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Metallic Solids02:37

Metallic Solids

21.6K
Metallic solids such as crystals of copper, aluminum, and iron are formed by metal atoms. The structure of metallic crystals is often described as a uniform distribution of atomic nuclei within a “sea” of delocalized electrons. The atoms within such a metallic solid are held together by a unique force known as metallic bonding that gives rise to many useful and varied bulk properties.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and...
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Ionic Crystal Structures02:42

Ionic Crystal Structures

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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...
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Lattice Centering and Coordination Number02:33

Lattice Centering and Coordination Number

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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...
16.3K
Structures of Solids02:22

Structures of Solids

22.5K
Solids in which the atoms, ions, or molecules are arranged in a definite repeating pattern are known as crystalline solids. Metals and ionic compounds typically form ordered, crystalline solids. A crystalline solid has a precise melting temperature because each atom or molecule of the same type is held in place with the same forces or energy. Amorphous solids or non-crystalline solids (or, sometimes, glasses) which lack an ordered internal structure and are randomly arranged. Substances that...
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Imperfections in Crystal Structure: Stoichiometric Point Defects01:26

Imperfections in Crystal Structure: Stoichiometric Point Defects

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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...
99
Imperfections in Crystal Structure: Non-Stoichiometric Defects01:29

Imperfections in Crystal Structure: Non-Stoichiometric Defects

99
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...
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Orientational Transition in a Liquid Crystal Triggered by the Thermodynamic Growth of Interfacial Wetting Sheets
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Orientational Transition in a Liquid Crystal Triggered by the Thermodynamic Growth of Interfacial Wetting Sheets

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Local structure order in Pd78Cu6Si16 liquid.

G Q Yue1, Y Zhang2, Y Sun2

  • 11] Shanghai Ultra-Precision Optical Manufacturing Engineering Center and Department of Optical Science and Engineering, Fudan University, Shanghai, 200433, China [2] Ames Laboratory, U. S. Department of Energy and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA.

Scientific Reports
|February 6, 2015
PubMed
Summary
This summary is machine-generated.

Short-range order in liquid palladium-copper-silicon (Pd78Cu6Si16) was investigated. Cooling increases icosahedral and face-centered cubic structures, with copper promoting glass formation.

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Area of Science:

  • Materials Science
  • Condensed Matter Physics
  • Computational Chemistry

Background:

  • Understanding short-range order (SRO) in liquid alloys is crucial for predicting material properties.
  • Palladium-copper-silicon (Pd-Cu-Si) alloys are of interest for their potential glass-forming abilities.

Purpose of the Study:

  • To investigate the short-range order (SRO) in the Pd78Cu6Si16 liquid alloy.
  • To elucidate the structural evolution and atomic arrangements upon cooling.

Main Methods:

  • High energy X-ray diffraction for experimental structural analysis.
  • Ab initio molecular dynamics (MD) simulations for theoretical modeling.
  • Structure analysis using Honeycutt-Andersen index, Voronoi tessellation, and atomic cluster alignment.

Main Results:

  • MD simulations accurately reproduced experimental pair correlation functions.
  • Silicon atoms exhibit uniform distribution, while copper atoms tend to aggregate.
  • Icosahedral and face-centered cubic SRO structures increase upon cooling.
  • A dominant Pd-centered Pd9Si2 motif, similar to crystalline structures, was identified.
  • Trigonal prism clusters, previously observed in Pd-based alloys, were confirmed.
  • Copper-centered clusters are predominantly icosahedral, suggesting a role in glass formation.

Conclusions:

  • The study provides detailed insights into the SRO of liquid Pd78Cu6Si16.
  • Copper addition appears to enhance the glass-forming ability of these alloys.
  • The findings contribute to the fundamental understanding of metallic glass structures.