Voir la notice de l'article provenant de la source Math-Net.Ru
[1] Romenskii E. I., “Termodinamicheski soglasovannaya sistema zakonov sokhraneniya techeniya szhimaemoi zhidkosti v poristoi uprugoi srede”, Sib. zhurn. industr. matem., 14:4 (2011), 86–97 | MR
[2] Godunov S. K., Romenskii E. I., Elementy mekhaniki sploshnoi sredy i zakony sokhraneniya, Nauchnaya kniga, Novosibirsk, 1998 | Zbl
[3] Dumbser M., Zanotti O., Hidalgo A., Balsara D. S., “ADER-WENO finite volume schemes with space-time adaptive mesh refinement”, J. Comput. Physics, 248:1 (2013), 257–286 | DOI | MR
[4] Dmitriev M. N., Romenskii E. I., “WENO/Runge–Kutta metod vysokoi tochnosti dlya modelirovaniya uprugikh voln”, Ufimsk. matem. zhurn., 2:1 (2010), 59–70 | Zbl
[5] Spiteri R. J., Ruuth S. J., “A new class of optimal high-order strong-stability preserving time discretization methods”, SIAM J. Numer. Anal., 40:2 (2002), 469–491 | DOI | MR | Zbl
[6] Gottlieb S., “On high order strong stability preserving Runge–Kutta and multi step time discretizations”, J. of Scientific Computing, 25:1–2 (2005), 105–128 | MR | Zbl
[7] Shu C. W., Essentially Non-Oscillatory and Weighted Essentially Non-Oscillatory Schemes for Hyperbolic Conservation Laws, NASA/CR-97-206253, ICASE Report No 97-65, 1997 | MR
[8] Dorovskii V. N., Romenskii E. I., Perepechko Yu. V., Fedorov A. I., “Rezonansnyi metod izmereniya pronitsaemosti gornykh porod”, Geologiya i Geofizika, 52:7 (2011), 950–961