Certain remarks to integral equations generated by the numerical-analytical method for solution of the boundary problems

In the paper the comparison method and the chosing of the appropriate norm of the comparison operator is used to establish the solvability of the integral-functional equation resulted by the application of the numeric-analytic method of solving of boundary value problems for ordinary differential-de...

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Дата:1992
Автор: Kwapisz, M.
Формат: Стаття
Мова:Англійська
Опубліковано: Institute of Mathematics, NAS of Ukraine 1992
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Назва журналу:Ukrains’kyi Matematychnyi Zhurnal
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Ukrains’kyi Matematychnyi Zhurnal
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author Kwapisz, M.
Kwapisz, M.
author_facet Kwapisz, M.
Kwapisz, M.
author_sort Kwapisz, M.
baseUrl_str https://umj.imath.kiev.ua/index.php/umj/oai
collection OJS
datestamp_date 2023-09-14T12:03:56Z
description In the paper the comparison method and the chosing of the appropriate norm of the comparison operator is used to establish the solvability of the integral-functional equation resulted by the application of the numeric-analytic method of solving of boundary value problems for ordinary differential-delay equations of the neutral type.
first_indexed 2026-03-24T03:33:59Z
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fulltext I{O POTKI IIOBI)];OMJIEHHH U DC 519.624. I M. Kwapisz, prof. (Th e Gdanst Univ., P o l and) Some remarks on an integral equation arising in applications of numerical­ a na lytic method of solving of boundary value problems fJ CKOTOpbie 33.l\IC'l3IUUI K HHTerpaJIJ>Hbl.l\f ypaBHCHHHM, 11o pomll,eHHhl.l\f 'IHCJICHHO-aHaJIHTH'I.eCIHil.\1 l\ICTOfl,0.1.U pcmeHJUI rpaHH'IHblX 33fl,3'1 In t he paper the comparison methob anb the chosing of the appropriate norm of the compari• son oper ator is used to est ablish the solvability of the integral-functional equation resulted by the appl icati on of the numeric-ana lytic method of solving of boundary value problems fm Ot• <lin an· differential-delay equations of the neutra l type. C nOMOlllblO MeTO,!la cpaB1IeHHll H Ha.nJie:>Kamero noJ(6opa HOpMbl onepaTopa cpaBHeHHSI ycTaHaB­ JH!BaeTCH pa3peUIHMOCTb IIHTerpo-cjlyHKUHOHaJibHOfO ypaBHeHHH, nopo:>K.nettnoro q11CJ1eHHO-aHa­ JIHTH'-!eCKIIM MeTO.llOM pernemrn rpam-1qHblX 3a,naq JlJlll O6blKHOBeHHb!X JlH<jxpepeHUHaJibH61.X ypaB· IJeHHtt HeiiTpaJll,HOro THna. 3a JlOIIOMOfOIO MeTOJ(Y uopi BHHHHH i HaJie:>KHOfO .no6opy HOJ)MH onepaTOpa nopiBHHHHH BC'PaHOB­ J\IO€TbCH pO3B0 ll3HiCTb iHTerpo-cjlyHKUiOHaJibHOfO piBHHHHH, nopon:>Kettor o '-ll-lCeJibHO-aHaJiiTHq­ HH~I MeTOJlOM JlO3B0 H3yBaHHH rpam1q1111x 3anaq JlJIH 3B11qafitt11X nmpepettuiaJibHIIX piBHHHb tteH• TpaJibHOro THny. The app lica tion of the numerical-analytic method (see and N. I. Ron to I 1, 2]) to the solution of the problem: x' (t) = f (t, x (a (t)), x' ((:) (t))), t E J = [0, T], by the su bstitution Ax (0) + Bx (1) = d I x (t) = x 0 + ) z (s) ds 0 leaas us (see 131) to the following system of equations A. M. Samoilenko T>O, (I) (2) (3) T a (t) a. <n z tt) = f (t, x, + a (t) cp (x 0) + - 7 ) z (s) ds - with - a-,;.t) S z (s) ds, z (13 (t))), et( I) I T cp (x0) - T ) z (s) ds = 0 0 0 cp (x0 ) = T- 1 B-1 (d - (A + B) x 0). (4) (5) It is assumed that fE C(J x R" x R", R"), a , f3E C(J, J), dER". A and B are n x n matrices. It is quite clear that the solution x* of (1), (2) is found when a solution (x~, z*) of the system (4), (5) is gi ven . The formu la (3) serves for the relation between the solutions. In the method we are dea ling with the sy tern 14), (5) is solved successively . As the fir st the equation (4) is solved with respect to z at the same time x11 is considered as a parameter. As a result of this we fin d a function z* ( .• x0 ) which together with eq uation (5) is used to find x0• • Finally the solution of (1), (2) is given by the equation x* (t) =-= = z* (t, x~). C M. KWAPISZ, 1992 128 1SSN 0041-6053. Ytcp. MaT. tJ1Cyp11., 1992, T. 44, M 1 The a im of the presen t paper is to di scuss the conditions under which the solution z* ( •, x0) of equa tion (4) can be obtained by the method of success ive approx imations Z1,-1- 1 (t, x 0) = (Fz,, ) (t , x 0) , k = 0, l, ... (6) with z0 choosen arb itr a ril!y . Here the operator F is defin ed by the ri ght han J s ide of equation (4). The convergence of t he seq uence {z1.} will be obt ained by the com para tive method (see e. g. [4-6]). We introduce the fo llowing assumptions Ass u m p t i on H1 . There are n x n matrices K and L with positive entries such that If (t, X , y) - f (t, X, !/) I :s;;; KI X - XI+ LI y - y I (7) for all t E J, x , y, x, y E Rn. Here I • I denotes the absolute value of the vec­ T tor, so Jx l =(lx1 l,-- -,l xn l) - Ass um p ti on H 2 . For any positiv e function h EC (J x R", R+) there exists the unique solution u0 EC (J X R", R.'.j.. ) of the comparison equation u (t, x0) = (Qu) (t, x0) + h (t, x0), (8) wi th the operator Q defined by the equation T - a (t) a(t) a (t) T (Qu) (t , x0 ) = T S Ku (s, x0 ) ds + ---;y- S Ku (s, x0 ) ds+ Lu (~ (t), x0). o a(t) ow for a fixed initial approximation 20 we define h (t, X 0) = I (Fz0) (t, X 0) - z0 (t, X0 ) I (9) and we construct the sequence {uh} by the formula Uk+l (t, X0) = {Qu") (t, X0) , k = l, 2, ... , t E J, X 0 E Rn, (10) for u0 defined by equat ion (8) with h given by equation (9). From Assumption H 2 it fo llows easily {see for the compara tive theory) tha t the sequence {uh} is nonincreas ing and converges a lmost uniformly {uniformly on any compact subset of J x Rn) to the zero fu ncti on. Moreover by the mathematical induct ion rule we get eas ily the following esti mations lz1<(t,x.)-z0 (t, x~)l :s;;; u0 (t,x0 ), k= O, 1,.... (11) I Zk+P (t, x0)- zk (t, X 0 ) :s;;; u ,, (t, X 0), k, P = 0, l, .... (12) From these estimations it follows the followin g Theorem. //' the assumptions H1 and H2 ·are satisfied then for every x0 E R_n there exists a unique solution z* ( ·, x0) of equation (4), moreover z* (t, Xe) = lim zh (t , x0), k-+ + oo, (13) (14) It follows from the given genera l discussion that now the crutial point is to find practica l sufficient condi tions wh ich quarantee that the Assumption H 2 holds true. There is an immedia te answer to our problem. It is enough to assume that some norm of the operator ~2 is less th an one . However there are many different norms of the same operator Q (they depend on the norm taken in the space of continuous functions where the opera tor is defined). ret us consider some specia l cases . I. If we take in the space C (J, R11 ) the standard supremum norm (the Tchebysheff norm) then we see tha t the Assumption H 2 holds if the condition holds. m\\kll+IIL!l<l, m = 21-1 max[{T-a(t))a(t):tEJJ (15) ISSN 0041-6053. YKp. Mar. "'YPH.., 1992, T. 44, M I 9-1-812 129 2. If we take in C (J, Rn) the following weighted norm II u l[1, = max [I u (t) [1, : t E J], I u (t) lb= max [b1 1 I ui (t) I: i = 1, 2, . .. , nl with b the positive eigenvector of the matrix mk + L corresponding to the eigenva lue which is equal to the spectral radius of that matrix (the existen­ ce of such eigenvector is quaranteed by the well known Perron theorem) then the Assumpt ion H 2 holds true when the spectral radius of mk + L is less than one (see 13]), i. e. p = p (mK + L) < I. In fact in this case we have I u (t) I~ Ii u l[ 1, • b, I (Qu) (t) I ~ II u li t (mK + L) b = p Ii u II,,· b what means that II Q lib~ p < I. (16) 3 . In the case a (t) = t, B (t) = t the condition (16) can be replaced by the following one (17) To get the result we need to employ the fo llowing norm II u !l ,,,c = max [(t (T - t) + c)- 1 I u (t) lb: t E JJ for the corresponding eigenvector b and suffic iently small positive number c. From this definit ion we have I u (i) I~ II u llb,c • (t (T- t) + c) b and consequently l T I (Qu) (t) I~ II u 11 ,, .c [r- 1 (T- t) 5 (s (T- s) + c) Kbds + r-'t 5 (s (T - s) + 0 + c) Kbds + (t (T - t) + c) Lb l ~ II u llb,c rr-'t (T - t ) (b- 1 (T2 + 4Tt - 4f2)+ + 2c) Kb+ (t (T - t) + c) LbJ. This implies the followin g inequality (t (T - t) + c)- 1 I (Qu) (t) I~ II u llb,c ((3- 'T + 2cT-1) Kb + Lb]= = II U ll h,c (p'b + 2cT-1/(b) ~ II U llb,c (p' + 2cT- 1 IJ Kb lib) b_ because Kb ~ II Kb ll bb. From the last inequali ty we find II Qu llb,c ~ (p ' + 2cT-' I! I< b IJ,,) JI U llb,c which means that II Q II"·' < I if p' < I and c is sufficiently small. 4. Observe that in the case a (t) = t, f:, (t) = t one can reason in a dif­ ferent way . lnder the condition p \l)< 1 the eq uation can be rewr itten in the equ ivalent iorm t T u (t) = r-' ( (T- t) S 1( 1u (s) ds + t I K1u (s) ds) + hi(t), (18) 0 t where Ki=(/ - L)-1K , h1 (t) = (/ - L)- 11i (t , Xg) - Now the Assumption H; is satisfied if the fo llowing conditions hold p (L) < I, p (3- 1T (/- L)- 1/() < 1. In this case it is worthy to observe that the substitution u (t) - hi(t) = v (t) in the equation (1 8) reduces this eq uation to the form which can be considered in the subsp ace of function of C (J, R") having the property max [(t (T- t))-1 1 v (t) I: t E J] < + =· 130 ISSN 0041-6053. Y1'p. Mar. ~ ypH., 1992, r. 44, M l Now the norm II u ll1;,c can be replaced by that which correspon ds to c = 0. 5 . Fina lly we will seek the solution of equation (18) by the Neumann series. For the conveni ence we will write K 1 and h1 as s imply K and h. Let l [ (Gu) (t) = r- 1 [iT - t) .\' K.u (s) ds + t S K.u (s) ds] , ( 19) 0 t += U0 (t) = ) (Gih) (t). "-' i = O (20) It is clear that the series (20) converges uniformly when the norm of the opera tor G is less than one . So one can use the results of our di scuss ion. Now we will presen t the aproach ba sed on some po intwise estimations. This will be close to the considera t ions given in the books l l, 2J. Let the sequence {a ;} be defi­ ned as follows ' T a 1+1 (t) = r-1 ( (T - t) .\' a; (s) ds + t Sa; (s) ds), a 0 (t) = l, i = 0, I, .. . 0 I (2 1) Take H E R", H>0 such that jh(t)l ~ H for tEJ. Now by the mathema­ tical induction rule we infer (22) By the dirrect calculations (see fl l) one can find that a 1 (f) ~ 2- 1Ta0 (f) , CG 2 (t) ~ 3-1Ta1 (t), a 3 (i) ~ 10-1T2a 1 (f), _a2; (t) ~ ( Jio r-~a2 (t), a 2;+!(t) ~ ( Jio r ai(t), i = l, 2, .... From th ese inequalities we get the estirnation i = l, 2, ... , - VTii ai(t) = - 3- a 1 (t) . (23) From (22) a nd (23) we have o ~ (G' (hJ (t) ~ ( .Ji0 xy-1a1 (t) KH, t E J, i = 1, 2, ..... Now we see that the series (20) converges uniformly when . T p ( V10 I< )< l. (24) Clearly the function u0 defined by (20) is a solution of ( 18) and u, (t) ~ h (t) + a,l (t) (' _ :ll) 1, rl KH . We observe a lso that in the case considered the corresponding functions u,. (see fo rmula ( 10'\ ) satisfy the re lation u,._(f) = r(G;h)(t)~a(t)(VT )''- 1 (1 - ·vT 1<·)- 1KI-J . (25) <'=k JU I d ' Now the estimation (14) takes the fo r,m for fl = I, 2, •.•. ISSN 0041-6058. Y,cp. MaT. (JfCypH., 1992, T. 44. NJ I 131 We observe that in the book [2, p. 13, 59] in t he correspondi ng es timations the the number 10 does not appear, it is replaced by the number n. In t he mer it there are no special reasons for the presence of this specific number. The onl y justificat ion is t ha t these two numbers are very close. Indeed , we haYe n = 3,141 59265 ... < -V IO = 3,1 6227766 .. .. As it was ment ioned at the beginning of the paper we are not in tend to di s­ cuss ia rther dete ils which are concerned with the solv ing the corresponding eq uation wh ich determines x~ . The readers are advised to consult t he publi­ cations l 1, 2, 7] for the necessary details. I. Samoilenko A . M., Ronto N. I. Numerica l-analytic methobs of investigating of peri odi c so lut ions (Russian).- Kiev: Vyssha Sk., 1976 .- 180 p. 2. Samoiienlw A. M., Ranlo N. 1. N um er ica I- ana lytic methods of invest igati ng bound ary value problems (Russian). - Kiev: Na uk. Dumka, 1986 .- 224 p. 3. Augustynowicz A . , Ku..•cpi,z M . On a nu merical -analitic methob of solv ing of boundary va · Jue prob lem for functional hifirenli al equat ion of neutral type// Math. Nachr.- 1990.- 145 .- P. 255- 269. 4. Kwapisz NI. A comparison theorem on the existence anb uniqueness of the solut ion ot an inlegra l-f unctiona I equati on / / Y 11 In t. Konf. uder N ichtlineare Schwingun!!en, Abhand ­ lum'.en i der Adw.- Ber li n: Aka b.-Verl., 1977.- P. 481-487. 5. Kwap isz M. On the comparison m_e lhob in the ex istence anb uniqueness t heory fo r eq ua tions in spaces of funct ions (Russian) / / Differentia I equations with deviated ar('.ument.- Kiev : Na uk. Dumka, 1977.- P. 148- 158. 6. Kwa pisz M . Some remarks on abstract form of iterative methods in functional equati on the­ ory // Comment. Math.- 1984. - 24.- P . 281-294. 7, Samoilenko A. M ., Ranlo N. I. A modifi cati on of numerical-analytic method of successive approx imations for boun dary va lue prob lems for ordinary dif ferenti al equa ti ons (Russian)/; Ukr. Math. J .- 1990,- 42 , N 8.- P, 1107-I I l6, Received 30.01.91 0120 0121 0122 0123 0124
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spelling umjimathkievua-article-78032023-09-14T12:03:56Z Certain remarks to integral equations generated by the numerical-analytical method for solution of the boundary problems Некоторые замечания к интегральным уравнениям , порожденным численно-аналитическим методом решения граничных задач Kwapisz, M. Kwapisz, M. - In the paper the comparison method and the chosing of the appropriate norm of the comparison operator is used to establish the solvability of the integral-functional equation resulted by the application of the numeric-analytic method of solving of boundary value problems for ordinary differential-delay equations of the neutral type. С помощью метода сравнения и надлежащего подбора нормы оператора сравнения устанавливается разрешимость интегро-функционального уравнения, порожденного численно-аналитическим методом решения граничных задач для обыкновенных дифференциальных уравнений нейтрального типа. За допомогою методу порівняння і належного добору норми оператора порівняння встановлюється розв’язність інтегро-функціонального рівняння, породженого чисельно-аналітичним методом розв’язування граничних задач для звичайних диференціальних рівнянь нейтрального типу. Institute of Mathematics, NAS of Ukraine 1992-02-04 Article Article application/pdf https://umj.imath.kiev.ua/index.php/umj/article/view/7803 Ukrains’kyi Matematychnyi Zhurnal; Vol. 44 No. 1 (1992); 128-132 Український математичний журнал; Том 44 № 1 (1992); 128-132 1027-3190 en https://umj.imath.kiev.ua/index.php/umj/article/view/7803/9471 Copyright (c) 1992 M. Kwapisz
spellingShingle Kwapisz, M.
Kwapisz, M.
Certain remarks to integral equations generated by the numerical-analytical method for solution of the boundary problems
title Certain remarks to integral equations generated by the numerical-analytical method for solution of the boundary problems
title_alt Некоторые замечания к интегральным уравнениям , порожденным численно-аналитическим методом решения граничных задач
title_full Certain remarks to integral equations generated by the numerical-analytical method for solution of the boundary problems
title_fullStr Certain remarks to integral equations generated by the numerical-analytical method for solution of the boundary problems
title_full_unstemmed Certain remarks to integral equations generated by the numerical-analytical method for solution of the boundary problems
title_short Certain remarks to integral equations generated by the numerical-analytical method for solution of the boundary problems
title_sort certain remarks to integral equations generated by the numerical-analytical method for solution of the boundary problems
topic_facet -
url https://umj.imath.kiev.ua/index.php/umj/article/view/7803
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