By Alexander B. Al’shin, Maxim O. Korpusov, Alexey G. Sveshnikov
The monograph is dedicated to the research of initial-boundary-value difficulties for multi-dimensional Sobolev-type equations over bounded domain names. The authors think of either particular initial-boundary-value difficulties and summary Cauchy difficulties for first-order (in the time variable) differential equations with nonlinear operator coefficients with recognize to spatial variables. the most target of the monograph is to procure adequate stipulations for international (in time) solvability, to acquire enough stipulations for blow-up of options at finite time, and to derive top and decrease estimates for the blow-up time. The monograph incorporates a mammoth checklist of references (440 goods) and offers an total view of the modern state of the art of the mathematical modeling of varied very important difficulties coming up in physics. because the checklist of references comprises many papers which were released formerly in simple terms in Russian examine journals, it may possibly additionally function a consultant to the Russian literature.
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Additional resources for Blow-up in Nonlinear Sobolev Type Equations (De Gruyter Series in Nonlinear Analysis and Applications)
The mobility is independent of r 2 R3 . r1 r2 ; t /. eE0 / and it has a sharp peak r1 D r2 (see ). R3 /. The following relation succeeds these assumptions and Eq. r; t /j2 : kr'k2 Á In the case of bounded semiconductors, there are other reasons that lead to nonlinear, nonlocal, pseudoparabolic equations. Let us consider the so-called two-temperature superheating mechanism when the free-electron temperature Te is higher than the phonon temperature T0 (see ). 73) T0 meas. jEj/ D dx ; jEj Œmeas.
19), we have a4 ; 2 R1 . We can mark an important property of the problems considered. In the absence of external electric ﬁeld (that is, quite naturally in a real physical situation), Eq. jr'j2 r'/ C j'jq3 ' D 0; q3 0; @t where the constants a3 , a4 , and are deﬁned as for Eqs. 19) and a3 0, a4 2 R1 , and 2 R1 . 30). 33) where a5 D 4 e 1 r3 e and D 1 C 4 ~0 . 33). 33). 2 Nonlinear waves of Oskolkov–Benjamin–Bona–Mahony type In [37, 312, 313], the following model, nonlinear, one-dimensional, pseudoparabolic equation was obtained: @u @t @u @u Cu @x @x @3 u D 0: @x 2 @t It describes nonlinear surface waves that spread along the axis Ox.
Such problems appear in the theory of viscoelastic liquids. , ). 2). 13) D @ a2 B0 a1 2 0 0 a1 C a3 B0 where al 0, l D 1; 3, are certain constants. 14) and ˇ can be positive or negative. , [226–228]). 15) (see ). Of course, taking into account an external magnetic ﬁeld, we see that Eqs. 13). 2) requires some modiﬁcation if a constant external electric ﬁeld E0 presents. 12), but, in the general case, with other parameters and, speciﬁcally, with the other index q2 0. 18) 2 where TO e is the temperature of free electrons and "2 is a small parameter.