{"title":"Unifying Theory of Scaling in Drop Impact: Forces and Maximum Spreading Diameter","authors":"Vatsal Sanjay, Detlef Lohse","doi":"10.1103/physrevlett.134.104003","DOIUrl":null,"url":null,"abstract":"The dynamics of drop impact on a rigid surface strongly depends on the droplet’s velocity, its size, and its material properties. The main characteristics are the droplet’s force exerted on the surface and its maximal spreading radius. The crucial question is how do they depend on the (dimensionless) control parameters, which are the Weber number W</a:mi>e</a:mi></a:mrow></a:math> (nondimensionalized kinetic energy) and the Ohnesorge number <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:mrow><c:mi>O</c:mi><c:mi>h</c:mi></c:mrow></c:math> (dimensionless viscosity). Here, we perform direct numerical simulations over the huge parameter range <e:math xmlns:e=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><e:mrow><e:mn>1</e:mn><e:mo>≤</e:mo><e:mi>W</e:mi><e:mi>e</e:mi><e:mo>≤</e:mo><e:msup><e:mrow><e:mn>10</e:mn></e:mrow><e:mrow><e:mn>3</e:mn></e:mrow></e:msup></e:mrow></e:math> and <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:mrow><g:msup><g:mrow><g:mn>10</g:mn></g:mrow><g:mrow><g:mo>−</g:mo><g:mn>3</g:mn></g:mrow></g:msup><g:mo>≤</g:mo><g:mi>O</g:mi><g:mi>h</g:mi><g:mo>≤</g:mo><g:msup><g:mrow><g:mn>10</g:mn></g:mrow><g:mrow><g:mn>2</g:mn></g:mrow></g:msup></g:mrow></g:math> and in particular develop a unifying theoretical approach, which is inspired by the Grossmann-Lohse theory for wall-bounded turbulence [Grossmann and Lohse, ; ]. The key idea is to split the energy dissipation rate into the different phases of the impact process, in which different physical mechanisms dominate. The theory can consistently and quantitatively account for the <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><i:mrow><i:mi>W</i:mi><i:mi>e</i:mi></i:mrow></i:math> and <k:math xmlns:k=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><k:mrow><k:mi>O</k:mi><k:mi>h</k:mi></k:mrow></k:math> dependences of the maximal impact force and the maximal spreading diameter over the huge parameter space. It also clarifies why viscous dissipation plays a significant role during impact, even for low-viscosity droplets (low <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><m:mi>O</m:mi><m:mi>h</m:mi></m:math>), in contrast to what had been assumed in some prior theories. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"17 2 1","pages":""},"PeriodicalIF":8.1000,"publicationDate":"2025-03-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical review letters","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevlett.134.104003","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
The dynamics of drop impact on a rigid surface strongly depends on the droplet’s velocity, its size, and its material properties. The main characteristics are the droplet’s force exerted on the surface and its maximal spreading radius. The crucial question is how do they depend on the (dimensionless) control parameters, which are the Weber number We (nondimensionalized kinetic energy) and the Ohnesorge number Oh (dimensionless viscosity). Here, we perform direct numerical simulations over the huge parameter range 1≤We≤103 and 10−3≤Oh≤102 and in particular develop a unifying theoretical approach, which is inspired by the Grossmann-Lohse theory for wall-bounded turbulence [Grossmann and Lohse, ; ]. The key idea is to split the energy dissipation rate into the different phases of the impact process, in which different physical mechanisms dominate. The theory can consistently and quantitatively account for the We and Oh dependences of the maximal impact force and the maximal spreading diameter over the huge parameter space. It also clarifies why viscous dissipation plays a significant role during impact, even for low-viscosity droplets (low Oh), in contrast to what had been assumed in some prior theories. Published by the American Physical Society2025
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