Finite-Time Stabilization in Problems with Free Boundary for Nonlinear Equations in Media with Fractal Geometry

By using the method of a priori estimates, we establish differential inequalities for energetic norms in $W^l_{2,r}$ of solutions of problems with a free bound in media with the fractal geometry for one-dimensional evolutionary equation. On the basis of these inequalities, we obtain estimates for...

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Date:2005
Main Authors: Berezovsky, A. A., Mitropolskiy, Yu. A., Shkhanukov-Lafishev, M. Kh., Березовский, А. А., Митропольский, Ю. А., Шхануков-Лафишев, М. Х.
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Published: Institute of Mathematics, NAS of Ukraine 2005
Online Access:https://umj.imath.kiev.ua/index.php/umj/article/view/3658
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Ukrains’kyi Matematychnyi Zhurnal
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author Berezovsky, A. A.
Mitropolskiy, Yu. A.
Shkhanukov-Lafishev, M. Kh.
Березовский, А. А.
Митропольский, Ю. А.
Шхануков-Лафишев, М. Х.
Березовский, А. А.
Митропольский, Ю. А.
Шхануков-Лафишев, М. Х.
author_facet Berezovsky, A. A.
Mitropolskiy, Yu. A.
Shkhanukov-Lafishev, M. Kh.
Березовский, А. А.
Митропольский, Ю. А.
Шхануков-Лафишев, М. Х.
Березовский, А. А.
Митропольский, Ю. А.
Шхануков-Лафишев, М. Х.
author_sort Berezovsky, A. A.
baseUrl_str https://umj.imath.kiev.ua/index.php/umj/oai
collection OJS
datestamp_date 2020-03-18T20:01:15Z
description By using the method of a priori estimates, we establish differential inequalities for energetic norms in $W^l_{2,r}$ of solutions of problems with a free bound in media with the fractal geometry for one-dimensional evolutionary equation. On the basis of these inequalities, we obtain estimates for the stabilization time $T$.
first_indexed 2026-03-24T02:46:36Z
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fulltext K�O�R�O�T�K�I���P�O�V�I�D�O�M�L�E�N�N�Q UDK 517.946.9 G. A. Mytropol\skyj, (Yn-t matematyky NAN Ukrayn¥, Kyev), M. X. Íxanukov-Lafyßev (Kabardyno-Balkar. un-t, Yn-t ynformatyky y problem rehyon. upravlenyq KBNC RAN, Nal\çyk, Rossyq) STABYLYZACYQ ZA KONEÇNOE VREMQ V ZADAÇAX SO SVOBODNOJ HRANYCEJ DLQ NELYNEJNÁX URAVNENYJ V SREDAX S FRAKTAL|NOJ HEOMETRYEJ By using the method of a priori estimates, we establish differential inequalities for energetic norms in W r2 1 , of solutions of problems with a free bound in media with the fractal geometry for one-dimen- sional evolutionary equation. On the basis of these inequalities, we obtain estimates for the stabilization time T. Metodom apriornyx ocinok vstanovleno dyferencial\ni nerivnosti dlq enerhetyçnyx norm v W r2 1 , rozv’qzkiv zadaç iz vil\nymy meΩamy v seredovywi z fraktal\nog heometri[g dlq odnovymirnoho evolgcijnoho rivnqnnq i na ]x osnovi otrymano ocinky dlq çasu stabilizaci] T. V poslednye hod¥ dlq opysanyq struktur¥ neuporqdoçenn¥x sred y protekag- wyx v nyx processov ßyroko yspol\zuetsq teoryq fraktalov [1 – 4]. Voznyka- gwye pry πtom dyfferencyal\n¥e uravnenyq naz¥vagtsq dyfferencyal\n¥- my uravnenyqmy v sredax s fraktal\noj heometryej [2]. V çastnosty, pry reße- nyy rqda problem πkolohyy voznykaet neobxodymost\ yssledovanyq πvolgcyon- n¥x zadaç so svobodn¥my hranycamy dlq nelynejn¥x uravnenyj v sredax s fraktal\noj strukturoj. V dal\nejßem budem rassmatryvat\ tol\ko odnomer- n¥e zadaçy, kohda yskomaq funkcyq zavysyt ot odnoj prostranstvennoj pere- mennoj. V πtom sluçae dlq opredelenyq funkcyj u = u ( x, t ) y s = s ( t ) , t > 0, poluçaem sledugwug zadaçu so svobodnoj hranycej dlq odnomernoho πvolgcy- onnoho uravnenyq: ∂ ∂ u t = 1 x x x u u x f uα α ψ∂ ∂ ∂ ∂     −( ) ( ) , x0 < x < s ( t ) , t > 0, u ( x, 0 ) = u0 ( x ) , x0 ≤ x ≤ s ( 0 ) , ψ( )u u x ∂ ∂ = γ u, x = x0 , t ≥ 0, (1) u = 0, ψ( )u u x ∂ ∂ = 0, x = s ( t ) , t ≥ 0, hde α = 0, 1, 2 sootvetstvenno pry ploskoj, cylyndryçeskoj y sferyçeskoj symmetryy; x0 = 0 pry 0 ≤ α < 1 y otlyçno ot nulq pry 1 ≤ α < 2, s ( t ) — mo- notonno nevozrastagwaq neprer¥vno dyfferencyruemaq funkcyq; s ′ ( t ) ≤ 0, s ( 0 ) = b > 0. V rabote predpolahaetsq suwestvovanye neotrycatel\noho reße- nyq zadaçy (1). Tol\ko pry πtyx uslovyqx budet poluçena ocenka dlq vremeny stabylyzacyy. Predstavlqet ynteres πvolgcyq prostranstvenno lokalyzovannoho naçal\- noho raspredelenyq u ( x, 0 ) = u0 ( x ) . V kaçestve u0 ( x ) moΩet b¥t\ prynqto toç- noe reßenye sootvetstvugwej (1) stacyonarnoj zadaçy dlq ψ ( u ) = u σ , f ( u ) = = u β , σ ≥ 0, 0 ≤ β < 1 [5]. © G. A. MYTROPOL|SKYJ, A. A. BEREZOVSKYJ, M. X. ÍXANUKOV-LAFYÍEV, 2005 ISSN 1027-3190. Ukr. mat. Ωurn., 2005, t. 57, # 7 997 998 G. A. MYTROPOL|SKYJ, , M. X. ÍXANUKOV-LAFYÍEV 1. Sluçaj slaboho v¥roΩdenyq. PoloΩym v uravnenyy (1) ψ ( u ) = u σ , 0 ≤ α < 1, γ = 0. Tohda poluçym zadaçu ∂ ∂ u t = 1 x x x u u x f uα α σ∂ ∂ ∂ ∂     − ( ), 0 < x < s ( t ) , t > 0 , (2) u ( x, 0 ) = u0 ( x ) , 0 ≤ x ≤ s ( 0 ) , (3) u u x x σ ∂ ∂ =0 = 0, t ≥ 0, (4) u = 0, u u x σ ∂ ∂ = 0, x = s ( t ) , t ≥ 0. (5) UmnoΩym dyfferencyal\noe uravnenye (2) skalqrno na x u t α σ( )1+ : ( ) ( ) ( ), ( ) ( ) , ( ) ( ), ( )u x u x u u u f u x ut t x x t t α σ α σ σ α σ1 1 1+ + +− + = 0 (6) y preobrazuem yntehral¥, vxodqwye v toΩdestvo (6). Dlq pervoho yntehrala poluçaem ( ), ( )u x ut t α σ1+ = ( ) / /1 2 2 0 2 + σ α σx u ut , (7) hde u 0 2 = ( u, u ) , ( u, ϑ ) t = u dx s t ϑ 0 ( ) ∫ . V dal\nejßem v oboznaçenyy ska- lqrnoho proyzvedenyq t budem opuskat\. Yntehryruq po çastqm s uçetom hra- nyçn¥x uslovyj (4), (5) y predpolahaq, çto s ′ ( t ) = O ( 1 ) , t ≥ 0, vtoroj ynteh- ral preobrazuem k vydu ( )( ) , ( )x u u ux x t α σ σ1+ = – 1 2 1 2 1 0 2 ( ) ( )/ + + σ α σd dt x u x . (8) Podstavlqq (7), (8) v toΩdestvo (6), poluçaem ( ) ( ), ( ) ( ) ( )/ / /( )1 1 2 1 2 2 0 2 1 2 1 0 2 + + + + + +σ σ α σ α σ α σx u u f u x u d dt x ut t x = 0. (9) Yspol\zuq dyfferencyal\noe uravnenye (2), pryvodym summu perv¥x dvux slahaem¥x yz toΩdestva (9) k vydu ( ) ( ), ( )/ / ( )1 2 2 0 2 1+ + +σ α σ α σx u u f u x ut t = = ( ) ( ) ( ) ( ) ( ) ( ) 1 1 0 2 0 + −      ∫ ∫σ α α σ σ α σ σ s t x x s t x x x x u u u dx x u u f u u dx . (10) Podstavlqq (10) v toΩdestvo (9), posle yntehryrovanyq po çastqm v poslednem yntehrale naxodym 1 2 1 1 1 2 1 0 2 1 2 0( ) ( ) ( ) ( )/ ( ) + + + + +∫σ σ α σ α σd dt x u x u g u dxx x s t + + σ σ α σ 1 1 2 0+ +∫ x u f u u dxx s t ( ) ( ) ( ) ≤ 0, (11) hde g ( u ) = ′f uu( ). ISSN 1027-3190. Ukr. mat. Ωurn., 2005, t. 57, # 7 STABYLYZACYQ ZA KONEÇNOE VREMQ V ZADAÇAX … 999 Ysxodq yz fyzyçeskoho sm¥sla, predpolahaem, çto f ( u ) — neotrycatel\naq monotonno vozrastagwaq funkcyq y f ( 0 ) = 0, a g ( u ) ≥ 0 — monotonno ub¥- vagwaq funkcyq. Yntehral¥, soderΩawyesq v (11), voobwe hovorq, nesobst- venn¥e, tak kak v sylu hranyçn¥x uslovyj x = s ( t ) , u = 0, f ( u ) = 0, g ( u ) = ∞ . Poπtomu pryvedenn¥e rassuΩdenyq spravedlyv¥ v klasse funkcyj, hde ras- smatryvaem¥e yntehral¥ koneçn¥. Yz (11) sleduet neravenstvo d dt x u x u g u dxx x s t α σ α σ/ ( ) ( ) ( ) ( )2 1 0 2 1 2 0 2+ ++ ∫ ≤ 0. (12) Poskol\ku dlq lgboj neprer¥vno dyfferencyruemoj po x na [ 0, s ( t ) ] , t > 0, funkcyy u ( x, t ) ≥ 0, obrawagwejsq v nul\ na hranyce x = s ( t ) ( u ( s ( t ), t ) = = 0 ) , v¥polnqetsq neravenstvo u ( x, t ) ≤ b x ux 1 01 − − α α α , b = s ( 0 ) = max ( ) t s t ≥0 , to g ( u ) ≥ g b x ux 1 2 01 − −       α α α / . (13) 1.1. Pust\ σ = 0. Tohda d dt x u x u g u dxx x s t α α/ ( ) ( )2 0 2 2 0 2+ ∫ ≤ 0. (14) S pomow\g (13) yz neravenstva (14) naxodym d dt x u x u g b x u dxx x x s t α α α α α / / ( ) 2 0 2 2 1 2 0 0 2 1 + −     − ∫ ≤ 0, yly dy dt g b y y+ −     − 2 1 1 α α ≤ 0, y = x ux α /2 0 2 , otkuda dlq vremeny stabylyzacyy, t. e. toho znaçenyq t = T , pry kotorom y ( T ) = 0, poluçaem ocenku T ≤ 1 2 1 0 0 1 y dy g b y y ( ) ∫ − −     α α < ∞ . 1.2. Pust\ σ > 0 , f ( u ) = cu β, c = const > 0, β > 0 . Tohda neravenstvo (12) prynymaet vyd d dt x u c x u u dxx x s t α σ α σ βσ β/ ( ) ( ) ( ) ( )2 1 0 2 1 2 1 0 2+ + −+ + ∫ ≤ 0. (15) Poskol\ku x u u dxx s t α σ β( ) ( ) 1 2 1 0 1+ −∫ ≥ x u dx b x u x s t x α σ α α σ β σ α ( ) ( ) ( ) / ( )/ ( ) 1 2 0 1 2 1 0 2 1 2 1 1 1+ − + − + ∫ ⋅ −        , ISSN 1027-3190. Ukr. mat. Ωurn., 2005, t. 57, # 7 1000 G. A. MYTROPOL|SKYJ, , M. X. ÍXANUKOV-LAFYÍEV yz (15) naxodym dy dt c yk+ +2 ( )σ β ≤ 0, k = 1 2 2 1 + + + β σ σ( ) . (16) Yz (16) dlq vremeny stabylyzacyy T poluçaem ocenku T ≤ 1 2 0 0 c dy yk y ( ) ( ) σ β+ ∫ < ∞ , k < 1, β < 1, y ( t ) = x ux α /2 0 2 . 2. Sluçaj syl\noho v¥roΩdenyq. Rassmotrym zadaçu ∂ ∂ u t = 1 x x x u u x f uα α σ∂ ∂ ∂ ∂     − ( ), x0 < x < s ( t ) , 0 < t < T , (17) u ( x, 0 ) = u0 ( x ) , x0 ≤ x ≤ s ( 0 ) , (18) u u x x x σ ∂ ∂ = 0 = 0, 1 ≤ α ≤ 2 , t > 0, (19) u = 0, u u x σ ∂ ∂ = 0, x = s ( t ) , t ≥ 0. (20) UmnoΩaq dyfferencyal\noe uravnenye (17) skalqrno na x u t α σ( )1+ y pro- vodq preobrazovanyq, analohyçn¥e yzloΩenn¥m v¥ße, s uçetom uslovyj (18) – (20) poluçaem neravenstvo d dt x u x u g u dxx x x s t α σ α σ/ ( ) ( ) ( ) ( )2 1 0 2 1 22 0 + ++ ∫ ≤ 0. (21) 2.1. Pust\ σ = 0. Poskol\ku u2 ( x ) ≤ dx x x u dx x s t x x s t α α 0 0 2 ( ) ( ) ∫ ∫ ≤ M x ux α /2 0 2 , hde M = ln , , b x b 0 1 1 1 1 pry pry α α α α = − >       − yz (21), uçyt¥vaq svojstva funkcyy g ( u ) , dlq vremeny stabylyzacyy poluçaem ocenku T ≤ dy g My y y 20 0 ( )∫ ( ) < ∞ , y ( t ) = x ux α /2 0 2 . 2.2. Pust\ σ > 0 , f ( u ) = cu β, c = const > 0. Tohda neravenstvo (21) pry- nymaet vyd d dt x u c x u u dxx x x s t α σ α σ ββ/ ( ) ( ) ( )2 1 0 2 1 2 12 1 0 + + −+ ∫ ≤ 0. (22) ISSN 1027-3190. Ukr. mat. Ωurn., 2005, t. 57, # 7 STABYLYZACYQ ZA KONEÇNOE VREMQ V ZADAÇAX … 1001 Yz neravenstva (22) sohlasno yzloΩennomu v¥ße alhorytmu naxodym ocenku dlq vremeny stabylyzacyy T ≤ v dy yk y 0 0( ) ∫ < ∞ , k < 1 ( β < 1 ) , hde k = 1 2 2 1 + + + β σ σ( ) , v = 1 2 0 1 2 1 c b xβ α β σ    − +( )/ ( ) . 1. Dynaryev O. G. Fyl\tracyq v trewynovatoj srede s fraktal\noj heometryej trewyn // Mexanyka Ωydkosty y haza. – 1990. – S. 66 – 70. 2. Mal\ßakov A. V. Uravnenye hydrodynamyky dlq poryst¥x sred so strukturoj porovoho prostranstva, obladagweho fraktal\noj heometryej // YnΩ.-fyz. Ωurn. – 1985. – 62, # 3. – S. 405 – 410. 3. Zel\dovyç Q. B., Sokolov D. D. Fraktal¥, podobye, promeΩutoçnaq asymptotyka // Uspexy fyz. nauk. – 1985. – 146, # 3. – S. 493 – 506. 4. Nyhmatullyn R. R. Reßenye obobwennoho uravnenyq perenosa v sredax s fraktal\noj heometryej // Phys. status. solidi. – 1986. – 133. 5. Mytropol\skyj G. A., Berezovskyj A. A., Íxanukov-Lafyßev M. X. Stabylyzacyq za ko- neçnoe vremq v zadaçax so svobodn¥my hranycamy dlq nekotor¥x klassov nelynejn¥x uravnenyj vtoroho porqdka // Ukr. mat. Ωurn. – 1999. – 51, # 2. – S. 214 – 223. Poluçeno 05.06.2001, posle dorabotky — 04.11.2002 ISSN 1027-3190. Ukr. mat. Ωurn., 2005, t. 57, # 7
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spelling umjimathkievua-article-36582020-03-18T20:01:15Z Finite-Time Stabilization in Problems with Free Boundary for Nonlinear Equations in Media with Fractal Geometry Стабилизация за конечное время в задачах со свободной границей для нелинейных уравнений в средах с фрактальной геометрией Berezovsky, A. A. Mitropolskiy, Yu. A. Shkhanukov-Lafishev, M. Kh. Березовский, А. А. Митропольский, Ю. А. Шхануков-Лафишев, М. Х. Березовский, А. А. Митропольский, Ю. А. Шхануков-Лафишев, М. Х. By using the method of a priori estimates, we establish differential inequalities for energetic norms in $W^l_{2,r}$ of solutions of problems with a free bound in media with the fractal geometry for one-dimensional evolutionary equation. On the basis of these inequalities, we obtain estimates for the stabilization time $T$. Методом апріорних оцінок встановлено диференціальні нерівності для енергетичних норм в $W^l_{2,r}$ розв&#039;язків задач із вільними межами в середовищі з фрактальною геометрією для одновимірного еволюційного рівняння і на їх основі отримано оцінки для часу стабілізації $T$. Institute of Mathematics, NAS of Ukraine 2005-07-25 Article Article application/pdf https://umj.imath.kiev.ua/index.php/umj/article/view/3658 Ukrains’kyi Matematychnyi Zhurnal; Vol. 57 No. 7 (2005); 997–1001 Український математичний журнал; Том 57 № 7 (2005); 997–1001 1027-3190 rus en https://umj.imath.kiev.ua/index.php/umj/article/view/3658/4046 https://umj.imath.kiev.ua/index.php/umj/article/view/3658/4047 Copyright (c) 2005 Berezovsky A. A.; Mitropolskiy Yu. A.; Shkhanukov-Lafishev M. Kh.
spellingShingle Berezovsky, A. A.
Mitropolskiy, Yu. A.
Shkhanukov-Lafishev, M. Kh.
Березовский, А. А.
Митропольский, Ю. А.
Шхануков-Лафишев, М. Х.
Березовский, А. А.
Митропольский, Ю. А.
Шхануков-Лафишев, М. Х.
Finite-Time Stabilization in Problems with Free Boundary for Nonlinear Equations in Media with Fractal Geometry
title Finite-Time Stabilization in Problems with Free Boundary for Nonlinear Equations in Media with Fractal Geometry
title_alt Стабилизация за конечное время в задачах со свободной границей для нелинейных уравнений в средах с фрактальной геометрией
title_full Finite-Time Stabilization in Problems with Free Boundary for Nonlinear Equations in Media with Fractal Geometry
title_fullStr Finite-Time Stabilization in Problems with Free Boundary for Nonlinear Equations in Media with Fractal Geometry
title_full_unstemmed Finite-Time Stabilization in Problems with Free Boundary for Nonlinear Equations in Media with Fractal Geometry
title_short Finite-Time Stabilization in Problems with Free Boundary for Nonlinear Equations in Media with Fractal Geometry
title_sort finite-time stabilization in problems with free boundary for nonlinear equations in media with fractal geometry
url https://umj.imath.kiev.ua/index.php/umj/article/view/3658
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