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Metallic Solids02:37

Metallic Solids

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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 malleability....
18.2K
Network Covalent Solids02:18

Network Covalent Solids

13.3K
Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
13.3K
Crystal Field Theory - Octahedral Complexes02:58

Crystal Field Theory - Octahedral Complexes

26.1K
Crystal Field Theory
To explain the observed behavior of transition metal complexes (such as colors), a model involving electrostatic interactions between the electrons from the ligands and the electrons in the unhybridized d orbitals of the central metal atom has been developed. This electrostatic model is crystal field theory (CFT). It helps to understand, interpret, and predict the colors, magnetic behavior, and some structures of coordination compounds of transition metals.
CFT focuses on...
26.1K
Crystal Field Theory - Tetrahedral and Square Planar Complexes02:46

Crystal Field Theory - Tetrahedral and Square Planar Complexes

41.4K
Tetrahedral Complexes
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...
41.4K
Lattice Centering and Coordination Number02:33

Lattice Centering and Coordination Number

9.5K
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...
9.5K
Conformations of Cyclohexane02:11

Conformations of Cyclohexane

12.1K
Cyclohexane does not exist in a planar form due to the high angle and torsional strain it would experience in the planar structure. Instead, it adopts non-planar chair and boat conformations.
The chair form is the most stable and derives its name from its resemblance to the “easy chair.” In the chair conformation, two carbon atoms are arranged out-of-plane — one above and one below, minimizing the torsional strain. In the chair form, the bond angle is very close to the ideal...
12.1K

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Updated: Jun 3, 2025

Characterization of Ultra-fine Grained and Nanocrystalline Materials Using Transmission Kikuchi Diffraction
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Characterization of Ultra-fine Grained and Nanocrystalline Materials Using Transmission Kikuchi Diffraction

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Clave para la formación hexagonal de diamantes: estudio teórico y experimental

Sheng-Cai Zhu1, Gu-Wen Chen1, Xiao-Hong Yuan2

  • 1School of Materials, Shenzhen Campus of Sun Yat-sen University, Shenzhen 518107, China.

Journal of the American Chemical Society
|January 6, 2025
PubMed
Resumen

Los científicos sintetizaron el diamante hexagonal (HD) simulando las transformaciones del grafito bajo condiciones específicas de presión y temperatura. Este avance aclara el mecanismo de formación y guía la síntesis futura de este material ultraduro.

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Área de la Ciencia:

  • Ciencias de los materiales
  • Física de la materia condensada
  • La cristalografía

Sus antecedentes:

  • El diamante hexagonal (HD), conocido por su dureza superior, ha sido difícil de sintetizar puramente bajo condiciones de alta presión y alta temperatura (HPHT).
  • Comprender el mecanismo de formación de grafito a diamante es crucial para una síntesis exitosa de HD.

Objetivo del estudio:

  • Para aclarar el mecanismo de formación del diamante hexagonal (HD) a partir del grafito.
  • Identificar las condiciones específicas requeridas para la síntesis de HD puro frente al diamante cúbico (CD).
  • Para guiar nuevas estrategias de síntesis para la EH.

Principales métodos:

  • Simulaciones dinámicas moleculares sistemáticas para observar la transición del grafito al HD.
  • Experimentos controlados a alta presión y temperatura (HPHT) para validar los resultados de las simulaciones.

Principales resultados:

  • Observación directa de un mecanismo de crecimiento de la nucleación para la transición de grafito a HD.
  • La formación de HD favorecida bajo compresión cuasi uniaxial con alta tensión a lo largo de la dirección del grafito y temperaturas suaves.
  • Formación de diamante cúbico (CD) favorecida cuando el apilamiento de la capa AB del grafito se destruye o se desliza libremente a temperaturas más altas.

Conclusiones:

  • Se han aclarado los mecanismos controlados por presión y temperatura que rigen las transiciones de grafito a diamante.
  • Se ha demostrado la síntesis exitosa de la EH en condiciones casi uniaxiales, validando las predicciones teóricas.
  • Propuso un nuevo enfoque para la síntesis de HD controlando el apilamiento del plano basal del grafito y el deslizamiento de la capa.