Thomas Podgorski, Jean-Marc Flesselles, Laurent Limat
{"title":"流动膜中干燥区域边界的曲率","authors":"Thomas Podgorski, Jean-Marc Flesselles, Laurent Limat","doi":"10.1016/S1296-2147(01)01249-5","DOIUrl":null,"url":null,"abstract":"<div><p>We study experimentally the shape of dry patches inside a film flowing along an inclined plane at relatively high value of the contact angle <em>θ</em>. Their radius of curvature R near apex, is given by <em>R</em>/<em>l</em><sub>c</sub>∼<em>l</em><sub>c</sub><em>V</em><sub>c</sub>/(<em>Γ</em> sin<em>α</em>)−<em>F</em>(<em>α</em>,<em>θ</em>), where <em>Γ</em> is the flow rate per unit length, <em>α</em> the plate slope, and <em>F</em>(<em>α</em>,<em>θ</em>) is a correction that increases with <em>θ</em> and decreases with <em>α</em> (<em>l</em><sub>c</sub> and <em>V</em><sub>c</sub> are the capillary length and the capillary velocity). A simple model allows us to recover this correction and also the existence of a critical flow rate above which dry patches disappear.</p></div>","PeriodicalId":100307,"journal":{"name":"Comptes Rendus de l'Académie des Sciences - Series IV - Physics-Astrophysics","volume":"2 9","pages":"Pages 1361-1367"},"PeriodicalIF":0.0000,"publicationDate":"2001-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/S1296-2147(01)01249-5","citationCount":"6","resultStr":"{\"title\":\"Courbure de la frontière d'une zone sèche dans un film en écoulement\",\"authors\":\"Thomas Podgorski, Jean-Marc Flesselles, Laurent Limat\",\"doi\":\"10.1016/S1296-2147(01)01249-5\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>We study experimentally the shape of dry patches inside a film flowing along an inclined plane at relatively high value of the contact angle <em>θ</em>. Their radius of curvature R near apex, is given by <em>R</em>/<em>l</em><sub>c</sub>∼<em>l</em><sub>c</sub><em>V</em><sub>c</sub>/(<em>Γ</em> sin<em>α</em>)−<em>F</em>(<em>α</em>,<em>θ</em>), where <em>Γ</em> is the flow rate per unit length, <em>α</em> the plate slope, and <em>F</em>(<em>α</em>,<em>θ</em>) is a correction that increases with <em>θ</em> and decreases with <em>α</em> (<em>l</em><sub>c</sub> and <em>V</em><sub>c</sub> are the capillary length and the capillary velocity). A simple model allows us to recover this correction and also the existence of a critical flow rate above which dry patches disappear.</p></div>\",\"PeriodicalId\":100307,\"journal\":{\"name\":\"Comptes Rendus de l'Académie des Sciences - Series IV - Physics-Astrophysics\",\"volume\":\"2 9\",\"pages\":\"Pages 1361-1367\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2001-11-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/S1296-2147(01)01249-5\",\"citationCount\":\"6\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Comptes Rendus de l'Académie des Sciences - Series IV - Physics-Astrophysics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S1296214701012495\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Comptes Rendus de l'Académie des Sciences - Series IV - Physics-Astrophysics","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S1296214701012495","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Courbure de la frontière d'une zone sèche dans un film en écoulement
We study experimentally the shape of dry patches inside a film flowing along an inclined plane at relatively high value of the contact angle θ. Their radius of curvature R near apex, is given by R/lc∼lcVc/(Γ sinα)−F(α,θ), where Γ is the flow rate per unit length, α the plate slope, and F(α,θ) is a correction that increases with θ and decreases with α (lc and Vc are the capillary length and the capillary velocity). A simple model allows us to recover this correction and also the existence of a critical flow rate above which dry patches disappear.