Geodesic
Behavior of the formal solution to a mixed problem for the wave equation
Žurnal vyčislitelʹnoj matematiki i matematičeskoj fiziki, Tome 56 (2016) no. 2, pp. 239-251 
A. P. Khromov. Behavior of the formal solution to a mixed problem for the wave equation. Žurnal vyčislitelʹnoj matematiki i matematičeskoj fiziki, Tome 56 (2016) no. 2, pp. 239-251. http://geodesic.mathdoc.fr/item/ZVMMF_2016_56_2_a6/
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Voir la notice de l'article provenant de la source Math-Net.Ru

The behavior of the formal solution, obtained by the Fourier method, to a mixed problem for the wave equation with arbitrary two-point boundary conditions and the initial condition $\varphi(x)$ (for zero initial velocity) with weaker requirements than those for the classical solution is analyzed. An approach based on the Cauchy–Poincare technique, consisting in the contour integration of the resolvent of the operator generated by the corresponding spectral problem, is used. Conditions giving the solution to the mixed problem when the wave equation is satisfied only almost everywhere are found. When $\varphi(x)$ is an arbitrary function from $L_2[0, 1]$, the formal solution converges almost everywhere and is a generalized solution to the mixed problem.

[1] Steklov V. A., Osnovnye zadachi matematicheskoi fiziki, Nauka, M., 1983

[2] Chernyatin V. A., Obosnovanie metoda Fure v smeshannoi zadache dlya uravnenii v chastnykh proizvodnykh, Izd-vo Mosk. un-ta, M., 1991

[3] Krylov A. N., O nekotorykh differentsialnykh uravneniyakh matematicheskoi fiziki, imeyuschikh prilozheniya v tekhnicheskikh voprosakh, GITTL, M.–L., 1950

[4] Burlutskaya M. Sh., Khromov A. P., “Rezolventnyi podkhod v metode Fure”, Dokl. AN, 458:2 (2014), 138–140 | DOI | MR | Zbl

[5] Burlutskaya M. Sh., Khromov A. P., “Rezolventnyi podkhod dlya volnovogo uravneniya”, Zh. vychisl. matem. i matem. fiz., 55:2 (2015), 229–241 | DOI | Zbl

[6] Khromov A. P., “O klassicheskom reshenii odnoi smeshannoi zadachi dlya volnovogo uravneniya”, Izv. Sarat. un-ta. Nov. ser. Ser. Matematika. Mekhanika. Informatika, 15:1 (2015), 56–66 | Zbl

[7] Naimark M. A., Lineinye differentsialnye operatory, Nauka, M., 1969 | MR

[8] Rasulov M. L., Metod konturnogo integrala, Nauka, M., 1964 | MR

[9] Vagabov A. I., Vvedenie v spektralnuyu teoriyu differentsialnykh operatorov, Izd-vo Rost. un-ta, Rostov n/D., 1994

[10] Marchenko V. A., Operatory Shturma–Liuvilya i ikh prilozheniya, Nauk. dumka, Kiev, 1977 | MR