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Large-Scale Self-Assembly in Weakly-Flocculated Suspensions
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Background:
Studies on the formation of colloidal crystals in concentrated suspensions
have mainly been based on dispersed suspensions with a repulsive inter-particle potential of hard or
nearly hard spheres. The self-assembly in weakly-flocculated suspensions has still been unrealized.
Here, we report on the formation of ordered structures in concentrated suspensions of nearly-hard
spherical particles with weakly-attractive inter-particle interactions that are an order of magnitude
higher than the particles’ thermal energy.
Methods:
In our case, the self-assembly in such suspensions is not thermodynamically driven, but an
external shear force must be applied. The driving force for the particles’ ordering is an increase in the
inter-particle interactions. This manifests itself in a decrease in the average angle between the interparticle
interaction direction and the applied shear stress direction.
Results:
For a successful ordering into a large-scale closed packed assembly, the external shear force
must not exceed the inter-particle attractive interaction for the minimum possible average angle (as in
the closed packed structures) but be high enough to enable the particles to move in the highly loaded
suspension.
Conclusion:
The developed method for the self-assembly of the weakly flocculated systems can be
applied very generally e.g. a control over a composition of heterogeneous colloidal crystals, manufacturing
of the large-scale photonic crystals or preparation of very densely packed compacts of particles
needed for the production of sintered ceramics.
Title: Large-Scale Self-Assembly in Weakly-Flocculated Suspensions
Description:
Background:
Studies on the formation of colloidal crystals in concentrated suspensions
have mainly been based on dispersed suspensions with a repulsive inter-particle potential of hard or
nearly hard spheres.
The self-assembly in weakly-flocculated suspensions has still been unrealized.
Here, we report on the formation of ordered structures in concentrated suspensions of nearly-hard
spherical particles with weakly-attractive inter-particle interactions that are an order of magnitude
higher than the particles’ thermal energy.
Methods:
In our case, the self-assembly in such suspensions is not thermodynamically driven, but an
external shear force must be applied.
The driving force for the particles’ ordering is an increase in the
inter-particle interactions.
This manifests itself in a decrease in the average angle between the interparticle
interaction direction and the applied shear stress direction.
Results:
For a successful ordering into a large-scale closed packed assembly, the external shear force
must not exceed the inter-particle attractive interaction for the minimum possible average angle (as in
the closed packed structures) but be high enough to enable the particles to move in the highly loaded
suspension.
Conclusion:
The developed method for the self-assembly of the weakly flocculated systems can be
applied very generally e.
g.
a control over a composition of heterogeneous colloidal crystals, manufacturing
of the large-scale photonic crystals or preparation of very densely packed compacts of particles
needed for the production of sintered ceramics.
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