Next Article in Journal
Removing Symmetry in Circulant Graphs and Point-Block Incidence Graphs
Previous Article in Journal
Modeling and Analysis of Cardiac Hybrid Cellular Automata via GPU-Accelerated Monte Carlo Simulation
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Initial-Boundary Value Problems for Nonlinear Dispersive Equations of Higher Orders Posed on Bounded Intervals with General Boundary Conditions

by
Nikolai A. Larkin
1,† and
Jackson Luchesi
2,*,†
1
Departamento de Matemática, Universidade Estadual de Maringá, Av. Colombo 5790: Agência UEM, Maringá, PR 87020-900, Brazil
2
Departamento de Matemática, Universidade Tecnológica Federal do Paraná—Câmpus Pato Branco, Via do Conhecimento Km 1, Pato Branco, PR 85503-390, Brazil
*
Author to whom correspondence should be addressed.
These authors contributed equally to this work.
Mathematics 2021, 9(2), 165; https://doi.org/10.3390/math9020165
Submission received: 19 November 2020 / Revised: 24 December 2020 / Accepted: 30 December 2020 / Published: 14 January 2021
(This article belongs to the Special Issue Dispersive Equations of Higher Orders)

Abstract

:
The present article concerns general mixed problems for nonlinear dispersive equations of any odd-orders posed on bounded intervals. The results on existence, uniqueness and exponential decay of solutions are presented.

1. Introduction

In this work, we formulate mixed problems with general boundary conditions for the following dispersive equation:
u t + j = 1 l ( 1 ) j + 1 D x 2 j + 1 u + u D x u = 0 , x ( 0 , L ) ; t > 0 ,
where L is an arbitrary real positive number and l N . We propose Equation (1) because it includes classical models such as the Korteweg-de Vries (KdV) equation, when l = 1 [1,2,3,4] and the Kawahara equation, when l = 2 [5,6,7,8]. Dispersive equations posed on bounded and unbounded intervals with the Dirichlet type boundary conditions were studied in [9,10,11,12,13,14,15,16,17,18,19]. It is known that the KdV and Kawahara equations were deduced on the whole real line, however, approximating the line either by bounded or unbounded intervals, one needs to consider initial-boundary value problems posed either on finite or semi-finite intervals [2,4,9,10,11,13,14,15,17,18,19,20,21,22].
Last years, publications on dispersive equations of higher orders appeared [14,16,23,24,25,26]. Usually, Dirichlet conditions such as D x i u ( t , 0 ) = D x i u ( t , L ) = D x l u ( t , L ) = 0 , i = 0 , , l 1 ; t > 0 were imposed for Equation (1), see [25,26]. In [27], general mixed problems for linear multi-dimensional ( 2 b + 1 ) -hyperbolic equations were studied by means of functional analisys methods. In [28], we have studied boundary value problems for the following linear stationary dispersive equations on bounded intervals subject to general boundary conditions at the endpoints of intervals:
λ u + j = 1 l ( 1 ) j + 1 D x 2 j + 1 u = f ( x ) , x ( 0 , L ) ; l N ,
where λ > 0 and f is a given function. Equation (2) appears while solving Equation (1) making use of either the semigroup theory or semi-discrete approaches [13]. We formulate well posed initial-boundary value problems to Equation (1) imposing the same boundary conditions as for Equation (2) [28].
Our goal is to prove the existence, uniqueness of local and global regular solutions for the formulated problems as well as exponential decay for small initial data.
This article has the following structure: Section 2 contains notations and preliminaries. In Section 3, we formulate the initial-boundary value problems. In Section 4, we prove local existence and uniqueness of regular solutions as well as a “smoothing effect” of them similar to one established in [29] for the initial problem of the KdV equation. In Section 5, the global existence and uniqueness of regular solutions have been established for arbitrary initial data. In Section 6, the existence and uniqueness of small global regular solutions as well as their exponential decay have been established. Section 7 is a conclusion.

2. Notations and Auxiliary Facts

For x ( 0 , L ) , symbols D i = D x i = i x i , i N ; D = D 1 denote the partial derivatives of order i. By · we denote the norm in L ( 0 , L ) . In what follows, we denote by ( · , · ) and · as the inner product and the norm in L 2 ( 0 , L ) and · H m , m N stands for the norm in L 2 -based Sobolev spaces [30].
Lemma 1
(See [26], Lemma 2.2). Let u belong to H 0 1 ( 0 , L ) , then the following inequality holds:
u 2 D u 1 2 u 1 2 .
Lemma 2
(See [31], p. 125). Suppose u and D m u , m N belong to L 2 ( 0 , L ) . Then for the derivatives D i u , 0 i < m , the following inequality holds:
D i u C 1 D m u i m u 1 i m + C 2 u ,
where C 1 , C 2 are constants depending only on L, m, i.
Lemma 3
(See [32]). Let u belong to H 0 1 ( 0 , L ) , then
u L π D u .

3. Formulation of the Problem

Consider the following evolution equation:
u t + j = 1 l ( 1 ) j + 1 D 2 j + 1 u + u D u = 0 , x ( 0 , L ) ; t > 0
subject to initial data
u ( 0 , x ) = u 0 ( x ) , x ( 0 , L ) ,
where u 0 is a given function. In [28], formulation of boundary value problems for the stationary linear equation Equation (2) on the interval ( 0 , L ) has been proposed. In the present work, we will use the same formulation for Equations (6) and (7):
l = 1 :
u ( t , 0 ) = u ( t , L ) = D u ( t , L ) = 0 , t > 0 ,
l 2 :
u ( t , 0 ) = u ( t , L ) = 0 , t > 0 ,
D i u ( t , 0 ) = j = 1 l a i j D j u ( t , 0 ) , i = l + 1 , , 2 l 1 ; t > 0 ,
D i u ( t , L ) = j = 1 l 1 b i j D j u ( t , L ) , i = l , , 2 l 1 ; t > 0 ,
where a i j , b i j are real constants. Assumptions on the coefficients imply that the L 2 -norm of the solutions of Equation (6) is decreasing. Multiplying Equation (6) by u and integrating over ( 0 , L ) , we get
1 2 d d t u 2 ( t ) + j = 1 l ( 1 ) j + 1 ( D 2 j + 1 u , u ) ( t ) = 0 .
A way to obtain d d t u 2 ( t ) 0 , t > 0 is to choose a i j , b i j such that j = 1 l ( 1 ) j + 1 ( D 2 j + 1 u , u ) ( t ) 0 , t > 0 . Making use of integration by parts, finite induction and Young’s inequality, we prove that the coefficients a i j , b i j satisfy the following conditions, see [28]:
For l = 2 :
B 1 = b 31 1 2 b 21 2 2 > 0 , A 1 = a 31 + 1 2 a 32 2 > 0 , A 2 = 1 4 .
This implies that b 31 > 1 2 , a 31 < 1 2 , and | a 32 | , | b 21 | should be sufficiently small or zero.
For l = 3 :
B 1 = b 31 b 51 1 2 b 31 2 1 2 ( | b 32 | + | b 52 | + | b 41 | ) > 0 , B 2 = b 42 1 2 b 32 2 1 2 ( | b 32 | + | b 52 | + | b 41 | ) > 0 , A 1 = a 51 1 2 1 2 ( | a 52 | + | a 41 | + | a 53 | ) > 0 , A 2 = a 42 + 1 2 1 2 ( | a 52 | + | a 41 | + | a 43 | ) > 0 , A 3 = 1 4 1 2 ( | a 53 | + | a 43 | ) > 0 .
This implies that b 51 < 1 2 , b 42 > 1 2 , a 51 > 1 2 , a 42 < 1 2 and the remaining coefficients in Inequality (13) should be sufficiently small or zero.
For l 4 :
B i = k = 1 2 k + i l l i ( 1 ) k + 1 b 2 k + i , i + ( 2 l ) + ( 1 l ) 2 b l i 2 1 2 j = 1 j i l 1 k = 1 2 k + i l l i | b 2 k + i , j | 2 > 0 , i = 1 , , l 1 , A i = k = 1 2 k + i l + 1 l i ( 1 ) k a 2 k + i , i + ( 5 2 l ) 1 2 j = 1 j i l 1 k = 1 2 k + i l + 1 l i | a 2 k + i , j | 2 1 2 k = 1 2 k + i l + 1 l i | a 2 k + i , l | > 0 , i = 1 , , l 1 , A l = 1 4 1 2 i = 1 l 1 k = 1 2 k + i l + 1 l i | a 2 k + i , l | > 0 .
It follows that
b l + 1 , l 1 > l 2 , b l + j , l j > 1 2 m = 1 j 1 2 | b l + 2 m 1 , l 2 m + 1 | 2 + l 2 , j = 3 , , l 1 ( j odd ) , b l + 2 , l 2 < 2 l , b l + j , l j < 1 2 m = 1 j 2 1 | b l + 2 m , l 2 m | 2 + 2 l , j = 4 , , l 1 ( j even ) , a l + 1 , l 1 < 5 2 l , a l + j , l j < 1 2 m = 1 j 1 2 | a l + 2 m 1 , l 2 m + 1 | 2 + 5 2 l , j = 3 , , l 1 ( j odd ) , a l + 2 , l 2 > 2 l 5 , a l + j , l j > 1 2 m = 1 j 2 1 | a l + 2 m , l 2 m | 2 + 2 l 5 , j = 4 , , l 1 ( j even )
and the remaining coefficients of the Inequality (14) should be sufficiently small or zero.
Assuming these coefficients equal to zero in Inequalities (12)–(14), we get the following boundary conditions for all l N , [28]:
u ( t , 0 ) = u ( t , L ) = D l u ( t , L ) = 0 , t > 0 , D l + j u ( t , 0 ) = a l + j , l j D l j u ( t , 0 ) , j = 1 , , l 1 ; t > 0 , D l + j u ( t , L ) = b l + j , l j D l j u ( t , L ) , j = 1 , , l 1 ; t > 0
with b 31 > 1 2 , a 31 < 1 2 for l = 2 ; b 51 < 1 2 , b 42 > 1 2 , a 51 > 1 2 , a 42 < 1 2 for l = 3 and Inequality (15) for l 4 .
Remark 1
(See [28], Remark 1). We call (10) and (11) general boundary conditions because they follow from a more general form:
i = 1 2 l 1 α k i D i u ( t , 0 ) = 0 , k = 1 , , l 1 ; t > 0 , i = 1 2 l 1 β k i D i u ( t , L ) = 0 , k = 1 , , l ; t > 0 ,
where α k i , β k i are real numbers.
Remark 2.
In this work, we will study the case l 2 . For the case l = 1 see [26].

4. Local Regular Solutions

Let T be a real positive number and Q T = ( 0 , T ) × ( 0 , L ) . Consider the linear evolution equation
u t + j = 1 l ( 1 ) j + 1 D 2 j + 1 u = g ( t , x ) in Q T
subject to initial-boundary conditions Equations (7) and (16), with the coefficients satisfying b 31 > 1 2 , a 31 < 1 2 for l = 2 ; b 51 < 1 2 , b 42 > 1 2 , a 51 > 1 2 , a 42 < 1 2 for l = 3 and Inequality (15) for l 4 , where g is a given function. Define the linear operator in L 2 ( 0 , L ) :
A u j = 1 l ( 1 ) j + 1 D 2 j + 1 u ;
D ( A ) { u H 2 l + 1 ( 0 , L ) : u satisfies   the   boundary   conditions E q u a t i o n ( 16 ) } .
Theorem 1
(See [28], Theorem 4.1). Let f L 2 ( 0 , L ) . Then for all λ > 0 a stationary equation: λ u + A u = f ( x ) , x ( 0 , L ) subject to boundary conditions Equation (16) (omitting t) admits a unique regular solution u = u ( x ) H 2 l + 1 ( 0 , L ) satisfying
u H 2 l + 1 C f
where C is a constant depending on L, l, λ, a l + j , l j , b l + j , l j , j = 1 , , l 1 .
Theorem 2.
Let T > 0 , u 0 D ( A ) and g H 1 ( 0 , T ; L 2 ( 0 , L ) ) be given. Then, problem Equations (7), (16) and (17) has a unique solution u = u ( t , x ) :
u C ( [ 0 , T ] ; D ( A ) ) C 1 ( [ 0 , T ] ; L 2 ( 0 , L ) ) .
Proof. 
Due to Theorem 1, the operator λ I + A is surjective for all λ > 0 . On the other hand, by in [28], (33), we obtain
( A u , u ) i = 1 l 1 B i ( D i u ( L ) ) 2 + i = 1 l A i ( D i u ( 0 ) ) 2 0 for   all u D ( A ) .
By the semigroup theory, the result is proven. (See [33], Lemma 2.2.3 and Corollary 2.4.2) □
Theorem 3.
Let u 0 D ( A ) . Then there exists a real T 0 ( 0 , T ) such that Equations (6), (7) and (16) has a unique regular solution u = u ( t , x ) :
u L ( 0 , T 0 ; H 2 l + 1 ( 0 , L ) ) L 2 ( 0 , T 0 ; H ( 2 l + 1 ) + l ( 0 , L ) ) ; u t L ( 0 , T 0 ; L 2 ( 0 , L ) ) L 2 ( 0 , T 0 ; H l ( 0 , L ) ) .
Proof. 
Define g = v D v ; v , v t L ( 0 , T ; L 2 ( 0 , L ) ) L 2 ( 0 , T ; H l ( 0 , L ) ) . Making use of Inequality (3), one can see that g H 1 ( 0 , T ; L 2 ( 0 , L ) ) , then by Theorem 2, we can define an operator P related to Equations (7), (16) and (17) such that v u = P v . Define the Banach space
E = { v ( t , x ) : v , v t L ( 0 , T ; L 2 ( 0 , L ) ) L 2 ( 0 , T ; H l ( 0 , L ) ) ; v ( 0 , · ) u 0 }
with the norm
v E 2 = ess sup t ( 0 , T ) { v 2 ( t ) + v t 2 ( t ) } + 0 T j = 1 l D j v 2 ( t ) + D j v t 2 ( t ) d t
and consider 1 < R < + such that
( 1 + L ) ( 1 + l ) 2 u 0 H l 4 + u 0 H 2 l + 1 2 M 2 M 1 R 2
and a ball B R = { v E : v E 2 8 R 2 } . Here, M 1 = min i { 1 , , l 1 } { B i , A i , A l } and M 2 is the maximum among the coefficients of the derivatives ( D l u ( t , 0 ) ) 2 , ( D i u ( t , 0 ) ) 2 , ( D i u ( t , L ) ) 2 , i = 1 , , l 1 ; t > 0 (see Inequality (19) and [28], p. 389).
Remark 3.
Note that by Inequalities (12)–(14), A l = 1 4 for all l 2 , therefore M 1 1 4 . On the other hand, 1 M 2 < + for all l 2 . This provides that M 1 M 2 1 4 for all l 2 .
Lemma 4.
There is a real T * > 0 such that P ( B R ) B R .
Proof. 
Let v B R , then due to Inequality (20), we get
D v 2 ( t ) D u 0 2 + 0 T D v 2 ( s ) + D v s 2 ( s ) d s M 1 M 2 + 8 R 2 9 R 2 , t ( 0 , T ) .
Making use of Inequalities (3) and (21), we find
v 2 ( t ) ( 34 ) R 2 , v t 2 ( t ) 2 [ 8 R 2 + D v t 2 ( t ) ] , t ( 0 , T ) .
Estimate 1.
Multiplying Equation (17) by 2 u , integrating over ( 0 , L ) and making use of Inequalities (21) and (22), we obtain
d d t u 2 ( t ) + 2 M 1 U ( t , 0 , L ) 2 ( v D v , u ) ( t ) v D v 2 ( t ) + u 2 ( t ) v 2 ( t ) D v 2 ( t ) + u 2 ( t ) C 1 + u 2 ( t ) , t ( 0 , T ) ,
where U ( t , 0 , L ) i = 1 l 1 ( D i u ( t , L ) ) 2 + ( D i u ( t , 0 ) ) 2 + ( D l u ( t , 0 ) ) 2 and C 1 = 9 ( 34 ) R 4 . By the Gronwall Lemma and Inequality (20),
u 2 ( t ) e T R 2 2 + C 1 T , t ( 0 , T ) .
For T 1 = min ln 2 , 2 M 1 R 2 C 1 M 2 , 2 M 1 R 2 C 1 M 2 L , we find
u 2 ( t ) 2 R 2 , t ( 0 , T 1 ) .
Substituting Inequality (24) into Inequality (23), integrating the result over ( 0 , T 1 ) and making use of Inequality (20), we get
0 T 1 U ( t , 0 , L ) d t 1 2 M 1 3 M 1 M 2 R 2 + M 1 M 2 R 2 = 2 R 2 M 2 .
Estimate 2.
Multiplying Equation (17) by 2 x u and making use of Inequalities (21), (22) and (24), we obtain
d d t ( x , u 2 ) ( t ) + 2 L i = 1 l 1 B i ( D i u ( t , L ) ) 2 2 M 2 U ( t , 0 , L ) + j = 1 l ( 2 j + 1 ) D j u 2 ( t ) L v D v 2 ( t ) + u 2 ( t ) L ( C 1 + 2 R 2 ) , t ( 0 , T 1 ) .
Integrating Inequality (26) over ( 0 , T 1 ) and making use of Inequalities (20) and (25), we conclude
0 T 1 j = 1 l D j u 2 ( t ) d t 2 R 2 .
Estimate 3.
Differentiating Equation (17) with respect to t, multiplying the result by 2 u t and making use of Inequalities (21) and (22), one gets for an arbitrary ε > 0
d d t u t 2 ( t ) + 2 M 1 U t ( t , 0 , L ) ε v t D v 2 ( t ) + v D v t 2 ( t ) + 2 ε u t 2 ( t ) ε C 2 1 + D v t 2 ( t ) + 2 ε u t 2 ( t ) , t ( 0 , T ) ,
where U t ( t , 0 , L ) i = 1 l 1 ( D i u t ( t , L ) ) 2 + ( D i u t ( t , 0 ) ) 2 + ( D l u t ( t , 0 ) ) 2 and C 2 = C 2 ( R ) is a fixed positive constant. Taking ε = M 1 ( 16 ) M 2 C 2 , we reduce it to the inequality
d d t u t 2 ( t ) + 2 M 1 U t ( t , 0 , L ) ( 32 ) M 2 C 2 M 1 u t 2 ( t ) + M 1 ( 16 ) M 2 1 + D v t 2 ( t ) , t ( 0 , T ) .
By the Gronwall Lemma,
u t 2 ( t ) e ( 32 ) M 2 C 2 M 1 T u t 2 ( 0 ) + M 1 ( 16 ) M 2 0 T 1 + D v t 2 ( t ) d t .
Due to Inequalities (3) and (20),
u t 2 ( 0 ) ( 1 + l ) u 0 D u 0 2 + u 0 H 2 l + 1 2 ( 1 + l ) 2 u 0 H l 4 + u 0 H 2 l + 1 2 M 1 ( 1 + L ) M 2 R 2 R 2 4 .
Choosing T 2 = min M 1 ln 2 ( 32 ) M 2 C 2 , M 1 2 ( 64 ) M 2 2 C 2 , 3 M 1 8 ( 16 ) M 2 C 2 L 2 , we find
u t 2 ( t ) 2 R 2 , t ( 0 , T 2 ) .
Substituting Inequality (29) into Inequality (28), integrating the result over ( 0 , T 2 ) and making use of Inequality (20), we get
0 T 2 U t ( t , 0 , L ) d t 1 2 M 1 M 1 M 2 R 2 + 2 M 1 M 2 R 2 + M 1 M 2 R 2 = 2 R 2 M 2 .
Estimate 4.
Differentiating Equation (17) with respect to t, multiplying the result by 2 x u t and making use of Inequalities (21), (22) and (29), we obtain
d d t ( x , u t 2 ) ( t ) + 2 L i = 1 l 1 B i ( D i u t ( t , L ) ) 2 2 M 2 U t ( t , 0 , L ) + j = 1 l ( 2 j + 1 ) D j u t 2 ( t ) ε L v t D v 2 ( t ) + v D v t 2 ( t ) + 2 L ε u t 2 ( t ) ε L C 2 1 + D v t 2 ( t ) + 4 L ε R 2 , t ( 0 , T 2 ) .
Taking ε = M 1 ( 16 ) M 2 C 2 L , integrating over ( 0 , T 2 ) , and making use of Inequalities (20) and (30), we find
0 T 2 j = 1 l D j u t 2 ( t ) d t 2 R 2 .
For T * = min { T 1 , T 2 } , it follows from Inequalities (24), (27), (29) and (31) that P v = u B R . This completes the proof of Lemma 4. □
Lemma 5.
There is a real T > 0 such that the mapping P is a contraction in B R .
Proof. 
For v 1 , v 2 B R , denote u i = P v i , i = 1 , 2 , w = v 1 v 2 , z = u 1 u 2 and Z ( t , 0 , L ) i = 1 l 1 [ ( D i z ( t , L ) ) 2 + ( D i z ( t , 0 ) ) 2 ] + ( D l z ( t , 0 ) ) 2 . Then z satisfies the equation
z t + j = 1 l ( 1 ) j + 1 D 2 j + 1 z = v 1 D w w D v 2 i n Q T ,
boundary conditions Equation (16) and initial data z ( 0 , · ) 0 .
Similar arguments used in the proof of Lemma 4 show that z E 1 2 w E . Therefore, P is a contraction in B R .  □
According to Lemmas 4 and 5 and the Banach Fixed Point Theorem with T 0 = min { T * , T } , problem Equations (6), (7) and (16) has a unique generalized solution u = u ( t , x ) :
u L ( 0 , T 0 ; H l ( 0 , L ) ) ;
u t L ( 0 , T 0 ; L 2 ( 0 , L ) ) L 2 ( 0 , T 0 ; H l ( 0 , L ) ) .
Rewrite Equation (6) in the form
u + j = 1 l ( 1 ) j + 1 D 2 j + 1 u = u u t u D u : = F ( t , x ) .
Due to Relations (33) and (34), it follows that u D u H 1 ( 0 , T 0 ; L 2 ( 0 , L ) ) , hence F L ( 0 , T 0 ; L 2 ( 0 , L ) ) . Making use of Inequality (18), we get
u L ( 0 , T 0 ; H 2 l + 1 ( 0 , L ) ) .
Acting as in [26], Lemma 4.3, we find
u L 2 ( 0 , T 0 ; H ( 2 l + 1 ) + l ( 0 , L ) ) .
Combining Relations (34), (36) and (37), we complete the proof of Theorem 3. □
Remark 4.
The local result presented in Theorem 3 can be obtained under the following boundary conditions:
D i u ( t , 0 ) = j = 0 l a i j D j u ( t , 0 ) , i = l + 1 , , 2 l ; t > 0 ,
D i u ( t , L ) = j = 0 l 1 b i j D j u ( t , L ) , i = l , , 2 l ; t > 0
instead of Equations (8)–(11) (see [28], Remark 3). We also call Equations (38) and (39) general boundary conditions because they follow from a more general form:
i = 0 2 l α k i D i u ( t , 0 ) = 0 , k = 1 , , l ; t > 0 i = 0 2 l β k i D i u ( t , L ) = 0 , k = 1 , , l + 1 ; t > 0 ,
where α k i , β k i are real numbers (see Remark 1).

5. Global Regular Solutions

Theorem 4.
Let u 0 H 2 l + 1 ( 0 , L ) satisfying Equation (16). Then for all T > 0 , problem Equations (6), (7) and (16) has a unique regular solution u = u ( t , x ) :
u L ( 0 , T ; H 2 l + 1 ( 0 , L ) ) L 2 ( 0 , T ; H ( 2 l + 1 ) + l ( 0 , L ) ) ; u t L ( 0 , T ; L 2 ( 0 , L ) ) L 2 ( 0 , T ; H l ( 0 , L ) ) .
Proof. 
We will obtain a priori estimates independent of t ( 0 , T ) .
Estimate 1.
Multiplying Equation (6) by 2 u , we obtain
2 ( u t , u ) ( t ) + 2 M 1 U ( t , 0 , L ) 0 ,
where U ( t , 0 , L ) i = 1 l 1 ( D i u ( t , L ) ) 2 + ( D i u ( t , 0 ) ) 2 + ( D l u ( t , 0 ) ) 2 and M 1 = min i { 1 , , l 1 } { B i , A i , A l } .
Consequently,
u ( t ) u 0 , t ( 0 , T ) .
Estimate 2.
Multiplying Equation (6) by 2 x u , we get
2 ( u t , x u ) ( t ) + 2 L i = 1 l 1 B i ( D i u ( t , L ) ) 2 2 M 2 U ( t , 0 , L ) + j = 1 l ( 2 j + 1 ) D j u 2 ( t ) + 2 ( u D u , x u ) ( t ) 0 ,
where M 2 is calculated in [28], p. 389. Making use of Inequalities (3) and (41), we estimate
2 ( u D u , x u ) ( t ) = 2 3 ( u , u 2 ) ( t ) 2 2 3 D u 1 2 ( t ) u 1 2 ( t ) u 2 ( t ) 2 2 3 D u 1 2 ( t ) u 0 5 2 D u 2 ( t ) C u 0 10 3 ,
where C is a positive constant. On the other hand, due to Inequality (40) and the fact that M 2 M 1 1 for all l 2 , we get
2 M 2 U ( t , 0 , L ) 2 M 2 M 1 ( u t , u ) ( t ) 2 ( u t , u ) ( t ) .
Substituting Inequalities (43) and (44) into Inequality (42), we find
d d t ( 1 + x , u 2 ) ( t ) + 2 D u 2 ( t ) + j = 2 l 1 ( 2 j + 1 ) D j u 2 ( t ) C u 0 10 3 .
After integration of Inequality (45) over ( 0 , T ) , we conclude
0 T j = 1 l D j u 2 ( t ) d t C u 0 2
where C = C ( T , L , l , u 0 ) is a positive constant.
Estimate 3.
Differentiate Equation (6) with respect to t, multiply the result by 2 u t to obtain
2 ( u t t , u t ) ( t ) + 2 M 1 U t ( t , 0 , L ) + 2 ( D [ u u t ] , u t ) ( t ) 0 ,
where U t ( t , 0 , L ) i = 1 l 1 ( D i u t ( t , L ) ) 2 + ( D i u t ( t , 0 ) ) 2 + ( D l u t ( t , 0 ) ) 2 . Making use of Inequalities (3) and (41), we estimate for an arbitrary ε > 0
2 ( D [ u u t ] , u t ) ( t ) = 2 ( u u t , D u t ) ( t ) 1 ε ( | u | 2 , | u t | 2 ) ( t ) ε D u t 2 ( t ) 2 ε D u ( t ) u ( t ) u t 2 ( t ) ε D u t 2 ( t ) 1 ε 2 u 0 2 + D u 2 ( t ) u t 2 ( t ) ε D u t 2 ( t ) .
Substituting Inequality (48) into Inequality (47), we find
U t ( t , 0 , L ) 1 M 1 ( u t t , u t ) ( t ) + 1 2 M 1 1 ε 2 u 0 2 + D u 2 ( t ) u t 2 ( t ) + ε 2 M 1 D u t 2 ( t ) .
Estimate 4.
Differentiate Equation (6) with respect to t, multiply the result by 2 x u t and integrate over ( 0 , L ) . The result reads
2 ( u t t , x u t ) ( t ) + 2 L i = 1 l 1 B i ( D i u t ( t , L ) ) 2 2 M 2 U t ( t , 0 , L ) + j = 1 l ( 2 j + 1 ) D j u t 2 ( t ) + 2 ( D [ u u t ] , x u t ) ( t ) 0 .
Making use of Inequalities (3) and (41), we estimate
2 ( D [ u u t ] , x u t ) ( t ) = 2 ( u u t , u t + x D u t ) ( t ) 2 ( | u | , u t 2 ) ( t ) L 2 ( u 2 , u t 2 ) ( t ) D u t 2 ( t ) 2 2 D u 1 2 ( t ) u 0 1 2 u t 2 ( t ) 2 L 2 D u ( t ) u 0 u t 2 ( t ) D u t 2 ( t ) C 1 + D u 2 ( t ) u t 2 ( t ) D u t 2 ( t )
for some positive constant C = C ( L , u 0 ) . On the other hand, taking into account Inequality (49) with ε = M 1 M 2 and exploiting the relation M 2 M 1 1 for all l 2 , we obtain
2 M 2 U t ( t , 0 , L ) 2 ( u t t , u t ) ( t ) C 1 + D u 2 ( t ) u t 2 ( t ) D u t 2 ( t )
for some positive constant C = C ( M 1 , M 2 , u 0 ) . Substituting Inequalities (51) and (52) into Inequality (50), we get
d d t ( 1 + x , u t 2 ) ( t ) + D u t 2 ( t ) + j = 2 l ( 2 j + 1 ) D j u t 2 ( t ) C 1 + D u 2 ( t ) ( 1 + x , u t 2 ) ( t ) .
Due to Inequality (46), 1 + D u 2 ( t ) L 1 ( 0 , T ) , whence by the Gronwall Lemma,
u t 2 ( t ) ( 1 + x , u t 2 ) ( t ) C u 0 H l 4 + u 0 H 2 l + 1 2 .
Substituting Inequality (54) into Inequality (53) and integrating over ( 0 , T ) , we find
0 T j = 1 l D j u t 2 ( t ) d t C u 0 H l 4 + u 0 H 2 l + 1 2
with a positive constant C = C ( T , L , l , a l + j , l j , b l + j , l j , u 0 ) , j = 1 , , l 1 .
Estimates Inequalities (41), (46), (54) and (55) allow us to extend the local solution ensured by Theorem 3 to all T > 0 and to prove the existence of a generalized solution u = u ( t , x ) :
u L ( 0 , T ; H l ( 0 , L ) ) ; u t L ( 0 , T ; L 2 ( 0 , L ) ) L 2 ( 0 , T ; H l ( 0 , L ) ) .
Acting as by the proof of Theorem 3 and making use of Relation (56), we get
u L ( 0 , T ; H 2 l + 1 ( 0 , L ) ) L 2 ( 0 , T ; H ( 2 l + 1 ) + l ( 0 , L ) ) .
The existence part of Theorem 4 is proved.
Lemma 6.
A regular solution of Equations (6), (7) and (16) is uniquelly defined.
Proof. 
Let u 1 and u 2 be two distinct regular solutions of Equations (6), (7) and (16), then the difference w = u 1 u 2 satisfies the equation
w t + j = 1 l ( 1 ) j + 1 D 2 j + 1 w + 1 2 D [ u 1 2 u 2 2 ] = 0 ,
boundary conditions Equation (16) and initial data w ( 0 , · ) 0 .
Estimate 5.
Multiplying Equation (57) by 2 w , we find
2 ( w t , w ) ( t ) + 2 M 1 W ( t , 0 , L ) + ( D [ u 1 2 u 2 2 ] , w ) ( t ) 0 ,
where W ( t , 0 , L ) i = 1 l 1 ( D i w ( t , L ) ) 2 + ( D i w ( t , 0 ) ) 2 + ( D l w ( t , 0 ) ) 2 . Since u 1 , u 2 are regular solutions of Equations (6), (7) and (16), then
u i H l ( t ) C < + , i = 1 , 2 for   a . e . t ( 0 , T ) ,
where C = C ( L , l , a l + j , l j , b l + j , l j ) , j = 1 , , 1 1 . Making use of Inequalities (3) and (59), we estimate for an arbitrary ε > 0
( D [ u 1 2 u 2 2 ] , w ) ( t ) ( | u 1 + u 2 | | w | , | D w | ) ( t ) u 1 + u 2 ( t ) 1 2 ε w 2 ( t ) + ε 2 D w 2 ( t ) 2 2 C 1 2 ε w 2 ( t ) + ε 2 D w 2 ( t ) .
Substituting Inequality (60) into Inequality (58), we obtain
W ( t , 0 , L ) 1 M 1 ( w t , w ) ( t ) + 2 C M 1 1 2 ε w 2 ( t ) + ε 2 D w 2 ( t ) .
Estimate 6.
Multiplying Equation (57) by 2 x w , we get
2 ( w t , x w t ) ( t ) + 2 L i = 1 l 1 B i ( D i w ( t , L ) ) 2 2 M 2 W ( t , 0 , L ) + j = 1 l ( 2 j + 1 ) D j w 2 ( t ) + 2 ( D [ u 1 2 u 2 2 ] , x w ) ( t ) 0 .
Making use of Inequalities (3) and (59), we estimate for an arbitrary ε > 0
2 ( D [ u 1 2 u 2 2 ] , x w ) ( t ) ( | u 1 + u 2 | | w | , | w | + x | D w | ) ( t ) u 1 + u 2 ( t ) w 2 ( t ) + 1 2 ε ( x , w 2 ) ( t ) + ε L 2 D w 2 ( t ) 2 2 C 1 + 1 2 ε ( 1 + x , w 2 ) ( t ) + ε L 2 D w 2 ( t ) .
Substituting Inequalities (61) and (63) into Inequality (62), we reduce it to the inequality
d d t ( 1 + x , w 2 ) ( t ) + 3 ε 2 C M 2 M 1 + 2 C L D w 2 ( t ) + j = 2 l ( 2 j + 1 ) D j w 2 ( t ) 2 C M 2 M 1 ε + 2 2 C 1 + 1 2 ε ( 1 + x , w 2 ) ( t ) .
Taking ε > 0 such that 3 ε 2 C M 2 M 1 + 2 C L > 0 and applying the Gronwall Lemma, we obtain w ( t ) 0 , t ( 0 , T ) . This completes the proof of Lemma 6. □
Uniqueness part of Theorem 4 is thereby proved. □

6. Exponential Decay of Small Regular Solutions

Theorem 5.
Let u 0 H 2 l + 1 ( 0 , L ) satisfy Equation (16) and
u 0 < min { m 1 , m 2 } ,
where
m 1 = π 2 C 0 L 2 3 / 4 , m 2 = π 2 L 2 2 2 K 0 ( 1 + C 1 K 0 ) 1 2 , K 0 = ( 1 + L ) ( 1 + l ) 2 u 0 H l 4 + u 0 H 2 l + 1 2 + ( 2 + L + C 0 u 0 4 / 3 ) u 0 2 1 / 3 , C 0 = 2 2 / 3 · 3 1 / 3 , C 1 = 2 L 2 2 + 2 M 2 2 2 M 1 2 u 0 1 / 2 .
Then Equations (6), (7) and (16) has a unique global regular solution u = u ( t , x ) :
u L ( ( 0 , + ) ; H 2 l + 1 ( 0 , L ) ) L 2 ( ( 0 , + ) ; H ( 2 l + 1 ) + l ( 0 , L ) ) ; u t L ( ( 0 , + ) ; L 2 ( 0 , L ) ) L 2 ( ( 0 , + ) ; H l ( 0 , L ) )
satisfying the inequalities:
u 2 ( t ) C e θ t , u t 2 ( t ) C e θ t , u H 2 l + 1 2 ( t ) C e θ t ,
where θ = π 2 / ( 1 + L ) L 2 .
Proof. 
We need global in t a priori estimates of local solutions in order to prolong them for all t > 0 .
Estimate 1.
Estimates Inequalities (40) and (41) are valid in our case:
U ( t , 0 , L ) ( u t , u ) M 1 ( t ) , u ( t ) u 0 t > 0 ,
where U ( t , 0 , L ) i = 1 l 1 ( D i u ( t , L ) ) 2 + ( D i u ( t , 0 ) ) 2 + ( D l u ( t , 0 ) ) 2 and M 1 = min i { 1 , , l 1 } { B i , A i , A l } .
Estimate 2.
Multiply Equation (6) by 2 x u and integrate over ( 0 , L ) to obtain
2 ( u t , x u ) ( t ) + 2 L i = 1 l 1 B i ( D i u ( t , L ) ) 2 2 M 2 U ( t , 0 , L ) + j = 1 l ( 2 j + 1 ) D j u 2 ( t ) + 2 ( u D u , x u ) ( t ) 0 ,
where M 2 is calculated in [28], p. 389. Making use of Inequalities (3) and (65), we estimate
2 ( u D u , x u ) ( t ) = 2 3 ( u , u 2 ) ( t ) 2 2 3 D u 1 2 ( t ) u 1 2 ( t ) u 2 ( t ) D u 2 ( t ) C 0 u 0 4 3 u 2 ( t ) ,
where C 0 = 2 2 / 3 · 3 1 / 3 . Substituting Inequalities (65) and (67) into Inequality (66) and using Equation (5), we get
d d t ( 1 + x , u 2 ) ( t ) + D u 2 ( t ) + j = 2 l ( 2 j + 1 ) D j u 2 ( t ) + 1 1 + L π 2 L 2 C 0 u 0 4 3 ( 1 + x , u 2 ) ( t ) 0 .
Due to Inequalities (5) and (64),
d d t ( 1 + x , u 2 ) ( t ) + θ ( 1 + x , u 2 ) ( t ) 0 ,
where θ = π 2 / ( 1 + L ) L 2 . Consequently
u 2 ( t ) C e θ t .
Estimate 3.
By Inequalities (3) and (65), Inequality (66) becomes
2 L i = 1 l 1 B i ( D i u ( t , L ) ) 2 + j = 1 l ( 2 j + 1 ) D j u 2 ( t ) 2 ( u t , ( 1 + x ) u ) ( t ) 2 ( u D u , x u ) ( t ) 2 ( 1 + L ) u t ( t ) u ( t ) + 2 2 3 D u 1 2 ( t ) u 1 2 ( t ) u 2 ( t ) D u 2 ( t ) + ( 1 + L ) u t 2 ( t ) + ( 1 + L + C 0 u 0 4 3 ) u 2 ( t ) .
Thus
u H l 2 ( t ) ( 1 + L ) u t 2 ( t ) + ( 2 + L + C 0 u 0 4 3 ) u 2 ( t ) .
Estimate 4.
Differentiate Equation (6) with respect to t, multiply the result by 2 u t and integrate over ( 0 , L ) to obtain
2 ( u t t , u t ) ( t ) + 2 M 1 U t ( t , 0 , L ) + 2 ( D [ u u t ] , u t ) ( t ) 0 ,
where U t ( t , 0 , L ) i = 1 l 1 ( D i u t ( t , L ) ) 2 + ( D i u t ( t , 0 ) ) 2 + ( D l u t ( t , 0 ) ) 2 . Repeating arguments used to prove Inequality (48), we estimate for an arbitrary ε > 0
2 ( D [ u u t ] , u t ) ( t ) 2 ε D u ( t ) u ( t ) u t 2 ( t ) ε D u t 2 ( t ) .
Substituting Inequality (71) into Inequality (70) and using Inequality (65), we find
U t ( t , 0 , L ) 1 M 1 ( u t t , u t ) ( t ) + 1 ε M 1 u 0 D u ( t ) u t 2 ( t ) + ε 2 M 1 D u t 2 ( t ) .
Estimate 5.
Differentiate Equation (6) with respect to t, multiply the result by 2 x u t to obtain
2 ( u t t , x u t ) ( t ) + 2 L i = 1 l 1 B i ( D i u t ( t , L ) ) 2 2 M 2 U t ( t , 0 , L ) I 1 + j = 1 l ( 2 j + 1 ) D j u t 2 ( t ) + 2 ( D [ u u t ] , x u t ) ( t ) I 2 0 .
Taking into account Inequality (72) with ε = M 1 2 M 2 and exploiting the relation M 2 M 1 1 for all l 2 , we obtain
I 1 2 ( u t t , u t ) ( t ) 4 M 2 2 M 1 2 u 0 D u ( t ) u t 2 ( t ) 1 2 D u t 2 ( t ) .
On the other hand, repeating arguments used to prove Inequality (51), we estimate
I 2 2 2 u 0 1 2 D u 1 2 ( t ) 1 + 2 L 2 2 u 0 1 2 D u 1 2 ( t ) u t 2 ( t ) 1 2 D u t 2 ( t ) .
Making use of Inequalities (65) and (69), we find
I 1 + I 2 2 ( u t t , u t ) ( t ) 2 2 u 0 1 2 D u 1 2 ( t ) 1 + 2 L 2 2 + 2 M 2 2 2 M 1 2 u 0 1 2 D u 1 2 ( t ) u t 2 ( t ) D u t 2 ( t ) 2 ( u t t , u t ) ( t ) 2 2 u 0 1 2 ( 1 + L ) u t 2 ( t ) + ( 2 + L + C 0 u 0 4 3 ) u 0 2 1 4 [ 1 + 2 L 2 2 + 2 M 2 2 2 M 1 2 u 0 1 2 × ( 1 + L ) u t 2 ( t ) + ( 2 + L + C 0 u 0 4 3 ) u 0 2 1 4 ] u t 2 ( t ) D u t 2 ( t ) .
Substituting I 1 + I 2 into Inequality (73), we get
d d t ( 1 + x , u t 2 ) ( t ) + D u t 2 ( t ) + j = 2 l ( 2 j + 1 ) D j u t 2 ( t ) + D u t 2 ( t ) 2 2 u 0 1 2 K ( t ) 1 + C 1 K ( t ) u t 2 ( t ) 0 .
Here
K ( t ) = ( 1 + L ) u t 2 ( t ) + ( 2 + L + C 0 u 0 4 / 3 ) u 0 2 1 / 3 , C 1 = 2 L 2 2 + 2 M 2 2 2 M 1 2 u 0 1 2 .
Using Inequality (5), this inequality can be rewritten as
d d t ( 1 + x , u t 2 ) ( t ) + D u t 2 ( t ) + j = 2 l ( 2 j + 1 ) D j u t 2 ( t ) + 1 1 + L π 2 L 2 2 2 u 0 1 2 K ( t ) 1 + C 1 K ( t ) ( 1 + x , u t 2 ) ( t ) 0 .
Taking into account Inequality (64), the fact that K ( 0 ) K 0 and standard arguments, see [14], we reduce it to the form
d d t ( 1 + x , u t 2 ) ( t ) + θ ( 1 + x , u t 2 ) ( t ) 0 ,
where θ = π 2 / ( 1 + L ) L 2 . This implies
u t 2 ( t ) ( 1 + x , u t 2 ) ( t ) C e θ t .
Returning to Inequality (74) with Inequality (76) and integrating over ( 0 , + ) , we obtain
u t L 2 ( ( 0 , + ) ; H l ( 0 , L ) ) .
Finally, substituting Inequalities (68) and (76) into Inequality (69), we find
u H l 2 ( t ) C e θ t .
Estimate 6.
(Regularity) Rewrite Equation (6) in the form
( 1 ) l + 1 D 2 l + 1 u = u t j = 1 l 1 ( 1 ) j + 1 D 2 j + 1 u u D u .
We estimate
D 2 l + 1 u ( t ) u t ( t ) + 2 j l 1 D 2 j + 1 u ( t ) + l 1 < 2 j < 2 l D 2 j + 1 u ( t ) + u D u ( t ) .
For l = 2 , we have 2 j l 1 D 2 j + 1 u ( t ) = 0 and for l 3 , due to Inequality (77),
2 j l 1 D 2 j + 1 u ( t ) l u H l ( t ) C e θ 2 t .
Making use of Inequalities (3) and (77), we obtain
u D u ( t ) 2 u H l 2 ( t ) C e θ t .
On the other hand, Inequality (4) implies
D 2 j + 1 u ( t ) C 1 j D 2 l + 1 u α j ( t ) u 1 α j ( t ) + C 2 j u ( t ) ( l 1 < 2 j < 2 l ) ,
where α j = 2 j + 1 2 l + 1 and C 1 j , C 2 j are constants depending on L, l. Making use of the Young inequality with an arbitrary ε > 0 , we get
D 2 j + 1 u ( t ) ε D 2 l + 1 u ( t ) + ( C j ( ε ) + C 2 j ) u ( t ) .
Summing over l 1 < 2 j < 2 l and taking into account Inequality (68), we find
l 1 < 2 j < 2 l D 2 j + 1 u ( t ) l ε D 2 l + 1 u ( t ) + C ( ε ) e θ 2 t .
Substituting Inequalities (76), (79), (80) and (81) into Inequality (78) and taking ε = 1 2 l , we obtain
D 2 l + 1 u ( t ) C 3 e θ 2 t + e θ t C e θ 2 t .
Again by Inequality (4), for all i = l + 1 , , 2 l , there are constants C 1 i , C 2 i depending only on L, l such that
D i u ( t ) C 1 i D 2 l + 1 u α i ( t ) u 1 α i ( t ) + C 2 i u ( t ) with α i = i 2 l + 1 .
By the Young inequality and Inequalities (68) and (82), we get
D i u ( t ) C e θ 2 t , i = l + 1 , , 2 l .
According to Inequalities (77), (82) and (83), we conclude that
u H 2 l + 1 2 ( t ) C e θ t
with θ = π 2 / ( 1 + L ) L 2 . Repeating the arguments that appears in the proof of Lemma 4.3 in [26], and taking into account Inequality (84), we establish a “smoothing effect”:
u L 2 ( ( 0 , + ) ; H ( 2 l + 1 ) + l ( 0 , L ) ) .
Similar arguments used in the proof of Lemma 6 with Inequality (77) instead of Inequality (59), show the uniqueness of the solution. The proof of Theorem 5 is complete. □

7. Conclusions

Making use of the formulation of a linear stationary version of Equation (1) in [28], we prove in Theorem 3 local existence and uniqueness of regular solutions. In Theorem 4, we prove global in t ( 0 , T ) existence and uniqueness of regular solution for arbitrary smooth initial data and arbitrary T > 0 . In Theorem 5, we prove global in t ( 0 , + ) existence and uniqueness of regular solutions as well as their exponential decay of u ( t ) , u t ( t ) and u H 2 l + 1 ( t ) for small initial data. A smoothing effect has been established: if u 0 H 2 l + 1 ( 0 , L ) , then u L 2 ( ( 0 , + ) ; H ( 2 l + 1 ) + l ( 0 , L ) ) . Our results can be used for constructing of numerical schemes while studying various models of initial-boundary value problems for higher-order dispersive equations.

Author Contributions

N.A.L. and J.L. contributed equally to this work. All authors have read and agreed to the published version of the manuscript.

Funding

Nikolai A. Larkin has been supported by Fundação Araucária, Paraná, Brazil.: Convênio Nº 307/2015, Protocolo No 45.703.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Not applicable.

Acknowledgments

The authors appreciate useful comments of reviewers.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Benia, Y.; Scapellato, A. Existence of solution to Korteweg-de Vries equation in a non-parabolic domain. Nonlinear Anal. 2020, 195, 111758. [Google Scholar] [CrossRef]
  2. Bona, J.L.; Sun, S.-M.; Zhang, B.-Y. A nonhomogeneous boundary-value problem for the Korteweg-de Vries equation posed on a finite domain. Commun. Part. Differ. Equ. 2003, 28, 1391–1436. [Google Scholar] [CrossRef]
  3. Jeffrey, A.; Kakutani, T. Weak nonlinear dispersive waves: A discussion centered around the Korteweg-de Vries equation. SIAM Rev. 1972, 14, 582–643. [Google Scholar] [CrossRef]
  4. Larkin, N.A.; Tronco, E. Nonlinear quarter-plane problem for the Korteweg-de Vries equation. Electron. J. Differ. Equ. 2011, 2011, 1–22. [Google Scholar]
  5. Biagioni, H.A.; Linares, F. On the Benney–Lin and Kawahara equations. J. Math. Anal. Appl. 1997, 211, 131–152. [Google Scholar] [CrossRef] [Green Version]
  6. Faminskii, A.V.; Martynov, E.V. On initial-boundary value problems on semiaxis for generalized Kawahara equation. Contemp. Math. Fundam. Dir. 2019, 65, 683–699. (In Russian) [Google Scholar] [CrossRef]
  7. Kawahara, T. Oscillatory solitary waves in dispersive media. J. Phys. Soc. Jpn. 1972, 33, 260–264. [Google Scholar] [CrossRef]
  8. Kuvshinov, R.V.; Faminskii, A.V. Mixed Problem for the Kawahara Equation in a Half-Strip. Differ. Equ. 2009, 45, 404–415. [Google Scholar] [CrossRef]
  9. Boutet de Monvel, A.; Shepelsky, D. Initial boundary value problem for the mKdV equation on a finite interval. Annales de l’institut Fourier 2004, 54, 1477–1495. [Google Scholar] [CrossRef] [Green Version]
  10. Bubnov, B.A. General boundary-value problems for the Korteweg-de Vries equation in a bounded domain. Differ. Uravn. 1979, 15, 26–31. [Google Scholar]
  11. Bubnov, B.A. Solvability in the large of nonlinear boundary-value problems for the Korteweg-de Vries equation in a bounded domain. Differ. Uravn. 1980, 16, 34–41. [Google Scholar]
  12. Ceballos, J.; Sepulveda, M.; Villagran, O. The Korteweg-de Vries- Kawahara equation in a bounded domain and some numerical results. Appl. Math. Comput. 2007, 190, 912–936. [Google Scholar] [CrossRef] [Green Version]
  13. Doronin, G.G.; Larkin, N.A. Kawahara equation in a bounded domain. Discret. Contin. Dyn. Syst. B 2008, 10, 783–799. [Google Scholar] [CrossRef]
  14. Faminskii, A.V.; Larkin, N.A. Initial-boundary value problems for quasilinear dispersive equations posed on a bounded interval. Electron. J. Differ. Equ. 2010, 2010, 1–20. [Google Scholar]
  15. Kramer, E.F. Nonhomogeneous Boundary Value Problems for the Korteweg-de Vries Equations on a Bounded Domain. Ph.D. Thesis, University of Cincinatti, Cincinnati, OH, USA, 2009. [Google Scholar]
  16. Larkin, N.A. Correct initial boundary value problems for dispersive equations. J. Math. Anal. Appl. 2008, 344, 1079–1092. [Google Scholar] [CrossRef] [Green Version]
  17. Larkin, N.A. Korteweg-de Vries and Kuramoto-Sivashinsky Equations in Bounded Domains. J. Math. Anal. Appl. 2004, 297, 169–185. [Google Scholar] [CrossRef]
  18. Larkin, N.A.; Luchesi, J. General Mixed Problems for the KdV Equations on Bounded Intervals. Electron. J. Differ. Equ. 2010, 2010, 1–17. [Google Scholar]
  19. Larkin, N.A.; Simões, M.H. The Kawahara equation on bounded intervals and on a half-line. Nonlinear Anal. 2015, 127, 397–412. [Google Scholar] [CrossRef]
  20. Capistrano-Filho, R.A.; Sun, S.-M.; Zhang, B.-Y. General Boundary Value Problems of the Korteweg-de Vries Equation on a Bounded Domain. Math. Control Relat. Fields 2018, 8, 583–605. [Google Scholar] [CrossRef] [Green Version]
  21. Coclite, G.M.; di Ruvo, L. On the initial-boundary value problem for a Kuramoto-Sinelshchikov type equation. Math. Eng. 2020, 3, 1–43. [Google Scholar] [CrossRef]
  22. Larkin, N.A.; Simões, M.H. General Boundary Conditions for the Kawahara Equations on Bounded Intervals. Electron. J. Differ. Equ. 2013, 2013, 1–21. [Google Scholar]
  23. Isaza, P.; Linares, F.; Ponce, G. Decay properties for solutions of fifth order nonlinear dispersive equations. J. Differ. Equ. 2015, 258, 764–795. [Google Scholar] [CrossRef]
  24. Kenig, C.E.; Ponce, G.; Vega, L. Higher -order nonlinear dispersive equations. Proc. Am. Math. Soc. 1994, 122, 157–166. [Google Scholar] [CrossRef]
  25. Larkin, N.A.; Luchesi, J. Higher-Order Stationary Dispersive Equations on Bounded Intervals. Adv. Math. Phys. 2018, 2018, 7874305. [Google Scholar] [CrossRef] [Green Version]
  26. Larkin, N.A.; Luchesi, J. Initial-boundary value problems for generalized dispersive equations of higher orders posed on bounded intervals. Appl. Math. Optim. 2019. [Google Scholar] [CrossRef]
  27. Volevich, L.R.; Gindikin, S.C. A mixed problem for (2b + 1)-hyperbolic equations. Tr. Mosk. Mat. Obs. 1981, 43, 197–259. (In Russian) [Google Scholar]
  28. Larkin, N.A.; Luchesi, J. Formulation of problems for stationary dispersive equations of higher orders on bounded intervals with general boundary conditions. Contemp. Math. 2020, 1. [Google Scholar] [CrossRef]
  29. Kato, T. On the Cauchy problem for the (generalized) Korteweg-de Vries equations. Adv. Math. Supl. Stud. Stud. Appl. Math. 1983, 8, 93–128. [Google Scholar]
  30. Adams, R.; Fournier, J. Sobolev Spaces, 2nd ed.; Elsevier Science Ltd.: Amsterdam, The Netherlands, 2003. [Google Scholar]
  31. Nirenberg, L. On elliptic partial differential equations. In Annali della Scuola Nomale Superiore di Pisa, Classe di Scienze 3a série; tome 13, n° 2; Springer: Berlin/Heidelberg, Germany, 1959; pp. 115–162. [Google Scholar]
  32. Nazarov, A.I.; Kuznetsov, N.G.; Poborchi, S.V.V.A. Steklov and Problem of Sharp (Exact) Constants in Inequalities of Mathematical Physics. arXiv 2013, arXiv:1307.8025v1. [Google Scholar]
  33. Zheng, S. Nonlinear Evolution Equations; Chapman Hill/CRC: Boca Raton, FL, USA, 2004. [Google Scholar]
Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Share and Cite

MDPI and ACS Style

Larkin, N.A.; Luchesi, J. Initial-Boundary Value Problems for Nonlinear Dispersive Equations of Higher Orders Posed on Bounded Intervals with General Boundary Conditions. Mathematics 2021, 9, 165. https://doi.org/10.3390/math9020165

AMA Style

Larkin NA, Luchesi J. Initial-Boundary Value Problems for Nonlinear Dispersive Equations of Higher Orders Posed on Bounded Intervals with General Boundary Conditions. Mathematics. 2021; 9(2):165. https://doi.org/10.3390/math9020165

Chicago/Turabian Style

Larkin, Nikolai A., and Jackson Luchesi. 2021. "Initial-Boundary Value Problems for Nonlinear Dispersive Equations of Higher Orders Posed on Bounded Intervals with General Boundary Conditions" Mathematics 9, no. 2: 165. https://doi.org/10.3390/math9020165

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop