STABILITY OF A LINEAR INTEGRO-DIFFERENTIAL EQUATION OF FIRST ORDER WITH VARIABLE DELAYS

Size: px
Start display at page:

Download "STABILITY OF A LINEAR INTEGRO-DIFFERENTIAL EQUATION OF FIRST ORDER WITH VARIABLE DELAYS"

Transcription

1 Bulletin of Mathematical Analyi and Application ISSN: , URL: Volume 1 Iue 2(218), Page STABILITY OF A LINEAR INTEGRO-DIFFERENTIAL EQUATION OF FIRST ORDER WITH VARIABLE DELAYS CEMİL TUNÇ, İREM AKBULUT Abtract. We conider a linear integro-differential equation (IDE) of firt order with two variable delay. We contruct new condition guaranteeing the trivial olution of thi IDE i table. The technique of the proof baed on the ue of the fixed-point theory. Our finding generalize and improve ome reult can be found in the literature. 1. Introduction It i well known from the related literature that the IDE are often ued to model ome practical problem in mechanic, phyic, biology, ecology and the other cientific field (ee, e.g. Burton [5], Levin [1], Rahman [14], Wazwaz [24] and their reference). Thi paper deal with the following linear IDE of the firt order with two variable delay dx dt = b(t)x a(t, )x()d, (1.1) where t, t R, x R, R = (, ), r i = [, ) [, ), (i = 1, 2), are continuou differentiable function uch that t r i (t) a t with r = max t {t r 1 (t), t r 2 (t)}, a : [ r, ) [ r, ) R and b : (, ) R are continuou function. In the pat decade, a number of reearche have dealt with qualitative behavior of linear and non-linear IDE by mean of the fixed point theory, the perturbation method, the variation of parameter formula, the Lyapunov function or functional method, etc., (ee Ardjouni and Djoudi [1], Becker and Burton [2], Burton ([3], [4]), Gabi et al. [6], Gözen and Tunç [7], Graef and Tunç [8], Jin and Luo [9], Levin [1], Pi ([11], [12]), Raffoul [13], Tunç ([15], [16],[17],[18], [19]), Tunç and Mohammed [2], Tunç and Tunç ([21], [22],[23]) and their reference). Among thee invetigation, the tability analyi of olution ha been an important topic for IDE with contant or variable delay and without delay. For variou model and kind of IDE, many ignificant reult have been preented, ee, for example, the reference of thi article and thoe regitered therein. Here, 2 Mathematic Subject Claification. 34K2, 45J5. Key word and phrae. Contraction mapping, tability, fixed point, integro-differential equation, variable delay, firt order. c 218 Univeriteti i Prihtinë, Prihtinë, Koovë. Submitted April 4, 218. Publihed May 15, 218. Communicate by Tongxing Li. 19

2 2 C. TUNÇ, İ. AKBULUT we would not give the detail of the work and their application. However, we would like to ummarize here a few related reult on the topic. Firt, in 1963, Levin [1] conidered the linear IDE dx dt = a(t )g(x())d and the author gave ufficient condition guaranteeing that if any olution of the above IDE exit on [, ), then the olution of thi IDE, it firt and econd order derivative tend to zero when t. The proof of the main reult of [1] involve the ue of a uitably choen Lyapunov function. Later, in 24, Burton [4] took into conideration the following non-linear IDE with contant delay of the form dx dt = t r a(t, )g(x())d. In [4], intead of uing a Lyapunov functional, the author tudied aymptotic tability of the above IDE by uing the concept of a contraction mapping in line with the fixed point theory for a cla of equation which ha been comprehenively tudied in the lat fifty year. The reult of [4] look very intereting. Finally, Jin and Luo [9] tudied a calar integro-differential equation (in both the linear and nonlinear cae) etablihing ufficient condition for the exitence, tability and aymptotic tability for the null olution. The IDE examined by the author are given by dx t dt = a(t, )x()d t r(t) and dx t dt = a(t, )g(x())d. t r(t) In [9], in order to have the poibility of applying Banach fixed point theorem, firt IDE i written in an equivalent form and if x(t) = ψ(t) on [ r, ), it i hown that the olution x(t) of firt IDE i bounded on [ r, ) and the trivial olution of the ame IDE i alo table. Under an additional condition, it i proved for the econd IDE that x(t) a t. The nonlinear cae (the econd IDE) look omewhat more complicated but it admit a treatment imilar to that of the former one. The motivation to conider IDE (1.1) and invetigation it ome qualitative propertie come from the paper of Levin [1], Burton [4], Jin and Luo [9] and the ource that found in the reference of thi article. Here, we give new reult on the boundedne, tability, aymptotic tability and ome other propertie of olution of IDE (1.1). The conidered IDE, the reult and aumption to be given here are different from that can be found in the literature and complete that one. Thee are the contribution of thi paper to the literature and it novelty and originality. The following definition may be ueful for reader. Definition 1. The zero olution of IDE (1.1) i aid to be table at t = if, for every, ε >, there exit a δ > uch that ψ : [ r, ] ( δ, δ) implie that x(t) < ε for t r.

3 STABILITY OF A LINEAR INTEGRO-DIFFERENTIAL EQUATION We can write IDE (1.1) a where G(t, ) = dx dt b(t)x = G(t, t r i (t))(1 r i(t))x(t r i (t)) t a(u, )du with G(t, t r i (t)) = d t G(t, )x()d, (1.2) dt ri(t) t a(u, t r i (t))du. (1.3) Theorem 1. If x(t) i a olution of IDE (1.1) on an interval [, T ) and atifie the initial condition x(t) = ψ(t) for t [ r, ], then x(t) i a olution of IE x(t) = 2 b()d)ψ() [b(u) G(t, u)]x(u)du b() r i() r i() [b(u) G(, u)]x(u)dud [b(u) G(, u)]ψ(u)du [b( r i () G(, r i ())](1 r i())x( r i ())d b()x()d (1.4) on [, T ), where b : [ r, ) R i an arbitrary continuou function. Converely, if a continuou function x(t) i equal to ψ(t) for t [ r, ] and i a olution of IE (1.4) on an interval [, τ), then x(t) i a olution of IDE (1.1) on [, τ). Proof. Multiplying both ide of IDE (1.2) by the factor exp( and integrating from to any t, t [, τ), then we get o that d dt x (t)exp( ( x()exp( = exp( exp( exp( ) = b(t)x(t) G(t, t r i (t))(1 r i(t))x(t r i (t)) [ d dt G(t, )x()d G(, r i ())(1 r i())x( r i ()) d d r i() G(, u)x(u)du]exp(.

4 22 C. TUNÇ, İ. AKBULUT Hence o that x(t)exp( x(t) = d d ψ()exp( = [ G(, r i ())(1 r i())x( r i ()) d d ψ() r i() Hence, we can write that x(t) = 2 b()d)ψ() r i() [ G(, u)x(u)du]exp( G(, r i ())(1 r i())x( r i ()) G(, u)x(u)du]exp( d d r i(). (1.5) [b(u) G(, u)]x(u)dud [b( r i ()) G(, r i ())](1 r i())x( r i ())d b()x()d. (1.6) We will now how that etimate (1.6) i equal to etimate (1.5). In fact, it follow from (1.6) that x(t) = 2 b()d)ψ() d d r i() d d G(, u)x(u)dud r i() b( r i ())(1 r i())x( r i ())d G( r i ())(1 r i())x( r i ())d b()x()d. b(u)x(u)dud

5 STABILITY OF A LINEAR INTEGRO-DIFFERENTIAL EQUATION Applying integration by part to the econd and third term of (1.6), we get x(t) = 2 = b()d)ψ() b()d) [b(u) G(, u)]x(u)du t r i() b() [b(u) G(, u)]x(u)dud r i() b()d)ψ() [b( r i ()) G(, r i ())](1 r i())x( r i ())d b()x()d b()d) [b(u) G(, u)]x(u)du r i() [b(u) G(t, u)]x(u)du b() [b(u) G(, u)]x(u)dud r i() 2 [b( r i ()) G(, r i ())](1 r i())x( r i ())d b()x()d, which lead to (1.4). Converely, uppoe that there exit a continuou function x(t) which i equal to ψ(t) on [ r, ] and atifie IE (1.4) on an interval [, τ). Then, the function x(t) i differentiable on [, τ) and if we calculate the time derivative of IE (1.4) with the aid of Leibniz rule, then we obtain IDE (1.2). Next, we will define a mapping directly from (1.4). By Theorem 1, a fixed point of that map will be a olution of IE (1.4) and IDE (1.1). To obtain tability of the zero olution of IDE (1.1), we need the mapping defined by IE (1.4) to map bounded function into bounded function. Let (C,. ) be the et of real-valued and bounded continuou function on [ r, ) with the upremum norm. that i, for φ C, φ = up{ φ(t) : t [ r, )}. In other word, we carry out our invetigation in the complete metric pace (C, ρ), where ρ denote the upremum (uniform) metric for φ 1, φ 2 C, and it i defined

6 24 C. TUNÇ, İ. AKBULUT by ρ(φ 1, φ 2 ) = φ 1 φ 2. For a given continuou initial function ψ : [ r, ) R, define the et C ψ C by C ψ = {φ : [ r, ) R φ C, φ(t) = ψ(t) for t [ r, ]}. Let. denote the upremum on [ r, ] or on [ r, ). Finally, note that (C ψ,. ) i itelf a complete metric pace ince C ψ i a cloed ubet of C. Theorem 2. Let b : [ r, ) R be a continuou function and T be a mapping on C ψ defined for φ C ψ by and (T φ)(t) = 2 b()d)ψ() (T φ)(t) = ψ(t) if t [ r, ] r i() [b(u) G(t, u)]φ(u)du b() [b(u) G(, u)]ψ(u)du r i() [b(u) G(, u)]φ(u)dud [b( r i ()) G(, r i ())](1 r i())φ( r i ())d b()φ()d. (1.7) Aume that there exit contant k and α > uch that and 2 b(u) G(t, u) du b()d k (1.8) b() b(u) G(, u) dud r i() b( r i ()) G(, r i ()) (1 r i() d b() d a (1.9) for t, then T : C ψ C ψ. Proof. For φ C ψ, T φ i continuou and agree with ψ on [ r, ] by virtue of

7 STABILITY OF A LINEAR INTEGRO-DIFFERENTIAL EQUATION the definition of T. In view of (1.8) and (1.9), for t >, we have (T φ)(t) exp(k) ψ() exp(k) r i() b(u) G(, u) φ(u) du α φ. Hence, ubject to the hypothee of Theorem 2, it i clear that (T φ)(t) exp(k) ψ (1 b(u) G(, u) du) α φ <. (1.1) r i() Thu, we can conclude that T φ C ψ. Theorem 3. Let k, α (, 1) and b : [ r, ) R be a continuou function uch that (1.8) and (1.9) hold for t. Then for each continuou function ψ : [ r, ] R, there i an unique continuou function x : [ r, ) R with x(t) = ψ(t) on [ r, ). In addition, x(t) i bounded on [ r, ) and the zero olution of IDE (1.1) i table at t =. Finally, if b()d (1.11) hold a t, then x(t) a t. Proof. We now take into conideration the pace C ψ defined by the continuou initial function ψ : [ r, ] R. For φ, η C ψ in the light of the hypothee of Theorem 3, it can be een that (T φ)(t) (T η)(t) b(u) G(t, u) φ(u) η(u) du b() r i() b( r i () G(, r i ())) 1 r i() φ( r i ()) η( r i ()) d 2 ( 2 b() φ() η() d b(u) G(t, u) du b() r i() b(u) G(, u) φ(u) η(u) dud b(u) G(, u) dud b( r i () G(, r i ())) 1 r i() d b() φ η d. By the definition of T and (1.9), T i a contraction mapping with contraction contant α. By Banach contraction mapping principle, T ha a unique fixed point x in C ψ which i a bounded and continuou function. By Theorem 3, it i a olution

8 26 C. TUNÇ, İ. AKBULUT of IDE (1.1) on [, ). It follow that x i the only bounded and continuou function atifying IDE (1.1) on [, ) and the initial condition. It i clear that the zero olution of IDE (1.1) i table. If x(t) i a olution with the initial function ψ on [ r, ], then, by (1.1), we have (1 α) x exp(k) ψ (1 b(u) G(, u) du). r i() Then, for each ε >, there exit a δ > uch that x(t) < ε for all t r if ψ < δ. Next we prove that the olution of IDE (1.1) tend to zero when (1.11) hold. Firt, we define a ubet C ψ of C ψ by C ψ = {φ : [ r, ) R φ C, φ(t) = ψ(t) for t [ r, ], φ(t) a t }. Since Cψ i a cloed ubet of C ψ and (Cψ, ρ) i complete, then the metric pace (Cψ, ρ) i alo complete. Now we how that (T φ)(t) a t when φ C ψ. By (1.7) and (1.9), we have (T φ)(t) b()d)( ψ() b(u) G(, u) )du α φ [t ri(t),t] I 4 I 5, r i() where t >, I 4 and I 5 denote fourth and fifth, ixth term of (1.7), repectively. We can prove that each of the above term tend to zero a t. In fact, it i eay to ee that the firt term tend to by (1.11) and the econd term approache zero a t ince t r i (t), i = 1, 2. Hence, for each ε >, there exit a M > uch that φ [M ri(m), ) ε 2α ince t r i (t) a t. Then, for t M we can ee that M M I 4 b() b(u) G(, u) dud φ T b() r i() r i() b(u) G(, u) dud φ [M ri(m), ). By (1.11), there exit a τ M uch that φ T < ε 2α for t > τ. Thu, for every ε > there exit a τ > uch that t > τ implie I 4 < ε, that i, I 4 a t. Similarly, we can how that I 5 tend to zero t. Thi yield (T φ)(t) a t, and hence T : Cψ C ψ. Therefore, T i a contraction on Cψ with a unique fixed point x. By Theorem 1, x i a olution of IDE (1.1) on [, ). Hence, x(t) i the only continuou olution of IDE (1.1) agreeing with the initial function ψ. Since x Cψ, then x(t) a t. We now give an example to how the applicability of Theorem 3. Example. Let u conider the following integro -differential equation of firt order with two variable delay, which i a pecial cae of IDE (1.1): x (t) =.2t t 2 1 x(t).2 2 x()d, (1.12) 1 T

9 STABILITY OF A LINEAR INTEGRO-DIFFERENTIAL EQUATION where r 1 (t) =.385t and r 2 (t) =.476t. When we compare IDE (1.12) with IDE (1.1) and take into conideration the hypothee of Theorem 3, it can eaily be een that and Hence, we have G(t, ) = For the function b(t), we obtain b()d = 1 5 Hence, clearly, it follow that Thu, the hypothei (1.11) hold. We alo have b(t) =.2t t 2 1 a(t, ) = b(u) G(t, u) du = By an eay calculation, we can get t.2.2( t) 2 du = d = 1 1 ln(t2 1). 1 1 ln(t2 1) when t. µ 1 (t) =.2u.2(u t) u 2 1 u 2 1 du.4u.2t =.615t u 2 du 1 = µ 1 (t) µ 2 (t)..615t.4u t u 2 1.2u.615t u t.4u.2t u 2 du 1 =.2ln(u 2 1) t.615t.2t arctan u t.615t =.2ln(t 2 1).2ln( t 2 1).2t arctan t.2t arctan.615t =.2t[arctan.615t arctan t].2ln(t 2 1).2ln( t 2 1). By the ame way, we can calculate µ 2 and obtain µ 2 (t) =.2t[arctan.524t arctan t].2ln(t 2 1).2ln( t 2 1). It i obviou that both of thee function, that i, µ 1 and µ 2 are increaing in [, ). We now need to find that lim t µ 1(t) lim t µ 2 (t).

10 28 C. TUNÇ, İ. AKBULUT If we do the neceary calculation, then lim µ 1(t) = lim [.2[(.615/.615t2 1) (1 1/t 2 )] t t 1/t 2 t 2 (1 1/t 2 ).2 ln( t 2 ( /t 2 ) )] 1 = lim.2[ t 1 1/t ln(1/ )] t 2 =.2[1 1/ ln(.615)] = and lim µ 2(t) = lim [.2[(.524/.524t2 1) (1 1/t 2 )] t t 1/t 2 t 2 (1 1/t 2 ).2 ln( t 2 ( /t 2 ) )] 1 = lim.2[ t 1 1/t ln(1/ )] t 2 =.2[1 1/ ln(.524)] = Hence, we have and b(u) G(t, u) <.7.8 =.15, =.2(2 1/.615).2(2 1/.524) b() b(u) G(, u) dud <.15, r i() b()d) b( r i () G(, r i ())) 1 r i() d <.2[(2 1/.615)].2[(2 1/.524)] = <.1 2 u u 2 1 ) 2 1/.615t 2 d u u 2 1 ) 2 1/.524t 2 d b() d <.3, repectively. Let α = =.7 < 1. Hence, we can conclude that x(t) of IDE (1.12) i bounded on [ r, ) and the zero olution of IDE (1.12) i aymptotically table.

11 STABILITY OF A LINEAR INTEGRO-DIFFERENTIAL EQUATION Reference [1] Ardjouni, A., Djoudi, A., Stability in nonlinear neutral integro-differential equation with variable delay uing fixed point theory. J. Appl. Math. Comput. 44 (214),no.1-2, [2] Becker, L.C., Burton, T. A., Stability, fixed point and invere of delay. Proc. Roy. Soc. Edinburgh Sect. A 136 (26), no. 2, [3] Burton, T. A., Stability by fixed point theory or Liapunov theory: a comparion. Fixed Point Theory 4 (23), no. 1, [4] Burton, T. A., Fixed point and tability of a non-convolution equation. Proc. Amer. Math. Soc. 132 (24), no. 12, [5] Burton, T.A., Stability by fixed point theory for functional differential equation. Dover Publication, Mineola, New York, 26. [6] Gabi, H., Ardjouni, A., Djoudi, A., Fixed point and tability of a cla of nonlinear delay integro-differential equation with variable delay. Facta Univ. Ser. Math. Inform. 32 (217), no. 1, [7] Gözen, M., Tunç, C., Stability in functional integro-differential equation of econd order with variable delay. J. Math. Fundam. Sci. 49 (217), no. 1, [8] Graef, J. R., Tunç, C., Continuability and boundedne of multi-delay functional integrodifferential equation of the econd order. Rev. R. Acad. Cienc. Exacta F. Nat. Ser. A Math. RACSAM 19 (215), no. 1, [9] Jin, C., Luo, J., Stability of an integro-differential equation. Comput. Math. Appl. 57 (29), no. 7, [1] Levin, J. J., The aymptotic behavior of the olution of a Volterra equation. Proc. Amer. Math. Soc. 14 (1963) [11] Pi, D., Study the tability of olution of functional differential equation via fixed point. Nonlinear Anal.74 (211), no.2, [12] Pi, D., Stability condition of econd order integro-differential equation with variable delay. Abtr. Appl. Anal. 214, Art. ID , 11 pp. [13] Raffoul, Y. N., Stability in neutral nonlinear differential equation with functional delay uing fixed-point theory. Math. Comput. Modelling, 4 (24) no.7-8, [14] Rahman, M., Integral equation and their application. WIT Pre, Southampton, 217. [15] Tunç, C., A note on the qualitative behavior of non-linear Volterra integro-differential equation. J. Egyptian Math. Soc. 24 (216), no. 2, [16] Tunç, C., New tability and boundedne reult to Volterra integro-differential equation with delay. J. Egyptian Math. Soc. 24 (216), no. 2, [17] Tunç, C., Stability and boundedne in Volterra-integro differential equation with delay. Dynam. Sytem Appl.26 (217), no.1, [18] Tunç, C., Qualitative propertie in nonlinear Volterra integro-differential equation with delay. Journal of Taibah Univerity for Science 11 (217), no.2, [19] Tunç, C., On the qualitative behavior of a functional differential equation of econd order. Appl. Appl. Math. 12 (217), no. 2, [2] Tunç, C., Mohammed, S. A., On the tability and intability of functional Volterra integrodifferential equation of firt order. Bull. Math. Anal. Appl. 9 (217), no. 1, [21] Tunç, C., Tunç, O., On the exponential tudy of olution of Volterra integro-differential equation with time lag. Electron. J. Math. Anal. Appl., 6 (1), (218), [22] Tunç, C., Tunç, O., New reult on the tability, integrability and boundedne in Volterra integro-differential equation. Bull. Comput. Appl. Math., 6 (1),(218), [23] Tunç, C., Tunç, O., On behavior of functional Volterra integro-differential equation with multiple time-lag. Journal of Taibah Univerity for Science, 12 (2), (218), [24] Wazwaz, A. M., Linear and nonlinear integral equation. Method and application. Higher Education Pre, Beijing, Springer, Heidelberg, 211. Cemİl Tunç Department of Mathematic Faculty of Science Van Yuzuncu Yil Univerity 658, Van-Turkey addre: cemtunc@yahoo.com

12 3 C. TUNÇ, İ. AKBULUT İrem Akbulut Department of Mathematic Faculty of Education Siirt Univerity 561, Siirt-Turkey addre:

Research Article Fixed Points and Stability in Nonlinear Equations with Variable Delays

Research Article Fixed Points and Stability in Nonlinear Equations with Variable Delays Hindawi Publihing Corporation Fixed Point Theory and Application Volume 21, Article ID 195916, 14 page doi:1.1155/21/195916 Reearch Article Fixed Point and Stability in Nonlinear Equation with Variable

More information

On mild solutions of a semilinear mixed Volterra-Fredholm functional integrodifferential evolution nonlocal problem in Banach spaces

On mild solutions of a semilinear mixed Volterra-Fredholm functional integrodifferential evolution nonlocal problem in Banach spaces MAEMAIA, 16, Volume 3, Number, 133 14 c Penerbit UM Pre. All right reerved On mild olution of a emilinear mixed Volterra-Fredholm functional integrodifferential evolution nonlocal problem in Banach pace

More information

TRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL

TRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL GLASNIK MATEMATIČKI Vol. 38583, 73 84 TRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL p-laplacian Haihen Lü, Donal O Regan and Ravi P. Agarwal Academy of Mathematic and Sytem Science, Beijing, China, National

More information

A THEOREM OF ROLEWICZ S TYPE FOR MEASURABLE EVOLUTION FAMILIES IN BANACH SPACES

A THEOREM OF ROLEWICZ S TYPE FOR MEASURABLE EVOLUTION FAMILIES IN BANACH SPACES Electronic Journal of Differential Equation, Vol. 21(21, No. 7, pp. 1 5. ISSN: 172-6691. URL: http://ejde.math.wt.edu or http://ejde.math.unt.edu ftp ejde.math.wt.edu (login: ftp A THEOREM OF ROLEWICZ

More information

INITIAL VALUE PROBLEMS OF FRACTIONAL ORDER HADAMARD-TYPE FUNCTIONAL DIFFERENTIAL EQUATIONS

INITIAL VALUE PROBLEMS OF FRACTIONAL ORDER HADAMARD-TYPE FUNCTIONAL DIFFERENTIAL EQUATIONS Electronic Journal of Differential Equation, Vol. 205 205), No. 77, pp. 9. ISSN: 072-669. URL: http://ejde.math.txtate.edu or http://ejde.math.unt.edu ftp ejde.math.txtate.edu INITIAL VALUE PROBLEMS OF

More information

On Uniform Exponential Trichotomy of Evolution Operators in Banach Spaces

On Uniform Exponential Trichotomy of Evolution Operators in Banach Spaces On Uniform Exponential Trichotomy of Evolution Operator in Banach Space Mihail Megan, Codruta Stoica To cite thi verion: Mihail Megan, Codruta Stoica. On Uniform Exponential Trichotomy of Evolution Operator

More information

Research Article Existence for Nonoscillatory Solutions of Higher-Order Nonlinear Differential Equations

Research Article Existence for Nonoscillatory Solutions of Higher-Order Nonlinear Differential Equations International Scholarly Reearch Network ISRN Mathematical Analyi Volume 20, Article ID 85203, 9 page doi:0.502/20/85203 Reearch Article Exitence for Nonocillatory Solution of Higher-Order Nonlinear Differential

More information

INITIAL-VALUE PROBLEMS FOR HYBRID HADAMARD FRACTIONAL DIFFERENTIAL EQUATIONS

INITIAL-VALUE PROBLEMS FOR HYBRID HADAMARD FRACTIONAL DIFFERENTIAL EQUATIONS Electronic Journal of Differential Equation, Vol. 204 204, No. 6, pp. 8. ISSN: 072-669. URL: http://ejde.math.txtate.edu or http://ejde.math.unt.edu ftp ejde.math.txtate.edu INITIAL-VALUE PROBLEMS FOR

More information

A SIMPLE NASH-MOSER IMPLICIT FUNCTION THEOREM IN WEIGHTED BANACH SPACES. Sanghyun Cho

A SIMPLE NASH-MOSER IMPLICIT FUNCTION THEOREM IN WEIGHTED BANACH SPACES. Sanghyun Cho A SIMPLE NASH-MOSER IMPLICIT FUNCTION THEOREM IN WEIGHTED BANACH SPACES Sanghyun Cho Abtract. We prove a implified verion of the Nah-Moer implicit function theorem in weighted Banach pace. We relax the

More information

FOURIER SERIES AND PERIODIC SOLUTIONS OF DIFFERENTIAL EQUATIONS

FOURIER SERIES AND PERIODIC SOLUTIONS OF DIFFERENTIAL EQUATIONS FOURIER SERIES AND PERIODIC SOLUTIONS OF DIFFERENTIAL EQUATIONS Nguyen Thanh Lan Department of Mathematic Wetern Kentucky Univerity Email: lan.nguyen@wku.edu ABSTRACT: We ue Fourier erie to find a neceary

More information

Unbounded solutions of second order discrete BVPs on infinite intervals

Unbounded solutions of second order discrete BVPs on infinite intervals Available online at www.tjna.com J. Nonlinear Sci. Appl. 9 206), 357 369 Reearch Article Unbounded olution of econd order dicrete BVP on infinite interval Hairong Lian a,, Jingwu Li a, Ravi P Agarwal b

More information

Chapter 4. The Laplace Transform Method

Chapter 4. The Laplace Transform Method Chapter 4. The Laplace Tranform Method The Laplace Tranform i a tranformation, meaning that it change a function into a new function. Actually, it i a linear tranformation, becaue it convert a linear combination

More information

SOME RESULTS ON INFINITE POWER TOWERS

SOME RESULTS ON INFINITE POWER TOWERS NNTDM 16 2010) 3, 18-24 SOME RESULTS ON INFINITE POWER TOWERS Mladen Vailev - Miana 5, V. Hugo Str., Sofia 1124, Bulgaria E-mail:miana@abv.bg Abtract To my friend Kratyu Gumnerov In the paper the infinite

More information

MULTIPLE POSITIVE SOLUTIONS OF BOUNDARY VALUE PROBLEMS FOR P-LAPLACIAN IMPULSIVE DYNAMIC EQUATIONS ON TIME SCALES

MULTIPLE POSITIVE SOLUTIONS OF BOUNDARY VALUE PROBLEMS FOR P-LAPLACIAN IMPULSIVE DYNAMIC EQUATIONS ON TIME SCALES Fixed Point Theory, 5(24, No. 2, 475-486 http://www.math.ubbcluj.ro/ nodeacj/fptcj.html MULTIPLE POSITIVE SOLUTIONS OF BOUNDARY VALUE PROBLEMS FOR P-LAPLACIAN IMPULSIVE DYNAMIC EQUATIONS ON TIME SCALES

More information

PRINCIPAL MATRIX SOLUTIONS AND VARIATION OF PARAMETERS FOR A VOLTERRA INTEGRO-DIFFERENTIAL EQUATION AND ITS ADJOINT

PRINCIPAL MATRIX SOLUTIONS AND VARIATION OF PARAMETERS FOR A VOLTERRA INTEGRO-DIFFERENTIAL EQUATION AND ITS ADJOINT Electronic Journal of Qualitative Theory of Differential Equation 2006, No. 14, 1-22; http://www.math.u-zeged.hu/ejqtde/ PRINCIPAL MATRIX SOLUTIONS AND VARIATION OF PARAMETERS FOR A VOLTERRA INTEGRO-DIFFERENTIAL

More information

General System of Nonconvex Variational Inequalities and Parallel Projection Method

General System of Nonconvex Variational Inequalities and Parallel Projection Method Mathematica Moravica Vol. 16-2 (2012), 79 87 General Sytem of Nonconvex Variational Inequalitie and Parallel Projection Method Balwant Singh Thakur and Suja Varghee Abtract. Uing the prox-regularity notion,

More information

KERNEL-RESOLVENT RELATIONS FOR AN INTEGRAL EQUATION

KERNEL-RESOLVENT RELATIONS FOR AN INTEGRAL EQUATION Ø Ñ Å Ø Ñ Ø Ð ÈÙ Ð Ø ÓÒ DOI: 1.478/v117-11-3-7 Tatra Mt. Math. Publ. 48 (11), 5 4 KERNEL-RESOLVENT RELATIONS FOR AN INTEGRAL EQUATION Theodore A. Burton ABSTRACT. Weconideracalarintegralequationz(t) =

More information

TAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES

TAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES TAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES DOUGLAS R. ANDERSON Abtract. We are concerned with the repreentation of polynomial for nabla dynamic equation on time cale. Once etablihed,

More information

THE HAUSDORFF MEASURE OF SIERPINSKI CARPETS BASING ON REGULAR PENTAGON

THE HAUSDORFF MEASURE OF SIERPINSKI CARPETS BASING ON REGULAR PENTAGON Anal. Theory Appl. Vol. 28, No. (202), 27 37 THE HAUSDORFF MEASURE OF SIERPINSKI CARPETS BASING ON REGULAR PENTAGON Chaoyi Zeng, Dehui Yuan (Hanhan Normal Univerity, China) Shaoyuan Xu (Gannan Normal Univerity,

More information

February 5, :53 WSPC/INSTRUCTION FILE Mild solution for quasilinear pde

February 5, :53 WSPC/INSTRUCTION FILE Mild solution for quasilinear pde February 5, 14 1:53 WSPC/INSTRUCTION FILE Mild olution for quailinear pde Infinite Dimenional Analyi, Quantum Probability and Related Topic c World Scientific Publihing Company STOCHASTIC QUASI-LINEAR

More information

One Class of Splitting Iterative Schemes

One Class of Splitting Iterative Schemes One Cla of Splitting Iterative Scheme v Ciegi and V. Pakalnytė Vilniu Gedimina Technical Univerity Saulėtekio al. 11, 2054, Vilniu, Lithuania rc@fm.vtu.lt Abtract. Thi paper deal with the tability analyi

More information

ON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION. Xiaoqun Wang

ON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION. Xiaoqun Wang Proceeding of the 2008 Winter Simulation Conference S. J. Maon, R. R. Hill, L. Mönch, O. Roe, T. Jefferon, J. W. Fowler ed. ON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION Xiaoqun Wang

More information

Research Article A New Kind of Weak Solution of Non-Newtonian Fluid Equation

Research Article A New Kind of Weak Solution of Non-Newtonian Fluid Equation Hindawi Function Space Volume 2017, Article ID 7916730, 8 page http://doi.org/10.1155/2017/7916730 Reearch Article A New Kind of Weak Solution of Non-Newtonian Fluid Equation Huahui Zhan 1 and Bifen Xu

More information

EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR CAPUTO-HADAMARD SEQUENTIAL FRACTIONAL ORDER NEUTRAL FUNCTIONAL DIFFERENTIAL EQUATIONS

EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR CAPUTO-HADAMARD SEQUENTIAL FRACTIONAL ORDER NEUTRAL FUNCTIONAL DIFFERENTIAL EQUATIONS Electronic Journal of Differential Equation, Vol. 207 207), No. 36, pp.. ISSN: 072-669. URL: http://ejde.math.txtate.edu or http://ejde.math.unt.edu EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR CAPUTO-HADAMARD

More information

Beta Burr XII OR Five Parameter Beta Lomax Distribution: Remarks and Characterizations

Beta Burr XII OR Five Parameter Beta Lomax Distribution: Remarks and Characterizations Marquette Univerity e-publication@marquette Mathematic, Statitic and Computer Science Faculty Reearch and Publication Mathematic, Statitic and Computer Science, Department of 6-1-2014 Beta Burr XII OR

More information

OSCILLATIONS OF A CLASS OF EQUATIONS AND INEQUALITIES OF FOURTH ORDER * Zornitza A. Petrova

OSCILLATIONS OF A CLASS OF EQUATIONS AND INEQUALITIES OF FOURTH ORDER * Zornitza A. Petrova МАТЕМАТИКА И МАТЕМАТИЧЕСКО ОБРАЗОВАНИЕ, 2006 MATHEMATICS AND EDUCATION IN MATHEMATICS, 2006 Proceeding of the Thirty Fifth Spring Conference of the Union of Bulgarian Mathematician Borovet, April 5 8,

More information

Some Sets of GCF ϵ Expansions Whose Parameter ϵ Fetch the Marginal Value

Some Sets of GCF ϵ Expansions Whose Parameter ϵ Fetch the Marginal Value Journal of Mathematical Reearch with Application May, 205, Vol 35, No 3, pp 256 262 DOI:03770/jin:2095-26520503002 Http://jmredluteducn Some Set of GCF ϵ Expanion Whoe Parameter ϵ Fetch the Marginal Value

More information

A PROOF OF TWO CONJECTURES RELATED TO THE ERDÖS-DEBRUNNER INEQUALITY

A PROOF OF TWO CONJECTURES RELATED TO THE ERDÖS-DEBRUNNER INEQUALITY Volume 8 2007, Iue 3, Article 68, 3 pp. A PROOF OF TWO CONJECTURES RELATED TO THE ERDÖS-DEBRUNNER INEQUALITY C. L. FRENZEN, E. J. IONASCU, AND P. STĂNICĂ DEPARTMENT OF APPLIED MATHEMATICS NAVAL POSTGRADUATE

More information

Bogoliubov Transformation in Classical Mechanics

Bogoliubov Transformation in Classical Mechanics Bogoliubov Tranformation in Claical Mechanic Canonical Tranformation Suppoe we have a et of complex canonical variable, {a j }, and would like to conider another et of variable, {b }, b b ({a j }). How

More information

Hybrid Projective Dislocated Synchronization of Liu Chaotic System Based on Parameters Identification

Hybrid Projective Dislocated Synchronization of Liu Chaotic System Based on Parameters Identification www.ccenet.org/ma Modern Applied Science Vol. 6, No. ; February Hybrid Projective Dilocated Synchronization of Liu Chaotic Sytem Baed on Parameter Identification Yanfei Chen College of Science, Guilin

More information

Advanced D-Partitioning Analysis and its Comparison with the Kharitonov s Theorem Assessment

Advanced D-Partitioning Analysis and its Comparison with the Kharitonov s Theorem Assessment Journal of Multidiciplinary Engineering Science and Technology (JMEST) ISSN: 59- Vol. Iue, January - 5 Advanced D-Partitioning Analyi and it Comparion with the haritonov Theorem Aement amen M. Yanev Profeor,

More information

Computers and Mathematics with Applications. Sharp algebraic periodicity conditions for linear higher order

Computers and Mathematics with Applications. Sharp algebraic periodicity conditions for linear higher order Computer and Mathematic with Application 64 (2012) 2262 2274 Content lit available at SciVere ScienceDirect Computer and Mathematic with Application journal homepage: wwweleviercom/locate/camwa Sharp algebraic

More information

SOME MONOTONICITY PROPERTIES AND INEQUALITIES FOR

SOME MONOTONICITY PROPERTIES AND INEQUALITIES FOR Kragujevac Journal of Mathematic Volume 4 08 Page 87 97. SOME MONOTONICITY PROPERTIES AND INEQUALITIES FOR THE p k-gamma FUNCTION KWARA NANTOMAH FATON MEROVCI AND SULEMAN NASIRU 3 Abtract. In thi paper

More information

Dragomir and Gosa type inequalities on b-metric spaces

Dragomir and Gosa type inequalities on b-metric spaces Karapınar and Noorwali Journal of Inequalitie and Application http://doi.org/10.1186/13660-019-1979-9 (019) 019:9 RESEARCH Open Acce Dragomir and Goa type inequalitie on b-metric pace Erdal Karapınar1*

More information

Linear System Fundamentals

Linear System Fundamentals Linear Sytem Fundamental MEM 355 Performance Enhancement of Dynamical Sytem Harry G. Kwatny Department of Mechanical Engineering & Mechanic Drexel Univerity Content Sytem Repreentation Stability Concept

More information

New bounds for Morse clusters

New bounds for Morse clusters New bound for More cluter Tamá Vinkó Advanced Concept Team, European Space Agency, ESTEC Keplerlaan 1, 2201 AZ Noordwijk, The Netherland Tama.Vinko@ea.int and Arnold Neumaier Fakultät für Mathematik, Univerität

More information

Extension of Inagaki General Weighted Operators. and. A New Fusion Rule Class of Proportional Redistribution of Intersection Masses

Extension of Inagaki General Weighted Operators. and. A New Fusion Rule Class of Proportional Redistribution of Intersection Masses Extenion of nagaki General Weighted Operator and A New Fuion Rule Cla of Proportional Reditribution of nterection Mae Florentin Smarandache Chair of Math & Science Depart. Univerity of New Mexico, Gallup,

More information

Laplace Adomian Decomposition Method for Solving the Nonlinear Volterra Integral Equation with Weakly Kernels

Laplace Adomian Decomposition Method for Solving the Nonlinear Volterra Integral Equation with Weakly Kernels Studie in Nonlinear Science (4): 9-4, ISSN -9 IDOSI Publication, Laplace Adomian Decompoition Method for Solving the Nonlinear Volterra Integral Equation with Weakly Kernel F.A. Hendi Department of Mathematic

More information

An Inequality for Nonnegative Matrices and the Inverse Eigenvalue Problem

An Inequality for Nonnegative Matrices and the Inverse Eigenvalue Problem An Inequality for Nonnegative Matrice and the Invere Eigenvalue Problem Robert Ream Program in Mathematical Science The Univerity of Texa at Dalla Box 83688, Richardon, Texa 7583-688 Abtract We preent

More information

NULL HELIX AND k-type NULL SLANT HELICES IN E 4 1

NULL HELIX AND k-type NULL SLANT HELICES IN E 4 1 REVISTA DE LA UNIÓN MATEMÁTICA ARGENTINA Vol. 57, No. 1, 2016, Page 71 83 Publihed online: March 3, 2016 NULL HELIX AND k-type NULL SLANT HELICES IN E 4 1 JINHUA QIAN AND YOUNG HO KIM Abtract. We tudy

More information

Reliability Analysis of Embedded System with Different Modes of Failure Emphasizing Reboot Delay

Reliability Analysis of Embedded System with Different Modes of Failure Emphasizing Reboot Delay International Journal of Applied Science and Engineering 3., 4: 449-47 Reliability Analyi of Embedded Sytem with Different Mode of Failure Emphaizing Reboot Delay Deepak Kumar* and S. B. Singh Department

More information

CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS

CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.1 INTRODUCTION 8.2 REDUCED ORDER MODEL DESIGN FOR LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.3

More information

696 Fu Jing-Li et al Vol. 12 form in generalized coordinate Q ffiq dt = 0 ( = 1; ;n): (3) For nonholonomic ytem, ffiq are not independent of

696 Fu Jing-Li et al Vol. 12 form in generalized coordinate Q  ffiq dt = 0 ( = 1; ;n): (3) For nonholonomic ytem, ffiq are not independent of Vol 12 No 7, July 2003 cfl 2003 Chin. Phy. Soc. 1009-1963/2003/12(07)/0695-05 Chinee Phyic and IOP Publihing Ltd Lie ymmetrie and conerved quantitie of controllable nonholonomic dynamical ytem Fu Jing-Li(ΛΠ±)

More information

Multi-dimensional Fuzzy Euler Approximation

Multi-dimensional Fuzzy Euler Approximation Mathematica Aeterna, Vol 7, 2017, no 2, 163-176 Multi-dimenional Fuzzy Euler Approximation Yangyang Hao College of Mathematic and Information Science Hebei Univerity, Baoding 071002, China hdhyywa@163com

More information

Research Article Triple Positive Solutions of a Nonlocal Boundary Value Problem for Singular Differential Equations with p-laplacian

Research Article Triple Positive Solutions of a Nonlocal Boundary Value Problem for Singular Differential Equations with p-laplacian Abtract and Applied Analyi Volume 23, Article ID 63672, 7 page http://dx.doi.org/.55/23/63672 Reearch Article Triple Poitive Solution of a Nonlocal Boundary Value Problem for Singular Differential Equation

More information

POINCARE INEQUALITY AND CAMPANATO ESTIMATES FOR WEAK SOLUTIONS OF PARABOLIC EQUATIONS

POINCARE INEQUALITY AND CAMPANATO ESTIMATES FOR WEAK SOLUTIONS OF PARABOLIC EQUATIONS Electronic Journal of Differential Equation, Vol. 206 (206), No. 204, pp. 8. ISSN: 072-669. URL: http://ejde.math.txtate.edu or http://ejde.math.unt.edu POINCARE INEQUALITY AND CAMPANATO ESTIMATES FOR

More information

Stochastic Optimization with Inequality Constraints Using Simultaneous Perturbations and Penalty Functions

Stochastic Optimization with Inequality Constraints Using Simultaneous Perturbations and Penalty Functions Stochatic Optimization with Inequality Contraint Uing Simultaneou Perturbation and Penalty Function I-Jeng Wang* and Jame C. Spall** The John Hopkin Univerity Applied Phyic Laboratory 11100 John Hopkin

More information

Michał Kisielewicz SOME OPTIMAL CONTROL PROBLEMS FOR PARTIAL DIFFERENTIAL INCLUSIONS

Michał Kisielewicz SOME OPTIMAL CONTROL PROBLEMS FOR PARTIAL DIFFERENTIAL INCLUSIONS Opucula Mathematica Vol. 28 No. 4 28 Dedicated to the memory of Profeor Andrzej Laota Michał Kiielewicz SOME OPTIMAL CONTROL PROBLEMS FOR PARTIAL DIFFERENTIAL INCLUSIONS Abtract. Partial differential incluion

More information

Characterizations of Type-2 Harmonic Curvatures and General Helices in Euclidean space E⁴ Faik Babadag

Characterizations of Type-2 Harmonic Curvatures and General Helices in Euclidean space E⁴ Faik Babadag Characterization of Type-2 Harmonic Curvature and General Helice in Euclidean pace E⁴ Faik Babadag Department of MATHEMATICS, KIRIKKALE Univerity, KIRIKKALE Email: faik.babadag@kku.edu.tr Abtract In thi

More information

INEQUALITIES FOR THE NUMERICAL RADIUS IN UNITAL NORMED ALGEBRAS

INEQUALITIES FOR THE NUMERICAL RADIUS IN UNITAL NORMED ALGEBRAS INEQUALITIES FOR THE NUMERICAL RADIUS IN UNITAL NORMED ALGEBRAS S.S. DRAGOMIR Abtract. In thi paper, ome ineualitie between the numerical radiu of an element from a unital normed algebra and certain emi-inner

More information

Approximate Analytical Solution for Quadratic Riccati Differential Equation

Approximate Analytical Solution for Quadratic Riccati Differential Equation Iranian J. of Numerical Analyi and Optimization Vol 3, No. 2, 2013), pp 21-31 Approximate Analytical Solution for Quadratic Riccati Differential Equation H. Aminikhah Abtract In thi paper, we introduce

More information

Dipartimento di Matematica

Dipartimento di Matematica Dipartimento di Matematica P. Bonicatto, L. Luardi Analyi of an integral equation ariing from a variational problem Rapporto interno N. 5, luglio 29 Politecnico di Torino Coro Duca degli Abruzzi, 24-29

More information

Given the following circuit with unknown initial capacitor voltage v(0): X(s) Immediately, we know that the transfer function H(s) is

Given the following circuit with unknown initial capacitor voltage v(0): X(s) Immediately, we know that the transfer function H(s) is EE 4G Note: Chapter 6 Intructor: Cheung More about ZSR and ZIR. Finding unknown initial condition: Given the following circuit with unknown initial capacitor voltage v0: F v0/ / Input xt 0Ω Output yt -

More information

The combined Laplace-homotopy analysis method for partial differential equations

The combined Laplace-homotopy analysis method for partial differential equations Available online at wwwir-publicationcom/jmc J Math Computer Sci 6 (26), 88 2 Reearch Article The combined Laplace-homotopy analyi method for partial differential equation Javad Vahidi Department of Mathematic,

More information

Representation Formulas of Curves in a Two- and Three-Dimensional Lightlike Cone

Representation Formulas of Curves in a Two- and Three-Dimensional Lightlike Cone Reult. Math. 59 (011), 437 451 c 011 Springer Bael AG 14-6383/11/030437-15 publihed online April, 011 DOI 10.1007/0005-011-0108-y Reult in Mathematic Repreentation Formula of Curve in a Two- and Three-Dimenional

More information

arxiv: v1 [math.mg] 25 Aug 2011

arxiv: v1 [math.mg] 25 Aug 2011 ABSORBING ANGLES, STEINER MINIMAL TREES, AND ANTIPODALITY HORST MARTINI, KONRAD J. SWANEPOEL, AND P. OLOFF DE WET arxiv:08.5046v [math.mg] 25 Aug 20 Abtract. We give a new proof that a tar {op i : i =,...,

More information

Manprit Kaur and Arun Kumar

Manprit Kaur and Arun Kumar CUBIC X-SPLINE INTERPOLATORY FUNCTIONS Manprit Kaur and Arun Kumar manpreet2410@gmail.com, arun04@rediffmail.com Department of Mathematic and Computer Science, R. D. Univerity, Jabalpur, INDIA. Abtract:

More information

Center Manifolds Optimal Regularity for Nonuniformly Hyperbolic Dynamics 1

Center Manifolds Optimal Regularity for Nonuniformly Hyperbolic Dynamics 1 São Paulo Journal of Mathematical Science 5, 1 (2011), 1 22 Center Manifold Optimal Regularity for Nonuniformly Hyperbolic Dynamic 1 Lui Barreira and Claudia Vall Abtract. For ufficiently mall perturbation

More information

Convex Hulls of Curves Sam Burton

Convex Hulls of Curves Sam Burton Convex Hull of Curve Sam Burton 1 Introduction Thi paper will primarily be concerned with determining the face of convex hull of curve of the form C = {(t, t a, t b ) t [ 1, 1]}, a < b N in R 3. We hall

More information

IEOR 3106: Fall 2013, Professor Whitt Topics for Discussion: Tuesday, November 19 Alternating Renewal Processes and The Renewal Equation

IEOR 3106: Fall 2013, Professor Whitt Topics for Discussion: Tuesday, November 19 Alternating Renewal Processes and The Renewal Equation IEOR 316: Fall 213, Profeor Whitt Topic for Dicuion: Tueday, November 19 Alternating Renewal Procee and The Renewal Equation 1 Alternating Renewal Procee An alternating renewal proce alternate between

More information

WELL-POSEDNESS OF A ONE-DIMENSIONAL PLASMA MODEL WITH A HYPERBOLIC FIELD

WELL-POSEDNESS OF A ONE-DIMENSIONAL PLASMA MODEL WITH A HYPERBOLIC FIELD WELL-POSEDNESS OF A ONE-DIMENSIONAL PLASMA MODEL WITH A HYPERBOLIC FIELD JENNIFER RAE ANDERSON 1. Introduction A plama i a partially or completely ionized ga. Nearly all (approximately 99.9%) of the matter

More information

Chapter 7. Root Locus Analysis

Chapter 7. Root Locus Analysis Chapter 7 Root Locu Analyi jw + KGH ( ) GH ( ) - K 0 z O 4 p 2 p 3 p Root Locu Analyi The root of the cloed-loop characteritic equation define the ytem characteritic repone. Their location in the complex

More information

Minimizing movements along a sequence of functionals and curves of maximal slope

Minimizing movements along a sequence of functionals and curves of maximal slope Minimizing movement along a equence of functional and curve of maximal lope Andrea Braide Dipartimento di Matematica, Univerità di Roma Tor Vergata via della ricerca cientifica 1, 133 Roma, Italy Maria

More information

Math 273 Solutions to Review Problems for Exam 1

Math 273 Solutions to Review Problems for Exam 1 Math 7 Solution to Review Problem for Exam True or Fale? Circle ONE anwer for each Hint: For effective tudy, explain why if true and give a counterexample if fale (a) T or F : If a b and b c, then a c

More information

Gain and Phase Margins Based Delay Dependent Stability Analysis of Two- Area LFC System with Communication Delays

Gain and Phase Margins Based Delay Dependent Stability Analysis of Two- Area LFC System with Communication Delays Gain and Phae Margin Baed Delay Dependent Stability Analyi of Two- Area LFC Sytem with Communication Delay Şahin Sönmez and Saffet Ayaun Department of Electrical Engineering, Niğde Ömer Halidemir Univerity,

More information

Lecture 21. The Lovasz splitting-off lemma Topics in Combinatorial Optimization April 29th, 2004

Lecture 21. The Lovasz splitting-off lemma Topics in Combinatorial Optimization April 29th, 2004 18.997 Topic in Combinatorial Optimization April 29th, 2004 Lecture 21 Lecturer: Michel X. Goeman Scribe: Mohammad Mahdian 1 The Lovaz plitting-off lemma Lovaz plitting-off lemma tate the following. Theorem

More information

Lecture 10 Filtering: Applied Concepts

Lecture 10 Filtering: Applied Concepts Lecture Filtering: Applied Concept In the previou two lecture, you have learned about finite-impule-repone (FIR) and infinite-impule-repone (IIR) filter. In thee lecture, we introduced the concept of filtering

More information

6. KALMAN-BUCY FILTER

6. KALMAN-BUCY FILTER 6. KALMAN-BUCY FILTER 6.1. Motivation and preliminary. A wa hown in Lecture 2, the optimal control i a function of all coordinate of controlled proce. Very often, it i not impoible to oberve a controlled

More information

A CATEGORICAL CONSTRUCTION OF MINIMAL MODEL

A CATEGORICAL CONSTRUCTION OF MINIMAL MODEL A ATEGORIAL ONSTRUTION OF MINIMAL MODEL A. Behera, S. B. houdhury M. Routaray Department of Mathematic National Intitute of Technology ROURKELA - 769008 (India) abehera@nitrkl.ac.in 512ma6009@nitrkl.ac.in

More information

Asymptotic behavior of solutions of mixed problem for linear thermo-elastic systems with microtemperatures

Asymptotic behavior of solutions of mixed problem for linear thermo-elastic systems with microtemperatures Mathematica Aeterna, Vol. 8, 18, no. 4, 7-38 Aymptotic behavior of olution of mixed problem for linear thermo-elatic ytem with microtemperature Gulhan Kh. Shafiyeva Baku State Univerity Intitute of Mathematic

More information

Control Systems Analysis and Design by the Root-Locus Method

Control Systems Analysis and Design by the Root-Locus Method 6 Control Sytem Analyi and Deign by the Root-Locu Method 6 1 INTRODUCTION The baic characteritic of the tranient repone of a cloed-loop ytem i cloely related to the location of the cloed-loop pole. If

More information

L 2 -transforms for boundary value problems

L 2 -transforms for boundary value problems Computational Method for Differential Equation http://cmde.tabrizu.ac.ir Vol. 6, No., 8, pp. 76-85 L -tranform for boundary value problem Arman Aghili Department of applied mathematic, faculty of mathematical

More information

On the regularity to the solutions of the Navier Stokes equations via one velocity component

On the regularity to the solutions of the Navier Stokes equations via one velocity component On the regularity to the olution of the Navier Stoke equation via one velocity component Milan Pokorný and Yong Zhou. Mathematical Intitute of Charle Univerity, Sokolovká 83, 86 75 Praha 8, Czech Republic

More information

Simple Observer Based Synchronization of Lorenz System with Parametric Uncertainty

Simple Observer Based Synchronization of Lorenz System with Parametric Uncertainty IOSR Journal of Electrical and Electronic Engineering (IOSR-JEEE) ISSN: 78-676Volume, Iue 6 (Nov. - Dec. 0), PP 4-0 Simple Oberver Baed Synchronization of Lorenz Sytem with Parametric Uncertainty Manih

More information

STOCHASTIC EVOLUTION EQUATIONS WITH RANDOM GENERATORS. By Jorge A. León 1 and David Nualart 2 CINVESTAV-IPN and Universitat de Barcelona

STOCHASTIC EVOLUTION EQUATIONS WITH RANDOM GENERATORS. By Jorge A. León 1 and David Nualart 2 CINVESTAV-IPN and Universitat de Barcelona The Annal of Probability 1998, Vol. 6, No. 1, 149 186 STOCASTIC EVOLUTION EQUATIONS WIT RANDOM GENERATORS By Jorge A. León 1 and David Nualart CINVESTAV-IPN and Univeritat de Barcelona We prove the exitence

More information

Robustness analysis for the boundary control of the string equation

Robustness analysis for the boundary control of the string equation Routne analyi for the oundary control of the tring equation Martin GUGAT Mario SIGALOTTI and Mariu TUCSNAK I INTRODUCTION AND MAIN RESULTS In thi paper we conider the infinite dimenional ytem determined

More information

ON THE SMOOTHNESS OF SOLUTIONS TO A SPECIAL NEUMANN PROBLEM ON NONSMOOTH DOMAINS

ON THE SMOOTHNESS OF SOLUTIONS TO A SPECIAL NEUMANN PROBLEM ON NONSMOOTH DOMAINS Journal of Pure and Applied Mathematic: Advance and Application Volume, umber, 4, Page -35 O THE SMOOTHESS OF SOLUTIOS TO A SPECIAL EUMA PROBLEM O OSMOOTH DOMAIS ADREAS EUBAUER Indutrial Mathematic Intitute

More information

THE MAXIMAL OPERATOR ON GENERALIZED ORLICZ SPACES

THE MAXIMAL OPERATOR ON GENERALIZED ORLICZ SPACES THE MAXIMAL OPERATOR ON GENERALIZED ORLICZ SPACES PETER A. HÄSTÖ ASTRACT. In thi note I preent a ufficient condition for the boundedne of the maximal operator on generalized Orlicz pace. The reult include

More information

EFFECT ON PERSISTENCE OF INTRA-SPECIFIC COMPETITION IN COMPETITION MODELS

EFFECT ON PERSISTENCE OF INTRA-SPECIFIC COMPETITION IN COMPETITION MODELS Electronic Journal of Differential Equation, Vol. 2007(2007, No. 25, pp. 0. ISSN: 072-669. URL: http://ejde.math.txtate.edu or http://ejde.math.unt.edu ftp ejde.math.txtate.edu (login: ftp EFFECT ON PERSISTENCE

More information

Convergence of an Approach for Solving Fredholm Functional Integral Equations

Convergence of an Approach for Solving Fredholm Functional Integral Equations Iranian Journal of Mathematical Science and Informatic Vol. 11, No. 1 (2016), pp 35-46 DOI: 10.7508/imi.2016.01.004 Convergence of an Approach for Solving Fredholm Functional Integral Equation Naer Aghazadeh,

More information

NORMAL MODE ANALYSIS OF SECOND-ORDER PROJECTION METHODS FOR INCOMPRESSIBLE FLOWS. Jae-Hong Pyo and Jie Shen. (Communicated by Z.

NORMAL MODE ANALYSIS OF SECOND-ORDER PROJECTION METHODS FOR INCOMPRESSIBLE FLOWS. Jae-Hong Pyo and Jie Shen. (Communicated by Z. DISCRETE AND CONTINUOUS Webite: http://aimcience.org DYNAMICAL SYSTEMS SERIES B Volume 5 Number 3 Augut 005 pp. 817 840 NORMAL MODE ANALYSIS OF SECOND-ORDER PROJECTION METHODS FOR INCOMPRESSIBLE FLOWS

More information

REVERSE HÖLDER INEQUALITIES AND INTERPOLATION

REVERSE HÖLDER INEQUALITIES AND INTERPOLATION REVERSE HÖLDER INEQUALITIES AND INTERPOLATION J. BASTERO, M. MILMAN, AND F. J. RUIZ Abtract. We preent new method to derive end point verion of Gehring Lemma uing interpolation theory. We connect revere

More information

Lecture 17: Analytic Functions and Integrals (See Chapter 14 in Boas)

Lecture 17: Analytic Functions and Integrals (See Chapter 14 in Boas) Lecture 7: Analytic Function and Integral (See Chapter 4 in Boa) Thi i a good point to take a brief detour and expand on our previou dicuion of complex variable and complex function of complex variable.

More information

Hyperbolic Partial Differential Equations

Hyperbolic Partial Differential Equations Hyperbolic Partial Differential Equation Evolution equation aociated with irreverible phyical procee like diffuion heat conduction lead to parabolic partial differential equation. When the equation i a

More information

Analysis of Step Response, Impulse and Ramp Response in the Continuous Stirred Tank Reactor System

Analysis of Step Response, Impulse and Ramp Response in the Continuous Stirred Tank Reactor System ISSN: 454-50 Volume 0 - Iue 05 May 07 PP. 7-78 Analyi of Step Repone, Impule and Ramp Repone in the ontinuou Stirred Tank Reactor Sytem * Zohreh Khohraftar, Pirouz Derakhhi, (Department of hemitry, Science

More information

AN EXAMPLE FOR THE GENERALIZATION OF THE INTEGRATION OF SPECIAL FUNCTIONS BY USING THE LAPLACE TRANSFORM

AN EXAMPLE FOR THE GENERALIZATION OF THE INTEGRATION OF SPECIAL FUNCTIONS BY USING THE LAPLACE TRANSFORM Journal of Inequalitie Special Function ISSN: 7-433, URL: http://www.iliria.com Volume 6 Iue 5, Page 5-3. AN EXAMPLE FOR THE GENERALIZATION OF THE INTEGRATION OF SPECIAL FUNCTIONS BY USING THE LAPLACE

More information

Existence of Countably Many Positive Solutions for Nonlinear Boundary Value Problems on Time Scales

Existence of Countably Many Positive Solutions for Nonlinear Boundary Value Problems on Time Scales Appl. Math. Inf. Sci. 8, No. 5, 77-87 4 77 Applied Mathematic & Information Science An International Journal http://dx.doi.org/.785/ami/85 Exitence of Countably Many Poitive Solution for Nonlinear Boundary

More information

MATEMATIK Datum: Tid: eftermiddag. A.Heintz Telefonvakt: Anders Martinsson Tel.:

MATEMATIK Datum: Tid: eftermiddag. A.Heintz Telefonvakt: Anders Martinsson Tel.: MATEMATIK Datum: 20-08-25 Tid: eftermiddag GU, Chalmer Hjälpmedel: inga A.Heintz Telefonvakt: Ander Martinon Tel.: 073-07926. Löningar till tenta i ODE och matematik modellering, MMG5, MVE6. Define what

More information

INTEGRAL CHARACTERIZATIONS FOR TIMELIKE AND SPACELIKE CURVES ON THE LORENTZIAN SPHERE S *

INTEGRAL CHARACTERIZATIONS FOR TIMELIKE AND SPACELIKE CURVES ON THE LORENTZIAN SPHERE S * Iranian Journal of Science & echnology ranaction A Vol No A Printed in he Ilamic epublic of Iran 8 Shiraz Univerity INEGAL CHAACEIZAIONS FO IMELIKE AND SPACELIKE CUVES ON HE LOENZIAN SPHEE S * M KAZAZ

More information

Weber Schafheitlin-type integrals with exponent 1

Weber Schafheitlin-type integrals with exponent 1 Integral Tranform and Special Function Vol., No., February 9, 47 53 Weber Schafheitlin-type integral with exponent Johanne Kellendonk* and Serge Richard Univerité de Lyon, Univerité Lyon, Intitut Camille

More information

A Constraint Propagation Algorithm for Determining the Stability Margin. The paper addresses the stability margin assessment for linear systems

A Constraint Propagation Algorithm for Determining the Stability Margin. The paper addresses the stability margin assessment for linear systems A Contraint Propagation Algorithm for Determining the Stability Margin of Linear Parameter Circuit and Sytem Lubomir Kolev and Simona Filipova-Petrakieva Abtract The paper addree the tability margin aement

More information

CHAPTER 4 DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL

CHAPTER 4 DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL 98 CHAPTER DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL INTRODUCTION The deign of ytem uing tate pace model for the deign i called a modern control deign and it i

More information

ON ASYMPTOTIC FORMULA OF THE PARTITION FUNCTION p A (n)

ON ASYMPTOTIC FORMULA OF THE PARTITION FUNCTION p A (n) #A2 INTEGERS 15 (2015) ON ASYMPTOTIC FORMULA OF THE PARTITION FUNCTION p A (n) A David Chritopher Department of Mathematic, The American College, Tamilnadu, India davchrame@yahoocoin M Davamani Chritober

More information

(3) A bilinear map B : S(R n ) S(R m ) B is continuous (for the product topology) if and only if there exist C, N and M such that

(3) A bilinear map B : S(R n ) S(R m ) B is continuous (for the product topology) if and only if there exist C, N and M such that The material here can be found in Hörmander Volume 1, Chapter VII but he ha already done almot all of ditribution theory by thi point(!) Johi and Friedlander Chapter 8. Recall that S( ) i a complete metric

More information

Delay-Dependent Stability Criteria for Linear Time-Delay System of Neutral Type

Delay-Dependent Stability Criteria for Linear Time-Delay System of Neutral Type World Academy of Science Engineering and Technology Vol:4 No:1 1 Delay-Dependent Stability Criteria for Linear Time-Delay Sytem of Neutral Type Myeongjin Park Ohmin Kwon Juhyun Park and Sangmoon Lee International

More information

Invariance of a Partial Differential Equation of Fractional Order under the Lie Group of Scaling Transformations

Invariance of a Partial Differential Equation of Fractional Order under the Lie Group of Scaling Transformations JOURNAL OF MATHEMATICAL ANALYSIS AND APPLICATIONS 7, 8197 1998 ARTICLE NO AY986078 Invariance of a Partial Differential Equation of Fractional Order under the Lie Group of Scaling Tranformation Evelyn

More information

Flag-transitive non-symmetric 2-designs with (r, λ) = 1 and alternating socle

Flag-transitive non-symmetric 2-designs with (r, λ) = 1 and alternating socle Flag-tranitive non-ymmetric -deign with (r, λ = 1 and alternating ocle Shenglin Zhou, Yajie Wang School of Mathematic South China Univerity of Technology Guangzhou, Guangdong 510640, P. R. China lzhou@cut.edu.cn

More information

ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS. Volker Ziegler Technische Universität Graz, Austria

ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS. Volker Ziegler Technische Universität Graz, Austria GLASNIK MATEMATIČKI Vol. 1(61)(006), 9 30 ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS Volker Ziegler Techniche Univerität Graz, Autria Abtract. We conider the parameterized Thue

More information

Standard Guide for Conducting Ruggedness Tests 1

Standard Guide for Conducting Ruggedness Tests 1 Deignation: E 69 89 (Reapproved 996) Standard Guide for Conducting Ruggedne Tet AMERICA SOCIETY FOR TESTIG AD MATERIALS 00 Barr Harbor Dr., Wet Conhohocken, PA 948 Reprinted from the Annual Book of ASTM

More information

On the Exact Value of Packing Spheres in a Class of Orlicz Function Spaces

On the Exact Value of Packing Spheres in a Class of Orlicz Function Spaces Jornal of Convex Analyi Volme 2004), No. 2, 39 400 On the Exact Vale of Packing Sphere in a Cla of Orlicz Fnction Space Received Jne 30, 2003 Revied mancript received October 6, 2003 Ya Qiang Yan Department

More information