Related Experiment Video
Updated: Apr 27, 2026

05:04
Determining the Mechanical Strength of Ultra-Fine-Grained Metals
Published on: November 22, 2021
1.7K
High-strength and high-ductility nanostructured and amorphous metallic materials
Hongning Kou1, Jian Lu, Ying Li
1Department of Mechanical and Biomedical Engineering, City University of Hong Kong, Tae Chee Avenue, Kowloon, Hong Kong, China.
Advanced Materials (Deerfield Beach, Fla.)
|July 1, 2014
Summary
Advanced nanomaterials and metallic glasses achieve high strength and ductility through multiscale heterogeneities. These materials offer an extraordinary balance of yield strength and uniform elongation, overcoming traditional trade-offs.
Area of Science:
- Materials Science
- Nanotechnology
- Mechanical Engineering
Background:
- Achieving materials with both high strength and high ductility is a long-standing challenge in materials science.
- Nanotechnology advancements have opened new avenues for developing materials with superior mechanical properties.
Purpose of the Study:
- To highlight novel strategies for optimizing advanced nanomaterials and metallic glasses.
- To present the concept of strain non-localization for ductility enhancement.
Main Methods:
- Reviewing newly developed strategies for advanced nanomaterials and metallic glasses.
- Presenting the concept of multiscale heterogeneities (macro, micro, nano, atomic scales).
Main Results:
- Identified strategies to optimize nanomaterials and metallic glasses for dual high strength and ductility.
- Demonstrated the role of multiscale heterogeneities in enhancing ductility of intrinsically brittle materials.
- Highlighted a new class of nanomaterials with an exceptional yield strength-uniform elongation relationship.
Conclusions:
- Multiscale heterogeneities are key to achieving high strength and ductility in advanced materials.
- Nanostructured metallic materials and bulk metallic glasses represent a promising new class of high-performance materials.
- Further research into nanoprecipitate-reinforced nanomaterials shows potential for exceptional mechanical properties.
Related Concept Videos
Metallic Solids
16.4K
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...
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and...
16.4K
Bonding in Metals
45.1K
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”.
45.1K
Network Covalent Solids
12.9K
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...
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...
12.9K
Stress-Strain Diagram - Ductile Materials
2.5K
The stress-strain relationship in ductile materials such as structural steel or aluminium is intricate and progresses through several stages. When a specimen is loaded, it initially exhibits a linear length increase, depicted by a steep straight line on the stress-strain diagram. It indicates the material is elastically deforming and will return to its original shape once unloaded. However, when a critical stress value is reached, plastic deformation begins. This stage sees substantial...
2.5K

