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Related Concept Videos

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....
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Properties of Transition Metals02:58

Properties of Transition Metals

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Transition metals are defined as those elements that have partially filled d orbitals. As shown in Figure 1, the d-block elements in groups 3–12 are transition elements. The f-block elements, also called inner transition metals (the lanthanides and actinides), also meet this criterion because the d orbital is partially occupied before the f orbitals.
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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
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Metallic bonds are formed between two metal atoms. A simplified model to describe metallic bonding has been developed by Paul Drüde called the “Electron Sea Model”. 
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Theory of Metallic Conduction01:17

Theory of Metallic Conduction

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The conduction of free electrons inside a conductor is best described by quantum mechanics. However, a classical model makes predictions close to the results of quantum mechanics. It is called the theory of metallic conduction.
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An electron moves through the crystal, containing positive ions,...
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Color in Coordination Complexes
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human...
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Cascade morphology transition in bcc metals.

Wahyu Setyawan1, Aaron P Selby, Niklas Juslin

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Summary
This summary is machine-generated.

Energetic atom collisions in solids show a morphological transition in defect production. This study defines a transition energy (μ) to compare different metals, presenting a formula for bcc metals based on displacement threshold energy (Ed).

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Area of Science:

  • Materials Science
  • Solid State Physics
  • Computational Materials Science

Background:

  • Energetic atom collisions in solids generate shockwaves with intricate structures.
  • Understanding defect production morphology is crucial for materials under extreme conditions.

Purpose of the Study:

  • To establish the existence of a morphological transition in energetic atom collision cascades.
  • To define a consistent energy domain for comparing defect production in different metals.
  • To develop an empirical formula for transition energy in bcc metals.

Main Methods:

  • Defining the morphological order parameter as the exponent 'b' in the defect production curve (N(F) ~ E(MD)(b)).
  • Normalizing cascade energy by the transition energy (μ) to compare different bcc metals (Cr, Fe, Mo, W).
  • Correlating transition energy (μ) with displacement threshold energy (Ed).

Main Results:

  • Demonstrated a morphological transition in defect production during energetic atom collisions.
  • Established a normalized energy domain for comparing defect responses across metals.
  • Presented an empirical formula for transition energy (μ) in bcc metals as a function of displacement threshold energy (Ed).

Conclusions:

  • The morphological transition provides a new parameter for characterizing defect cascades.
  • The normalized energy approach allows for consistent comparison of metal responses.
  • The derived formula aids in predicting transition energy for bcc metals based on fundamental properties.