scholarly journals Analytical solution for Stokes flow inside an evaporating sessile drop: Spherical and cylindrical cap shapes

2009 ◽  
Vol 21 (4) ◽  
pp. 042102 ◽  
Author(s):  
Hassan Masoud ◽  
James D. Felske
1995 ◽  
Vol 50 (20) ◽  
pp. 3313-3317 ◽  
Author(s):  
V.N. Burganos ◽  
F.A. Coutelieris ◽  
G. Dassios ◽  
A.C. Payatakes

2016 ◽  
Vol 26 (3/4) ◽  
pp. 1226-1239 ◽  
Author(s):  
Kai Wang ◽  
Shiting Wen ◽  
Rizwan Zahoor ◽  
Ming Li ◽  
Božidar Šarler

Purpose – The purpose of this paper is to find solution of Stokes flow problems with Dirichlet and Neumann boundary conditions in axisymmetry using an efficient non-singular method of fundamental solutions that does not require an artificial boundary, i.e. source points of the fundamental solution coincide with the collocation points on the boundary. The fundamental solution of the Stokes pressure and velocity represents analytical solution of the flow due to a singular Dirac delta source in infinite space. Design/methodology/approach – Instead of the singular source, a non-singular source with a regularization parameter is employed. Regularized axisymmetric sources were derived from the regularized three-dimensional sources by integrating over the symmetry coordinate. The analytical expressions for related Stokes flow pressure and velocity around such regularized axisymmetric sources have been derived. The solution to the problem is sought as a linear combination of the fields due to the regularized sources that coincide with the boundary. The intensities of the sources are chosen in such a way that the solution complies with the boundary conditions. Findings – An axisymmetric driven cavity numerical example and the flow in a hollow tube and flow between two concentric tubes are chosen to assess the performance of the method. The results of the newly developed method of regularized sources in axisymmetry are compared with the results obtained by the fine-grid second-order classical finite difference method and analytical solution. The results converge with a finer discretization, however, as expected, they depend on the value of the regularization parameter. The method gives accurate results if the value of this parameter scales with the typical nodal distance on the boundary. Originality/value – Analytical expressions for the axisymmetric blobs are derived. The method of regularized sources is for the first time applied to axisymmetric Stokes flow problems.


2019 ◽  
Vol 873 ◽  
pp. 72-88 ◽  
Author(s):  
Tianyi Li ◽  
Aravinda Kar ◽  
Ranganathan Kumar

An analytical solution of a biharmonic equation is presented in axisymmetric toroidal coordinates for Stokes flow due to surface tension gradient on the free surface of sessile drops. The stream function profiles exhibit clockwise and counter-clockwise toroidal volumes. The ring or dot formed by the downward dividing streamlines between these volumes predicts the experimentally deposited particle ring or dot well. This finding suggests that the downward dividing streamline can be taken to be a reasonable indicator of where deposition occurs. Different light patterns directed at different locations of the droplet can give rise to a single spot or ring. A relationship between the positions of the light intensity peak and possible locations of particle deposition is analysed to demonstrate that the streamlines can be generated on-demand to achieve particle deposition at predetermined locations on the substrate. Toroidal corner vortices called Moffatt eddies have appeared in other corner flows and develop in this optical Marangoni flow as well near the contact line.


Author(s):  
A. Merlen ◽  
C. Frankiewicz

Micropumps are a necessary device for microfluidics. Many solutions are possible and technical devices are numerous. In this paper, we have developed an analytical solution for the peristaltic technique in microchannels that enlighten some physical limitations. We have then compared this solution to a numerical one that also provides results when no theoretical results were found. The squeezing of the wall, in the peristaltic technique, is represented by the corner formed by a rolling cylinder on a wall (cf. fig.1).


Sign in / Sign up

Export Citation Format

Share Document