Related Experiment Video
Updated: Mar 19, 2026

09:50
Preparation and Reactivity of Gasless Nanostructured Energetic Materials
Published on: April 2, 2015
10.7K
Intermetallic reaction and eutectic transitions tune the reactivity in core-shell Mg/Ni nanoparticles
Mahbub Chowdhury1, Lei Yang1, Brandon Wagner2
1Departments of Chemical Engineering and Materials Science, University of California, Riverside, California 92521, USA. mrz@engr.ucr.edu.
Physical Chemistry Chemical Physics : PCCP
|March 18, 2026
Summary
Researchers tuned nickel-coated magnesium nanoparticles to enhance energetic materials. Adjusting the nickel shell thickness lowered ignition temperatures by up to 200 °C, improving safety and energy release control.
Area of Science:
- Materials Science
- Nanotechnology
- Chemical Engineering
Background:
- Energetic materials require interface tuning for performance and safety.
- Core-shell architectures can trigger pre-ignition reactions in metallic fuels.
Purpose of the Study:
- Investigate dynamic interfacial reactions and diffusion in nickel-coated magnesium nanoparticles.
- Understand how core-shell structure affects energetic material properties.
- Develop strategies for safer energetic materials with controlled energy release.
Main Methods:
- Synthesized nickel-coated magnesium nanoparticles.
- Utilized in situ transmission electron microscopy (TEM) for real-time observation.
- Employed ex situ reactivity characterization.
- Analyzed interfacial reactions and diffusion pathways under controlled heating.
Main Results:
- Observed outward diffusion of magnesium (Mg) into the nickel (Ni) shell, forming Mg2Ni.
- Exothermic alloying rapidly increased particle temperature and initiated eutectic melting.
- Achieved accelerated Mg transport at lower temperatures compared to uncoated Mg.
- Reduced ignition temperature by up to ~200 °C by tuning Ni-shell thickness.
Conclusions:
- Core-shell architecture significantly influences energetic material behavior.
- Tuning shell thickness offers a method to control ignition temperature and enhance safety.
- Provides insights for designing advanced energetic materials with tailored energy release.
Related Concept Videos
Properties of Transition Metals
30.6K
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.
30.6K
Bonding in Metals
55.6K
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”.
55.6K
Theory of Metallic Conduction
1.9K
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.
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
1.9K
Metallic Solids
21.3K
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....
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
21.3K
Ferromagnetism
3.4K
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
3.4K

