Sinking of small sphere at low Reynolds number through interface

A dense solid sphere gently released on an air-liquid interface slowly sinks into liquid due to gravity, while the motion is resisted by viscous and capillary forces. Here, we predict the sinking velocity of the interface-straddling sphere by a simplified model and experimentally corroborate the res...

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Published inPhysics of fluids (1994) Vol. 23; no. 7; pp. 072104 - 072104-9
Main Authors Lee, Duck-Gyu, Kim, Ho-Young
Format Journal Article
LanguageEnglish
Published Melville, NY American Institute of Physics 01.07.2011
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Abstract A dense solid sphere gently released on an air-liquid interface slowly sinks into liquid due to gravity, while the motion is resisted by viscous and capillary forces. Here, we predict the sinking velocity of the interface-straddling sphere by a simplified model and experimentally corroborate the results. The viscous drag on the sphere is determined by integrating the surface stress, which is the solution of the Stokes equation, over the wetted area that changes with time. To compute the interfacial tension force that depends on the meniscus profile, we solve the dynamic boundary condition for the normal and tangential stresses at the air-liquid interface. The predicted sinking velocity, a function of the sphere density and radius, liquid density, viscosity and surface tension, and the dynamic contact angle, is in good agreement with the experimental measurements except for the late stages when meniscus snapping occurs. We also construct a scaling law for the steady velocity of a sinking sphere, which gives the characteristic sinking time.
AbstractList A dense solid sphere gently released on an air-liquid interface slowly sinks into liquid due to gravity, while the motion is resisted by viscous and capillary forces. Here, we predict the sinking velocity of the interface-straddling sphere by a simplified model and experimentally corroborate the results. The viscous drag on the sphere is determined by integrating the surface stress, which is the solution of the Stokes equation, over the wetted area that changes with time. To compute the interfacial tension force that depends on the meniscus profile, we solve the dynamic boundary condition for the normal and tangential stresses at the air-liquid interface. The predicted sinking velocity, a function of the sphere density and radius, liquid density, viscosity and surface tension, and the dynamic contact angle, is in good agreement with the experimental measurements except for the late stages when meniscus snapping occurs. We also construct a scaling law for the steady velocity of a sinking sphere, which gives the characteristic sinking time.
Author Kim, Ho-Young
Lee, Duck-Gyu
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  surname: Kim
  fullname: Kim, Ho-Young
  email: hyk@snu.ac.kr. Tel.: 82-2-880-9286. Fax: 82-2-880-9287.
  organization: School of Mechanical and Aerospace Engineering, Seoul National University, Seoul 151-744, South Korea
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Issue 7
Keywords Gas liquid interface
Low Reynolds number
Theoretical study
Hydrodynamics
Immersion
Spheres
Experimental study
Viscous fluids
Language English
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Snippet A dense solid sphere gently released on an air-liquid interface slowly sinks into liquid due to gravity, while the motion is resisted by viscous and capillary...
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SubjectTerms Applied fluid mechanics
Exact sciences and technology
Fluid dynamics
Fundamental areas of phenomenology (including applications)
Hydrodynamics, hydraulics, hydrostatics
Physics
Title Sinking of small sphere at low Reynolds number through interface
URI http://dx.doi.org/10.1063/1.3614536
Volume 23
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