Research Article Cubic Spline Collocation Method for Fractional Differential Equations

Size: px
Start display at page:

Download "Research Article Cubic Spline Collocation Method for Fractional Differential Equations"

Transcription

1 Hndaw Publshng orporaon Journal of Appled Mahemacs Volume 3, Arcle ID 8645, pages hp://dx.do.org/.55/3/8645 Research Arcle ubc Splne ollocaon Mehod for Fraconal Dfferenal Equaons Shu-Png Yang and A-Guo Xao Deparmen of Mahemacs, Huzhou Unversy, Guangdong 567, hna School of Mahemacs and ompuaonal Scence, Hunan Key Laboraory for ompuaon and Smulaon n Scence and Engneerng, Xangan Unversy, Hunan 45, hna orrespondence should be addressed o A-Guo Xao; xag@xu.edu.cn Receved February 3; Revsed 7 Aprl 3; Acceped 7 May 3 Academc Edor: Alan Mranvlle opyrgh 3 S.-P. Yang and A.-G. Xao. Ths s an open access arcle dsrbued under he reave ommons Arbuon Lcense, whch perms unresrced use, dsrbuon, and reproducon n any medum, provded he orgnal work s properly ced. We dscuss he cubc splne collocaon mehod wh wo parameers for solvng he nal value problems (IVPs of fraconal dfferenal equaons (FDEs. Some resuls of he local runcaon error, he convergence, and he sably of hs mehod for IVPs of FDEs are obaned. Some numercal examples verfy our heorecal resuls.. Inroducon Inherecenpasyears,heuseoffraconaldfferenal equaons (FDEs has ganed consderable populary n some felds (e.g., nonlnear oscllaon of earhquake [], flud-dynamc raffc model [], maeral vscoelasc heory and physcs [3 6], ec.. Based on hese requremens, he numercal approach has become very mporan o solve FDEs and analyze he expermenal daa whch are descrbed n a fraconal way. The numercal approaches o FDEs have been recenly suded by numerous auhors [6 5]. However, he sae of ar s far less advanced for general fraconal order dfferenal equaons. In he recen years, splne collocaon mehods ncludng wavele mehods have been successfully appled o some nal value problems (IVPs and nal-boundary valueproblemsoffdes[6 3]. Pedas and Tamme [6, 8] dscussed splne collocaon mehods for some classes of IVPs of lnear mulerm fraconal dfferenal equaons and obaned he correspondng convergence resuls. L e al. [9] used he hgher-order pecewse nerpolaon for he fraconal negral and fraconal dervaves, proposed a hgherorder algorhm based on he Smpson mehod for FDEs, and gave he error and sably resuls. L []appledhecubcbsplne wavele collocaon mehod o FDEs by he approach ha such problems are convered no a sysem of algebrac equaons whch s suable for compuer programmng. I s worh noce ha he splne collocaon mehods for he IVPs of FDEs are ofen acheved by her solvng of he equvalen IVPs of negral equaons wh weakly sngular kernels. In hs paper, he cubc splne collocaon mehod s desgned o solve drecly he IVPs of general FDEs. And he correspondng heorecal resuls of he local runcaon error, he convergence, and he sably of he cubc splne collocaon mehod for he IVPs of general FDEs are gven. Ths paper s organzed as follows. In Secon, we propose he splne cubc collocaon mehod for solvng he IVPs of FDEs. In Secon 3, he correspondng heorecal resuls of he convergence and he sably are also gven. In Secon 4, he heorecal resuls are denfed by some numercal examples. In he followng ex, we frs recall he basc defnons of fraconal calculus [6]. Usually, a Dα denoes he apuo fraconal dervave of order α as a Dα y ( I n α D n y ( = { Γ (n α ( τ n α d n y (τ dτ, a dτn = >a, f n <α<n, { d n { d n y (, f α=n, (

2 Journal of Appled Mahemacs where D n s he classcal dfferenal operaor of order n, y( s n mes connuously dfferenable, and I α denoes he negral operaor of order α as I α y ( = { { ( τ α y (τ dτ, a { I, > a, f α>, f α=, where I s he deny operaor. As s well known, here are some dfferen defnons of fraconal operaor excep he apuo fraconal dervave. From a heorecal pon of vew, he mos naural approach s he Remann-Louvlle defnon as R a Dα y ( =Dn I n a y ( d n = Γ (n α d n ( τ n α y (τ dτ, a >a,n <α n. The relaonshp beween he apuo defnon and he Remann-Louvlle defnon can be gven by he followng Lemma. Lemma (see [5, 6]. Le α>and n= α. Assume ha f( s n mes connuously dfferenable, D α f and R D α f exs; hen ( (3 R D α f ( = D α n f ( + f k ( Γ (k α+ ( k α. (4 k=. ubc Splne ollocaon Mehod for FDEs onsder he nal value problem Dα y ( =f(,y(, I=[, T], <α, y ( =y, where f:[,t] R Rs a gven connuous mappng and sasfes he Lpschz condon f (, y f(, z L y z, I = [, T], y,z R. (6 I s well known ha he IVP (5sequvalenoheproblem [4] y ( =y( + ( τ α f(τ,y(τdτ, y ( =y. Le = h ( =,,...,N, h = T/N,N > be he grd ponsof he unformparonof [, T] no he subnervals (5 (7 I =[, ], =,,...,N.OneachsubnervalI,hecubc -splne funcon S(, h canberepresenedas where S (, h S (, h =S (, h, (8 =(+ ( h h S ( + ( ( h 3 S ( +(+ h ( S ( ( ( h, h 3 S ( and S(, h = S ( =y,s ( =hy (. Le ξ=( /h [, ], ξ= ξ=( /h.wecan wre (9as S (, h =S ( + ξh, h (9 = ξ (ξ + S ( +ξ ξs ( +ξ (ξ+s ( ξ ξs (, ( where S ( =S(,h y(, S ( =hs (,h hy (, =,,...,N.Obvously,S(, h [, T], ands(, h y(, for all [,T]. Remark. In hs algorhm, he nal value y ( mus be provded, bu does no need o be gven n problem. Tha s, f we approxmae y (, hen he approxmaon of y ( s gven by usng he low-order mehods. In hs paper, we obaned approxmaon of y ( by usng one-order BDF mehod. Tha s, Then y(h y(h = y + y ( where h s a ny sepsze. h α Γ (α+ f(,y. ( y(h y (, ( h By usng he collocaon condons n each subnerval I and (5, we have Dα S(, h = +φh =f( +φh,s( + φh, h, φ {φ,φ }, (3

3 Journal of Appled Mahemacs 3 where φ,φ are he collocaon pons, and < φ < φ, s a consan. And accordng o (, we have ( S( +φ,h = (φ (φ + φ φ S ( ( S( +φ,h φ (φ + φ φ S ( +( φ (φ + φ φ φ (φ + φ φ ( S ( S ( n= [ 6φ (n, φ j S ( n +(φ (n, φ j φ (n, φ j 3φ (n, φ j S ( n +6φ (n, φ j S ( +(φ (n, φ j 3φ (n, φ j S ( n ] =Γ(4 α h α f( +φ j h, S ( +φ j h, j =,, (6 =(φ,φ ( S ( S ( +D(φ,φ ( S ( S (, (4 where φ j = φ j,=,. Usng he defnon of he apuo fraconal dervave n heform ( andusng(3, we have Γ ( α [ [ +φ j h n n= n S (τ, h dτ ( +φ j h τ α S (τ, h dτ ( +φ j h τ α ] ] =f( +φ j h, S ( +φ j h, h, j =,. Through calculaon, we can ge 6φ α j (α 3+φS ( +φ α j ( 3 + α + 3φ S ( (5 where φ (n, φ j =( n+φ j α ( α(3 α ( n+φ j α (3 α, φ (n, φ j = ( n+φ j α ( α(3 α ( n+φ j α (3 α +( n+φ j α (3 α, φ (n, φ j =φ (n, φ j +( n+φ j α ( α(3 α +( n+φ j α (3 α +( n+φ j 3 α ( n+φ j 3 α. (7 +6φ α j (α 3+φS ( +φ α j ( φ j +4φ j α+6φ j +6 5α+α S ( In order o oban he correspondng eraon formula, we denoe 6φ α (α 3+φ φ α ( 3 + α + 3φ A =( 6φ α (α 3+φ φ α ( 3 + α + 3φ, 6φ α (α 3+φ φ α ( φ +4φα+6φ +6 5α+α B =( 6φ α (α 3+φ φ α ( φ +4φα+6φ +6 5α+α, H ( = ( ( n= n= [ 6φ (n, φ S ( n +(φ (n, φ φ (n, φ 3φ (n, φ S ( n +6φ (n, φ S ( n +(φ (n, φ 3φ (n, φ S ( n ] [ 6φ (n, φ S ( n +(φ (n, φ φ (n, φ 3φ (n, φ S ( n +6φ (n, φ S ( n +(φ (n, φ 3φ (n, φ S ( n ]. (8

4 4 Journal of Appled Mahemacs Obvously, follows from he nequales φ <φ hahemarx A s nverble, and S = A BS +Γ(4 α h α A f A H (, (9 where f =(f +φ,f +φ T S =(S (,S ( T, =(f( +φ,s( +φ,h,f( +φ,s( +φ,h T. ( Le A= A B, B = A, H( = A H (. ( Then, follows ha S =AS +h α Γ (4 α Bf +H(. ( For (, we can oban her numercal soluons by usng he Newon erave mehod. In addon, applyng he collocaon condons n each subnerval I and usng (7, we have S(, h = +φh =y + +φh ( +φh τ α f(τ,s (τ, hdτ, φ {φ,φ }, (3 where φ,φ are he collocaon pons, < φ <φ, and S (, h =(+ ( h h S ( + ( ( h 3 S ( +(+ h ( S ( ( ( h, h 3 S ( (4 where S(, h = S ( = y, S ( = hy (, S ( = S(,h y(, S ( =hs (,h hy (, =,,...,N. Inhspaper,forconvenence,hecubcsplnecollocaon mehod based on he drec dscrezaon wh (3 scalled drec splne collocaon mehod (DSM for shor; and he cubc splne collocaon mehod based on he fraconal order negral equaons (7and(7 s called ndrec splne collocaon mehod (ISM for shor. 3. Theorecal Resuls Lemma 3 (see [5]. Suppose ha z n, n =,,...,N, and sasfy z n h α n c (n j α z j +c, n=,,...,n, (5 = where <α, c, c >s ndependen of h>.then z n c E α (c (nh α, n=,,...,n, (6 where E α s a Mag-Leffler funcon. Lemma 4. Assume ha he funcon g( [, T]. Then, for all φ [, ], [, T h],onehas +h (s τ α g (τ dτ +h = g ( + φh (s τ α dτ + o (h, (7 where <α, <s Ts a consan and sasfes +h=s or s ( + h h, (, ], o( s nfnesmal of hgher order. Proof. Usng he Taylor formula, we have g (τ = g ( + φh + g ( + φh (τ φh + o (h, τ [, + h]. Applyng he negral mean value heorem, we can oban +h (s τ α g (τ dτ +h = (s τ α (g(+φh+g ( + φh (τ φh+o(h dτ +h = g ( + φh (s τ α dτ +g +h ( + φh (s τ α (τ φhdτ+o(h +h = g ( + φh (s τ α dτ +g +h ( + φh (ξ φh (s τ α dτ + o (h +h = g ( + φh (s τ α dτ +g ( + φh (ξ φh [ α ((s α (s h α ] + o (h, (8 (9

5 Journal of Appled Mahemacs 5 where ξ [,+h].snceg( [, T], g ( s bounded on [, T].Wehave +h (s τ α g (τ dτ +h = g ( + φh (s τ α dτ +O(h α [(s α (s h α ] +o(h. onsder he followng. ( If s=+h,hen +h (s τ α g (τ dτ +h =g(+φh (s τ α dτ +O(h α [(+h α ]+o(h +h =g(+φh (s τ α dτ +O(h α hα +o(h +h =g(+φh (s τ α dτ +O(h +α +o(h +h =g(+φh (s τ α dτ + o (h. ( If h s ( + h,hen (3 (3 (s τ α (s (+h α α h α, τ [, + h], α [(s α (s h α ] Thus, +h = (s τ α +h dτ α h α dτ = α h α. (3 α [(s α (s h α ]=o(. (33 By means of (3, Lemma4s esablshed obvously. Theorem 5 (he local runcaon error. If he analycal soluon of he problem (5 y( 4 [, T], hen he local runcaon error of DSM s O(h 4. Proof. Applyng he Taylor expanson and he defnon of S(, h,wehave y ( =(+ ( h h y( + ( ( h 3 hy ( +(+ h ( y( h ( ( h 3 hy ( +O(( 4 = y ( +O(( 4, y ( = y ( +O(( 3, [, ]. (34 From he defnon of he apuo fraconal dervave, we oban Γ ( α [ [ Tha s, +φ j h n= n n (y (τ +O((τ 3 dτ ( +φ j h τ α y (τ dτ ( +φ j h τ α ] ] =f( +φ j h, y( +φ j h + O(φ j h 4, j =,. (35 +φjh Γ ( α y (τ dτ ( +φ j h τ α =f( +φ j h, y( +φ j h + O(φ j h 4 Γ ( α [ n= [ where j=,.moreover, y( ( hy ( n n y( =A( hy ( +hα Γ (4 α B y (τ dτ ( +φ j h τ α 3 +φ j h O((τ dτ + ] ( +φ j h τ α, ] f( +φ h, y( +φ h + O(φ h 4 ( f( +φ h, y( +φ h + O(φ h 4 (36

6 6 Journal of Appled Mahemacs h α A { n= ( { { n= n n n n y (τ dτ ( +φ h τ α y (τ dτ ( +φ h τ α 3 +φh Γ ( α O((τ dτ ( +φ h τ α } + ( 3 +φh Γ ( α O((τ dτ. ( +φ h τ α } ( } (37 Supposng S(, h = y(, for all [, ],and subsung y( no (3, we have y( y( ( hy ( =A( hy ( +hα Γ (4 α B f( +φ h, S ( +φ h, h ( f( +φ h, S ( +φ h, h + H ( +T, H ( = h α A ( ( = h α A ( n= n= n= n= n n n n n n n n S (τ, h dτ ( +φ h τ α S (τ, h dτ ( +φ h τ α y (τ dτ ( +φ h τ α (38 y (τ dτ, ( +φ h τ α S (, h =(+ ( h h y( + ( ( h 3 hy ( +(+ h ( y( h ( ( h 3 hy (, where T s he local runcaon error. (39 ombnng (38, (37whheLpschzcondonyelds T O((φ h 4 hα LΓ (4 α B ( O((φ h 4 +h α A ( Γ ( α (φ h α O(h3, Γ ( α (φ h α O(h3 T h 4, (4 where s an approprae posve consan. And he norm s he -norm of he marx ( n hs paper. ToproveheconvergenceofDSMforheproblem(5, we frs gve he followng lemmas. Lemma 6. If he analycal soluon of he problem (5 y( 4 [, T] and he marxes (φ,φ and D(φ,φ n (4 sasfy ha D (φ,φ exss, and D (φ,φ (φ,φ <, (4 hen he numercal soluons of ISM for problem (5 S(, h sasfy ha lm h S(, h = y(. Proof. For (3, we have S(, h = +φ j h =y + +φjh ( +φ j h τ α f(τ,s (τ, hdτ, S( +φ j h, h S (, h =y, j =,, =y + +φjh [ ( +φ j h τ α f(τ,s (τ, hdτ n= n ( +φ j h τ α f(τ,s (τ, hdτ] n j =,. (4 I follows from (7 ha he analycal soluon y( of he problem (5 sasfes y( +φ j h =y(+ +φjh [ ( +φ j h τ α f(τ,y(τdτ

7 Journal of Appled Mahemacs 7 n= Moreover, (44 and(45 yeld S( +φ j h, h y ( +φ j h = +φjh { ( +φ j h τ α n= n ( +φ j h τ α f(τ,y(τdτ], n [f(τ,s (τ, h f(τ,y(τ] dτ n ( +φ j h τ α n j =,. (43 [f(τ,s (τ, h f(τ,y(τ] dτ} n= n ( +φ j h τ α n f(τ,s (τ, h f(τ,y(τ dτ} L +φjh { ( +φ j h τ α S (τ, h y(τ dτ + n= = hα L { φj n= n ( +φ j h τ α S (τ, h y(τ dτ} n (φ j τ α S( + τh, h y ( +τh dτ ( n+φ j τ α S( n + τh, h y ( n +τh dτ}, j =,. = hα φ j { (φ j ξ α [f ( +ξh,s( + ξh, h n= ( + φ j n ξ α f ( +ξh,y( + ξh ] dξ [f( n +ξh,s( n + ξh, h f ( n +ξh,y( n + ξh] dξ}, j =,. I follows from he defnon of S(, h ha ( y( +hu (u + u u y( +hv =(u V (V + V V ( y( hy ( +( u (u+ u u V (V + V V ( y( + hy ( + =(u, V ( y hy +D(u, V ( y + hy + +O(h 4, u,v [, ], (45 (46 By usng he Lpschz condon, we have S( +φ j h, h y ( +φ j h +φjh = { ( +φ j h τ α [f(τ,s (τ, h f(τ,y(τ] dτ (44 where u= u,v = V.Obvously,for(4and(46, he marxes (u, V and D(u, V are connuous on [, ] [, ]; hus, we have ( S( +hu,h y( +hu S( +hv,h y( +hv =( u (u + u V V (V + V V S( ( S ( y( hy ( n= n ( +φ j h τ α n [f(τ,s (τ, h f(τ,y(τ] dτ} +φjh { ( +φ j h τ α f(τ,s (τ, h f(τ,y(τ dτ +( u (u+ u u V (V + V V =(u, V ( S( y( S ( hy ( S( ( + y( + S ( + hy ( + +D(u, V ( S( + y( + S ( + hy ( + +O(h4, u, V [, ]. (47

8 8 Journal of Appled Mahemacs Therefore, here exs λ >,λ >such ha λ = sup u<v (u, V, λ = sup u<v D (u, V, λ=λ +λ. Obvously, φ j (φ j ξ α dξ = α (φ j ξ α φ j = α (φ j α α, φ j [,]. Applyng he negral mean heorem, we have ( n+φ j ξ α dξ =( n+φ j θ α ( θ ( n α ( + φ α j θ n ( n α ( + φ j n α. (48 (49 (5 I follows from he nequales < φ <φ and n ha ( n + φ j ξ α dξ ( n α ( + φ α j n ( n α ( + φ j α ( n α α, j =,. ombnng (45, (48, and (49 wh(5 and defnng ε =( S( S( y(, hy ( ε S( +φ,h y( +φ =(, S( +φ,h y( +φ X = max { n + ε n }, where +φj = +φ j h, j =,,wecanoban ε hα L[ (λ ε +λ ε + α + h 4 ((+ hα Γ (α+ + α n= ( n α (λ ε n +λ ε n+ ] (5 (5 h α L[ Γ (α+ λx + α n= ( n α λx n ]+ h 4, (53 where, are some posve consans. If he marx D(φ,φ s nverble, hen follows from (47hawehave ( Hence, S ( + y( + S ( + hy ( + = D (φ,φ (φ,φ ( S ( y( S ( hy ( +D (φ,φ ( S( +hφ,h y( +hφ S( +hφ,h y( +hφ +O(h 4. ε + D (φ,φ (φ,φ ε + D (φ,φ ε + 3 h 4 D (φ,φ (φ,φ X + D (φ,φ ε + 3 h 4, (54 (55 where 3 s an approprae posve consan. Take ε l+ = max n + ε n =X, l.thenx l = max n l+ ε n = ε l+, X =X l,and X l = ε l+ D (φ,φ (φ,φ ε l + D (φ,φ ε l + 3 h 4 D (φ,φ (φ,φ X l + D (φ,φ ε l + 3 h 4. Snce D (φ,φ (φ,φ <,wehave (56 ( D (φ,φ (φ,φ X l D (φ,φ ε l + 3 h 4, X l ε l + 4 h 4, (57

9 Journal of Appled Mahemacs 9 where = D (φ,φ /( D (φ,φ (φ,φ, 4 s an approprae posve consan. Accordng o (53, we oban X l h α L[ Γ (α+ λx l + l α n= ( h α Lλ Γ (α+ X l h α L( (l n α λx n ]+ 5 h 4, l α n= (l n α λx n + 5 h 4, (58 where 5 > s an approprae consan. Obvously, here exs (, and h >such ha h α Lλ/Γ(α+ < for h<h.thus, X l h α Lλ ( ( l α n= Le = α λ/( Γ(α;hen (l n α X n + 6 h 4. (59 ε + X l h α l ( (l n α X n + 6 h 4, (6 n= where 6 >s an approprae consan. Applyng Lemma 3, we ge By means of (4, (47, we oban sup S (, h y( T max { sup (u, V N ε u<v + sup D (u, V ε + }+ 7 h 4 u<v (λ +λ E α ( T α 6 h h 4 [ 7 +(λ +λ 6 E α ( T α ] h 4, where 7 s a posve consan. onsequenly, we have Remark 7. ( If φ =φ,hen s nverble, and (63 lm h S (, h =y(. (64 φ (φ + φ φ D(φ,φ =( (65 φ (φ + φ φ ε + X l 6 h 4 E α ((lh α 6 h 4 E α ( T α. (6 By usng he convergence of he Mag-Leffler funcon E α (z [6], we have + φ D φ (φ,φ =( ( φ +φ 3 + φ φ ( φ +φ + φ φ ( φ +φ. ( φ φ ( φ +φ X l, ε + (h. (6 ( onsder (φ φ +φ +φ ( +φ ( +φ D φ (φ,φ (φ,φ =( φ φ 3φ +φ φ 3φ +φ φ φ ( + φ ( +φ φ φ φ φ φ +3 φ φ φ. (67 When D (φ,φ (φ,φ <, herangeofvalues φ,φ canbeobanedbyusngalgorhm 8, whchcanbe shown n Fgures and,respecvely. Algorhm 8. For φ For φ <φ f D (φ,φ (φ,φ < record φ,φ ; end end end plo(φ,φ.

10 Journal of Appled Mahemacs φ.94 φ φ φ (a (b Fgure : The range of values φ,φ when D <(a or D <(b. and he perurbed problem φ Dα z ( =f(, z (, I = [, T], <α, z ( =z, (69 where f sasfes he Lpschz condon (6,respecvely.Then here exss he consan h >such ha, for all h<h,when ys( n,h zs( n,h y z, here exss he consan >such ha ys( n,h zs( n,h y z ;here > s a consan, n=,,...,n. Proof. Frsly, we gve he proof of he concluson (. Applyng DSM, we have φ Fgure : The range of values φ,φ when D <. Dα S (, h = +φh =f( +φh,s( +φh,h, Snce S(, h [, T],weoban =,...,N. (7 Lemma 9. If he analycal soluon of he problem (5 y( 4 [, T], he splne funcons S(, h and S(, h defned as (9 and (4 on he same grds are he numercal soluons of he problem (5 obaned by DSM and ISM, respecvely; hen we have he followng conclusons. ( If lm h S(, h = y(, henlm h S(, h = y(, where y( s he analycal soluon of he problem (5. ( Assume ha ys(, h, zs(, h and ys(, h, zs(, h are he numercal soluons obaned by DSM and ISM for he problem Dα y ( =f(,y(, I=[, T], <α, y ( =y, (68 S( + φh, h =y + +φh =y + [ n= ( +φh τ α Dα τs (τ, h dτ n ( +φh τ α Dα τs (τ, h dτ n +φh + ( +φh τ α Dα τs (τ, h dτ]. (7

11 Journal of Appled Mahemacs I follows from Lemma 4 ha S( + φh, h =y =y + [ n= ( Dα τ S (τ, h τ= n +φ n ( +φh τ α dτ + o (h n + Dα τ S(τ, h τ= +φh +φh ( +φh τ α dτ + o (h ] + [ Dα τ S (τ, h τ= n +φ n= n ( +φh τ α dτ n + Dα τ S (τ, h τ= +φh =y + [ n= +φh + ( +φh τ α f (τ, S (τ, h dτ + o (h ]+o( n ( +φh τ α f (τ, S (τ, h dτ n +φh + ( +φh τ α f (τ, S (τ, h dτ] + o (, (74 where here exss a consan 8 >,γ>such ha o( = 8 h γ. Based on he defnons of S(, h, S(, h,followsha S( +φ j h, h S( +φ j h, h +φjh { ( +φ j h τ α [f(τ, S (τ, h f(τ,s (τ, h] dτ +φh ( +φh τ α dτ] + o (, where o( as h. By means of (7and(7, we oban S( + φh, h =y + [ f( n +φ,s( n +φ,h n= Applyng Lemma4,we ge S( + φh, h =y + [ n ( +φh τ α dτ n +f( +φh,s( + φh, h +φh ( +φh τ α dτ] + o (. n= n ( ( +φh τ α n f (τ, S (τ, h dτ + o (h (7 ( h γ n= n ( +φ j h τ α n [f(τ, S (τ, h f(τ,s (τ, h] dτ} +φjh { ( +φ j h τ α f (τ, S (τ, h f(τ,s (τ, h dτ n= n ( +φ j h τ α n f (τ, S (τ, h f(τ,s (τ, h dτ} + 8 h γ L +φjh { ( +φ j h τ α n= S (τ, h S (τ, h dτ n ( +φ j h τ α n S (τ, h S (τ, h dτ} + 8 h γ, j =,. (75

12 Journal of Appled Mahemacs Based on he smlar proof o ha of Lemma6, follows from Lemma 3 and he nequaly D (φ,φ (φ,φ < ha ε 9 h γ E α ( T α, =,,...,N, (76 where S( S ( ε =(, (77 S( S ( and s defned n Lemma 6, 9 >s a consan. By means of he convergence of he Mag-Leffler funcon E α (z [6], we ge From Lemma 6,wehave ε, h ; lm S (, h = lm S (, h. (78 h h lm S (, h =y(, h (79 lm S (, h = lm S (, h =y(. h h Now, we gve he proof of he concluson ( of Lemma 6. Accordng o he concluson (, we ge ys ( n, h zs ( n,h = ys ( n,h ys( n,h+ys( n,h Theorem (convergence of DSM. If he analycal soluon of he problem (5 y( 4 [, T] and he marxes (φ,φ and D(φ,φ of (4 sasfy ha D (φ,φ exss, and D (φ,φ (φ,φ <, (83 hen DSM s convergen, and lm h S(, h = y(. Proof. Ths resul follows drecly from Lemmas 6 and 9. Now, we consder he sably of DSM. Theorem (sably of DSM. If he analycal soluon of he problem (5 y( 4 [, T] and he marxes (φ,φ and D(φ,φ n (4 sasfy ha D (φ,φ exss and D (φ,φ (φ,φ <, (84 hen ISM s sable; ha s f ISM s, appled o solve he problem (68 and he perurbed problem (69, respecvely, hen, for all <h<h (h >s a consan, one has ( where ε y z, =,,...,N, (85 zs( n,h+zs( n, h zs ( n,h ys ( n,h ys( n,h + ys( n,h zs( n,h (8 ys( ε =( zs ( ys( zs (, (86 + zs( n,h zs( n,h max N ye (,h + max N ze (,h + y z, n=,,...,n, where ye(, h = ys(, h ys(, h, ze(, h = zs(, h zs(, h. Accordng o he proof of he concluson (, here exss h >such ha, for all h<h, Then, max N ye (,h + max N ze (,h y z. (8 ys ( n, h zs ( n,h (+ y z, n=,,...,n. (8 Obvously, ake =+ ; hence, he concluson ( s rgh. ( > s a consan, {ys (,ys ( } are he numercal soluons of he problem (68,and{zS (,zs ( } are he numercal soluons of he perurbed problem (69,and sup ys (, h zs (, h y z, (87 T where >s a consan, ys(, h s he numercal soluon of he problem (68,andzS(, h s he numercal soluon of he problem (69. Moreover, DSM s sable. Proof. Accordng o Lemma 9, f ISM s sable, hendsm ssable.inhefollowngex,wegveheproofofsablyof ISM.

13 Journal of Appled Mahemacs 3 By usng ISM o solve he problem (68andheproblem (69, we have [f(τ,ys (τ, h f(τ,zs (τ, h] dτ} ys (, h = +φ j h =y + +φjh ( +φ j h τ α f(τ,ys (τ, h dτ, j =,, ys (, h =y, zs (, h = +φ j h =z + +φjh ( +φ j h τ α f(τ,zs (τ, h dτ, j =,, zs (, h =z. (88 =(y z + hα φ j { (φ j ξ α [f( +ξh,ys( + ξh, h f ( +ξh,zs( + ξh, h] dξ n= ( + φ j n ξ α [f( n +ξh,ys( n + ξh, h f ( n +ξh,zs( n + ξh, h] dξ}, The prevous equaons can be wren as ys( +φ j h, h =y + +φjh [ ( +φ j h τ α f(τ,ys (τ, hdτ n= n ( +φ j h τ α f(τ,ys (τ, hdτ], n Applyng he Lpschz condon, we ge ys( +φ j h, h zs( +φ j h, h y z j =,. (9 zs( +φ j h, h =z + +φjh [ ( +φ j h τ α f(τ,zs (τ, hdτ Thus, n= ys( +φ j h, h zs( +φ j h, h =(y z + +φ j h { ( +φ j h τ α j =,, (89 n ( +φ j h τ α f(τ,zs (τ, hdτ], n [f(τ,ys (τ, h f(τ,zs (τ, h] dτ n= n ( +φ j h τ α n j =,. (9 +φjh + { ( +φ j h τ α [f(τ,ys (τ, h f(τ,zs (τ, h] dτ y z n= n ( +φ j h τ α n + +φjh { ( +φ j h τ α [f(τ,ys (τ, h f(τ,zs (τ, h] dτ} f(τ,ys (τ, h f(τ,zs (τ, h dτ n= n ( +φ j h τ α n f(τ,ys (τ, h f(τ,zs (τ, h dτ} y z + L +φjh { ( +φ j h τ α

14 4 Journal of Appled Mahemacs y( Numercal soluon by DSM Exac soluon Fgure 3: The error beween he numercal soluons and he exac soluon of Example ; α =.75. ys (τ, h zs (τ, h dτ n= n ( +φ j h τ α n ys( ε =( zs ( ys( zs (, X = max { n + ε n }, ε ys( +φ,h zs( +φ,h =(, ys( +φ,h zs( +φ,h where +φj = +φ j h, j =,. I follows from (9, (93, (49, and (5ha ε y z +h α L[ y z + (λ ε +λ ε + α α n= ( n α (λ ε n +λ ε n+ ] +h α L[ Γ (α+ (λx + n= α ( n α (λx n ] (93 (94 = y z ys (τ, h zs (τ, h dτ} y z +h α L[ Γ (α+ λx + + hα L { φj (φ j τ α ys( + τh, h zs( + τh, h dτ n= ( n + φ j τ α ys( n + τh, h zs( n + τh, h dτ}, α n= ( n α λx n ]. Take ε l+ =max n + { ε n } = X ;hence,x =X l, l. Accordng o he fac ha D(φ,φ s nverble and D (φ,φ (φ,φ <,wehave X l = ε l+ D (φ,φ (φ,φ ε l (9 + D (φ,φ ε l where j=,. Noe ha he defnons of ys(, h, zs(, h. Le λ = sup u<v (u, V, λ = max D (u, V, u<v λ=λ +λ, D (φ,φ (φ,φ X l + D (φ,φ ε l, ( D (φ,φ (φ,φ X l D (φ,φ ε l. (95 Moreover, X l ε l, (96

15 Journal of Appled Mahemacs 5.3 3E 7.5.5E 7. y(.5. Error E 7.5E 7 E 7.5 5E Numercal soluon by DSM Exac soluon Absolue error (a (b Fgure 4: The error beween he numercal soluons and he exac soluon of he problem (9; h =.5, α =.. where = D (φ,φ /( D (φ,φ (φ,φ. By means of (94, we have X l y z + h α L[ Γ (α+ λx l (97 Applyng Lemma3 yelds X l ( y z E α ((lh α ( y z E α ( T α. ( ( h α Lλ Γ (α+ X l + l α n= (l n α λx n ], Usng he convergence of Mag-Leffler funcon E α (z and denong = ( E α ( T α, ( y z (98 we oban + Lh α ( l α n= (l n α λx n. ε + X =X l y z. (3 Obvously, here exs (, and h h α Lλ/Γ(α + <as h<h.then > such ha Moreover, from he defnons of ys(, h and zs(, h,we have X l ( ( y z + h α L l α n= Le = α Lλ/( Γ(α.Weoban X l ( l (l n α X n. (99 y z + hα (l n α X n. ( n= ( ys( +hu,h zs( +hu,h ys( +hv,h zs( +hv,h ( =( u (u + u ys V V (V + V V ( +( u (u+ u u V (V + zs ( ys ( zs ( ( ys V V ( + zs( + ys ( + zs( +

16 6 Journal of Appled Mahemacs Table : The absolue errors of DSM (φ =.85, φ =.99 and he mehods repored n [, ]; α =.5. Error by DSM Error by [] Errorby[] Table : The absolue errors of DSM (φ =.9, φ =.98 and he mehods repored n [, ]; α =.75. Error by DSM Error by [] Errorby[] =(u, V ( ys( ys ( zs ( ys ( +D(u, V ( By means of (3, we ge zs ( + zs( + ys ( + zs( + sup ys (, h zs (, h T, u,v [, ]. max { sup (u, V N ε u<v + sup D (u, V ε + } u<v (λ +λ y z y z, (4 (5 where =(λ +λ ; ha s, ISM s sable. Accordng o Lemma 9,DSMssable. 4. Illusrave Examples In order o demonsrae our heorecal resuls, we apply DSM o he problem (5 and presen some numercal examples n hs secon. Le N error L =h S(,h y(, error L order L order L = N =(h = S(,h y( = log / error L (h/ error L (h, / = log / error L (h/ error L (h, (6,

17 Journal of Appled Mahemacs 7 Table 3: The error beween he numercal soluons and he exac soluon of he problem (9; α =.5, φ =.88, φ =.98. h error L Order L error L Order L / / / / / Table 4: The error beween he numercal soluons and he exac soluon of he problem (9; α =.75, φ =.95, φ =.99. h error L Order L error L Order L / / / / / where error (h s he error funcon whch depends on he sepsze h. Example. onsder he nal value problem [, ] Dα y ( = y( + + α Γ (3 α, The exac soluon s y( =. I=[, ], <α<, y ( =. (7 For dfferen values of α (,,henumercalsoluons for problem (7 are obaned by usng DSM, fas wavele collocaon mehod (FWM for shor repored n [], and he mehod repored n []. When α =.5,hemesepsze h = /6; he absolue errors of DSM, FWM, and he mehod repored n []are shown n Table.When α =.75, h = /6; he absolue errors of hese mehods are shown n Table. The numercal soluons and he exac soluon are shown n Fgure 3. From he numercal resuls, he resuls obaned by DSM are beer han by FWM and he mehod repored n [] n erms of accuracy f he exac soluon s suffcenly smooh. Therefore, DSM s a vald mehod n solvng fraconal dfferenal equaon. Example. onsder he nal value problem [] 43 Dα y ( = Γ (9 α 8 α 3 Γ (5+α/ Γ (5 α/ 4 α/ Γ (+α +(3 α/ 4 3 y( 3/, The exac soluon s y( = α/ + (9/4 α.obvously, y( 4 [, ]. In order o verfy our heorecal resuls, we modfy problem (8 as follows: 43 Dα y ( = Γ (9 α 8 α 3 Γ (7+α/ Γ (7 α/ 6 α/ Γ (5+α 4 +( 3 +α/ 4 3 y( 3/, y ( =, <α. The exac soluon s y( = α/ + (9/4 4+α. I=[, ], (9 Tables 3 and 4 ls he errors and he error orders of DSM wh α=.5and α =.75 and show ha he errors beween he numercal soluons and he exac soluon are very small, respecvely. Fgures 4 and 5 llusrae hgh accuracy of DSM wh φ =.9, φ =.98 and show ha he error s also very small. All of he numercal resuls show ha DSM for solvng nonlnear FDEs s convergen and he mehod s robus. Example 3. onsder he nal value problem Dα y ( +y ( =f(, I = [, T], <α, y ( =θ ( andheperurbedproblem I=[, ], Dα z ( +z ( =f(, I = [, T], < α, z ( =θ. ( y ( =, <α. (8

18 8 Journal of Appled Mahemacs.5 E 5. y(.5. Error.5E 5 E 5.5 5E Numercal soluon by DSM Exac soluon (a Absolue error (b Fgure 5: The error beween he numercal soluons and he exac soluon of he problem (9; α =.9, h =.5. y( θ =. θ =. (a Error Absolue error (b Fgure 6: The numercal resuls of he problems (and(; h =.5, T =., α =.8, θ =., θ =., φ =.9, φ =.98. We use he cubc splne collocaon mehod o solve he problems ( and(, respecvely. Selecng f( = sn(, T =, θ =., θ =., weobanhenumercal resuls gven n Fgure 6. Whenf( = sn(, T =, θ =., θ =., he numercal resuls are gven n Fgure 7. When f( = e, T =, θ =., θ =., henumercal resuls are shown n Fgure 8. From hese fgures, we can see ha he absolue errors of he numercal soluons of he problems ( and( decrease and fnally end o as ncreases. Thus, we can draw he concluson ha he cubc splne collocaon mehod for nonlnear FDEs s sable. The numercal resuls verfy our heorecal resuls. 5. oncluson Inhspaper,hecubcsplnecollocaonmehodwhwo parameers s successfully appled o he IVPs of general FDEs. The resul of he local runcaon error of hs mehod sgven.andheconvergenceandsablyresulsofhecubc

19 Journal of Appled Mahemacs 9 4 y( θ = θ = (a Error Absolue error (b Fgure 7: The numercal resuls of he problems (and(; h =.5, α =.8, θ =., θ =., φ =.9, φ =.98. y(, z( θ = θ = (a Error Absolue error (b Fgure 8: The numercal resuls of he problems (and(; h =.5, α =.8, θ =., θ =., φ =.9, φ =.98. splne collocaon mehod for he fraconal order negral equaons whch s equvalen o he IVPs of general FDEs are obaned. By usng he relaonshp beween he numercal soluons from he cubc splne mehod for he IVPs of general FDEs and he numercal soluons obaned from he cubc splne mehod for he correspondng equvalen IVPs of fraconal order negral equaons, we also oban some resuls of he convergence and he sably of he mehod for he IVPs of general FDEs. Some numercal examples successfully verfy our heorecal resuls and show ha he gven mehod s effcen. Acknowledgmens Ths work s suppored by projecs from NSF of hna (no. 73, no. 63, and no. 6444, Program for hangjang Scholars and Innovave Research Team n Unversy of hna (no. IRT79, he Ad Program

20 Journal of Appled Mahemacs for Scence and Technology Innovave Research Team n Hgher Educaonal Insuons of Hunan Provnce of hna, Huzhou Scence and Technology Program (no. 3, and NSF of Huzhou Unversy (no. YB5. References [] D. Delbosco and L. Rodno, Exsence and unqueness for a nonlnear fraconal dfferenal equaon, Journal of Mahemacal Analyss and Applcaons, vol.4,no.,pp.69 65, 996. [] J. H. He, Some applcaons of nonlnear fraconal dfferenal equaons and herapproxmaons, Bullen of Scence, Technology,vol.5,no.,pp.86 9,999. [3] V. V. Uchakn and R. T. Sbaov, Fraconal heory for ranspor n dsordered semconducors, ommuncaons n Nonlnear Scence and Numercal Smulaon, vol.3,no.4,pp.75 77, 8. [4] V. E. Tarasov and G. M. Zaslavsky, Fraconal dynamcs of sysems wh long-range neracon, ommuncaons n Nonlnear Scence and Numercal Smulaon, vol.,no.8,pp , 6. [5] K. Dehelm, The Analyss of Fraconal Dfferenal Equaons, vol. 4 of Lecure Noes n Mahemacs, Sprnger, Berln, Germany,. [6] I. Podlubny, Fraconal Dfferenal Equaons,vol.98ofMahemacs n Scence and Engneerng, Academc Press, New York, NY, USA, 999. [7] h. Lubch, Runge-Kua heory for Volerra and Abel negral equaons of he second knd, Mahemacs of ompuaon, vol. 4, no. 63, pp. 87, 983. [8] h. Lubch, Fraconal lnear mulsep mehods for Abel- Volerra negral equaons of he second knd, Mahemacs of ompuaon,vol.45,no.7,pp ,985. [9] h. Lubch, Dscrezed fraconal calculus, SIAM Journal on Mahemacal Analyss,vol.7,no.3,pp.74 79,986. [] K. Dehelm, An algorhm for he numercal soluon of dfferenal equaons of fraconal order, Elecronc Transacons on Numercal Analyss,vol.5,pp. 6,997. [] K. Dehelm and G. Walz, Numercal soluon of fraconal order dfferenal equaons by exrapolaon, Numercal Algorhms,vol.6,no.3-4,pp.3 53,997. [] K.Dehelm,N.J.Ford,andA.D.Freed, Apredcor-correcor approach for he numercal soluon of fraconal dfferenal equaons, Nonlnear Dynamcs,vol.9,no. 4,pp.3,. [3] K. Dehelm and N. J. Ford, Numercal soluon of he Bagley- Torvk equaon, BIT,vol.4, no.3,pp ,. [4] F. Lu, V. Anh, and I. Turner, Numercal soluon of he space fraconal Fokker-Planck equaon, Journalofompuaonal and Appled Mahemacs, vol. 66, pp. 9 9, 4. [5] F.Lu,P.Zhuang,V.Anh,I.Turner,andK.Burrage, Sably and convergence of he dfference mehods for he space-me fraconal advecon-dffuson equaon, Appled Mahemacs and ompuaon,vol.9,no.,pp.,7. [6] A. Pedas and E. Tamme, Splne collocaon mehods for lnear mul-erm fraconal dfferenal equaons, Journal of ompuaonal and Appled Mahemacs, vol.36,no.,pp ,. [7] A. Pedas and E. Tamme, Splne collocaon mehod for negrodfferenal equaons wh weakly sngular kernels, Journal of ompuaonal and Appled Mahemacs,vol.97,no.,pp.53 69, 6. [8] A. Pedas and E. Tamme, On he convergence of splne collocaon mehods for solvng fraconal dfferenal equaons, Journal of ompuaonal and Appled Mahemacs,vol.35,no., pp ,. [9]. L, A. hen, and J. Ye, Numercal approaches o fraconal calculus and fraconal ordnary dfferenal equaon, Journal of ompuaonal Physcs,vol.3,no.9,pp ,. [] J. T. Kemppanen and K. M. Ruosalanen, On he splne collocaon mehod for he sngle layer equaon relaed o mefraconal dffuson, Numercal Algorhms, vol.57,no.3,pp ,. [] X. L, Numercal soluon of fraconal dfferenal equaons usng cubc B-splne wavele collocaon mehod, ommuncaons n Nonlnear Scence and Numercal Smulaon,vol.7,no., pp ,. [] F. Dubos and S. Mengué, Mxed collocaon for fraconal dfferenal equaons, Numercal Algorhms, vol.34,no. 4, pp. 33 3, 3. [3] E. A. Rawashdeh, Numercal soluon of semdfferenal equaons by collocaon mehod, Appled Mahemacs and ompuaon,vol.74,no.,pp ,6. [4] M. Welbeer, Effcen Numercal Mehods for Fraconal Dfferenal Equaons and her Analycal Background, Paperfleger, 6. [5] J. Dxon and S. McKee, Weakly sngular dscree Gronwall nequales, Zeschrf für Angewande Mahemak und Mechank, vol. 66, no., pp , 986.

21 Advances n Operaons Research Hndaw Publshng orporaon hp:// Volume 4 Advances n Decson Scences Hndaw Publshng orporaon hp:// Volume 4 Journal of Appled Mahemacs Algebra Hndaw Publshng orporaon hp:// Hndaw Publshng orporaon hp:// Volume 4 Journal of Probably and Sascs Volume 4 The Scenfc World Journal Hndaw Publshng orporaon hp:// Hndaw Publshng orporaon hp:// Volume 4 Inernaonal Journal of Dfferenal Equaons Hndaw Publshng orporaon hp:// Volume 4 Volume 4 Subm your manuscrps a hp:// Inernaonal Journal of Advances n ombnaorcs Hndaw Publshng orporaon hp:// Mahemacal Physcs Hndaw Publshng orporaon hp:// Volume 4 Journal of omplex Analyss Hndaw Publshng orporaon hp:// Volume 4 Inernaonal Journal of Mahemacs and Mahemacal Scences Mahemacal Problems n Engneerng Journal of Mahemacs Hndaw Publshng orporaon hp:// Volume 4 Hndaw Publshng orporaon hp:// Volume 4 Volume 4 Hndaw Publshng orporaon hp:// Volume 4 Dscree Mahemacs Journal of Volume 4 Hndaw Publshng orporaon hp:// Dscree Dynamcs n Naure and Socey Journal of Funcon Spaces Hndaw Publshng orporaon hp:// Absrac and Appled Analyss Volume 4 Hndaw Publshng orporaon hp:// Volume 4 Hndaw Publshng orporaon hp:// Volume 4 Inernaonal Journal of Journal of Sochasc Analyss Opmzaon Hndaw Publshng orporaon hp:// Hndaw Publshng orporaon hp:// Volume 4 Volume 4

Existence and Uniqueness Results for Random Impulsive Integro-Differential Equation

Existence and Uniqueness Results for Random Impulsive Integro-Differential Equation Global Journal of Pure and Appled Mahemacs. ISSN 973-768 Volume 4, Number 6 (8), pp. 89-87 Research Inda Publcaons hp://www.rpublcaon.com Exsence and Unqueness Resuls for Random Impulsve Inegro-Dfferenal

More information

Approximate Analytic Solution of (2+1) - Dimensional Zakharov-Kuznetsov(Zk) Equations Using Homotopy

Approximate Analytic Solution of (2+1) - Dimensional Zakharov-Kuznetsov(Zk) Equations Using Homotopy Arcle Inernaonal Journal of Modern Mahemacal Scences, 4, (): - Inernaonal Journal of Modern Mahemacal Scences Journal homepage: www.modernscenfcpress.com/journals/jmms.aspx ISSN: 66-86X Florda, USA Approxmae

More information

On One Analytic Method of. Constructing Program Controls

On One Analytic Method of. Constructing Program Controls Appled Mahemacal Scences, Vol. 9, 05, no. 8, 409-407 HIKARI Ld, www.m-hkar.com hp://dx.do.org/0.988/ams.05.54349 On One Analyc Mehod of Consrucng Program Conrols A. N. Kvko, S. V. Chsyakov and Yu. E. Balyna

More information

A NEW TECHNIQUE FOR SOLVING THE 1-D BURGERS EQUATION

A NEW TECHNIQUE FOR SOLVING THE 1-D BURGERS EQUATION S19 A NEW TECHNIQUE FOR SOLVING THE 1-D BURGERS EQUATION by Xaojun YANG a,b, Yugu YANG a*, Carlo CATTANI c, and Mngzheng ZHU b a Sae Key Laboraory for Geomechancs and Deep Underground Engneerng, Chna Unversy

More information

On computing differential transform of nonlinear non-autonomous functions and its applications

On computing differential transform of nonlinear non-autonomous functions and its applications On compung dfferenal ransform of nonlnear non-auonomous funcons and s applcaons Essam. R. El-Zahar, and Abdelhalm Ebad Deparmen of Mahemacs, Faculy of Scences and Humanes, Prnce Saam Bn Abdulazz Unversy,

More information

HEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD

HEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD Journal of Appled Mahemacs and Compuaonal Mechancs 3, (), 45-5 HEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD Sansław Kukla, Urszula Sedlecka Insue of Mahemacs,

More information

Method of upper lower solutions for nonlinear system of fractional differential equations and applications

Method of upper lower solutions for nonlinear system of fractional differential equations and applications Malaya Journal of Maemak, Vol. 6, No. 3, 467-472, 218 hps://do.org/1.26637/mjm63/1 Mehod of upper lower soluons for nonlnear sysem of fraconal dfferenal equaons and applcaons D.B. Dhagude1 *, N.B. Jadhav2

More information

GENERATING CERTAIN QUINTIC IRREDUCIBLE POLYNOMIALS OVER FINITE FIELDS. Youngwoo Ahn and Kitae Kim

GENERATING CERTAIN QUINTIC IRREDUCIBLE POLYNOMIALS OVER FINITE FIELDS. Youngwoo Ahn and Kitae Kim Korean J. Mah. 19 (2011), No. 3, pp. 263 272 GENERATING CERTAIN QUINTIC IRREDUCIBLE POLYNOMIALS OVER FINITE FIELDS Youngwoo Ahn and Kae Km Absrac. In he paper [1], an explc correspondence beween ceran

More information

On the numerical treatment ofthenonlinear partial differentialequation of fractional order

On the numerical treatment ofthenonlinear partial differentialequation of fractional order IOSR Journal of Mahemacs (IOSR-JM) e-iss: 2278-5728, p-iss: 239-765X. Volume 2, Issue 6 Ver. I (ov. - Dec.26), PP 28-37 www.osrjournals.org On he numercal reamen ofhenonlnear paral dfferenalequaon of fraconal

More information

( ) () we define the interaction representation by the unitary transformation () = ()

( ) () we define the interaction representation by the unitary transformation () = () Hgher Order Perurbaon Theory Mchael Fowler 3/7/6 The neracon Represenaon Recall ha n he frs par of hs course sequence, we dscussed he chrödnger and Hesenberg represenaons of quanum mechancs here n he chrödnger

More information

Research Article Adaptive Synchronization of Complex Dynamical Networks with State Predictor

Research Article Adaptive Synchronization of Complex Dynamical Networks with State Predictor Appled Mahemacs Volume 3, Arcle ID 39437, 8 pages hp://dxdoorg/55/3/39437 Research Arcle Adapve Synchronzaon of Complex Dynamcal eworks wh Sae Predcor Yunao Sh, Bo Lu, and Xao Han Key Laboraory of Beng

More information

[ ] 2. [ ]3 + (Δx i + Δx i 1 ) / 2. Δx i-1 Δx i Δx i+1. TPG4160 Reservoir Simulation 2018 Lecture note 3. page 1 of 5

[ ] 2. [ ]3 + (Δx i + Δx i 1 ) / 2. Δx i-1 Δx i Δx i+1. TPG4160 Reservoir Simulation 2018 Lecture note 3. page 1 of 5 TPG460 Reservor Smulaon 08 page of 5 DISCRETIZATIO OF THE FOW EQUATIOS As we already have seen, fne dfference appromaons of he paral dervaves appearng n he flow equaons may be obaned from Taylor seres

More information

Relative controllability of nonlinear systems with delays in control

Relative controllability of nonlinear systems with delays in control Relave conrollably o nonlnear sysems wh delays n conrol Jerzy Klamka Insue o Conrol Engneerng, Slesan Techncal Unversy, 44- Glwce, Poland. phone/ax : 48 32 37227, {jklamka}@a.polsl.glwce.pl Keywor: Conrollably.

More information

V.Abramov - FURTHER ANALYSIS OF CONFIDENCE INTERVALS FOR LARGE CLIENT/SERVER COMPUTER NETWORKS

V.Abramov - FURTHER ANALYSIS OF CONFIDENCE INTERVALS FOR LARGE CLIENT/SERVER COMPUTER NETWORKS R&RATA # Vol.) 8, March FURTHER AALYSIS OF COFIDECE ITERVALS FOR LARGE CLIET/SERVER COMPUTER ETWORKS Vyacheslav Abramov School of Mahemacal Scences, Monash Unversy, Buldng 8, Level 4, Clayon Campus, Wellngon

More information

Volatility Interpolation

Volatility Interpolation Volaly Inerpolaon Prelmnary Verson March 00 Jesper Andreasen and Bran Huge Danse Mares, Copenhagen wan.daddy@danseban.com brno@danseban.com Elecronc copy avalable a: hp://ssrn.com/absrac=69497 Inro Local

More information

Comparison of Differences between Power Means 1

Comparison of Differences between Power Means 1 In. Journal of Mah. Analyss, Vol. 7, 203, no., 5-55 Comparson of Dfferences beween Power Means Chang-An Tan, Guanghua Sh and Fe Zuo College of Mahemacs and Informaon Scence Henan Normal Unversy, 453007,

More information

A DECOMPOSITION METHOD FOR SOLVING DIFFUSION EQUATIONS VIA LOCAL FRACTIONAL TIME DERIVATIVE

A DECOMPOSITION METHOD FOR SOLVING DIFFUSION EQUATIONS VIA LOCAL FRACTIONAL TIME DERIVATIVE S13 A DECOMPOSITION METHOD FOR SOLVING DIFFUSION EQUATIONS VIA LOCAL FRACTIONAL TIME DERIVATIVE by Hossen JAFARI a,b, Haleh TAJADODI c, and Sarah Jane JOHNSTON a a Deparen of Maheacal Scences, Unversy

More information

Cubic Bezier Homotopy Function for Solving Exponential Equations

Cubic Bezier Homotopy Function for Solving Exponential Equations Penerb Journal of Advanced Research n Compung and Applcaons ISSN (onlne: 46-97 Vol. 4, No.. Pages -8, 6 omoopy Funcon for Solvng Eponenal Equaons S. S. Raml *,,. Mohamad Nor,a, N. S. Saharzan,b and M.

More information

Chapter Lagrangian Interpolation

Chapter Lagrangian Interpolation Chaper 5.4 agrangan Inerpolaon Afer readng hs chaper you should be able o:. dere agrangan mehod of nerpolaon. sole problems usng agrangan mehod of nerpolaon and. use agrangan nerpolans o fnd deraes and

More information

Let s treat the problem of the response of a system to an applied external force. Again,

Let s treat the problem of the response of a system to an applied external force. Again, Page 33 QUANTUM LNEAR RESPONSE FUNCTON Le s rea he problem of he response of a sysem o an appled exernal force. Agan, H() H f () A H + V () Exernal agen acng on nernal varable Hamlonan for equlbrum sysem

More information

Attribute Reduction Algorithm Based on Discernibility Matrix with Algebraic Method GAO Jing1,a, Ma Hui1, Han Zhidong2,b

Attribute Reduction Algorithm Based on Discernibility Matrix with Algebraic Method GAO Jing1,a, Ma Hui1, Han Zhidong2,b Inernaonal Indusral Informacs and Compuer Engneerng Conference (IIICEC 05) Arbue educon Algorhm Based on Dscernbly Marx wh Algebrac Mehod GAO Jng,a, Ma Hu, Han Zhdong,b Informaon School, Capal Unversy

More information

Solution in semi infinite diffusion couples (error function analysis)

Solution in semi infinite diffusion couples (error function analysis) Soluon n sem nfne dffuson couples (error funcon analyss) Le us consder now he sem nfne dffuson couple of wo blocks wh concenraon of and I means ha, n a A- bnary sysem, s bondng beween wo blocks made of

More information

P R = P 0. The system is shown on the next figure:

P R = P 0. The system is shown on the next figure: TPG460 Reservor Smulaon 08 page of INTRODUCTION TO RESERVOIR SIMULATION Analycal and numercal soluons of smple one-dmensonal, one-phase flow equaons As an nroducon o reservor smulaon, we wll revew he smples

More information

John Geweke a and Gianni Amisano b a Departments of Economics and Statistics, University of Iowa, USA b European Central Bank, Frankfurt, Germany

John Geweke a and Gianni Amisano b a Departments of Economics and Statistics, University of Iowa, USA b European Central Bank, Frankfurt, Germany Herarchcal Markov Normal Mxure models wh Applcaons o Fnancal Asse Reurns Appendx: Proofs of Theorems and Condonal Poseror Dsrbuons John Geweke a and Gann Amsano b a Deparmens of Economcs and Sascs, Unversy

More information

Existence of Time Periodic Solutions for the Ginzburg-Landau Equations. model of superconductivity

Existence of Time Periodic Solutions for the Ginzburg-Landau Equations. model of superconductivity Journal of Mahemacal Analyss and Applcaons 3, 3944 999 Arcle ID jmaa.999.683, avalable onlne a hp:www.dealbrary.com on Exsence of me Perodc Soluons for he Gnzburg-Landau Equaons of Superconducvy Bxang

More information

In the complete model, these slopes are ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL. (! i+1 -! i ) + [(!") i+1,q - [(!

In the complete model, these slopes are ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL. (! i+1 -! i ) + [(!) i+1,q - [(! ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL The frs hng o es n wo-way ANOVA: Is here neracon? "No neracon" means: The man effecs model would f. Ths n urn means: In he neracon plo (wh A on he horzonal

More information

FTCS Solution to the Heat Equation

FTCS Solution to the Heat Equation FTCS Soluon o he Hea Equaon ME 448/548 Noes Gerald Reckenwald Porland Sae Unversy Deparmen of Mechancal Engneerng gerry@pdxedu ME 448/548: FTCS Soluon o he Hea Equaon Overvew Use he forward fne d erence

More information

New M-Estimator Objective Function. in Simultaneous Equations Model. (A Comparative Study)

New M-Estimator Objective Function. in Simultaneous Equations Model. (A Comparative Study) Inernaonal Mahemacal Forum, Vol. 8, 3, no., 7 - HIKARI Ld, www.m-hkar.com hp://dx.do.org/.988/mf.3.3488 New M-Esmaor Objecve Funcon n Smulaneous Equaons Model (A Comparave Sudy) Ahmed H. Youssef Professor

More information

A New Generalized Gronwall-Bellman Type Inequality

A New Generalized Gronwall-Bellman Type Inequality 22 Inernaonal Conference on Image, Vson and Comung (ICIVC 22) IPCSIT vol. 5 (22) (22) IACSIT Press, Sngaore DOI:.7763/IPCSIT.22.V5.46 A New Generalzed Gronwall-Bellman Tye Ineualy Qnghua Feng School of

More information

Research Article Numerical Approximation of Higher-Order Solutions of the Quadratic Nonlinear Stochastic Oscillatory Equation Using WHEP Technique

Research Article Numerical Approximation of Higher-Order Solutions of the Quadratic Nonlinear Stochastic Oscillatory Equation Using WHEP Technique Hndaw Publshng Corporaon Journal of Appled Mahemacs Volume 3, Arcle ID 68537, pages hp://dx.do.org/.55/3/68537 Research Arcle Numercal Approxmaon of Hgher-Order Soluons of he Quadrac Nonlnear Sochasc Oscllaory

More information

CS434a/541a: Pattern Recognition Prof. Olga Veksler. Lecture 4

CS434a/541a: Pattern Recognition Prof. Olga Veksler. Lecture 4 CS434a/54a: Paern Recognon Prof. Olga Veksler Lecure 4 Oulne Normal Random Varable Properes Dscrmnan funcons Why Normal Random Varables? Analycally racable Works well when observaon comes form a corruped

More information

Survival Analysis and Reliability. A Note on the Mean Residual Life Function of a Parallel System

Survival Analysis and Reliability. A Note on the Mean Residual Life Function of a Parallel System Communcaons n Sascs Theory and Mehods, 34: 475 484, 2005 Copyrgh Taylor & Francs, Inc. ISSN: 0361-0926 prn/1532-415x onlne DOI: 10.1081/STA-200047430 Survval Analyss and Relably A Noe on he Mean Resdual

More information

Lecture 18: The Laplace Transform (See Sections and 14.7 in Boas)

Lecture 18: The Laplace Transform (See Sections and 14.7 in Boas) Lecure 8: The Lalace Transform (See Secons 88- and 47 n Boas) Recall ha our bg-cure goal s he analyss of he dfferenal equaon, ax bx cx F, where we emloy varous exansons for he drvng funcon F deendng on

More information

Some Numerical Methods For Solving Fractional Parabolic Partial Differential Equations

Some Numerical Methods For Solving Fractional Parabolic Partial Differential Equations Eng.& Tech. Journal,Vol.28, No.2, 2 Some Numercal Mehods For Solvng Fraconal Parabolc Paral Dfferenal Dr. Osama H.Mohammed*, Ibsam K.Hanan* & Akram A. Al-Sabbagh* Receved on: 7//29 Acceped on:/4/2 Absrac

More information

3. OVERVIEW OF NUMERICAL METHODS

3. OVERVIEW OF NUMERICAL METHODS 3 OVERVIEW OF NUMERICAL METHODS 3 Inroducory remarks Ths chaper summarzes hose numercal echnques whose knowledge s ndspensable for he undersandng of he dfferen dscree elemen mehods: he Newon-Raphson-mehod,

More information

Implementation of Quantized State Systems in MATLAB/Simulink

Implementation of Quantized State Systems in MATLAB/Simulink SNE T ECHNICAL N OTE Implemenaon of Quanzed Sae Sysems n MATLAB/Smulnk Parck Grabher, Mahas Rößler 2*, Bernhard Henzl 3 Ins. of Analyss and Scenfc Compung, Venna Unversy of Technology, Wedner Haupsraße

More information

ON THE WEAK LIMITS OF SMOOTH MAPS FOR THE DIRICHLET ENERGY BETWEEN MANIFOLDS

ON THE WEAK LIMITS OF SMOOTH MAPS FOR THE DIRICHLET ENERGY BETWEEN MANIFOLDS ON THE WEA LIMITS OF SMOOTH MAPS FOR THE DIRICHLET ENERGY BETWEEN MANIFOLDS FENGBO HANG Absrac. We denfy all he weak sequenal lms of smooh maps n W (M N). In parcular, hs mples a necessary su cen opologcal

More information

J i-1 i. J i i+1. Numerical integration of the diffusion equation (I) Finite difference method. Spatial Discretization. Internal nodes.

J i-1 i. J i i+1. Numerical integration of the diffusion equation (I) Finite difference method. Spatial Discretization. Internal nodes. umercal negraon of he dffuson equaon (I) Fne dfference mehod. Spaal screaon. Inernal nodes. R L V For hermal conducon le s dscree he spaal doman no small fne spans, =,,: Balance of parcles for an nernal

More information

Ordinary Differential Equations in Neuroscience with Matlab examples. Aim 1- Gain understanding of how to set up and solve ODE s

Ordinary Differential Equations in Neuroscience with Matlab examples. Aim 1- Gain understanding of how to set up and solve ODE s Ordnary Dfferenal Equaons n Neuroscence wh Malab eamples. Am - Gan undersandng of how o se up and solve ODE s Am Undersand how o se up an solve a smple eample of he Hebb rule n D Our goal a end of class

More information

Online Supplement for Dynamic Multi-Technology. Production-Inventory Problem with Emissions Trading

Online Supplement for Dynamic Multi-Technology. Production-Inventory Problem with Emissions Trading Onlne Supplemen for Dynamc Mul-Technology Producon-Invenory Problem wh Emssons Tradng by We Zhang Zhongsheng Hua Yu Xa and Baofeng Huo Proof of Lemma For any ( qr ) Θ s easy o verfy ha he lnear programmng

More information

A new type of the Gronwall-Bellman inequality and its application to fractional stochastic differential equations

A new type of the Gronwall-Bellman inequality and its application to fractional stochastic differential equations Wu, Cogen Mahemacs 7, 4: 7978 hp://dxdoorg/8/3383577978 APPLIED & INTERDISCIPLINARY MATHEMATICS RESEARCH ARTICLE A new ype of he Gronwall-Bellman nequaly and s applcaon o fraconal sochasc dfferenal equaons

More information

Fuzzy Set Theory in Modeling Uncertainty Data. via Interpolation Rational Bezier Surface Function

Fuzzy Set Theory in Modeling Uncertainty Data. via Interpolation Rational Bezier Surface Function Appled Mahemacal Scences, Vol. 7, 013, no. 45, 9 38 HIKARI Ld, www.m-hkar.com Fuzzy Se Theory n Modelng Uncerany Daa va Inerpolaon Raonal Bezer Surface Funcon Rozam Zakara Deparmen of Mahemacs, Faculy

More information

CH.3. COMPATIBILITY EQUATIONS. Continuum Mechanics Course (MMC) - ETSECCPB - UPC

CH.3. COMPATIBILITY EQUATIONS. Continuum Mechanics Course (MMC) - ETSECCPB - UPC CH.3. COMPATIBILITY EQUATIONS Connuum Mechancs Course (MMC) - ETSECCPB - UPC Overvew Compably Condons Compably Equaons of a Poenal Vecor Feld Compably Condons for Infnesmal Srans Inegraon of he Infnesmal

More information

Scattering at an Interface: Oblique Incidence

Scattering at an Interface: Oblique Incidence Course Insrucor Dr. Raymond C. Rumpf Offce: A 337 Phone: (915) 747 6958 E Mal: rcrumpf@uep.edu EE 4347 Appled Elecromagnecs Topc 3g Scaerng a an Inerface: Oblque Incdence Scaerng These Oblque noes may

More information

Track Properities of Normal Chain

Track Properities of Normal Chain In. J. Conemp. Mah. Scences, Vol. 8, 213, no. 4, 163-171 HIKARI Ld, www.m-har.com rac Propes of Normal Chan L Chen School of Mahemacs and Sascs, Zhengzhou Normal Unversy Zhengzhou Cy, Hennan Provnce, 4544,

More information

CS286.2 Lecture 14: Quantum de Finetti Theorems II

CS286.2 Lecture 14: Quantum de Finetti Theorems II CS286.2 Lecure 14: Quanum de Fne Theorems II Scrbe: Mara Okounkova 1 Saemen of he heorem Recall he las saemen of he quanum de Fne heorem from he prevous lecure. Theorem 1 Quanum de Fne). Le ρ Dens C 2

More information

Dual Approximate Dynamic Programming for Large Scale Hydro Valleys

Dual Approximate Dynamic Programming for Large Scale Hydro Valleys Dual Approxmae Dynamc Programmng for Large Scale Hydro Valleys Perre Carpener and Jean-Phlppe Chanceler 1 ENSTA ParsTech and ENPC ParsTech CMM Workshop, January 2016 1 Jon work wh J.-C. Alas, suppored

More information

Li An-Ping. Beijing , P.R.China

Li An-Ping. Beijing , P.R.China A New Type of Cpher: DICING_csb L An-Png Bejng 100085, P.R.Chna apl0001@sna.com Absrac: In hs paper, we wll propose a new ype of cpher named DICING_csb, whch s derved from our prevous sream cpher DICING.

More information

M. Y. Adamu Mathematical Sciences Programme, AbubakarTafawaBalewa University, Bauchi, Nigeria

M. Y. Adamu Mathematical Sciences Programme, AbubakarTafawaBalewa University, Bauchi, Nigeria IOSR Journal of Mahemacs (IOSR-JM e-issn: 78-578, p-issn: 9-765X. Volume 0, Issue 4 Ver. IV (Jul-Aug. 04, PP 40-44 Mulple SolonSoluons for a (+-dmensonalhroa-sasuma shallow waer wave equaon UsngPanlevé-Bӓclund

More information

FI 3103 Quantum Physics

FI 3103 Quantum Physics /9/4 FI 33 Quanum Physcs Aleander A. Iskandar Physcs of Magnesm and Phooncs Research Grou Insu Teknolog Bandung Basc Conces n Quanum Physcs Probably and Eecaon Value Hesenberg Uncerany Prncle Wave Funcon

More information

Linear Response Theory: The connection between QFT and experiments

Linear Response Theory: The connection between QFT and experiments Phys540.nb 39 3 Lnear Response Theory: The connecon beween QFT and expermens 3.1. Basc conceps and deas Q: ow do we measure he conducvy of a meal? A: we frs nroduce a weak elecrc feld E, and hen measure

More information

CONSISTENT EARTHQUAKE ACCELERATION AND DISPLACEMENT RECORDS

CONSISTENT EARTHQUAKE ACCELERATION AND DISPLACEMENT RECORDS APPENDX J CONSSTENT EARTHQUAKE ACCEERATON AND DSPACEMENT RECORDS Earhqake Acceleraons can be Measred. However, Srcres are Sbjeced o Earhqake Dsplacemens J. NTRODUCTON { XE "Acceleraon Records" }A he presen

More information

Part II CONTINUOUS TIME STOCHASTIC PROCESSES

Part II CONTINUOUS TIME STOCHASTIC PROCESSES Par II CONTINUOUS TIME STOCHASTIC PROCESSES 4 Chaper 4 For an advanced analyss of he properes of he Wener process, see: Revus D and Yor M: Connuous marngales and Brownan Moon Karazas I and Shreve S E:

More information

The Finite Element Method for the Analysis of Non-Linear and Dynamic Systems

The Finite Element Method for the Analysis of Non-Linear and Dynamic Systems Swss Federal Insue of Page 1 The Fne Elemen Mehod for he Analyss of Non-Lnear and Dynamc Sysems Prof. Dr. Mchael Havbro Faber Dr. Nebojsa Mojslovc Swss Federal Insue of ETH Zurch, Swzerland Mehod of Fne

More information

Lecture 11 SVM cont

Lecture 11 SVM cont Lecure SVM con. 0 008 Wha we have done so far We have esalshed ha we wan o fnd a lnear decson oundary whose margn s he larges We know how o measure he margn of a lnear decson oundary Tha s: he mnmum geomerc

More information

THE PREDICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS

THE PREDICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS THE PREICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS INTROUCTION The wo dmensonal paral dfferenal equaons of second order can be used for he smulaon of compeve envronmen n busness The arcle presens he

More information

Dynamic Team Decision Theory. EECS 558 Project Shrutivandana Sharma and David Shuman December 10, 2005

Dynamic Team Decision Theory. EECS 558 Project Shrutivandana Sharma and David Shuman December 10, 2005 Dynamc Team Decson Theory EECS 558 Proec Shruvandana Sharma and Davd Shuman December 0, 005 Oulne Inroducon o Team Decson Theory Decomposon of he Dynamc Team Decson Problem Equvalence of Sac and Dynamc

More information

Numerical solution of second-order hyperbolic telegraph equation via new cubic trigonometric B-splines approach

Numerical solution of second-order hyperbolic telegraph equation via new cubic trigonometric B-splines approach Nazr e al., Cogen Mahemacs 17, : 13861 hps://do.org/18/3311835.17.13861 APPLIED & INTERDISCIPLINARY MATHEMATICS RESEARCH ARTICLE Numercal soluon of second-order hyperbolc elegraph equaon va new cubc rgonomerc

More information

SOME NOISELESS CODING THEOREMS OF INACCURACY MEASURE OF ORDER α AND TYPE β

SOME NOISELESS CODING THEOREMS OF INACCURACY MEASURE OF ORDER α AND TYPE β SARAJEVO JOURNAL OF MATHEMATICS Vol.3 (15) (2007), 137 143 SOME NOISELESS CODING THEOREMS OF INACCURACY MEASURE OF ORDER α AND TYPE β M. A. K. BAIG AND RAYEES AHMAD DAR Absrac. In hs paper, we propose

More information

Mohammad H. Al-Towaiq a & Hasan K. Al-Bzoor a a Department of Mathematics and Statistics, Jordan University of

Mohammad H. Al-Towaiq a & Hasan K. Al-Bzoor a a Department of Mathematics and Statistics, Jordan University of Ths arcle was downloaded by: [Jordan Unv. of Scence & Tech] On: 05 Aprl 05, A: 0:4 Publsher: Taylor & Francs Informa Ld Regsered n England and ales Regsered umber: 07954 Regsered offce: Mormer House, 37-4

More information

Notes on the stability of dynamic systems and the use of Eigen Values.

Notes on the stability of dynamic systems and the use of Eigen Values. Noes on he sabl of dnamc ssems and he use of Egen Values. Source: Macro II course noes, Dr. Davd Bessler s Tme Seres course noes, zarads (999) Ineremporal Macroeconomcs chaper 4 & Techncal ppend, and Hamlon

More information

Robustness Experiments with Two Variance Components

Robustness Experiments with Two Variance Components Naonal Insue of Sandards and Technology (NIST) Informaon Technology Laboraory (ITL) Sascal Engneerng Dvson (SED) Robusness Expermens wh Two Varance Componens by Ana Ivelsse Avlés avles@ns.gov Conference

More information

Higher-order numerical scheme for linear quadratic problems with bang bang controls

Higher-order numerical scheme for linear quadratic problems with bang bang controls Compu Opm Appl DOI 1.17/s1589-17-9948-z Hgher-order numercal scheme for lnear quadrac problems wh bang bang conrols T. Scarnc 1 V. M. Velov Receved: 3 June 17 The Auhors 17. Ths arcle s an open access

More information

Comb Filters. Comb Filters

Comb Filters. Comb Filters The smple flers dscussed so far are characered eher by a sngle passband and/or a sngle sopband There are applcaons where flers wh mulple passbands and sopbands are requred Thecomb fler s an example of

More information

Density Matrix Description of NMR BCMB/CHEM 8190

Density Matrix Description of NMR BCMB/CHEM 8190 Densy Marx Descrpon of NMR BCMBCHEM 89 Operaors n Marx Noaon If we say wh one bass se, properes vary only because of changes n he coeffcens weghng each bass se funcon x = h< Ix > - hs s how we calculae

More information

e-journal Reliability: Theory& Applications No 2 (Vol.2) Vyacheslav Abramov

e-journal Reliability: Theory& Applications No 2 (Vol.2) Vyacheslav Abramov June 7 e-ournal Relably: Theory& Applcaons No (Vol. CONFIDENCE INTERVALS ASSOCIATED WITH PERFORMANCE ANALYSIS OF SYMMETRIC LARGE CLOSED CLIENT/SERVER COMPUTER NETWORKS Absrac Vyacheslav Abramov School

More information

5th International Conference on Advanced Design and Manufacturing Engineering (ICADME 2015)

5th International Conference on Advanced Design and Manufacturing Engineering (ICADME 2015) 5h Inernaonal onference on Advanced Desgn and Manufacurng Engneerng (IADME 5 The Falure Rae Expermenal Sudy of Specal N Machne Tool hunshan He, a, *, La Pan,b and Bng Hu 3,c,,3 ollege of Mechancal and

More information

Delay-Range-Dependent Stability Analysis for Continuous Linear System with Interval Delay

Delay-Range-Dependent Stability Analysis for Continuous Linear System with Interval Delay Inernaonal Journal of Emergng Engneerng esearch an echnology Volume 3, Issue 8, Augus 05, PP 70-76 ISSN 349-4395 (Prn) & ISSN 349-4409 (Onlne) Delay-ange-Depenen Sably Analyss for Connuous Lnear Sysem

More information

Performance Analysis for a Network having Standby Redundant Unit with Waiting in Repair

Performance Analysis for a Network having Standby Redundant Unit with Waiting in Repair TECHNI Inernaonal Journal of Compung Scence Communcaon Technologes VOL.5 NO. July 22 (ISSN 974-3375 erformance nalyss for a Nework havng Sby edundan Un wh ang n epar Jendra Sngh 2 abns orwal 2 Deparmen

More information

On elements with index of the form 2 a 3 b in a parametric family of biquadratic elds

On elements with index of the form 2 a 3 b in a parametric family of biquadratic elds On elemens wh ndex of he form a 3 b n a paramerc famly of bquadrac elds Bora JadrevĆ Absrac In hs paper we gve some resuls abou prmve negral elemens p(c p n he famly of bcyclc bquadrac elds L c = Q ) c;

More information

( t) Outline of program: BGC1: Survival and event history analysis Oslo, March-May Recapitulation. The additive regression model

( t) Outline of program: BGC1: Survival and event history analysis Oslo, March-May Recapitulation. The additive regression model BGC1: Survval and even hsory analyss Oslo, March-May 212 Monday May 7h and Tuesday May 8h The addve regresson model Ørnulf Borgan Deparmen of Mahemacs Unversy of Oslo Oulne of program: Recapulaon Counng

More information

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 5 Lecure 0 Canoncal Transformaons (Chaper 9) Wha We Dd Las Tme Hamlon s Prncple n he Hamlonan formalsm Dervaon was smple δi δ Addonal end-pon consrans pq H( q, p, ) d 0 δ q ( ) δq ( ) δ

More information

Density Matrix Description of NMR BCMB/CHEM 8190

Density Matrix Description of NMR BCMB/CHEM 8190 Densy Marx Descrpon of NMR BCMBCHEM 89 Operaors n Marx Noaon Alernae approach o second order specra: ask abou x magnezaon nsead of energes and ranson probables. If we say wh one bass se, properes vary

More information

Normal Random Variable and its discriminant functions

Normal Random Variable and its discriminant functions Noral Rando Varable and s dscrnan funcons Oulne Noral Rando Varable Properes Dscrnan funcons Why Noral Rando Varables? Analycally racable Works well when observaon coes for a corruped snle prooype 3 The

More information

Variants of Pegasos. December 11, 2009

Variants of Pegasos. December 11, 2009 Inroducon Varans of Pegasos SooWoong Ryu bshboy@sanford.edu December, 009 Youngsoo Cho yc344@sanford.edu Developng a new SVM algorhm s ongong research opc. Among many exng SVM algorhms, we wll focus on

More information

Decentralised Sliding Mode Load Frequency Control for an Interconnected Power System with Uncertainties and Nonlinearities

Decentralised Sliding Mode Load Frequency Control for an Interconnected Power System with Uncertainties and Nonlinearities Inernaonal Research Journal of Engneerng and echnology IRJE e-iss: 2395-0056 Volume: 03 Issue: 12 Dec -2016 www.re.ne p-iss: 2395-0072 Decenralsed Sldng Mode Load Frequency Conrol for an Inerconneced Power

More information

Observer Design for Nonlinear Systems using Linear Approximations

Observer Design for Nonlinear Systems using Linear Approximations Observer Desgn for Nonlnear Ssems sng Lnear Appromaons C. Navarro Hernandez, S.P. Banks and M. Aldeen Deparmen of Aomac Conrol and Ssems Engneerng, Unvers of Sheffeld, Mappn Sree, Sheffeld S 3JD. e-mal:

More information

Tight results for Next Fit and Worst Fit with resource augmentation

Tight results for Next Fit and Worst Fit with resource augmentation Tgh resuls for Nex F and Wors F wh resource augmenaon Joan Boyar Leah Epsen Asaf Levn Asrac I s well known ha he wo smple algorhms for he classc n packng prolem, NF and WF oh have an approxmaon rao of

More information

Handout # 6 (MEEN 617) Numerical Integration to Find Time Response of SDOF mechanical system Y X (2) and write EOM (1) as two first-order Eqs.

Handout # 6 (MEEN 617) Numerical Integration to Find Time Response of SDOF mechanical system Y X (2) and write EOM (1) as two first-order Eqs. Handou # 6 (MEEN 67) Numercal Inegraon o Fnd Tme Response of SDOF mechancal sysem Sae Space Mehod The EOM for a lnear sysem s M X DX K X F() () X X X X V wh nal condons, a 0 0 ; 0 Defne he followng varables,

More information

COMPUTER SCIENCE 349A SAMPLE EXAM QUESTIONS WITH SOLUTIONS PARTS 1, 2

COMPUTER SCIENCE 349A SAMPLE EXAM QUESTIONS WITH SOLUTIONS PARTS 1, 2 COMPUTE SCIENCE 49A SAMPLE EXAM QUESTIONS WITH SOLUTIONS PATS, PAT.. a Dene he erm ll-ondoned problem. b Gve an eample o a polynomal ha has ll-ondoned zeros.. Consder evaluaon o anh, where e e anh. e e

More information

A NUMERICAL SCHEME FOR BSDES. BY JIANFENG ZHANG University of Southern California, Los Angeles

A NUMERICAL SCHEME FOR BSDES. BY JIANFENG ZHANG University of Southern California, Los Angeles The Annals of Appled Probably 24, Vol. 14, No. 1, 459 488 Insue of Mahemacal Sascs, 24 A NUMERICAL SCHEME FOR BSDES BY JIANFENG ZHANG Unversy of Souhern Calforna, Los Angeles In hs paper we propose a numercal

More information

2 Aggregate demand in partial equilibrium static framework

2 Aggregate demand in partial equilibrium static framework Unversy of Mnnesoa 8107 Macroeconomc Theory, Sprng 2009, Mn 1 Fabrzo Perr Lecure 1. Aggregaon 1 Inroducon Probably so far n he macro sequence you have deal drecly wh represenave consumers and represenave

More information

APPROXIMATE ANALYTIC SOLUTIONS OF A NONLINEAR ELASTIC WAVE EQUATIONS WITH THE ANHARMONIC CORRECTION

APPROXIMATE ANALYTIC SOLUTIONS OF A NONLINEAR ELASTIC WAVE EQUATIONS WITH THE ANHARMONIC CORRECTION THE PUBLISHING HOUSE PROCEEDINGS OF THE ROMANIAN ACADEMY Seres A OF THE ROMANIAN ACADEMY Volume 6 Number /5 pp 8 86 APPROXIMATE ANALYTIC SOLUTIONS OF A NONLINEAR ELASTIC WAVE EQUATIONS WITH THE ANHARMONIC

More information

Robust and Accurate Cancer Classification with Gene Expression Profiling

Robust and Accurate Cancer Classification with Gene Expression Profiling Robus and Accurae Cancer Classfcaon wh Gene Expresson Proflng (Compuaonal ysems Bology, 2005) Auhor: Hafeng L, Keshu Zhang, ao Jang Oulne Background LDA (lnear dscrmnan analyss) and small sample sze problem

More information

Theoretical Analysis of Biogeography Based Optimization Aijun ZHU1,2,3 a, Cong HU1,3, Chuanpei XU1,3, Zhi Li1,3

Theoretical Analysis of Biogeography Based Optimization Aijun ZHU1,2,3 a, Cong HU1,3, Chuanpei XU1,3, Zhi Li1,3 6h Inernaonal Conference on Machnery, Maerals, Envronmen, Boechnology and Compuer (MMEBC 6) Theorecal Analyss of Bogeography Based Opmzaon Aun ZU,,3 a, Cong U,3, Chuanpe XU,3, Zh L,3 School of Elecronc

More information

A-posteriori estimates for backward SDEs

A-posteriori estimates for backward SDEs A-poseror esmaes for backward SDEs Chrsan Bender 1, Jessca Sener 1 Aprl 4, 01 Suppose an approxmaon o he soluon of a backward SDE s pre-compued by some numercal algorhm. In hs paper we provde a-poseror

More information

@FMI c Kyung Moon Sa Co.

@FMI c Kyung Moon Sa Co. Annals of Fuzzy Mahemacs and Informacs Volume 8, No. 2, (Augus 2014), pp. 245 257 ISSN: 2093 9310 (prn verson) ISSN: 2287 6235 (elecronc verson) hp://www.afm.or.kr @FMI c Kyung Moon Sa Co. hp://www.kyungmoon.com

More information

NATIONAL UNIVERSITY OF SINGAPORE PC5202 ADVANCED STATISTICAL MECHANICS. (Semester II: AY ) Time Allowed: 2 Hours

NATIONAL UNIVERSITY OF SINGAPORE PC5202 ADVANCED STATISTICAL MECHANICS. (Semester II: AY ) Time Allowed: 2 Hours NATONAL UNVERSTY OF SNGAPORE PC5 ADVANCED STATSTCAL MECHANCS (Semeser : AY 1-13) Tme Allowed: Hours NSTRUCTONS TO CANDDATES 1. Ths examnaon paper conans 5 quesons and comprses 4 prned pages.. Answer all

More information

UNIVERSITAT AUTÒNOMA DE BARCELONA MARCH 2017 EXAMINATION

UNIVERSITAT AUTÒNOMA DE BARCELONA MARCH 2017 EXAMINATION INTERNATIONAL TRADE T. J. KEHOE UNIVERSITAT AUTÒNOMA DE BARCELONA MARCH 27 EXAMINATION Please answer wo of he hree quesons. You can consul class noes, workng papers, and arcles whle you are workng on he

More information

First-order piecewise-linear dynamic circuits

First-order piecewise-linear dynamic circuits Frs-order pecewse-lnear dynamc crcus. Fndng he soluon We wll sudy rs-order dynamc crcus composed o a nonlnear resse one-por, ermnaed eher by a lnear capacor or a lnear nducor (see Fg.. Nonlnear resse one-por

More information

Response of MDOF systems

Response of MDOF systems Response of MDOF syses Degree of freedo DOF: he nu nuber of ndependen coordnaes requred o deerne copleely he posons of all pars of a syse a any nsan of e. wo DOF syses hree DOF syses he noral ode analyss

More information

Sampling Procedure of the Sum of two Binary Markov Process Realizations

Sampling Procedure of the Sum of two Binary Markov Process Realizations Samplng Procedure of he Sum of wo Bnary Markov Process Realzaons YURY GORITSKIY Dep. of Mahemacal Modelng of Moscow Power Insue (Techncal Unversy), Moscow, RUSSIA, E-mal: gorsky@yandex.ru VLADIMIR KAZAKOV

More information

Stability Analysis of Fuzzy Hopfield Neural Networks with Timevarying

Stability Analysis of Fuzzy Hopfield Neural Networks with Timevarying ISSN 746-7659 England UK Journal of Informaon and Compung Scence Vol. No. 8 pp.- Sably Analyss of Fuzzy Hopfeld Neural Neworks w mevaryng Delays Qfeng Xun Cagen Zou Scool of Informaon Engneerng Yanceng

More information

A NOVEL NETWORK METHOD DESIGNING MULTIRATE FILTER BANKS AND WAVELETS

A NOVEL NETWORK METHOD DESIGNING MULTIRATE FILTER BANKS AND WAVELETS A NOVEL NEWORK MEHOD DESIGNING MULIRAE FILER BANKS AND WAVELES Yng an Deparmen of Elecronc Engneerng and Informaon Scence Unversy of Scence and echnology of Chna Hefe 37, P. R. Chna E-mal: yan@usc.edu.cn

More information

Generalized double sinh-gordon equation: Symmetry reductions, exact solutions and conservation laws

Generalized double sinh-gordon equation: Symmetry reductions, exact solutions and conservation laws IJS (05) 9A: 89-96 Iranan Journal of Scence & echnology hp://ss.shrazu.ac.r Generalzed double snh-gordon equaon: Symmery reducons eac soluons and conservaon laws G. Magalawe B. Muaeea and C. M. Khalque

More information

Review of Numerical Schemes for Two Point Second Order Non-Linear Boundary Value Problems

Review of Numerical Schemes for Two Point Second Order Non-Linear Boundary Value Problems Proceedngs of e Pasan Academ of Scences 5 (: 5-58 (5 Coprg Pasan Academ of Scences ISS: 377-969 (prn, 36-448 (onlne Pasan Academ of Scences Researc Arcle Revew of umercal Scemes for Two Pon Second Order

More information

PHYS 705: Classical Mechanics. Canonical Transformation

PHYS 705: Classical Mechanics. Canonical Transformation PHYS 705: Classcal Mechancs Canoncal Transformaon Canoncal Varables and Hamlonan Formalsm As we have seen, n he Hamlonan Formulaon of Mechancs,, are ndeenden varables n hase sace on eual foong The Hamlon

More information

Including the ordinary differential of distance with time as velocity makes a system of ordinary differential equations.

Including the ordinary differential of distance with time as velocity makes a system of ordinary differential equations. Soluons o Ordnary Derenal Equaons An ordnary derenal equaon has only one ndependen varable. A sysem o ordnary derenal equaons consss o several derenal equaons each wh he same ndependen varable. An eample

More information

T q (heat generation) Figure 0-1: Slab heated with constant source 2 = q k

T q (heat generation) Figure 0-1: Slab heated with constant source 2 = q k IFFERETIL EQUTIOS, PROBLE BOURY VLUE 5. ITROUCTIO s as been noed n e prevous caper, boundary value problems BVP for ordnary dfferenal equaons ave boundary condons specfed a more an one pon of e ndependen

More information

FRACTIONAL OPTICAL SOLITARY WAVE SOLUTIONS OF THE HIGHER-ORDER NONLINEAR SCHRÖDINGER EQUATION

FRACTIONAL OPTICAL SOLITARY WAVE SOLUTIONS OF THE HIGHER-ORDER NONLINEAR SCHRÖDINGER EQUATION THE PUBLISHING HOUSE PROCEEDINGS OF THE ROMANIAN ACADEMY Seres A OF THE ROMANIAN ACADEMY Volume Number /00x pp. 9 00 FRACTIONAL OPTICAL SOLITARY WAVE SOLUTIONS OF THE HIGHER-ORDER NONLINEAR SCHRÖDINGER

More information