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Related Concept Videos

Metallic Solids02:37

Metallic Solids

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. Many...
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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...
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...

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Determining the Mechanical Strength of Ultra-Fine-Grained Metals
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Dislocations in nanostructured two-phase Fe30Ni20Mn20Al30.

X Wu1, I Baker

  • 1Thayer School of Engineering, Dartmouth College, Hanover, New Hampshire 03755-8000, USA.

Microscopy Research and Technique
|January 22, 2013
PubMed
Summary

Dislocations in Fe-Ni-Mn-Al alloys exhibit different slip behaviors. At high temperatures, slip occurs via a<100> dislocations in the B2 phase, contrasting previous findings at room temperature.

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Area of Science:

  • Materials Science
  • Metallurgy
  • Solid Mechanics

Background:

  • Previous research identified a/2<111> Burgers vectors for dislocations in Fe30Ni20Mn25Al25 at room temperature.
  • Dislocations in the previous study glided in pairs on {110} and {112} planes, uncoupled in the b.c.c. phase and connected by an anti-phase boundary in the B2 phase.

Purpose of the Study:

  • To analyze dislocation behavior in the B2 phases of a related two-phase alloy, Fe30Ni20Mn20Al30, at elevated temperatures.
  • To investigate the slip vector of dislocations in Fe-Ni-Mn-Al alloys under specific high-temperature deformation conditions.

Main Methods:

  • Compression testing of Fe30Ni20Mn20Al30 alloy at 873 K with a strain rate of 5 × 10⁻⁴ s⁻¹.
  • Analysis of dislocation structures and slip vectors within the B2 phases of the alloy post-deformation.

Main Results:

  • Slip in the ~5 nm-wide B2 phases of Fe30Ni20Mn20Al30 occurs via the glide of a<100> dislocations.
  • Observed slip vector differs from the a/2<111> Burgers vectors reported for room temperature deformation in a similar alloy.

Conclusions:

  • The study demonstrates a shift in dislocation glide mechanism to a<100> dislocations in the B2 phase at 873 K.
  • Differences in composition and/or deformation temperature are suggested as potential reasons for the observed variation in slip vectors between different B2 phases and deformation conditions.