About Us

Executive Editor:
Publishing house "Academy of Natural History"

Editorial Board:
Asgarov S. (Azerbaijan), Alakbarov M. (Azerbaijan), Aliev Z. (Azerbaijan), Babayev N. (Uzbekistan), Chiladze G. (Georgia), Datskovsky I. (Israel), Garbuz I. (Moldova), Gleizer S. (Germany), Ershina A. (Kazakhstan), Kobzev D. (Switzerland), Kohl O. (Germany), Ktshanyan M. (Armenia), Lande D. (Ukraine), Ledvanov M. (Russia), Makats V. (Ukraine), Miletic L. (Serbia), Moskovkin V. (Ukraine), Murzagaliyeva A. (Kazakhstan), Novikov A. (Ukraine), Rahimov R. (Uzbekistan), Romanchuk A. (Ukraine), Shamshiev B. (Kyrgyzstan), Usheva M. (Bulgaria), Vasileva M. (Bulgar).

Additional Information

Authors

Login to Personal account

Home / Issues / № 2, 2013

Materials of the conference "EDUCATION AND SCIENCE WITHOUT BORDERS"

MATHEMATICAL MODELLING OF THE TASKS OF HYDRODYNAMICS BY THE METHOD OF FICTITIOUS AREAS
Kuttykozhayeva Shakharzat Nurtaevna, Bekteleuova Akbota Algabasovna

In this work given a justification of the method of fictitious domains. For the first time obtained not improving mark of convergence rate of the solving the from auxiliary problem to solving the original problem at the time when the small parameter strive to zero.

The fictitious domain method is one of the known methods of approximate solutions of boundary value problems in mathematical physics. In general fictitious domain method is justified for the linear boundary value problems of mathematical physics. In this work is devoted to substantiation of the fictitious domain method for nonlinear elliptic equations. A new method of obtaining best possible rate of convergence of solutions in the method of fictitious domains .

Let's consider the boundary value problem for nonlinear elliptic equations in area with border area

, (1)

. (2)

As method of fictitious domains for the continuation of the lower coefficient in the auxiliary area with border Ø, solving equation with small parameter

, (3)

, (4)

where - continued with zero out of and

Next one notations used are from the monograph

Definition 2.1.1. Generalized solution of the exercises (3), (4) is the function , that is satisfying the integral identity

(5)

for all .

Theorem 1. Let’s . Then there exists a unique weak solution (3)-(4) and it is satisfied the estimate

(6)

where

at that, when this solution converges to the generalized solution of the problem (1), (2).

Definition 2. Stronger solution of the problem (3)-(4) is called function , that satisfying to equation (3) almost everywhere.

Theorem 2.1.2. Let’s . Then there a stronger solution of the problem (3)-(4) and it is satisfied the estimate

, where at . (7)

Theorem 2. Let’s . Then

(8)

- positive constant that not depend from .



References:
1. Вабищевич П.Н. Метод фиктивных областей для задачи математической физики.- Москва: Изд. МГУ, 1991. – 156 с.

2. Смагулов Ш.С. Метод фиктивных областей для краевой задачи уравнений Навье-Стокса .- Новосибирск, 1979,(Предпринт/ВЦ СО АН СССР, №68.-С. 68-73.

3. Коновалов А.Н. Численные методы механики сплошной среды.-1972.-Т.3,№5. –С. 52-67.



Bibliographic reference

Kuttykozhayeva Shakharzat Nurtaevna, Bekteleuova Akbota Algabasovna MATHEMATICAL MODELLING OF THE TASKS OF HYDRODYNAMICS BY THE METHOD OF FICTITIOUS AREAS . International Journal Of Applied And Fundamental Research. – 2013. – № 2 –
URL: www.science-sd.com/455-24310 (21.11.2024).