( ) ( ) ( ) ( ) ( ) t ( ) ( ) ( ) ( ) [ ) Abstract. Keywords. 1. Introduction. Yunlong Gao, Yuting Sun, Guoguang Lin

Size: px
Start display at page:

Download "( ) ( ) ( ) ( ) ( ) t ( ) ( ) ( ) ( ) [ ) Abstract. Keywords. 1. Introduction. Yunlong Gao, Yuting Sun, Guoguang Lin"

Transcription

1 Ieraioal Joural of Moder Noliear Theory ad Applicaio hp://wwwcirporg/oural/ia ISSN Olie: ISSN Pri: The Global Aracor ad Their Haudorff ad Fracal Dieio Eiaio for he Higher-Order Noliear Kirchhoff-Type Euaio wih Srog Liear Dapig Yulog Gao Yuig Su Guoguag Li Depare of Maheaic Yua Uiveriy Kuig Chia How o cie hi paper: Gao YL Su YT ad Li GG (6 The Global Aracor ad Their Haudorff ad Fracal Dieio Eiaio for he Higher-Order Noliear Kirchhoff-Type Euaio wih Srog Liear Dapig Ieraioal Joural of Moder Noliear Theory ad Applicaio hp://dxdoiorg/436/ia6548 Received: Ocober 6 Acceped: Noveber 6 Publihed: Noveber 3 6 Copyrigh 6 by auhor ad Scieific Reearch Publihig Ic Thi work i liceed uder he Creaive Coo Aribuio Ieraioal Licee (CC BY 4 hp://creaivecooorg/licee/by/4/ Ope Acce Abrac I hi paper we udy he logie behavior of oluio o he iiial boudary value proble for a cla of rogly daped Higher-order Kirchhoff ype euaio: u + u + D u u+ g u = f x A fir we prove he exiece ad uiuee of he oluio by priori eiaio ad he Galerki ehod The we obai o he exiece of he global aracor A la we coider ha he eiaio of he upper boud of Haudorff ad fracal dieio for he global aracor are obaied Keyword Noliear Higher-Order Kirchhoff Type Euaio The Exiece ad Uiuee The Global Aracor Haudorff Dieio Fracal Dieio Iroducio I hi paper we are cocered wih he exiece of global aracor ad Haudorff ad Fracal dieio eiaio for he followig oliear Higher-order Kirchhoff-ype euaio: [ u( x u ( x u ( x u ( x x u + u + D u u+ g u = f x x Ω + ( = = Ω ( i u u( x = = i= x Ω ( + (3 i v DOI: 436/ia6548 Noveber 3 6

2 Y L Gao e al where > i a ieger coa ad > i a poiive coa Moreover Ω i a bouded doai i R wih he ooh boudary Ω ad v i he ui ouward oral o Ω g( u i a oliear fucio pecified laer Recely Maria Ghii ad Maio Gobbio [] udied pecral gap global oluio for degeerae Kirchhoff euaio Give a coiuou fucio :[ + [ + hey coider he Cauchy proble: where [ Ω u x + ux d x ux = x Ω T (4 u = u u = u (5 Ω R i a ope e ad u ad u deoe he gradie ad he Laplacia of u wih repec o he pace variable They prove ha for uch iiial daa ( u u here exi wo pair of iiial daa ( ( ˆ ˆ u u u u for which he oluio i global ad uch ha u = u + uˆ ˆ u = u+ u Yag Zhiia Dig Pegya ad Lei Li [] udied Logie dyaic of he Kirchhoff euaio wih fracioal dapig ad upercriical olieariy: where α u M u u+ u + f u = g x x Ω > (6 u = u x = u x u x = Ω u x (7 α Ω i a bouded doai R N wih he ooh boudary Ω ad he olieariy f ( u ad exeral force er g will be pecified The ai reul are focued o he relaiohip aog he growh expoe p of he olieariy f ( u ad well-poede They how ha (i eve if p i up o he upercriical rage ha i p < N + 4α ( N 4 α + he well-poede ad he logie behavior of he o- luio of he euaio are of he characer of he parabolic euaio; (ii whe N + 4α N + 4 p < he correpodig ubcla G of he lii oluio exi N 4α + N 4 + ad poee a weak global aracor Yag Zhiia Dig Pegya ad Liu Zhiig [3] udied he Global aracor for he Kirchhoff ype euaio wih rog oliear dapig ad upercriical olieariy: φ + u σ u u u u+ f u = h x i Ω (8 u x = u x = u x u x = u x x Ω (9 Ω where Ω i a bouded doai i ad f ( are oliear fucio ad N R wih he ooh boudary Ω ( σ φ ( h x i a exeral force er They prove ha i ricly poiive iffe facor ad upercriical olieariy cae here exi a global fiie-dieioal aracor i he aural eergy pace edowed wih rog opology Li Fucai [4] udied he global exiece ad blow-up of oluio for a higher-order 86

3 Y L Gao e al oliear Kirchhoff-ype hyperbolic euaio: Ω r p u + Du d x u+ u u = u ux Ω > ( i u u( x = = i= x Ω > ( i v u x = u x u x = u x ( where pr Ω i a bouded doai R wih a ooh boudary Ω ad a ui ouer oral v Seig + p+ E = u + D u u p+ ( + p+ Aue ha p aifie he codiio: p for N > ; p > for N N (3 Their ai reul are he wo heore: Theore Suppoe ha p r ad codiio (3 hold The for ay iiial daa ( u u H ( Ω H ( Ω H ( Ω he oluio of ( - ( exi globally Theore Suppoe ha p > ax { r } ad codiio ( hold The for ay iiial daa ( u u H ( Ω H ( Ω H ( Ω he oluio of ( - ( blow up a fiie ie i L p + or provided ha E < Li Ya [5] udied The Aypoic Behavior of Soluio for a Noliear Higher Order Kirchhoff Type Euaio: β Ω u + D u d x u+ u + g u = i Q = Ω + (4 i u u( x = = i= o Σ = Γ ( + (5 i v where Ω i a ope bouded e of ui oral vecor The fucio u x = u x u x = u x i x Ω (6 R wih ooh boudary Γ ad he g C aifie he followig codiio: G li if G ( g( r d r; = (7 ( g li if = (8 where γ ( γ ( 3 γ ( 4 C > uch ha γ < + = < = = Furherore here exi C G ( g li if (9 A la Li Ya udied he aypoic behavior of oluio for proble (4 - (6 For he o of he cholar repreeed by Yag Zhiia have udied all kid of low order Kirchhoff euaio ad oly a all uber of cholar have udied he 87

4 Y L Gao e al blow-up ad aypoic behavior of oluio for higher-order Kirchhoff euaio So i hi coex we udy he high-order Kirchhoff euaio i very eaigful I order o udy he high-order oliear Kirchhoff euaio wih he dapig er we borrow oe of Li Ya [5] parial aupio ( - (3 for he oliear er g i he euaio I order o prove ha he lea we have iproved he reul fro aupio ( - (3 uch ha < C The uder all aupio we prove uu L + ; H Ω H Ω ha he euaio ha a uiue ooh oluio ( ad obai he oluio eigroup S : H H H H Ω Ω Ω Ω ha global aracor Fially we prove he euaio ha fiie Haudorff dieio ad Fracal dieio by referece o he lieraure [7] For ore relaed reul we refer he reader o [6] [7] [8] [9] [] I order o ake hee euaio ore oral i ecio ad i ecio 3 oe aupio oaio ad he ai reul are aed Uder hee aupio we prove he exiece ad uiuee of oluio he we obai he global aracor for he proble ( - (3 Accordig o [6] [7] [8] [9] [] i ecio 4 we coider ha he global aracor of he above eioed proble ( - (3 ha fiie Haudorff dieio ad fracal dieio Preliiarie For coveiece we deoe he or ad calar produc i L ( Ω by ad f = f ( x p p k k k k L = L ( Ω H = H ( Ω H = H ( Ω = = p Accordig o [5] we pree oe aupio ad oaio eeded i he proof of g u C Ω aifie ha G = g r d r he our reul For hi reao we aue oliear er (H Seig G( (H If L p L ; li if ; ( ( where r < + ( = r < ( = r = ( g li up = ( r 3 4 (H 3 There exi coa C > uch ha C G ( (H 4 There exi coa C > uch ha where p ; g li if (3 ( p p g C + (4 g C + (5 88

5 Y L Gao e al For every γ > by (H -(H 3 ad apply Poicaré ieualiy here exi coa C ( γ > uch ha J( u + γ D u + C( γ u H ( Ω (6 ( g( u u CJ ( u γ Du C( γ u H + + Ω (7 i idepede of γ Ω Ω Ω where J( u = G( u d x< C Ω Lea Aue (H -(H 3 hold ad ( u u H L f x L The he oluio ( uv of he proble ( - (3 aifie ( uv L ( + ; H ( Ω L( Ω ad ( C C + + D u + v y e + + C + (8 4 C 6λ C λ + λ + + where v = u + u < < i λ + λ 4 i he fir eigevalue of i H ( Ω ad y u u + = + D u + D u + + J( u + C + + γ w C = f + C ( γ CC ( γ + γ = > γ λ = > { λ ( } w= i + Thu here exi ha ( uv D u v E H Proof We ake he calar produc i E ad = Ω > uch = + > (9 Ω L Ω L of euaio ( wih ( u u D u u g( u v ( f ( x v v = u + u The = ( Afer a copuaio i ( we have d = + ( d ( u v v v ( uv ( ( ( + d u v = D u + D v D u ( d d + + D u u v = D u + D u d ( g( u v J( u ( g( u u Collecig wih ( - (4 we obai fro ( ha + (3 d = + (4 d d + v D u + D u + J u v + u v d + ( ( + D v D u + D u + g u u = f x v (5 89

6 Y L Gao e al Sice v = u + u ad 4 C 6λ C + λ + + < < by uig Hölder i- 4 λ i + λ eualiy Youg ieualiy ad Poicaré ieualiy we deal wih he er i (5 oe by oe a follow: u v u v D u v (6 λ D v λ v (7 By (7 we ca obai ( g( u u CJ( u D u C( γ (8 λ where γ = > λ Becaue of f ( x L Ω we ca obai ( By (6 - (9 i follow fro ha f f x v f v + v (9 d v D u + D u + J( u + ( λ v d + + D u + D u + CJ( u f + C ( γ λ By Youg ieualiy ad < < < we have + λ D u + D u + ( D u ( ( + D u D u + ( By ( we ge + ( λ v D u + D u + C J u + + = ( λ v + ( + D u + + ( D u D u CJ( u w v + D u + C J u + + w v D u + D u + CJ( u + { λ } where w= ( + i (3 9

7 Y L Gao e al By ( ad ubiuig (3 io ( we receive d + v D u + D u + + J( u d w v D u + D u + + CJ u + + w f + C γ (4 Sice ( C + + 6λ C < < ad < C < we ge 4 { } w= i λ + C (5 By (6 ad ( we have + D u + D u + + J u + C + + ( D u J( u C( γ + + where γ = > Cobiig wih (5 ad (6 forula (4 io ( γ d + v D u + D u + + J( u + C( γ d C v D u + D u + + J( u + C( γ + + w f + C ( γ CC ( γ + + y = v D u + D u + + J u + C γ + + i iplified a We e d d y C y C where C = f + C( γ CC( γ (6 (7 The (7 + (8 w + Fro cocluio (6 we kow y So by Growall ieualiy we obai y y e + (9 C C C γ + + D u D u + + where y = u + u D u + D u + + J( u + C By geeralized Youg ieualiy we have + The we ge ( + ( D u D u + + (3 9

8 Y L Gao e al By (6 ad (3 we have y v D u D u J u C = ( γ + ( ( v + D u + D u J u C( γ ( D u ( v { }( v D u i ( v D u = Cobiig wih (9 ad (3we obai C C + + D u + v y( e + + ( C + The C + + ( uv = D u + v + H ( Ω L ( Ω ( li C + So here exi E ad = Ω > uch ha ( uv D u v E H (3 (3 (33 = + > (34 Ω L Ω Lea I addiio o he aupio of Lea (H - (H 4 hold If (H 5 : f x H u u H H uv of he pro- ( Ω ad ( ( Ω ( Ω The he oluio ble ( - (3 aifie ( uv L ( + ; H ( Ω H ( Ω ad D u D v where ( z ( D f + C 3 e α + + (35 T α T v u u = + ad T i{ if D u } z D u D u D u D u H Ω λ i he fir eigevalue of i = + + α { i λ M} = Thu here exi E ad = = Ω > uch ha ( uv D u D v E H = + > (36 Ω H Ω Proof Takig L -ier produc by ( v = u + u i ( we have u + u + D u u+ g u v = f x v (37 Afer a copuaio i (37 oe by oe a follow d ( u ( v = D v D v + ( D u D v d d D v D v D u D v d λ (38 9

9 Y L Gao e al ( ( D u ( u ( v d u v = D v D u D u (39 d D u d d = D u D u D u + D u D u d d By Youg ieualiy we ge g ( u D v ( (4 g u v g u D v (4 Nex o eiae + ad Youg ieualiy we have By p K > uch ha u L p io g u i (4 By (H 4 : ( p g C p ( + d Ω p p ( + + Ω p ( C + C u dx g u C u x Ω C C u C u dx p p L ( Ω C Ω+ C u ad Ebedig Theore he p H Ω L K D u (4 Ω So here exi D u bouded by lea The (4 ur Ω 3( Collecig wih (43 fro (4 we have g u C pc K Ω (43 ( g( u v By f ( x H ( C D v 3 (44 Ω ad Youg ieualiy we obai f x v = ( D f x D v D f + D v (45 Iegraig (38 - (4 (44 - (45 fro (37 eail d D v + ( D u D u + D v ( + D v d d + D u + D u D u D f C + d λ By Poicaré ieualiy uch ha λ D v D v So (46 ur io d D v + ( D u D u + ( λ D v d d + D u + D u D u D f C + 3 d λ 3 (46 (47 93

10 Y L Gao e al Fir we ake proper uch ha λ > ad D u a The we aue ha here exi M > uch ha M > ad M D u D u D u d λ o > by La- d < + The forula i iplified d M D u + D u M (48 By Growall ieualiy we ge d λ M ( M λ D u < D u e + M O accou of Lea we kow Naely we prove ha here are M > ake (49 D u i bouded So he hypohei i rue d < + (5 M D u D u D u d λ Subiuig (5 io (47 we receive + ( + ( λ ( 3 d D v D u D u D v d + M D u D u D f + C Takig α { i λ M} = he where ( (5 d z + αz D f + C 3 (5 d z = D v + D u D u By Growall ieualiy we have D f + C 3 e + (53 α α z z where = + + ( Le T = i{ if D u } o we ge The z D u D u D u D u So here exi D v D u z ( D f + C 3 e α + + (54 T α T D f + C 3 li ( uv = D u + D v (55 H ( Ω H ( Ω α T E ad = Ω > uch ha ( uv D u D v E H = + > (56 Ω H Ω 94

11 Y L Gao e al 3 Global Aracor 3 The Exiece ad Uiuee of Soluio Theore 3 Aue (H - (H 4 hold ad ( u u H H f ( x H ( Ω v u u ( u( x v( x L ( ; H H Ω Ω = + So Euaio ( exi a uiue ooh oluio + Ω Ω (3 Proof By he Galerki ehod Lea ad Lea we ca eaily obai he exiece of Soluio Nex we prove he uiuee of Soluio i deail Aue uv are wo oluio of he proble ( - (3 le w= u v he w x = w x = w x = w x = ad he wo euaio ubrac ad obai w w D u u D v v g( u g( v = (3 By uliplyig (3 by w we ge ( w w D u u D v v g u g v w = (33 d w w = w (34 d ( w w ( D u ( u D v ( vw = ( ( + ( ( = D w (35 ( D u w w D u D v v w d = D u D w D u D u D w d + D u D v vw Exploiig (34 - (36 we receive d ( w + D u D w + D w d ( g( u g( v w = D u D u D w D u D v v w (36 (37 I (37 accordig o Lea ad Lea uch ha ( θ ( θ ( θ ( D u D w D u D v v w D u D w + 4 D u + θ D v D u D w v w + C4 D w C5 D w w C C C4 ( + D w + w 5 5 where < θ < C ( > ad 4 C5 θ > are coa (38 95

12 Y L Gao e al By (H 4 we obai ( g( u g( v w ( θ ( θ ( g u v ww g ( θu ( θ v w w = + + p ( θ ( θ Ω p ( θ ( θ C ( + u + v dx w w (39 C + u+ v w w ( θ λ CC p D w w 6 where C C ( θ p λ ( θ λ ( θ λ CC p w + CC p D w = > i coa Fro he above we have ( ( θ ( d C w D u D w C CC w D w d For (3 becaue D u So we have d d where D u i bouded The here exi > ( w + D u D w 7 ( θ C5 C4( + + CC 6 w ( θ C4 C5 CC ( C w + D u D w D u D w ( θ ( θ C5 C4 C5 CC 6 C7 = i C4 + + CC wall ieualiy for (3 we obai C 7 ( uch ha (3 (3 By uig Gro- w + D u D w w + D u D w e = (3 Hece we ca ge w + D u D w = Tha how ha w = D u D w = (33 Tha i Therefore w( x = (34 u = v (35 So we ge he uiuee of he oluio 96

13 Y L Gao e al S are he eigroup op- + = = where I i a ui 3 Global Aracor Theore 3 [] Le E be a Baach pace ad { } eraor o E S : E E S( τ S S( τ( τ S I operaorse S( aify he follow codiio: R > u R i exi a coa S i uiforly bouded aely E o ha ( [ I exi a bouded aborbig e B o ha C R S u C R + ; (36 E E aely B E i exi a coa S B B (37 ; where B ad B are bouded e 3 Whe > S( i a copleely coiuou operaor Therefore he eigroup operaor S( exi a copac global aracor Theore 33 Uder he aue of Lea Lea ad Theore 3 euaio have global aracor ( B = ω = S B (38 τ τ { : H H H H } where B = uv H Ω H Ω uv = u + v R + R B i he bouded aborbig e of H S = > ; li di S B = here H ad aifie ( ( B H H ad i i a bouded e ( y H H di S B = up if S x y (39 x B Proof Uder he codiio of Theore 3 i exi he oluio eigroup S( S : H H H H here E = H ( Ω H ( Ω ( Fro Lea o Lea we ca ge ha B H ( Ω H ( Ω i a uv R bouded e ha iclude i he ball { H } H H H H H H H R + C ( u v B S u v = u + v u + v + C Thi how ha S( i uiforly bouded i H ( Ω H ( Ω ( Furherore for ay ( u v H ( Ω H ( Ω whe ax { } have H H H H (3 we S u v = u + v R + R (3 So we ge B i he bouded aborbig e (3 Sice E : = H Ω H Ω E : = H Ω L ( Ω i copac ebedded which ea ha he bouded e i E i he copac e i E o he eigroup operaor S( exi a copac global aracor 97

14 Y L Gao e al 4 The Eiae of he Upper Boud of Haudorff ad Fracal Dieio for he Global Aracor We rewrie he proble ( - (3: Le Au u + Au+ Au Au+ gu = f x i Ω R + (4 u x = u x ; u x = u x x Ω (4 i u + u( x Ω = = ( i = i Ω R (43 i v = u where Ω i a bouded doai i N wih ooh boudary Ω i poiive coa ad i poiive ieger The liearized euaio of he above euaio a follow: U + AU = FU (44 U = ξ U = ζ (45 Le U H ( Ω proble (44 - (45 have a uiue oluio U i he oluio of proble (44 - (45 We ca prove ha he ( ( U L T H Ω U L T L Ω The euaio (44 i he liearized euaio by he Euaio (47 Defie he L : L U u u ϕ = u u appig ζ = here = le u u { } { u u } ϕ = ϕ + ξζ = + ξ + ζ le ϕ R E ϕ = ϕ = { } S ϕ ϕ ϕ S u u { } = E ϕ R E = H ( Ω ( Ω Ł Lea 4 [6] Aue H i a Hilber pace E i a copac e of H S : E H i a coiuou appig aify he follow codiio S ( E = E > ; If S( i Fréche differeiable i exi i a bouded liear differeial operaor + L ( ϕ CR; LE ( E > ha i ϕ ϕ ( ϕ ( S S L u v { ξζ } E E { ξζ} The proof of lea 4 ee ref [6] i oied here Accordig o Lea 4 we ca ge he followig heore : Theore 4 [6] [7] Le i he global aracor ha we obai i ecio 3I ha cae ha fiie Haudorff dieio ad Fracal dieio i 6 H ( Ω H ( Ω ha i dh ( df ( 5 5 Proof Firly we rewrie he euaio (4 (4 io he fir order abrac evoluio euaio i E Rϕ uu u + i a ioorphic ap- Le Ψ= = { + } le R :{ uu } { uu u} pig So le i he global aracor of { S( } of { S } he R i alo he global aracor ad hey have he ae dieio The Ψ aifie a follow: 98

15 Y L Gao e al { u } T u u T T where Ψ= { + } ( Ψ = = Ψ +ΛΨ+ g Ψ = f (46 Ψ = + (47 { } { } uu u g g u f f x Λ = I I + A u A A I A I T (48 Ψ : = F Ψ = f ΛΨ g Ψ (49 P = F ( Ψ (4 P P g P where P { UU U} T g P g( uu +Λ + Ψ = (4 { } T = + Ψ = The iiial codiio (45 ca be wrie i he followig for: ωω { ξζ} E P = = (4 We ake N he coider he correpodig oluio: ( P = P P P; P E of he iiial value: ( ω = ω ω ω; ω E i he Euaio (4 - (4 So here i ( d e TrF S τ Ψ Q τ τ = ω ω ω P P P fro E ψ ( τ = S ( τ Ψ we ge S ( τ :{ u v = u+ u} { u( τ v( τ = u ( τ + u( τ } ψ ( τ = { u( τ v ( τ = u ( τ + u( τ } here u i he oluio of proble (4-(43; repree he ouer produc T repre he race Q ( τ = Q ( τ Ψ ; ω ω ω E i a orhogoal proecio fro he pace E = o he ubpace paed by { P( τ P( τ P ( τ } For a give ie τ le φ ( τ = ξ ( τ ζ ( τ = φ ( τ i he { } { } = adard orhogoal bai of he pace Q ( τ pa P ( τ P ( τ P ( τ Fro he above we have E = ( Ψ( τ ( τ = ( Ψ( τ ( τ φ ( τ φ ( τ TrF Q F Q = ( F ( ( τ φ ( τ φ ( τ = Ψ = where ( i he ier produc i E F φ φ φ φ g u ξ ξ E The ({ ξζ }{ ξζ } ( ξξ ( ζζ E ( Ψ = ( Λ ( ( ( ( A u ( A ( A ( ξ ζ E E = + ; E E Λ φ φ = ξ + ξ ζ + ξ ζ + ζ ζ ζ = ξ + ( ( ξ ζ + λ A u ( ξ ζ + λ ζ ζ a + (43 (44 99

16 Y L Gao e al where + + A u λ ( λ + + A u λ a : = i Now uppoe ha { } E Ψ = { u u + u } E u D( A ; D( A = { u Au } The here i a [ ] o ake he appig g : D( A ρ ( u u accordig o heore 33 i a bouded aborbig e i ie here are he followig reul: R A up u D( A Au < R = up Aξ < ; A { ξζ } where g ( u ξ ζ ee: obaied: ρ ( g u r < v g u ξ ζ r ξ ζ ( E A he ae (45 Copreheive above ca be F Ψ φ φ a ξ + ζ + r ξ ζ (46 a r ( ξ + ζ + ξ a ξ + ζ = φ = due o φ ( τ i a adard orhogoal bai i E E Q τ So { } ( F ( E = a Ψ τ φ τ φ τ + ξ (47 = a r Alo o all akig ξ λ (48 = = So TrF a r Ψ + (49 ( ( τ Q( τ λ a = Le u aue ha { u u } i euivale o { } ( Ψ Ψ = u u+ u R The TrF S τ Q τ dτ = = (4 up up Ψ R ω E ω E = li up Accordig o (49 (4 o a r + a a r + a = = λ λ (4

17 Y L Gao e al Therefore he Lyapuov expoe of (or R i uiforly bouded a r µ + µ + + µ + λ (4 a Fro wha ha bee dicued above i exi a ad r are coa he ( λ = = a (43 6r a r 5a λ (44 a = r a = (45 + a λ i i= ( + ax (46 5 Accordig o he referece [6] [7] we iediaely o he Haudorff dieio ad 6 dh df 5 5 fracal dieio are repecively 5 Cocluio I hi paper we prove ha he higher-order oliear Kirchhoff euaio wih liear dapig i L (( + ; H ( Ω H ( Ω ha a uiue ooh oluio ( uu Fur- her we obai he oluio eigroup S : H ( Ω H ( Ω H ( Ω H ( Ω ha global aracor Fially we prove he euaio ha fiie Haudorff dieio L + ; H Ω H Ω ( ad Fracal dieio i Ackowledgee The auhor expre heir icere hak o he aoyou reviewer for hi/her careful readig of he paper givig valuable coe ad uggeio Thee coribuio grealy iproved he paper Fud Thi work i uppored by he Naioal Naural Sciece Foudaio of People Republic of Chia uder Gra 5676 Referece [] Ghii M ad Gobbio M (9 Specral Gap Global Soluio for Degeerae Kirchhoff Euaio Noliear Aalyi hp://doiorg/6/a99 [] Yag ZJ Dig PY ad Li L (6 Logie Dyaic of he Kirchhoff Euaio wih Fracioal Dapig ad Supercriical Nolieariy Joural of Maheaical Aalyi Applicaio hp://doiorg/6/aa6479 [3] Yag ZJ Dig PY ad Liu ZM (4 Global Aracor for he Kirchhoff Type Euaio wih Srog Noliear Dapig ad Supercriical Nolieariy Applied Maheaic Leer 33-7 hp://doiorg/6/al44

18 Y L Gao e al [4] Li FC (4 Global Exiece ad Blow-Up of Soluio for a Higher-Order Kirchhoff- Type Euaio wih Noliear Diipaio Applied Maheaic Leer hp://doiorg/6/a374 [5] Li Y ( The Aypoic Behavior of Soluio for a Noliear Higher Order Kirchhoff Type Euaio Joural of Souhwe Chia Noral Uiveriy [6] Tea R (998 Ifiie Dieioal Dyaic Sye i Mechaic ad Phyic Spriger New York [7] Wu JZ ad Li GG (9 The Global Aracor of he Boie Euaio wih Dapig Ter ad I Dieio Eiaio Joural of Yua Uiveriy [8] Yag ZJ (7 Logie Behavior of he Kirchhoff Type Euaio wih Srog Dapig o R Joural of Differeial Euaio N hp://doiorg/6/de784 [9] Yag ZJ ad Liu ZM (5 Expoeial Aracor for he Kirchhoff Euaio wih Srog Noliear Dapig ad Supercriical Nolieariy Applied Maheaic Leer hp://doiorg/6/al59 [] Li GG ( Noliear Evoluio Euaio Yua Uiveriy Pre Kuig Subi or recoed ex aucrip o SCIRP ad we will provide be ervice for you: Accepig pre-ubiio iuirie hrough Eail Facebook LikedI Twier ec A wide elecio of oural (icluive of 9 ubec ore ha oural Providig 4-hour high-ualiy ervice Uer-friedly olie ubiio ye Fair ad wif peer-review ye Efficie ypeeig ad proofreadig procedure Diplay of he reul of dowload ad vii a well a he uber of cied aricle Maxiu dieiaio of your reearch work Subi your aucrip a: hp://paperubiiocirporg/ Or coac ia@cirporg

EXISTENCE THEORY OF RANDOM DIFFERENTIAL EQUATIONS D. S. Palimkar

EXISTENCE THEORY OF RANDOM DIFFERENTIAL EQUATIONS D. S. Palimkar Ieraioal Joural of Scieific ad Research Publicaios, Volue 2, Issue 7, July 22 ISSN 225-353 EXISTENCE THEORY OF RANDOM DIFFERENTIAL EQUATIONS D S Palikar Depare of Maheaics, Vasarao Naik College, Naded

More information

Types Ideals on IS-Algebras

Types Ideals on IS-Algebras Ieraioal Joural of Maheaical Aalyi Vol. 07 o. 3 635-646 IARI Ld www.-hikari.co hp://doi.org/0.988/ija.07.7466 Type Ideal o IS-Algebra Sudu Najah Jabir Faculy of Educaio ufa Uiveriy Iraq Copyrigh 07 Sudu

More information

State-Space Model. In general, the dynamic equations of a lumped-parameter continuous system may be represented by

State-Space Model. In general, the dynamic equations of a lumped-parameter continuous system may be represented by Sae-Space Model I geeral, he dyaic equaio of a luped-paraeer coiuou ye ay be repreeed by x & f x, u, y g x, u, ae equaio oupu equaio where f ad g are oliear vecor-valued fucio Uig a liearized echique,

More information

Meromorphic Functions Sharing Three Values *

Meromorphic Functions Sharing Three Values * Alied Maheaic 11 718-74 doi:1436/a11695 Pulihed Olie Jue 11 (h://wwwscirporg/joural/a) Meroorhic Fucio Sharig Three Value * Arac Chagju Li Liei Wag School o Maheaical Sciece Ocea Uiveriy o Chia Qigdao

More information

BE.430 Tutorial: Linear Operator Theory and Eigenfunction Expansion

BE.430 Tutorial: Linear Operator Theory and Eigenfunction Expansion BE.43 Tuorial: Liear Operaor Theory ad Eigefucio Expasio (adaped fro Douglas Lauffeburger) 9//4 Moivaig proble I class, we ecouered parial differeial equaios describig rasie syses wih cheical diffusio.

More information

The Time-optimal Problems for the Fuzzy R-solution of the Control Linear Fuzzy Integro-Differential Inclusions

The Time-optimal Problems for the Fuzzy R-solution of the Control Linear Fuzzy Integro-Differential Inclusions Aerica Joural of Modelig ad Opiizaio 23 Vol. No. 2 6- Available olie a hp://pub.ciepub.co/ajo//2/ Sciece ad Educaio Publihig DOI:.269/ajo--2- he ie-opial Proble for he Fuzzy R-oluio of he Corol Liear Fuzzy

More information

A Comparative Study of Adomain Decompostion Method and He-Laplace Method

A Comparative Study of Adomain Decompostion Method and He-Laplace Method Applied Mahemaic,, 5, 5-6 Publihed Olie December i SciRe. hp://www.cirp.org/joural/am hp://d.doi.org/.6/am..5 A Comparaive Sudy of Adomai Decompoio Mehod ad He-Laplace Mehod Badradee A. A. Adam, Deparme

More information

Computable Analysis of the Solution of the Nonlinear Kawahara Equation

Computable Analysis of the Solution of the Nonlinear Kawahara Equation Diache Lu e al IJCSE April Vol Iue 49-64 Compuale Aalyi of he Soluio of he Noliear Kawahara Equaio Diache Lu Jiai Guo Noliear Scieific eearch Ceer Faculy of Sciece Jiagu Uiveri Zhejiag Jiagu 3 Chia dclu@uj.edu.c

More information

Hadamard matrices from the Multiplication Table of the Finite Fields

Hadamard matrices from the Multiplication Table of the Finite Fields adamard marice from he Muliplicaio Table of he Fiie Field 신민호 송홍엽 노종선 * Iroducio adamard mari biary m-equece New Corucio Coe Theorem. Corucio wih caoical bai Theorem. Corucio wih ay bai Remark adamard

More information

The Inverse of Power Series and the Partial Bell Polynomials

The Inverse of Power Series and the Partial Bell Polynomials 1 2 3 47 6 23 11 Joural of Ieger Sequece Vol 15 2012 Aricle 1237 The Ivere of Power Serie ad he Parial Bell Polyomial Miloud Mihoubi 1 ad Rachida Mahdid 1 Faculy of Mahemaic Uiveriy of Sciece ad Techology

More information

SLOW INCREASING FUNCTIONS AND THEIR APPLICATIONS TO SOME PROBLEMS IN NUMBER THEORY

SLOW INCREASING FUNCTIONS AND THEIR APPLICATIONS TO SOME PROBLEMS IN NUMBER THEORY VOL. 8, NO. 7, JULY 03 ISSN 89-6608 ARPN Jourl of Egieerig d Applied Sciece 006-03 Ai Reerch Publihig Nework (ARPN). All righ reerved. www.rpjourl.com SLOW INCREASING FUNCTIONS AND THEIR APPLICATIONS TO

More information

MODERN CONTROL SYSTEMS

MODERN CONTROL SYSTEMS MODERN CONTROL SYSTEMS Lecure 9, Sae Space Repreeaio Emam Fahy Deparme of Elecrical ad Corol Egieerig email: emfmz@aa.edu hp://www.aa.edu/cv.php?dip_ui=346&er=6855 Trafer Fucio Limiaio TF = O/P I/P ZIC

More information

CHARACTERIZATIONS OF THE NON-UNIFORM IN TIME ISS PROPERTY AND APPLICATIONS

CHARACTERIZATIONS OF THE NON-UNIFORM IN TIME ISS PROPERTY AND APPLICATIONS CHARACTERIZATIONS OF THE NON-UNIFORM IN TIME ISS PROPERTY AND APPLICATIONS I. Karafyllis ad J. Tsiias Depare of Maheaics, Naioal Techical Uiversiy of Ahes, Zografou Capus 578, Ahes, Greece Eail: jsi@ceral.ua.gr.

More information

MALAYSIAN JOURNAL OF MATHEMATICAL SCIENCES. Boundary Value Problem for the Higher Order Equation with Fractional Derivative

MALAYSIAN JOURNAL OF MATHEMATICAL SCIENCES. Boundary Value Problem for the Higher Order Equation with Fractional Derivative Malaysia Joural of Maheaical Scieces 7(): 3-7 (3) MALAYSIAN JOURNAL OF MATHEMATICAL SCIENCES Joural hoepage: hp://eispe.up.edu.y/joural Boudary Value Proble for he Higher Order Equaio wih Fracioal Derivaive

More information

arxiv: v1 [math.nt] 13 Dec 2010

arxiv: v1 [math.nt] 13 Dec 2010 WZ-PROOFS OF DIVERGENT RAMANUJAN-TYPE SERIES arxiv:0.68v [mah.nt] Dec 00 JESÚS GUILLERA Abrac. We prove ome diverge Ramauja-ype erie for /π /π applyig a Bare-iegral raegy of he WZ-mehod.. Wilf-Zeilberger

More information

A quadratic convergence method for the management equilibrium model

A quadratic convergence method for the management equilibrium model (IJACSA Ieraioal Joural of Advaced Copuer Sciece ad Applicaios Vol No 9 03 A quadraic covergece ehod for he aagee equilibriu odel Jiayi Zhag Feixia School Liyi Uiversiy Feixia Shadog PRChia Absrac i his

More information

Research Article A Generalized Nonlinear Sum-Difference Inequality of Product Form

Research Article A Generalized Nonlinear Sum-Difference Inequality of Product Form Joural of Applied Mahemaics Volume 03, Aricle ID 47585, 7 pages hp://dx.doi.org/0.55/03/47585 Research Aricle A Geeralized Noliear Sum-Differece Iequaliy of Produc Form YogZhou Qi ad Wu-Sheg Wag School

More information

1 Notes on Little s Law (l = λw)

1 Notes on Little s Law (l = λw) Copyrigh c 26 by Karl Sigma Noes o Lile s Law (l λw) We cosider here a famous ad very useful law i queueig heory called Lile s Law, also kow as l λw, which assers ha he ime average umber of cusomers i

More information

Economics 8723 Macroeconomic Theory Problem Set 3 Sketch of Solutions Professor Sanjay Chugh Spring 2017

Economics 8723 Macroeconomic Theory Problem Set 3 Sketch of Solutions Professor Sanjay Chugh Spring 2017 Deparme of Ecoomic The Ohio Sae Uiveriy Ecoomic 8723 Macroecoomic Theory Problem Se 3 Skech of Soluio Profeor Sajay Chugh Sprig 27 Taylor Saggered Nomial Price-Seig Model There are wo group of moopoliically-compeiive

More information

Ruled surfaces are one of the most important topics of differential geometry. The

Ruled surfaces are one of the most important topics of differential geometry. The CONSTANT ANGLE RULED SURFACES IN EUCLIDEAN SPACES Yuuf YAYLI Ere ZIPLAR Deparme of Mahemaic Faculy of Sciece Uieriy of Aara Tadoğa Aara Turey yayli@cieceaaraedur Deparme of Mahemaic Faculy of Sciece Uieriy

More information

arxiv:math/ v1 [math.fa] 1 Feb 1994

arxiv:math/ v1 [math.fa] 1 Feb 1994 arxiv:mah/944v [mah.fa] Feb 994 ON THE EMBEDDING OF -CONCAVE ORLICZ SPACES INTO L Care Schü Abrac. I [K S ] i wa how ha Ave ( i a π(i) ) π i equivale o a Orlicz orm whoe Orlicz fucio i -cocave. Here we

More information

Variational Iteration Method for Solving Differential Equations with Piecewise Constant Arguments

Variational Iteration Method for Solving Differential Equations with Piecewise Constant Arguments I.J. Egieerig ad Maufacurig, 1,, 36-43 Publihed Olie April 1 i MECS (hp://www.mec-pre.e) DOI: 1.5815/ijem.1..6 Available olie a hp://www.mec-pre.e/ijem Variaioal Ieraio Mehod for Solvig Differeial Equaio

More information

Comparison between Fourier and Corrected Fourier Series Methods

Comparison between Fourier and Corrected Fourier Series Methods Malaysia Joural of Mahemaical Scieces 7(): 73-8 (13) MALAYSIAN JOURNAL OF MATHEMATICAL SCIENCES Joural homepage: hp://eispem.upm.edu.my/oural Compariso bewee Fourier ad Correced Fourier Series Mehods 1

More information

On a Grouping Method for Constructing Mixed Orthogonal Arrays

On a Grouping Method for Constructing Mixed Orthogonal Arrays Ope Joural of Saiic 01 188-197 hp://dxdoiorg/1046/oj010 Publihed Olie April 01 (hp://wwwscirporg/joural/oj) O a Groupig Mehod for Corucig Mixed Orhogoal Array Chug-Yi Sue Depare of Maheaic Clevelad Sae

More information

Two Implicit Runge-Kutta Methods for Stochastic Differential Equation

Two Implicit Runge-Kutta Methods for Stochastic Differential Equation Alied Mahemaic, 0, 3, 03-08 h://dx.doi.org/0.436/am.0.306 Publihed Olie Ocober 0 (h://www.scirp.org/oural/am) wo mlici Ruge-Kua Mehod for Sochaic Differeial quaio Fuwe Lu, Zhiyog Wag * Dearme of Mahemaic,

More information

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002 ME 31 Kiemaic ad Dyamic o Machie S. Lamber Wier 6.. Forced Vibraio wih Dampig Coider ow he cae o orced vibraio wih dampig. Recall ha he goverig diereial equaio i: m && c& k F() ad ha we will aume ha he

More information

TIME RESPONSE Introduction

TIME RESPONSE Introduction TIME RESPONSE Iroducio Time repoe of a corol yem i a udy o how he oupu variable chage whe a ypical e ipu igal i give o he yem. The commoly e ipu igal are hoe of ep fucio, impule fucio, ramp fucio ad iuoidal

More information

Mean Square Convergent Finite Difference Scheme for Stochastic Parabolic PDEs

Mean Square Convergent Finite Difference Scheme for Stochastic Parabolic PDEs America Joural of Compuaioal Mahemaics, 04, 4, 80-88 Published Olie Sepember 04 i SciRes. hp://www.scirp.org/joural/ajcm hp://dx.doi.org/0.436/ajcm.04.4404 Mea Square Coverge Fiie Differece Scheme for

More information

Review - Week 10. There are two types of errors one can make when performing significance tests:

Review - Week 10. There are two types of errors one can make when performing significance tests: Review - Week Read: Chaper -3 Review: There are wo ype of error oe ca make whe performig igificace e: Type I error The ull hypohei i rue, bu we miakely rejec i (Fale poiive) Type II error The ull hypohei

More information

A Note on Random k-sat for Moderately Growing k

A Note on Random k-sat for Moderately Growing k A Noe o Radom k-sat for Moderaely Growig k Ju Liu LMIB ad School of Mahemaics ad Sysems Sciece, Beihag Uiversiy, Beijig, 100191, P.R. Chia juliu@smss.buaa.edu.c Zogsheg Gao LMIB ad School of Mahemaics

More information

On the 2-Domination Number of Complete Grid Graphs

On the 2-Domination Number of Complete Grid Graphs Ope Joural of Dicrete Mathematic, 0,, -0 http://wwwcirporg/oural/odm ISSN Olie: - ISSN Prit: - O the -Domiatio Number of Complete Grid Graph Ramy Shahee, Suhail Mahfud, Khame Almaea Departmet of Mathematic,

More information

FIXED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE

FIXED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE Mohia & Samaa, Vol. 1, No. II, December, 016, pp 34-49. ORIGINAL RESEARCH ARTICLE OPEN ACCESS FIED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE 1 Mohia S. *, Samaa T. K. 1 Deparme of Mahemaics, Sudhir Memorial

More information

A Hilbert-type fractal integral inequality and its applications

A Hilbert-type fractal integral inequality and its applications Liu ad Su Joural of Ieualiies ad Alicaios 7) 7:83 DOI.86/s366-7-36-9 R E S E A R C H Oe Access A Hilber-e fracal iegral ieuali ad is alicaios Qiog Liu ad Webig Su * * Corresodece: swb5@63.com Dearme of

More information

CHAPTER 2 Quadratic diophantine equations with two unknowns

CHAPTER 2 Quadratic diophantine equations with two unknowns CHAPTER - QUADRATIC DIOPHANTINE EQUATIONS WITH TWO UNKNOWNS 3 CHAPTER Quadraic diophaie equaio wih wo ukow Thi chaper coi of hree ecio. I ecio (A), o rivial iegral oluio of he biar quadraic diophaie equaio

More information

Fermat Numbers in Multinomial Coefficients

Fermat Numbers in Multinomial Coefficients 1 3 47 6 3 11 Joural of Ieger Sequeces, Vol. 17 (014, Aricle 14.3. Ferma Numbers i Muliomial Coefficies Shae Cher Deparme of Mahemaics Zhejiag Uiversiy Hagzhou, 31007 Chia chexiaohag9@gmail.com Absrac

More information

Basic Results in Functional Analysis

Basic Results in Functional Analysis Preared by: F.. ewis Udaed: Suday, Augus 7, 4 Basic Resuls i Fucioal Aalysis f ( ): X Y is coiuous o X if X, (, ) z f( z) f( ) f ( ): X Y is uiformly coiuous o X if i is coiuous ad ( ) does o deed o. f

More information

Homotopy Analysis Method for Solving Fractional Sturm-Liouville Problems

Homotopy Analysis Method for Solving Fractional Sturm-Liouville Problems Ausralia Joural of Basic ad Applied Scieces, 4(1): 518-57, 1 ISSN 1991-8178 Homoopy Aalysis Mehod for Solvig Fracioal Surm-Liouville Problems 1 A Neamay, R Darzi, A Dabbaghia 1 Deparme of Mahemaics, Uiversiy

More information

Matrix Form of The Bayes Theorem And Diagnostic Tests

Matrix Form of The Bayes Theorem And Diagnostic Tests IOSR Joural of Maheaic IOSR-JM e-issn: 78-578, p-issn: 319-765X. Volue 14, Iue 6 Ver. I Nov - Dec 018, PP 01-06 www.iorjoural.org Marix For of The Baye Theore Ad Diagoic Te María Magdala Pérez-Nio 1 Joé

More information

E will be denoted by n

E will be denoted by n JASEM ISSN 9-8362 All rigs reserved Full-ex Available Olie a p:// wwwbiolieorgbr/ja J Appl Sci Eviro Mg 25 Vol 9 3) 3-36 Corollabiliy ad Null Corollabiliy of Liear Syses * DAVIES, I; 2 JACKREECE, P Depare

More information

A TAUBERIAN THEOREM FOR THE WEIGHTED MEAN METHOD OF SUMMABILITY

A TAUBERIAN THEOREM FOR THE WEIGHTED MEAN METHOD OF SUMMABILITY U.P.B. Sci. Bull., Series A, Vol. 78, Iss. 2, 206 ISSN 223-7027 A TAUBERIAN THEOREM FOR THE WEIGHTED MEAN METHOD OF SUMMABILITY İbrahim Çaak I his paper we obai a Tauberia codiio i erms of he weighed classical

More information

In this section we will study periodic signals in terms of their frequency f t is said to be periodic if (4.1)

In this section we will study periodic signals in terms of their frequency f t is said to be periodic if (4.1) Fourier Series Iroducio I his secio we will sudy periodic sigals i ers o heir requecy is said o be periodic i coe Reid ha a sigal ( ) ( ) ( ) () or every, where is a uber Fro his deiiio i ollows ha ( )

More information

Approximating Solutions for Ginzburg Landau Equation by HPM and ADM

Approximating Solutions for Ginzburg Landau Equation by HPM and ADM Available a hp://pvamu.edu/aam Appl. Appl. Mah. ISSN: 193-9466 Vol. 5, No. Issue (December 1), pp. 575 584 (Previously, Vol. 5, Issue 1, pp. 167 1681) Applicaios ad Applied Mahemaics: A Ieraioal Joural

More information

THE FINITE HAUSDORFF AND FRACTAL DIMENSIONS OF THE GLOBAL ATTRACTOR FOR A CLASS KIRCHHOFF-TYPE EQUATIONS

THE FINITE HAUSDORFF AND FRACTAL DIMENSIONS OF THE GLOBAL ATTRACTOR FOR A CLASS KIRCHHOFF-TYPE EQUATIONS European Journal of Maheaics and Copuer Science Vol 4 No 7 ISSN 59-995 HE FINIE HAUSDORFF AND FRACAL DIMENSIONS OF HE GLOBAL ARACOR FOR A CLASS KIRCHHOFF-YPE EQUAIONS Guoguang Lin & Xiangshuang Xia Deparen

More information

Existence of Solutions for Volterra Integro-Differential Equations with Implicit Derivative

Existence of Solutions for Volterra Integro-Differential Equations with Implicit Derivative Ieraioal Joural o Scieiic a Iovaive Mahemaical Reearch IJSIMR Volume 6 Iue 4 8 PP -5 ISSN 347-37X Pri & ISSN 347-34 Olie DOI: hp://xoiorg/43/347-3464 wwwarcjouralorg Exiece o Soluio or Volerra Iegro-Diereial

More information

VISCOSITY APPROXIMATION TO COMMON FIXED POINTS OF kn- LIPSCHITZIAN NONEXPANSIVE MAPPINGS IN BANACH SPACES

VISCOSITY APPROXIMATION TO COMMON FIXED POINTS OF kn- LIPSCHITZIAN NONEXPANSIVE MAPPINGS IN BANACH SPACES Joral o Maheaical Scieces: Advaces ad Alicaios Vole Nber 9 Pages -35 VISCOSIY APPROXIMAION O COMMON FIXED POINS OF - LIPSCHIZIAN NONEXPANSIVE MAPPINGS IN BANACH SPACES HONGLIANG ZUO ad MIN YANG Deare o

More information

New Results on Oscillation of even Order Neutral Differential Equations with Deviating Arguments

New Results on Oscillation of even Order Neutral Differential Equations with Deviating Arguments Advace i Pue Maheaic 9-53 doi: 36/ap3 Pubihed Oie May (hp://wwwscirpog/oua/ap) New Reu o Ociaio of eve Ode Neua Diffeeia Equaio wih Deviaig Ague Abac Liahog Li Fawei Meg Schoo of Maheaica Sye Sciece aiha

More information

The universal vector. Open Access Journal of Mathematical and Theoretical Physics [ ] Introduction [ ] ( 1)

The universal vector. Open Access Journal of Mathematical and Theoretical Physics [ ] Introduction [ ] ( 1) Ope Access Joural of Mahemaical ad Theoreical Physics Mii Review The uiversal vecor Ope Access Absrac This paper akes Asroheology mahemaics ad pus some of i i erms of liear algebra. All of physics ca be

More information

PRIMARY DECOMPOSITION, ASSOCIATED PRIME IDEALS AND GABRIEL TOPOLOGY

PRIMARY DECOMPOSITION, ASSOCIATED PRIME IDEALS AND GABRIEL TOPOLOGY Orietal J. ath., Volue 1, Nuber, 009, Page 101-108 009 Orietal Acadeic Publiher PRIARY DECOPOSITION, ASSOCIATED PRIE IDEALS AND GABRIEL TOPOLOGY. EL HAJOUI, A. IRI ad A. ZOGLAT Uiverité ohaed V aculté

More information

Turkish Journal of. Analysis and Number Theory. Volume 3, Number 6,

Turkish Journal of. Analysis and Number Theory. Volume 3, Number 6, ISSN (Pri) : - ISSN (Olie) : - Volue, Nuber 6, 5 hp://jahuedur hp://wwwciepubco/joural/ja Turih Joural of Aalyi ad Nuber Theory Sciece ad Educaio Publihig Haa Kalyocu Uiveriy Sca o view hi joural o your

More information

PIECEWISE N TH ORDER ADOMIAN POLYNOMIAL STIFF DIFFERENTIAL EQUATION SOLVER 13

PIECEWISE N TH ORDER ADOMIAN POLYNOMIAL STIFF DIFFERENTIAL EQUATION SOLVER 13 Abrac PIECEWISE N TH ORDER ADOMIAN POLYNOMIAL A piecewie h order Adomia polyomial olver for iiial value differeial equaio capable of olvig highly iff problem i preeed here. Thi powerful echique which employ

More information

Approximately Quasi Inner Generalized Dynamics on Modules. { } t t R

Approximately Quasi Inner Generalized Dynamics on Modules. { } t t R Joural of Scieces, Islamic epublic of Ira 23(3): 245-25 (22) Uiversiy of Tehra, ISSN 6-4 hp://jscieces.u.ac.ir Approximaely Quasi Ier Geeralized Dyamics o Modules M. Mosadeq, M. Hassai, ad A. Nikam Deparme

More information

Solution of the Hyperbolic Partial Differential Equation on Graphs and Digital Spaces: a Klein Bottle a Projective Plane and a 4D Sphere

Solution of the Hyperbolic Partial Differential Equation on Graphs and Digital Spaces: a Klein Bottle a Projective Plane and a 4D Sphere Soluio of he Hyperbolic Parial Differeial Equaio o Graph ad Digial Space: a Klei Bole a Projecive Plae ad a 4D Sphere Alexader V. Evako Diae, Laboraory of Digial Techologie, Mocow, Ruia Email addre: evakoa@mail.ru

More information

Chattering Free with Noise Reduction in Sliding-Mode Observers Using Frequency Domain Analysis

Chattering Free with Noise Reduction in Sliding-Mode Observers Using Frequency Domain Analysis Chaerig Free wih Noie Reducio i Slidig-Mode Oerver Uig Frequecy Doai Aalyi M. Hajaipour, M. Farrokhi * Depare of Elecrical Egieerig, Ira Uiveriy of Sciece ad echology, ehra 6846, IRAN hi paper pree aalyi

More information

Curvilinear Motion: Normal and Tangential Components

Curvilinear Motion: Normal and Tangential Components 15 Crviliear Moio: Noral ad Tageial Copoe Ref: Hibbeler 1.7, Bedford & Fowler: Dyaic.3 Whe he pah of a paricle i kow, a - coordiae ye wih a origi a he locaio of he paricle (a a ia i ie) ca be helpfl i

More information

Présentée pour obtenir le grade de. Docteur en Science **************TITRE**************

Présentée pour obtenir le grade de. Docteur en Science **************TITRE************** UNIVRSITÉ MOHAMD KHIDR FACULTÉ DS SCINCS XACTS T SCINC D LA NATUR T D LA VI BISKRA *************************** THÈS Préeée pour obeir le grade de Doceur e Sciece Spécialié: Probabilié **************TITR**************

More information

Online Supplement to Reactive Tabu Search in a Team-Learning Problem

Online Supplement to Reactive Tabu Search in a Team-Learning Problem Olie Suppleme o Reacive abu Search i a eam-learig Problem Yueli She School of Ieraioal Busiess Admiisraio, Shaghai Uiversiy of Fiace ad Ecoomics, Shaghai 00433, People s Republic of Chia, she.yueli@mail.shufe.edu.c

More information

Exercise: Show that. Remarks: (i) Fc(l) is not continuous at l=c. (ii) In general, we have. yn ¾¾. Solution:

Exercise: Show that. Remarks: (i) Fc(l) is not continuous at l=c. (ii) In general, we have. yn ¾¾. Solution: Exercie: Show ha Soluio: y ¾ y ¾¾ L c Þ y ¾¾ p c. ¾ L c Þ F y (l Fc (l I[c,(l "l¹c Þ P( y c

More information

Theoretical Physics Prof. Ruiz, UNC Asheville, doctorphys on YouTube Chapter Q Notes. Laplace Transforms. Q1. The Laplace Transform.

Theoretical Physics Prof. Ruiz, UNC Asheville, doctorphys on YouTube Chapter Q Notes. Laplace Transforms. Q1. The Laplace Transform. Theoreical Phyic Prof. Ruiz, UNC Aheville, docorphy o YouTue Chaper Q Noe. Laplace Traform Q1. The Laplace Traform. Pierre-Simo Laplace (1749-187) Courey School of Mhemic ad Siic Uiveriy of S. Adrew, Scolad

More information

EXPONENTIAL STABILITY ANALYSIS FOR NEURAL NETWORKS WITH TIME-VARYING DELAY AND LINEAR FRACTIONAL PERTURBATIONS

EXPONENTIAL STABILITY ANALYSIS FOR NEURAL NETWORKS WITH TIME-VARYING DELAY AND LINEAR FRACTIONAL PERTURBATIONS 46 Joural of arie Sciece ad echology Vol. No. pp. 46-53 (4) DOI:.69/JS-3-7-3 EXPONENIL SBILIY NLYSIS FOR NEURL NEWORKS WIH IE-VRYING DELY ND LINER FRCIONL PERURBIONS Chag-Hua Lie ad Ker-Wei Yu Key word:

More information

CLOSED FORM EVALUATION OF RESTRICTED SUMS CONTAINING SQUARES OF FIBONOMIAL COEFFICIENTS

CLOSED FORM EVALUATION OF RESTRICTED SUMS CONTAINING SQUARES OF FIBONOMIAL COEFFICIENTS PB Sci Bull, Series A, Vol 78, Iss 4, 2016 ISSN 1223-7027 CLOSED FORM EVALATION OF RESTRICTED SMS CONTAINING SQARES OF FIBONOMIAL COEFFICIENTS Emrah Kılıc 1, Helmu Prodiger 2 We give a sysemaic approach

More information

N! AND THE GAMMA FUNCTION

N! AND THE GAMMA FUNCTION N! AND THE GAMMA FUNCTION Cosider he produc of he firs posiive iegers- 3 4 5 6 (-) =! Oe calls his produc he facorial ad has ha produc of he firs five iegers equals 5!=0. Direcly relaed o he discree! fucio

More information

( ) ( ) ( ) ( ) ( ) ( ) ( ) (2)

( ) ( ) ( ) ( ) ( ) ( ) ( ) (2) UD 5 The Geeralized Riema' hypohei SV aya Khmelyy, Uraie Summary: The aricle pree he proo o he validiy o he geeralized Riema' hypohei o he bai o adjume ad correcio o he proo o he Riema' hypohei i he wor

More information

Fuzzy Dynamic Equations on Time Scales under Generalized Delta Derivative via Contractive-like Mapping Principles

Fuzzy Dynamic Equations on Time Scales under Generalized Delta Derivative via Contractive-like Mapping Principles Idia Joural of Sciece ad echology Vol 9(5) DOI: 7485/ijs/6/v9i5/8533 July 6 ISSN (Pri) : 974-6846 ISSN (Olie) : 974-5645 Fuzzy Dyamic Euaios o ime Scales uder Geeralized Dela Derivaive via Coracive-lie

More information

MORE COMMUTATOR INEQUALITIES FOR HILBERT SPACE OPERATORS

MORE COMMUTATOR INEQUALITIES FOR HILBERT SPACE OPERATORS terat. J. Fuctioal alyi Operator Theory ad pplicatio 04 Puhpa Publihig Houe llahabad dia vailable olie at http://pph.co/oural/ifaota.ht Volue Nuber 04 Page MORE COMMUTTOR NEQULTES FOR HLERT SPCE OPERTORS

More information

Lecture 25 Outline: LTI Systems: Causality, Stability, Feedback

Lecture 25 Outline: LTI Systems: Causality, Stability, Feedback Lecure 5 Oulie: LTI Sye: Caualiy, Sabiliy, Feebac oucee: Reaig: 6: Lalace Trafor. 37-49.5, 53-63.5, 73; 7: 7: Feebac. -4.5, 8-7. W 8 oe, ue oay. Free -ay eeio W 9 will be oe oay, ue e Friay (o lae W) Fial

More information

APPROXIMATE SOLUTION OF FRACTIONAL DIFFERENTIAL EQUATIONS WITH UNCERTAINTY

APPROXIMATE SOLUTION OF FRACTIONAL DIFFERENTIAL EQUATIONS WITH UNCERTAINTY APPROXIMATE SOLUTION OF FRACTIONAL DIFFERENTIAL EQUATIONS WITH UNCERTAINTY ZHEN-GUO DENG ad GUO-CHENG WU 2, 3 * School of Mahemaics ad Iformaio Sciece, Guagi Uiversiy, Naig 534, PR Chia 2 Key Laboraory

More information

Journal of Mechanical Science and Technology 23 (2009) 1058~1064. Dynamic behaviors of nonlinear fractional-order differential oscillator

Journal of Mechanical Science and Technology 23 (2009) 1058~1064. Dynamic behaviors of nonlinear fractional-order differential oscillator Joural of Mechaical Sciece ad Techology 3 (9) 58~64 Joural of Mechaical Sciece ad Techology www.sprigerlik.com/coe/738-494x DOI.7/s6-9-34-4 Dyamic behaviors of oliear fracioal-order differeial oscillaor

More information

Conditional distributions, exchangeable particle systems, and stochastic partial differential equations

Conditional distributions, exchangeable particle systems, and stochastic partial differential equations Codiioal diribuio, exchageable paricle yem, ad ochaic parial differeial equaio Da Cria, Thoma G. Kurz, Yoojug Lee 23 July 2 Abrac Sochaic parial differeial equaio whoe oluio are probabiliy-meaurevalued

More information

Ideal Amplifier/Attenuator. Memoryless. where k is some real constant. Integrator. System with memory

Ideal Amplifier/Attenuator. Memoryless. where k is some real constant. Integrator. System with memory Liear Time-Ivaria Sysems (LTI Sysems) Oulie Basic Sysem Properies Memoryless ad sysems wih memory (saic or dyamic) Causal ad o-causal sysems (Causaliy) Liear ad o-liear sysems (Lieariy) Sable ad o-sable

More information

David Randall. ( )e ikx. k = u x,t. u( x,t)e ikx dx L. x L /2. Recall that the proof of (1) and (2) involves use of the orthogonality condition.

David Randall. ( )e ikx. k = u x,t. u( x,t)e ikx dx L. x L /2. Recall that the proof of (1) and (2) involves use of the orthogonality condition. ! Revised April 21, 2010 1:27 P! 1 Fourier Series David Radall Assume ha u( x,) is real ad iegrable If he domai is periodic, wih period L, we ca express u( x,) exacly by a Fourier series expasio: ( ) =

More information

F D D D D F. smoothed value of the data including Y t the most recent data.

F D D D D F. smoothed value of the data including Y t the most recent data. Module 2 Forecasig 1. Wha is forecasig? Forecasig is defied as esimaig he fuure value ha a parameer will ake. Mos scieific forecasig mehods forecas he fuure value usig pas daa. I Operaios Maageme forecasig

More information

A note on deviation inequalities on {0, 1} n. by Julio Bernués*

A note on deviation inequalities on {0, 1} n. by Julio Bernués* A oe o deviaio iequaliies o {0, 1}. by Julio Berués* Deparameo de Maemáicas. Faculad de Ciecias Uiversidad de Zaragoza 50009-Zaragoza (Spai) I. Iroducio. Le f: (Ω, Σ, ) IR be a radom variable. Roughly

More information

On The Eneström-Kakeya Theorem

On The Eneström-Kakeya Theorem Applied Mahemaics,, 3, 555-56 doi:436/am673 Published Olie December (hp://wwwscirporg/oural/am) O The Eesröm-Kakeya Theorem Absrac Gulsha Sigh, Wali Mohammad Shah Bharahiar Uiversiy, Coimbaore, Idia Deparme

More information

10.3 Autocorrelation Function of Ergodic RP 10.4 Power Spectral Density of Ergodic RP 10.5 Normal RP (Gaussian RP)

10.3 Autocorrelation Function of Ergodic RP 10.4 Power Spectral Density of Ergodic RP 10.5 Normal RP (Gaussian RP) ENGG450 Probabiliy ad Saisics for Egieers Iroducio 3 Probabiliy 4 Probabiliy disribuios 5 Probabiliy Desiies Orgaizaio ad descripio of daa 6 Samplig disribuios 7 Ifereces cocerig a mea 8 Comparig wo reames

More information

Available online at J. Math. Comput. Sci. 4 (2014), No. 4, ISSN:

Available online at   J. Math. Comput. Sci. 4 (2014), No. 4, ISSN: Available olie a hp://sci.org J. Mah. Compu. Sci. 4 (2014), No. 4, 716-727 ISSN: 1927-5307 ON ITERATIVE TECHNIQUES FOR NUMERICAL SOLUTIONS OF LINEAR AND NONLINEAR DIFFERENTIAL EQUATIONS S.O. EDEKI *, A.A.

More information

Some Properties of Semi-E-Convex Function and Semi-E-Convex Programming*

Some Properties of Semi-E-Convex Function and Semi-E-Convex Programming* The Eighh Ieraioal Symposium o Operaios esearch ad Is Applicaios (ISOA 9) Zhagjiajie Chia Sepember 2 22 29 Copyrigh 29 OSC & APOC pp 33 39 Some Properies of Semi-E-Covex Fucio ad Semi-E-Covex Programmig*

More information

Energy Density / Energy Flux / Total Energy in 1D. Key Mathematics: density, flux, and the continuity equation.

Energy Density / Energy Flux / Total Energy in 1D. Key Mathematics: density, flux, and the continuity equation. ecure Phys 375 Eergy Desiy / Eergy Flu / oal Eergy i D Overview ad Moivaio: Fro your sudy of waves i iroducory physics you should be aware ha waves ca raspor eergy fro oe place o aoher cosider he geeraio

More information

S n. = n. Sum of first n terms of an A. P is

S n. = n. Sum of first n terms of an A. P is PROGREION I his secio we discuss hree impora series amely ) Arihmeic Progressio (A.P), ) Geomeric Progressio (G.P), ad 3) Harmoic Progressio (H.P) Which are very widely used i biological scieces ad humaiies.

More information

Extended Laguerre Polynomials

Extended Laguerre Polynomials I J Coemp Mah Scieces, Vol 7, 1, o, 189 194 Exeded Laguerre Polyomials Ada Kha Naioal College of Busiess Admiisraio ad Ecoomics Gulberg-III, Lahore, Pakisa adakhaariq@gmailcom G M Habibullah Naioal College

More information

Turing-Computability of Solution of Hirota Equation Dianchen Lu1, a and Liming Fu1, b

Turing-Computability of Solution of Hirota Equation Dianchen Lu1, a and Liming Fu1, b Ieraioal Coferece o Comper Sciece a Elecroic Techology (ICCSET ) Trig-Compailiy of Solio of iroa Eqaio Diache L a a Limig F Facly of Sciece Jiag Uiveriy Zheiag Jiag 3P..Chia a Email: cl@.e.c Email: 6786997@qq.com

More information

Calculus Limits. Limit of a function.. 1. One-Sided Limits...1. Infinite limits 2. Vertical Asymptotes...3. Calculating Limits Using the Limit Laws.

Calculus Limits. Limit of a function.. 1. One-Sided Limits...1. Infinite limits 2. Vertical Asymptotes...3. Calculating Limits Using the Limit Laws. Limi of a fucio.. Oe-Sided..... Ifiie limis Verical Asympoes... Calculaig Usig he Limi Laws.5 The Squeeze Theorem.6 The Precise Defiiio of a Limi......7 Coiuiy.8 Iermediae Value Theorem..9 Refereces..

More information

Research Article Generalized Equilibrium Problem with Mixed Relaxed Monotonicity

Research Article Generalized Equilibrium Problem with Mixed Relaxed Monotonicity e Scieific World Joural, Aricle ID 807324, 4 pages hp://dx.doi.org/10.1155/2014/807324 Research Aricle Geeralized Equilibrium Problem wih Mixed Relaxed Moooiciy Haider Abbas Rizvi, 1 Adem KJlJçma, 2 ad

More information

u t u 0 ( 7) Intuitively, the maximum principles can be explained by the following observation. Recall

u t u 0 ( 7) Intuitively, the maximum principles can be explained by the following observation. Recall Oct. Heat Equatio M aximum priciple I thi lecture we will dicu the maximum priciple ad uiquee of olutio for the heat equatio.. Maximum priciple. The heat equatio alo ejoy maximum priciple a the Laplace

More information

Applied Mathematical Sciences, Vol. 9, 2015, no. 3, HIKARI Ltd,

Applied Mathematical Sciences, Vol. 9, 2015, no. 3, HIKARI Ltd, Applied Mathematical Sciece Vol 9 5 o 3 7 - HIKARI Ltd wwwm-hiaricom http://dxdoiorg/988/am54884 O Poitive Defiite Solutio of the Noliear Matrix Equatio * A A I Saa'a A Zarea* Mathematical Sciece Departmet

More information

TAKA KUSANO. laculty of Science Hrosh tlnlersty 1982) (n-l) + + Pn(t)x 0, (n-l) + + Pn(t)Y f(t,y), XR R are continuous functions.

TAKA KUSANO. laculty of Science Hrosh tlnlersty 1982) (n-l) + + Pn(t)x 0, (n-l) + + Pn(t)Y f(t,y), XR R are continuous functions. Iera. J. Mah. & Mah. Si. Vol. 6 No. 3 (1983) 559-566 559 ASYMPTOTIC RELATIOHIPS BETWEEN TWO HIGHER ORDER ORDINARY DIFFERENTIAL EQUATIONS TAKA KUSANO laculy of Sciece Hrosh llersy 1982) ABSTRACT. Some asympoic

More information

Physics 240: Worksheet 16 Name

Physics 240: Worksheet 16 Name Phyic 4: Workhee 16 Nae Non-unifor circular oion Each of hee proble involve non-unifor circular oion wih a conan α. (1) Obain each of he equaion of oion for non-unifor circular oion under a conan acceleraion,

More information

A New Type of q-szász-mirakjan Operators

A New Type of q-szász-mirakjan Operators Filoat 3:8 07, 567 568 https://doi.org/0.98/fil7867c Published by Faculty of Scieces ad Matheatics, Uiversity of Niš, Serbia Available at: http://www.pf.i.ac.rs/filoat A New Type of -Szász-Miraka Operators

More information

An interesting result about subset sums. Nitu Kitchloo. Lior Pachter. November 27, Abstract

An interesting result about subset sums. Nitu Kitchloo. Lior Pachter. November 27, Abstract A ieresig resul abou subse sums Niu Kichloo Lior Pacher November 27, 1993 Absrac We cosider he problem of deermiig he umber of subses B f1; 2; : : :; g such ha P b2b b k mod, where k is a residue class

More information

Completeness of Random Exponential System in Half-strip

Completeness of Random Exponential System in Half-strip 23-24 Prepri for School of Mahemaical Scieces, Beijig Normal Uiversiy Compleeess of Radom Expoeial Sysem i Half-srip Gao ZhiQiag, Deg GuaTie ad Ke SiYu School of Mahemaical Scieces, Laboraory of Mahemaics

More information

Bernstein Direct Method for Solving. Variational Problems

Bernstein Direct Method for Solving. Variational Problems Ieraioal Maheaical Foru, 5,, o. 48, 35-37 Bersei Direc Mehod for Solvig Variaioal Probles Sadeep Dixi*, Viee K. Sigh**, Ai K. Sigh*, O P. Sigh* *Depare of Applied Maheaics, Isiue of echology, Baaras Hidu

More information

Prakash Chandra Rautaray 1, Ellipse 2

Prakash Chandra Rautaray 1, Ellipse 2 Prakash Chadra Rauara, Ellise / Ieraioal Joural of Egieerig Research ad Alicaios (IJERA) ISSN: 48-96 www.ijera.com Vol. 3, Issue, Jauar -Februar 3,.36-337 Degree Of Aroimaio Of Fucios B Modified Parial

More information

Stability. Outline Stability Sab Stability of Digital Systems. Stability for Continuous-time Systems. system is its stability:

Stability. Outline Stability Sab Stability of Digital Systems. Stability for Continuous-time Systems. system is its stability: Oulie Sabiliy Sab Sabiliy of Digial Syem Ieral Sabiliy Exeral Sabiliy Example Roo Locu v ime Repoe Fir Orer Seco Orer Sabiliy e Jury e Rouh Crierio Example Sabiliy A very impora propery of a yamic yem

More information

Numerical Solution of Parabolic Volterra Integro-Differential Equations via Backward-Euler Scheme

Numerical Solution of Parabolic Volterra Integro-Differential Equations via Backward-Euler Scheme America Joural of Compuaioal ad Applied Maemaics, (6): 77-8 DOI:.59/.acam.6. Numerical Soluio of Parabolic Volerra Iegro-Differeial Equaios via Bacward-Euler Sceme Ali Filiz Deparme of Maemaics, Ada Mederes

More information

A note on Generalized Hermite polynomials

A note on Generalized Hermite polynomials INTERNATIONAL JOURNAL OF APPLIED MATHEMATICS AND INFORMATICS Volue 8 14 A oe o Geeralized Herie poloials Cleee Cesarao Absrac B sarig fro he geeral heor of he oevariable Herie poloials we will iroduce

More information

A PROBABILITY PROBLEM

A PROBABILITY PROBLEM A PROBABILITY PROBLEM A big superarket chai has the followig policy: For every Euros you sped per buy, you ear oe poit (suppose, e.g., that = 3; i this case, if you sped 8.45 Euros, you get two poits,

More information

Suggested Solutions to Assignment 1 (REQUIRED)

Suggested Solutions to Assignment 1 (REQUIRED) EC 45 dvaced Macroecoomic Irucor: Sharif F ha Deparme of Ecoomic Wilfrid Laurier Uiveri Wier 28 Suggeed Soluio o igme (REQUIRED Toal Mar: 5 Par True/ Fale/ Ucerai Queio [2 mar] Explai wh he followig aeme

More information

UNIVERSITY OF TORONTO Faculty of Arts and Science MAY 2006 EXAMINATIONS ECO220Y1Y PART 1 OF 2. Duration - 3 hours

UNIVERSITY OF TORONTO Faculty of Arts and Science MAY 2006 EXAMINATIONS ECO220Y1Y PART 1 OF 2. Duration - 3 hours UNIVERSITY OF TORONTO Faculy of Ar ad Sciece MAY 6 EXAMINATIONS ECOYY PART OF Duraio - hour Eamiaio Aid: Calculaor, wo piece of paper wih ay yped or hadwrie oe (ma. ize: 8.5 ; boh ide of paper ca be ued)

More information

LOWER BOUNDS FOR THE BLOW-UP TIME OF NONLINEAR PARABOLIC PROBLEMS WITH ROBIN BOUNDARY CONDITIONS

LOWER BOUNDS FOR THE BLOW-UP TIME OF NONLINEAR PARABOLIC PROBLEMS WITH ROBIN BOUNDARY CONDITIONS Electroic Joural of Differetial Equatios, Vol. 214 214), No. 113, pp. 1 5. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.ut.edu ftp ejde.math.txstate.edu LOWER BOUNDS FOR THE BLOW-UP

More information

STRONG DEVIATION THEOREMS FOR THE SEQUENCE OF CONTINUOUS RANDOM VARIABLES AND THE APPROACH OF LAPLACE TRANSFORM

STRONG DEVIATION THEOREMS FOR THE SEQUENCE OF CONTINUOUS RANDOM VARIABLES AND THE APPROACH OF LAPLACE TRANSFORM Joural of Statitic: Advace i Theory ad Applicatio Volume, Number, 9, Page 35-47 STRONG DEVIATION THEORES FOR THE SEQUENCE OF CONTINUOUS RANDO VARIABLES AND THE APPROACH OF LAPLACE TRANSFOR School of athematic

More information

ODEs II, Supplement to Lectures 6 & 7: The Jordan Normal Form: Solving Autonomous, Homogeneous Linear Systems. April 2, 2003

ODEs II, Supplement to Lectures 6 & 7: The Jordan Normal Form: Solving Autonomous, Homogeneous Linear Systems. April 2, 2003 ODEs II, Suppleme o Lecures 6 & 7: The Jorda Normal Form: Solvig Auoomous, Homogeeous Liear Sysems April 2, 23 I his oe, we describe he Jorda ormal form of a marix ad use i o solve a geeral homogeeous

More information