2012
DOI: 10.1063/1.3701615
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Communication: Bulkiness versus anisotropy: The optimal shape of polarizable Brownian nanoparticles for alignment in electric fields

Abstract: Self-assembly and alignment of anisotropic colloidal particles are important processes that can be influenced by external electric fields. However, dielectric nanoparticles are generally hard to align this way because of their small size and low polarizability. In this work, we employ the coupled dipole method to show that the minimum size parameter for which a particle may be aligned using an external electric field depends on the dimension ratio that defines the exact shape of the particle. We show, for rods… Show more

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Cited by 12 publications
(12 citation statements)
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“…While the rods in dilute dispersions are randomly oriented, they align when an electric field is applied . From theory, it is known that the shape of the particle matters for the alignment in electric fields . Since the ends of our rods are not identical in shape, it would therefore be interesting to investigate the influence of this anisotropy on the alignment.…”
Section: Resultsmentioning
confidence: 99%
“…While the rods in dilute dispersions are randomly oriented, they align when an electric field is applied . From theory, it is known that the shape of the particle matters for the alignment in electric fields . Since the ends of our rods are not identical in shape, it would therefore be interesting to investigate the influence of this anisotropy on the alignment.…”
Section: Resultsmentioning
confidence: 99%
“…Both the orientation-dependent energy and the dipolar interactions have been calculated for a wide range of odd-shaped particles such as dumbbells, bowls, cubes, rods, and platelets, using the coupled dipole method. [27][28][29] In this work, we explore the effect of an external uniaxial eld on the phase behavior of cube-shaped colloidal particles, using both experiments and simulations.…”
Section: Introductionmentioning
confidence: 99%
“…Recently, the CDM has been employed to calculate interactions between, and also the polarizability of, nanoclusters of various sizes and shapes. [35][36][37][38][39][40][41] Furthermore, the accuracy of the first-, second-and third-order approximations of the CDM have been compared to the CDM itself in the context of graphitic nanostructures, yielding similar results to ours. 40 For reasons that will be explained shortly, the CDM is only valid for non-metallic particles made of a material that satisfies a 0 /α 1/3 0 1.7, where a 0 is the lattice constant and α 0 the atomic polarizability associated with the material.…”
Section: Introductionmentioning
confidence: 54%