Metzler Matrix Transform Determination using a Nonsmooth Optimization Technique with an Application to Interval Observers

Size: px
Start display at page:

Download "Metzler Matrix Transform Determination using a Nonsmooth Optimization Technique with an Application to Interval Observers"

Transcription

1 Downloae 4/7/18 to Reistribution subject to SIAM license or copyright; see Metzler Matrix Transform Determination using a Nonsmooth Optimization Technique with an Application to Interval Observers Abstract Emmanuel Chambon, Pierre Apkarian Laurent Burlion The paper eals with the esign of cooperative systems which formulates as computing a state coorinate transform such that the resulting ynamics are both stable an cooperative. The esign of cooperative systems is a key problem to etermine interval observers. Solutions are provie in the literature to transform any system into a cooperative system. A novel approach is propose which reformulates into a stabilization problem. A solution is foun using nonsmooth optimization techniques. 1 Introuction. Cooperative systems that is systems whose Jacobian matrix is Metzler (see Definition 2.1) have the interesting property to keep partial orering between two trajectories [15, 1]. Such a property makes them key caniates for use as interval observers where the goal is to enclose a given variable x(t) between two other timeepenent variables x(t) x(t) x(t) especially when information on any external isturbance is not available. Relate works inclue for example [9]. Many systems incluing the consiere generic launch vehicle moel are however not cooperative. A solution to this problem was propose in [13] where a time-varying change of coorinates is use to efine interval observers applie to linear time-invariant non-cooperative systems. It was inee shown in [12] that in some cases no timeinvariant change of coorinates can be foun to guarantee exponential stability of the obtaine interval observer. Despite its theoretical interest an the guarantees it offers, this approach may be har to implement in practice. More recent works like [14] an [6] interestingly propose techniques to fin a static state coorinate transform P an an observer gain L so that M = P(A LC)P 1 is Metzler even for a non-metzler matrix A. Methos base on the numerical resolution of a Sylvester equation were propose. In these methos This article contains figures in color for better unerstaning. Onera The French Aerospace Lab, BP7425, 2 avenue Éouar Belin, FR-3155 Toulouse Ceex 4, France. Corresponing author: Emmanuel.Chambon@onera.fr. a target matrix M must be provie which may reuce the set of acceptable solutions. A similar approach is use in [4] with the aim to overcome the mentione limitation of time-invariant change of coorinates. A specific interval observer structure making use of classical observers is evelope with an application to nonlinear systems affine in the unmeasure part of the state variables. It is however assume that the static matrix transform is known. In this paper an alternative technique to these methos is propose. A Metzler Matrix Transform synthesis metho is evelope where the computation of both P an L is performe simultaneously which results in M not being fixe a priori. As far as control theory is concerne, nonsmooth H synthesis optimization techniques as presente in [3, 2] offer the possibility to tune a structure controller against multiple control requirements. Recent avances [1] also make it possible to take multiple moels into account when robustness is at stake. Amissible requirements inclue close-loop poles location or noise rejection. In this article, this control approach will be use to specify estimation quality requirements on gain L which will be use within a Luenberger observer. It is also shown that the problem of fining a pair (P,L) such that M = P(A LC)P 1 is Hurwitz Metzler may be expresse as a control problem on which these techniques will be use. Computing a Metzler Matrix Transform is ifficult. After reformulation into a control problem so as to use nonsmooth H synthesis techniques, a numerical solution to this mathematical problem is propose. Definitions an notations are recalle in 2. The paper is structure as follows. In 3 (resp. 4) the consiere mathematical (resp. control) problem is expose. A solution to these problems is then propose in 5. The theory of interval observers an how they can be use to eterministically bracket an estimation error is presente in 6. Examples of applications are etaile in 7. In particular, the algorithm an interval observer approach are teste on a generic launch vehicle rigi moel in Copyright by SIAM.

2 2 Definitions an notations. The Laplace transform is enote s. Given two integers (i,j) symbol δ ij is efine by (4.3) min p { } max Twi z i (C(s,p)) 2/ i=1,...,n soft Downloae 4/7/18 to Reistribution subject to SIAM license or copyright; see (2.1) (i,j), δ ij = { 1 if i = j otherwise Unless mentione, i an j are integer variables satisfying 1 i,j n where n refers to a matrix imension. I stans for ientity matrix with aequate imension. For a given matrix A R n m, let enote A + = max(a,) an A = A + A where max is the element-wise operator. Definition 2.1. Let A = (a ij ) R n n. The matrix A is sai to be Metzler if (2.2) i j, a ij The matrix A is Hurwitz if all its eigenvalues real parts are strictly negative. Definition 2.2. For given matrices A an C, a Metzler Matrix Transform is a pair (P,L) with P R n n an L R n m s.t. P (A LC)P 1 is Metzler. 3 Problem statement. Let G = (A,B,C,D) a system with n states, m n measurements. It is suppose (A, C) is observable. The following problem is consiere for which an optimization-base solution is propose in 5. Problem 3.1. Fin a Metzler Matrix Transform(P, L) such that M = P (A LC)P 1 is Hurwitz Metzler. In this approach L is use to place poles so that a Hurwitz matrix is obtaine. It can be ientifie to an observer gain. In resulting new coorinates, G reformulates into G = ( M,PB,CP 1,D ). 4 Control problem (application specific). When system G or G expresse in new coorinates shoul be observe or stabilize, this becomes a control problem. Using nonsmooth H control formalism, this problem can be formulate as follows Problem 4.1. Let C(s,p) be a collection of LTI systems epening on tunable parameters p. Let n soft an n har two positive integers an w an z two vectors of R n soft+n har. For a given integer i n soft + n har, the transfer functions between input w i an output z i over the collection C is enote T wi z i (C(s,p)). The problem is to fin p satisfying subject to T wj z j (C(s,p)) 2/ 1 with j = 1,...,n har. To solve this control problem optimization-base techniques can be use like nonsmooth H synthesis as presente in [1]. These techniques were implemente into numerical solvers as presente in [8]. More specifically the systune routine from the Matlab c Robust Control Toolbox 212b an higher can be use. An optimal solution is foun when the algorithm manages to rive har constraints below unity while minimizing soft constraints (also calle objectives). In 5 it will be shown that problem 3.1 reformulates into an optimization problem which can be solve using these optimization-base techniques. 5 Propose solution. Before going into the etails of the metho, the reaer shoul be remine that the propose solution is: a numerical solution: it is obtaine using an optimization algorithm; A local optimal solution: because the problem is non-convex in (P, L) algorithm converges towars an optimal local solution. Multiple ranom restarts of the optimization algorithmcanbeusetofinanoptimalsolutiononalarger set of solutions. In case some targete properties of the solution are not satisfie, it may be necessary to weaken some of the formulate constraints. It may help the optimization algorithm to fin a better local solution. 5.1 Note on the existence of a trivial solution. Since iagonal matrices comply with efinition 2.1 there exists a trivial solution to problem 3.1. Proof. With (A, C) observable, choose L so that A LC eigenvalues are negative real numbers an choose P as the matrix of associate eigenvectors. Then M = P (A LC)P 1 is iagonal Hurwitz hence is a solution to problem 3.1. Note this trivial solution may not satisfy control requirements state in problem 4.1. Also this may lea to large gains L when using pole placement methos. 5.2 Note on Sylvester equation approach. To fin Metzler Matrix Transform (P,L) such that M = 26 Copyright by SIAM.

3 Downloae 4/7/18 to Reistribution subject to SIAM license or copyright; see P(A LC)P 1 is Metzler, one can solve the following Sylvester equation as suggeste in [14] (5.4) PA MP = QC where A is known, L has been obtaine solving a pole placement problem an (M,Q = PL) are arbitrarily chosen such that M an A LC have the same eigenvalues an M is Hurwitz Metzler. Note however that this equation has a unique solution if an only if A an M have istinct eigenvalues. Because the approach presente in the sequel oes not rely on an a priori choice of M or Q it offers more freeom in the resolution. On the other han, the contingency of a local vs. global optimization technique has to be accepte. 5.3 Metzler conitions stabilization problem. Let M = P (A LC)P 1 R n n where P an L are ecision variables. For M to be Metzler, the n(n 1) following inequalities must be satisfie (5.5) i j, M ij = [ P (A LC)P 1] ij = i P (A LC)P 1 j where i = (δ ik ) 1 k n is a column vector. For a given pair (i,j), with i j, the corresponing inequality can be seen as an anti-stabilization problem in the ecision variables P an L. 5.4 Control synthesis approach an moels. To fin a pair (P,L) satisfying both M = P(A LC)P 1 an control constraints expresse on G (eventually consiere in-line with other systems), any nonsmooth nonconvex optimization technique can be use. It is propose to use the approach presente in [1] which can hanle multiple moels to synthesize control laws accoring to specifie constraints. As far as the conitions in 5.3 are consiere, the constraints can be reformulate into the propose control framework. The following fictitious 1 systems are consiere (5.6) i j, G ij M = [ Mij (P,L) R 1 1 n 1 From a control point of view, ensuring i j, M ij is equivalent to stabilizing these systems G ij M. The following collections are consiere in the control synthesis 1 In the sense they have no input nor output. ] (C1){ n(n} 1) uniimensional fictitious systems G ij M on which a requirement on close-loop i,j poles location is expresse (minimum ecay an max frequency); (C2) (optional) { } n(n 1) uniimensional fictitious systems G ij M withstatematrixm ij (P,L) Mij max. i,j This helps to restrict the set of acceptable solutions when < Mij max < +. As such, upon multiple restarts, the optimization algorithm converges more easily ue to limitation of the initialising variables excursion aroun a smaller set of potential local optima; (C3) Original plant moel G = (A,B,C,D) in-line with aitional systems eventually epening on L an aitional variables to enforce system stabilization or estimation criteria; (C4) (optional) any other moel to enforce specific properties. 6 Application to Interval Observers. The algorithm was evelope towars a specific application to interval observers which is presente here. The theory presente in this section is inspire from the works in [13] an [14]. Since the propose algorithm also synthesizes an observer gain L, it is propose to bracket the estimation error using interval observers so as to frame the plant state x in return. 6.1 Plant moel. The following plant moel expresse in the state space is consiere. Using Popov- Belevitch-Hautus Lemma, observability of(a, C) can be checke to account for possibly unobservable eigenvalues. ẋ = Ax+B ( +B ) u u (6.7) (G) = Ax+B u y = Cx where x R n an y R m with m n. Initial conitions are given by a vector x. Input is an unknown isturbance but it is suppose there exists known bouns an such that t, (t) (t) (t). It is suppose a ynamic controller K(s) has been esigne ensuring system stability in these conitions. Stabilizing output-feeback control law u = K(s)y is then applie to the system. 6.2 Luenberger observer. The following Luenberger observer is consiere 27 Copyright by SIAM.

4 Downloae 4/7/18 to Reistribution subject to SIAM license or copyright; see x = A x+b u u+l(y C x) (6.8) (G obs ) ŷ = C x x() = x The objective is to ensure minimal estimation error. 6.3 Estimation error system Let e = x x the estimation error, it is inferre (6.9) ė = (A LC)e+B with e() = e = x x. The objective is to fin (e,e,e,e ) s.t. for e [e,e ] then t, e(t) e(t) e(t). The pair (e,e ) is suppose known from now on. 6.4 Interval observer. To use the results presente in [14], a Metzler Matrix Transform nees to be foun an the error estimation system expresse into the corresponing new coorinates. It is suppose synthesis in 5 has returne (P,L) s.t. M = P (A LC)P 1 is Hurwitz Metzler an estimation quality requirements on system (6.9) are satisfie. Using the change of coorinates e z = Pe, system (6.9) becomes (6.1) ė z = P (A LC)P 1 e z +PB = Me z +B where B = PB. Using [5, Lemma 1] an notations in 2, an interval observer for system (6.1) is given by (6.11) uner initial conitions (6.12) { ėz = Me z +B + B ė z = Me z +B + B e z () = P + e P e e z () = P + e P e This interval observer is compose of two autonomous systems (no epenency on system output y). Let T = P 1, the bouns on e are obtaine using [5, Lemma 1]: (6.13) { e = T + e z T e z e = T + e z T e z Then for an initial estimation error e [e,e ], a time-varying bracketing of the state x is obtaine as x+e x x+e. The system compose of autonomous systems (6.11) with output y e = (e,e) is calle (G e ). 7 Examples. The following examples are use to emonstrate the possibilities of the algorithm etaile here with an application to interval observers. Note that syntheses were performe using systune function from the Robust Control Toolbox 214b [11] correctly parametrize to benefit from the Parallel Computing Toolbox. Other implementations may be use. 7.1 Thir-orer system with unobservable moe. This example is inspire from the partial linear system example presente in [14]. It is given by 2 (7.14) A = , C = [ 1 ] 3 4 The matrix B is not recalle here since no isturbance input is consiere. The problem reuces to fining a suitable Metzler Matrix Transform with limite control constraints. Note however that the complex moe 4±j 3 is not observable. To solve this problem, collections (C1) an (C2) with n = 3 an (i,j), Mij max = 1 are use. Moreover using (C4), A LC eigenvalues real part are force to stay within [ 1, 3.1 3]. A solution is typically foun in less than 5 iterations an after 3 restarts. The following results have been compute (7.15) M = , P = , L = It is reaily verifie that M = P(A LC)P 1 is Hurwitz Metzler. Accoring to results in 6 one can note that the estimation error epens on the initial error but converges towars zero since no other isturbance is consiere. 7.2 Sixth-orer system with two complex moes. This example is inspire from the one presente in [13]. It is given by (7.16) A = , B = 5 4, C = [ 1 ], D = [ 1 ] 28 Copyright by SIAM.

5 Downloae 4/7/18 to Reistribution subject to SIAM license or copyright; see The first input correspons to a isturbance input on the measurement. Its effect on the estimation quality nees to be mitigate using an appropriate isturbance rejection requirement. Note that since y = Cx+, the estimation error system is efine by (7.17) ė = (A LC)e L rather than by (6.9). To solve this problem, a collection of synthesis moels compose of (C1) to (C4) with n = 6 an (i,j), Mij max = is use. Estimation quality is ensure through minimization of the H 2 - norm of the transfer from to e using moel (C3). Stability of the estimation error subsystem is ensure through (C4) where A LC eigenvalues real parts are forcetostayintheinterval [ 1, 3.1 3]. Asolution is typically foun in 897 iterations an after 4 restarts, see (7.18) on Fig. 1. A similar construction to the one presente in 6 can then be use to frame state x. 7.3 Fifth-orer rigi launcher longituinal moel. The approach in 6 is applie to a generic rigi launch vehicle longituinal moel with unknown win input. No uncertainty is consiere in this article. Like other examples, the metho propose in 5 is use to compute P an L. Simulations are then run using a simplifie win profile Moel. The moel (7.19) in Fig. 2 is consiere where the first input correspons to the unknown win input an D =. The secon input correspons to the thruster orientation input signal to which the stabilizing control law is applie. Note that n = Synthesis an results. To solve the problem, the collections of moels (C1) to (C4) are use where (i,j), Mij max = 5 an A LC eigenvalues real parts are force to lie in [ 1.1 2, 1.1 2]. Using moel (C3) a minimization constraint on the weighte H 2 norm from unknown input R to estimation error e R 5 is expresse. The optimization algorithm generally gives a solution in aroun 11 iterations an 6 restarts. Results are shown in (7.2) in Fig Simulation. Since the system is unstable, the simulation is performe after structure H synthesis of a ynamic stabilizing controller K(s) for this system. As this is not the main purpose of this work, it is not etaile here. Fig. 3 illustrates how the ifferent systems G, G obs an G e are relate. Note that system G e oes not interact with the stabilize plant moel. Using win profile shown in Fig. 4 with +/ 7 m/s uncertainty on win spee, the results shown in Fig. 5 u G e G K e e z y G obs Figure3: Simulationmoelwhere(G e )isacombination of two autonomous systems. an 6 are obtaine. As expecte it is interesting to note that espite state estimate is use to express bounaries on the state, it oes not necessarily lie in the resulting interval [ x+e, x+e] since e (resp. e) can be positive (resp. negative). 7.4 Execution summary. Executions were performe running Matlab c R214b with Parallel Computing Toolbox version 6.5 on a Winows c 7 64 bits station with 8 Go RAM an Intel c Xeon processor E5-167 v2 3 GHz (qua-core). A summary of these executions for each example is shown in Table 1. Note the number of iterations an time results are only inicative since they may vary from one run to another but they are representative of the complexity of the problem. 8 Conclusions. In this article an application of nonsmooth optimization techniques [1] to numerically solve a mathematical problem combine to a control problem has been pre- Win spee (m/s) Simulation time (s) Figure 4: Win spee profile (in blue) an known bouns an use in simulation. x 29 Copyright by SIAM.

6 Downloae 4/7/18 to Reistribution subject to SIAM license or copyright; see (7.18) M = , P = , L = Figure 1: A solution obtaine on example (7.16) (7.19) A = , B = , C = (7.2) M = , P = , L = Figure 2: Rigi launch vehicle longituinal moel with etectors ynamics (top, see 7.3) an obtaine Metzler Matrix Transform (bottom). Ex. Res. Dim. (n) # Moels Restarts Iter. Ref. (7.14) (7.15) [14] (7.16) (7.18) [13] (7.19) (7.2) Table 1: Metzler Matrix Transform synthesis typical execution summary. sente. To etermine a Metzler Matrix Transform the corresponing mathematical problem 3.1 was reformulate into a control problem 4.1. Combine with control requirements, a local optimal solution to this problem can be foun. This approach has been successfully applie to various examples incluing a rigi launch vehicle moel. In comparison with other methos, this approach allows for simultaneous tuning of P an L an oes not make assumption on the targete M matrix structure. Moreover, by benefiting from observer structures as propose in [14] an [4] implementing the resulting interval observer is straightforwar in practise. Further improvements will be eicate to reuce complexity since non-negligible computing resources are neee with multiple algorithm restarts before converging towars an acceptable solution especially in the case of higher-imensional problems. Other problems coul also be consiere like fining static P such that P [A(y) L(y)C]P 1 is Metzler where y R m is the known system output signal. The interest woul be to benefit from the interval observer structure propose in [4]. In this work knowing such P is consiere an hy- 21 Copyright by SIAM.

7 Downloae 4/7/18 to Reistribution subject to SIAM license or copyright; see excapt eψ evz.1 eẋcapt e ψ Figure 5: Simulation results on example (7.19): estimation error e = x x is represente in blue. The bouns obtaine using interval observer expression as in (6.11) are represente in re an green. xcapt ψ Time(s) 33.6 vz Time(s) ẋcapt Time(s) 1 3 Time(s).5 5 ψ Time(s) Figure 6: Simulation results on example (7.19) using win profile in Fig. 4: the state (blue), the state estimate (magenta) an the upper (resp. lower) boun (re, resp. green) are represente. Zoom is performe on otherwise inistinguishable curves. pothesis, which might be limiting. Also note that other systems like positive continuous-time linear systems [7] also have a Metzler state-space matrix which gives hints on a wier scope for this article. References [1] P. Apkarian, Tuning controllers against multiple esign requirements, in Proc. of the American Control Conference, Washington, USA, June 213, pp [2] P. Apkarian an D. Noll, Nonsmooth H synthesis, IEEE Transactions on Automatic Control, 51 (26), pp [3] J. V. Burke, D. Henrion, A. S. Lewis, an M. L. Overton, HIFOO a MATLAB package for fixeorer controller esign an H optimization, in Proc. of the 5th IFAC Symposium on Robust Control Design, Toulouse, France, Aug. 26. [4] T. N. Dinh, F. Mazenc, an S.-I. Niculescu, Interval observer compose of observers for nonlinear systems, in Proc. of the European Control Conference, Strasbourg, France, June 214, pp [5] D. Efimov, T. Raïssi, S. Chebotarev, an A. Zolghari, Interval state observer for nonlinear timevarying systems, Automatica, 49 (213), pp [6] D. Efimov, T. Raïssi, an A. Zolghari, Control of nonlinear an LPV systems: Interval observer-base framework, IEEE Transactions on Automatic Control, 58 (213), pp [7] L. Farina an S. Rinali, Positive Linear Systems: Theory an Applications, John Wiley & Sons, 2. [8] P. Gahinet an P. Apkarian, Frequency-omain tuning of fixe-structure control systems, in Proc. of the UKACC International Conference on Control, Sept. 212, pp [9] J. L. Gouzé, A. Rapaport, an M. Z. Haj- Saok, Interval observers for uncertain biological systems, Ecological Moelling, 133 (2), pp [1] L. Mailleret, Stabilisation globale es systèmes positifs mal connus - Applications en Biologie, PhD thesis, Université e Nice Sophia-Antipolis, Nice, May 24. [11] MATLAB, Robust Control Toolbox version 5.2 (R214b), The MathWorks Inc., Natick, Massachusetts, 214. [12] F. Mazenc an O. Bernar, Asymptotically stable interval observers for planar systems with complex poles, IEEE Transactions on Automatic Control, 55 (21), pp [13], Interval observers for linear time-invariant systems with isturbances, Automatica, 47 (211), pp [14] T. Raïssi, D. Efimov, an A. Zolghari, Interval state estimation for a class of nonlinear systems, IEEE Transactions on Automatic Control, 57 (212), pp [15] H. L. Smith, Monotone ynamical systems: an introuction to the theory of competitive an cooperative systems, Bulletin of the American Mathematical Society, 33 (1996), pp Copyright by SIAM.

Optimal Variable-Structure Control Tracking of Spacecraft Maneuvers

Optimal Variable-Structure Control Tracking of Spacecraft Maneuvers Optimal Variable-Structure Control racking of Spacecraft Maneuvers John L. Crassiis 1 Srinivas R. Vaali F. Lanis Markley 3 Introuction In recent years, much effort has been evote to the close-loop esign

More information

Adaptive Gain-Scheduled H Control of Linear Parameter-Varying Systems with Time-Delayed Elements

Adaptive Gain-Scheduled H Control of Linear Parameter-Varying Systems with Time-Delayed Elements Aaptive Gain-Scheule H Control of Linear Parameter-Varying Systems with ime-delaye Elements Yoshihiko Miyasato he Institute of Statistical Mathematics 4-6-7 Minami-Azabu, Minato-ku, okyo 6-8569, Japan

More information

Separation Principle for a Class of Nonlinear Feedback Systems Augmented with Observers

Separation Principle for a Class of Nonlinear Feedback Systems Augmented with Observers Proceeings of the 17th Worl Congress The International Feeration of Automatic Control Separation Principle for a Class of Nonlinear Feeback Systems Augmente with Observers A. Shiriaev, R. Johansson A.

More information

Laplacian Cooperative Attitude Control of Multiple Rigid Bodies

Laplacian Cooperative Attitude Control of Multiple Rigid Bodies Laplacian Cooperative Attitue Control of Multiple Rigi Boies Dimos V. Dimarogonas, Panagiotis Tsiotras an Kostas J. Kyriakopoulos Abstract Motivate by the fact that linear controllers can stabilize the

More information

EE 370L Controls Laboratory. Laboratory Exercise #7 Root Locus. Department of Electrical and Computer Engineering University of Nevada, at Las Vegas

EE 370L Controls Laboratory. Laboratory Exercise #7 Root Locus. Department of Electrical and Computer Engineering University of Nevada, at Las Vegas EE 370L Controls Laboratory Laboratory Exercise #7 Root Locus Department of Electrical an Computer Engineering University of Nevaa, at Las Vegas 1. Learning Objectives To emonstrate the concept of error

More information

Diagonalization of Matrices Dr. E. Jacobs

Diagonalization of Matrices Dr. E. Jacobs Diagonalization of Matrices Dr. E. Jacobs One of the very interesting lessons in this course is how certain algebraic techniques can be use to solve ifferential equations. The purpose of these notes is

More information

APPROXIMATE SOLUTION FOR TRANSIENT HEAT TRANSFER IN STATIC TURBULENT HE II. B. Baudouy. CEA/Saclay, DSM/DAPNIA/STCM Gif-sur-Yvette Cedex, France

APPROXIMATE SOLUTION FOR TRANSIENT HEAT TRANSFER IN STATIC TURBULENT HE II. B. Baudouy. CEA/Saclay, DSM/DAPNIA/STCM Gif-sur-Yvette Cedex, France APPROXIMAE SOLUION FOR RANSIEN HEA RANSFER IN SAIC URBULEN HE II B. Bauouy CEA/Saclay, DSM/DAPNIA/SCM 91191 Gif-sur-Yvette Ceex, France ABSRAC Analytical solution in one imension of the heat iffusion equation

More information

Criteria for Global Stability of Coupled Systems with Application to Robust Output Feedback Design for Active Surge Control

Criteria for Global Stability of Coupled Systems with Application to Robust Output Feedback Design for Active Surge Control Criteria for Global Stability of Couple Systems with Application to Robust Output Feeback Design for Active Surge Control Shiriaev, Anton; Johansson, Rolf; Robertsson, Aners; Freiovich, Leoni 9 Link to

More information

Math 342 Partial Differential Equations «Viktor Grigoryan

Math 342 Partial Differential Equations «Viktor Grigoryan Math 342 Partial Differential Equations «Viktor Grigoryan 6 Wave equation: solution In this lecture we will solve the wave equation on the entire real line x R. This correspons to a string of infinite

More information

A new approach to explicit MPC using self-optimizing control

A new approach to explicit MPC using self-optimizing control 28 American Control Conference Westin Seattle Hotel, Seattle, Washington, USA June -3, 28 WeA3.2 A new approach to explicit MPC using self-optimizing control Henrik Manum, Sriharakumar Narasimhan an Sigur

More information

VIRTUAL STRUCTURE BASED SPACECRAFT FORMATION CONTROL WITH FORMATION FEEDBACK

VIRTUAL STRUCTURE BASED SPACECRAFT FORMATION CONTROL WITH FORMATION FEEDBACK AIAA Guiance, Navigation, an Control Conference an Exhibit 5-8 August, Monterey, California AIAA -9 VIRTUAL STRUCTURE BASED SPACECRAT ORMATION CONTROL WITH ORMATION EEDBACK Wei Ren Ranal W. Bear Department

More information

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs Lectures - Week 10 Introuction to Orinary Differential Equations (ODES) First Orer Linear ODEs When stuying ODEs we are consiering functions of one inepenent variable, e.g., f(x), where x is the inepenent

More information

ELEC3114 Control Systems 1

ELEC3114 Control Systems 1 ELEC34 Control Systems Linear Systems - Moelling - Some Issues Session 2, 2007 Introuction Linear systems may be represente in a number of ifferent ways. Figure shows the relationship between various representations.

More information

Lower bounds on Locality Sensitive Hashing

Lower bounds on Locality Sensitive Hashing Lower bouns on Locality Sensitive Hashing Rajeev Motwani Assaf Naor Rina Panigrahy Abstract Given a metric space (X, X ), c 1, r > 0, an p, q [0, 1], a istribution over mappings H : X N is calle a (r,

More information

Euler equations for multiple integrals

Euler equations for multiple integrals Euler equations for multiple integrals January 22, 2013 Contents 1 Reminer of multivariable calculus 2 1.1 Vector ifferentiation......................... 2 1.2 Matrix ifferentiation........................

More information

19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control

19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control 19 Eigenvalues, Eigenvectors, Orinary Differential Equations, an Control This section introuces eigenvalues an eigenvectors of a matrix, an iscusses the role of the eigenvalues in etermining the behavior

More information

BEYOND THE CONSTRUCTION OF OPTIMAL SWITCHING SURFACES FOR AUTONOMOUS HYBRID SYSTEMS. Mauro Boccadoro Magnus Egerstedt Paolo Valigi Yorai Wardi

BEYOND THE CONSTRUCTION OF OPTIMAL SWITCHING SURFACES FOR AUTONOMOUS HYBRID SYSTEMS. Mauro Boccadoro Magnus Egerstedt Paolo Valigi Yorai Wardi BEYOND THE CONSTRUCTION OF OPTIMAL SWITCHING SURFACES FOR AUTONOMOUS HYBRID SYSTEMS Mauro Boccaoro Magnus Egerstet Paolo Valigi Yorai Wari {boccaoro,valigi}@iei.unipg.it Dipartimento i Ingegneria Elettronica

More information

Design A Robust Power System Stabilizer on SMIB Using Lyapunov Theory

Design A Robust Power System Stabilizer on SMIB Using Lyapunov Theory Design A Robust Power System Stabilizer on SMIB Using Lyapunov Theory Yin Li, Stuent Member, IEEE, Lingling Fan, Senior Member, IEEE Abstract This paper proposes a robust power system stabilizer (PSS)

More information

Implicit Lyapunov control of closed quantum systems

Implicit Lyapunov control of closed quantum systems Joint 48th IEEE Conference on Decision an Control an 28th Chinese Control Conference Shanghai, P.R. China, December 16-18, 29 ThAIn1.4 Implicit Lyapunov control of close quantum systems Shouwei Zhao, Hai

More information

ensembles When working with density operators, we can use this connection to define a generalized Bloch vector: v x Tr x, v y Tr y

ensembles When working with density operators, we can use this connection to define a generalized Bloch vector: v x Tr x, v y Tr y Ph195a lecture notes, 1/3/01 Density operators for spin- 1 ensembles So far in our iscussion of spin- 1 systems, we have restricte our attention to the case of pure states an Hamiltonian evolution. Toay

More information

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions Working Paper 2013:5 Department of Statistics Computing Exact Confience Coefficients of Simultaneous Confience Intervals for Multinomial Proportions an their Functions Shaobo Jin Working Paper 2013:5

More information

LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION

LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION The Annals of Statistics 1997, Vol. 25, No. 6, 2313 2327 LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION By Eva Riccomagno, 1 Rainer Schwabe 2 an Henry P. Wynn 1 University of Warwick, Technische

More information

State observers and recursive filters in classical feedback control theory

State observers and recursive filters in classical feedback control theory State observers an recursive filters in classical feeback control theory State-feeback control example: secon-orer system Consier the riven secon-orer system q q q u x q x q x x x x Here u coul represent

More information

Free rotation of a rigid body 1 D. E. Soper 2 University of Oregon Physics 611, Theoretical Mechanics 5 November 2012

Free rotation of a rigid body 1 D. E. Soper 2 University of Oregon Physics 611, Theoretical Mechanics 5 November 2012 Free rotation of a rigi boy 1 D. E. Soper 2 University of Oregon Physics 611, Theoretical Mechanics 5 November 2012 1 Introuction In this section, we escribe the motion of a rigi boy that is free to rotate

More information

Optimization based robust control

Optimization based robust control Optimization based robust control Didier Henrion 1,2 Draft of March 27, 2014 Prepared for possible inclusion into The Encyclopedia of Systems and Control edited by John Baillieul and Tariq Samad and published

More information

Time Headway Requirements for String Stability of Homogeneous Linear Unidirectionally Connected Systems

Time Headway Requirements for String Stability of Homogeneous Linear Unidirectionally Connected Systems Joint 48th IEEE Conference on Decision an Control an 8th Chinese Control Conference Shanghai, PR China, December 6-8, 009 WeBIn53 Time Heaway Requirements for String Stability of Homogeneous Linear Uniirectionally

More information

APPPHYS 217 Thursday 8 April 2010

APPPHYS 217 Thursday 8 April 2010 APPPHYS 7 Thursay 8 April A&M example 6: The ouble integrator Consier the motion of a point particle in D with the applie force as a control input This is simply Newton s equation F ma with F u : t q q

More information

This module is part of the. Memobust Handbook. on Methodology of Modern Business Statistics

This module is part of the. Memobust Handbook. on Methodology of Modern Business Statistics This moule is part of the Memobust Hanbook on Methoology of Moern Business Statistics 26 March 2014 Metho: Balance Sampling for Multi-Way Stratification Contents General section... 3 1. Summary... 3 2.

More information

The Exact Form and General Integrating Factors

The Exact Form and General Integrating Factors 7 The Exact Form an General Integrating Factors In the previous chapters, we ve seen how separable an linear ifferential equations can be solve using methos for converting them to forms that can be easily

More information

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson JUST THE MATHS UNIT NUMBER 10.2 DIFFERENTIATION 2 (Rates of change) by A.J.Hobson 10.2.1 Introuction 10.2.2 Average rates of change 10.2.3 Instantaneous rates of change 10.2.4 Derivatives 10.2.5 Exercises

More information

Nested Saturation with Guaranteed Real Poles 1

Nested Saturation with Guaranteed Real Poles 1 Neste Saturation with Guarantee Real Poles Eric N Johnson 2 an Suresh K Kannan 3 School of Aerospace Engineering Georgia Institute of Technology, Atlanta, GA 3332 Abstract The global stabilization of asymptotically

More information

Time-of-Arrival Estimation in Non-Line-Of-Sight Environments

Time-of-Arrival Estimation in Non-Line-Of-Sight Environments 2 Conference on Information Sciences an Systems, The Johns Hopkins University, March 2, 2 Time-of-Arrival Estimation in Non-Line-Of-Sight Environments Sinan Gezici, Hisashi Kobayashi an H. Vincent Poor

More information

Acute sets in Euclidean spaces

Acute sets in Euclidean spaces Acute sets in Eucliean spaces Viktor Harangi April, 011 Abstract A finite set H in R is calle an acute set if any angle etermine by three points of H is acute. We examine the maximal carinality α() of

More information

Systems & Control Letters

Systems & Control Letters Systems & ontrol Letters ( ) ontents lists available at ScienceDirect Systems & ontrol Letters journal homepage: www.elsevier.com/locate/sysconle A converse to the eterministic separation principle Jochen

More information

Examining Geometric Integration for Propagating Orbit Trajectories with Non-Conservative Forcing

Examining Geometric Integration for Propagating Orbit Trajectories with Non-Conservative Forcing Examining Geometric Integration for Propagating Orbit Trajectories with Non-Conservative Forcing Course Project for CDS 05 - Geometric Mechanics John M. Carson III California Institute of Technology June

More information

Problem Sheet 2: Eigenvalues and eigenvectors and their use in solving linear ODEs

Problem Sheet 2: Eigenvalues and eigenvectors and their use in solving linear ODEs Problem Sheet 2: Eigenvalues an eigenvectors an their use in solving linear ODEs If you fin any typos/errors in this problem sheet please email jk28@icacuk The material in this problem sheet is not examinable

More information

Calculus of Variations

Calculus of Variations 16.323 Lecture 5 Calculus of Variations Calculus of Variations Most books cover this material well, but Kirk Chapter 4 oes a particularly nice job. x(t) x* x*+ αδx (1) x*- αδx (1) αδx (1) αδx (1) t f t

More information

Agmon Kolmogorov Inequalities on l 2 (Z d )

Agmon Kolmogorov Inequalities on l 2 (Z d ) Journal of Mathematics Research; Vol. 6, No. ; 04 ISSN 96-9795 E-ISSN 96-9809 Publishe by Canaian Center of Science an Eucation Agmon Kolmogorov Inequalities on l (Z ) Arman Sahovic Mathematics Department,

More information

Closed and Open Loop Optimal Control of Buffer and Energy of a Wireless Device

Closed and Open Loop Optimal Control of Buffer and Energy of a Wireless Device Close an Open Loop Optimal Control of Buffer an Energy of a Wireless Device V. S. Borkar School of Technology an Computer Science TIFR, umbai, Inia. borkar@tifr.res.in A. A. Kherani B. J. Prabhu INRIA

More information

Robust Forward Algorithms via PAC-Bayes and Laplace Distributions. ω Q. Pr (y(ω x) < 0) = Pr A k

Robust Forward Algorithms via PAC-Bayes and Laplace Distributions. ω Q. Pr (y(ω x) < 0) = Pr A k A Proof of Lemma 2 B Proof of Lemma 3 Proof: Since the support of LL istributions is R, two such istributions are equivalent absolutely continuous with respect to each other an the ivergence is well-efine

More information

Exponential Tracking Control of Nonlinear Systems with Actuator Nonlinearity

Exponential Tracking Control of Nonlinear Systems with Actuator Nonlinearity Preprints of the 9th Worl Congress The International Feeration of Automatic Control Cape Town, South Africa. August -9, Exponential Tracking Control of Nonlinear Systems with Actuator Nonlinearity Zhengqiang

More information

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x) Y. D. Chong (2016) MH2801: Complex Methos for the Sciences 1. Derivatives The erivative of a function f(x) is another function, efine in terms of a limiting expression: f (x) f (x) lim x δx 0 f(x + δx)

More information

Chapter 2 Lagrangian Modeling

Chapter 2 Lagrangian Modeling Chapter 2 Lagrangian Moeling The basic laws of physics are use to moel every system whether it is electrical, mechanical, hyraulic, or any other energy omain. In mechanics, Newton s laws of motion provie

More information

Convergence of Random Walks

Convergence of Random Walks Chapter 16 Convergence of Ranom Walks This lecture examines the convergence of ranom walks to the Wiener process. This is very important both physically an statistically, an illustrates the utility of

More information

Table of Common Derivatives By David Abraham

Table of Common Derivatives By David Abraham Prouct an Quotient Rules: Table of Common Derivatives By Davi Abraham [ f ( g( ] = [ f ( ] g( + f ( [ g( ] f ( = g( [ f ( ] g( g( f ( [ g( ] Trigonometric Functions: sin( = cos( cos( = sin( tan( = sec

More information

Qubit channels that achieve capacity with two states

Qubit channels that achieve capacity with two states Qubit channels that achieve capacity with two states Dominic W. Berry Department of Physics, The University of Queenslan, Brisbane, Queenslan 4072, Australia Receive 22 December 2004; publishe 22 March

More information

UNIFYING PCA AND MULTISCALE APPROACHES TO FAULT DETECTION AND ISOLATION

UNIFYING PCA AND MULTISCALE APPROACHES TO FAULT DETECTION AND ISOLATION UNIFYING AND MULISCALE APPROACHES O FAUL DEECION AND ISOLAION Seongkyu Yoon an John F. MacGregor Dept. Chemical Engineering, McMaster University, Hamilton Ontario Canaa L8S 4L7 yoons@mcmaster.ca macgreg@mcmaster.ca

More information

Separation of Variables

Separation of Variables Physics 342 Lecture 1 Separation of Variables Lecture 1 Physics 342 Quantum Mechanics I Monay, January 25th, 2010 There are three basic mathematical tools we nee, an then we can begin working on the physical

More information

PDE Notes, Lecture #11

PDE Notes, Lecture #11 PDE Notes, Lecture # from Professor Jalal Shatah s Lectures Febuary 9th, 2009 Sobolev Spaces Recall that for u L loc we can efine the weak erivative Du by Du, φ := udφ φ C0 If v L loc such that Du, φ =

More information

CHAPTER 1 : DIFFERENTIABLE MANIFOLDS. 1.1 The definition of a differentiable manifold

CHAPTER 1 : DIFFERENTIABLE MANIFOLDS. 1.1 The definition of a differentiable manifold CHAPTER 1 : DIFFERENTIABLE MANIFOLDS 1.1 The efinition of a ifferentiable manifol Let M be a topological space. This means that we have a family Ω of open sets efine on M. These satisfy (1), M Ω (2) the

More information

Stability region estimation for systems with unmodeled dynamics

Stability region estimation for systems with unmodeled dynamics Stability region estimation for systems with unmoele ynamics Ufuk Topcu, Anrew Packar, Peter Seiler, an Gary Balas Abstract We propose a metho to compute invariant subsets of the robust region-of-attraction

More information

Experimental Robustness Study of a Second-Order Sliding Mode Controller

Experimental Robustness Study of a Second-Order Sliding Mode Controller Experimental Robustness Stuy of a Secon-Orer Sliing Moe Controller Anré Blom, Bram e Jager Einhoven University of Technology Department of Mechanical Engineering P.O. Box 513, 5600 MB Einhoven, The Netherlans

More information

On Characterizing the Delay-Performance of Wireless Scheduling Algorithms

On Characterizing the Delay-Performance of Wireless Scheduling Algorithms On Characterizing the Delay-Performance of Wireless Scheuling Algorithms Xiaojun Lin Center for Wireless Systems an Applications School of Electrical an Computer Engineering, Purue University West Lafayette,

More information

Lagrangian and Hamiltonian Mechanics

Lagrangian and Hamiltonian Mechanics Lagrangian an Hamiltonian Mechanics.G. Simpson, Ph.. epartment of Physical Sciences an Engineering Prince George s Community College ecember 5, 007 Introuction In this course we have been stuying classical

More information

Switching Time Optimization in Discretized Hybrid Dynamical Systems

Switching Time Optimization in Discretized Hybrid Dynamical Systems Switching Time Optimization in Discretize Hybri Dynamical Systems Kathrin Flaßkamp, To Murphey, an Sina Ober-Blöbaum Abstract Switching time optimization (STO) arises in systems that have a finite set

More information

Linear First-Order Equations

Linear First-Order Equations 5 Linear First-Orer Equations Linear first-orer ifferential equations make up another important class of ifferential equations that commonly arise in applications an are relatively easy to solve (in theory)

More information

Predictive Control of a Laboratory Time Delay Process Experiment

Predictive Control of a Laboratory Time Delay Process Experiment Print ISSN:3 6; Online ISSN: 367-5357 DOI:0478/itc-03-0005 Preictive Control of a aboratory ime Delay Process Experiment S Enev Key Wors: Moel preictive control; time elay process; experimental results

More information

We G Model Reduction Approaches for Solution of Wave Equations for Multiple Frequencies

We G Model Reduction Approaches for Solution of Wave Equations for Multiple Frequencies We G15 5 Moel Reuction Approaches for Solution of Wave Equations for Multiple Frequencies M.Y. Zaslavsky (Schlumberger-Doll Research Center), R.F. Remis* (Delft University) & V.L. Druskin (Schlumberger-Doll

More information

Survey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013

Survey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013 Survey Sampling Kosuke Imai Department of Politics, Princeton University February 19, 2013 Survey sampling is one of the most commonly use ata collection methos for social scientists. We begin by escribing

More information

TMA 4195 Matematisk modellering Exam Tuesday December 16, :00 13:00 Problems and solution with additional comments

TMA 4195 Matematisk modellering Exam Tuesday December 16, :00 13:00 Problems and solution with additional comments Problem F U L W D g m 3 2 s 2 0 0 0 0 2 kg 0 0 0 0 0 0 Table : Dimension matrix TMA 495 Matematisk moellering Exam Tuesay December 6, 2008 09:00 3:00 Problems an solution with aitional comments The necessary

More information

Logarithmic spurious regressions

Logarithmic spurious regressions Logarithmic spurious regressions Robert M. e Jong Michigan State University February 5, 22 Abstract Spurious regressions, i.e. regressions in which an integrate process is regresse on another integrate

More information

Accelerate Implementation of Forwaring Control Laws using Composition Methos Yves Moreau an Roolphe Sepulchre June 1997 Abstract We use a metho of int

Accelerate Implementation of Forwaring Control Laws using Composition Methos Yves Moreau an Roolphe Sepulchre June 1997 Abstract We use a metho of int Katholieke Universiteit Leuven Departement Elektrotechniek ESAT-SISTA/TR 1997-11 Accelerate Implementation of Forwaring Control Laws using Composition Methos 1 Yves Moreau, Roolphe Sepulchre, Joos Vanewalle

More information

Diophantine Approximations: Examining the Farey Process and its Method on Producing Best Approximations

Diophantine Approximations: Examining the Farey Process and its Method on Producing Best Approximations Diophantine Approximations: Examining the Farey Process an its Metho on Proucing Best Approximations Kelly Bowen Introuction When a person hears the phrase irrational number, one oes not think of anything

More information

Minimum-time constrained velocity planning

Minimum-time constrained velocity planning 7th Meiterranean Conference on Control & Automation Makeonia Palace, Thessaloniki, Greece June 4-6, 9 Minimum-time constraine velocity planning Gabriele Lini, Luca Consolini, Aurelio Piazzi Università

More information

TRAJECTORY TRACKING FOR FULLY ACTUATED MECHANICAL SYSTEMS

TRAJECTORY TRACKING FOR FULLY ACTUATED MECHANICAL SYSTEMS TRAJECTORY TRACKING FOR FULLY ACTUATED MECHANICAL SYSTEMS Francesco Bullo Richar M. Murray Control an Dynamical Systems California Institute of Technology Pasaena, CA 91125 Fax : + 1-818-796-8914 email

More information

Lecture 2 Lagrangian formulation of classical mechanics Mechanics

Lecture 2 Lagrangian formulation of classical mechanics Mechanics Lecture Lagrangian formulation of classical mechanics 70.00 Mechanics Principle of stationary action MATH-GA To specify a motion uniquely in classical mechanics, it suffices to give, at some time t 0,

More information

Total Energy Shaping of a Class of Underactuated Port-Hamiltonian Systems using a New Set of Closed-Loop Potential Shape Variables*

Total Energy Shaping of a Class of Underactuated Port-Hamiltonian Systems using a New Set of Closed-Loop Potential Shape Variables* 51st IEEE Conference on Decision an Control December 1-13 212. Maui Hawaii USA Total Energy Shaping of a Class of Uneractuate Port-Hamiltonian Systems using a New Set of Close-Loop Potential Shape Variables*

More information

Left-invariant extended Kalman filter and attitude estimation

Left-invariant extended Kalman filter and attitude estimation Left-invariant extene Kalman filter an attitue estimation Silvere Bonnabel Abstract We consier a left-invariant ynamics on a Lie group. One way to efine riving an observation noises is to make them preserve

More information

6 General properties of an autonomous system of two first order ODE

6 General properties of an autonomous system of two first order ODE 6 General properties of an autonomous system of two first orer ODE Here we embark on stuying the autonomous system of two first orer ifferential equations of the form ẋ 1 = f 1 (, x 2 ), ẋ 2 = f 2 (, x

More information

THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE

THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE Journal of Soun an Vibration (1996) 191(3), 397 414 THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE E. M. WEINSTEIN Galaxy Scientific Corporation, 2500 English Creek

More information

Advanced Partial Differential Equations with Applications

Advanced Partial Differential Equations with Applications MIT OpenCourseWare http://ocw.mit.eu 18.306 Avance Partial Differential Equations with Applications Fall 2009 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.eu/terms.

More information

Lower Bounds for the Smoothed Number of Pareto optimal Solutions

Lower Bounds for the Smoothed Number of Pareto optimal Solutions Lower Bouns for the Smoothe Number of Pareto optimal Solutions Tobias Brunsch an Heiko Röglin Department of Computer Science, University of Bonn, Germany brunsch@cs.uni-bonn.e, heiko@roeglin.org Abstract.

More information

On Decentralized Optimal Control and Information Structures

On Decentralized Optimal Control and Information Structures 2008 American Control Conference Westin Seattle Hotel, Seattle, Washington, USA June 11-13, 2008 FrC053 On Decentralize Optimal Control an Information Structures Naer Motee 1, Ali Jababaie 1 an Bassam

More information

Interpolated Rigid-Body Motions and Robotics

Interpolated Rigid-Body Motions and Robotics Interpolate Rigi-Boy Motions an Robotics J.M. Selig Faculty of Business, Computing an Info. Management. Lonon South Bank University, Lonon SE AA, U.K. seligjm@lsbu.ac.uk Yaunquing Wu Dept. Mechanical Engineering.

More information

Distributed coordination control for multi-robot networks using Lyapunov-like barrier functions

Distributed coordination control for multi-robot networks using Lyapunov-like barrier functions IEEE TRANSACTIONS ON 1 Distribute coorination control for multi-robot networks using Lyapunov-like barrier functions Dimitra Panagou, Dušan M. Stipanović an Petros G. Voulgaris Abstract This paper aresses

More information

TEMPORAL AND TIME-FREQUENCY CORRELATION-BASED BLIND SOURCE SEPARATION METHODS. Yannick DEVILLE

TEMPORAL AND TIME-FREQUENCY CORRELATION-BASED BLIND SOURCE SEPARATION METHODS. Yannick DEVILLE TEMPORAL AND TIME-FREQUENCY CORRELATION-BASED BLIND SOURCE SEPARATION METHODS Yannick DEVILLE Université Paul Sabatier Laboratoire Acoustique, Métrologie, Instrumentation Bât. 3RB2, 8 Route e Narbonne,

More information

Parameter estimation: A new approach to weighting a priori information

Parameter estimation: A new approach to weighting a priori information Parameter estimation: A new approach to weighting a priori information J.L. Mea Department of Mathematics, Boise State University, Boise, ID 83725-555 E-mail: jmea@boisestate.eu Abstract. We propose a

More information

Situation awareness of power system based on static voltage security region

Situation awareness of power system based on static voltage security region The 6th International Conference on Renewable Power Generation (RPG) 19 20 October 2017 Situation awareness of power system base on static voltage security region Fei Xiao, Zi-Qing Jiang, Qian Ai, Ran

More information

State-Space Model for a Multi-Machine System

State-Space Model for a Multi-Machine System State-Space Moel for a Multi-Machine System These notes parallel section.4 in the text. We are ealing with classically moele machines (IEEE Type.), constant impeance loas, an a network reuce to its internal

More information

Output Feedback Stabilization of Nonlinear Systems with Delayed Output

Output Feedback Stabilization of Nonlinear Systems with Delayed Output 5 American Control Conference June 8-1 5 Portlan OR USA FrC15 Output Feeback Stabilization of Nonlinear Systems with Delaye Output Xianfu Zhang Zhaolin Cheng an Xing-Ping Wang Abstract: It is propose a

More information

SYNCHRONOUS SEQUENTIAL CIRCUITS

SYNCHRONOUS SEQUENTIAL CIRCUITS CHAPTER SYNCHRONOUS SEUENTIAL CIRCUITS Registers an counters, two very common synchronous sequential circuits, are introuce in this chapter. Register is a igital circuit for storing information. Contents

More information

The Optimal Steady-State Control Problem

The Optimal Steady-State Control Problem SUBMITTED TO IEEE TRANSACTIONS ON AUTOMATIC CONTROL. THIS VERSION: OCTOBER 31, 218 1 The Optimal Steay-State Control Problem Liam S. P. Lawrence Stuent Member, IEEE, John W. Simpson-Porco, Member, IEEE,

More information

Interconnected Systems of Fliess Operators

Interconnected Systems of Fliess Operators Interconnecte Systems of Fliess Operators W. Steven Gray Yaqin Li Department of Electrical an Computer Engineering Ol Dominion University Norfolk, Virginia 23529 USA Abstract Given two analytic nonlinear

More information

Multi-agent Systems Reaching Optimal Consensus with Time-varying Communication Graphs

Multi-agent Systems Reaching Optimal Consensus with Time-varying Communication Graphs Preprints of the 8th IFAC Worl Congress Multi-agent Systems Reaching Optimal Consensus with Time-varying Communication Graphs Guoong Shi ACCESS Linnaeus Centre, School of Electrical Engineering, Royal

More information

Physics 5153 Classical Mechanics. The Virial Theorem and The Poisson Bracket-1

Physics 5153 Classical Mechanics. The Virial Theorem and The Poisson Bracket-1 Physics 5153 Classical Mechanics The Virial Theorem an The Poisson Bracket 1 Introuction In this lecture we will consier two applications of the Hamiltonian. The first, the Virial Theorem, applies to systems

More information

A PID-Sliding Mode Control Design for a Coupled Tank

A PID-Sliding Mode Control Design for a Coupled Tank International Conference CRATT 0, Raes, Tunisia 0 A PID-Sliing Moe Control Design for a Couple Tank Ahme RHIF, Zohra Karous, Naceur BenHaj Braiek Avance System Laboratory, Polytechnic School of Tunisia

More information

Optimization of Geometries by Energy Minimization

Optimization of Geometries by Energy Minimization Optimization of Geometries by Energy Minimization by Tracy P. Hamilton Department of Chemistry University of Alabama at Birmingham Birmingham, AL 3594-140 hamilton@uab.eu Copyright Tracy P. Hamilton, 1997.

More information

OPTIMAL CONTROL PROBLEM FOR PROCESSES REPRESENTED BY STOCHASTIC SEQUENTIAL MACHINE

OPTIMAL CONTROL PROBLEM FOR PROCESSES REPRESENTED BY STOCHASTIC SEQUENTIAL MACHINE OPTIMA CONTRO PROBEM FOR PROCESSES REPRESENTED BY STOCHASTIC SEQUENTIA MACHINE Yaup H. HACI an Muhammet CANDAN Department of Mathematics, Canaale Onseiz Mart University, Canaale, Turey ABSTRACT In this

More information

Optimized Schwarz Methods with the Yin-Yang Grid for Shallow Water Equations

Optimized Schwarz Methods with the Yin-Yang Grid for Shallow Water Equations Optimize Schwarz Methos with the Yin-Yang Gri for Shallow Water Equations Abessama Qaouri Recherche en prévision numérique, Atmospheric Science an Technology Directorate, Environment Canaa, Dorval, Québec,

More information

Capacity Analysis of MIMO Systems with Unknown Channel State Information

Capacity Analysis of MIMO Systems with Unknown Channel State Information Capacity Analysis of MIMO Systems with Unknown Channel State Information Jun Zheng an Bhaskar D. Rao Dept. of Electrical an Computer Engineering University of California at San Diego e-mail: juzheng@ucs.eu,

More information

F 1 x 1,,x n. F n x 1,,x n

F 1 x 1,,x n. F n x 1,,x n Chapter Four Dynamical Systems 4. Introuction The previous chapter has been evote to the analysis of systems of first orer linear ODE s. In this chapter we will consier systems of first orer ODE s that

More information

Maximizing the Closed Loop Asymptotic Decay Rate for the Two-Mass-Spring Control Problem

Maximizing the Closed Loop Asymptotic Decay Rate for the Two-Mass-Spring Control Problem Maximizing the Closed Loop Asymptotic Decay Rate for the Two-Mass-Spring Control Problem Didier Henrion 1,2 Michael L. Overton 3 May 12, 2006 Abstract We consider the following problem: find a fixed-order

More information

Dissipative numerical methods for the Hunter-Saxton equation

Dissipative numerical methods for the Hunter-Saxton equation Dissipative numerical methos for the Hunter-Saton equation Yan Xu an Chi-Wang Shu Abstract In this paper, we present further evelopment of the local iscontinuous Galerkin (LDG) metho esigne in [] an a

More information

Nonlinear Adaptive Ship Course Tracking Control Based on Backstepping and Nussbaum Gain

Nonlinear Adaptive Ship Course Tracking Control Based on Backstepping and Nussbaum Gain Nonlinear Aaptive Ship Course Tracking Control Base on Backstepping an Nussbaum Gain Jialu Du, Chen Guo Abstract A nonlinear aaptive controller combining aaptive Backstepping algorithm with Nussbaum gain

More information

arxiv:hep-th/ v1 3 Feb 1993

arxiv:hep-th/ v1 3 Feb 1993 NBI-HE-9-89 PAR LPTHE 9-49 FTUAM 9-44 November 99 Matrix moel calculations beyon the spherical limit arxiv:hep-th/93004v 3 Feb 993 J. Ambjørn The Niels Bohr Institute Blegamsvej 7, DK-00 Copenhagen Ø,

More information

NDI-BASED STRUCTURED LPV CONTROL A PROMISING APPROACH FOR AERIAL ROBOTICS

NDI-BASED STRUCTURED LPV CONTROL A PROMISING APPROACH FOR AERIAL ROBOTICS NDI-BASED STRUCTURED LPV CONTROL A PROMISING APPROACH FOR AERIAL ROBOTICS J-M. Biannic AERIAL ROBOTICS WORKSHOP OCTOBER 2014 CONTENT 1 Introduction 2 Proposed LPV design methodology 3 Applications to Aerospace

More information

Schrödinger s equation.

Schrödinger s equation. Physics 342 Lecture 5 Schröinger s Equation Lecture 5 Physics 342 Quantum Mechanics I Wenesay, February 3r, 2010 Toay we iscuss Schröinger s equation an show that it supports the basic interpretation of

More information

1 dx. where is a large constant, i.e., 1, (7.6) and Px is of the order of unity. Indeed, if px is given by (7.5), the inequality (7.

1 dx. where is a large constant, i.e., 1, (7.6) and Px is of the order of unity. Indeed, if px is given by (7.5), the inequality (7. Lectures Nine an Ten The WKB Approximation The WKB metho is a powerful tool to obtain solutions for many physical problems It is generally applicable to problems of wave propagation in which the frequency

More information

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012 CS-6 Theory Gems November 8, 0 Lecture Lecturer: Alesaner Mąry Scribes: Alhussein Fawzi, Dorina Thanou Introuction Toay, we will briefly iscuss an important technique in probability theory measure concentration

More information

Permanent vs. Determinant

Permanent vs. Determinant Permanent vs. Determinant Frank Ban Introuction A major problem in theoretical computer science is the Permanent vs. Determinant problem. It asks: given an n by n matrix of ineterminates A = (a i,j ) an

More information