Titlebook: Evolution Equations of von Karman Type; Pascal Cherrier,Albert Milani Book 2015 Springer International Publishing Switzerland 2015 35K55,3

共同生活

Aurora A. C. Teixeira,Ricardo CastroIn this chapter we assume that . ≥ 2, . ≥ 1, with . + . ≥ 4, and prove Theorem . on the uniformly local strong well-posedness of problem (VKH) in the space ., for some . ∈ ]0, .] independent of ..

arthrodesis

Margaret Patrickson,Alison Say,Leonie HalloIn this chapter we first review a number of results on the regularity of the functions . = .(.., . , ..) and . = .(.) in the framework of the Hardy space ., and then use these results to prove the well-posedness of the von Karman equations (3) and (4) in ..

汇总

具体

Conducive

The Hardy Space , and the Case , = 1,In this chapter we first review a number of results on the regularity of the functions . = .(.., . , ..) and . = .(.) in the framework of the Hardy space ., and then use these results to prove the well-posedness of the von Karman equations (3) and (4) in ..

sebaceous-gland

David B. Audretsch,Julie Ann Elstonf our knowledge, uniqueness of weak solutions to problem (VKH) is open, and presumably not to be expected; in contrast, uniqueness does hold in the physically relevant case of the von Karman equations (3) and (4) in ., that is, when . = 1; we briefly comment of this result, due to Favini et al., [16

场所

https://doi.org/10.1007/978-3-319-02384-7 if . = 2 there is only one kind of semi-strong solution, corresponding to . = 1). Accordingly, we assume that . [recall (.)], and look for solutions of problem (VKH) in the space ., for some . ∈ ]0, .].

chuckle

João J. Ferreira,Cristina I. Fernandes, for some . ∈ ]0, .] independent of .. This means that, under the assumption (.) (that is, again, .. ∈ .. and .), we show that there is . ∈ ]0, .], independent of ., and a unique ., solution of problem (VKP). In addition, this solution depends continuously on the data .. and ., in the sense of (.).

巫婆

1862-9113 s of arbitrary even dimension. Each of these problems consists of a system that results from the coupling of two highly nonlinear partial differential equations, one hyperbolic or parabolic and the other elliptic. These systems take their name from a formal analogy with the von Karman equations in t

inconceivable

Book 2015e problems consists of a system that results from the coupling of two highly nonlinear partial differential equations, one hyperbolic or parabolic and the other elliptic. These systems take their name from a formal analogy with the von Karman equations in the theory of elasticity in two dimensional