities And Positive Semi-Definite lock-matrices 15

More information

A Slice Based 3-D Schur-Cohn Stability Criterion

A Slice Based 3-D Schur-Cohn Stability Criterion A Slice Based 3-D Schur-Cohn Stability Criterion Ioana Serban, Mohamed Najim To cite this version: Ioana Serban, Mohamed Najim. A Slice Based 3-D Schur-Cohn Stability Criterion. ICASSP 007, Apr 007, Honolulu,

More information

Separator Algebra for State Estimation

Separator Algebra for State Estimation Separator Algebra for State Estimation Luc Jaulin To cite this version: Luc Jaulin. Separator Algebra for State Estimation. SMART 2015, Sep 2015, Manchester, United Kingdom. 2015,. HAL Id: hal-01236498

More information

A novel method for estimating the flicker level generated by a wave energy farm composed of devices operated in variable speed mode

A novel method for estimating the flicker level generated by a wave energy farm composed of devices operated in variable speed mode A novel method for estimating the flicker level generated by a wave energy farm composed of devices operated in variable speed mode Anne Blavette, Dara O Sullivan, Ray Alcorn, Mohamed Machmoum, Michael

More information

Water Vapour Effects in Mass Measurement

Water Vapour Effects in Mass Measurement Water Vapour Effects in Mass Measurement N.-E. Khélifa To cite this version: N.-E. Khélifa. Water Vapour Effects in Mass Measurement. Measurement. Water Vapour Effects in Mass Measurement, May 2007, Smolenice,

More information