Matches in SemOpenAlex for { <https://semopenalex.org/work/W2147327725> ?p ?o ?g. }
- W2147327725 endingPage "760" @default.
- W2147327725 startingPage "735" @default.
- W2147327725 abstract "In one space dimension, we consider source-type (self-similar) solutions to the thin-film equation with vanishing slope at the edge of their support (zero contact-angle condition) in the range of mobility exponents $ninleft(frac 3 2,3right)$ . This range contains the physically relevant case n =2 (Navier slip). The existence and (up to a spatial scaling) uniqueness of these solutions has been established in [3] (Bernis, F., Peletier, L. A. & Williams, S. M. (1992) Source type solutions of a fourth-order nonlinear degenerate parabolic equation. Nonlinear Anal . 18 , 217–234). It is also shown there that the leading-order expansion near the edge of the support coincides with that of a travelling-wave solution. In this paper we substantially sharpen this result, proving that the higher order correction is analytic with respect to two variables: the first one is just the spatial variable whereas the second one is a (generically irrational, in particular for n =2) power of it, which naturally emerges from a linearisation of the operator around the travelling-wave solution. This result shows that – as opposed to the case of n =1 (Darcy) or to the case of the porous medium equation (the second-order analogue of the thin-film equation) – in this range of mobility exponents, source-type solutions are not smooth at the edge of their support even when the behaviour of the travelling wave is factored off. We expect the same singular behaviour for a generic solution to the thin-film equation near its moving contact line. As a consequence, we expect a (short-time or small-data) well-posedness theory – of which this paper is a natural prerequisite – to be more involved than in the case n =1." @default.
- W2147327725 created "2016-06-24" @default.
- W2147327725 creator A5013982659 @default.
- W2147327725 creator A5049147245 @default.
- W2147327725 creator A5073872018 @default.
- W2147327725 date "2013-05-22" @default.
- W2147327725 modified "2023-09-26" @default.
- W2147327725 title "Regularity of source-type solutions to the thin-film equation with zero contact angle and mobility exponent between 3/2 and 3" @default.
- W2147327725 cites W1588713757 @default.
- W2147327725 cites W1967357680 @default.
- W2147327725 cites W1971723555 @default.
- W2147327725 cites W1978198939 @default.
- W2147327725 cites W1979080982 @default.
- W2147327725 cites W1988974595 @default.
- W2147327725 cites W2018371111 @default.
- W2147327725 cites W2032994472 @default.
- W2147327725 cites W2049585229 @default.
- W2147327725 cites W2055054359 @default.
- W2147327725 cites W2078279585 @default.
- W2147327725 cites W2082853067 @default.
- W2147327725 cites W2083250674 @default.
- W2147327725 cites W2087522722 @default.
- W2147327725 cites W2103642749 @default.
- W2147327725 cites W2155788949 @default.
- W2147327725 cites W2158169385 @default.
- W2147327725 cites W2165304323 @default.
- W2147327725 doi "https://doi.org/10.1017/s0956792513000156" @default.
- W2147327725 hasPublicationYear "2013" @default.
- W2147327725 type Work @default.
- W2147327725 sameAs 2147327725 @default.
- W2147327725 citedByCount "34" @default.
- W2147327725 countsByYear W21473277252014 @default.
- W2147327725 countsByYear W21473277252015 @default.
- W2147327725 countsByYear W21473277252016 @default.
- W2147327725 countsByYear W21473277252017 @default.
- W2147327725 countsByYear W21473277252018 @default.
- W2147327725 countsByYear W21473277252019 @default.
- W2147327725 countsByYear W21473277252020 @default.
- W2147327725 countsByYear W21473277252021 @default.
- W2147327725 countsByYear W21473277252022 @default.
- W2147327725 countsByYear W21473277252023 @default.
- W2147327725 crossrefType "journal-article" @default.
- W2147327725 hasAuthorship W2147327725A5013982659 @default.
- W2147327725 hasAuthorship W2147327725A5049147245 @default.
- W2147327725 hasAuthorship W2147327725A5073872018 @default.
- W2147327725 hasConcept C10138342 @default.
- W2147327725 hasConcept C121332964 @default.
- W2147327725 hasConcept C134306372 @default.
- W2147327725 hasConcept C138885662 @default.
- W2147327725 hasConcept C158622935 @default.
- W2147327725 hasConcept C162324750 @default.
- W2147327725 hasConcept C182306322 @default.
- W2147327725 hasConcept C18903297 @default.
- W2147327725 hasConcept C2777021972 @default.
- W2147327725 hasConcept C2777299769 @default.
- W2147327725 hasConcept C2780388253 @default.
- W2147327725 hasConcept C2780813799 @default.
- W2147327725 hasConcept C33923547 @default.
- W2147327725 hasConcept C37914503 @default.
- W2147327725 hasConcept C41895202 @default.
- W2147327725 hasConcept C62520636 @default.
- W2147327725 hasConcept C72319582 @default.
- W2147327725 hasConcept C86803240 @default.
- W2147327725 hasConceptScore W2147327725C10138342 @default.
- W2147327725 hasConceptScore W2147327725C121332964 @default.
- W2147327725 hasConceptScore W2147327725C134306372 @default.
- W2147327725 hasConceptScore W2147327725C138885662 @default.
- W2147327725 hasConceptScore W2147327725C158622935 @default.
- W2147327725 hasConceptScore W2147327725C162324750 @default.
- W2147327725 hasConceptScore W2147327725C182306322 @default.
- W2147327725 hasConceptScore W2147327725C18903297 @default.
- W2147327725 hasConceptScore W2147327725C2777021972 @default.
- W2147327725 hasConceptScore W2147327725C2777299769 @default.
- W2147327725 hasConceptScore W2147327725C2780388253 @default.
- W2147327725 hasConceptScore W2147327725C2780813799 @default.
- W2147327725 hasConceptScore W2147327725C33923547 @default.
- W2147327725 hasConceptScore W2147327725C37914503 @default.
- W2147327725 hasConceptScore W2147327725C41895202 @default.
- W2147327725 hasConceptScore W2147327725C62520636 @default.
- W2147327725 hasConceptScore W2147327725C72319582 @default.
- W2147327725 hasConceptScore W2147327725C86803240 @default.
- W2147327725 hasIssue "5" @default.
- W2147327725 hasLocation W21473277251 @default.
- W2147327725 hasOpenAccess W2147327725 @default.
- W2147327725 hasPrimaryLocation W21473277251 @default.
- W2147327725 hasRelatedWork W1031267077 @default.
- W2147327725 hasRelatedWork W1996310820 @default.
- W2147327725 hasRelatedWork W2022107723 @default.
- W2147327725 hasRelatedWork W2037685882 @default.
- W2147327725 hasRelatedWork W2320384189 @default.
- W2147327725 hasRelatedWork W2354466087 @default.
- W2147327725 hasRelatedWork W3095873045 @default.
- W2147327725 hasRelatedWork W3201468793 @default.
- W2147327725 hasRelatedWork W4256644568 @default.
- W2147327725 hasRelatedWork W4297194799 @default.
- W2147327725 hasVolume "24" @default.
- W2147327725 isParatext "false" @default.
- W2147327725 isRetracted "false" @default.