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 
227 
 
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: