REVISTA DE LA UNIVERSIDAD DEL ZULIA. 3ª época. Año 14, N° 39, 2023
Y. Kostikov & A. Romanenkov /// On solution of pseudohyperbolic equation… 225-232
DOI: http://dx.doi.org/10.46925//rdluz.39.12
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solution are obtained in the assumption of solution existence. In modern publications the
significant attention is also paid to the research of inverse problems. Thus, for example, the
renewal of the right part of one-dimensional equation is discussed in (Kenzhebai, 2021), and
inverse problems for pseudohyperbolic equation are studied in (Kurmanbaeva, 2016), and the
existence and uniqueness conditions for the solution of a special boundary value problem are
obtained for constant coefficients of linear one-dimensional equation.
Generalized Aller equation of fractional order is considered in (Gekkieva, Karmokov,
Kerefov, 2020; Kerefov, Gekkieva, 2019), for which the exact solution is written out in the
form of finite integral formula. The integral operator kernel is explicitly written out in
(Kerefov, Gekkieva, 2019), with the help of which the exact solution of the second boundary
value problem is specified.
The aim of the work is to form the exact solution in the form of Fourier series of the
first initial boundary value problem for pseudohyperbolic equation. The application of
Fourier method (method of variable separation, for example, in (Ewans, (2003) is usually
successful; due to the mixed derivative availability the variables cannot be separated directly.
Therefore, referring to the type of boundary conditions and type of the differential operator
in the equation (1), we will search for the solution in the following form:
where parameter, which can be a complex number.
The aim of the work is to obtain an exact solution of the initial boundary value
problem in the form of a Fourier series using a special representation of the solution in the
form of formula (4).
Obtaining of exact solution. Then we apply the expression for the required function
from (4) to the equation (1):
After grouping the summands in (5) and simplifying by , we have
The equation (6) is a linear equation with constant coefficients, the solution of which
can be easily written out: