Successive ApproxiInations and Osgood's Theorenl

Size: px
Start display at page:

Download "Successive ApproxiInations and Osgood's Theorenl"

Transcription

1 Revisa de la Unin Maemaica Argenina Vlumen 40, Niimers 3 y 4, Successive ApprxiInains and Osgd's Therenl Calix P. Caldern Virginia N. Vera de Seri.July 29, 1996 Absrac The Picard's mehd fr slving Y' = f (x, y), y (x) = Y, is cnsidered here fr If (x, YI) - f (x, Y2)1 :::; 'P (IYI - Y21). I is shwn ha fr raher general Osgd's funcins 'P, he difference f w successive apprximains cnverges a expnenially decreasing rae. An applicain parablic parial differenial equains is given as well. Key Wrds: Successive apprximains. Thereical apprxi. main f sluins. Osgd's funcins. 1 Inrducin In a landmark paper W. Osgd (1898) inrduced a cndiin weaker han he well knwn Cauchy-Lipschiz ne ha guaranees he uniqueness f he sluin f he iniial value prblem fr a firs rder equain. Laer, A. Winner (1946) shwed ha Osgd's uniqueness cndiin implies he cnvergence f he successive apprximain n a sufficienly small inerval. Laer n, J. Lasalle (1949) exended Winner's mehd he case f he uniqueness cndiin fr he sluin given by P. Mnel and M. Nagum in Lasalle's mehd is essenially Winner's bu adaped a differen cndiin. One f he imprvemens inrduced by Lasalle is he fac ha he zer apprximain can be chsen be anyne bu sufficienly small in L 1991 Mahemaics Subjec Classificain: Primary 34A45 Secndary 35K05

2 74 nrm. Lasalle and Winner's papers raise quesins cncerning he speed f he cnvergence f he successive apprximains. I is he aim f his paper answer hese quesins fr he cases f raher general Osgd's funcins. In fac, we shw ha in cases such as r.p () = Ilgl,8 0 < f3 ::; 1, he difference f w successive apprximains IYn+! - Yn I cnverges a expnenially decreasing speed. The resul in his paper can be easily exended he case f firs rder sysems very much in he same way as Lasalle (1949). Fr such a generalizain we refer he reader he paper by Lasalle.. We will deal wih he equain Y' = f (x, y) wih iniial cndiin Y (x) = Y. f is a cninuus funcin which verifies ha If (x, yj) - f (x, Y2)1 ::; r.p (IYI - Y2J), where a ::; x ::; band c ::; Y ::; d. r.p saisfies he mdified Osgd's cndiins belw in 2.1. Fr he sake f simpliciy we may assume ha -a ::; x ::; a, -c ::; Y ::; c and X = 0, Y = O. We cnsider he successive apprximains x Yn+! (x) = J and sudy he mdali.y f cnvergence f f (, Yn ()) d fr Ixl ::; {j and {j > 0 suiably small. Wihin ha range we will have fr n ;:::: n, fr sme n, r,o < r < I, and C a psiive cnsan. Cnsider he auxiliary ierain x Zn+! (4) = J r.p (zn ()) d, in general Wn ::; Zn. We sudy he speed f cnvergence zer f Zn (x), which aumaically will imply he resul. In he final secin we briefly indicae sme her applicains parablic parial differenial equains. '(1)

3 75 2 Osgd's funcins A real valued funcin <p is an Osgd's funcin if he fllwing cndiins are me: 1) <p is nn-negaive cninuus and mnne n (0,6), fr sme 6 > O. 2) f; <p(~) = 00, fr any :, 0 < : ~ 6. Remark 1 1) and 2) abve imply immediaely ha limx + <p (x) = 0 and ha i.p is nn-decreasing. We will define <p (0) =. 2.1 Mdified Osgd's cndiin Thrughu his paper we shall be cncerned wih Osgd's funcins f he ype b i.p() = JW~s) ds, where b > 0 is a given cnsan. W is a nn-negaive cninuus nndecreasing funcin n [0, b], such ha Nice ha i.p (0+) = O. Frm nw n we will assume b ~ 1. b J W ~s) ds =00. D Occasinally we use he nain (Y () = f w(s) ds.. 8 Lemma 1 The funcin i.p saisfies he fllwing prperies: (i) There is sme a, a> 0, such ha <p (a) = a. (ii) lim <p' () > l. -+O+ There is sme 6,0 < 6 ~ a, such ha fr,o < ~ 6, i hlds ha (iii)i.p' and (Yare decreasing, (iv) (Y (n) ~ n(y (b,,;;:l ), fr all n = 1,2,... (v) he quien ;,<l) = :Jl) is bunded, and (vi)<p2f) = a2 () is increasing. b

4 76 Prf. (i) hlds because 'P (0) = 0, 'P (b) = 0 and 'P is cncave. (ii) and (iii) fllw frm he represenain 'P' () = a () - w () = lb W (s ) ds - w (). s (iv) We shw he case b = 1, he hers fllw by cnsidering he funcin it (T) = a (bt) and he change f variable = bt. Le a, (3, 0 < a, (3 ~ 1, hen J w (as) ds + J w (s) ds < J w (s) ds + J w (s) ds s s - s s (3 0: (3 0: a (a) + a (,8). ( ) ~.. u() 1 0+ V <p'() = u()-w() ---+,as ---+ (vi) i (a ()2) = a ()(a() - 2w ()) >. 2.2 Ms cmmn mdified Osgd's funcins I is sraighfrward shw ha he fllwing funcins saisfy he mdified Osgd's cndiins: 'Pk () = (lg (1/ ) )(31 (lg lg (l/))f32... (lg lg lg (1 /) )(3" fr sme 0 ~,8i < 1, i = 1,..., k - 1,0 <,8k ~ 1, k = 1,2,... These are he ms cmmn mdified Osgd's funcins. Observe ha fr all f hem, he cnsan b saisfies ha b ~ 1. 3 Auxiliary lemmaa Frm nw n we will assume b ~ 1. The fllwing lemmaa are he echnical ls fr prving ha Ilwnll ~ Crn fr sme r, 0 < r < 1, C a psiive cnsan. Assume ha 0 < ~ I), where I) > 0 is as in Lemma 1.

5 77 L (( )n) A <p(x+1 emma 2 'P >''P x ~ nb x ' fr any >. ~ 1,n = 1,2,... Prf. Frm 'P () = fj () and Lemma 1 ( iii), (iv) i fllws ha 'P (>''P (x) - >''P (x fj (>''P (x) - >''P (x fj (>.xnfj (x)n) < >''P (x fj (xn) < n~'p (x (J (x) >. 'P (x+1 - n- b x L x ()n 1 <p(:i:),,+l <p(x)n+1 _ emma 3 10 'P d ~ <p'(x) n+1 ~ n+1,n - 1,2,... Prf. Lemma 1 (iii) and (ii) imply ha r 'P ( d < r 'P ( <p' () d = _1_'P (x+1 < 'P (x+1 J - J 'P' (x) 'P' (x) n n + 1 Lemma 4 There exiss a psiive cnsan C such ha I: ~ d ~ n~l 'P (x) n,,n = 1,2,... 'Prf. Lemma 1 (v)-{vi) and Lemma 3 give r 'P(r d J _ r 'P ()2 'P (-2 d J < 'P (X)2 r 'P (r-2 d x J 'P(X)2 1 'P(xr- 1 < '-x-'p'(x) n-1 C (-n < n_ 1'P x ). Lemma 5 Le Z be a nn-negaive funcin defined fr Ixl ~ fj, Z (x) ~ 1], x fj and 1] small enugh. Suppse Zn+ 1 (x) = I 'P (Zn ()) d, hen,

6 78 ~ Zl (x) ~X, ~ Zn(X) ~ cn-2cp(x)", n = 2,3,..., C > 1 a suiable cnsan. Prf. cp is a cninuus funcin wih cp (0) = 0, s fr 11 > 0 sufficienly small, IX ~ Zl (x) ~ I cp (1IZID d ~ x.., Pu C = ~', where 0' is as in Lemma 4 and such ha 0' > b. Fr n = 2, we use Lemma 3 ge x x 1 ~ Z2 (x) ~ I cp (Zl (» d ~ I cp () d ~ "2CP (X)2 ~ cp (X)2.. 0 Nw, by inducin n n, fr n Z 2, Z < zn+1 (x) == I cp{zn (» d ~ I 'P (cn-2cp() d 0 cn-2 IX cp ()"+l < n-- d b < cn-2 C' ()n+1 n---cp x b n _ n-lcp (x)"+1, IX because f Lemmas 2 and 4. 4 Rae f cnvergence f he successive apprximains In rder analyze he rae f cnvergence f Wn, bserve ha IX W'HI (x) ~ I If (, Yn+l (» - f (, Yn (»1 d ~ I cp (wn (» d. 0 Z

7 79 We will cnsider a differen ierain. If we begin wih small iniial values, namely: W (x) $.1], fr Ixl $. 6, we sudy he auxiliary ierain z Zn+l (x) = J I' (Zn ()) d, where Z = 1]. I is clear ha WI $. Zl and, in general Wn $. Zn, which is a cnsequence f he mnniciy f <p Then i will be enugh prve he esimae (1) fr Zn. I will be wrh nice ha because f he cncaviy f <p, plus <p (0) =. The nex sep will be sudy he speed f cnvergence zer f Zn (x), Ixl ::; 6 and shw ha fr Zn (x) he esimae (1) is valid. Indeed, frm Lemma 5, here exiss a cnsan C > 1 such ha 0 $. Zn (x) $. C n - 2<p (x. By he cninuiy f <p and he fac ha <p(0) = 0, fr any r, 0 < r < 1, here is sme 6',0 < 6' $. 6, fr which C<p (x) $. r, fr Ixl $. 6'. Thus, we have prven he fllwing herem: Therem 6 Le f be a cninuus funcins n he recangle R = [-c, c] x [-d,d]. Suppse ha fr Ixl$. c,iyil $. d, i = 1,2, where <p verifies he mdifiea Osgd's cndiins saed in secin 2.1. Then, he successive apprximains z YnH (x) = J IYl $. 1],1]> 0 sufficienly small, saisfy f (, Yn ()) d, 6. fr sme r,o < r < 1, sme C large enugh and Ixl $. 6, fr sme psiive

8 80 5 An applicain parial differenial equains Cnsider he fllwing parablic parial differenial equain U=~u+F(u,x,), U(x,O) = O. Assume ha F is a cninuus funcin ha saisfies where IIIL!; is an ad-hc nrm in he space variables and i.p is a mdified Osgd's funcin as in secin 2.l. Le K (x, ) be he usual L1 fundamenal sluin! and implemen he ierains Un+1 (x, ) = J fa"" K(x - y, - T) F (un (y, T), y, T) dydt, U is chsen be C in R m wih small L nrm. Then I\Un+1 -'- unll x, which is a funcin f, saisfies ha IIUn+l - unllx S; J llfa", K (x - y, - T) (F (un, y, T) - F (un_i, y, T)) dy IL dt < jllf (un,., T) - F (un-i," T)llx dt < J'P (liun - un-illx) dt. Wih a similar prcedure as he ne emplyed befre, by chsing U suiably small in he apprpriae ad-hc nrm, i fllws ha fr 0 S; < {;, sme {; > 0 and sme r, 0 < r < 1. 1 As i is well knwn, B. Frank Jnffi has cnsruced fundamenal sluins ha are n f he usual ype.

9 81 References [1] Iyanaga, S., Uber die Uniasbedingungen der Lasung der DifIerenialgleichung, Jap. J. Mah. 5 (1928), [2] LaSalle, J. Uniqueness herems and successive apprximains, Annals f Mahemaics 50 (1949), [3] Mnel, P., Sur 1 'inegrale superieure e 1 'inegrale inferieure d 'une equain difierenielle, Bull. Sci. Mah. (2) 50 (1926), [4] Muller, M., Uber das Fundamenalherem in der Therie der gewahnlichen DifIerenialgleichungen, Mah. Zei. 26 (1927), [5] Nagum, M., Eine hinreichende Bedingung fur die Uni a der Lasung vn DifIerenialgleichungen erser Ordnung, Jap. J. Mah. 3 (1926), [6] Osgd, W., Beweise der Exisenz einer Lasung der DifIerenialgleichungen dy/dx = f(x,y) hne Hinzunahme der Cauchy-Lipschizschen Bedingung, Mnashefe fur Mah. und Physik 9 (1898), [7] Perrn, 0., Eine hinreichende Bed.ingung fur die Unia der Lasung vn DifIerenialgleichungen erser Ordnung, Mah. Zei. 28 (1928), [8] Winner, A., On he cnvergence f successive apprximains, Amer. J. Mah. 68 (1946), Insiu de Ciencias Basicas, Universidad Nacinal de Cuy Deparmen f Mahemaics, Saisics and Cmpuer Sciences, Universiy f illinis a Chicag Faculad de Ciencias Ecnmicas, Universidad Nacinal de Cuy Cenr U niversiari 5500 Mendza Argenina address:vvera@raiz.uncu.edu.ar Recibid en Ags de 1996

MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.265/15.070J Fall 2013 Lecture 15 10/30/2013. Ito integral for simple processes

MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.265/15.070J Fall 2013 Lecture 15 10/30/2013. Ito integral for simple processes MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.65/15.7J Fall 13 Lecure 15 1/3/13 I inegral fr simple prcesses Cnen. 1. Simple prcesses. I ismery. Firs 3 seps in cnsrucing I inegral fr general prcesses 1 I inegral

More information

Brace-Gatarek-Musiela model

Brace-Gatarek-Musiela model Chaper 34 Brace-Gaarek-Musiela mdel 34. Review f HJM under risk-neural IP where f ( T Frward rae a ime fr brrwing a ime T df ( T ( T ( T d + ( T dw ( ( T The ineres rae is r( f (. The bnd prices saisfy

More information

Lecture 4 ( ) Some points of vertical motion: Here we assumed t 0 =0 and the y axis to be vertical.

Lecture 4 ( ) Some points of vertical motion: Here we assumed t 0 =0 and the y axis to be vertical. Sme pins f erical min: Here we assumed and he y axis be erical. ( ) y g g y y y y g dwnwards 9.8 m/s g Lecure 4 Accelerain The aerage accelerain is defined by he change f elciy wih ime: a ; In analgy,

More information

10.7 Temperature-dependent Viscoelastic Materials

10.7 Temperature-dependent Viscoelastic Materials Secin.7.7 Temperaure-dependen Viscelasic Maerials Many maerials, fr example plymeric maerials, have a respnse which is srngly emperaure-dependen. Temperaure effecs can be incrpraed in he hery discussed

More information

Convex Stochastic Duality and the Biting Lemma

Convex Stochastic Duality and the Biting Lemma Jurnal f Cnvex Analysis Vlume 9 (2002), N. 1, 237 244 Cnvex Schasic Dualiy and he Biing Lemma Igr V. Evsigneev Schl f Ecnmic Sudies, Universiy f Mancheser, Oxfrd Rad, Mancheser, M13 9PL, UK igr.evsigneev@man.ac.uk

More information

Answers: ( HKMO Heat Events) Created by: Mr. Francis Hung Last updated: 21 September 2018

Answers: ( HKMO Heat Events) Created by: Mr. Francis Hung Last updated: 21 September 2018 nswers: (009-0 HKMO Hea Evens) reaed by: Mr. Francis Hung Las updaed: Sepember 08 09-0 Individual 6 7 7 0 Spare 8 9 0 08 09-0 8 0 0.8 Spare Grup 6 0000 7 09 8 00 9 0 0 Individual Evens I In hw many pssible

More information

5.1 Angles and Their Measure

5.1 Angles and Their Measure 5. Angles and Their Measure Secin 5. Nes Page This secin will cver hw angles are drawn and als arc lengh and rains. We will use (hea) represen an angle s measuremen. In he figure belw i describes hw yu

More information

Productivity changes of units: A directional measure of cost Malmquist index

Productivity changes of units: A directional measure of cost Malmquist index Available nline a hp://jnrm.srbiau.ac.ir Vl.1, N.2, Summer 2015 Jurnal f New Researches in Mahemaics Science and Research Branch (IAU Prduciviy changes f unis: A direcinal measure f cs Malmquis index G.

More information

AP Physics 1 MC Practice Kinematics 1D

AP Physics 1 MC Practice Kinematics 1D AP Physics 1 MC Pracice Kinemaics 1D Quesins 1 3 relae w bjecs ha sar a x = 0 a = 0 and mve in ne dimensin independenly f ne anher. Graphs, f he velciy f each bjec versus ime are shwn belw Objec A Objec

More information

Stability of the SDDRE based Estimator for Stochastic Nonlinear System

Stability of the SDDRE based Estimator for Stochastic Nonlinear System 26 ISCEE Inernainal Cnference n he Science f Elecrical Engineering Sabiliy f he SDDRE based Esimar fr Schasic Nnlinear Sysem Ilan Rusnak Senir Research Fellw, RAFAEL (63, P.O.Bx 225, 322, Haifa, Israel.;

More information

Lyapunov Stability Stability of Equilibrium Points

Lyapunov Stability Stability of Equilibrium Points Lyapunv Stability Stability f Equilibrium Pints 1. Stability f Equilibrium Pints - Definitins In this sectin we cnsider n-th rder nnlinear time varying cntinuus time (C) systems f the frm x = f ( t, x),

More information

- polynomial with real coefficients.

- polynomial with real coefficients. THE ASYMPTOTIC BEHAVIOUR OF SOLUTIONS OF BOUNDARY VALUE PROBLEMS FOR LINEARIZED KdV EQUATION Barabash Tayana O., Eidel'man Samuil D. (Ukraine,Kiev) I.Saemen fhe prblem.we invesigaehe asympicbehaviur (when

More information

PRINCE SULTAN UNIVERSITY Department of Mathematical Sciences Final Examination Second Semester (072) STAT 271.

PRINCE SULTAN UNIVERSITY Department of Mathematical Sciences Final Examination Second Semester (072) STAT 271. PRINCE SULTAN UNIVERSITY Deparmen f Mahemaical Sciences Final Examinain Secnd Semeser 007 008 (07) STAT 7 Suden Name Suden Number Secin Number Teacher Name Aendance Number Time allwed is ½ hurs. Wrie dwn

More information

The Components of Vector B. The Components of Vector B. Vector Components. Component Method of Vector Addition. Vector Components

The Components of Vector B. The Components of Vector B. Vector Components. Component Method of Vector Addition. Vector Components Upcming eens in PY05 Due ASAP: PY05 prees n WebCT. Submiing i ges yu pin ward yur 5-pin Lecure grade. Please ake i seriusly, bu wha cuns is wheher r n yu submi i, n wheher yu ge hings righ r wrng. Due

More information

Kinematics Review Outline

Kinematics Review Outline Kinemaics Review Ouline 1.1.0 Vecrs and Scalars 1.1 One Dimensinal Kinemaics Vecrs have magniude and direcin lacemen; velciy; accelerain sign indicaes direcin + is nrh; eas; up; he righ - is suh; wes;

More information

99 Union Matematica Argen tina Volumen 4 1, 1, PROBLEMS FOR A SE M I - I N F I N ITE STR I P WITH A N O N - U N I F O R M H EAT S O U RCE

99 Union Matematica Argen tina Volumen 4 1, 1, PROBLEMS FOR A SE M I - I N F I N ITE STR I P WITH A N O N - U N I F O R M H EAT S O U RCE Revisa de la 99 Unin Maemaica Argen ina Vlumen 4 1 1 1 998 S O M E N O N L I N EA R H EAT C O N D U CTI O N PROBLEMS FOR A SE M I - I N F I N ITE STR I P WITH A N O N - U N I F O R M H EAT S O U RCE Dming

More information

E Z, (n l. and, if in addition, for each integer n E Z there is a unique factorization of the form

E Z, (n l. and, if in addition, for each integer n E Z there is a unique factorization of the form Revista Clmbiana de Matematias Vlumen II,1968,pags.6-11 A NOTE ON GENERALIZED MOBIUS f-functions V.S. by ALBIS In [1] the ncept f a cnjugate pair f sets f psi tive integers is int~dued Briefly, if Z dentes

More information

(1.1) (f'(z),y-x)>f(y)-f(x).

(1.1) (f'(z),y-x)>f(y)-f(x). PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Vlume 122, Number 4, December 1994 MEAN VALUE INEQUALITIES F. H. CLARKE AND YU. S. LEDYAEV (Cmmunicaed by Andrew Bruckner) Absrac. We prve a new ype f mean

More information

Numerical solution of some types of fractional optimal control problems

Numerical solution of some types of fractional optimal control problems Numerical Analysis and Scienific mpuing Preprin Seria Numerical sluin f sme ypes f fracinal pimal cnrl prblems N.H. Sweilam T.M. Al-Ajmi R.H.W. Hppe Preprin #23 Deparmen f Mahemaics Universiy f Husn Nvember

More information

arxiv:math/ v1 [math.nt] 3 Nov 2005

arxiv:math/ v1 [math.nt] 3 Nov 2005 arxiv:mah/0511092v1 [mah.nt] 3 Nov 2005 A NOTE ON S AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION D. A. GOLDSTON AND S. M. GONEK Absrac. Le πs denoe he argumen of he Riemann zea-funcion a he poin 1 + i. Assuming

More information

A NOTE ON THE EXISTENCE OF AN OPTIMAL SOLUTION FOR CONCAVE INFINITE HORIZON ECONOMIC MODELS

A NOTE ON THE EXISTENCE OF AN OPTIMAL SOLUTION FOR CONCAVE INFINITE HORIZON ECONOMIC MODELS A NOTE ON THE EXISTENCE OF AN OPTIMAL SOLUTION FOR CONCAVE INFINITE HORIZON ECONOMIC MODELS by Smdeb Lahiri Discussin Paper N. 221, Sepember 1985 Cener fr Ecnmic Research Deparmen f Ecnmics Universiy f

More information

ISSN: (Online) GAP FUNCTION ON VARIATIONAL-LIKE INEQUALITY IN BANACH SPACE ABSTRACT

ISSN: (Online) GAP FUNCTION ON VARIATIONAL-LIKE INEQUALITY IN BANACH SPACE ABSTRACT Indian JSciRes (: 93-99, 5 ISSN: 976-876 (Prin ISSN: 5-38(Onine GAP FUNCTION ON VARIATIONAL-LIE INEQUALITY IN BANACH SPACE ABDUL RAOUF a AND SHIVANI SHARMA b ab Deparmen Mahemaics, Gv P G Cege Rauri, Rauri,

More information

f t(y)dy f h(x)g(xy) dx fk 4 a. «..

f t(y)dy f h(x)g(xy) dx fk 4 a. «.. CERTAIN OPERATORS AND FOURIER TRANSFORMS ON L2 RICHARD R. GOLDBERG 1. Intrductin. A well knwn therem f Titchmarsh [2] states that if fel2(0, ) and if g is the Furier csine transfrm f/, then G(x)=x~1Jx0g(y)dy

More information

A Note on the Approximation of the Wave Integral. in a Slightly Viscous Ocean of Finite Depth. due to Initial Surface Disturbances

A Note on the Approximation of the Wave Integral. in a Slightly Viscous Ocean of Finite Depth. due to Initial Surface Disturbances Applied Mahemaical Sciences, Vl. 7, 3, n. 36, 777-783 HIKARI Ld, www.m-hikari.cm A Ne n he Apprximain f he Wave Inegral in a Slighly Viscus Ocean f Finie Deph due Iniial Surface Disurbances Arghya Bandypadhyay

More information

Motion Along a Straight Line

Motion Along a Straight Line PH 1-3A Fall 010 Min Alng a Sraigh Line Lecure Chaper (Halliday/Resnick/Walker, Fundamenals f Physics 8 h ediin) Min alng a sraigh line Sudies he min f bdies Deals wih frce as he cause f changes in min

More information

Research & Reviews: Journal of Statistics and Mathematical Sciences

Research & Reviews: Journal of Statistics and Mathematical Sciences Research & Reviews: Jural f Saisics ad Mahemaical Scieces iuus Depedece f he Slui f A Schasic Differeial Equai Wih Nlcal diis El-Sayed AMA, Abd-El-Rahma RO, El-Gedy M Faculy f Sciece, Alexadria Uiversiy,

More information

Properties Of Solutions To A Generalized Liénard Equation With Forcing Term

Properties 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 information

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales

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 information

GAMS Handout 2. Utah State University. Ethan Yang

GAMS Handout 2. Utah State University. Ethan Yang Uah ae Universiy DigialCmmns@UU All ECAIC Maerials ECAIC Repsiry 2017 GAM Handu 2 Ehan Yang yey217@lehigh.edu Fllw his and addiinal wrs a: hps://digialcmmns.usu.edu/ecsaic_all Par f he Civil Engineering

More information

THE DETERMINATION OF CRITICAL FLOW FACTORS FOR NATURAL GAS MIXTURES. Part 3: The Calculation of C* for Natural Gas Mixtures

THE DETERMINATION OF CRITICAL FLOW FACTORS FOR NATURAL GAS MIXTURES. Part 3: The Calculation of C* for Natural Gas Mixtures A REPORT ON THE DETERMINATION OF CRITICAL FLOW FACTORS FOR NATURAL GAS MIXTURES Par 3: The Calculain f C* fr Naural Gas Mixures FOR NMSPU Deparmen f Trade and Indusry 151 Buckingham Palace Rad Lndn SW1W

More information

Existence Theory of Second Order Random Differential Equations

Existence 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 information

Asymptotic instability of nonlinear differential equations

Asymptotic 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 information

Lecture 3: Resistive forces, and Energy

Lecture 3: Resistive forces, and Energy Lecure 3: Resisive frces, and Energy Las ie we fund he velciy f a prjecile ving wih air resisance: g g vx ( ) = vx, e vy ( ) = + v + e One re inegrain gives us he psiin as a funcin f ie: dx dy g g = vx,

More information

Module 4. Analysis of Statically Indeterminate Structures by the Direct Stiffness Method. Version 2 CE IIT, Kharagpur

Module 4. Analysis of Statically Indeterminate Structures by the Direct Stiffness Method. Version 2 CE IIT, Kharagpur Mdle Analysis f Saically Indeerminae Srcres by he Direc Siffness Mehd Versin CE IIT, Kharagr Lessn The Direc Siffness Mehd: Temerare Changes and Fabricain Errrs in Trss Analysis Versin CE IIT, Kharagr

More information

(Communicated at the meeting of September 25, 1948.) Izl=6 Izl=6 Izl=6 ~=I. max log lv'i (z)1 = log M;.

(Communicated at the meeting of September 25, 1948.) Izl=6 Izl=6 Izl=6 ~=I. max log lv'i (z)1 = log M;. Mathematics. - On a prblem in the thery f unifrm distributin. By P. ERDÖS and P. TURÁN. 11. Ommunicated by Prf. J. G. VAN DER CORPUT.) Cmmunicated at the meeting f September 5, 1948.) 9. Af ter this first

More information

SMKA NAIM LILBANAT KOTA BHARU KELANTAN. SEKOLAH BERPRESTASI TINGGI. Kertas soalan ini mengandungi 7 halaman bercetak.

SMKA NAIM LILBANAT KOTA BHARU KELANTAN. SEKOLAH BERPRESTASI TINGGI. Kertas soalan ini mengandungi 7 halaman bercetak. Name : Frm :. SMKA NAIM LILBANAT 55 KOTA BHARU KELANTAN. SEKOLAH BERPRESTASI TINGGI PEPERIKSAAN PERCUBAAN SPM / ADDITIONAL MATHEMATICS Keras ½ Jam ½ Jam Unuk Kegunaan Pemeriksa Arahan:. This quesin paper

More information

An Introduction to Malliavin calculus and its applications

An 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 information

An Introduction to Wavelet Analysis. with Applications to Vegetation Monitoring

An Introduction to Wavelet Analysis. with Applications to Vegetation Monitoring An Inrducin Wavele Analysis wih Applicains Vegeain Mniring Dn Percival Applied Physics Labrary, Universiy f Washingn Seale, Washingn, USA verheads fr alk available a hp://saff.washingn.edu/dbp/alks.hml

More information

ON STABILITY OF CONTROLLED SYSTEMS IN BANACH SPACES. M. Megan, Timi~oara, Romania. 1. Introduction

ON STABILITY OF CONTROLLED SYSTEMS IN BANACH SPACES. M. Megan, Timi~oara, Romania. 1. Introduction GLASNIK MATEMATICKI Vl. 18 (38) (1983), 187-201. ON STABILITY OF CONTROLLED SYSTEMS IN BANACH SPACES M. Megan, Timi~ara, Rmania Absrac. In his paper we sudy sabiliy prperies fr linear sysems, he evluin

More information

Predator - Prey Model Trajectories and the nonlinear conservation law

Predator - 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 information

On the Resistance of an Infinite Square Network of Identical Resistors (Theoretical and Experimental Comparison)

On the Resistance of an Infinite Square Network of Identical Resistors (Theoretical and Experimental Comparison) On he esisance f an Infinie Square Newrk f Idenical esisrs (Thereical and Experimenal Cmparisn) J. H. Asad, A. Sakai,. S. Hiawi and J. M. Khalifeh Deparmen f Phsics, Universi f Jrdan, Amman-1194, Jrdan.

More information

Homology groups of disks with holes

Homology groups of disks with holes Hmlgy grups f disks with hles THEOREM. Let p 1,, p k } be a sequence f distinct pints in the interir unit disk D n where n 2, and suppse that fr all j the sets E j Int D n are clsed, pairwise disjint subdisks.

More information

Perturbation approach applied to the asymptotic study of random operators.

Perturbation approach applied to the asymptotic study of random operators. Perturbatin apprach applied t the asympttic study f rm peratrs. André MAS, udvic MENNETEAU y Abstract We prve that, fr the main mdes f stchastic cnvergence (law f large numbers, CT, deviatins principles,

More information

ON THE ABSOLUTE CONVERGENCE OF A SERIES ASSOCIATED WITH A FOURIER SERIES. R. MOHANTY and s. mohapatra

ON THE ABSOLUTE CONVERGENCE OF A SERIES ASSOCIATED WITH A FOURIER SERIES. R. MOHANTY and s. mohapatra ON THE ABSOLUTE CONVERGENCE OF A SERIES ASSOCIATED WITH A FOURIER SERIES R. MOHANTY and s. mhapatra 1. Suppse/(i) is integrable L in ( ir, it) peridic with perid 2ir, and that its Furier series at / =

More information

Physics 111. Exam #1. September 28, 2018

Physics 111. Exam #1. September 28, 2018 Physics xam # Sepember 8, 08 ame Please read and fllw hese insrucins carefully: Read all prblems carefully befre aemping slve hem. Yur wrk mus be legible, and he rganizain clear. Yu mus shw all wrk, including

More information

Large-scale Distance Metric Learning with Uncertainty

Large-scale Distance Metric Learning with Uncertainty i Large-scale Disance Meric Learning wih Uncerainy Qi Qian Jiasheng Tang Ha Li Shenghu Zhu Rng Jin Alibaba Grup, Bellevue, WA, 98004, USA {qi.qian, jiasheng.js, liha.lh, shenghu.zhu, jinrng.jr}@alibaba-inc.cm

More information

A Generalized Schwarz Splitting Method Based on Hermite Collocation for Elliptic Boundary Value Problems

A Generalized Schwarz Splitting Method Based on Hermite Collocation for Elliptic Boundary Value Problems Purdue Universiy Purdue e-pubs Deparmen f Cmpuer Science Technical Reprs Deparmen f Cmpuer Science 1993 A Generalized Schwarz Spliing Mehd Based n Hermie Cllcain fr Ellipic Bundary Value Prblems Yu-Ling

More information

Generalized Chebyshev polynomials

Generalized 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 information

Physics Courseware Physics I Constant Acceleration

Physics Courseware Physics I Constant Acceleration Physics Curseware Physics I Cnsan Accelerain Equains fr cnsan accelerain in dimensin x + a + a + ax + x Prblem.- In he 00-m race an ahlee acceleraes unifrmly frm res his p speed f 0m/s in he firs x5m as

More information

CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS

CERTAIN 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 information

The lower limit of interval efficiency in Data Envelopment Analysis

The lower limit of interval efficiency in Data Envelopment Analysis Jurnal f aa nelpmen nalysis and ecisin Science 05 N. (05) 58-66 ailable nline a www.ispacs.cm/dea lume 05, Issue, ear 05 ricle I: dea-00095, 9 Pages di:0.5899/05/dea-00095 Research ricle aa nelpmen nalysis

More information

Solutions of Sample Problems for Third In-Class Exam Math 246, Spring 2011, Professor David Levermore

Solutions of Sample Problems for Third In-Class Exam Math 246, Spring 2011, Professor David Levermore Soluions of Sample Problems for Third In-Class Exam Mah 6, Spring, Professor David Levermore Compue he Laplace ransform of f e from is definiion Soluion The definiion of he Laplace ransform gives L[f]s

More information

Convergence of the Neumann series in higher norms

Convergence 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 information

Fractional Order Disturbance Observer based Robust Control

Fractional Order Disturbance Observer based Robust Control 201 Inernainal Cnference n Indusrial Insrumenain and Cnrl (ICIC) Cllege f Engineering Pune, India. May 28-30, 201 Fracinal Order Disurbance Observer based Rbus Cnrl Bhagyashri Tamhane 1, Amrua Mujumdar

More information

Visco-elastic Layers

Visco-elastic Layers Visc-elasic Layers Visc-elasic Sluins Sluins are bained by elasic viscelasic crrespndence principle by applying laplace ransfrm remve he ime variable Tw mehds f characerising viscelasic maerials: Mechanical

More information

Ann. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL:

Ann. 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 information

Mapping Properties Of The General Integral Operator On The Classes R k (ρ, b) And V k (ρ, b)

Mapping Properties Of The General Integral Operator On The Classes R k (ρ, b) And V k (ρ, b) Applied Mahemaics E-Noes, 15(215), 14-21 c ISSN 167-251 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Mapping Properies Of The General Inegral Operaor On The Classes R k (ρ, b) And V k

More information

Ramsey model. Rationale. Basic setup. A g A exogenous as in Solow. n L each period.

Ramsey model. Rationale. Basic setup. A g A exogenous as in Solow. n L each period. Ramsey mdel Rainale Prblem wih he Slw mdel: ad-hc assumpin f cnsan saving rae Will cnclusins f Slw mdel be alered if saving is endgenusly deermined by uiliy maximizain? Yes, bu we will learn a l abu cnsumpin/saving

More information

CLASSICAL SOLUTIONS OF THE NAVIER-STOKES EQUATIONS. John G. Heywood University of British Columbia (1) Vancouver, Canada

CLASSICAL SOLUTIONS OF THE NAVIER-STOKES EQUATIONS. John G. Heywood University of British Columbia (1) Vancouver, Canada CLASSICAL SOLUTIONS OF THE NAVIER-STOKES EQUATIONS Jhn G. Heywd Universiy f Briish Clumbia (1) Vancuver, Canada i. Inrducin The simples, ms elemenary prfs f he exisence f sluins f he Navier-Skes equains

More information

L p -L q -Time decay estimate for solution of the Cauchy problem for hyperbolic partial differential equations of linear thermoelasticity

L 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 information

ON THE COMPONENT DISTRIBUTION COEFFICIENTS AND SOME REGULARITIES OF THE CRYSTALLIZATION OF SOLID SOLUTION ALLOYS IN MULTICOMPONENT SYSTEMS*

ON THE COMPONENT DISTRIBUTION COEFFICIENTS AND SOME REGULARITIES OF THE CRYSTALLIZATION OF SOLID SOLUTION ALLOYS IN MULTICOMPONENT SYSTEMS* METL 006.-5.5.006, Hradec nad Mravicí ON THE OMPONENT DISTRIUTION OEFFIIENTS ND SOME REGULRITIES OF THE RYSTLLIZTION OF SOLID SOLUTION LLOYS IN MULTIOMPONENT SYSTEMS* Eugenij V.Sidrv a, M.V.Pikunv b, Jarmír.Drápala

More information

Solutions to Assignment 1

Solutions to Assignment 1 MA 2326 Differenial Equaions Insrucor: Peronela Radu Friday, February 8, 203 Soluions o Assignmen. Find he general soluions of he following ODEs: (a) 2 x = an x Soluion: I is a separable equaion as we

More information

Math 334 Fall 2011 Homework 11 Solutions

Math 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 information

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson

Oscillation 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 information

Math 23 Spring Differential Equations. Final Exam Due Date: Tuesday, June 6, 5pm

Math 23 Spring Differential Equations. Final Exam Due Date: Tuesday, June 6, 5pm Mah Spring 6 Differenial Equaions Final Exam Due Dae: Tuesday, June 6, 5pm Your name (please prin): Insrucions: This is an open book, open noes exam. You are free o use a calculaor or compuer o check your

More information

A new Type of Fuzzy Functions in Fuzzy Topological Spaces

A new Type of Fuzzy Functions in Fuzzy Topological Spaces IOSR Jurnal f Mathematics (IOSR-JM e-issn: 78-578, p-issn: 39-765X Vlume, Issue 5 Ver I (Sep - Oct06, PP 8-4 wwwisrjurnalsrg A new Type f Fuzzy Functins in Fuzzy Tplgical Spaces Assist Prf Dr Munir Abdul

More information

The Buck Resonant Converter

The Buck Resonant Converter EE646 Pwer Elecrnics Chaper 6 ecure Dr. Sam Abdel-Rahman The Buck Resnan Cnverer Replacg he swich by he resnan-ype swich, ba a quasi-resnan PWM buck cnverer can be shwn ha here are fur mdes f pera under

More information

STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS WITH VARIABLE DELAYS

STABILITY 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 information

Essential Maps and Coincidence Principles for General Classes of Maps

Essential 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 information

u(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

u(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 information

Orthogonal Rational Functions, Associated Rational Functions And Functions Of The Second Kind

Orthogonal 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 information

CHAPTER 7 CHRONOPOTENTIOMETRY. In this technique the current flowing in the cell is instantaneously stepped from

CHAPTER 7 CHRONOPOTENTIOMETRY. In this technique the current flowing in the cell is instantaneously stepped from CHAPTE 7 CHONOPOTENTIOMETY In his echnique he curren flwing in he cell is insananeusly sepped frm zer sme finie value. The sluin is n sirred and a large ecess f suppring elecrlye is presen in he sluin;

More information

A Note on Superlinear Ambrosetti-Prodi Type Problem in a Ball

A 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 information

Differential Equations

Differential 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 information

Coherent PSK. The functional model of passband data transmission system is. Signal transmission encoder. x Signal. decoder.

Coherent PSK. The functional model of passband data transmission system is. Signal transmission encoder. x Signal. decoder. Cheren PSK he funcinal mdel f passand daa ransmissin sysem is m i Signal ransmissin encder si s i Signal Mdular Channel Deecr ransmissin decder mˆ Carrier signal m i is a sequence f syml emied frm a message

More information

Intuitionistic Fuzzy 2-norm

Intuitionistic 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 information

Lecture II Simple One-Dimensional Vibrating Systems

Lecture II Simple One-Dimensional Vibrating Systems UIUC Physics 406 Acusical Physics f Music Lecure II Simple One-Dimensinal Vibraing Sysems One mehd f prducing a sund relies n a physical bjec (e.g. varius ypes f musical insrumens sringed and wind insrumens

More information

CS Homework Week 2 ( 2.25, 3.22, 4.9)

CS Homework Week 2 ( 2.25, 3.22, 4.9) CS3150 - Homework Week 2 ( 2.25, 3.22, 4.9) Dan Li, Xiaohui Kong, Hammad Ibqal and Ihsan A. Qazi Deparmen of Compuer Science, Universiy of Pisburgh, Pisburgh, PA 15260 Inelligen Sysems Program, Universiy

More information

DIFFERENTIAL EQUATIONS

DIFFERENTIAL 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 information

Impact Switch Study Modeling & Implications

Impact Switch Study Modeling & Implications L-3 Fuzing & Ordnance Sysems Impac Swich Sudy Mdeling & Implicains Dr. Dave Frankman May 13, 010 NDIA 54 h Annual Fuze Cnference This presenain cnsiss f L-3 Crprain general capabiliies infrmain ha des

More information

On Gronwall s Type Integral Inequalities with Singular Kernels

On 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 information

A NOTE ON S(t) AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION

A NOTE ON S(t) AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION Bull. London Mah. Soc. 39 2007 482 486 C 2007 London Mahemaical Sociey doi:10.1112/blms/bdm032 A NOTE ON S AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION D. A. GOLDSTON and S. M. GONEK Absrac Le πs denoe he

More information

A Simple Set of Test Matrices for Eigenvalue Programs*

A Simple Set of Test Matrices for Eigenvalue Programs* Simple Set f Test Matrices fr Eigenvalue Prgrams* By C. W. Gear** bstract. Sets f simple matrices f rder N are given, tgether with all f their eigenvalues and right eigenvectrs, and simple rules fr generating

More information

Nonlinear Fuzzy Stability of a Functional Equation Related to a Characterization of Inner Product Spaces via Fixed Point Technique

Nonlinear 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 information

Positive continuous solution of a quadratic integral equation of fractional orders

Positive 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 information

International Journal of Scientific & Engineering Research, Volume 4, Issue 10, October ISSN

International 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 information

KEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow

KEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow 1 KEY Mah 4 Miderm I Fall 8 secions 1 and Insrucor: Sco Glasgow Please do NOT wrie on his eam. No credi will be given for such work. Raher wrie in a blue book, or on our own paper, preferabl engineering

More information

Notes for Lecture 17-18

Notes 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 information

arxiv: v1 [math.ca] 15 Nov 2016

arxiv: 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 information

Supplement for Stochastic Convex Optimization: Faster Local Growth Implies Faster Global Convergence

Supplement 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 information

MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE

MODULE 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 information

On a Fractional Stochastic Landau-Ginzburg Equation

On 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 information

A Sharp Existence and Uniqueness Theorem for Linear Fuchsian Partial Differential Equations

A Sharp Existence and Uniqueness Theorem for Linear Fuchsian Partial Differential Equations A Sharp Exisence and Uniqueness Theorem for Linear Fuchsian Parial Differenial Equaions Jose Ernie C. LOPE Absrac This paper considers he equaion Pu = f, where P is he linear Fuchsian parial differenial

More information

Class Meeting # 10: Introduction to the Wave Equation

Class Meeting # 10: Introduction to the Wave Equation MATH 8.5 COURSE NOTES - CLASS MEETING # 0 8.5 Inroducion o PDEs, Fall 0 Professor: Jared Speck Class Meeing # 0: Inroducion o he Wave Equaion. Wha is he wave equaion? The sandard wave equaion for a funcion

More information

MA 366 Review - Test # 1

MA 366 Review - Test # 1 MA 366 Review - Tes # 1 Fall 5 () Resuls from Calculus: differeniaion formulas, implici differeniaion, Chain Rule; inegraion formulas, inegraion b pars, parial fracions, oher inegraion echniques. (1) Order

More information

A Necessary and Sufficient Condition for the Solutions of a Functional Differential Equation to Be Oscillatory or Tend to Zero

A 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 information

BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS

BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS XUAN THINH DUONG, JI LI, AND ADAM SIKORA Absrac Le M be a manifold wih ends consruced in [2] and be he Laplace-Belrami operaor on M

More information

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004

ODEs 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 information

On some Properties of Conjugate Fourier-Stieltjes Series

On some Properties of Conjugate Fourier-Stieltjes Series Bullein of TICMI ol. 8, No., 24, 22 29 On some Properies of Conjugae Fourier-Sieljes Series Shalva Zviadadze I. Javakhishvili Tbilisi Sae Universiy, 3 Universiy S., 86, Tbilisi, Georgia (Received January

More information

Math 10B: Mock Mid II. April 13, 2016

Math 10B: Mock Mid II. April 13, 2016 Name: Soluions Mah 10B: Mock Mid II April 13, 016 1. ( poins) Sae, wih jusificaion, wheher he following saemens are rue or false. (a) If a 3 3 marix A saisfies A 3 A = 0, hen i canno be inverible. True.

More information