Dedicated to the memory of Professor Dragoslav S. Mitrinovic 1. INTRODUCTION. Let E :[0;+1)!Rbe a nonnegative, non-increasing, locally absolutely
|
|
- Gladys Butler
- 6 years ago
- Views:
Transcription
1 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 a nonnegaive, non-increasing, locally absoluely coninuous funcion. Assume ha here exiss anoher locally absoluely coninuous funcion :[;)!Rand here are hree real numbers a, b and such ha (1) jj ae in [; ) and (2) be E a.e. in [; ): How can we esimae E()? Problems of his ype ofen appear during he sudy of dissipaive linear evoluionary problems where E denoes he energy of he soluion. I is sucien o consider he case where E() = 1. Indeed, if E() =, hen E. On he oher hand, if E() >, hen replacing E,, a and b respecively by E=E(), E() 1, ae() and ae(),we obain a soluion of (1), (2) saisfying E() = 1. We will herefore assume in he sequel ha (3) E()=1: Le us briey recall he Liapunov mehod as usually applied o his problem (see e.g. [1], [4], [5], [1], [11]). Fix a real number d saisfying (4) d>a and d b; 1991 Mahemaics Subjec Classicaion: 26D1 55
2 56 Vilmos Komornik and consider he funcion F := de+. One can readily verify ha F :[;)!R is nonnegaive, non-increasing, locally absoluely coninuous. Furhermore, and (d a)e F (d + a)e in [; ) F (d+a) 1 F a.e. in [; ): Dividing by F and inegraing i follows ha F ()e F () =(d+a) if =; (F() + (d + a) 1 ) if 6= and herefore E() < : d+a d a e =(d+a) if =; if 6= d+a d a d+a+ d+a for all such ha E() >. Nex we minimize he righ-hand side of his esimae wih respec o d saisfying (4). Since (as we shall see a he end of his paper) his mehod does no lead o sharp esimaes, we only consider henceforh he special case where Then we have = and a (5) E() d + a d a e =(d+a) =: f(d) for all and for all d saisfying (4). (Observe ha his inequaliy makes sense and remains valid wihou he assumpion E() >.) An easy compuaion shows ha f (d) =e =(d+a) ( 2a)d ( +2a)a (d a) 2 (d+a) Hence f is decreasing (resp. increasing) if ( 2a)d ( + 2a)a < (resp. > ). If 2a, hen f is decreasing in (a; ) and ends o 1 as!. Therefore we only obain he rivial esimae E() 1. If >2a, hen f decreases in (a; A) and increases in (A; ) where A = +2a 2a a (>a): We disinguish wo cases: If b A, hen choosing d = A in (5) we obain ha E() 2a e ( 2a)=(2a) :
3 Dierenial and inegral inequaliies 57 If b A, hen choosing d = b in (5) we conclude ha E() b + a b a e =(b+a) : If b a, hen b A for all >2a. If b > a, hen b A if and only if 2a <2a b+a b a. We have hus proven he following: Proposiion 1. If E, solve (1) following esimaes : (6) E() (3) wih =and a>, hen we have he 1 if 2a; 2a e(2a )=(2a) if b a and 2a; 2a e(2a )=(2a) if b>aand 2a 2a b+a b+a b a e =(b+a) if b>aand 2a b+a b a. b a ; Despie he very frequen applicaion of his mehod, he above esimaes are no opimal. Applying a dieren mehod we shall prove Theorem 2. a) The problem (1) (3) has no soluion unless > 1,aand a + b>. b) If E, solve (1){(3) wih some >, hen we have he following esimaes : b1) If a<ba, hen (7) E() ( 1 if (a + b); a+b+ (a+b)(1+) if (a + b), and in he second case he inequaliy is sric ; b2) If b>a, hen () E() ( 1 if 2a; a+b+ a+b+2a if 2a. c) If E, solve (1) (3) wih =, hen we have he following esimaes : c1) If a<ba, hen 1 if a + b; (9) E() e (a+b )=(a+b) if a + b, and in he second case he inequaliy is sric ; c2) If b>a, hen 1 if 2a; (1) E() e (2a )=(a+b) if 2a.
4 5 Vilmos Komornik d) If E, solve (1) (3) wih some 1 < <, hen we have he following esimaes : d1) If a<ba; hen (11) E() 1 if (a + b); a+b+ (a+b)(1+) if (a + b) <(a+b)=jj; if (a + b)=jj, and in he second case he inequaliy is sric ; d2) If b>a, hen (12) E() 1 if 2a; a+b+ a+b+2a if 2a (a + b)=jj; if (a + b)=jj. The above esimaes are opimal. Remark. Leing! in he formulae corresponding o 6= we nd he formulae for =. For he proof of Theorem 2, we will have o sudy a closely relaed inegral inequaliy, already used in [2], [3], [6]{[9]: (13) Z E(s) ds TE(); : Here we only assume ha E : [;)!R is a nonnegaive, non-increasing (hence measurable) funcion and ha, T are given real numbers. If E() =, hen E. If E() >, hen replacing E by E=E() and T by TE() we obain a soluion of (13) such ha E()=1. Furhermore, in order o avoid he rivial soluion 1 if =; E() = if >, we shall only consider consider soluions of (13) such ha (14) E() = 1 and E 6 in (;1): The following resul, ineresing in iself, complees some earlier heorems of Haraux [2], [3]: Theorem 3. a) The problem (13) (14) has no soluion unless > 1and T >. b) If E solves (13) (14) wih some >, hen we have he following esimaes : ( 1 if T ; (15) E() T + if T. T +T
5 Dierenial and inegral inequaliies 59 Moreover, he second inequaliy is sric if E is righ coninuous. d) If E solves (13) (14) wih =, hen we have he following esimaes : 1 if T ; (16) E() e (T )=T if T. Moreover, he second inequaliy is sric if E is righ coninuous. e) If E solves (13) (14) wih some 1 <<, hen we have he following esimaes : (17) E() 1 if T ; T + T +T if T <T=jj; if T=jj. Moreover, he second inequaliy is sric if E is righ coninuous. These esimaes are opimal. Remark. As in he preceding resuls, leing! in he formulae corresponding o 6= we nd he formulae for =. 2. PROOF Of THEOREM 3 If 1, hen (13) is meaningful only if E() > for all >. However, hen E(s) E() = 1 for all s and herefore he inegral on he lef-hand side of (14) is innie. If T, hen (13) implies a once ha E vanishes in (; ), conradicing (14). Thus par a) of he heorem is proven. Henceforh we may herefore assume ha > 1 and T >. If T, hen he esimaes E() 1 of (15){(17) follow simply from he non-increasingness of E. Also, here is nohing o prove ifbwhere We mayhus assume ha T <<B. The formula B = supfr j E(r) > g: F (r) = Z r E(s) ds denes a nonnegaive, non-increasing and locally absoluely coninuous funcion F :[;1)!R. I follows from (13) ha F T 1 F
6 6 Vilmos Komornik almos everywhere in (; 1). Dividing by F and inegraing in (;s), we obain for every <s<bhe following inequaliies: F (s) (F () + T 1 s) if 6= ; F()e s=t if =. Since F () T by (13) (14); hese inequaliies remain valid if we replace F () by T.Furhermore, we have F(s) Z T+()s s E(r) dr (T + s)e(t +()s) : Therefore, we deduce from he preceding inequaliies he esimaes (T + s)e(t +()s) (T + T 1 s) if 6= ; Te s=t if =, or equivalenly, E(T +()s) ( T+s if 6= ; T e s=t if =, for all <s<b. If, hen hese esimaes obviously remain valid for all s>. Choosing s = T hence (15) (16) follow. If 1 <<, hen he righ-hand side of he above esimae is meaningless for s T=jj. Hence E() = for all T=jj, proving he hird inequaliy in (17). Furhermore, he above esimae obviously remains valid for all <s<t=jj. Since T <<Bimplies ha < T <T=jj,wemaychoose s = T in he above esimae, and he second inequaliy of (17) follows. Now assume ha E is righ coninuous and prove ha he second inequaliies of (15) (17) are sric. Assume on he conrary ha we have equaliy in he second inequaliy of one of he formulae (15) (17) for some T : (1) E( )= ( T+ T +T if 6= ; e (T )=T if =. Using he righ coninuiy ofein, here is a consan <<1 such ha I follows ha he funcion Z Z E ds E ds: G() =n E() if ; if >
7 Dierenial and inegral inequaliies 61 also saises (13) (14); even if we replace he consan T in (13) by T. Applying he already proved (weak) esimaes (15) (17); we have G( ) ( T+ T+T if 6= ; e (T )=(T) if =. (Noe ha he hird case in (17) canno occur because G( ) > by assumpion.) Using (1) and he equaliy G( )=E( )>, i follows ha ( T + T +T T+ T+T if 6= ; e (T )=T e (T )=(T) if =. Bu boh inequaliies conradic he propery <1. Le us now urn o he proof of he opimaliy of he esimaes (15) (17): Fix > 1, T > and arbirarily. If <T, hen we have o consruc a soluion of (13) (14) such ha E() = E( ) = 1. Choose simply E() =n 1 if T ; if >T. The vericaion of (13) is immediae: he case >T is rivial, while for T we have Z Z T E(s) ds 1dsT=TE(): Wemayeven consruc coninuous examples, e.g., ( 1 if ; E() = (T )=(T ) if T ; if >T. If T (for ) or T <T=jj(for consruc a soluion of (13) (14) such ha If =, hen le us choose E( )= E() = If 6=, hen le us choose E() = ( T+ T +T if 6= ; e (T )=T if =. ( e =T if T ; e ( T )=T if T ; if >. T+ T T + T +T if T ; if T ; if >. 1 <<), hen we haveo
8 62 Vilmos Komornik (Noe ha hese funcions are no coninuous.) The only nonrivial propery overify is (13) for T. Since E = TE in (; T ) in all cases, we have in fac equaliy: Z E(s) ds = Z ( T )=() = TE() TE = TE(): E(s) ds + + T The proof of Theorem 3 is compleed. Z ( T )=() E T E(s) ds T 3. PROOF OF THEOREM 2 We begin wih a lemma relaing he problem (1) (13) (14): (3) o he inegral inequaliy Lemma 4. If E, solve (1) (3) wih some a, b and, hen E also solves (13) (14) wih he same and wih T = a + b. Proof. Since he soluions E of (1) (3) are coninuous, (3) implies (14). I follows from (1) (2) and from he non-increasingness of E ha (19) Z E(s) ds [be + ] 2(jaj + jbj)e() for all < <. Leing! hence we conclude ha Z E(s) ds 2(jaj + jbj)e() for all. Applying Theorem 3 i follows ha E( )! as!1. Using (1) we also obain ha ( )! as!. Hence, leing!1in he rs inequaliy of (19), we conclude ha Z Applying (1) again, hence (13) follows. 2 E(s) ds be()+(): I follows a once from (1) and (3) ha a. The res of par a and pars b1, c1, d1 Theorem 2 follow a once from Lemma 4 and Theorem 3, including he sric inequaliies. I remains o prove he esimaes (), (1) and (12). Since he inequaliy E() 1isobvious, we haveoprove for > 1, b > aand >2ahe
9 following esimaes: (2) E() Dierenial and inegral inequaliies 63 a+b+ a+b+2a if >; e (2a )=(a+b) if =; a+b+ a+b+2a if < and (a + b)=jj; if < and >(a+b)=jj: Clearly, wemayalso assume ha <B:= supfr j E(r) > g: Dividing he inequaliy (2) by E, hen inegraing in (;) and using (1), we obain ha whence Z be 1 E ds (b + a + a) Z 1 E 1 ds Z =[ E 1 ] + 1 ( )E 2 E ds ae() + ae() ( )a Z Compuing he inegral, i follows easily ha E() E 1 E ds ae() + ae() : a+b+ a+b+2a if >; e (2a )=(a+b) if =; a+b+ a+b+2a if <. Z E 1 E ds; Comparing wih (2), i only remains o show ha E() =if < and > (a+b)=jj. Le us observe ha for < he righ-hand side of he las inequaliy vanishes for =(a+b)=jj. I canno occur if E() >, herefore E((a+b)=jj) = and our claim follows. Now we are going o prove he opimaliy of our esimaes (7) (12): Fix > 1, a, b> aarbirarily. Furhermore, x arbirarily if and x < (a + b)=jj arbirarily if 1 <<. Le us dene a number R in he following way: se R = < : if b a and <a+b; if b>aand < 2a; (a+b)( 2a) if b>aand 2a. a+b+2a
10 64 Vilmos Komornik Furhermore, choose an arbirary number (21) a b 1+ <R if b a and a + b; is value will be precised laer. These deniions are correc and R in all cases. Nex we dene he funcion E. For >we se where E() = For =we dene E() = a+b+ if R; a+b E(R) if R< ; E(R) 1+ ( )E(R) a+b ( R)E(R) if >. < : e =(a+b) if R; E(R) if R< ; E(R)e ( )=(a+b+r ) if >. Finally, for 1 <<we se a+b+ if R; a+b E(R) if R< E() = ; E(R) 1+ ( )E(R) a+b ( R)E(R) if << ; if, = + a + b ( R)E(R) jje(r) : If, hen a + b + > ; hence E() is correcly dened and sricly posiive. In paricular, E(R) >. Le us show ha (22) ( R)E(R) <a+b and (23) ( R)E(R) 2a: Indeed, if b a and <a+b, hen If b>aand < 2a, hen ( R)E(R) = <a+b2a: ( R)E(R) = < 2a <a+b:
11 If b>aand 2a, hen Dierenial and inegral inequaliies 65 ( R)E(R) =2a<a+b by a simple compuaion. Finally, ifbaand a + b, hen ( R)E(R) = ( R)(a + b) a + b + R because R>( a b)=(1 + ) (see (21)). <a+b2a Using (22) one can readily verify ha E is a correcly dened, nonnegaive, non-increasing, locally absoluely coninuous funcion for all, and E() = 1. Le us assume for he momen he exisence of a locally absoluely coninuous funcion saisfying (1) (2); and prove he opimaliy of he esimaes of Theorem 2. Le us compue E( )=E(R). If b>a, hen E( )= 1 if < 2a; a+b+ a+b+2a if 2a and 6= ; e (2a )=(a+b) if 2a and =. This proves he opimaliy of he esimaes (), (1), (12). If b a, hen E( )= 1 if <a+b; if a + b and 6= ; a+b+r a+b e R=(a+b) if a + b and =. Leing R! ( a b)=(1 + ) (see (21)) hence he opimaliy of he esimaes (7), (9), (11) follows. I remains o consruc a locally absoluely coninuous funcion :[;)! Rsaisfying (1) and (2). Dene () = < : ae() if R; ae(r) ( R)E(R) if R ; (a ( R)E(R) )E() if. Then is locally absoluely coninuous. R; for >Ri follows easily using (23): The propery (1) is obvious for ae() () (a ( R)E(R) )E() ae(): Nex we claim ha = be E a.e. in [; ); in paricular, (2) is saised. Indeed, in (;R) wehave (be + )() =(a+b)e ()= E() :
12 66 Vilmos Komornik In (R; )wehave In ( ; ) wehave (be + )() = E(R) = E() : (be + )() =(a+b ( R)E(R) )E ()= E() by anoher simple compuaion. The proof of Theorem 2 is compleed. 4. COMPARISON OF PROPOSITION 1 AND THEOREM 2 We are going o show ha he esimaes of Proposiion 1 are opimal only in rivial cases. As in Proposiion 1, assume ha = and a>. a) If b a, hen (1) (3) has no soluion; his was no revealed by he Liapunov mehod: we only obained in his case he esimae 1 if 2a; E() 2a e(2a )=(2a) if 2a (cf. (6)). b) If a<ba, hen we have o compare he esimaes (6) and (9). For a + b hey boh give E() 1. For a + b<2ahe esimae (9) is beer because e (a+b )=(a+b) < 1: Finally, for >2ahe esimae (9) is beer again because Indeed, we have e (a+b )=(a+b) < 2a e(2a )=(2a) : e (a+b )=(a+b) e (2a )=(2a) < 2a e(2a )=(2a) : c) If b>a, hen we have o compare he esimaes (6) and (1). For 2a hey boh give E() 1. In order o show ha for 2a b+a he esimae (1) is beer han (6), we b a have o prove ha (24) e (2a )=(a+b) < b + a b a e =(a+b) : Puing x =2a=(a + b) wehave < x <1, and he inequaliy akes he form e x < (1 x). This inequaliy is rivially saised: e x = 1X i=1 x i i! < 1X i=1 x i =(1 x):
13 Dierenial and inegral inequaliies 67 Finally, in order o show ha for 2a <2a b+a he esimae (1) is beer b a han (6), we haveoprove he inequaliy e (2a )=(a+b) < 2a e(2a )=(2a) : Keeping a and xed, le us increase b unil =2a b+a (hen he lef-hand side b a of he inequaliy increases). Then our inequaliy coincides wih (24) and he claim follows. REFERENCES 1. F. Conrad, B. Rao: Decay of soluions of wave equaions in a sar-shaped domain wih nonlinear boundary feedback. Asympoic Anal., 7 (1993), 159{ A. Haraux: Oscillaions forcees pour cerains sysemes dissipaifs non lineaires. Publicaion du Laboraoire d'analyse Numerique No. 71, Universie Pierre e Marie Curie, Paris, A. Haraux:,Semi-groupes lineaires e equaions d'evoluion lineaires periodiques. Publicaion du Laboraoire d'analyse Numerique No. 711, Universie Pierre e Marie Curie, Paris, A. Haraux, E. Zuazua: Decay esimaes for some semilinear damped hyperbolic problems. Arch. Ra. Mech. Anal. (19), 191{ V. Komornik, E. Zuazua: A direc mehod for he boundary sabilizaion of he wave equaion. J. Mah. Pures Appl., 69 (199), 33{ V. Komornik: Rapid boundary sabilizaion of he wave equaion. SIAM J. Conrol Op., 29 (1991), 197{2. 7. V. Komornik: On he nonlinear boundary sabilizaion of he wave equaion. Chin. Ann. of Mah. 14B:2 (1993), 153{164.. V. Komornik: On he nonlinear boundary sabilizaion of Kirchho plaes. Nonlinear Di. Equaions and Appl. (NoDEA) 1 (1994), 323{ V. Komornik: Boundary sabilizaion, observaion and conrol of Maxwell's equaions. PanAmerican Mah. J., 4 (1994) No. 4, 47{ J. Lagnese: Boundary Sabilizaion of Thin Plaes. SIAM Sudies in Appl. Mah., Philadelphia, E. Zuazua: Uniform sabilizaion of he wave equaion by nonlinear boundary feedback. SIAM J. Conrol Op. 2 (199), 265{26. Isiu de Recherche Mahemaique Avancee, (Received Sepember 15, 1995) Universie Louis Paseur e C.N.R.S, 7, rue Rene Descares, 674 Srasbourg Cedex, France
The 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 information4 Sequences of measurable functions
4 Sequences of measurable funcions 1. Le (Ω, A, µ) be a measure space (complee, afer a possible applicaion of he compleion heorem). In his chaper we invesigae relaions beween various (nonequivalen) convergences
More informationHamilton- J acobi Equation: Weak S olution We continue the study of the Hamilton-Jacobi equation:
M ah 5 7 Fall 9 L ecure O c. 4, 9 ) Hamilon- J acobi Equaion: Weak S oluion We coninue he sudy of he Hamilon-Jacobi equaion: We have shown ha u + H D u) = R n, ) ; u = g R n { = }. ). In general we canno
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 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 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 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 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 informationMath 334 Fall 2011 Homework 11 Solutions
Dec. 2, 2 Mah 334 Fall 2 Homework Soluions Basic Problem. Transform he following iniial value problem ino an iniial value problem for a sysem: u + p()u + q() u g(), u() u, u () v. () Soluion. Le v u. Then
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 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 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 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 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 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 informationHamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t
M ah 5 2 7 Fall 2 0 0 9 L ecure 1 0 O c. 7, 2 0 0 9 Hamilon- J acobi Equaion: Explici Formulas In his lecure we ry o apply he mehod of characerisics o he Hamilon-Jacobi equaion: u + H D u, x = 0 in R n
More informationLecture 20: Riccati Equations and Least Squares Feedback Control
34-5 LINEAR SYSTEMS Lecure : Riccai Equaions and Leas Squares Feedback Conrol 5.6.4 Sae Feedback via Riccai Equaions A recursive approach in generaing he marix-valued funcion W ( ) equaion for i for he
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 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 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 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 informationSOLUTIONS TO ECE 3084
SOLUTIONS TO ECE 384 PROBLEM 2.. For each sysem below, specify wheher or no i is: (i) memoryless; (ii) causal; (iii) inverible; (iv) linear; (v) ime invarian; Explain your reasoning. If he propery is no
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 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 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 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 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 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 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 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 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 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 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 informationBoundedness and Stability of Solutions of Some Nonlinear Differential Equations of the Third-Order.
Boundedness Sabili of Soluions of Some Nonlinear Differenial Equaions of he Third-Order. A.T. Ademola, M.Sc. * P.O. Arawomo, Ph.D. Deparmen of Mahemaics Saisics, Bowen Universi, Iwo, Nigeria. Deparmen
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 informationSome Ramsey results for the n-cube
Some Ramsey resuls for he n-cube Ron Graham Universiy of California, San Diego Jozsef Solymosi Universiy of Briish Columbia, Vancouver, Canada Absrac In his noe we esablish a Ramsey-ype resul for cerain
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 informationEchocardiography Project and Finite Fourier Series
Echocardiography Projec and Finie Fourier Series 1 U M An echocardiagram is a plo of how a porion of he hear moves as he funcion of ime over he one or more hearbea cycles If he hearbea repeas iself every
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 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 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 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 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 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 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 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 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 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 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 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 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 information23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes
Represening Periodic Funcions by Fourier Series 3. Inroducion In his Secion we show how a periodic funcion can be expressed as a series of sines and cosines. We begin by obaining some sandard inegrals
More informationGMM - Generalized Method of Moments
GMM - Generalized Mehod of Momens Conens GMM esimaion, shor inroducion 2 GMM inuiion: Maching momens 2 3 General overview of GMM esimaion. 3 3. Weighing marix...........................................
More informationA NOTE ON THE STRUCTURE OF BILATTICES. A. Avron. School of Mathematical Sciences. Sackler Faculty of Exact Sciences. Tel Aviv University
A NOTE ON THE STRUCTURE OF BILATTICES A. Avron School of Mahemaical Sciences Sacler Faculy of Exac Sciences Tel Aviv Universiy Tel Aviv 69978, Israel The noion of a bilaice was rs inroduced by Ginsburg
More informationAn Introduction to Backward Stochastic Differential Equations (BSDEs) PIMS Summer School 2016 in Mathematical Finance.
1 An Inroducion o Backward Sochasic Differenial Equaions (BSDEs) PIMS Summer School 2016 in Mahemaical Finance June 25, 2016 Chrisoph Frei cfrei@ualbera.ca This inroducion is based on Touzi [14], Bouchard
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 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 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 informationChapter 6. Systems of First Order Linear Differential Equations
Chaper 6 Sysems of Firs Order Linear Differenial Equaions We will only discuss firs order sysems However higher order sysems may be made ino firs order sysems by a rick shown below We will have a sligh
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 informationTHE WAVE EQUATION. part hand-in for week 9 b. Any dilation v(x, t) = u(λx, λt) of u(x, t) is also a solution (where λ is constant).
THE WAVE EQUATION 43. (S) Le u(x, ) be a soluion of he wave equaion u u xx = 0. Show ha Q43(a) (c) is a. Any ranslaion v(x, ) = u(x + x 0, + 0 ) of u(x, ) is also a soluion (where x 0, 0 are consans).
More informationTwo Coupled Oscillators / Normal Modes
Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own
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 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 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 informationExpert Advice for Amateurs
Exper Advice for Amaeurs Ernes K. Lai Online Appendix - Exisence of Equilibria The analysis in his secion is performed under more general payoff funcions. Wihou aking an explici form, he payoffs of he
More informationt 2 B F x,t n dsdt t u x,t dxdt
Evoluion Equaions For 0, fixed, le U U0, where U denoes a bounded open se in R n.suppose ha U is filled wih a maerial in which a conaminan is being ranspored by various means including diffusion and convecion.
More informationMemoirs on Dierential Equations and Mathematical Physics Volume 11, 1997, 9{46 Dimitri Dzhgarkava PROBLEM OF OPTIMAL CONTROL WITH ONE-SIDED MIXED REST
Memoirs on Dierenial Equaions and Mahemaical Physics Volume 11, 1997, 9{46 Dimiri Dzhgarkava PROBLEM OF OPTIMAL CONTROL WITH ONE-SIDED MIXED RESTRICTIONS FOR CONTROLLED OBJECTS DESCRIBED BY INTEGRAL EQUATIONS
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 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 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 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 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 informationNotes for Lecture 17-18
U.C. Berkeley CS278: Compuaional Complexiy Handou N7-8 Professor Luca Trevisan April 3-8, 2008 Noes for Lecure 7-8 In hese wo lecures we prove he firs half of he PCP Theorem, he Amplificaion Lemma, up
More informationMATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018
MATH 5720: Gradien Mehods Hung Phan, UMass Lowell Ocober 4, 208 Descen Direcion Mehods Consider he problem min { f(x) x R n}. The general descen direcions mehod is x k+ = x k + k d k where x k is he curren
More informationSections 2.2 & 2.3 Limit of a Function and Limit Laws
Mah 80 www.imeodare.com Secions. &. Limi of a Funcion and Limi Laws In secion. we saw how is arise when we wan o find he angen o a curve or he velociy of an objec. Now we urn our aenion o is in general
More informationt + t sin t t cos t sin t. t cos t sin t dt t 2 = exp 2 log t log(t cos t sin t) = Multiplying by this factor and then integrating, we conclude that
ODEs, Homework #4 Soluions. Check ha y ( = is a soluion of he second-order ODE ( cos sin y + y sin y sin = 0 and hen use his fac o find all soluions of he ODE. When y =, we have y = and also y = 0, so
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 informationSMT 2014 Calculus Test Solutions February 15, 2014 = 3 5 = 15.
SMT Calculus Tes Soluions February 5,. Le f() = and le g() =. Compue f ()g (). Answer: 5 Soluion: We noe ha f () = and g () = 6. Then f ()g () =. Plugging in = we ge f ()g () = 6 = 3 5 = 5.. There is a
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 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 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 informationPhysics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle
Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,
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 informationMath 315: Linear Algebra Solutions to Assignment 6
Mah 35: Linear Algebra s o Assignmen 6 # Which of he following ses of vecors are bases for R 2? {2,, 3, }, {4,, 7, 8}, {,,, 3}, {3, 9, 4, 2}. Explain your answer. To generae he whole R 2, wo linearly independen
More informationSupplement for Stochastic Convex Optimization: Faster Local Growth Implies Faster Global Convergence
Supplemen for Sochasic Convex Opimizaion: Faser Local Growh Implies Faser Global Convergence Yi Xu Qihang Lin ianbao Yang Proof of heorem heorem Suppose Assumpion holds and F (w) obeys he LGC (6) Given
More informationThe following report makes use of the process from Chapter 2 in Dr. Cumming s thesis.
Zaleski 1 Joseph Zaleski Mah 451H Final Repor Conformal Mapping Mehods and ZST Hele Shaw Flow Inroducion The Hele Shaw problem has been sudied using linear sabiliy analysis and numerical mehods, bu a novel
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 informationTHE 2-BODY PROBLEM. FIGURE 1. A pair of ellipses sharing a common focus. (c,b) c+a ROBERT J. VANDERBEI
THE 2-BODY PROBLEM ROBERT J. VANDERBEI ABSTRACT. In his shor noe, we show ha a pair of ellipses wih a common focus is a soluion o he 2-body problem. INTRODUCTION. Solving he 2-body problem from scrach
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 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 informationIMPLICIT AND INVERSE FUNCTION THEOREMS PAUL SCHRIMPF 1 OCTOBER 25, 2013
IMPLICI AND INVERSE FUNCION HEOREMS PAUL SCHRIMPF 1 OCOBER 25, 213 UNIVERSIY OF BRIISH COLUMBIA ECONOMICS 526 We have exensively sudied how o solve sysems of linear equaions. We know how o check wheher
More informationInstructor: Barry McQuarrie Page 1 of 5
Procedure for Solving radical equaions 1. Algebraically isolae one radical by iself on one side of equal sign. 2. Raise each side of he equaion o an appropriae power o remove he radical. 3. Simplify. 4.
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 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 informationApproximation Algorithms for Unique Games via Orthogonal Separators
Approximaion Algorihms for Unique Games via Orhogonal Separaors Lecure noes by Konsanin Makarychev. Lecure noes are based on he papers [CMM06a, CMM06b, LM4]. Unique Games In hese lecure noes, we define
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 informationNONSMOOTHING IN A SINGLE CONSERVATION LAW WITH MEMORY
Elecronic Journal of Differenial Equaions, Vol. 2(2, No. 8, pp. 8. ISSN: 72-669. URL: hp://ejde.mah.sw.edu or hp://ejde.mah.un.edu fp ejde.mah.sw.edu ejde.mah.un.edu (login: fp NONSMOOTHING IN A SINGLE
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 information