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

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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 ..

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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

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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,?.].

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Jo?o 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