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Related Concept Videos

Imperfections in Crystal Structure: Stoichiometric Point Defects01:26

Imperfections in Crystal Structure: Stoichiometric Point Defects

Schottky defects arise when some lattice points in a crystal, such as those in NaCl, remain unoccupied, creating lattice vacancies without disturbing the overall electrical neutrality of the crystal. This defect is common in ionic crystals where the positive and negative ions are similar in size, as seen in sodium chloride and cesium chloride. The presence of Schottky defects enables the crystal to conduct electricity to a small extent through an ionic mechanism. Electric fields cause nearby...
Imperfections in Crystal Structure: Point, Line and Plane Defects01:25

Imperfections in Crystal Structure: Point, Line and Plane Defects

A perfect crystal, in theory, has a uniform structure with the same unit cell and lattice points throughout. However, any deviation from this periodic arrangement is known as an imperfection or defect. These defects can be categorized into three types: point, line, and plane defects.Point defects occur when there is a deviation from the ideal due to missing atoms, displaced atoms, or additional atoms. These imperfections might occur due to imperfect packing during crystallization or because of...
Imperfections in Crystal Structure: Non-Stoichiometric Defects01:29

Imperfections in Crystal Structure: Non-Stoichiometric Defects

Non-stoichiometric defects refer to a type of defect in the crystal structure of a compound where the ratio of its constituent elements deviates from the ideal stoichiometric ratio. There are two main types of non-stoichiometric defects: metal excess defects and metal deficiency defects.Metal excess defects occur when there is a slight surplus of metal ions than what is required by the stoichiometric ratio of the compound. For example, heating a sodium chloride crystal in sodium vapor results...
Ionic Crystal Structures02:42

Ionic Crystal Structures

Ionic crystals consist of two or more different kinds of ions that usually have different sizes. The packing of these ions into a crystal structure is more complex than the packing of metal atoms that are the same size.
Most monatomic ions behave as charged spheres, and their attraction for ions of opposite charge is the same in every direction. Consequently, stable structures for ionic compounds result (1) when ions of one charge are surrounded by as many ions as possible of the opposite...
Potential Due to a Polarized Object01:29

Potential Due to a Polarized Object

A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
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Lattice Centering and Coordination Number

The structure of a crystalline solid, whether a metal or not, is best described by considering its simplest repeating unit, which is referred to as its unit cell. The unit cell consists of lattice points that represent the locations of atoms or ions. The entire structure then consists of this unit cell repeating in three dimensions. The three different types of unit cells present in the cubic lattice are illustrated in Figure 1.
Types of Unit Cells
Imagine taking a large number of identical...

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Novel Techniques for Observing Structural Dynamics of Photoresponsive Liquid Crystals
10:35

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Published on: May 29, 2018

Defect structures in nematic liquid crystals around charged particles.

K Tojo1, A Furukawa, T Araki

  • 1Department of Physics, Kyoto University, Sakyo-ku, Kyoto 606-8502, Japan.

The European Physical Journal. E, Soft Matter
|September 17, 2009
PubMed
Summary

This study numerically investigates liquid crystal defects around charged particles. Novel "ansa" defects form when dielectric anisotropy is negative, influencing particle pair alignment.

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Area of Science:

  • Materials Science
  • Condensed Matter Physics
  • Soft Matter Physics

Background:

  • Nematic liquid crystals exhibit complex behavior around impurities.
  • Charged particles introduce electrostatic interactions that can deform the director field.
  • Understanding defect formation is crucial for liquid crystal display technology and advanced materials.

Purpose of the Study:

  • To numerically investigate orientation deformations in nematic liquid crystals induced by charged particles.
  • To characterize novel defect structures, such as "ansa" defects.
  • To analyze the influence of dielectric anisotropy and particle charge on defect formation and particle alignment.

Main Methods:

  • Utilizing a Ginzburg-Landau theory framework.
  • Implementing numerical simulations with an inhomogeneous electric field.
  • Analyzing director orientation and free energy minimization.

Main Results:

  • Saturn-ring defects are observed for positive dielectric anisotropy (ε₁ > 0).
  • Novel "ansa" defects (disclination lines) appear for negative dielectric anisotropy (ε₁ < 0).
  • Oppositely charged particle pairs align parallel (ε₁ > 0) or perpendicular (ε₁ < 0) to the background director; identically charged pairs show reversed preferences.
  • Competition between charge-induced and short-range anchoring is examined, with long-range electrostatics dominating far from the surface.

Conclusions:

  • Charged particles induce distinct defect structures in nematic liquid crystals based on dielectric anisotropy.
  • The alignment of charged particle pairs is dictated by electrostatic interactions and dielectric properties.
  • Electrostatic interactions play a significant role in director orientation, especially in competition with surface anchoring effects.