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Article

Existence and Uniqueness Theorem for a Solution to a Class of a Third-Order Nonlinear Differential Equation in the Domain of Analyticity

Institute of Digital Technologies and Modeling in Construction, Moscow State University of Civil Engineering, Yaroslavskoe Shosse, 26, 129337 Moscow, Russia
*
Author to whom correspondence should be addressed.
Axioms 2022, 11(5), 203; https://doi.org/10.3390/axioms11050203
Submission received: 10 March 2022 / Revised: 13 April 2022 / Accepted: 22 April 2022 / Published: 25 April 2022

Abstract

:
The paper considers the specifics of nonlinear differential equations that have applications in different areas. Earlier, the authors proved the existence and uniqueness theorem for a solution to a class of non-linear differential equations in a neighborhood of a moving singular point. In this paper, we consider the first problem of studying a third-order nonlinear differential equation in the domain of analyticity. An analytical approximate solution is built, taking into account the solution search area. A priori estimates of the analytical approximate solution are obtained, and the technology of their optimization using a posteriori ones is illustrated. The result of a numerical experiment is presented. The presented results allow to expand the class of nonlinear differential equations for describing various phenomena and processes.

1. Introduction

Recently, much attention has been paid to nonlinear differential equations for applications in various fields. In particular, a mathematical model based on a nonlinear differential equation [1,2] with moving singular points is used to study cantilever structures. To study wave processes in elastic beams, in [3], a third-order differential equation is considered in an implicit form. The paper [4] considers wave processes in beams based on the generalized Korteweg–de Vries–Burgers equation. During the transition to a stationary process, the equation is reduced to an ordinary differential equation. By varying the parameters of the equation, it is possible to ensure that this equation passes to the class of differential equations we are considering. One of the main points to unite these papers consists on the authors not taking into account the features of nonlinear differential equations. In [5], this study was continued, a solution was proposed to a class of nonlinear differential equations, where the presence of moving singular points was proved. At the same time, the authors demonstrate the practical application of series with fractional negative powers that do not currently have a generally accepted terminology. If in the paper [5] a study was carried out with regard to a neighborhood of a moving singular point, then in this paper the study is continued in the domain of analyticity. An analytical approximate solution is constructed, with a guarantee that there are no moving singular points in the area under consideration. Taking into account the specifics of the equations, we can conclude that the solution search area is divided into two parts: the analyticity area and the neighborhood of the moving singular point. A technique for optimizing a priori estimates of an analytical approximate solution using a posteriori estimates is shown. We pay attention to the results of publications [6,7,8,9,10,11,12], which present the development of the theory of nonlinear differential equations for other classes of equations.

2. Research Methods

Let us consider the following differential equation:
y = a 7 ( x ) y 7 + a 6 ( x ) y 6 + a 5 ( x ) y 5 + a 4 ( x ) y 4 + a 3 ( x ) y 3 + a 2 ( x ) y 2 + a 1 ( x ) y + a 0 ( x ) .
Based on the replacement proposed in paper [5]
y ( x ) = u ( x ) · z ( x ) + v ( x ) ,
we bring Equation (1) to the normal form
z = z 7 ( x ) + r ( x ) .
Let us consider the Cauchy problem
y = y 7 ( x ) + r ( x ) ,
y ( x 0 ) = y 0 , y ( x 0 ) = y 1 , y ( x 0 ) = y 2 .
Theorem 1.
We require the fulfillment of two conditions:
  • r ( x ) C in the domain x x 0 < ρ 1 where 0 < ρ 1 = c o n s t ;
  • M n : r ( n ) ( x 0 ) n ! M n , M n = c o n s t , then there is a unique solution to the Cauchy problem (4)–(5) that can be represented as a regular series
    y ( x ) = 0 C n ( x x 0 ) n ,
    in the domain x x 0 < ρ 2 , where
    ρ 2 = min ρ 1 , 1 ( M + 1 ) 2 , M = max y 0 , y 1 , y 2 , sup n r ( n ) ( x 0 ) n ! , n = 0 , 1 , 2 ,
Proof. 
We build a solution to the problem (4)–(5) for the domain of analyticity in the form of a regular series (6), where C 0 0 . By the condition of the theorem, the function can also be represented by a regular series:
r ( x ) = 0 A n ( x x 0 ) n .
Let us place (6) and (7) into the Equation (4) and we obtain
0 C n ( x x 0 ) n 3 n ( n 1 ) ( n 2 ) = 0 C * * * * n ( x x 0 ) n + 0 A n ( x x 0 ) n ,
The equality of the series in the latter implies the equality of the coefficients at the corresponding powers of the left and right sides. This procedure leads to the following recurrence relation:
n ( n 1 ) ( n 2 ) C n = C n 3 * * * + A n 3 ,
where C n * * * * = i = 0 n C i C j * * * , C n * * * = i = 0 n C i * C j * * , C n * * = i = 0 n C i * C j * , C n * = i = 0 n C i C n i .
The uniqueness of the coefficients implies the uniqueness of solution (6).
Let us prove the validity of the following estimates for the coefficients of the desired series (6):
C 3 k ( M + 1 ) 6 k + 1 3 k ( 3 k 1 ) ( 3 k 2 ) = E 3 k , C 3 k + 1 ( M + 1 ) 6 k + 1 3 k ( 3 k 1 ) ( 3 k + 1 ) = E 3 k + 1 , C 3 k + 2 ( M + 1 ) 6 k + 1 3 k ( 3 k + 1 ) ( 3 k + 2 ) = E 3 k + 2 ,
where
M = max y 0 , y 1 , y 2 , sup n r ( n ) ( x 0 ) n ! , n = 0 , 1 , 2 ,
We limit ourselves to the variant of estimating the coefficient C 3 k + 3 . In this case, taking into account estimates (8) and decomposition C n * * * * , we have:
C 3 k + 3 = 1 ( 3 k + 2 ) 3 k ( 3 k + 1 ) C 3 k 2 * * * * + A 3 k 2 =
= 1 ( 3 k + 2 ) 3 k ( 3 k + 1 ) i = 0 3 k C i j = 0 3 k i C j l = 0 3 k i j C l m = 0 3 k i j l C m C 3 k i j l m + A 3 k 2
1 ( 3 k + 2 ) 3 k ( 3 k + 1 ) i 0 k ( M + 1 ) 6 i + 1 ( 3 i + 2 ) 3 i * ( 3 i + 1 ) j 0 k i ( M + 1 ) 6 j + 1 ( 3 j + 2 ) 3 j * ( 3 j + 1 ) ×
× l 0 k i j ( M + 1 ) 6 l + 1 ( 3 l + 2 ) 3 l * ( 3 l + 1 ) m 0 k i j l ( M + 1 ) 6 m + 1 ( 3 m + 2 ) 3 m * ( 3 m + 1 ) ×
× ( M + 1 ) 6 ( k i j l m ) + 1 ( 3 ( k i j l m ) + 2 ) 3 ( k i j l m ) * ( 3 ( k i j l m ) + 1 ) + M =
( M + 1 ) 6 k + 5 ( 3 k + 2 ) 3 k ( 3 k + 1 ) i 0 k 1 ( 3 i + 2 ) 3 i * ( 3 i + 1 ) j 0 k i 1 ( 3 j + 2 ) 3 j * ( 3 j + 1 ) ×
× l 0 k i j 1 ( 3 l + 2 ) 3 l * ( 3 l + 1 ) m 0 k i j l 1 ( 3 m + 2 ) 3 m * ( 3 m + 1 ) ×
× 1 ( 3 ( k i j l m ) + 2 ) 3 ( k i j l m ) * ( 3 ( k i j l m ) + 1 ) + M
( M + 1 ) 6 k + 5 ( 6 k + 5 ) ( 6 k + 3 ) ( 6 k + 1 ) + M ( M + 1 ) 6 k + 7 ( 6 k + 5 ) ( 6 k + 3 ) ( 6 k + 1 ) ,
where
i * = 1 , i f i = 0 i , i f i 0 , j * = 1 , i f j = 0 j , i f j 0 , l * = 1 , i f l = 0 l , i f l 0 , m * = 1 , i f m = 0 m , i f m 0 ,
( k i j l m ) * = 1 , i f m = k i j l , ( k i j l m ) , i f m k i j l . .
Thus, we are convinced of the estimate of the coefficient C 3 k + 3 . The subsequent estimates in (6) are proved by analogy.
We introduce the next series
0 E n ( x x 0 ) n ,
which is major for the formal series
0 C n ( x x 0 ) n .
Based on the regularity of estimates (8), we represent the series (9) in the following form:
0 E n ( x x 0 ) n = 0 E 3 k ( x x 0 ) 3 k + 0 E 3 k + 1 ( x x 0 ) 3 k + 1 + 0 E 3 k + 2 ( x x 0 ) 3 k + 2 .
Further, for each of the three series on the right-hand side, taking into account estimates (8), we obtain the convergence domain according to d’Alembert:
x x 0 < 1 ( M + 1 ) 6 1 3 = 1 ( M + 1 ) 2 .
Assuming that ρ 2 = min ρ 1 , 1 ( M + 1 ) 2 , we are convinced of the convergence of series (10) in the region under consideration.
The proved theorem allows constructing an analytical approximate solution in the way as follows:
y N ( x ) = 0 N C n ( x x 0 ) n .
Theorem 2.
We require conditions 1 and 2 of theorem 1 to be satisfied. Then, for an analytical approximate solution (11) of the Cauchy problem (4)–(5) in the domain
x x 0 < ρ 2
the error estimate is fair
Δ y N ( x ) = y ( x ) y N ( x ) Δ ,
where
Δ = ( M + 1 ) 2 N + 3 1 ( M + 1 ) 6 x x 0 3 x x 0 N 1 ×
× 1 N ( N 1 ) ( N 2 ) + x x 0 N ( N 1 ) ( N + 1 ) + x x 0 2 N ( N + 1 ) ( N + 2 )
in case N + 1 = 3 k ,
Δ = ( M + 1 ) 2 N + 1 1 ( M + 1 ) 6 x x 0 3 x x 0 N ×
× 1 N ( N 1 ) ( N 2 ) + x x 0 N ( N 1 ) ( N + 1 ) + x x 0 2 N ( N + 1 ) ( N + 2 )
two variants N + 1 = 3 k + 1 , and
Δ = ( M + 1 ) 2 N 1 1 ( M + 1 ) 6 x x 0 3 x x 0 N + 1 ×
× 1 N ( N 1 ) ( N 2 ) + x x 0 N ( N 1 ) ( N + 1 ) + x x 0 2 N ( N + 1 ) ( N + 2 )
with N + 1 = 3 k + 2 , where ρ 2 = min ρ 1 , 1 ( M + 1 ) 4 ,
M = max y 0 , y 1 , y 2 , sup n r ( n ) ( x 0 ) n ! , n = 0 , 1 , 2 , . N 3 .
Proof. 
We limit ourselves to prove the case for N + 1 = 3 k . Let us express Δ y N ( x ) as:
Δ y N ( x ) = y ( x ) y N ( x ) = 0 C n ( x x 0 ) n 0 N C n ( x x 0 ) n = N + 1 C n ( x x 0 ) n
Taking into account the regularity of the coefficients C n from Theorem 1, we obtain:
Δ y N ( x ) = N + 1 C n ( x x 0 ) n N + 1 C n × x x 0 n N + 1 E 3 k x x 0 3 k +
+ N + 1 E 3 k + 1 x x 0 3 k + 1 + N + 1 E 3 k + 2 x x 0 3 k + 2 = N + 1 ( M + 1 ) 6 k + 1 3 k ( 3 k 1 ) ( 3 k 2 ) x x 0 3 k +
N + 1 ( M + 1 ) 6 k + 1 3 k ( 3 k 1 ) ( 3 k + 1 ) x x 0 3 k + 1 + N + 1 ( M + 1 ) 6 k + 1 3 k ( 3 k + 1 ) ( 3 k + 2 ) x x 0 3 k + 2
( M + 1 ) 6 k + 1 1 ( M + 1 ) 6 x x 0 3 x x 0 3 k 1 3 k ( 3 k 1 ) ( 3 k 2 ) + x x 0 3 k ( 3 k 1 ) ( 3 k + 1 ) +
+ x x 0 2 3 k ( 3 k + 1 ) ( 3 k + 2 ) ( M + 1 ) 2 N + 3 1 ( M + 1 ) 6 x x 0 3 x x 0 N 1 1 N ( N 1 ) ( N 2 ) +
+ x x 0 N ( N 1 ) ( N + 1 ) + x x 0 2 N ( N + 1 ) ( N + 2 ) .
Similarly, we obtain estimates for the approximate solution (11) in case N + 1 = 3 k + 1 and N + 1 = 3 k + 2 , which is also valid in the domain x x 0 < ρ 2 . □

3. The Discussion of the Results Numerical Experiment

Let us consider the Cauchy problem (5) and (6), where r ( x ) = 0 , y ( 0 ) = 1 4 , y ( 0 ) = 3 10 , y ( 0 ) = 1 . The Cauchy problem (4) and (5) under given conditions is not solvable in quadratures. The calculation results are presented in Table 1.

4. Conclusions

In this paper, we present a study of the considered class of nonlinear equations in the domain of analyticity, and prove the theorem of the existence and uniqueness of the solution. A formula is obtained for determining the area of analyticity of the solution. A priori estimates of the error of the analytical approximate solution are obtained, and a numerical experiment is carried out, confirming the adequacy of the obtained theoretical positions with the experimental calculations. A technique for optimizing a priori estimates by using a posteriori ones is given.

Author Contributions

Conceptualization, V.O.; methodology, V.O.; validation, V.O.; formal analysis, V.O. and M.G.; investigation, V.O. and M.G.; resources, V.O. and M.G.; data curation, V.O. and M.G.; writing-original draft preparation, V.O. and M.G; supervision, V.O.; project administration, V.O.; funding acquisition, V.O. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Data Availability Statement

The statistical data presented in the article does not require copyright. They are freely available and are listed at the reference address in the bibliography.

Acknowledgments

The authors express their gratitude to the reviewers for valuable comments, who allowed us to improve the content of the article, and to the editors of the journal for their positive attitude towards our work.

Conflicts of Interest

The authors declare no conflict of interest.

References

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Table 1. Numerical characteristics of an analytically approximate solution.
Table 1. Numerical characteristics of an analytically approximate solution.
x 1 y 9 ( x 1 ) Δ 1 Δ 2
0.120.29320.0070.0005
where x 1 is the value of the argument, falls within the scope of Theorem 2, (12); y 9 ( x ) is an analytically approximate solution (11); Δ 1 —a priori estimate; Δ 2 —a posteriori estimate. For Δ 2 = 0.0005 by Theorem 2, we determine N = 14 . The summands from 10 to 14 in the total sum do not exceed the required accuracy of ε = 0.0005, therefore, for N = 9 we obtain a value y 9 ( x 1 ) with an accuracy of ε = 0.0005.
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Orlov, V.; Gasanov, M. Existence and Uniqueness Theorem for a Solution to a Class of a Third-Order Nonlinear Differential Equation in the Domain of Analyticity. Axioms 2022, 11, 203. https://doi.org/10.3390/axioms11050203

AMA Style

Orlov V, Gasanov M. Existence and Uniqueness Theorem for a Solution to a Class of a Third-Order Nonlinear Differential Equation in the Domain of Analyticity. Axioms. 2022; 11(5):203. https://doi.org/10.3390/axioms11050203

Chicago/Turabian Style

Orlov, Victor, and Magomedyusuf Gasanov. 2022. "Existence and Uniqueness Theorem for a Solution to a Class of a Third-Order Nonlinear Differential Equation in the Domain of Analyticity" Axioms 11, no. 5: 203. https://doi.org/10.3390/axioms11050203

APA Style

Orlov, V., & Gasanov, M. (2022). Existence and Uniqueness Theorem for a Solution to a Class of a Third-Order Nonlinear Differential Equation in the Domain of Analyticity. Axioms, 11(5), 203. https://doi.org/10.3390/axioms11050203

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