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Mixed and boundary value problems for hyperbolic equations and systems

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Problems of finding solutions of (systems of) partial differential equations of hyperbolic type that satisfy specific conditions on the boundaries of their domains (or on parts of it) (see Boundary conditions; Initial conditions).

A boundary value problem for (a system of) hyperbolic equations in some domain of a Euclidean space is called a mixed or initial boundary value problem if the desired solution, as well as the boundary conditions, must also satisfy initial conditions, or if the support of the boundary data consists of both characteristic and non-characteristic oriented manifolds.

For second-order hyperbolic equations, the support of the initial data in a mixed problem is the spatially-oriented part of . On the time-oriented part of , the boundary conditions are usually of the same type as for parabolic equations (see Mixed and boundary value problems for parabolic equations and systems).

Let be a domain in of points with a sufficiently smooth boundary , and let

Consider in the second-order linear hyperbolic equation

(1)

where summation is from 1 to over repeated subscripts , and the form must be positive definite.

The basic mixed problems for equation (1) can be combined into the following: One has to find a solution of equation (1) in that satisfies the initial conditions

(2)

on and one of the boundary conditions

(3)
(4)
(5)

on , where is a co-normal with respect to the operator . Problems (2), (3); (2), (4); and (2), (5) are usually called the first, second and third mixed problem for equation (1), respectively.

Under fairly general assumptions on the coefficients of (1) and on the boundary , and also on the given functions, one can prove the existence and uniqueness of both regular and generalized solutions of all three mixed problems. The structural and differentiability properties of these solutions in the closed domain in dependence on the smoothness of the boundary have also been investigated [8]. When , the solutions of the mixed problems can be obtained in explicit form.

Mixed problems have been investigated for a wide class of linear and non-linear hyperbolic equations and systems (see Quasi-linear hyperbolic equations and systems). There is a satisfactory theory of mixed problems for strictly-hyperbolic equations and systems of the form

with initial data on the spatially-oriented part of the boundary of lying in the plane . There has also been a successful study of mixed problems for hyperbolic equations and systems in case the supports of the initial or the boundary conditions are surfaces of degenerate type or of the order of these equations (see Degenerate partial differential equation). Most substantial results have been obtained for second-order linear equations of the form

with coefficients satisfying the condition

where and are positive constants, and especially for equations of the form

(6)

Mixed problems with interior or exterior boundary conditions (see Exterior and interior boundary value problems) result from mathematical models of many processes in the theory of scattering of waves on obstructions. For example, the Sommerfeld radiation condition (see Radiation conditions) results from the problem of finding a solution of the wave equation

for all points lying outside a bounded domain , given that the derivative of in the direction of the exterior normal to vanishes for any moment of time , where the initial conditions correspond to a planar wave running from infinity in the direction of the -axis.

The basic boundary value problems for hyperbolic equations and systems are the Goursat and the Darboux–Picard problems and their multi-dimensional analogues (see Goursat problem; Cauchy characteristic problem, and also [1]).

The Goursat and Darboux–Picard problems, and various generalizations of them, have been thoroughly investigated for second-order hyperbolic equations and systems with split principal parts of the form

where , and are given real -matrices, and is a given and $u$ the desired -dimensional vector. Substantial results have also been obtained for a fairly wide class of systems of second-order hyperbolic equations with non-split principal parts in the absence of parabolic degeneracy. It has been shown that the characteristic Goursat problem

for the hyperbolic system

with two independent variables , does not have a unique solution, and the effect of the lowest terms on the well-posedness of this problem has been found [3]. The influence of the nature of parabolic degeneracy on the well-posedness of both the local and the non-local boundary value problem for degenerate hyperbolic equations and systems has been thoroughly investigated [3]. This applies in particular to basic (local) boundary value problems for linear degenerate hyperbolic equations of the form

in bounded domains with an arbitrary piecewise-smooth boundary, and the influence of the order of non-characteristic degeneracy on the well-posedness of the Darboux problem and the non-equivalence of characteristics as supports of boundary conditions has been described (see [10]).

As to finding multi-dimensional analogues of the Darboux and Tricomi problems (see Mixed-type differential equation), much work has been done on non-local boundary value problems, and especially on problems with a shift (see [9]), for hyperbolic equations with a given condition on the characteristic parts of the boundary that connect pointwise the values of the desired solution and its (fractional) derivatives or integrals of some specific order.

Many boundary value problems with a shift that have been studied with great completeness and generality in the case of equation (1) are encompassed by the following formulation. In the domain bounded by the characteristics

and the interval : on the line , one has to find a (sufficiently smooth) solution of equation (1) that satisfies on the local condition

(7)

and on the non-local condition

(8)

Here , , are given functions, is the fractional integro-differential operator of order defined by

if , and by

if , where is the gamma-function, is the integer part of and is the point of intersection of the characteristic emanating from with the characteristic of equation (1):

A detailed study has been made of boundary value problems with a shift for an equation of the form (1) which, in characteristic coordinates and , reduces to an Euler–Darboux–Poisson equation

A special case of the problems (7), (8) is the Darboux problem, which asks for a (sufficiently smooth) solution of equation (6) satisfying the (local) boundary conditions

or

The condition , or the Gellerstedt condition , , , is essential in order that the Darboux problem be well-posed (see [3], [10]).

A qualitatively new multi-dimensional analogue of the Darboux problem is the Bitsadze problem, which in the case of the wave equation can be posed in the following way (see [1]). In the domain bounded by a part of the plane and the two characteristic surfaces

and

one has to find a solution of the equation satisfying , or , .

Other multi-dimensional analogues have been studied, both of the Darboux problem and of non-local boundary value problems (of the type (2), (3)) for hyperbolic equations in special domains, for which the non-characteristic part of the boundary is usually a spatially-oriented surface. Most complete results have been obtained in the case of the Euler–Darboux–Poisson equation .

For an equation of the form

much attention has been devoted to the following non-local problem. In the domain one has to find a (sufficiently smooth) solution of equation

given that, for all ,

or

where are given points in the interval .

A new aspect in the theory of boundary value problems is the study of third-order hyperbolic equations of the form

(10)

which lie at the basis of mathematical models for many processes and phenomena in the theory of mass or heat transfer in porous media. An extensive theory has been developed of both local and non-local linear boundary value problems for hyperbolic equations of the form (10), and in particular, an analogue of the Riemann method has been devised.

For linear symmetric hyperbolic systems of the first order (see Linear hyperbolic partial differential equation and system), a study has been made, within the limits of the theory of systems of first-order equations, of boundary value problems with admissible boundary conditions on (see [6]).

The Dirichlet problem is not, in general, well-posed for hyperbolic equations and systems in arbitrary domains. By methods of energy estimates and integral equations the well-posedness of this problem has been established for a wide class of second-order hyperbolic equations in special cylindrical domains.

References

[1] A.V. Bitsadze, "Certain classes of partial differential equations" , Moscow (1981) (In Russian)
[2] V.S. Vladimirov, "Equations of mathematical physics" , MIR (1984) (Translated from Russian)
[3] S. Gellerstedt, "Sur une équation linéaire aux derivées partielles du type mixte" Ark. Mat. Astr. Fys. , 25A : 29 (1937) pp. 1–23
[4] S.K. Godunov, "The equations of mathematical physics" , Moscow (1979) (In Russian)
[5] T.D. Dzhuraev, "Boundary value problems for equations of mixed and mixed-composite type" , Tashkent (1979) (In Russian)
[6] A.A. Dezin, "General questions in the theory of boundary value problems" , Moscow (1980) (In Russian)
[7] M.M. Lavrent'ev, V.G. Romanov, V.G. Vasil'ev, "Multidimensional inverse problems for differential equations" , Springer (1970) (Translated from Russian)
[8] O.A. Ladyzhenskaya, "A mixed problem for a hyperbolic equation" , Moscow (1953) (In Russian)
[9] A.M. Nakhushev, "Certain boundary value problems for hyperbolic equations and for equations of mixed type" Differential Eq. , 5 : 1 (1969) pp. 37–57 Differentsial'nye Uravn. , 5 : 1 (1969) pp. 44–59
[10] A.M. Nakhushev, "Darboux's problem for degenerate hyperbolic equations" Differential Eq. , 7 : 1 (1971) pp. 41–48 Differentsial'nye Uravn. , 7 : 1 (1971) pp. 49–56
[11] M.S. Salakhitdinov, "Equations of mixed-composite type" , Tashkent (1974) (In Russian)
[12] A.N. [A.N. Tikhonov] Tichonoff, A.A. Samarskii, "Differentialgleichungen der mathematischen Physik" , Deutsch. Verlag Wissenschaft. (1959) (Translated from Russian)
[13] M.Kh. Shkhanukov, "Boundary-value problems for a third-order equation occurring in the modelling of water filtration in porous media" Differential Eq. , 18 : 4 (1982) pp. 509–517 Differentsial'nye Uravn. , 18 : 4 (1982) pp. 689–698


Comments

Concerning the terminology "mixed" see (the editorial comment to) Mixed and boundary value problems for parabolic equations and systems.

How to Cite This Entry:
Mixed and boundary value problems for hyperbolic equations and systems. Encyclopedia of Mathematics. URL: http://www.encyclopediaofmath.org/index.php?title=Mixed_and_boundary_value_problems_for_hyperbolic_equations_and_systems&oldid=29417
This article was adapted from an original article by A.M. Nakhushev (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article