LIMIT AND INTEGRAL PROPERTIES OF PRINCIPAL SOLUTIONS FOR HALF-LINEAR DIFFERENTIAL EQUATIONS. 1. Introduction
|
|
- Rafe Morris
- 5 years ago
- Views:
Transcription
1 ARCHIVUM MATHEMATICUM (BRNO) Tomus 43 (2007), LIMIT AND INTEGRAL PROPERTIES OF PRINCIPAL SOLUTIONS FOR HALF-LINEAR DIFFERENTIAL EQUATIONS Mariella Cecchi, Zuzana Došlá and Mauro Marini Absrac. Some asympoic properies of principal soluions of he halflinear differenial equaion (*) (a()φ(x )) + b()φ(x) = 0, Φ(u) = u p 2 u, p > 1, is he p-laplacian operaor, are considered. I is shown ha principal soluions of (*) are, roughly speaking, he smalles soluions in a neighborhood of infiniy, like in he linear case. Some inegral characerizaions of principal soluions of (1), which complees previous resuls, are presened as well. Consider he half-linear equaion 1. Inroducion (1) ( a()φ(x ) ) + b()φ(x) = 0, where he funcions a, b are coninuous and posiive for 0, and Φ(u) = u p 2 u, p > 1. When (1) is nonoscillaory, he asympoic behavior of is soluions has been considered in many papers, see, e.g., [3, 4, 7, 9, 10, 11, 14, 15], he monographs [1, 8, 17] and references herein. In paricular, when (1) is nonoscillaory, he concep of a principal soluion has been formulaed for (1) in [11, 17], by exending he analogous one saed for he linear equaion (2) ( a()x ) + b()x = 0, 2000 Mahemaics Subjec Classificaion : 34C10, 34C11. Key words and phrases : half-linear equaion, principal soluion, limi characerizaion, inegral characerizaion. Suppored by he Research Projec MSMT of he Minisry of Educaion of he Czech Republic, and by he gran A of he Gran Agency of he Academy of Sciences of he Czech Republic. Received March 30, 2006.
2 76 M. CECCHI, Z. DOŠLÁ AND M. MARINI see, e.g., [13, Chaper 11]. More precisely, a nonrivial soluion u of (1) is called a principal soluion of (1) if for every nonrivial soluion x of (1) such ha x λu, λ R, we have (3) u () u() < x () x() for large. As in he linear case, he principal soluion u exiss and is unique up o a consan facor. Any nonrivial soluion x λu is called nonprincipal soluion. Denoe J a = 0 d Φ ( a() ), J b = 0 b()d, where Φ is he inverse of he map Φ, i.e. Φ (u) = u p 2 u, p = p/(p 1). The quesion concerning limi and inegral characerizaions of principal soluions, like in he linear case, has been posed in [7] and parially solved in [3] under any of he following assumpions (4) i) J a =, p 2, ii) J b =, 1 < p 2, iii) J a + J b <. In his paper we coninue such a sudy, by assuming (5) J a + J b =. We will characerize principal soluions of (1) by means of some limi or inegral properies, which exend our quoed resuls in [3]. The paper is organized as follows. In Secion 2 some preliminary resuls, concerning he classificaion of soluions of (1), are given. In Secion 3 principal soluions of (1) are characerized by showing ha hey are, roughly speaking, he smalles soluions in a neighborhood of infiniy, like in he linear case. Some inegral characerizaions of principal soluions of (1) are presened in Secion 4, compleing in such a way our previous resuls in [3]. Some open problems complee he paper. 2. Preliminaries We sar his secion by recalling some basic resuls, which will be useful in he sequel. I is easy o verify ha he quasi-derivaive y = x [1] of any soluion x of (1), where x [1] () = a()φ ( x () ), is a soluion of he so-called reciprocal equaion ( (6) Φ ( 1 ) ) ( Φ (y ) + Φ 1 ) Φ (y) = 0, b() a() which is obained from (1) by inerchanging he funcion a wih Φ (1/b) and b wih Φ (1/a). Conversely, he quasiderivaive y [1] () = Φ (1/b())Φ (y ()) of any soluion y of (6) is a soluion of (1). Observe ha J a [J b ] for (1) plays he same role as J b [J a ] for (6) and vice versa.
3 HALF-LINEAR DIFFERENTIAL EQUATIONS 77 In view of posiiveness of a and b, (1) and (6) have he same characer wih respec o he oscillaion, i.e. (1) is nonoscillaory if and only if (6) is nonoscillaory. When J a = J b =, hen (1) is oscillaory (see, e.g., [8, Th ]). If eiher J a =, J b < or J a <, J b =, hen boh oscillaion and nonoscillaion can occur (see, e.g., [8, 3.1]). Principal soluions of (1) and (6) are relaed, as he following resul, which can be proved by using he same argumen as in [3, Theorem 1], shows. Proposiion 1. Le (1) be nonoscillaory and assume (5). A soluion u of (1) is a principal soluion if and only if v = u [1] is a principal soluion of (6). When (1) is nonoscillaory, aking ino accoun ha (6) is nonoscillaory oo, we have ha any nonrivial soluion x of (1) belongs o one of he following wo classes: The following holds. M + = {x soluion of (1) : x 0 : x()x () > 0 for > x } M = {x soluion of (1) : x 0 : x()x () < 0 for > x }. Proposiion 2. Le (1) be nonoscillaory and assume (5). Le S be he se of nonrivial soluions of (1). Then J a = S M + ; J b = S M. Moreover, (1) does no have soluions x such ha (7) lim x() = c x, lim x [1] () = d x, 0 < c x <, 0 < d x <. Proof. The firs saemen follows by using a similar argumen as in [3, Lemma 1] (see also [8, Lemmas 4.1.3, 4.1.4]). Now le us prove (7). Assume J a = and le x be a soluion of (1) saisfying (7). Then x M + and, wihou loss of generaliy, suppose x() > 0, x () > 0 for large. From x [1] () = a()φ(x ()) we obain for large (8) x () 1 Φ (a()), where he symbol g 1 () g 2 () means ha g 1 ()/g 2 () has a finie nonzero limi, as. From (8) we obain ha x is unbounded (as ), which is a conradicion. The case J b = can be reaed by using a similar argumen. Noice ha if he assumpion (5) is no verified, hen boh saemens in Proposiion 2 fail, as i follows, for insance, from [12, Theorem 3] and applying his resul o he reciprocal equaion (6).
4 78 M. CECCHI, Z. DOŠLÁ AND M. MARINI In virue of he posiiveness of he funcions a, b, and Proposiion 2, boh classes M +, M can be divided, a-priori, ino he following subclasses: M + l,0 = { x M + : lim x() = c x, lim x [1] () = 0, 0 < c x < }, M +,0 = { x M + : lim x() =, lim x [1] () = 0 }, M +,l = { x M + : lim x() =, lim x [1] () = d x, 0 < d x < }, M 0,l = { x M : lim x() = 0, lim x [1] () = d x, 0 < d x < }, M 0, = { x M : lim x() = 0, lim x [1] () = }, M l, = { x M : lim x() = c x, lim x [1] () =, 0 < c x < }. The exisence of soluions in hese subclasses depends on he convergence or divergence of he following inegrals: T J 1 = lim Φ ( 1 )Φ ( ) b(s) ds d, T a() and 0 T J 2 = lim Φ ( 1 )Φ ( T ) b(s) ds d, T 0 a() T ( T Y 1 = lim b()φ Φ ( 1 ) ) ds d, T 0 a(s) T Y 2 = lim b()φ T 0 ( 0 0 Φ ( 1 ) ) ds d. a(s) Clearly, for he linear equaion (2) we have J 1 = Y 1, J 2 = Y 2. Observe ha he inegral J 1 for (1) plays he same role as Y 2 for (6) and vice versa; analogously J 2 for (1) plays he same role as Y 1 for (6) and vice versa. The following holds. Lemma A. Concerning he muual behavior of J 1, Y 1, he only possible cases are he following: J 1 = Y 1 = for 1 < p J 1 =, Y 1 < for 2 < p J 1 <, Y 1 = for 1 < p < 2 J 1 <, Y 1 < for 1 < p. Analogously for J 2, Y 2, he only possible cases are J 2 = Y 2 = for 1 < p J 2 =, Y 2 < for 2 < p J 2 <, Y 2 = for 1 < p < 2 J 2 <, Y 2 < for 1 < p. Moreover, if J 2 + Y 2 =, hen J a =, and, if J 1 + Y 1 =, hen J b =.
5 HALF-LINEAR DIFFERENTIAL EQUATIONS 79 Proof. The possible cases for J i, Y i (i = 1, 2) follow from [6, Corollary 1 and Examples 1, 2]. The relaions beween J i, Y i and J a, J b follow from [2, Lemma 2]. The following holds. Theorem A. i 1 ) Assume J a =. Then i 2 ) Assume J b =. Then M + l,0 J 2 <, M +,l Y 2 <. M 0,l Y 1 <, M l, J 1 <. Proof. Claim i 1 ) follows, for insance, from [14, Th.s 4.1 and 4.2 ] (see also [12, Secion 4], [16, Th. 4.3], in which a more general equaion is considered). Claim i 2 ) follows by applying i 1 ) o he reciprocal equaion (6). 3. Limi characerizaion When (1) is nonoscillaory, in [7] he quesion, wheher principal soluions are smalles soluions in a neighborhood of infiniy also in he half-linear case, has been posed. This problem has been solved in [3, Theorem 2] under any of assumpions in (4). To exend such a resul, he following uniqueness resul plays an imporan role. Theorem B. Le η 0 be a given consan. i 1 ) Assume J a =, J 2 <. Then here exiss a unique soluion x of (1) such ha x M + and lim x() = η. i 2 ) Assume J b =, Y 1 <. Then here exiss a unique soluion x of (1) such ha x M and lim x [1] () = η. Proof. Claim i 1 ) follows from [14, Theorem 4.3] (see also [8, Theorem 4.1.7]). Claim i 2 ) follows by applying i 1 ) o he reciprocal equaion (6). The following holds. Theorem 1. Le u be a soluion of (1) and assume eiher i 1 ) J a =, J 2 < or i 2 ) J b =, Y 1 <. Then u is a principal soluion if and only if for any nonrivial soluion x of (1) such ha x λu, λ R, we have u() (9) lim x() = 0. Proof. If (9) holds for any nonrivial soluion x of (1) such ha x λu, λ R, hen, by using he same argumen as in [3, Theorem 2], u is a principal soluion of (1). Conversely, suppose ha u is a principal soluion and le us show ha (9) holds for any nonrivial soluion x of (1) such ha x λu, λ R if eiher i 1 ) or i 2 ) holds. Assume case i 1 ). By Theorem A, we have M + l,0 and so (1) is nonoscillaory. Wihou loss of generaliy, suppose u evenually posiive. We claim ha u is
6 80 M. CECCHI, Z. DOŠLÁ AND M. MARINI bounded (as ). Assume ha u is unbounded and consider x M + l,0 such ha x is evenually posiive. From (3), he raio u/x is evenually posiive decreasing, which yields a conradicion because lim l [u()/x()] =. Then u is bounded and so u M + l,0. For any nonrivial soluion x of (1), such ha x λu, in view of Theorem B, we obain ha x is unbounded and so (9) holds. Now assume case i 2 ). Again by Theorem A, we have M 0,l and so (1) is nonoscillaory. Wihou loss of generaliy, suppose u and x evenually posiive. In view of Proposiion 2, we have u [1] () < 0, x [1] () < 0 for large. From (3), we obain for large u [1] () ( u() ) (10) x [1] () > Φ > 0. x() Applying Proposiion 1, u [1] is a principal soluion of (6). Since for (6) he case i 1 ) holds, we obain u [1] () lim x [1] () = 0 and so, from (10), he asserion follows. From Theorem B, Theorem 1 and Theorem 2 in [3], we obain he following. Corollary 1. The se of principal soluions of (1) is eiher M + l,0 or M 0,l according o eiher J a =, J 2 <, or J b =, Y 1 <, respecively. Remark 1. Summarizing Theorem 1 and [3, Theorem 2] (which holds under any of assumpions in (4)), and aking ino accoun Lemma A, we obain ha, if (1) is nonoscillaory, hen he limi characerizaion of principal soluions (9) holds in any case excep he following wo cases (11) J 2 = Y 2 =, 1 < p < 2 ; J 1 = Y 1 =, p > 2. When any of hese cases occurs (and (1) is nonoscillaory), we conjecure ha he limi characerizaion (9) coninues o hold, as he following example suggess. Example 1. Consider he Euler ype equaion ( 1) (12) ( Φ(x ) ) + ( γ ) pφ(x) = 0, where γ = (p 1)/p, 1 < p < 2. Obviously, J a = J 2 = and u() = γ is a soluion of (12). Moreover, any nonrivial soluion x λu, λ R, saisfies x() γ (log ) 2/p, and u() = γ is a principal soluion of (12) (see, e.g., [8, Example iii)]). Obviously, (9) is saisfied. 4. Inegral characerizaions I is well-known, see e.g. [13, Ch. XI, Theorem 6.4], ha, if he linear equaion (2) is nonoscillaory, hen principal soluions u of (2) can be equivalenly
7 HALF-LINEAR DIFFERENTIAL EQUATIONS 81 characerized by one of he following condiions (in which x denoes an arbirary nonrivial soluion of (2), linearly independen of u): (π 1) (π 2 ) (π 3) u () u() < x () x() u() lim x() = 0; for large ; d a()u 2 () =. The characerizaions (π 1 ), (π 2 ) depend on all he soluions of (2). Even if his is no a serious disadvanage in he linear case, because of he reducion of order formula, he characerizaion (π 3 ) seems prefereable, since i is, roughly speaking, self-conained. In his secion we sudy he possible exensions of he inegral characerizaion (π 3 ) o he half-linear case. In [7] principal soluions u of (1) have been characerized by means of he following inegral (13) Q u := u () u 2 ()u [1] () d. In paricular, when b may change is sign, he following holds. Theorem C [7, Theorem 3.1]. Suppose ha (1) is nonoscillaory and le 1 < p 2. If x is a nonprincipal soluion of (1), hen Q x <. When b() > 0, such a resul has been parially exended in [3] by he following way. Theorem D [3, Theorems 3, 4]. Le (1) be nonoscillaory and assume any of condiions i) J a =, p 2, ii) J b =, 1 < p 2. A soluion u of (1) is a principal soluion if and only if Q u =. In addiion in [3, Corrigendum] an example is given, illusraing ha he characerizaion (13) canno be exended o he case J a =, 1 < p < 2, wihou any addiional assumpions. Here we exend Theorems C, D by inroducing a new inegral characerizaion of principal soluions. Consider he inegral (14) R u := b()φ(u()) u()(u [1] ()) 2 d, which arises considering Q y, where y = u [1] is a soluion of he reciprocal equaion (6). Concerning he characerizaion of nonprincipal soluions, he following resul exends Theorem C.
8 82 M. CECCHI, Z. DOŠLÁ AND M. MARINI Theorem 2. Le (1) be nonoscillaory and assume (5). If x is a nonprincipal soluion of (1), hen Q x < and R x <. To prove his resul, he following lemma is useful. Lemma 1. Assume ha (1) is nonoscillaory and (5) holds. If x is a nonprincipal soluion of (1), hen lim sup x()x [1] () = or lim inf x()x[1] () =, according o J a = or J b =, respecively. Proof. Le J a =. Assume ha here exiss a consan h > 0 such ha for large x()x [1] () < h. Because x is a nonprincipal soluion, in view of Theorem A and Corollary 1, x is unbounded. Then x () Q x = x 2 ()x [1] () d 1 x () h x() d =, which conradics Theorem C or Theorem D, according o 1 < p 2 or p 2, respecively. Now le J b =. Consider he reciprocal equaion (6): applying he firs par of he proof and using Proposiion 1, we obain limsup y()y [1] () = for any nonprincipal soluion y of (6). Because y()y [1] () = x()x [1] (), he asserion follows. Proof of Theorem 2. Taking ino accoun Lemma 1 and using he ideniy T we obain x (s) x 2 (s)x [1] (s) ds = 1 x(t)x [1] (T) 1 x()x [1] () + Q x = 1 x(t)x [1] (T) + R x T b(s)φ(x(s)) x(s)(x [1] (s)) 2 ds, and so boh inegrals Q x, R x have he same behavior. Thus, if 1 < p 2, he asserion follows from Theorem C and if p > 2, he asserion follows applying again Theorem C o he reciprocal equaion (6). Concerning principal soluions, he following holds. Theorem 3. Le (1) be nonoscillaory and le u be a principal soluion of (1). i 1 ) Assume J a =. In addiion, when J 2 =, suppose p 2. Then R u =. i 2 ) Assume J b =. In addiion, when Y 1 =, suppose 1 < p 2. Then Q u =.
9 HALF-LINEAR DIFFERENTIAL EQUATIONS 83 Proof. Claim i 1 ). Since (1) is nonoscillaory, we have J b < (see, e.g., [8, Theorem 1.2.9]). By Proposiion 2 we have S M +. Wihou loss of generaliy, assume u() > 0, u [1] () > 0 for T 0. We have Then T u (s) u 2 (s)u [1] (s) ds = 1 u(t)u [1] (T) 1 u()u [1] () + < (15) Q u 1 u(t)u [1] (T) + T 1 u(t)u [1] (T) + R u. T b(s)φ(u(s)) u(s)(u [1] (s)) 2 ds. b(s)φ(u(s)) u(s)(u [1] (s)) 2 ds When p 2, from Theorem D we have Q u = and so (15) yields R u =. Now le 1 < p < 2. By assumpions and Lemma A we have J 2 < and so, in view of Corollary 1, u M + l,0. By using he l Hospial rule, we have (16) u [1] () b(s)ds. Thus, aking ino accoun ha J b < we obain R u b() (u [1] ()) 2 d = b() ( b(s)ds ) 2 d =. Claim i 2 ). The asserion follows by applying claim i 1 ) o he reciprocal equaion (6) and using Proposiion 1. From Theorems 2, 3 we obain he following. Corollary 2. Le (1) be nonoscillaory and assume (5). In addiion, when J 2 =, suppose p 2 and when Y 1 =, suppose 1 < p 2. A soluion u of (1) is a principal soluion if and only if Q u + R u =. Noice ha, when J a + J b <, he inegral characerizaion (13) fails, as, for insance, Example 2 in [3] shows. The same example illusraes ha also he inegral characerizaion (14) fails. We close his secion by sudying he behavior of inegrals Q u, R u, where u is a principal soluion of (1). The following holds. Theorem 4. Le u be a principal soluion of (1). i 1 ) Assume J a =, J 2 <. Then Q u = if and only if ( 1 ) 1/(p 1) ( (2 p)/(p 1) (17) b(s)ds) d =. a() 0 i 2 ) Assume J b =, Y 1 <. Then R u = if and only if (18) b()( ( 1 ) 1/(p 1)ds ) p 2d =. a(s)
10 84 M. CECCHI, Z. DOŠLÁ AND M. MARINI Proof. Wihou loss of generaliy, assume u() > 0 for large. Claim i 1 ). Inegraing (1) on (, ) and aking ino accoun ha, in view of Corollary 1, u M + l,0, (16) holds and so ( 1 ) (p 2)/(p 1) ( u () p 2 (p 2)/(p 1) b(s)ds). a() Thus (19) u () u [1] () = 1 a() from which he asserion follows. Claim i 2 ). Inegraing he equaliy 1 ( 1 ) 1/(p 1) ( (2 p)/(p 1) b(s)ds) u () p 2, a() u () = Φ ( u [1] () a() on (, ) and aking ino accoun ha, in view of Corollary 1, u M 0,l, we have u() Φ ( 1 ) ds, a(s) and herefore b()φ(u()) u() from which he asserion follows. ( b() ) ( 1 ) 1/(p 1)ds ) p 2, a(s) Remark 2. Using he previous resuls and inegral relaions saed in [5, Lemma 1], i is easy o show when he inegrals Q u, R u have he same behavior for any principal soluion u of (1). We sar by considering he case J a =. If p 2, from Theorems D and 3 we have Q u = R u =. Now consider he case J 2 <, 1 < p < 2 (and J a = ). By applying [5, Lemma 1] wih µ = (p 1)/(2 p) and λ = p 1 and aking ino accoun µ > λ, we obain ( 1 ) 1/(p 1) ( (2 p)/(p 1)d Y 2 = = b(s)ds) =. a() Thus, if Y 2 =, in virue of Theorems 3, 4, we have Q u = R u =. Observe ha when J a =, J 2 <, Y 2 <, 1 < p < 2, he condiion (17) can fail, as he example in [3, Corrigendum] shows. In such a circumsance, again from Theorems 3, 4, we have Q u <, R u = and so he inegrals Q u, R u have a differen behavior. In he case J b = he siuaion is similar. By applying he above argumen o he reciprocal equaion (6) we obain ha Q u = R u = when 1 < p 2. The same conclusion holds if J 1 <, Y 1 = and 1 < p < 2. Finally, when J b =, J 1 <, Y 1 <, p > 2, he condiion (18) can fail, and i is easy o produce an example in which Q u =, R u <. Remark 3. Analogously o he limi characerizaion, i remains an open problem o find an inegral characerizaion of principal soluions in boh cases (11).
11 HALF-LINEAR DIFFERENTIAL EQUATIONS 85 When b may change is sign, he limi and inegral characerizaion of he principal soluions have been parially solved in [4] provided J a <. These problems remain open in he opposie case J a = as well. References [1] Agarwal, R. P., Grace, S. R., O Regan, D., Oscillaion Theory for Second Order Linear, Half-linear, Superlinear and Sublinear Dynamic Equaions, Kluwer Acad. Publ., Dordrech, The Neherlands, [2] Cecchi, M., Došlá, Z., Marini, M., On nonoscillaory soluions of differenial equaions wih p-laplacian, Adv. Mah. Sci. Appl (2001), [3] Cecchi M., Došlá Z., Marini M., Half-linear equaions and characerisic properies of he principal soluion, J. Differenial Equ. 208, 2005, ; Corrigendum, J. Differenial Equaions 221 (2006), [4] Cecchi, M., Došlá, Z., Marini, M., Half-linear differenial equaions wih oscillaing coefficien, Differenial Inegral Equaions (2005), [5] Cecchi, M., Došlá, Z., Marini, M., Vrkoč, I., Inegral condiions for nonoscillaion of second order nonlinear differenial equaions, Nonlinear Anal. 64 (2006), [6] Došlá, Z., Vrkoč, I., On exension of he Fubini heorem and is applicaion o he second order differenial equaions, Nonlinear Anal. 57 (2004), [7] Došlý, O., Elber, Á., Inegral characerizaion of he principal soluion of half-linear second order differenial equaions, Sudia Sci. Mah. Hungar. 36 (2000), [8] Došlý, O., Řehák, P., Half-linear Differenial Equaions, Norh-Holland, Mahemaics Sudies 202, Elsevier, Amserdam, [9] Došlý, O., Řezničková, J., Regular half-linear second order differenial equaions, Arch. Mah. (Brno) 39 (2003), [10] Elber, Á., On he half-linear second order differenial equaions, Aca Mah. Hungar. 49 (1987), [11] Elber, Á., Kusano, T.: Principal soluions of non-oscillaory half-linear differenial equaions, Adv. Mah. Sci. Appl. 8 2 (1998), [12] Fan, X., Li, W. T., Zhong, C., A classificaion scheme for posiive soluions of second order ieraive differenial equaions, Elecron. J. Differenial Equaions 25 (2000), [13] Harman, P., Ordinary Differenial Equaions, 2nd ed., Birkhäuser, Boson Basel Sugar, [14] Hoshino, H., Imabayashi, R., Kusano, T., Tanigawa, T., On second-order half-linear oscillaions, Adv. Mah. Sci. Appl. 8 1 (1998), [15] Jaroš, J., Kusano, T., Tanigawa, T., Nonoscillaion heory for second order half-linear differenial equaions in he framework of regular variaion, Resuls Mah. 43 (2003), [16] Jingfa, W., On second order quasilinear oscillaions, Funkcial. Ekvac. 41 (1998), [17] Mirzov, J. D., Asympoic Properies of Soluions of he Sysems of Nonlinear Nonauonomous Ordinary Differenial Equaions, (Russian), Maikop, Adygeja Publ., 1993; he english version: Folia Fac. Sci. Naur. Univ. Masaryk. Brun. Mah
12 86 M. CECCHI, Z. DOŠLÁ AND M. MARINI Deparmen of Elecronics and Telecommunicaions Universiy of Florence, Via S. Mara Florence, Ialy mariella.cecchi@unifi.i Deparmen of Mahemaics, Masaryk Universiy Janáčkovo nám. 2a, Brno, Czech Republic dosla@mah.muni.cz Deparmen of Elecronics and Telecommunicaion Universiy of Florence, Via S. Mara Florence, Ialy mauro.marini@unifi.i
MONOTONE 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 informationThe Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales
Advances in Dynamical Sysems and Applicaions. ISSN 0973-5321 Volume 1 Number 1 (2006, pp. 103 112 c Research India Publicaions hp://www.ripublicaion.com/adsa.hm The Asympoic Behavior of Nonoscillaory Soluions
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 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 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 informationOSCILLATION CONSTANT FOR MODIFIED EULER TYPE HALF-LINEAR EQUATIONS
Elecronic Journal of Differenial Equaions, Vol. 205 (205), No. 220, pp. 4. ISSN: 072-669. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu fp ejde.mah.xsae.edu OSCILLATION CONSTANT FOR MODIFIED EULER
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 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 informationCHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR
Annales Academiæ Scieniarum Fennicæ Mahemaica Volumen 31, 2006, 39 46 CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR Joaquim Marín and Javier
More informationOSCILLATION 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 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 informationOn Third Order Differential Equations with Property A and B
Journal of Maemaical Analysis Applicaions 3, 5955 999 Aricle ID jmaa.998.647, available online a p:www.idealibrary.com on On Tird Order Differenial Equaions wi Propery A B Mariella Cecci Deparmen of Elecronic
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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 informationGCD AND LCM-LIKE IDENTITIES FOR IDEALS IN COMMUTATIVE RINGS
GCD AND LCM-LIKE IDENTITIES FOR IDEALS IN COMMUTATIVE RINGS D. D. ANDERSON, SHUZO IZUMI, YASUO OHNO, AND MANABU OZAKI Absrac. Le A 1,..., A n n 2 be ideals of a commuaive ring R. Le Gk resp., Lk denoe
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 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 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 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 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 informationBOUNDED VARIATION SOLUTIONS TO STURM-LIOUVILLE PROBLEMS
Elecronic Journal of Differenial Equaions, Vol. 18 (18, No. 8, pp. 1 13. ISSN: 17-6691. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu BOUNDED VARIATION SOLUTIONS TO STURM-LIOUVILLE PROBLEMS JACEK
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 informationAverage Number of Lattice Points in a Disk
Average Number of Laice Poins in a Disk Sujay Jayakar Rober S. Sricharz Absrac The difference beween he number of laice poins in a disk of radius /π and he area of he disk /4π is equal o he error in he
More informationSobolev-type Inequality for Spaces L p(x) (R N )
In. J. Conemp. Mah. Sciences, Vol. 2, 27, no. 9, 423-429 Sobolev-ype Inequaliy for Spaces L p(x ( R. Mashiyev and B. Çekiç Universiy of Dicle, Faculy of Sciences and Ars Deparmen of Mahemaics, 228-Diyarbakir,
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 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 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 informationt is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...
Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger
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 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 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 informationPRECISE ASYMPTOTIC BEHAVIOR OF STRONGLY DECREASING SOLUTIONS OF FIRST-ORDER NONLINEAR FUNCTIONAL DIFFERENTIAL EQUATIONS
Elecronic Journal of Differenial Equaions, Vol. 204 204), No. 206, pp. 4. ISSN: 072-669. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu fp ejde.mah.xsae.edu PRECISE ASYMPTOTIC BEHAVIOR OF STRONGLY
More informationGeneralized Chebyshev polynomials
Generalized Chebyshev polynomials Clemene Cesarano Faculy of Engineering, Inernaional Telemaic Universiy UNINETTUNO Corso Viorio Emanuele II, 39 86 Roma, Ialy email: c.cesarano@unineunouniversiy.ne ABSTRACT
More information1 Solutions to selected problems
1 Soluions o seleced problems 1. Le A B R n. Show ha in A in B bu in general bd A bd B. Soluion. Le x in A. Then here is ɛ > 0 such ha B ɛ (x) A B. This shows x in B. If A = [0, 1] and B = [0, 2], hen
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 informationA problem related to Bárány Grünbaum conjecture
Filoma 27:1 (2013), 109 113 DOI 10.2298/FIL1301109B Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma A problem relaed o Bárány Grünbaum
More informationSPECTRAL EVOLUTION OF A ONE PARAMETER EXTENSION OF A REAL SYMMETRIC TOEPLITZ MATRIX* William F. Trench. SIAM J. Matrix Anal. Appl. 11 (1990),
SPECTRAL EVOLUTION OF A ONE PARAMETER EXTENSION OF A REAL SYMMETRIC TOEPLITZ MATRIX* William F Trench SIAM J Marix Anal Appl 11 (1990), 601-611 Absrac Le T n = ( i j ) n i,j=1 (n 3) be a real symmeric
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 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 informationChallenge Problems. DIS 203 and 210. March 6, (e 2) k. k(k + 2). k=1. f(x) = k(k + 2) = 1 x k
Challenge Problems DIS 03 and 0 March 6, 05 Choose one of he following problems, and work on i in your group. Your goal is o convince me ha your answer is correc. Even if your answer isn compleely correc,
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 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 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 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 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 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 informationPOSITIVE PERIODIC SOLUTIONS OF NONAUTONOMOUS FUNCTIONAL DIFFERENTIAL EQUATIONS DEPENDING ON A PARAMETER
POSITIVE PERIODIC SOLUTIONS OF NONAUTONOMOUS FUNCTIONAL DIFFERENTIAL EQUATIONS DEPENDING ON A PARAMETER GUANG ZHANG AND SUI SUN CHENG Received 5 November 21 This aricle invesigaes he exisence of posiive
More informationON THE WAVE EQUATION WITH A TEMPORAL NON-LOCAL TERM
Dynamic Sysems and Applicaions 16 (7) 665-67 ON THE WAVE EQUATION WITH A TEMPORAL NON-LOCAL TERM MOHAMED MEDJDEN AND NASSER-EDDINE TATAR Universié des Sciences e de la Technologie, Houari Boumedienne,
More informationOSCILLATION BEHAVIOUR OF FIRST ORDER NEUTRAL DELAY DIFFERENTIAL EQUATIONS (Gelagat Ayunan bagi Persamaan Pembezaan Tunda Neutral Peringkat Pertama)
Journal of Qualiy Measuremen and Analysis Jurnal Pengukuran Kualii dan Analisis JQMA () 5, 6-67 OSCILLATION BEHAVIOUR OF FIRST ORDER NEUTRAL DELAY DIFFERENTIAL EQUATIONS (Gelaga Ayunan bagi Persamaan Pembezaan
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 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 informationA Note on the Qualitative Behavior of Some Second Order Nonlinear Equation
Available a hp://pvamu.edu/aam Appl. Appl. Mah. ISSN: 93-9466 Vol. 8, Issue (December 3), pp. 767 776 Applicaions and Applied Mahemaics: An Inernaional Journal (AAM) A Noe on he Qualiaive Behavior of Some
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 informationProduct of Fuzzy Metric Spaces and Fixed Point Theorems
In. J. Conemp. Mah. Sciences, Vol. 3, 2008, no. 15, 703-712 Produc of Fuzzy Meric Spaces and Fixed Poin Theorems Mohd. Rafi Segi Rahma School of Applied Mahemaics The Universiy of Noingham Malaysia Campus
More information11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu
ON EQUATIONS WITH SETS AS UNKNOWNS BY PAUL ERDŐS AND S. ULAM DEPARTMENT OF MATHEMATICS, UNIVERSITY OF COLORADO, BOULDER Communicaed May 27, 1968 We shall presen here a number of resuls in se heory concerning
More information14 Autoregressive Moving Average Models
14 Auoregressive Moving Average Models In his chaper an imporan parameric family of saionary ime series is inroduced, he family of he auoregressive moving average, or ARMA, processes. For a large class
More informationd 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3
and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or
More informationarxiv: v1 [math.pr] 19 Feb 2011
A NOTE ON FELLER SEMIGROUPS AND RESOLVENTS VADIM KOSTRYKIN, JÜRGEN POTTHOFF, AND ROBERT SCHRADER ABSTRACT. Various equivalen condiions for a semigroup or a resolven generaed by a Markov process o be of
More informationA Note on Superlinear Ambrosetti-Prodi Type Problem in a Ball
A Noe on Superlinear Ambrosei-Prodi Type Problem in a Ball by P. N. Srikanh 1, Sanjiban Sanra 2 Absrac Using a careful analysis of he Morse Indices of he soluions obained by using he Mounain Pass Theorem
More informationA remark on the H -calculus
A remark on he H -calculus Nigel J. Kalon Absrac If A, B are secorial operaors on a Hilber space wih he same domain range, if Ax Bx A 1 x B 1 x, hen i is a resul of Auscher, McInosh Nahmod ha if A has
More informationENGI 9420 Engineering Analysis Assignment 2 Solutions
ENGI 940 Engineering Analysis Assignmen Soluions 0 Fall [Second order ODEs, Laplace ransforms; Secions.0-.09]. Use Laplace ransforms o solve he iniial value problem [0] dy y, y( 0) 4 d + [This was Quesion
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 informationOscillation of solutions to delay differential equations with positive and negative coefficients
Elecronic Journal of Differenial Equaions, Vol. 2000(2000), No. 13, pp. 1 13. ISSN: 1072-6691. URL: hp://ejde.mah.sw.edu or hp://ejde.mah.un.edu fp ejde.mah.sw.edu fp ejde.mah.un.edu (login: fp) Oscillaion
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 informationHeat kernel and Harnack inequality on Riemannian manifolds
Hea kernel and Harnack inequaliy on Riemannian manifolds Alexander Grigor yan UHK 11/02/2014 onens 1 Laplace operaor and hea kernel 1 2 Uniform Faber-Krahn inequaliy 3 3 Gaussian upper bounds 4 4 ean-value
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 informationImproved Approximate Solutions for Nonlinear Evolutions Equations in Mathematical Physics Using the Reduced Differential Transform Method
Journal of Applied Mahemaics & Bioinformaics, vol., no., 01, 1-14 ISSN: 179-660 (prin), 179-699 (online) Scienpress Ld, 01 Improved Approimae Soluions for Nonlinear Evoluions Equaions in Mahemaical Physics
More informationLINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS
LINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS MICHAEL DORFF AND J. SZYNAL Absrac. Differen mehods have been used in sudying he univalence of he inegral ) α ) f) ) J α, f)z) = f ) d, α,
More informationGRADIENT ESTIMATES FOR A SIMPLE PARABOLIC LICHNEROWICZ EQUATION. Osaka Journal of Mathematics. 51(1) P.245-P.256
Tile Auhor(s) GRADIENT ESTIMATES FOR A SIMPLE PARABOLIC LICHNEROWICZ EQUATION Zhao, Liang Ciaion Osaka Journal of Mahemaics. 51(1) P.45-P.56 Issue Dae 014-01 Tex Version publisher URL hps://doi.org/10.18910/9195
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 informationu(x) = e x 2 y + 2 ) Integrate and solve for x (1 + x)y + y = cos x Answer: Divide both sides by 1 + x and solve for y. y = x y + cos x
. 1 Mah 211 Homework #3 February 2, 2001 2.4.3. y + (2/x)y = (cos x)/x 2 Answer: Compare y + (2/x) y = (cos x)/x 2 wih y = a(x)x + f(x)and noe ha a(x) = 2/x. Consequenly, an inegraing facor is found wih
More informationResearch Article Limit-Point/Limit-Circle Results for Superlinear Damped Equations
Hindawi Publishing Corporaion Absrac and Applied Analysis Volume, Aricle ID 78476, pages hp://dx.doi.org/.55//78476 Research Aricle Limi-Poin/Limi-Circle Resuls for Superlinear Damped Equaions M. Barušek
More information23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes
Half-Range Series 2.5 Inroducion In his Secion we address he following problem: Can we find a Fourier series expansion of a funcion defined over a finie inerval? Of course we recognise ha such a funcion
More informationSolution of Integro-Differential Equations by Using ELzaki Transform
Global Journal of Mahemaical Sciences: Theory and Pracical. Volume, Number (), pp. - Inernaional Research Publicaion House hp://www.irphouse.com Soluion of Inegro-Differenial Equaions by Using ELzaki Transform
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 informationIntuitionistic Fuzzy 2-norm
In. Journal of Mah. Analysis, Vol. 5, 2011, no. 14, 651-659 Inuiionisic Fuzzy 2-norm B. Surender Reddy Deparmen of Mahemaics, PGCS, Saifabad, Osmania Universiy Hyderabad - 500004, A.P., India bsrmahou@yahoo.com
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 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 informationDifferential Harnack Estimates for Parabolic Equations
Differenial Harnack Esimaes for Parabolic Equaions Xiaodong Cao and Zhou Zhang Absrac Le M,g be a soluion o he Ricci flow on a closed Riemannian manifold In his paper, we prove differenial Harnack inequaliies
More informationODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004
ODEs II, Lecure : Homogeneous Linear Sysems - I Mike Raugh March 8, 4 Inroducion. In he firs lecure we discussed a sysem of linear ODEs for modeling he excreion of lead from he human body, saw how o ransform
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 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 information