Difference between revisions of "Evaporation-Driven Assembly of Colloidal Particles"

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(Theories and Simulations)
(Theories and Simulations)
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[[Image:Wiki4_Figure2.jpg]]
 
[[Image:Wiki4_Figure2.jpg]]
  
To understand why these particular packings arise, the authors then study the theoretical basis for the packing selection. For large enough volumes, the minimum energy configuration is a spherical droplet where the particles do not interact. However, when the volume of the droplet decreases to the critical volume (<math>V_C</math>), the droplet cannot remain spherical as the particles come close together. At this critical volume the particles reach a critical packing that is determined by the "cone of influence" of each particle. The cone of influence is a cone that starts at the center of the drop and extends out, tangent to the particle, to intersect with the surface of the droplet. The interactions between the particles on the surface of the droplet are directly related with the interactions between the intersections of the cones of influence of the particles with the surface of the droplet. So, the problem of packing particles on the droplet at the critical volume is like packing circles on a sphere.  
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To understand why these particular packings arise, the authors then study the theoretical basis for the packing selection. For large enough volumes, the minimum energy configuration is a spherical droplet where the particles do not interact. However, when the volume of the droplet decreases to the critical volume (<math>V_C</math>), the droplet cannot remain spherical as the particles come close together. At this critical volume the particles reach a critical packing that is determined by the "cone of influence" of each particle. The cone of influence is a cone that starts at the center of the drop and extends out, tangent to the particle, to intersect with the surface of the droplet. The interactions between the particles on the surface of the droplet are directly related with the interactions between the intersections of the cones of influence of the particles with the surface of the droplet. So, the problem of packing particles on the droplet at the critical volume is like packing circles on a sphere. Most circle packings are unique for a given number of circles. However, there are some numbers of circles (5, 19, 20, 23, ...) where there is a degree of freedom that arises from on of the circles being free to 'rattle' around. There are also some numbers of circles (such as 15) where here are two (or more) different configurations that work.  
  
Below <math>V_C</math>
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Below <math>V_C</math>
  
 
==Results and Conclusions==
 
==Results and Conclusions==

Revision as of 03:16, 24 November 2012

Wiki entry by Emily Gehrels, Fall 2012

Based on the article: Lauga, E., Brenner, M.P. (2004). Evaporation-Driven Assembly of Colloidal Particles. Physical Review Letters, 93, 238301.

Background

Vinny Manoharan wrote a paper describing how clusters of small (d=844nm) polystyrene spheres could be formed in reproducible configurations by dispersing them in a toluene-water emulsion and then preferentially evaporating the toluene. The geometries that formed minimized the second moment of the cluster as defined by <math>\mathcal{M}=\sum_{i}||r_i-r_o||^2</math>. This paper examines the theoretical basis for these findings.

Theories and Simulations

For a droplet with particles attached to the surface, the particles arrange themselves in such a way to minimize the total surface energy between the particles and the drop, the drop and the surrounding medium and the particle and the surrounding medium. A program (Brakke's Surface Evolver) was used to simulate the equilibrium positions of particles in a droplet. The system was initialized with a certain number of particles positioned randomly on the droplet and then the volume of the drop was slowly decreased in steps. At each step the particles were moved to the positions that minimized the energy. The final packings (when the dop volume went to zero) in the simulation agreed with the experimentally observed results as seen in the figure below where in each pair of images the left image is the experimentally observed packing and the right image is the packing obtained from the numerical simulation.

Wiki4 Figure2.jpg

To understand why these particular packings arise, the authors then study the theoretical basis for the packing selection. For large enough volumes, the minimum energy configuration is a spherical droplet where the particles do not interact. However, when the volume of the droplet decreases to the critical volume (<math>V_C</math>), the droplet cannot remain spherical as the particles come close together. At this critical volume the particles reach a critical packing that is determined by the "cone of influence" of each particle. The cone of influence is a cone that starts at the center of the drop and extends out, tangent to the particle, to intersect with the surface of the droplet. The interactions between the particles on the surface of the droplet are directly related with the interactions between the intersections of the cones of influence of the particles with the surface of the droplet. So, the problem of packing particles on the droplet at the critical volume is like packing circles on a sphere. Most circle packings are unique for a given number of circles. However, there are some numbers of circles (5, 19, 20, 23, ...) where there is a degree of freedom that arises from on of the circles being free to 'rattle' around. There are also some numbers of circles (such as 15) where here are two (or more) different configurations that work.

Below <math>V_C</math>

Results and Conclusions