Copyright 2012 IEEE. Personal use of this material is permitted. Permission from IEEE must be obtained for all other uses, in any current or future
|
|
- Sabrina Chandler
- 5 years ago
- Views:
Transcription
1 Copyrigt 212 IEEE. Personal use of tis material is permitted. Permission from IEEE must be obtained for all oter uses, in any current or future media, including reprinting/republising tis material for advertising or promotional purposes, creating new collective works, for resale or redistribution to servers or lists, or reuse of any copyrigted component of tis work in oter works.
2 1 Exponential Stability of Integral Delay Systems wit a Class of Analytic Kernels Sabine Mondié and Daniel Melcor-Aguilar Abstract Te exponential stability of a class of integral delay systems wit analytic kernels is investigated by using te Lyapunov-Krasovskii functional approac. Sufcient delaydependent stability conditions and exponential estimates for te solutions are derived. Special attention is paid to te particular cases of polynomial and exponential kernels. Index Terms Integral delay system, exponential stability, Lyapunov-Krasovskii functionals. I. INTRODUCTION Integral delay systems play an important role in several stability problems of time-delay systems. Tis class of systems is found as delay approximations of te partial differential equations for describing te propagation penomena in excitable media [18], in te stability analysis of additional dynamics introduced by some system transformations [3], [5], [6], [7], in te internal stability problem of controllers used for nite spectrum assignment of time-delay systems [9], as well as in te stability analysis of some difference operators in neutral type functional differential equations [4], [8]. Lyapunov-Krasovskii teorems for integral delay systems ave been recently introduced in [12]. It as been sown tere tat new type of Lyapunov-Krasovskii conditions are required in order to properly address te dynamics of tis class of systems. General expressions of quadratic functionals wit a given time derivative are provided. Te functionals are sown to be useful in solutions of suc problems as te estimations of robustness bounds and calculations of exponential estimates for te solutions of exponentially stable integral delay systems. However, tere are still some tecnical difculties, associated wit te positivity ceck of suc functionals, limiting teir practical application to te stability analysis of integral delay systems. Tis motivated te work [13] were it was sown tat, based on te general expressions of functionals presented in [12], various reduced type functionals can be constructed to obtain stability conditions formulated directly in terms of te coefcients of some classes of integral delay systems. In te present paper, we address te exponential stability of a special class of integral delay systems wit analytic kernels. For suc integral systems, we derive sufcient delaydependent stability conditions, expressed in terms of linear matrix inequalities, by using te Lyapunov-Krasovskii functional approac. Tis work was supported by CONACYT under Grants and S. Mondié is wit te Department of Automatic Control, CINVESTAV-IPN, A.P , 73, México, DF, México. smondie@ctrl.cinvestav.mx D. Melcor-Aguilar is wit te Division of Applied Matematics, IPICYT, 78216, San Luis Potosí, SLP, México. dmelcor@ipicyt.edu.mx Te special class of integral delay systems under consideration includes tose wit polynomial and exponential kernels, wic found important applications in te internal stability problem of controllers used for te nite spectrum assignment of input time-delay systems, a topic tat as received a sustained attention in te past few years, see for instance [2], [14], [15], [16], [21], [22], and tat was proposed as an interesting open problem in te survey paper [2]. We ere address suc a problem from a Lyapunov-Krasovskii framework and develop a linear matrix inequalities formulation for it. More explicitly, a design metod guaranteeing a numerically safe implementation of te controllers and a prescribed decay rate of te closed-loop system solutions is proposed. We believe tat suc an approac to te problem is completely new. Te paper is structured as follows In section II, preliminaries concerning te class of integral delay systems to be considered, basic facts about te solutions and Lyapunov-Krasovskii stability conditions are introduced. Te main results are given in section III. First, we consider integral delay systems wit a general class of analytic kernels. Ten, te special cases of integral delay systems wit polynomial and exponential kernels are addressed. In all cases, exponential estimates and delay-dependent conditions for te exponential stability are expressed in terms of linear matrix inequalities. In section IV, we apply te obtained results to te internal stability problem of controllers used for te nite spectrum assignment of timedelay systems. Several concluding remarks end te paper. Notation Trougout te paper we will use te Euclidean norm for vectors and te induced norm for matrices, bot denoted by kk. We denote by A T te transpose of A, I n and n stand for te identity and zero matrices of nn dimension, wile min (A) and max (A) denote te smallest and largest eigenvalues of a symmetric matrix A, respectively. II. PRELIMINARIES In tis contribution we focus on te exponential stability of te class of integral delay systems wit analytic kernels described by were and x(t) = G T B()x(t + )d; 8t ; (1) G T = G T G T 1 G T N B() T = B () T B 1 () T B N () T ;
3 2 wit G 2 R n(n+1)m and B() 2 R n(n+1)m a continuously differentiable matrix function dened for 2 [ ; ] wic satises te following assumptions Tere exists a matrix M 2 R n(n+1)n(n+1) suc tat _ B() = MB(); 8 2 [ ; ] (2) Tere exists > suc tat for all 2 [ ; ] < min B T ()B() (3) Remark 1 Classes of kernels tat satisfy te assumptions (2) and (3) include tose written in a polynomial basis as well as transcendental kernels suc as exponential ones. Remark 2 It is important to point out tat te special class of functional difference equations (1), wit analytic kernels satisfying (2) and (3), belongs to te class of retarded type delay system, see [12] for discussions and te section below concerning solutions and stability concept. For te case of functional difference equations of te neutral type, te approac developed in [12] cannot be directly applied and Lyapunov stability conditions as tose proposed in [19] are more appropriate. A. Solutions and stability concept In order to dene a particular solution of (1) an initial vector function '(); 2 [ ; ) sould be given. We assume tat ' belongs to te space of piecewise continuous bounded functions PC([ ; ); R m ), equipped wit te uniform norm k'k = sup 2[ ;) k'()k. Given any initial function ' 2 PC([ ; ); R m ); tere exists a unique solution x(t; ') of (1) wic is dened for all t 2 [ ; 1) wit x(t; ') = '(t); t 2 [ ; ) Tis solution is continuous and differentiable for all t 2 (; 1) ; and it suffers a jump discontinuity given by x(; ') = x(; ') x( ; ') = G T B()'()d '( ) Denition 3 [4] System (1) is said to be exponentially stable if tere exist > and > suc tat every solution of (1) satises te inequality kx(t; ')k k'k e t ; 8t Remark 4 Notice tat differentiation of te integral equation (1) is not an option for investigating its exponential stability since te resulting differential system wit distributed delay _x(t) = G T B()x(t) G T B( )x(t ) G T _ B()x(t + )d; is not exponentially stable as it admits any constant vector as a solution, see [12] for a detailed analysis. For any t we denote te restriction of te solution x(t; ') on te interval [t ; t) by x t (') = fx(t + ; '); 2 [ ; )g. Wen te initial function is irrelevant, we simply write x(t) and x t instead of x(t; ') and x t (') B. Lyapunov stability conditions Te observation in Remark 4 motivated te autors of te work [12] to derive new Lyapunov stability conditions for integral delay systems of te form in (1). In particular, it was tere sown tat integral type quadratic functions are te natural lower bounds for te Lyapunov functionals in contrast wit quadratic lower bounds of Lyapunov functionals for differential delay systems. We ere present a new formulation of te general result on Lyapunov type conditions for te exponential stability of integral delay systems given in [12]. Tis formulation, in te spirit of te one introduced in [17] for retarded differential delay systems, enances te role of te exponential decay rate. Following [12], by noting tat for t 2 [; ), x t (') belongs to PC([ ; ); R m ), and tat for t ; x t (') belongs to te space of continuous vector functions C([ ; ); R m ), it ten follows tat, in a Lyapunov-Krasovskii functional framework, te functionals sould be dened on te innite-dimensional space PC([ ; ); R m ) Teorem 5 [12] Let tere exists a functional v PC([ ; ); R m )! R suc tat 1 k'()k 2 d v (') 2 k'()k 2 d; (4) for some < 1 2 Given > ; if along solutions of (1) te inequality d dt v(x t (')) + 2v(x t (')) ; 8t ; (5) olds, ten were kx(t; ')k k'k e t ; 8t ; (6) = max 2[ ;] G T B() r 2 (7) 1 Based on tis fundamental result, te following sufcient stability condition is obtained in [13] by using a particular Lyapunov functional satisfying te Teorem conditions. Lemma 6 [13] System (1) is exponentially stable if max G T B() < 1 (8) 2[ ;] Tis inequality is valid for integral delay systems wit more general kernels tan tose satisfying te assumptions (2) and (3). Indeed, te only assumption needed on te matrix function B() is continuity on te interval [ ; ] However, inequality (8) may be very conservative for kernels satisfying te assumptions (2) and (3) as it as been illustrated in [13] for te case of constant kernels. It is wort mentioning tat (8) can also be obtained via frequency-domain tecniques, see [1] and [11]. III. MAIN RESULTS In tis section, sufcient delay-dependent conditions for te exponential stability of integral delay systems of te form of (1), wit kernels satisfying (2) and (3), are obtained by presenting a particular functional satisfying te conditions of Teorem 5.
4 3 Consider te functional candidate v(') = ' T ()B T ()e 2 [P + ( + ) Q] B()'()d; (9) were P; Q 2 R n(n+1)n(n+1) are positive denite matrices and is a positive constant. From (9) it follows tat v(') max (P + Q) and max (P + Q) v(') e 2 min (P ) e 2 min (P ) ' T ()B T ()B()'()d max (B T ()B()) k'()k 2 d; ' T ()B T ()B()'()d min (B T ()B()) k'()k 2 d; ence te functional (9) satises te following inequalities 1 k'()k 2 d v(') 2 k'()k 2 d; wit 1 = e 2 min (P ) min min(b T ()B()) ; (1) 2[ ;] 2 = max (P + Q) max max(b T ()B()) (11) 2[ ;] Te time derivative of functional (9) along te trajectories of system (1) is suc tat Z d T dt v(x t) + 2v(x t ) = G T B()x(t + )d B T () [P + Q] B() G T B()x(t + )d x T (t + )B T ()e 2 fq + [P + ( + ) Q] M) +M T [P + ( + ) Q] B()x(t + )d x T (t )e 2 B T ( )P B( )x(t ) By using te Jensen integral inequality we ave T G T B()x(t + )d B T () [P + Q] B() G T B()x(t + )d x T (t + )B() T GB T () [P + Q] B()G T B()x(t + ) d We terefore get te following inequality for te derivative d dt v(x t) + 2v(x t ) e 2 x T (t + )B T () ()B()x(t + )d; were () = Q + M T [P + ( + ) Q] + [P + ( + ) Q] M e 2 GB T () [P + Q] B()G T Tus, if () > ; 8 2 [ ; ] ; ten te exponential stability of (1) follows. Observing tat ( + ) ( ) + () = Q + M T [P + ( + ) Q] + [P + ( + ) Q] M ( + ) e2 + GB T () [P + Q] B()G T ; and taking into account te convexity of te exponential function ( + ) e2 + e 2 ; 8 2 [ ; ] ; one as tat () > ; 8 2 [ ; ] ; if and only if () > and ( ) > Summarizing te above, we can state te following result. Teorem 7 An integral delay system (1), wit a kernel satisfying (2) and (3), is exponentially stable wit a decay rate if tere exist positive denite matrices P; Q 2 R n(n+1)n(n+1) suc tat and Q + M T [P + Q] + [P + Q] M GB T () [P + Q] B()G T > ; (12) Q + M T P + P M e 2 GB T () [P + Q] B()G T > ; (13) Furtermore, for any initial condition ' 2 PC([ ; ); R m ); te solution x(t; ') of (1) satises te exponential upper bound (6), were ; 1 and 2 are determined by (7), (1) and (11), respectively. A. Integral delay systems wit polynomial and exponential kernels For n = m and matrix functions B() of te form B() T = I n I n I n N ; (14) we get te following result. Corollary 8 System (1) wit a matrix function B() of te form (14) is exponentially stable wit a decay rate if tere exists positive denite matrices P; Q 2 R n(n+1)n(n+1) suc tat (12) and (13) olds, were te matrix M is given by 2 3 n n n I n n n M =. n 2I.. n n n n NI n n Note tat in tis particular case of polynomial kernels te positive constants 1 and 2 ; respectively dened by (1) and (11), take te form 1 = e 2 min (P ); 2 = ( N ) max (P + Q)
5 4 TABLE I Maximum delay value for different decays Corollary Norm condition (8) 988 For m = n and kernels of te form G T B() = G T e A ; te following result is obtained. Corollary 9 System (1) wit a matrix function B() of te form (14) is exponentially stable if tere exist positive denite matrices P; Q 2 R nn suc tat (12) and (13) old wit M = A Remark 1 In te case of integral delay systems wit constant kernels G T B() = G T ; sufcient conditions for te exponential stability can be derived eiter from Corollary 8 (N = ) or Corollary 9 (A is te null matrix). In tis case, te conditions of Teorem 7 reduce to Q e 2 G [P + Q] G T > For =, tese conditions are te same as tose obtained in [13]. Now we illustrate te main results by some examples. Example 11 Consider te integral delay system were x(t) = A = e A x(t + )d; (15) For = ; by using Corollary 9, we found a feasible solution of te matrix inequalities (12)-(13) for delay values 199 For instance, for = 199 we obtain te following numerical values for matrices P and Q P =, Q = In Table I, we present te maximum delay value computed by using Corollary 9, for different Te results are less conservative tan te norm condition (8) wic, in te case of exponential kernels, provides always maximum delay values less tan one. Example 12 Consider now te system (15) wit A = 1 Because of te particular form of matrix A; te critical delay value can be computed analytically by using frequency-domain tecniques. Simple calculations based on te caracteristic function s + e s 2 1 f(s) = s sow tat (15) is exponentially stable for all delay values < 1 For tis particular matrix A; e A = I 2 + A; tis integral system can also be viewed as one aving a polynomial kernel G T B() wit G T = I 2 A and B() T = I 2 I 2 T TABLE II Maximum delay value for different decays Corollary Corollary Norm condition (8) 77 For different ; by applying Corollaries 8 and 9, we obtain te maximum delay value given in Table II. For = ; Corollaries 8 and 9 bot give max = 999 wic coincides wit te exact critical delay value and improves te maximum max = 77 obtained from te norm condition (8). We also see tat in tis case for > ; Corollary 8 provides less conservative results tan Corollary 9. In order to illustrate te computation of te -factor involved in te exponential upper bound (6), let us consider, in tis numerical example, tat = 1 and = 5 Direct calculations derived from (7), (1) and (11) yield = 87696; 1 = 129 and 2 = 24164; respectively. Ten, it follows tat every solution x(t; ') of (15), ' 2 PC([ 5; ); R 2 ); admits te exponential upper bound kx(t; ')k k'k 5 e t ; 8t IV. APPLICATION TO THE FINITE SPECTRUM ASSIGNMENT PROBLEM In tis section, we apply te obtained results in developing a design metod for tackling te numerical implementation problem of control laws wit distributed delay wic assign a nite spectrum to input delay systems. Tis problem concerns systems of te form _x(t) = Ax(t) + Bu(t ); (16) were A 2 R nn, B 2 R nm and > is te input delay. Te predictor like control law u(t) = K e A x(t) + e A Bu(t + )d (17) assigns a nite spectrum to te delay free closed-loop system (16)-(17) wic coincides wit te spectrum of te matrix A + BK, see [9]. Te practical value of suc a result is limited by te instability penomenon linked to te numerical implementation of te integral term in (17). It as been sown in [2], [15], [21] tat if te integral is approximated by a nite sum ten te resulting closed-loop delay system may become unstable if te ideal controller is not internally stable. A denite result as been demonstrated in [14] a necessary and sufcient condition for a numerically safe implementation (by using any type of numerical integration rule) of te controller (17) is bot te stability of te ideal closed-loop system (16)-(17), i.e., A+BK is Hurwitz, and te stability of te internal dynamics of te controller (17), i.e., te stability of te integral delay system z(t) = Ke A Bz(t + )d (18) Based on tis observation, by combining known results on matrix inequalities for guaranteeing tat all eigenvalues of te
6 5 matrix A + BK ave real parts less tan a certain prescribed [1] wit Teorem 7 applied to te integral delay system (18), wit G T = K; B() = e A B and M = A; we easily arrive at te following result. Proposition 13 Te input delay system (16), were witout loss of generality we can assume tat te matrix B is full column rank, admits a numerically safe implementation of te control law (17) wit a guaranteed decay rate for te closedloop system solutions, if tere exists a matrix K 2 R mn and positive denite matrices R; P; Q 2 R nn suc tat (A + BK + I) T R + R(A + BK + I) < ; (19) Q A T [P + Q] [P + Q] A K T B T [P + Q] BK > ; (2) Q A T P P A e 2 K T B T [P + Q] BK > (21) Te controller syntesis conditions of Proposition 13 involve nonlinear terms. Of course, condition (19) can be expressed as a linear matrix inequality pre- and post multiplying inequality (19) by te matrix S = R 1 and ten setting K = KS yields SA T + AS + K T B T + B K + 2S < ; (22) wic is linear in te variables S and K As a consequence, an easy way to solve te syntesis problem is rst to nd a feasible set (S; K) satisfying inequality (22). Ten set K = KS 1 and solve te linear matrix inequalities (2) and (21) for te variables P and Q However, wit additional computational effort, te syntesis conditions can be expressed as a set of linear matrix inequalities to be solved simultaneously and for wic better results can be obtained as presented next. First, by using te elimination procedure along wit Finsler's Lemma, te inequality (22) can be expressed as SA T + AS + 2S BB T < ; (23) for some scalar, see [1], and if tere exist positive denite matrix S and a scalar suc tat (23) olds, ten a feedback gain is given by K = 2 BT S 1 (24) Because of te omogeneity of (23) in S and, we can assume tat is positive and select = 2 Substituting (24) into inequalities (2) and (21) one obtains Q A T [P + Q] [P + Q] A S 1 BB T [P + Q] BB T S 1 > Q A T P P A e 2 S 1 BB T [P + Q] BB T S 1 > Ten, by introducing a new variable Y and a positive scalar suc tat Y > S 1 and (P + Q) 1 > I, respectively, te TABLE III Maximum delay value, feedback gain and ideal closed-loop eigenvalues. 5 1 max K ( 5; 267) ( 54; 14) ( 215; 29) ( 81 s 1; i 52 52i 14 13i 2 above two inequalities can be replaced by Q A T [P + Q] [P + Q] A Y BB T BB T Y I > ; (25) Q A T P P A Y BB T BB T Y e 2 > ; (26) I Y I > ; (27) I S (P + Q) < I; (28) were Scur complement as been applied to obtain te rst tree inequalities wile te last one directly follows by noting tat (P + Q) 1 > I is equivalent to (P + Q) < I Summarizing te above, if tere exist positive denite matrices P; Q; S; Y and a positive scalar suc tat te inequalities (23), (25)-(28) old, ten te feedback gain K = B T S 1 acieves a successful numerical implementation of te controller (17), wit guaranteed decay rate for te closed-loop system solutions. We use tis linear inequality formulation in te following illustrative examples. Example 14 Let us consider te input delay system (16) wit system matrices 1 A = and B = 1 Te corresponding linear system represents a double integrator wit delayed input, wic is commonly found in mecanical systems. Te maximum delay value max and te corresponding feedback gain K; computed by solving (23), (25)-(28) for different decays, and te ideal closed-loop eigenvalues s 1;2 are displayed in Table 3. We see tat for = ; a numerical safe implementation of te controller (17) can be acieved for any satisfying < 1 In tis particular case, in order to illustrate tat a feasible solution can be found for an arbitrarily large delay, te feedback gain K and te corresponding ideal closed-loop eigenvalues are computed for a delay value = 1 in Table III. Te example tat follows represents te linearization of a uid-ow model for describing te beavior of some classes of TCP/AQM networks, see [11] and te references terein for details. For suc a system, te application of te controller (17) as been recently proposed in [11]. It was sown tere tat for any given set of network parameters tere always exists a feedback gain suc tat a numerically safe implementation of te controller (17) can be acieved. Suc a result was proved by using te sufcient condition (8) wic, unlike te present approac, does not provide an estimate of te decay rate for te closed-loop system solutions.
7 6 TABLE IV Feedback gain and ideal closed-loop eigenvalues for different K (147; 1) (328; 3) (585; 9) s 1;2 6479; i i Example 15 Te linearized TCP/AQM network model of te form (16) as system matrices 2n A = 2 c c 2 n and B = 2n c 2 were n represents te number of TCP ows, c is te link capacity and denotes te round-trip time (delay). We ere apply te results of tis section in computing te feedback gain for guaranteeing a numerical implementation of te controller along wit a certain prescribed decay rate For network parameters n = 4; = 7 and c = 3, te inequalities (23), (25)-(28) are feasible for a maximum decay rate max = 848 Te computed feedback gain and te corresponding ideal closed-loop eigenvalues for different max are displayed in Table IV. V. CONCLUDING REMARKS In tis paper, delay-dependent sufcient conditions for te exponential stability of some classes of integral delay systems wit analytic kernels, wic found important applications in several stability problems of time-delay systems, are given. Te results are obtained by using te Lyapunov-Krasovskii functional approac recently developed in [12] and [13] for integral delay systems. An application to te nite spectrum assignment problem of input delay systems is also presented. As a result, a novel linear matrix inequality formulation for guaranteeing a numerically safe implementation of te controllers and a prescribed decay rate for te closed-loop system solutions is proposed. [8] V.B. Kolmanovskii, A. Myskis, Introduction to te Teory and Applications of Functional Differential Equations, Kluwer, te Neterlands, [9] A.Z. Manitus, A.W. Olbrot, Finite spectrum assignment problem for systems wit delays, IEEE Trans. Automat. Control, 24, [1] D. Melcor-Aguilar, B. Tristán-Tristán, On te implementation of control laws for nite spectrum assignment te multiple delays case, in Proc. of 4t IEEE Conf. Electr. Electron. Eng. México City, México, 27. [11] D. Melcor-Aguilar, On te stability of AQM controllers suppporting TCP Flows, Topics in Time-Delay Systems, Lect. Notes Control Inf. Sci., 388, , Springer-Verlag, Berlin, 29. [12] D. Melcor-Aguilar, V. Karitonov, R. Lozano, Stability conditions for integral delay systems, Int. J. Robust. Nonlinear Control, 2, 1-15, 21. [13] D. Melcor-Aguilar, On stability of integral delay systems, Appl. Mat. and Comput., 217, , 21. [14] W. Miciels, S. Mondié, D. Roose and M. Dambrine, Te effect of te approximating distributed delay control law on stability, in Advances of Time-Delay Systems, Lect. Notes Comput. Sci. Eng., 38, 27-22, Springer-Verlag, 24. [15] S. Mondié, M. Dambrine and O. Santos, Approximation of control law wit distributed delays A necessary condition for stability, Kybernetica, 38 (5), , 21. [16] S. Mondié and W. Miciels, Finite spectrum assignment of unstable time-delay systems wit a safe implementation, IEEE Trans. Automat. Control, 48 (12), , 23. [17] S. Mondié and V. Karitonov, Exponential Estimates for Retarded Time-Delay Systems An LMI Approac, IEEE Trans. Automat. Control, 5 (2), , 25. [18] S.-I. Niculescu, Delay Effects on Stability A Robust Control Approac, Lect. Notes Control Inf. Sci., 269, Springer-Verlag, Berlin, 21. [19] P. Pepe, Te Liapunov's second metod for continuous time difference equations, Int. J. Control, 13, , 23. [2] J.-P. Ricard, Time-delay systems an overview of some recent advances and open problems, Automatica, 39 (1), , 23. [21] V. Van Assce, M. Dambrine and J.-F. Lafay, Some problems arising in te implementation of distributed-delay control laws, in Proc. 38t IEEE Conf. Decision Control, Poenix, AZ, , [22] Q.-C. Zong, On distributed delay in linear control laws-part I discretedelay implementations, IEEE Trans. Automat. Control, 49 (11), , 24. VI. ACKNOWLEDGMENT Te autors wis to tank te anonymous Reviewers and Associate Editor P. Pepe for teir careful reading and valuable suggestions tat elped us to improve te work. REFERENCES [1] S. Boyd, L.E. Gaoui, E. Feron and V. Blakrisnan, Linear Matrix Inequalities in System and Control Teory, 15, SIAM, Piladelpia, [2] K. Engelborgs, M. Dambrine, and D. Roose, Limitations of a class of stabilization metods for delay systems, IEEE Trans. Automat. Control., 46 (2), , 21. [3] K. Gu, S.-I. Niculescu, Additional Dynamics in Transformed Time- Delay Systems, IEEE Trans. Autom. Control, 45, , 2. [4] J. Hale, S.M. Verduyn-Lunel, Introduction to Functional Differential Equations. Springer-Verlag, New York, [5] V. Karitonov, D. Melcor-Aguilar, On delay-dependent stability conditions, Syst. Control Lett., 4,71-76, 2. [6] V. Karitonov, D. Melcor-Aguilar, On delay-dependent stability conditions for time-varying systems, Syst. Control Lett., 46, [7] V. Karitonov, D. Melcor-Aguilar, Additional dynamics for general class of time-delay systems, IEEE Trans. Autom. Control, 48, , 23.
Finite Spectrum Assignment of Unstable Time-Delay Systems With a Safe Implementation
IEEE TRANSACTIONS ON AUTOMATIC CONTROL, VOL. 48, NO. 12, DECEMBER 23 227 Finite Spectrum Assignment of Unstable Time-Delay Systems Wit a Safe Implementation Sabine Mondié and Wim Miciels Abstract Te instability
More informationVolume 29, Issue 3. Existence of competitive equilibrium in economies with multi-member households
Volume 29, Issue 3 Existence of competitive equilibrium in economies wit multi-member ouseolds Noriisa Sato Graduate Scool of Economics, Waseda University Abstract Tis paper focuses on te existence of
More informationSampled-data implementation of derivative-dependent control using artificial delays
1 Sampled-data implementation of derivative-dependent control using artificial delays Anton Selivanov and Emilia Fridman, Senior Member, IEEE arxiv:1801.05696v1 [mat.oc] 17 Jan 2018 Abstract We study a
More informationOSCILLATION OF SOLUTIONS TO NON-LINEAR DIFFERENCE EQUATIONS WITH SEVERAL ADVANCED ARGUMENTS. Sandra Pinelas and Julio G. Dix
Opuscula Mat. 37, no. 6 (2017), 887 898 ttp://dx.doi.org/10.7494/opmat.2017.37.6.887 Opuscula Matematica OSCILLATION OF SOLUTIONS TO NON-LINEAR DIFFERENCE EQUATIONS WITH SEVERAL ADVANCED ARGUMENTS Sandra
More informationGlobal Output Feedback Stabilization of a Class of Upper-Triangular Nonlinear Systems
9 American Control Conference Hyatt Regency Riverfront St Louis MO USA June - 9 FrA4 Global Output Feedbac Stabilization of a Class of Upper-Triangular Nonlinear Systems Cunjiang Qian Abstract Tis paper
More informationInfluence of the Stepsize on Hyers Ulam Stability of First-Order Homogeneous Linear Difference Equations
International Journal of Difference Equations ISSN 0973-6069, Volume 12, Number 2, pp. 281 302 (2017) ttp://campus.mst.edu/ijde Influence of te Stepsize on Hyers Ulam Stability of First-Order Homogeneous
More information232 Calculus and Structures
3 Calculus and Structures CHAPTER 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS FOR EVALUATING BEAMS Calculus and Structures 33 Copyrigt Capter 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS 17.1 THE
More informationch (for some fixed positive number c) reaching c
GSTF Journal of Matematics Statistics and Operations Researc (JMSOR) Vol. No. September 05 DOI 0.60/s4086-05-000-z Nonlinear Piecewise-defined Difference Equations wit Reciprocal and Cubic Terms Ramadan
More informationTHE STURM-LIOUVILLE-TRANSFORMATION FOR THE SOLUTION OF VECTOR PARTIAL DIFFERENTIAL EQUATIONS. L. Trautmann, R. Rabenstein
Worksop on Transforms and Filter Banks (WTFB),Brandenburg, Germany, Marc 999 THE STURM-LIOUVILLE-TRANSFORMATION FOR THE SOLUTION OF VECTOR PARTIAL DIFFERENTIAL EQUATIONS L. Trautmann, R. Rabenstein Lerstul
More information4. The slope of the line 2x 7y = 8 is (a) 2/7 (b) 7/2 (c) 2 (d) 2/7 (e) None of these.
Mat 11. Test Form N Fall 016 Name. Instructions. Te first eleven problems are wort points eac. Te last six problems are wort 5 points eac. For te last six problems, you must use relevant metods of algebra
More informationA = h w (1) Error Analysis Physics 141
Introduction In all brances of pysical science and engineering one deals constantly wit numbers wic results more or less directly from experimental observations. Experimental observations always ave inaccuracies.
More informationNumerical Experiments Using MATLAB: Superconvergence of Nonconforming Finite Element Approximation for Second-Order Elliptic Problems
Applied Matematics, 06, 7, 74-8 ttp://wwwscirporg/journal/am ISSN Online: 5-7393 ISSN Print: 5-7385 Numerical Experiments Using MATLAB: Superconvergence of Nonconforming Finite Element Approximation for
More information1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point
MA00 Capter 6 Calculus and Basic Linear Algebra I Limits, Continuity and Differentiability Te concept of its (p.7 p.9, p.4 p.49, p.55 p.56). Limits Consider te function determined by te formula f Note
More informationA SHORT INTRODUCTION TO BANACH LATTICES AND
CHAPTER A SHORT INTRODUCTION TO BANACH LATTICES AND POSITIVE OPERATORS In tis capter we give a brief introduction to Banac lattices and positive operators. Most results of tis capter can be found, e.g.,
More informationROBUST REDUNDANCY RELATIONS FOR FAULT DIAGNOSIS IN NONLINEAR DESCRIPTOR SYSTEMS
Proceedings of te IASTED International Conference Modelling Identification and Control (AsiaMIC 23) April - 2 23 Puket Tailand ROBUST REDUNDANCY RELATIONS FOR FAULT DIAGNOSIS IN NONLINEAR DESCRIPTOR SYSTEMS
More information1 Calculus. 1.1 Gradients and the Derivative. Q f(x+h) f(x)
Calculus. Gradients and te Derivative Q f(x+) δy P T δx R f(x) 0 x x+ Let P (x, f(x)) and Q(x+, f(x+)) denote two points on te curve of te function y = f(x) and let R denote te point of intersection of
More informationContinuity and Differentiability of the Trigonometric Functions
[Te basis for te following work will be te definition of te trigonometric functions as ratios of te sides of a triangle inscribed in a circle; in particular, te sine of an angle will be defined to be te
More informationParameter Fitted Scheme for Singularly Perturbed Delay Differential Equations
International Journal of Applied Science and Engineering 2013. 11, 4: 361-373 Parameter Fitted Sceme for Singularly Perturbed Delay Differential Equations Awoke Andargiea* and Y. N. Reddyb a b Department
More informationMATH1151 Calculus Test S1 v2a
MATH5 Calculus Test 8 S va January 8, 5 Tese solutions were written and typed up by Brendan Trin Please be etical wit tis resource It is for te use of MatSOC members, so do not repost it on oter forums
More informationDifferentiation in higher dimensions
Capter 2 Differentiation in iger dimensions 2.1 Te Total Derivative Recall tat if f : R R is a 1-variable function, and a R, we say tat f is differentiable at x = a if and only if te ratio f(a+) f(a) tends
More informationMore on generalized inverses of partitioned matrices with Banachiewicz-Schur forms
More on generalized inverses of partitioned matrices wit anaciewicz-scur forms Yongge Tian a,, Yosio Takane b a Cina Economics and Management cademy, Central University of Finance and Economics, eijing,
More informationPre-Calculus Review Preemptive Strike
Pre-Calculus Review Preemptive Strike Attaced are some notes and one assignment wit tree parts. Tese are due on te day tat we start te pre-calculus review. I strongly suggest reading troug te notes torougly
More informationMAT244 - Ordinary Di erential Equations - Summer 2016 Assignment 2 Due: July 20, 2016
MAT244 - Ordinary Di erential Equations - Summer 206 Assignment 2 Due: July 20, 206 Full Name: Student #: Last First Indicate wic Tutorial Section you attend by filling in te appropriate circle: Tut 0
More informationConverse Lyapunov-Krasovskii Theorems for Systems Described by Neutral Functional Differential Equation in Hale s Form
Converse Lyapunov-Krasovskii Theorems for Systems Described by Neutral Functional Differential Equation in Hale s Form arxiv:1206.3504v1 [math.ds] 15 Jun 2012 P. Pepe I. Karafyllis Abstract In this paper
More informationNumerical Differentiation
Numerical Differentiation Finite Difference Formulas for te first derivative (Using Taylor Expansion tecnique) (section 8.3.) Suppose tat f() = g() is a function of te variable, and tat as 0 te function
More informationOrder of Accuracy. ũ h u Ch p, (1)
Order of Accuracy 1 Terminology We consider a numerical approximation of an exact value u. Te approximation depends on a small parameter, wic can be for instance te grid size or time step in a numerical
More informationMAT Calculus for Engineers I EXAM #1
MAT 65 - Calculus for Engineers I EXAM # Instructor: Liu, Hao Honor Statement By signing below you conrm tat you ave neiter given nor received any unautorized assistance on tis eam. Tis includes any use
More informationNumerical Solution of One Dimensional Nonlinear Longitudinal Oscillations in a Class of Generalized Functions
Proc. of te 8t WSEAS Int. Conf. on Matematical Metods and Computational Tecniques in Electrical Engineering, Bucarest, October 16-17, 2006 219 Numerical Solution of One Dimensional Nonlinear Longitudinal
More informationStability and Stabilizability of Linear Parameter Dependent System with Time Delay
Proceedings of te International MultiConference of Engineers and Computer Scientists 2008 Vol II IMECS 2008, 19-21 Marc, 2008, Hong Kong Stability and Stabilizability of Linear Parameter Dependent System
More informationOn convexity of polynomial paths and generalized majorizations
On convexity of polynomial pats and generalized majorizations Marija Dodig Centro de Estruturas Lineares e Combinatórias, CELC, Universidade de Lisboa, Av. Prof. Gama Pinto 2, 1649-003 Lisboa, Portugal
More informationPreconditioning in H(div) and Applications
1 Preconditioning in H(div) and Applications Douglas N. Arnold 1, Ricard S. Falk 2 and Ragnar Winter 3 4 Abstract. Summarizing te work of [AFW97], we sow ow to construct preconditioners using domain decomposition
More informationDelay-Dependent Exponential Stability of Linear Systems with Fast Time-Varying Delay
International Mathematical Forum, 4, 2009, no. 39, 1939-1947 Delay-Dependent Exponential Stability of Linear Systems with Fast Time-Varying Delay Le Van Hien Department of Mathematics Hanoi National University
More informationPoisson Equation in Sobolev Spaces
Poisson Equation in Sobolev Spaces OcMountain Dayligt Time. 6, 011 Today we discuss te Poisson equation in Sobolev spaces. It s existence, uniqueness, and regularity. Weak Solution. u = f in, u = g on
More informationNew Lyapunov Krasovskii functionals for stability of linear retarded and neutral type systems
Systems & Control Letters 43 (21 39 319 www.elsevier.com/locate/sysconle New Lyapunov Krasovskii functionals for stability of linear retarded and neutral type systems E. Fridman Department of Electrical
More informationComplete Quadratic Lyapunov functionals using Bessel-Legendre inequality
Complete Quadratic Lyapunov functionals using Bessel-Legendre inequality Alexandre Seuret Frédéric Gouaisbaut To cite tis version: Alexandre Seuret Frédéric Gouaisbaut Complete Quadratic Lyapunov functionals
More informationSome Review Problems for First Midterm Mathematics 1300, Calculus 1
Some Review Problems for First Midterm Matematics 00, Calculus. Consider te trigonometric function f(t) wose grap is sown below. Write down a possible formula for f(t). Tis function appears to be an odd,
More informationChapter 2. Limits and Continuity 16( ) 16( 9) = = 001. Section 2.1 Rates of Change and Limits (pp ) Quick Review 2.1
Capter Limits and Continuity Section. Rates of Cange and Limits (pp. 969) Quick Review..... f ( ) ( ) ( ) 0 ( ) f ( ) f ( ) sin π sin π 0 f ( ). < < < 6. < c c < < c 7. < < < < < 8. 9. 0. c < d d < c
More informationMath 1210 Midterm 1 January 31st, 2014
Mat 110 Midterm 1 January 1st, 01 Tis exam consists of sections, A and B. Section A is conceptual, wereas section B is more computational. Te value of every question is indicated at te beginning of it.
More informationMath 31A Discussion Notes Week 4 October 20 and October 22, 2015
Mat 3A Discussion Notes Week 4 October 20 and October 22, 205 To prepare for te first midterm, we ll spend tis week working eamples resembling te various problems you ve seen so far tis term. In tese notes
More informationERROR BOUNDS FOR THE METHODS OF GLIMM, GODUNOV AND LEVEQUE BRADLEY J. LUCIER*
EO BOUNDS FO THE METHODS OF GLIMM, GODUNOV AND LEVEQUE BADLEY J. LUCIE* Abstract. Te expected error in L ) attimet for Glimm s sceme wen applied to a scalar conservation law is bounded by + 2 ) ) /2 T
More informationAMS 147 Computational Methods and Applications Lecture 09 Copyright by Hongyun Wang, UCSC. Exact value. Effect of round-off error.
Lecture 09 Copyrigt by Hongyun Wang, UCSC Recap: Te total error in numerical differentiation fl( f ( x + fl( f ( x E T ( = f ( x Numerical result from a computer Exact value = e + f x+ Discretization error
More informationDepartment of Statistics & Operations Research, Aligarh Muslim University, Aligarh, India
Open Journal of Optimization, 04, 3, 68-78 Publised Online December 04 in SciRes. ttp://www.scirp.org/ournal/oop ttp://dx.doi.org/0.436/oop.04.34007 Compromise Allocation for Combined Ratio Estimates of
More informationUniversity Mathematics 2
University Matematics 2 1 Differentiability In tis section, we discuss te differentiability of functions. Definition 1.1 Differentiable function). Let f) be a function. We say tat f is differentiable at
More informationConvex Optimization Approach to Dynamic Output Feedback Control for Delay Differential Systems of Neutral Type 1,2
journal of optimization theory and applications: Vol. 127 No. 2 pp. 411 423 November 2005 ( 2005) DOI: 10.1007/s10957-005-6552-7 Convex Optimization Approach to Dynamic Output Feedback Control for Delay
More informationGeneric maximum nullity of a graph
Generic maximum nullity of a grap Leslie Hogben Bryan Sader Marc 5, 2008 Abstract For a grap G of order n, te maximum nullity of G is defined to be te largest possible nullity over all real symmetric n
More information1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t).
. Consider te trigonometric function f(t) wose grap is sown below. Write down a possible formula for f(t). Tis function appears to be an odd, periodic function tat as been sifted upwards, so we will use
More informationDecay of solutions of wave equations with memory
Proceedings of te 14t International Conference on Computational and Matematical Metods in Science and Engineering, CMMSE 14 3 7July, 14. Decay of solutions of wave equations wit memory J. A. Ferreira 1,
More informationLIMITS AND DERIVATIVES CONDITIONS FOR THE EXISTENCE OF A LIMIT
LIMITS AND DERIVATIVES Te limit of a function is defined as te value of y tat te curve approaces, as x approaces a particular value. Te limit of f (x) as x approaces a is written as f (x) approaces, as
More information158 Calculus and Structures
58 Calculus and Structures CHAPTER PROPERTIES OF DERIVATIVES AND DIFFERENTIATION BY THE EASY WAY. Calculus and Structures 59 Copyrigt Capter PROPERTIES OF DERIVATIVES. INTRODUCTION In te last capter you
More informationBrazilian Journal of Physics, vol. 29, no. 1, March, Ensemble and their Parameter Dierentiation. A. K. Rajagopal. Naval Research Laboratory,
Brazilian Journal of Pysics, vol. 29, no. 1, Marc, 1999 61 Fractional Powers of Operators of sallis Ensemble and teir Parameter Dierentiation A. K. Rajagopal Naval Researc Laboratory, Wasington D. C. 2375-532,
More informationInf sup testing of upwind methods
INTERNATIONAL JOURNAL FOR NUMERICAL METHODS IN ENGINEERING Int. J. Numer. Met. Engng 000; 48:745 760 Inf sup testing of upwind metods Klaus-Jurgen Bate 1; ;, Dena Hendriana 1, Franco Brezzi and Giancarlo
More informationNumerical Analysis MTH603. dy dt = = (0) , y n+1. We obtain yn. Therefore. and. Copyright Virtual University of Pakistan 1
Numerical Analysis MTH60 PREDICTOR CORRECTOR METHOD Te metods presented so far are called single-step metods, were we ave seen tat te computation of y at t n+ tat is y n+ requires te knowledge of y n only.
More informationNUMERICAL DIFFERENTIATION. James T. Smith San Francisco State University. In calculus classes, you compute derivatives algebraically: for example,
NUMERICAL DIFFERENTIATION James T Smit San Francisco State University In calculus classes, you compute derivatives algebraically: for example, f( x) = x + x f ( x) = x x Tis tecnique requires your knowing
More informationReflection Symmetries of q-bernoulli Polynomials
Journal of Nonlinear Matematical Pysics Volume 1, Supplement 1 005, 41 4 Birtday Issue Reflection Symmetries of q-bernoulli Polynomials Boris A KUPERSHMIDT Te University of Tennessee Space Institute Tullaoma,
More informationZuerst erschienen in: IEEE Trans. on Autom. Control 44 (1999), S DOI: /
Ilcmann, Acim ; Townley, Stuart: Adaptive Sampling Control of Hig-Gain Stabilizable Systems Zuerst erscienen in: IEEE Trans. on Autom. Control 44 (999), S.96-966 DOI:.9/9.793786 IEEE TRASACTIOS O AUTOMATIC
More informationSECTION 1.10: DIFFERENCE QUOTIENTS LEARNING OBJECTIVES
(Section.0: Difference Quotients).0. SECTION.0: DIFFERENCE QUOTIENTS LEARNING OBJECTIVES Define average rate of cange (and average velocity) algebraically and grapically. Be able to identify, construct,
More informationThe derivative function
Roberto s Notes on Differential Calculus Capter : Definition of derivative Section Te derivative function Wat you need to know already: f is at a point on its grap and ow to compute it. Wat te derivative
More informationSECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY
(Section 3.2: Derivative Functions and Differentiability) 3.2.1 SECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY LEARNING OBJECTIVES Know, understand, and apply te Limit Definition of te Derivative
More informationEects of small delays on stability of singularly perturbed systems
Automatica 38 (2002) 897 902 www.elsevier.com/locate/automatica Technical Communique Eects of small delays on stability of singularly perturbed systems Emilia Fridman Department of Electrical Engineering
More informationResearch Article Error Analysis for a Noisy Lacunary Cubic Spline Interpolation and a Simple Noisy Cubic Spline Quasi Interpolation
Advances in Numerical Analysis Volume 204, Article ID 35394, 8 pages ttp://dx.doi.org/0.55/204/35394 Researc Article Error Analysis for a Noisy Lacunary Cubic Spline Interpolation and a Simple Noisy Cubic
More informationLyapunov characterization of input-to-state stability for semilinear control systems over Banach spaces
Lyapunov caracterization of input-to-state stability for semilinear control systems over Banac spaces Andrii Mironcenko a, Fabian Wirt a a Faculty of Computer Science and Matematics, University of Passau,
More informationSubdifferentials of convex functions
Subdifferentials of convex functions Jordan Bell jordan.bell@gmail.com Department of Matematics, University of Toronto April 21, 2014 Wenever we speak about a vector space in tis note we mean a vector
More informationRecall from our discussion of continuity in lecture a function is continuous at a point x = a if and only if
Computational Aspects of its. Keeping te simple simple. Recall by elementary functions we mean :Polynomials (including linear and quadratic equations) Eponentials Logaritms Trig Functions Rational Functions
More informationJournal of Computational and Applied Mathematics
Journal of Computational and Applied Matematics 94 (6) 75 96 Contents lists available at ScienceDirect Journal of Computational and Applied Matematics journal omepage: www.elsevier.com/locate/cam Smootness-Increasing
More informationMaterial for Difference Quotient
Material for Difference Quotient Prepared by Stepanie Quintal, graduate student and Marvin Stick, professor Dept. of Matematical Sciences, UMass Lowell Summer 05 Preface Te following difference quotient
More informationLEAST-SQUARES FINITE ELEMENT APPROXIMATIONS TO SOLUTIONS OF INTERFACE PROBLEMS
SIAM J. NUMER. ANAL. c 998 Society for Industrial Applied Matematics Vol. 35, No., pp. 393 405, February 998 00 LEAST-SQUARES FINITE ELEMENT APPROXIMATIONS TO SOLUTIONS OF INTERFACE PROBLEMS YANZHAO CAO
More informationCombining functions: algebraic methods
Combining functions: algebraic metods Functions can be added, subtracted, multiplied, divided, and raised to a power, just like numbers or algebra expressions. If f(x) = x 2 and g(x) = x + 2, clearly f(x)
More informationEfficient algorithms for for clone items detection
Efficient algoritms for for clone items detection Raoul Medina, Caroline Noyer, and Olivier Raynaud Raoul Medina, Caroline Noyer and Olivier Raynaud LIMOS - Université Blaise Pascal, Campus universitaire
More informationChapter 2 Limits and Continuity
4 Section. Capter Limits and Continuity Section. Rates of Cange and Limits (pp. 6) Quick Review.. f () ( ) () 4 0. f () 4( ) 4. f () sin sin 0 4. f (). 4 4 4 6. c c c 7. 8. c d d c d d c d c 9. 8 ( )(
More informationHow to Find the Derivative of a Function: Calculus 1
Introduction How to Find te Derivative of a Function: Calculus 1 Calculus is not an easy matematics course Te fact tat you ave enrolled in suc a difficult subject indicates tat you are interested in te
More informationMATH1131/1141 Calculus Test S1 v8a
MATH/ Calculus Test 8 S v8a October, 7 Tese solutions were written by Joann Blanco, typed by Brendan Trin and edited by Mattew Yan and Henderson Ko Please be etical wit tis resource It is for te use of
More informationNumerical analysis of a free piston problem
MATHEMATICAL COMMUNICATIONS 573 Mat. Commun., Vol. 15, No. 2, pp. 573-585 (2010) Numerical analysis of a free piston problem Boris Mua 1 and Zvonimir Tutek 1, 1 Department of Matematics, University of
More information1. Introduction. We consider the model problem: seeking an unknown function u satisfying
A DISCONTINUOUS LEAST-SQUARES FINITE ELEMENT METHOD FOR SECOND ORDER ELLIPTIC EQUATIONS XIU YE AND SHANGYOU ZHANG Abstract In tis paper, a discontinuous least-squares (DLS) finite element metod is introduced
More informationMVT and Rolle s Theorem
AP Calculus CHAPTER 4 WORKSHEET APPLICATIONS OF DIFFERENTIATION MVT and Rolle s Teorem Name Seat # Date UNLESS INDICATED, DO NOT USE YOUR CALCULATOR FOR ANY OF THESE QUESTIONS In problems 1 and, state
More information7 Semiparametric Methods and Partially Linear Regression
7 Semiparametric Metods and Partially Linear Regression 7. Overview A model is called semiparametric if it is described by and were is nite-dimensional (e.g. parametric) and is in nite-dimensional (nonparametric).
More informationTaylor Series and the Mean Value Theorem of Derivatives
1 - Taylor Series and te Mean Value Teorem o Derivatives Te numerical solution o engineering and scientiic problems described by matematical models oten requires solving dierential equations. Dierential
More informationLecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator.
Lecture XVII Abstract We introduce te concept of directional derivative of a scalar function and discuss its relation wit te gradient operator. Directional derivative and gradient Te directional derivative
More informationPolynomial Interpolation
Capter 4 Polynomial Interpolation In tis capter, we consider te important problem of approximatinga function fx, wose values at a set of distinct points x, x, x,, x n are known, by a polynomial P x suc
More information(a) At what number x = a does f have a removable discontinuity? What value f(a) should be assigned to f at x = a in order to make f continuous at a?
Solutions to Test 1 Fall 016 1pt 1. Te grap of a function f(x) is sown at rigt below. Part I. State te value of eac limit. If a limit is infinite, state weter it is or. If a limit does not exist (but is
More informationETNA Kent State University
Electronic Transactions on Numerical Analysis. Volume 34, pp. 14-19, 2008. Copyrigt 2008,. ISSN 1068-9613. ETNA A NOTE ON NUMERICALLY CONSISTENT INITIAL VALUES FOR HIGH INDEX DIFFERENTIAL-ALGEBRAIC EQUATIONS
More informationON THE GLOBAL STABILITY OF AN SIRS EPIDEMIC MODEL WITH DISTRIBUTED DELAYS. Yukihiko Nakata. Yoichi Enatsu. Yoshiaki Muroya
Manuscript submitted to AIMS Journals Volume X, Number X, XX 2X Website: ttp://aimsciences.org pp. X XX ON THE GLOBAL STABILITY OF AN SIRS EPIDEMIC MODEL WITH DISTRIBUTED DELAYS Yukiiko Nakata Basque Center
More informationPOLYNOMIAL AND SPLINE ESTIMATORS OF THE DISTRIBUTION FUNCTION WITH PRESCRIBED ACCURACY
APPLICATIONES MATHEMATICAE 36, (29), pp. 2 Zbigniew Ciesielski (Sopot) Ryszard Zieliński (Warszawa) POLYNOMIAL AND SPLINE ESTIMATORS OF THE DISTRIBUTION FUNCTION WITH PRESCRIBED ACCURACY Abstract. Dvoretzky
More informationDIFFERENTIAL POLYNOMIALS GENERATED BY SECOND ORDER LINEAR DIFFERENTIAL EQUATIONS
Journal o Applied Analysis Vol. 14, No. 2 2008, pp. 259 271 DIFFERENTIAL POLYNOMIALS GENERATED BY SECOND ORDER LINEAR DIFFERENTIAL EQUATIONS B. BELAÏDI and A. EL FARISSI Received December 5, 2007 and,
More informationQuantum Numbers and Rules
OpenStax-CNX module: m42614 1 Quantum Numbers and Rules OpenStax College Tis work is produced by OpenStax-CNX and licensed under te Creative Commons Attribution License 3.0 Abstract Dene quantum number.
More informationCharacterization of reducible hexagons and fast decomposition of elementary benzenoid graphs
Discrete Applied Matematics 156 (2008) 1711 1724 www.elsevier.com/locate/dam Caracterization of reducible exagons and fast decomposition of elementary benzenoid graps Andrej Taranenko, Aleksander Vesel
More informationContinuity. Example 1
Continuity MATH 1003 Calculus and Linear Algebra (Lecture 13.5) Maoseng Xiong Department of Matematics, HKUST A function f : (a, b) R is continuous at a point c (a, b) if 1. x c f (x) exists, 2. f (c)
More informationLogarithmic functions
Roberto s Notes on Differential Calculus Capter 5: Derivatives of transcendental functions Section Derivatives of Logaritmic functions Wat ou need to know alread: Definition of derivative and all basic
More informationChapter 5 FINITE DIFFERENCE METHOD (FDM)
MEE7 Computer Modeling Tecniques in Engineering Capter 5 FINITE DIFFERENCE METHOD (FDM) 5. Introduction to FDM Te finite difference tecniques are based upon approximations wic permit replacing differential
More informationMANY scientific and engineering problems can be
A Domain Decomposition Metod using Elliptical Arc Artificial Boundary for Exterior Problems Yajun Cen, and Qikui Du Abstract In tis paper, a Diriclet-Neumann alternating metod using elliptical arc artificial
More informationThe Verlet Algorithm for Molecular Dynamics Simulations
Cemistry 380.37 Fall 2015 Dr. Jean M. Standard November 9, 2015 Te Verlet Algoritm for Molecular Dynamics Simulations Equations of motion For a many-body system consisting of N particles, Newton's classical
More informationCopyright c 2008 Kevin Long
Lecture 4 Numerical solution of initial value problems Te metods you ve learned so far ave obtained closed-form solutions to initial value problems. A closedform solution is an explicit algebriac formula
More information3.4 Worksheet: Proof of the Chain Rule NAME
Mat 1170 3.4 Workseet: Proof of te Cain Rule NAME Te Cain Rule So far we are able to differentiate all types of functions. For example: polynomials, rational, root, and trigonometric functions. We are
More informationMass Lumping for Constant Density Acoustics
Lumping 1 Mass Lumping for Constant Density Acoustics William W. Symes ABSTRACT Mass lumping provides an avenue for efficient time-stepping of time-dependent problems wit conforming finite element spatial
More informationComplexity of Decoding Positive-Rate Reed-Solomon Codes
Complexity of Decoding Positive-Rate Reed-Solomon Codes Qi Ceng 1 and Daqing Wan 1 Scool of Computer Science Te University of Oklaoma Norman, OK73019 Email: qceng@cs.ou.edu Department of Matematics University
More informationCrouzeix-Velte Decompositions and the Stokes Problem
Crouzeix-Velte Decompositions and te Stokes Problem PD Tesis Strauber Györgyi Eötvös Loránd University of Sciences, Insitute of Matematics, Matematical Doctoral Scool Director of te Doctoral Scool: Dr.
More informationBlueprint End-of-Course Algebra II Test
Blueprint End-of-Course Algebra II Test for te 2001 Matematics Standards of Learning Revised July 2005 Tis revised blueprint will be effective wit te fall 2005 administration of te Standards of Learning
More informationSuperconvergence of energy-conserving discontinuous Galerkin methods for. linear hyperbolic equations. Abstract
Superconvergence of energy-conserving discontinuous Galerkin metods for linear yperbolic equations Yong Liu, Ci-Wang Su and Mengping Zang 3 Abstract In tis paper, we study superconvergence properties of
More informationThe Krewe of Caesar Problem. David Gurney. Southeastern Louisiana University. SLU 10541, 500 Western Avenue. Hammond, LA
Te Krewe of Caesar Problem David Gurney Souteastern Louisiana University SLU 10541, 500 Western Avenue Hammond, LA 7040 June 19, 00 Krewe of Caesar 1 ABSTRACT Tis paper provides an alternative to te usual
More informationAnalysis of an SEIR Epidemic Model with a General Feedback Vaccination Law
Proceedings of te World Congress on Engineering 5 Vol WCE 5 July - 3 5 London U.K. Analysis of an ER Epidemic Model wit a General Feedback Vaccination Law M. De la en. Alonso-Quesada A.beas and R. Nistal
More informationAn approximation method using approximate approximations
Applicable Analysis: An International Journal Vol. 00, No. 00, September 2005, 1 13 An approximation metod using approximate approximations FRANK MÜLLER and WERNER VARNHORN, University of Kassel, Germany,
More information