The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales
|
|
- Kathlyn King
- 5 years ago
- Views:
Transcription
1 Advances in Dynamical Sysems and Applicaions. ISSN Volume 1 Number 1 (2006, pp c Research India Publicaions hp:// The Asympoic Behavior of Nonoscillaory Soluions of Some Nonlinear Dynamic Equaions on Time Scales Xiangyun Shi 1, Xueyong Zhou 1 and Weiping Yan 2 1 Deparmen of Mahemaics, Xinyang Normal Universiy, Xinyang , Henan, P.R. China Corresponding auhor: xiangyunshi@126.com 2 Deparmen of Mahemaics, Shanxi Universiy, Taiyuan , Shanxi, P.R. China Absrac In his paper, he asympoic behavior of nonoscillaory soluions of he nonlinear dynamic equaion on ime scales r(g(y ( ] f(, y( = 0, 0 is considered under he condiion 0 ( m1 = for m 1 0. r( Three sufficien and necessary condiions are obained, which include and improve M.R.S. Kulenović and Ć. Ljubović s recen resuls in he coninuous case 5] and provide some new resuls in he discree case, as well as oher more general siuaions. AMS subjec classificaion: 39A10. Keywords: Time scales, dynamic equaion, asympoic behavior, nonoscillaory soluions. Received December 15, 2005; Acceped March 12, 2006
2 104 Xiangyun Shi, Xueyong Zhou and Weiping Yan 1. Inroducion The sudy of dynamic equaions on ime scales is an area of mahemaics ha recenly has received a lo of aenion. I has been creaed in order o unify he sudy of differenial equaions and difference equaions, and we refer he reader o he paper 3] for a comprehensive reamen of he subjec. Much recen research has been given o he asympoic properies of soluions of differenial equaion r(g(y ( ] p(f(y( = 0, R. We refer he reader o he papers 4, 5]. Bu i s discree counerpar r(g( y( ] p(f(y( = 0, N has few resuls. In his paper, we consider he dynamic equaion r(g(y ( ] f(, y( = 0, 0 (1.1 under he condiions (A 1 r C 1 rd (0,, (0, ]. (A 2 f C(T R, R, f is coninuously increasing wih respec o he second variable and yf(, y > 0, for y 0. (A 3 g C 1 R, R], g is a sricly increasing differeniable funcion on R and yg(y > 0, for y 0. If T = R, f(, y( = p(y(, hen equaion (1.1 reduces o he differenial equaion in 5]. If T = N, he difference equaion r(g( y( ] f(, y( = 0, N is anoher special case of (1.1. The aim of his paper, on he one hand, is o revisi he proofs of all heorems in 5] which use he Knaser Tarski fixed-poin heorem under decreasing mapping, on he oher hand, is o exend he resuls ha we have obained o he discree case as well as o more general siuaions. The paper is organized as follows: In he nex secion we presen some basic definiions concerning he calculus on ime scales. In Secion 3, we give hree sufficien and necessary condiions for he asympoic behavior of every nonoscillaory soluion of (1.1. In he final secion, we also apply our resuls o discree sysems by wo examples.
3 Nonoscillaory Soluions of Some Nonlinear Dynamic Equaions Some Definiions on Time Scales A ime scale T is an arbirary nonempy closed subse of real numbers R. Assume ha T has he opology ha i inheris from he sandard opology on R. We define he forward and backward jump operaors σ, ρ : T T by σ( := inf{s T : s > } and ρ( := inf{s T : s < }. The poin T is called righ-scaered, righ-dense, lef-scaered, lef-dense if σ( >, σ( =, ρ( <, ρ( = holds, respecively. The se T κ is derived from he ime scale T as follows. If T has a lef-scaered maximum, hen T κ = T { }. Oherwise, T κ = T. For a, b T wih a b, define he closed inerval a, b] in T by a, b] = { T : a b}. Oher open, half-open inervals in T can be similarly defined. Definiion 2.1. If f : T R is a funcion and T κ, hen he -derivaive of f a he poin is defined o be he number f ( wih he propery ha for each ɛ > 0, here is a neighborhood U of such ha (f(σ( f(s f ((σ( s ɛ σ( s for all s U. The funcion f is called -differeniable on T if f ( exiss for all T κ. Definiion 2.2. If F = f holds on T κ, hen we define he inegral of f by s f(τ τ = F ( F (s, s, T κ. We refer o 1,2,6] for addiional deails concerning he calculus on ime scales. By a soluion of (1.1, we mean a nonrivial real valued funcion x saisfying equaion (1.1 for 0. A soluion x of (1.1 is said o be oscillaory if i is neiher evenually posiive nor negaive; oherwise, i is nonoscillaory. 3. Main Resuls and Proof The following resul provides useful informaion on he global asympoic behavior of nonoscillaory soluions of (1.1. Lemma 3.1. Le (A 1 (A 3 be saisfied. If ( (A 4 m1 r( = for m 1 0 0
4 106 Xiangyun Shi, Xueyong Zhou and Weiping Yan holds, hen every soluion y of (1.1 evenually saisfies eiher y( K 1 or y( ( K 2 + M1 s, where K 1, K 2 and M 1 are posiive consans. Furhermore, r(s every posiive (negaive nondecreasing (nonincreasing soluion ends o + (. Proof. Wihou loss of generaliy, we can assume y( > 0 evenually, ha is y( > 0 for 1 0. Equaion (1.1 implies r(g(y ( ] > 0 for 1. Then here exiss 2 > 1 such ha r(g(y ( has consan sign for 2. If r(g(y ( < 0 for 2, hen (A 1 and (A 3 imply y ( < 0 for 2, ha is, y( is an evenually posiive decreasing funcion, so here exis consans K 1 > 0 and 3 2 such ha y( K 1 for 3. If r(g(y ( > 0 for 2, hen y ( > 0 for 2. Now, r(g(y ( is an evenually posiive increasing funcion, so here exis consans M 1 ( > 0, and 2 such ha r(g(y ( M 1 holds for. Then y ( M1 holds for. Inegraing his inequaliy from r( o > we obain The proof is complee. y( y( + ( M1 s, y( = K 2 > 0. r(s Now we are ready o presen he main resuls of his paper. Theorem 3.2. Assume ha (A 1 (A 4 hold. Then every, in absolue value, nondecreasing soluion y of (1.1 saisfies lim y( <, if and only if here exiss a consan C 0 such ha ( 1 f(s, C s <. (3.1 0 r( 0 Proof. Wihou loss of generaliy, we can suppose ha y( > 0 evenually. Firs assume ha (3.1 holds. Then 0 and C > 0 can be chosen such ha ( 1 f(s, C s C r( 2. If we can prove ha y is he soluion of he dynamic equaion y( = C ( 1 s 2 + f(u, y(u u s, r(s hen we can see ha y is he desired soluion of (1.1. Now we consruc he sequence {x m }: x 0 ( = C 2, x m ( = C ( r(s f(u, x m 1 (u u s, m = 1, 2. s
5 Nonoscillaory Soluions of Some Nonlinear Dynamic Equaions 107 Thus C 2 x 0 x 1 x 2 x m 1 x m C. Then he limi of he sequence {x m } exiss. We denoe i by x, i.e., Furher, lim x m( = x (. m f(s, x m f(s, C, ( 1 f(s, x m s C r( 2 hold. By Lebesgue s dominaed convergence heorem, we have lim x m( = C ( 1 s m 2 + f(u, lim r(s x m 1(u u s. T m 0 Tha is, x ( = C ( r(s f(u, x (u u s. So x saisfies (1.1. Furhermore, he limi of x ( as exiss. Conversely, le y > 0 be a bounded nondecreasing soluion of (1.1. Then s lim y( = m (0,. Le 0 be such ha y( m 2 for. Inegraing (1.1 from o we have which yields r( g(y ( = r( g(y ( + f(s, y(s s ( s, m s, 2 f f(s, y(s s ( 1 ( y ( f s, m s. r( 2 Inegraing his inequaliy from o >, and leing, we obain ( 1 ( s, m s <. r( 2 f The proof is complee.
6 108 Xiangyun Shi, Xueyong Zhou and Weiping Yan The nex resul gives a characerizaion of anoher ype of asympoic soluion. Theorem 3.3. If (A 1 (A 4 are saisfied, g(y = y α, for every y 0, α = p q (p, q are boh odd (3.2 and α > 1, hen equaion (1.1 has an, in absolue value, nondecreasing soluion y, such ha y( MR(, 0, for some consan M > 1, if and only if f(, ±mr(, 0 < (3.3 for some m > 1, where R(, 0 = 0 0 ( 1 s. r(s Proof. Wihou loss of generaliy, we assume y( > 0 evenually. Firs assume (3.3 holds. Then we can find m 1 > 0, 0 such ha f(, mr(, m 1, and (1 + m 1 1/α m. If we can prove ha y is he soluion of he dynamic equaion ( 1 y( = r(s + 1 s f(u, y(u u s, r(s hen we can see ha he funcion y is a nondecreasing soluion of (1.1. Now we consruc he sequence {x m }: Then x 0 = R(,, ( 1 x m = r(s + 1 r(s f(u, x m 1 (u u s. s R(, x 0 x 1 x m 1 x m mr(,. Obviously, he limi of he sequence {x m } exiss. We denoe i by x. Applying Lebesgue s dominaed convergence heorem, we have ( 1 x ( = r(s + 1 s f(u, x (u u s. r(s Then y saisfies (3.1 and when, y( mr(, 0. Conversely, if y( > 0, 1 0, le y be a nondecreasing soluion wih he propery lim y( = MR(, 0. Then here exiss L > 0 such ha MR(, 0 y( LR(, 0, and r(g(y ( > 0.
7 Nonoscillaory Soluions of Some Nonlinear Dynamic Equaions 109 We will show ha lim r(g(y ( <. Obviously, he limi exiss because r(g(y ( is an evenually posiive and increasing funcion. If lim r(g(y ( =, hen ( here exiss such ha r(g(y ( > M for. This implies y ( M and y( M 1/α R(, 0, and consequenly, r( y( R(, 0 M 1/α > M, which is a conradicion. Therefore, he limi of r(g(y ( exiss, say m, and we have 2m r(g(y ( = r( g(y ( + f(s, LR(s, s 0 s, which shows ha (3.3 is saisfied. The proof is complee. f(s, y(s s Remark 3.4. If T = R, hen y( = O(R(, 0, ha is, y( and R(, 0 are infiniy of he same order. Nex we characerize bounded soluions under he condiion (A 4. Theorem 3.5. Consider (1.1 under condiions (A 1 (A 4 and (3.2. Le y be an, in absolue value, nonincreasing soluion of (1.1. Then lim y( = K (0, if and only if here is a consan C 0 such ha ( 1 f(s, C s r( <. (3.4 0 Proof. Wihou loss of generaliy, we can assume y( > 0 evenually. If (3.4 holds, hen 0 and C > 0 can be chosen such ha ( 1 f(s, C s < C r( 2. Since g is an odd funcion, if y is he soluion of dynamic equaion y( = C ( f(u, C u s, r(s hen y is a nonincreasing soluion of (1.1. Now we consruc he sequence {x m (}: x 0 ( = C 2, x m ( = C 2 + ( 1 r(s s s f(u, x m 1 u s.
8 110 Xiangyun Shi, Xueyong Zhou and Weiping Yan Then C 2 = x 0( x 1 ( x m ( C. Clearly, he limi of he sequence {x m } exiss. We denoe i by x. Applying Lebesgue s dominaed convergence heorem, we have x ( = C ( f(u, x (u u s. r(s Then equaion (1.1 has an, in absolue value, nonincreasing soluion. Conversely, le y > 0 be a bounded nonincreasing soluion of (1.1 and lim y( = K (0,. Then y ( < 0 evenually and y( K for large enough. Equaion 2 (1.1 implies lim r(g(y ( = L (, 0. Now, we will show L = 0. Oherwise, L < 0 and so evenually ( ( L 1 r(g(y ( L y ( = L 1/α. r( r( Inegraing his relaion from o, we obain y( y( + L 1/α s ( 1 s, r(s which by (A 4 implies ha lim y( =. This is an immediae conradicion. Thus, L = 0. Inegraing (1.1 from o, we ge so ha r(g(y ( = g(y ( ( 1 r( f(s, y(s s Inegraing his inequaliy from o we obain f(s, K/2 s, f(s, K/2 s. y( K + ( 1 r(s Then (3.4 is saisfied. The proof is complee. s f(u, K 2 u s. In he presen paper, we will apply he resuls of he above heorems o wo discree cases. Example 3.6. If T = N, hen (1.1 reduces o he difference equaion r((g( y( ] f(, y( = 0, N. (3.5
9 Nonoscillaory Soluions of Some Nonlinear Dynamic Equaions 111 Le r( 1, g(u = u α = u α sgnu, f(u 1, u 2 = (u 1 +u 2 β = u 1 +u 2 β sgnu 2. (3.6 Now (3.5 can be wrien as ( y(n α (n + y(n β = 0, n N. (3.7 n 1 ] 1/α In his special case, (3.1 becomes (l + C β < for some C > 0. By n=n 0 l=n 0 Theorem 3.2, if β < α 1, (3.7 has a nondecreasing bounded soluion. In fac n 1 ] 1/α (l + C β (n n0 (n 1 + C β] 1/α (n 1 + C β+1 α, n=n 0 l=n 0 n=n 0 n=n 0 if β < α 1, he progression (n + C β+1 α is convergen, so he progression n=n 0 n 1 ] 1/α (l + C β is also convergen. l=n 0 n=n 0 Example 3.7. If T = hn, h > 0, and (3.6 hold, hen (1.1 can be wrien as (y ( α ] ( + y( β = 0, hn. (3.8 In his case, condiion (3.1 becomes h h n=n 0 /h n 1 l=n 0 /h (hl + C β 1/α <, where α = p/q (p and q are boh odd. By Theorem 3.2, if β < α 1, hen equaion (3.8 has a nondecreasing bounded posiive soluion. In fac, h n=n 0 /h h n 1 l=n 0 /h (hl + C β 1/α < h n=n 0 /h Thus, if β < α 1, he progression is convergen. References (h n 0 (hn h + C β ] 1/α. 1] Ravi Agarwal, Marin Bohner, Donal O Regan, and Allan Peerson. Dynamic equaions on ime scales: a survey. J. Compu. Appl. Mah., 141(1-2:1 26, 2002.
10 112 Xiangyun Shi, Xueyong Zhou and Weiping Yan 2] Marin Bohner and Allan Peerson. Dynamic equaions on ime scales. Birkhäuser Boson Inc., Boson, MA, ] Sefan Hilger. Analysis on measure chains a unified approach o coninuous and discree calculus. Resuls Mah., 18(1-2:18 56, ] M. R. S. Kulenović. Asympoic behavior of soluions of cerain differenial equaions and inequaliies of second order. Rad. Ma., 1(2: , ] M. R. S. Kulenović and Ć. Ljubović. The asympoic behavior of nonoscillaory soluions of some nonlinear differenial equaions. Nonlinear Anal., 42(5, Ser. A: Theory Mehods: , ] B. G. Zhang and Xinghua Deng. Oscillaion of delay differenial equaions on ime scales. Mah. Compu. Modelling, 36(11-13: , 2002.
OSCILLATION OF SECOND-ORDER DELAY AND NEUTRAL DELAY DYNAMIC EQUATIONS ON TIME SCALES
Dynamic Sysems and Applicaions 6 (2007) 345-360 OSCILLATION OF SECOND-ORDER DELAY AND NEUTRAL DELAY DYNAMIC EQUATIONS ON TIME SCALES S. H. SAKER Deparmen of Mahemaics and Saisics, Universiy of Calgary,
More informationEXISTENCE OF NON-OSCILLATORY SOLUTIONS TO FIRST-ORDER NEUTRAL DIFFERENTIAL EQUATIONS
Elecronic Journal of Differenial Equaions, Vol. 206 (206, No. 39, pp.. ISSN: 072-669. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu fp ejde.mah.xsae.edu EXISTENCE OF NON-OSCILLATORY SOLUTIONS TO
More informationAnn. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL:
Ann. Func. Anal. 2 2011, no. 2, 34 41 A nnals of F uncional A nalysis ISSN: 2008-8752 elecronic URL: www.emis.de/journals/afa/ CLASSIFICAION OF POSIIVE SOLUIONS OF NONLINEAR SYSEMS OF VOLERRA INEGRAL EQUAIONS
More informationOscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson
PROCEEDINGS OF THE FOURTH INTERNATIONAL CONFERENCE ON DYNAMICAL SYSTEMS AND DIFFERENTIAL EQUATIONS May 4 7, 00, Wilmingon, NC, USA pp 0 Oscillaion of an Euler Cauchy Dynamic Equaion S Huff, G Olumolode,
More informationA Necessary and Sufficient Condition for the Solutions of a Functional Differential Equation to Be Oscillatory or Tend to Zero
JOURNAL OF MAEMAICAL ANALYSIS AND APPLICAIONS 24, 7887 1997 ARICLE NO. AY965143 A Necessary and Sufficien Condiion for he Soluions of a Funcional Differenial Equaion o Be Oscillaory or end o Zero Piambar
More informationOn Oscillation of a Generalized Logistic Equation with Several Delays
Journal of Mahemaical Analysis and Applicaions 253, 389 45 (21) doi:1.16/jmaa.2.714, available online a hp://www.idealibrary.com on On Oscillaion of a Generalized Logisic Equaion wih Several Delays Leonid
More informationExistence of non-oscillatory solutions of a kind of first-order neutral differential equation
MATHEMATICA COMMUNICATIONS 151 Mah. Commun. 22(2017), 151 164 Exisence of non-oscillaory soluions of a kind of firs-order neural differenial equaion Fanchao Kong Deparmen of Mahemaics, Hunan Normal Universiy,
More informationPOSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION
Novi Sad J. Mah. Vol. 32, No. 2, 2002, 95-108 95 POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION Hajnalka Péics 1, János Karsai 2 Absrac. We consider he scalar nonauonomous neural delay differenial
More informationHILLE AND NEHARI TYPE CRITERIA FOR THIRD-ORDER DYNAMIC EQUATIONS
HILLE AND NEHARI TYPE CRITERIA FOR THIRD-ORDER DYNAMIC EQUATIONS L. ERBE, A. PETERSON AND S. H. SAKER Absrac. In his paper, we exend he oscillaion crieria ha have been esablished by Hille [15] and Nehari
More informationProperties Of Solutions To A Generalized Liénard Equation With Forcing Term
Applied Mahemaics E-Noes, 8(28), 4-44 c ISSN 67-25 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Properies Of Soluions To A Generalized Liénard Equaion Wih Forcing Term Allan Kroopnick
More informationExistence Theory of Second Order Random Differential Equations
Global Journal of Mahemaical Sciences: Theory and Pracical. ISSN 974-32 Volume 4, Number 3 (22), pp. 33-3 Inernaional Research Publicaion House hp://www.irphouse.com Exisence Theory of Second Order Random
More informationExistence of positive solution for a third-order three-point BVP with sign-changing Green s function
Elecronic Journal of Qualiaive Theory of Differenial Equaions 13, No. 3, 1-11; hp://www.mah.u-szeged.hu/ejqde/ Exisence of posiive soluion for a hird-order hree-poin BVP wih sign-changing Green s funcion
More informationStability and Bifurcation in a Neural Network Model with Two Delays
Inernaional Mahemaical Forum, Vol. 6, 11, no. 35, 175-1731 Sabiliy and Bifurcaion in a Neural Nework Model wih Two Delays GuangPing Hu and XiaoLing Li School of Mahemaics and Physics, Nanjing Universiy
More informationEIGENVALUE PROBLEMS FOR SINGULAR MULTI-POINT DYNAMIC EQUATIONS ON TIME SCALES
Elecronic Journal of Differenial Equaions, Vol. 27 (27, No. 37, pp. 3. ISSN: 72-669. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu EIGENVALUE PROBLEMS FOR SINGULAR MULTI-POINT DYNAMIC EQUATIONS ON
More informationLIMIT AND INTEGRAL PROPERTIES OF PRINCIPAL SOLUTIONS FOR HALF-LINEAR DIFFERENTIAL EQUATIONS. 1. Introduction
ARCHIVUM MATHEMATICUM (BRNO) Tomus 43 (2007), 75 86 LIMIT AND INTEGRAL PROPERTIES OF PRINCIPAL SOLUTIONS FOR HALF-LINEAR DIFFERENTIAL EQUATIONS Mariella Cecchi, Zuzana Došlá and Mauro Marini Absrac. Some
More informationSTABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS WITH VARIABLE DELAYS
Elecronic Journal of Differenial Equaions, Vol. 217 217, No. 118, pp. 1 14. ISSN: 172-6691. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS
More informationDynamic Systems and Applications 12 (2003) A SECOND-ORDER SELF-ADJOINT EQUATION ON A TIME SCALE
Dynamic Sysems and Applicaions 2 (2003) 20-25 A SECOND-ORDER SELF-ADJOINT EQUATION ON A TIME SCALE KIRSTEN R. MESSER Universiy of Nebraska, Deparmen of Mahemaics and Saisics, Lincoln NE, 68588, USA. E-mail:
More informationarxiv: v1 [math.gm] 4 Nov 2018
Unpredicable Soluions of Linear Differenial Equaions Mara Akhme 1,, Mehme Onur Fen 2, Madina Tleubergenova 3,4, Akylbek Zhamanshin 3,4 1 Deparmen of Mahemaics, Middle Eas Technical Universiy, 06800, Ankara,
More informationON THE OSCILLATION OF THIRD ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS. Cairo University, Orman, Giza 12221, Egypt
a 1/α s)ds < Indian J. pre appl. Mah., 396): 491-507, December 2008 c Prined in India. ON THE OSCILLATION OF THIRD ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS SAID R. GRACE 1, RAVI P. AGARWAL 2 AND MUSTAFA
More informationPredator - Prey Model Trajectories and the nonlinear conservation law
Predaor - Prey Model Trajecories and he nonlinear conservaion law James K. Peerson Deparmen of Biological Sciences and Deparmen of Mahemaical Sciences Clemson Universiy Ocober 28, 213 Ouline Drawing Trajecories
More informationApproximating positive solutions of nonlinear first order ordinary quadratic differential equations
Dhage & Dhage, Cogen Mahemaics (25, 2: 2367 hp://dx.doi.org/.8/233835.25.2367 APPLIED & INTERDISCIPLINARY MATHEMATICS RESEARCH ARTICLE Approximaing posiive soluions of nonlinear firs order ordinary quadraic
More informationarxiv: v1 [math.ca] 15 Nov 2016
arxiv:6.599v [mah.ca] 5 Nov 26 Counerexamples on Jumarie s hree basic fracional calculus formulae for non-differeniable coninuous funcions Cheng-shi Liu Deparmen of Mahemaics Norheas Peroleum Universiy
More informationPositive continuous solution of a quadratic integral equation of fractional orders
Mah. Sci. Le., No., 9-7 (3) 9 Mahemaical Sciences Leers An Inernaional Journal @ 3 NSP Naural Sciences Publishing Cor. Posiive coninuous soluion of a quadraic inegral equaion of fracional orders A. M.
More informationNonlinear Fuzzy Stability of a Functional Equation Related to a Characterization of Inner Product Spaces via Fixed Point Technique
Filoma 29:5 (2015), 1067 1080 DOI 10.2298/FI1505067W Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma Nonlinear Fuzzy Sabiliy of a Funcional
More informationMonotonic Solutions of a Class of Quadratic Singular Integral Equations of Volterra type
In. J. Conemp. Mah. Sci., Vol. 2, 27, no. 2, 89-2 Monoonic Soluions of a Class of Quadraic Singular Inegral Equaions of Volerra ype Mahmoud M. El Borai Deparmen of Mahemaics, Faculy of Science, Alexandria
More informationCERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS
SARAJEVO JOURNAL OF MATHEMATICS Vol.10 (22 (2014, 67 76 DOI: 10.5644/SJM.10.1.09 CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS ALMA OMERSPAHIĆ AND VAHIDIN HADŽIABDIĆ Absrac. This paper presens sufficien
More informationSome New Uniqueness Results of Solutions to Nonlinear Fractional Integro-Differential Equations
Annals of Pure and Applied Mahemaics Vol. 6, No. 2, 28, 345-352 ISSN: 2279-87X (P), 2279-888(online) Published on 22 February 28 www.researchmahsci.org DOI: hp://dx.doi.org/.22457/apam.v6n2a Annals of
More informationMODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE
Topics MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES 2-6 3. FUNCTION OF A RANDOM VARIABLE 3.2 PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE 3.3 EXPECTATION AND MOMENTS
More informationEssential Maps and Coincidence Principles for General Classes of Maps
Filoma 31:11 (2017), 3553 3558 hps://doi.org/10.2298/fil1711553o Published by Faculy of Sciences Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma Essenial Maps Coincidence
More informationAn Introduction to Malliavin calculus and its applications
An Inroducion o Malliavin calculus and is applicaions Lecure 5: Smoohness of he densiy and Hörmander s heorem David Nualar Deparmen of Mahemaics Kansas Universiy Universiy of Wyoming Summer School 214
More informationSTABILITY OF PEXIDERIZED QUADRATIC FUNCTIONAL EQUATION IN NON-ARCHIMEDEAN FUZZY NORMED SPASES
Novi Sad J. Mah. Vol. 46, No. 1, 2016, 15-25 STABILITY OF PEXIDERIZED QUADRATIC FUNCTIONAL EQUATION IN NON-ARCHIMEDEAN FUZZY NORMED SPASES N. Eghbali 1 Absrac. We deermine some sabiliy resuls concerning
More informationBoundedness and Exponential Asymptotic Stability in Dynamical Systems with Applications to Nonlinear Differential Equations with Unbounded Terms
Advances in Dynamical Sysems and Applicaions. ISSN 0973-531 Volume Number 1 007, pp. 107 11 Research India Publicaions hp://www.ripublicaion.com/adsa.hm Boundedness and Exponenial Asympoic Sabiliy in Dynamical
More informationApplied Mathematics Letters. Oscillation results for fourth-order nonlinear dynamic equations
Applied Mahemaics Leers 5 (0) 058 065 Conens liss available a SciVerse ScienceDirec Applied Mahemaics Leers jornal homepage: www.elsevier.com/locae/aml Oscillaion resls for forh-order nonlinear dynamic
More informationExistence of multiple positive periodic solutions for functional differential equations
J. Mah. Anal. Appl. 325 (27) 1378 1389 www.elsevier.com/locae/jmaa Exisence of muliple posiive periodic soluions for funcional differenial equaions Zhijun Zeng a,b,,libi a, Meng Fan a a School of Mahemaics
More informationRepresentation of Stochastic Process by Means of Stochastic Integrals
Inernaional Journal of Mahemaics Research. ISSN 0976-5840 Volume 5, Number 4 (2013), pp. 385-397 Inernaional Research Publicaion House hp://www.irphouse.com Represenaion of Sochasic Process by Means of
More informationCONTRIBUTION TO IMPULSIVE EQUATIONS
European Scienific Journal Sepember 214 /SPECIAL/ ediion Vol.3 ISSN: 1857 7881 (Prin) e - ISSN 1857-7431 CONTRIBUTION TO IMPULSIVE EQUATIONS Berrabah Faima Zohra, MA Universiy of sidi bel abbes/ Algeria
More informationSOME PROPERTIES OF GENERALIZED STRONGLY HARMONIC CONVEX FUNCTIONS MUHAMMAD ASLAM NOOR, KHALIDA INAYAT NOOR, SABAH IFTIKHAR AND FARHAT SAFDAR
Inernaional Journal o Analysis and Applicaions Volume 16, Number 3 2018, 427-436 URL: hps://doi.org/10.28924/2291-8639 DOI: 10.28924/2291-8639-16-2018-427 SOME PROPERTIES OF GENERALIZED STRONGLY HARMONIC
More informationEXERCISES FOR SECTION 1.5
1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler
More informationDIFFERENTIAL EQUATIONS
ne. J. Ma. Mah. Vo1. {1978)1-1 BEHAVOR OF SECOND ORDER NONLNEAR DFFERENTAL EQUATONS RNA LNG Deparmen of Mahemaics California Sae Universiy Los Angeles, California 93 (Received November 9, 1977 and in revised
More information2. Nonlinear Conservation Law Equations
. Nonlinear Conservaion Law Equaions One of he clear lessons learned over recen years in sudying nonlinear parial differenial equaions is ha i is generally no wise o ry o aack a general class of nonlinear
More informationTO our knowledge, most exciting results on the existence
IAENG Inernaional Journal of Applied Mahemaics, 42:, IJAM_42 2 Exisence and Uniqueness of a Periodic Soluion for hird-order Delay Differenial Equaion wih wo Deviaing Argumens A. M. A. Abou-El-Ela, A. I.
More informationVariational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations
IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728, p-issn: 2319-765X. Volume 1, Issue 6 Ver. II (Nov - Dec. 214), PP 48-54 Variaional Ieraion Mehod for Solving Sysem of Fracional Order Ordinary Differenial
More informationMatrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality
Marix Versions of Some Refinemens of he Arihmeic-Geomeric Mean Inequaliy Bao Qi Feng and Andrew Tonge Absrac. We esablish marix versions of refinemens due o Alzer ], Carwrigh and Field 4], and Mercer 5]
More informationUndetermined coefficients for local fractional differential equations
Available online a www.isr-publicaions.com/jmcs J. Mah. Compuer Sci. 16 (2016), 140 146 Research Aricle Undeermined coefficiens for local fracional differenial equaions Roshdi Khalil a,, Mohammed Al Horani
More informationAsymptotic instability of nonlinear differential equations
Elecronic Journal of Differenial Equaions, Vol. 1997(1997), No. 16, pp. 1 7. ISSN: 172-6691. URL: hp://ejde.mah.sw.edu or hp://ejde.mah.un.edu fp (login: fp) 147.26.13.11 or 129.12.3.113 Asympoic insabiliy
More informationInternational Journal of Scientific & Engineering Research, Volume 4, Issue 10, October ISSN
Inernaional Journal of Scienific & Engineering Research, Volume 4, Issue 10, Ocober-2013 900 FUZZY MEAN RESIDUAL LIFE ORDERING OF FUZZY RANDOM VARIABLES J. EARNEST LAZARUS PIRIYAKUMAR 1, A. YAMUNA 2 1.
More informationCash Flow Valuation Mode Lin Discrete Time
IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728,p-ISSN: 2319-765X, 6, Issue 6 (May. - Jun. 2013), PP 35-41 Cash Flow Valuaion Mode Lin Discree Time Olayiwola. M. A. and Oni, N. O. Deparmen of Mahemaics
More informationExistence of positive solutions for second order m-point boundary value problems
ANNALES POLONICI MATHEMATICI LXXIX.3 (22 Exisence of posiive soluions for second order m-poin boundary value problems by Ruyun Ma (Lanzhou Absrac. Le α, β, γ, δ and ϱ := γβ + αγ + αδ >. Le ψ( = β + α,
More informationSection 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients
Secion 3.5 Nonhomogeneous Equaions; Mehod of Undeermined Coefficiens Key Terms/Ideas: Linear Differenial operaor Nonlinear operaor Second order homogeneous DE Second order nonhomogeneous DE Soluion o homogeneous
More informationOptimality Conditions for Unconstrained Problems
62 CHAPTER 6 Opimaliy Condiions for Unconsrained Problems 1 Unconsrained Opimizaion 11 Exisence Consider he problem of minimizing he funcion f : R n R where f is coninuous on all of R n : P min f(x) x
More informationDISCRETE GRONWALL LEMMA AND APPLICATIONS
DISCRETE GRONWALL LEMMA AND APPLICATIONS JOHN M. HOLTE MAA NORTH CENTRAL SECTION MEETING AT UND 24 OCTOBER 29 Gronwall s lemma saes an inequaliy ha is useful in he heory of differenial equaions. Here is
More informationEXISTENCE AND UNIQUENESS THEOREMS ON CERTAIN DIFFERENCE-DIFFERENTIAL EQUATIONS
Elecronic Journal of Differenial Equaions, Vol. 29(29), No. 49, pp. 2. ISSN: 72-669. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu fp ejde.mah.xsae.edu EXISTENCE AND UNIQUENESS THEOREMS ON CERTAIN
More informationarxiv: v1 [math.fa] 9 Dec 2018
AN INVERSE FUNCTION THEOREM CONVERSE arxiv:1812.03561v1 [mah.fa] 9 Dec 2018 JIMMIE LAWSON Absrac. We esablish he following converse of he well-known inverse funcion heorem. Le g : U V and f : V U be inverse
More informationChapter 2. First Order Scalar Equations
Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.
More informationBifurcation Analysis of a Stage-Structured Prey-Predator System with Discrete and Continuous Delays
Applied Mahemaics 4 59-64 hp://dx.doi.org/.46/am..4744 Published Online July (hp://www.scirp.org/ournal/am) Bifurcaion Analysis of a Sage-Srucured Prey-Predaor Sysem wih Discree and Coninuous Delays Shunyi
More informationMONOTONE SOLUTIONS OF TWO-DIMENSIONAL NONLINEAR FUNCTIONAL DIFFERENTIAL SYSTEMS
Dynamic Sysems and Applicaions 7 2008 595-608 MONOONE SOLUIONS OF WO-DIMENSIONAL NONLINEAR FUNCIONAL DIFFERENIAL SYSEMS MARIELLA CECCHI, ZUZANA DOŠLÁ, AND MAURO MARINI Depar. of Elecronics and elecommunicaions,
More informationOSCILLATION THEORY OF DYNAMIC EQUATIONS ON TIME SCALES
Universiy of Nebraska - Lincoln DigialCommons@Universiy of Nebraska - Lincoln Disseraions, heses, and Suden Research Papers in Mahemaics Mahemaics, Deparmen of 4-28-2008 OSCILLAION HEORY OF DYNAMIC EQUAIONS
More informationOn the Oscillation of Nonlinear Fractional Differential Systems
On he Oscillaion of Nonlinear Fracional Differenial Sysems Vadivel Sadhasivam, Muhusamy Deepa, Nagamanickam Nagajohi Pos Graduae and Research Deparmen of Mahemaics,Thiruvalluvar Governmen Ars College (Affli.
More informationOn Carlsson type orthogonality and characterization of inner product spaces
Filoma 26:4 (212), 859 87 DOI 1.2298/FIL124859K Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma On Carlsson ype orhogonaliy and characerizaion
More informationEXISTENCE AND ITERATION OF MONOTONE POSITIVE POLUTIONS FOR MULTI-POINT BVPS OF DIFFERENTIAL EQUATIONS
U.P.B. Sci. Bull., Series A, Vol. 72, Iss. 3, 2 ISSN 223-727 EXISTENCE AND ITERATION OF MONOTONE POSITIVE POLUTIONS FOR MULTI-POINT BVPS OF DIFFERENTIAL EQUATIONS Yuji Liu By applying monoone ieraive meho,
More informationOn fuzzy normed algebras
Available online a www.jnsa.com J. Nonlinear Sci. Appl. 9 (2016), 5488 5496 Research Aricle On fuzzy normed algebras Tudor Bînzar a,, Flavius Paer a, Sorin Nădăban b a Deparmen of Mahemaics, Poliehnica
More informationSOME MORE APPLICATIONS OF THE HAHN-BANACH THEOREM
SOME MORE APPLICATIONS OF THE HAHN-BANACH THEOREM FRANCISCO JAVIER GARCÍA-PACHECO, DANIELE PUGLISI, AND GUSTI VAN ZYL Absrac We give a new proof of he fac ha equivalen norms on subspaces can be exended
More informationThe L p -Version of the Generalized Bohl Perron Principle for Vector Equations with Infinite Delay
Advances in Dynamical Sysems and Applicaions ISSN 973-5321, Volume 6, Number 2, pp. 177 184 (211) hp://campus.ms.edu/adsa The L p -Version of he Generalized Bohl Perron Principle for Vecor Equaions wih
More informationResearch Article Existence and Uniqueness of Periodic Solution for Nonlinear Second-Order Ordinary Differential Equations
Hindawi Publishing Corporaion Boundary Value Problems Volume 11, Aricle ID 19156, 11 pages doi:1.1155/11/19156 Research Aricle Exisence and Uniqueness of Periodic Soluion for Nonlinear Second-Order Ordinary
More informationOn the probabilistic stability of the monomial functional equation
Available online a www.jnsa.com J. Nonlinear Sci. Appl. 6 (013), 51 59 Research Aricle On he probabilisic sabiliy of he monomial funcional equaion Claudia Zaharia Wes Universiy of Timişoara, Deparmen of
More informationASYMPTOTIC FORMS OF WEAKLY INCREASING POSITIVE SOLUTIONS FOR QUASILINEAR ORDINARY DIFFERENTIAL EQUATIONS
Elecronic Journal of Differenial Equaions, Vol. 2007(2007), No. 126, pp. 1 12. ISSN: 1072-6691. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu fp ejde.mah.xsae.edu (login: fp) ASYMPTOTIC FORMS OF
More informationOSCILLATION OF THIRD-ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS
Elecronic Journal of Qualiaive Theory of Differenial Equaions 2010, No. 43, 1-10; hp://www.mah.u-szeged.hu/ejqde/ OSCILLATION OF THIRD-ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS B. BACULÍKOVÁ AND J. DŽURINA
More informationDifferential Equations
Mah 21 (Fall 29) Differenial Equaions Soluion #3 1. Find he paricular soluion of he following differenial equaion by variaion of parameer (a) y + y = csc (b) 2 y + y y = ln, > Soluion: (a) The corresponding
More informationSOME INEQUALITIES AND ABSOLUTE MONOTONICITY FOR MODIFIED BESSEL FUNCTIONS OF THE FIRST KIND
Commun. Korean Mah. Soc. 3 (6), No., pp. 355 363 hp://dx.doi.org/.434/ckms.6.3..355 SOME INEQUALITIES AND ABSOLUTE MONOTONICITY FOR MODIFIED BESSEL FUNCTIONS OF THE FIRST KIND Bai-Ni Guo Feng Qi Absrac.
More informationExample on p. 157
Example 2.5.3. Le where BV [, 1] = Example 2.5.3. on p. 157 { g : [, 1] C g() =, g() = g( + ) [, 1), var (g) = sup g( j+1 ) g( j ) he supremum is aken over all he pariions of [, 1] (1) : = < 1 < < n =
More informationMath 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities:
Mah 4 Eam Review Problems Problem. Calculae he 3rd Taylor polynomial for arcsin a =. Soluion. Le f() = arcsin. For his problem, we use he formula f() + f () + f ()! + f () 3! for he 3rd Taylor polynomial
More informationOn Two Integrability Methods of Improper Integrals
Inernaional Journal of Mahemaics and Compuer Science, 13(218), no. 1, 45 5 M CS On Two Inegrabiliy Mehods of Improper Inegrals H. N. ÖZGEN Mahemaics Deparmen Faculy of Educaion Mersin Universiy, TR-33169
More informationSOLUTIONS APPROACHING POLYNOMIALS AT INFINITY TO NONLINEAR ORDINARY DIFFERENTIAL EQUATIONS
Elecronic Journal of Differenial Equaions, Vol. 2005(2005, No. 79, pp. 1 25. ISSN: 1072-6691. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu fp ejde.mah.xsae.edu (login: fp SOLUIONS APPROACHING POLYNOMIALS
More informationSolutions from Chapter 9.1 and 9.2
Soluions from Chaper 9 and 92 Secion 9 Problem # This basically boils down o an exercise in he chain rule from calculus We are looking for soluions of he form: u( x) = f( k x c) where k x R 3 and k is
More informationFractional Method of Characteristics for Fractional Partial Differential Equations
Fracional Mehod of Characerisics for Fracional Parial Differenial Equaions Guo-cheng Wu* Modern Teile Insiue, Donghua Universiy, 188 Yan-an ilu Road, Shanghai 51, PR China Absrac The mehod of characerisics
More informationPERMANENCE (or persistence) is an important property
Engineering Leers, 5:, EL_5 6 Permanence and Exincion of Delayed Sage-Srucured Predaor-Prey Sysem on Time Scales Lili Wang, Pingli Xie Absrac This paper is concerned wih a delayed Leslie- Gower predaor-prey
More informationOn Gronwall s Type Integral Inequalities with Singular Kernels
Filoma 31:4 (217), 141 149 DOI 1.2298/FIL17441A Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma On Gronwall s Type Inegral Inequaliies
More informationOrthogonal Rational Functions, Associated Rational Functions And Functions Of The Second Kind
Proceedings of he World Congress on Engineering 2008 Vol II Orhogonal Raional Funcions, Associaed Raional Funcions And Funcions Of The Second Kind Karl Deckers and Adhemar Bulheel Absrac Consider he sequence
More informationA New Perturbative Approach in Nonlinear Singularity Analysis
Journal of Mahemaics and Saisics 7 (: 49-54, ISSN 549-644 Science Publicaions A New Perurbaive Approach in Nonlinear Singulariy Analysis Ta-Leung Yee Deparmen of Mahemaics and Informaion Technology, The
More informationTHE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX
J Korean Mah Soc 45 008, No, pp 479 49 THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX Gwang-yeon Lee and Seong-Hoon Cho Reprined from he Journal of he
More informationConvergence of the Neumann series in higher norms
Convergence of he Neumann series in higher norms Charles L. Epsein Deparmen of Mahemaics, Universiy of Pennsylvania Version 1.0 Augus 1, 003 Absrac Naural condiions on an operaor A are given so ha he Neumann
More information18 Biological models with discrete time
8 Biological models wih discree ime The mos imporan applicaions, however, may be pedagogical. The elegan body of mahemaical heory peraining o linear sysems (Fourier analysis, orhogonal funcions, and so
More informationMATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence
MATH 433/533, Fourier Analysis Secion 6, Proof of Fourier s Theorem for Poinwise Convergence Firs, some commens abou inegraing periodic funcions. If g is a periodic funcion, g(x + ) g(x) for all real x,
More informationOscillation Properties of a Logistic Equation with Several Delays
Journal of Maheaical Analysis and Applicaions 247, 11 125 Ž 2. doi:1.16 jaa.2.683, available online a hp: www.idealibrary.co on Oscillaion Properies of a Logisic Equaion wih Several Delays Leonid Berezansy
More informationFirst-Order Recurrence Relations on Isolated Time Scales
Firs-Order Recurrence Relaions on Isolaed Time Scales Evan Merrell Truman Sae Universiy d2476@ruman.edu Rachel Ruger Linfield College rruger@linfield.edu Jannae Severs Creighon Universiy jsevers@creighon.edu.
More informationdi Bernardo, M. (1995). A purely adaptive controller to synchronize and control chaotic systems.
di ernardo, M. (995). A purely adapive conroller o synchronize and conrol chaoic sysems. hps://doi.org/.6/375-96(96)8-x Early version, also known as pre-prin Link o published version (if available):.6/375-96(96)8-x
More informationResearch Article Existence and Uniqueness of Positive and Nondecreasing Solutions for a Class of Singular Fractional Boundary Value Problems
Hindawi Publishing Corporaion Boundary Value Problems Volume 29, Aricle ID 42131, 1 pages doi:1.1155/29/42131 Research Aricle Exisence and Uniqueness of Posiive and Nondecreasing Soluions for a Class of
More informationMulti-component Levi Hierarchy and Its Multi-component Integrable Coupling System
Commun. Theor. Phys. (Beijing, China) 44 (2005) pp. 990 996 c Inernaional Academic Publishers Vol. 44, No. 6, December 5, 2005 uli-componen Levi Hierarchy and Is uli-componen Inegrable Coupling Sysem XIA
More informationOn the Stability of the n-dimensional Quadratic and Additive Functional Equation in Random Normed Spaces via Fixed Point Method
In. Journal of Mah. Analysis, Vol. 7, 013, no. 49, 413-48 HIKARI Ld, www.m-hikari.com hp://d.doi.org/10.1988/ijma.013.36165 On he Sabiliy of he n-dimensional Quadraic and Addiive Funcional Equaion in Random
More informationFréchet derivatives and Gâteaux derivatives
Fréche derivaives and Gâeaux derivaives Jordan Bell jordan.bell@gmail.com Deparmen of Mahemaics, Universiy of Torono April 3, 2014 1 Inroducion In his noe all vecor spaces are real. If X and Y are normed
More informationA NEW APPROACH FOR STUDYING FUZZY FUNCTIONAL EQUATIONS
IJMMS 28:12 2001) 733 741 PII. S0161171201006639 hp://ijmms.hindawi.com Hindawi Publishing Corp. A NEW APPROACH FOR STUDYING FUZZY FUNCTIONAL EQUATIONS ELIAS DEEBA and ANDRE DE KORVIN Received 29 January
More informationNote on oscillation conditions for first-order delay differential equations
Elecronic Journal of Qualiaive Theory of Differenial Equaions 2016, No. 2, 1 10; doi: 10.14232/ejqde.2016.1.2 hp://www.ah.u-szeged.hu/ejqde/ Noe on oscillaion condiions for firs-order delay differenial
More informationL 1 -Solutions for Implicit Fractional Order Differential Equations with Nonlocal Conditions
Filoma 3:6 (26), 485 492 DOI.2298/FIL66485B Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma L -Soluions for Implici Fracional Order Differenial
More informationStochastic Model for Cancer Cell Growth through Single Forward Mutation
Journal of Modern Applied Saisical Mehods Volume 16 Issue 1 Aricle 31 5-1-2017 Sochasic Model for Cancer Cell Growh hrough Single Forward Muaion Jayabharahiraj Jayabalan Pondicherry Universiy, jayabharahi8@gmail.com
More informationDedicated to the memory of Professor Dragoslav S. Mitrinovic 1. INTRODUCTION. Let E :[0;+1)!Rbe a nonnegative, non-increasing, locally absolutely
Univ. Beograd. Publ. Elekroehn. Fak. Ser. Ma. 7 (1996), 55{67. DIFFERENTIAL AND INTEGRAL INEQUALITIES Vilmos Komornik Dedicaed o he memory of Professor Dragoslav S. Mirinovic 1. INTRODUCTION Le E :[;)!Rbe
More informationL p -L q -Time decay estimate for solution of the Cauchy problem for hyperbolic partial differential equations of linear thermoelasticity
ANNALES POLONICI MATHEMATICI LIV.2 99) L p -L q -Time decay esimae for soluion of he Cauchy problem for hyperbolic parial differenial equaions of linear hermoelasiciy by Jerzy Gawinecki Warszawa) Absrac.
More informationHamilton Jacobi equations
Hamilon Jacobi equaions Inoducion o PDE The rigorous suff from Evans, mosly. We discuss firs u + H( u = 0, (1 where H(p is convex, and superlinear a infiniy, H(p lim p p = + This by comes by inegraion
More informationOn a Fractional Stochastic Landau-Ginzburg Equation
Applied Mahemaical Sciences, Vol. 4, 1, no. 7, 317-35 On a Fracional Sochasic Landau-Ginzburg Equaion Nguyen Tien Dung Deparmen of Mahemaics, FPT Universiy 15B Pham Hung Sree, Hanoi, Vienam dungn@fp.edu.vn
More informationA Note on the Equivalence of Fractional Relaxation Equations to Differential Equations with Varying Coefficients
mahemaics Aricle A Noe on he Equivalence of Fracional Relaxaion Equaions o Differenial Equaions wih Varying Coefficiens Francesco Mainardi Deparmen of Physics and Asronomy, Universiy of Bologna, and he
More informationOrdinary Differential Equations
Ordinary Differenial Equaions 5. Examples of linear differenial equaions and heir applicaions We consider some examples of sysems of linear differenial equaions wih consan coefficiens y = a y +... + a
More information