. ISSN (print), (online) International Journal of Nonlinear Science Vol.6(2008) No.3,pp
|
|
- Bennett Underwood
- 5 years ago
- Views:
Transcription
1 . ISSN (print), (online) International Journal of Nonlinear Science Vol.6(8) No.3,pp A Bouneness Criterion for Fourth Orer Nonlinear Orinary Differential Equations with Delay Cemil Tunç Department of Mathematics, Faculty of Arts an Sciences Yüüncü Yıl University, 658, Van, TURKEY. (Receive 6 September 7, March accepte 8) Abstract: In this paper, by using Lyapunov s secon metho, we stuy a certain fourth orer nonlinear orinary elay ifferential equation an obtain some sufficient conitions for the bouneness of solutions of this equation. Keywors: fourth orer nonlinear elay ifferential equation; bouneness; lyapunov functional AMS Classification number: 34K. 1 Introuction Especially, since 196s many goo books, most of them are in Russian literature, ealt with elay ifferential equations. For a comprehensive treatment of subject we refer the reaer to the book by Burton [1], Èl sgol ts [], Èl sgol ts an Norkin [3], Hale [4], Hale an Veruyn Lunel [5], Kolmanovskii an Myshkis [6], Kolmanovskii an Nosov [7], Krasovskii [8], Yoshiawa [13] an the references citie in these books. With respect to our observations from the literature, it is only foun two works achieve on the bouneness of solutions of fourth orer nonlinear elay ifferential equations. These works can be summarie as follows: First, in 1989, Okoronkwo [1] consiere the fourth-orer nonlinear elay ifferential equation of the form x (4) (t) + f(x (t))x (t) + α x (t) + β x (t h) + g(x (t h)) + α 4 x(t) + β 4 x(t h) = p(t). Subject specifie conitions impose on the functions f, g, p an the constants α, α 4, β, β 4 appeare in this equation, he establishe some sufficient conitions that guarantee the bouneness of the solutions of the equation. Later, in, Tejumola&Tchegnani [11] took into consieration the fourth-orer nonlinear elay ifferential equation x (4) (t) + ϕ(t, x(t), x (t), x (t), x (t))x (t) + ψ(t, x (t τ), x (t τ)) + χ(t, x(t τ), x (t τ)) +h(x(t τ)) = p (t, x(t), x (t), x (t), x (t), x(t τ), x (t τ), x (t τ)). They prove a result [11, Theorem.4] on the uniformly boune an uniformly ultimately boune of solutions of this equation. In this paper we are concerne with the fourth orer nonlinear elay ifferential equations of the type x (4) (t) + ϕ(x (t))x (t) + h(x (t r)) + φ(x (t r)) + f(x(t r)) = p(t, x(t), x (t), x (t), x (t), x(t r), x (t r), x (t r)) (1) Corresponing author. aress: cemtunc@yahoo.com Copyright c Worl Acaemic Press, Worl Acaemic Union IJNS /18
2 196 International Journal of Nonlinear Science,Vol.6(8),No.3,pp in which ϕ, h, φ, f an p epen only on the variables isplaye explicitly an r is a positive constant, fixe elay; the primes in equation (1) enote ifferentiation with respect to t, t [, ). It is assume as basic that the functions ϕ, h, φ, f an p are continuous in their respective arguments an satisfy a Lipschit conition in x(t), x (t), x (t), x (t), x(t r), x (t r) an x (t r); h() = φ() = f() = an the erivatives φ x φ (x ) an f x f (x) exist an are also continuous. Equation (1) can be transforme into an equivalent system of the form u = ϕ()u h() φ(y) f(x) + + x = y, y =, = u, h ((s))u(s)s + φ (y(s))(s)s f (x(s))y(s)s + p(t, x(t), y(t), (t), u(t), x(t r), y(t r), (t r)) where x(t), y(t), (t) an u(t) are respectively abbreviate as x, y, an u throughout the paper. All solutions consiere are also assume to be real value. It shoul be note in proving the main result of this paper we make use of Lyapunov s secon metho [9] as in Okoronkwo [1] an Tejumola an Tchegnani [11]. Our assumptions an the Lyapunov functional use here will be completely ifferent than that in Okoronkwo [1] an Tejumola &Tchegnani [11]. Preliminaries In orer to reach our main result, we give some important basic information for the general non-autonomous elay ifferential system (see also Èl sgol ts [], Èl sgol ts an Norkin [3], Hale [4], Hale an Veruyn Lunel [5], Kolmanovskii an Myshkis [6], Kolmanovskii an Nosov [7], Krasovskii [8] ). Now, we consier the general non-autonomous elay ifferential system ẋ = f(t, x t ), x t (θ) = x(t + θ), θ, t, (3) where f : [, ) C H R n is a continuous mapping, f(t, ) =, an we suppose that f takes close boune sets into boune sets of R n. Here (C,. ) is the Banach space of continuous function φ : [, ] R n with supremum norm, r >,C H is the open H -ball in C ; C H := {φ (C [, ], R n ) : φ < H}. Stanar existence theory, see Burton [1, pp.31], shows that if φ C H an t, then there is at least one continuous solution x(t, t, φ) such that on [t, t + α) satisfying equation (3) for t > t, x t (s, t, φ) = φ t (s) an α is a positive constant. If there is a close subset B C H such that the solution remains in B, then α =. Further, the symbol. will enote the norm in R n with x = max 1 i n x i. Definition 1 (See [1, pp.3].) A continuous function W : [, ) [, ) with W () =, W (s) > if s >, an W strictly increasing is a wege. (We enote weges by W or W i, where i an integer.) Definition (See [1, pp. 6].) Let V (t, φ) be a continuous functional efine for t, φ C H. The erivative of V along solutions of (3) will be enote by V (3) an is efine by the following relation V (3) (t, φ) = lim sup h where x(t, φ) is the solution of (3) with x t (t, φ) = φ. V (t + h, x t+h (t, φ)) V (t, x t (t, φ)), h Definition 3 (See [13, pp.184].) A function x(t, φ) is sai to be a solution of (3) with the initial conition φ C H at t = t, t, if there is a constant A > such that x(t, φ) is a function from [t h, t + A] into R n with the properties: (i) x t (t, φ) C H for t t < t + A, (ii) x t (t, φ) = φ, (iii) x(t, φ) satisfies (3) for t t < t + A. () IJNS for contribution: eitor@nonlinearscience.org.uk
3 Cemil Tunç: A Bouneness Criterion for Fourth Orer Nonlinear Orinary 197 Theorem 1 (See [13, pp.184].) If f(t, φ) in (3) is continuous in t, φ, for every φ C H1, H 1 < H, an t, t < c, where c is a positive constant, then there exist a solution of (3) with initial value φ at t = t, an this solution has a continuous erivative for t > t. 3 Main result First, we introuce the following notations: ϕ 1 () = 1 ϕ(τ)τ, ϕ(), = an φ 1 (y) = { φ(y) y, y φ (), y =. Our main result is the following theorem. Theorem In aition to the basic assumptions impose on ϕ, h, φ, f an p, we assume the following conitions are satisfie: (i) There are positive constants α 1, α, α 3, α 4,, L, 1,, 3 an ε such that α 1 α α 3 α 3 φ (y) α 1 α 4 ϕ() > for all y an, in which ε α 1 α 3 D, D = α 1α + α α 3 α 4 ; (ii) < α 4 α 1 4α 3 < f (x) α 4 for all x; (iii) φ (y) α 3 an φ 1 (y) α 3 < ε (iv) h() α α 3 8α 4 (v) ϕ() α 1, ϕ 1 () ϕ() < 8α 3 α4 α 1 α 3 for all y; α 1 for all, ( ) an h () L for all ; for all ; α 1 α 3 (vi) p(t, x(t), y(t), (t), u(t), x(t r), y(t r), (t r)) q(t), where max q(t) < an q L 1 (, ), L 1 (, ) is space of integrable Lebesgue functions. Then, there exists a finite positive constant K such that the solution x(t) of equation (1) efine by the initial functions x(t) = φ(t), x (t) = φ (t), x (t) = φ (t), x (t) = φ (t) satisfies the inequalities x(t) K, x (t) K, x (t) K, x (t) K for all t t, where φ C 3 ([t r, t ], R), provie that { εα 3 r < min ( α 4 + L + α 1 α + λ), 8α 1 α 3 (α 1 α + L + α 4 + µ), } εα 1 ( 1 α 1 α + 1 L + 1 α 4 + ρ) with λ = α 4 ( ) >, µ = α 1α ( ) > an ρ = L ( ) >. Remark 3 Making use of conitions(i),(iii) an (v) of Theorem we obtain that ϕ() < α α 3 α 4, φ (y) < α 1 α. IJNS homepage:
4 198 International Journal of Nonlinear Science,Vol.6(8),No.3,pp Proof. Now, to verify Theorem, we introuce the Lyapunov functional x y V (x t, y t, t, u t ) = f(ξ)ξ + α y 1 α 4 y + φ(η)η + 1 h(ζ)ζ + ϕ(τ)ττ + 1 u + f(x)y + 1 f(x) + 1 φ(y) + y ϕ(τ)τ + yu + u + λ y (θ)θs (4) +µ (θ)θs+ρ u (θ)θs where 1 = ε + 1, = ε + α 4, α 1 α 3 an λ, µ an µ are some positive constants which will be etermine later in the proof. In view of the assumptions of Theorem, one can easily obtain that ( ) ( ) ( ) V ε α 4 α 1 4α 3 x + α4 y + 8α 1 α + εu 3 4α 1 α 3 +λ y (θ)θs+µ (θ)θs+ρ u (θ)θs D 1 x + D y + D 3 + D 4 u +λ y (θ)θs (5) +µ (θ)θs+ρ u (θ)θs D 1 x + D y + D 3 + D 4 u ( D 5 x + y + + u ), ( ) where D 1 = 1 ε α 4 α 1 4α 3, D = α 4, D 8α 1 α 3 = 3 16α 1 α, D 4 = ε an D 5 = min {D 1, D, D 3, D 4 }. 3 (See, also, for the etails of the operations to Tunç [1]). Now, ifferentiating the functional V = V (x t, y t, t, u t ) in (4), we have [ ] [ ] t V (x t, y t, t, u t ) = [α 4 f (x)]. y + 1 h() 1 φ (y) ϕ 1 () [ ] [α 4 f (x)] [ 1 ϕ() 1] u φ(y) y α 4 y [ h() α ] y 1 [α 4 f (x)] y +( 1 u + + y)p(t, x(t), y(t), (t), u(t), x(t r), y(t r), (t r)) +( 1 u + + y) h ((s))u(s)s + ( 1 u + + y) φ (y(s))(s)s (6) +( 1 u + + y) +µ r µ f (x(s))y(s)s + λy r λ (s)s + ρu r ρ u (s)s. y (s)s IJNS for contribution: eitor@nonlinearscience.org.uk
5 Cemil Tunç: A Bouneness Criterion for Fourth Orer Nonlinear Orinary 199 By following some similar lines taken place in Tunç [1], one can easily obtain that t V (x t, y t, t, u t ) ( ) ( ) εα 3 y 8α 1 α 3 (εα 1 )u + ( 1 u + + y) +( 1 u + + y) φ (y(s))(s)s + ( 1 u + + y) h ((s))u(s)s f (x(s))y(s)s +( 1 u + + y)p(t, x(t), y(t), (t), u(t), x(t r), y(t r), (t r)) +λy r λ y (s)s + µ r µ (s)s + ρu r ρ u (s)s. Now, in view of the assumptions f (x) α 4, φ (y) α 1 α, h () L an ab a + b, it follows the following inequalities for some terms containe in (6): ( 1 u + + y) h ((s))u(s)s 1L ru (t) + L r (t) + L ry (t) ( 1 u + + y) + L ( ) u (s)s, φ (y(s))(s)s 1α 1 α ru (t) + α 1α r (t) + α 1 α ry (t) an ( 1 u + + y) + α 1α ( ) (s)s f (x(s))y(s)s 1α 4 ru (t) + α 4 r (t) + α 4 ry (t) Substituting these estimates into (6) we get + α 4 ( ) y (s)s. t V (x t, y t, t, u t ) [ εα 3 1 ( α 4 + L + α 1 α + λ)r ] y ( ) 8α 1 α 3 1 (α 1α + L + α 4 + µ)r +( 1 u + + y)p(t, x(t), y(t), (t), u(t), x(t r), y(t r), (t r)) ( εα 1 1 ( 1α 1 α + 1 L + 1 α 4 + ρ)r ) u + [ α 4 ( ) λ ] t + [ α 1 α ( ) µ ] + [ L ( ) ρ ] t y (s)s (s)s u (s)s. IJNS homepage:
6 International Journal of Nonlinear Science,Vol.6(8),No.3,pp an Let us choose Hence λ = α 4 ( ) >, µ = α 1α ( ) > ρ = L ( ) >. t V (x t, y t, t, u t ) [ εα 3 1 ( α 4 + L + α 1 α + λ)r ] y Now, in fact, we can obtain t V (x t, y t, t, u t ) τ(y + + u ) ( ) 8α 1 α 3 1 (α 1α + L + α 4 + µ)r ( εα 1 1 ( 1α 1 α + 1 L + 1 α 4 + ρ)r ) u +( 1 u + + y)p(t, x(t), y(t), (t), u(t), x(t r), y(t r), (t r)). + 1 u + + y p(t, x(t), y(t), (t), u(t), x(t r), y(t r), (t r)) for some constant τ > provie that { εα 3 r < min ( α 4 + L + α 1 α + λ), 8α 1 α 3 (α 1 α + L + α 4 + µ), } εα 1 ( 1 α 1 α + 1 L + 1 α 4 + ρ) Therefore t V (x t, y t, t, u t ) 1 u + + y p(t, x(t), y(t), (t), u(t), x(t r), y(t r), (t r)) D 6 ( y + + u ) q(t) for a constant D 6 > by (vi), where D 6 = max { 1, 1, }. Now, making use of the inequalities y < 1 + y, < 1 + an u < 1 + u, it is clear that t V (x ( t, y t, t, u t ) D y + + u ) q(t). By (5), we also have ( y + + u ) ( x + y + + u ) D5 1 V (x t, y t, t, u t ). Hence t V (x t, y t, t, u t ) D 6 ( 3 + D 1 5 V (x t, y t, t, u t ) ) q(t) = 3D 6 q(t) + D 6 D 1 5 V (x t, y t, t, u t )q(t). Now, integrating the last inequality from to t, using the assumption q L 1 (, ) an Gronwall- Rei-Bellman inequality, we obtain V (x t, y t, t, u t ) V (x, y,, u ) + 3D 6 A + D 6 D5 1 (V (x s, y s, s, u s )) q(s)s ( (V (x, y,, u ) + 3D 6 A) exp D 6 D5 1 ) q(s)s (V (x, y,, u ) + 3D 6 A) exp ( D 6 D 1 5 A) = K 1 <, (7) IJNS for contribution: eitor@nonlinearscience.org.uk
7 Cemil Tunç: A Bouneness Criterion for Fourth Orer Nonlinear Orinary 1 where K 1 > is a constant, K 1 = (V (x, y,, u ) + 3D 6 A) exp ( D 6 D5 1 A) = K 1 < an A = q(s)s. Now, the inequalities (5) an (7) together yiels that x (t) + y (t) + (t) + u (t) D 1 5 V (x t, y t, t, u t ) K, where K = K 1 D5 1. Thus, we can conclue that for all t t. That is, for all t t. The proof of Theorem is complete. References x(t) K, y(t) K, (t) K, u(t) K x(t) K, x (t) K, x (t) K, x (t) K [1] T.A.Burton: Stability an perioic solutions of orinary an functional ifferential equations. Acaemic Press, Orlano(1985). [] L. È.Èl sgol ts: Introuction to the theory of ifferential equations with eviating arguments. Translate from the Russian by Robert J. McLaughlin Holen-Day, Inc., San Francisco, Calif.-Lonon- Amsteram(1966). [3] L. È. Èl sgol ts, S. B. Norkin: Introuction to the theory an application of ifferential equations with eviating arguments. Translate from the Russian by John L. Casti. Mathematics in Science an Engineering, Vol. 15. Acaemic Press [A Subsiiary of Harcourt Brace Jovanovich, Publishers], New York-Lonon(1973). [4] J. Hale: Theory of functional ifferential equations. Springer-Verlag, New York-Heielberg(1977). [5] J. Hale, S. M. Veruyn Lunel: Introuction to functional-ifferential equations. Applie Mathematical Sciences, 99. Springer-Verlag, New York(1993). [6] V. Kolmanovskii, A. Myshkis: Introuction to the theory an applications of functional ifferential equations. Kluwer Acaemic Publishers, Dorrecht(1999). [7] V. B. Kolmanovskii, V. R. Nosov: Stability of functional-ifferential equations. Mathematics in Science an Engineering, Acaemic Press, Inc. [Harcourt Brace Jovanovich, Publishers], Lonon(1986). [8] N. N. Krasovskii: Stability of motion. Applications of Lyapunov s secon metho to ifferential systems an equations with elay. Translate by J. L. Brenner Stanfor University Press, Stanfor, Calif (1963). [9] A.M.Lyapunov: Stability of Motion. Acaemic Press, Lonon(1966). [1] O. E. Okoronkwo: On stability an bouneness of solutions of a certain fourth-orer elay ifferential equation, Internat. J. Math. Math. Sci. 1(3): (1989). [11] H. O. Tejumola, B. Tchegnani: Stability, bouneness an existence of perioic solutions of some thir an fourth orer nonlinear elay ifferential equations. J. Nigerian Math. Soc. 19: 9-19 (). [1] C.Tunç: On the stability of solutions of certain fourth-orer elay ifferential equations.applie Mathematics an Mechanics (English Eition). 7(8): (6). [13] T.Yoshiawa: Stability theory by Liapunov s secon metho. The Mathematical Society of Japan,Tokyo(1966). IJNS homepage:
Stability of solutions to linear differential equations of neutral type
Journal of Analysis an Applications Vol. 7 (2009), No.3, pp.119-130 c SAS International Publications URL : www.sasip.net Stability of solutions to linear ifferential equations of neutral type G.V. Demienko
More informationAsymptotic stability of solutions of a class of neutral differential equations with multiple deviating arguments
Bull. Math. Soc. Sci. Math. Roumanie Tome 57(15) No. 1, 14, 11 13 Asymptotic stability of solutions of a class of neutral differential equations with multiple deviating arguments by Cemil Tunç Abstract
More informationEXPONENTIAL STABILITY OF SOLUTIONS TO NONLINEAR TIME-DELAY SYSTEMS OF NEUTRAL TYPE GENNADII V. DEMIDENKO, INESSA I. MATVEEVA
Electronic Journal of Differential Equations, Vol. 2016 (2016), No. 19, pp. 1 20. ISSN: 1072-6691. URL: http://eje.math.txstate.eu or http://eje.math.unt.eu ftp eje.math.txstate.eu EXPONENTIAL STABILITY
More information6 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 informationOn Some Qualitiative Properties of Solutions to Certain Third Order Vector Differential Equations with Multiple Constant Deviating Arguments
ISSN 749-3889 (print) 749-3897 (online) International Journal of Nonlinear Science Vol.6(8) No.3pp.8-9 On Some Qualitiative Properties of Solutions to Certain Third Order Vector Differential Equations
More informationAdaptive 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 informationNOTES ON EULER-BOOLE SUMMATION (1) f (l 1) (n) f (l 1) (m) + ( 1)k 1 k! B k (y) f (k) (y) dy,
NOTES ON EULER-BOOLE SUMMATION JONATHAN M BORWEIN, NEIL J CALKIN, AND DANTE MANNA Abstract We stuy a connection between Euler-MacLaurin Summation an Boole Summation suggeste in an AMM note from 196, which
More informationCalculus 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 informationESTIMATES FOR SOLUTIONS TO A CLASS OF NONLINEAR TIME-DELAY SYSTEMS OF NEUTRAL TYPE
Electronic Journal of Differential Equations Vol. 2015 2015) No. 34 pp. 1 14. ISSN: 1072-6691. URL: http://eje.math.txstate.eu or http://eje.math.unt.eu ftp eje.math.txstate.eu ESTIMATES FOR SOLUTIONS
More informationSTABILITY ESTIMATES FOR SOLUTIONS OF A LINEAR NEUTRAL STOCHASTIC EQUATION
TWMS J. Pure Appl. Math., V.4, N.1, 2013, pp.61-68 STABILITY ESTIMATES FOR SOLUTIONS OF A LINEAR NEUTRAL STOCHASTIC EQUATION IRADA A. DZHALLADOVA 1 Abstract. A linear stochastic functional ifferential
More information19 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 informationA Boundedness Theorem for a Certain Third Order Nonlinear Differential Equation
Journal of Mathematics Statistics 4 ): 88-93, 008 ISSN 1549-3644 008 Science Publications A Bouneness Theorem for a Certain Thir Orer Nonlinear Differential Equation AT Aemola, R Kehine OM Ogunlaran Department
More informationA Note on Exact Solutions to Linear Differential Equations by the Matrix Exponential
Avances in Applie Mathematics an Mechanics Av. Appl. Math. Mech. Vol. 1 No. 4 pp. 573-580 DOI: 10.4208/aamm.09-m0946 August 2009 A Note on Exact Solutions to Linear Differential Equations by the Matrix
More informationMARKO NEDELJKOV, DANIJELA RAJTER-ĆIRIĆ
GENERALIZED UNIFORMLY CONTINUOUS SEMIGROUPS AND SEMILINEAR HYPERBOLIC SYSTEMS WITH REGULARIZED DERIVATIVES MARKO NEDELJKOV, DANIJELA RAJTER-ĆIRIĆ Abstract. We aopt the theory of uniformly continuous operator
More informationThe effect of dissipation on solutions of the complex KdV equation
Mathematics an Computers in Simulation 69 (25) 589 599 The effect of issipation on solutions of the complex KV equation Jiahong Wu a,, Juan-Ming Yuan a,b a Department of Mathematics, Oklahoma State University,
More informationd dx [xn ] = nx n 1. (1) dy dx = 4x4 1 = 4x 3. Theorem 1.3 (Derivative of a constant function). If f(x) = k and k is a constant, then f (x) = 0.
Calculus refresher Disclaimer: I claim no original content on this ocument, which is mostly a summary-rewrite of what any stanar college calculus book offers. (Here I ve use Calculus by Dennis Zill.) I
More informationLogarithmic 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 informationAbstract A nonlinear partial differential equation of the following form is considered:
M P E J Mathematical Physics Electronic Journal ISSN 86-6655 Volume 2, 26 Paper 5 Receive: May 3, 25, Revise: Sep, 26, Accepte: Oct 6, 26 Eitor: C.E. Wayne A Nonlinear Heat Equation with Temperature-Depenent
More informationLectures - 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 informationCEMİL TUNÇ* ABSTRACT. Keywords: Delay differential equation; fourth and fifth order; instability; Lyapunov-Krasovskii functional ABSTRAK
Sains Malaysiana 40(12)(2011): 1455 1459 On the Instability of Solutions of Nonlinear Delay Differential Equations of Fourth Fifth Order (Kestabilan Penyelesaian Persamaan Pembezaan Tunda Tak Linear Tertib
More informationAgmon 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 informationFURTHER BOUNDS FOR THE ESTIMATION ERROR VARIANCE OF A CONTINUOUS STREAM WITH STATIONARY VARIOGRAM
FURTHER BOUNDS FOR THE ESTIMATION ERROR VARIANCE OF A CONTINUOUS STREAM WITH STATIONARY VARIOGRAM N. S. BARNETT, S. S. DRAGOMIR, AND I. S. GOMM Abstract. In this paper we establish an upper boun for the
More informationarxiv: v1 [math.ds] 21 Sep 2017
UNBOUNDED AND BLOW-UP SOLUTIONS FOR A DELAY LOGISTIC EQUATION WITH POSITIVE FEEDBACK arxiv:709.07295v [math.ds] 2 Sep 207 ISTVÁN GYŐRI, YUKIHIKO NAKATA, AND GERGELY RÖST Abstract. We stuy boune, unboune
More informationJUST 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 informationELEC3114 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 informationOscillations in a van der Pol equation with delayed argument
J. Math. Anal. Appl. 275 (22) 789 83 www.acaemicpress.com Oscillations in a van er Pol equation with elaye argument J.C.F. e Oliveira CCEN niversiae Feeral o Pará, Av. Augusto Correia, 4, CEP 6623-22,
More informationMethod of Lyapunov functionals construction in stability of delay evolution equations
J. Math. Anal. Appl. 334 007) 1130 1145 www.elsevier.com/locate/jmaa Metho of Lyapunov functionals construction in stability of elay evolution equations T. Caraballo a,1, J. Real a,1, L. Shaikhet b, a
More informationThe 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 informationWELL-POSEDNESS OF A POROUS MEDIUM FLOW WITH FRACTIONAL PRESSURE IN SOBOLEV SPACES
Electronic Journal of Differential Equations, Vol. 017 (017), No. 38, pp. 1 7. ISSN: 107-6691. URL: http://eje.math.txstate.eu or http://eje.math.unt.eu WELL-POSEDNESS OF A POROUS MEDIUM FLOW WITH FRACTIONAL
More informationNonlinear Control Systems
Nonlinear Control Systems António Pedro Aguiar pedro@isr.ist.utl.pt 3. Fundamental properties IST-DEEC PhD Course http://users.isr.ist.utl.pt/%7epedro/ncs2012/ 2012 1 Example Consider the system ẋ = f
More informationCHAPTER 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 informationLagrangian 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 informationON THE RIEMANN EXTENSION OF THE SCHWARZSCHILD METRICS
ON THE RIEANN EXTENSION OF THE SCHWARZSCHILD ETRICS Valerii Dryuma arxiv:gr-qc/040415v1 30 Apr 004 Institute of athematics an Informatics, AS R, 5 Acaemiei Street, 08 Chisinau, olova, e-mail: valery@ryuma.com;
More informationSOME RESULTS ASSOCIATED WITH FRACTIONAL CALCULUS OPERATORS INVOLVING APPELL HYPERGEOMETRIC FUNCTION
Volume 29), Issue, Article 4, 7 pp. SOME RESULTS ASSOCIATED WITH FRACTIONAL CALCULUS OPERATORS INVOLVING APPELL HYPERGEOMETRIC FUNCTION R. K. RAINA / GANPATI VIHAR, OPPOSITE SECTOR 5 UDAIPUR 332, RAJASTHAN,
More informationA global Implicit Function Theorem without initial point and its applications to control of non-affine systems of high dimensions
J. Math. Anal. Appl. 313 (2006) 251 261 www.elsevier.com/locate/jmaa A global Implicit Function Theorem without initial point an its applications to control of non-affine systems of high imensions Weinian
More informationApproximate reduction of dynamic systems
Systems & Control Letters 57 2008 538 545 www.elsevier.com/locate/sysconle Approximate reuction of ynamic systems Paulo Tabuaa a,, Aaron D. Ames b, Agung Julius c, George J. Pappas c a Department of Electrical
More informationA nonlinear inverse problem of the Korteweg-de Vries equation
Bull. Math. Sci. https://oi.org/0.007/s3373-08-025- A nonlinear inverse problem of the Korteweg-e Vries equation Shengqi Lu Miaochao Chen 2 Qilin Liu 3 Receive: 0 March 207 / Revise: 30 April 208 / Accepte:
More informationMathematical Review Problems
Fall 6 Louis Scuiero Mathematical Review Problems I. Polynomial Equations an Graphs (Barrante--Chap. ). First egree equation an graph y f() x mx b where m is the slope of the line an b is the line's intercept
More information2 GUANGYU LI AND FABIO A. MILNER The coefficient a will be assume to be positive, boune, boune away from zero, an inepenent of t; c will be assume con
A MIXED FINITE ELEMENT METHOD FOR A THIRD ORDER PARTIAL DIFFERENTIAL EQUATION G. Li 1 an F. A. Milner 2 A mixe finite element metho is escribe for a thir orer partial ifferential equation. The metho can
More informationExponential 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 informationOn some parabolic systems arising from a nuclear reactor model
On some parabolic systems arising from a nuclear reactor moel Kosuke Kita Grauate School of Avance Science an Engineering, Wasea University Introuction NR We stuy the following initial-bounary value problem
More informationParametric optimization of a neutral system with two delays and PD-controller
10.2478/acsc-2013-0008 Archives of Control Sciences Volume 23LIX, 2013 No. 2, pages 131 143 Parametric optimization of a neutral system with two elays an PD-controller JÓZEF DUDA In this paper a parametric
More informationLie symmetry and Mei conservation law of continuum system
Chin. Phys. B Vol. 20, No. 2 20 020 Lie symmetry an Mei conservation law of continuum system Shi Shen-Yang an Fu Jing-Li Department of Physics, Zhejiang Sci-Tech University, Hangzhou 3008, China Receive
More informationarxiv: v1 [math-ph] 5 May 2014
DIFFERENTIAL-ALGEBRAIC SOLUTIONS OF THE HEAT EQUATION VICTOR M. BUCHSTABER, ELENA YU. NETAY arxiv:1405.0926v1 [math-ph] 5 May 2014 Abstract. In this work we introuce the notion of ifferential-algebraic
More informationComputing 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 information1 Heisenberg Representation
1 Heisenberg Representation What we have been ealing with so far is calle the Schröinger representation. In this representation, operators are constants an all the time epenence is carrie by the states.
More informationIntroduction to the Vlasov-Poisson system
Introuction to the Vlasov-Poisson system Simone Calogero 1 The Vlasov equation Consier a particle with mass m > 0. Let x(t) R 3 enote the position of the particle at time t R an v(t) = ẋ(t) = x(t)/t its
More informationARBITRARY NUMBER OF LIMIT CYCLES FOR PLANAR DISCONTINUOUS PIECEWISE LINEAR DIFFERENTIAL SYSTEMS WITH TWO ZONES
Electronic Journal of Differential Equations, Vol. 2015 (2015), No. 228, pp. 1 12. ISSN: 1072-6691. URL: http://eje.math.txstate.eu or http://eje.math.unt.eu ftp eje.math.txstate.eu ARBITRARY NUMBER OF
More informationSystems & 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 informationDiscrete Operators in Canonical Domains
Discrete Operators in Canonical Domains VLADIMIR VASILYEV Belgoro National Research University Chair of Differential Equations Stuencheskaya 14/1, 308007 Belgoro RUSSIA vlaimir.b.vasilyev@gmail.com Abstract:
More informationSwitching 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 informationLower 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 informationOn the qualitative properties of differential equations of third order with retarded argument
Proyecciones Journal of Mathematics Vol. 33, N o 3, pp. 325-347, September 2014. Universidad Católica del Norte Antofagasta - Chile On the qualitative properties of differential equations of third order
More informationINVERSE PROBLEM OF A HYPERBOLIC EQUATION WITH AN INTEGRAL OVERDETERMINATION CONDITION
Electronic Journal of Differential Equations, Vol. 216 (216), No. 138, pp. 1 7. ISSN: 172-6691. URL: http://eje.math.txstate.eu or http://eje.math.unt.eu INVERSE PROBLEM OF A HYPERBOLIC EQUATION WITH AN
More informationEXPONENTIAL FOURIER INTEGRAL TRANSFORM METHOD FOR STRESS ANALYSIS OF BOUNDARY LOAD ON SOIL
Tome XVI [18] Fascicule 3 [August] 1. Charles Chinwuba IKE EXPONENTIAL FOURIER INTEGRAL TRANSFORM METHOD FOR STRESS ANALYSIS OF BOUNDARY LOAD ON SOIL 1. Department of Civil Engineering, Enugu State University
More informationGLOBAL DYNAMICS OF THE SYSTEM OF TWO EXPONENTIAL DIFFERENCE EQUATIONS
Electronic Journal of Mathematical Analysis an Applications Vol. 7(2) July 209, pp. 256-266 ISSN: 2090-729X(online) http://math-frac.org/journals/ejmaa/ GLOBAL DYNAMICS OF THE SYSTEM OF TWO EXPONENTIAL
More informationChaos, Solitons and Fractals Nonlinear Science, and Nonequilibrium and Complex Phenomena
Chaos, Solitons an Fractals (7 64 73 Contents lists available at ScienceDirect Chaos, Solitons an Fractals onlinear Science, an onequilibrium an Complex Phenomena journal homepage: www.elsevier.com/locate/chaos
More informationInternational Journal of Pure and Applied Mathematics Volume 35 No , ON PYTHAGOREAN QUADRUPLES Edray Goins 1, Alain Togbé 2
International Journal of Pure an Applie Mathematics Volume 35 No. 3 007, 365-374 ON PYTHAGOREAN QUADRUPLES Eray Goins 1, Alain Togbé 1 Department of Mathematics Purue University 150 North University Street,
More informationBEYOND 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 informationSOME LYAPUNOV TYPE POSITIVE OPERATORS ON ORDERED BANACH SPACES
Ann. Aca. Rom. Sci. Ser. Math. Appl. ISSN 2066-6594 Vol. 5, No. 1-2 / 2013 SOME LYAPUNOV TYPE POSITIVE OPERATORS ON ORDERED BANACH SPACES Vasile Dragan Toaer Morozan Viorica Ungureanu Abstract In this
More informationOPTIMAL CONTROL OF A PRODUCTION SYSTEM WITH INVENTORY-LEVEL-DEPENDENT DEMAND
Applie Mathematics E-Notes, 5(005), 36-43 c ISSN 1607-510 Available free at mirror sites of http://www.math.nthu.eu.tw/ amen/ OPTIMAL CONTROL OF A PRODUCTION SYSTEM WITH INVENTORY-LEVEL-DEPENDENT DEMAND
More informationθ x = f ( x,t) could be written as
9. Higher orer PDEs as systems of first-orer PDEs. Hyperbolic systems. For PDEs, as for ODEs, we may reuce the orer by efining new epenent variables. For example, in the case of the wave equation, (1)
More informationLinear and quadratic approximation
Linear an quaratic approximation November 11, 2013 Definition: Suppose f is a function that is ifferentiable on an interval I containing the point a. The linear approximation to f at a is the linear function
More informationOn the Inclined Curves in Galilean 4-Space
Applie Mathematical Sciences Vol. 7 2013 no. 44 2193-2199 HIKARI Lt www.m-hikari.com On the Incline Curves in Galilean 4-Space Dae Won Yoon Department of Mathematics Eucation an RINS Gyeongsang National
More informationUniqueness of limit cycles of the predator prey system with Beddington DeAngelis functional response
J. Math. Anal. Appl. 290 2004 113 122 www.elsevier.com/locate/jmaa Uniqueness of limit cycles of the preator prey system with Beington DeAngelis functional response Tzy-Wei Hwang 1 Department of Mathematics,
More informationThe Ehrenfest Theorems
The Ehrenfest Theorems Robert Gilmore Classical Preliminaries A classical system with n egrees of freeom is escribe by n secon orer orinary ifferential equations on the configuration space (n inepenent
More informationGLOBAL SOLUTIONS FOR 2D COUPLED BURGERS-COMPLEX-GINZBURG-LANDAU EQUATIONS
Electronic Journal of Differential Equations, Vol. 015 015), No. 99, pp. 1 14. ISSN: 107-6691. URL: http://eje.math.txstate.eu or http://eje.math.unt.eu ftp eje.math.txstate.eu GLOBAL SOLUTIONS FOR D COUPLED
More informationMath 300 Winter 2011 Advanced Boundary Value Problems I. Bessel s Equation and Bessel Functions
Math 3 Winter 2 Avance Bounary Value Problems I Bessel s Equation an Bessel Functions Department of Mathematical an Statistical Sciences University of Alberta Bessel s Equation an Bessel Functions We use
More informationA medical image encryption algorithm based on synchronization of time-delay chaotic system
Av. Manuf. (1) 5:15 1 DOI 1.1/s3-1-1-5 A meical image encryption algorithm base on synchronization of time-elay chaotic system Hua Wang 1 Jian-Min Ye 1 Hang-Feng Liang 1 Zhong-Hua Miao 1 Receive: 9 October
More informationMultiplicity Results of Positive Solutions for Nonlinear Three-Point Boundary Value Problems on Time Scales
Avances in Dynamical Systems an Applications ISSN 973-532, Volume 4, Number 2, pp. 243 253 (29) http://campus.mst.eu/asa Multiplicity Results of Positive Solutions for Nonlinear Three-Point Bounary Value
More informationWUCHEN LI AND STANLEY OSHER
CONSTRAINED DYNAMICAL OPTIMAL TRANSPORT AND ITS LAGRANGIAN FORMULATION WUCHEN LI AND STANLEY OSHER Abstract. We propose ynamical optimal transport (OT) problems constraine in a parameterize probability
More informationMulti-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 informationA new proof of the sharpness of the phase transition for Bernoulli percolation on Z d
A new proof of the sharpness of the phase transition for Bernoulli percolation on Z Hugo Duminil-Copin an Vincent Tassion October 8, 205 Abstract We provie a new proof of the sharpness of the phase transition
More informationApplications of the Wronskian to ordinary linear differential equations
Physics 116C Fall 2011 Applications of the Wronskian to orinary linear ifferential equations Consier a of n continuous functions y i (x) [i = 1,2,3,...,n], each of which is ifferentiable at least n times.
More informationContinuous observer design for nonlinear systems with sampled and delayed output measurements
Preprints of th9th Worl Congress The International Feeration of Automatic Control Continuous observer esign for nonlinear systems with sample an elaye output measurements Daoyuan Zhang Yanjun Shen Xiaohua
More informationFLUCTUATIONS IN THE NUMBER OF POINTS ON SMOOTH PLANE CURVES OVER FINITE FIELDS. 1. Introduction
FLUCTUATIONS IN THE NUMBER OF POINTS ON SMOOTH PLANE CURVES OVER FINITE FIELDS ALINA BUCUR, CHANTAL DAVID, BROOKE FEIGON, MATILDE LALÍN 1 Introuction In this note, we stuy the fluctuations in the number
More informationConservation laws a simple application to the telegraph equation
J Comput Electron 2008 7: 47 51 DOI 10.1007/s10825-008-0250-2 Conservation laws a simple application to the telegraph equation Uwe Norbrock Reinhol Kienzler Publishe online: 1 May 2008 Springer Scienceusiness
More informationProblem 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 informationarxiv: v1 [physics.class-ph] 20 Dec 2017
arxiv:1712.07328v1 [physics.class-ph] 20 Dec 2017 Demystifying the constancy of the Ermakov-Lewis invariant for a time epenent oscillator T. Pamanabhan IUCAA, Post Bag 4, Ganeshkhin, Pune - 411 007, Inia.
More informationDissipative 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 informationANALYSIS OF A GENERAL FAMILY OF REGULARIZED NAVIER-STOKES AND MHD MODELS
ANALYSIS OF A GENERAL FAMILY OF REGULARIZED NAVIER-STOKES AND MHD MODELS MICHAEL HOLST, EVELYN LUNASIN, AND GANTUMUR TSOGTGEREL ABSTRACT. We consier a general family of regularize Navier-Stokes an Magnetohyroynamics
More informationIndirect Adaptive Fuzzy and Impulsive Control of Nonlinear Systems
International Journal of Automation an Computing 7(4), November 200, 484-49 DOI: 0007/s633-00-053-7 Inirect Aaptive Fuzzy an Impulsive Control of Nonlinear Systems Hai-Bo Jiang School of Mathematics, Yancheng
More informationAccelerate 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 informationOn the Periodic Solutions of Certain Fifth Order Nonlinear Vector Differential Equations
On the Periodic Solutions of Certain Fifth Order Nonlinear Vector Differential Equations Melike Karta Department of Mathematics, Faculty of Science and Arts, Agri Ibrahim Cecen University, Agri, E-mail:
More informationDISCONTINUOUS DYNAMICAL SYSTEMS AND FRACTIONAL-ORDERS DIFFERENCE EQUATIONS
Journal of Fractional Calculus Applications, Vol. 4(1). Jan. 2013, pp. 130-138. ISSN: 2090-5858. http://www.fcaj.webs.com/ DISCONTINUOUS DYNAMICAL SYSTEMS AND FRACTIONAL-ORDERS DIFFERENCE EQUATIONS A.
More informationMath Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors
Math 18.02 Notes on ifferentials, the Chain Rule, graients, irectional erivative, an normal vectors Tangent plane an linear approximation We efine the partial erivatives of f( xy, ) as follows: f f( x+
More informationExponential asymptotic property of a parallel repairable system with warm standby under common-cause failure
J. Math. Anal. Appl. 341 (28) 457 466 www.elsevier.com/locate/jmaa Exponential asymptotic property of a parallel repairable system with warm stanby uner common-cause failure Zifei Shen, Xiaoxiao Hu, Weifeng
More informationMath 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 informationCalculus and optimization
Calculus an optimization These notes essentially correspon to mathematical appenix 2 in the text. 1 Functions of a single variable Now that we have e ne functions we turn our attention to calculus. A function
More informationMartin Luther Universität Halle Wittenberg Institut für Mathematik
Martin Luther Universität alle Wittenberg Institut für Mathematik Weak solutions of abstract evolutionary integro-ifferential equations in ilbert spaces Rico Zacher Report No. 1 28 Eitors: Professors of
More informationEnergy behaviour of the Boris method for charged-particle dynamics
Version of 25 April 218 Energy behaviour of the Boris metho for charge-particle ynamics Ernst Hairer 1, Christian Lubich 2 Abstract The Boris algorithm is a wiely use numerical integrator for the motion
More informationWell-posedness of hyperbolic Initial Boundary Value Problems
Well-poseness of hyperbolic Initial Bounary Value Problems Jean-François Coulombel CNRS & Université Lille 1 Laboratoire e mathématiques Paul Painlevé Cité scientifique 59655 VILLENEUVE D ASCQ CEDEX, France
More informationPartial Differential Equations
Chapter Partial Differential Equations. Introuction Have solve orinary ifferential equations, i.e. ones where there is one inepenent an one epenent variable. Only orinary ifferentiation is therefore involve.
More informationA Weak First Digit Law for a Class of Sequences
International Mathematical Forum, Vol. 11, 2016, no. 15, 67-702 HIKARI Lt, www.m-hikari.com http://x.oi.org/10.1288/imf.2016.6562 A Weak First Digit Law for a Class of Sequences M. A. Nyblom School of
More informationSYSTEMS OF DIFFERENTIAL EQUATIONS, EULER S FORMULA. where L is some constant, usually called the Lipschitz constant. An example is
SYSTEMS OF DIFFERENTIAL EQUATIONS, EULER S FORMULA. Uniqueness for solutions of ifferential equations. We consier the system of ifferential equations given by x = v( x), () t with a given initial conition
More informationSturm-Liouville Theory
LECTURE 5 Sturm-Liouville Theory In the three preceing lectures I emonstrate the utility of Fourier series in solving PDE/BVPs. As we ll now see, Fourier series are just the tip of the iceberg of the theory
More informationASYMPTOTICS TOWARD THE PLANAR RAREFACTION WAVE FOR VISCOUS CONSERVATION LAW IN TWO SPACE DIMENSIONS
TANSACTIONS OF THE AMEICAN MATHEMATICAL SOCIETY Volume 35, Number 3, Pages 13 115 S -9947(999-4 Article electronically publishe on September, 1999 ASYMPTOTICS TOWAD THE PLANA AEFACTION WAVE FO VISCOUS
More informationOn classical orthogonal polynomials and differential operators
INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS A: MATHEMATICAL AND GENERAL J. Phys. A: Math. Gen. 38 2005) 6379 6383 oi:10.1088/0305-4470/38/28/010 On classical orthogonal polynomials an ifferential
More informationOn 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 informationmodel considered before, but the prey obey logistic growth in the absence of predators. In
5.2. First Orer Systems of Differential Equations. Phase Portraits an Linearity. Section Objective(s): Moifie Preator-Prey Moel. Graphical Representations of Solutions. Phase Portraits. Vector Fiels an
More information