... 2 2.1 . ... L|y - y |, (t, y ), (t, y ) Q. 7 , y1 (t) y2 (t) [t0 - T , t0 + T ] y1 (t) = f1 (t, y1 (t)), y1 (t0 ) = y01 , t[t0 -T ,t0 +T ] y2 (t) = f2 (t, y2 (t)), y2 (t0 ) = y02 , max |y1 (t) - y2 (t)| |y 01 - y02 | T max |f1 (t, y ) - f2 (t, y )| exp{LT }. (1.3) (t,y )Q . ... 2.1. 2.1.1: y (t; y0 ) = y0 exp{at} a. T > 0 [0, T ]: t[0,T ] max |y (t; y0 ) - y (t; y0 )| |y0 - y0 | ... Cij exp{ s}, s 0. 2.2. p = max Rek , k=1,...,n 25 | ... C exp{(p + )s}, C = i,j =1,...,n max Cij . ...

Еще в разделе: (Показать все результаты (>2) - mph.cs.msu.ru/ )

• http://mph.cs.msu.ru/stud/2009_ODU-1-RazgulinDenisov.pdf

INTERNATIONAL STANDARD ISO TS 15391 Technical specification Version 2004 October ______________________________________________________________ Space Environment (Natural and Artificial) Probabilistic model for fluences and peak fluxes of solar energetic particles Part I Protons Memorandum Reference No. ISO 15391 SPACE ENVIRONMENT (NATURAL AND ARTIFICIAL) Probabilistic model for fluences and peak fluxes of solar energetic particles: Part I - protons 1 Memorandum-2004 (October) (Memorandum is compiled by

Еще в разделе: (Показать все результаты (>3) - srd.sinp.msu.ru/ )

... Продолжены теоретические и экспериментальные исследования динамики поляризации излучения иттербиевого волоконного лазера с двойной оболочкой. ... International Conference Laser and Laser-information technologies: fundamental problems and Applications, ILLA 2006, p.83. ... Dynamical characteristics of generation of two-frequencies lasers with orthogonal polarizations //Proceedings of 8th International Conference on Laser and Fiber-Optical Networks Modeling, LFNM-2006, Kharkiv, Ukraine, July, 2006, pp...

365. Лаборатория Термохимии МГУ

366. http://hea.phys.msu.ru/pdf/pashkov.pdf