Magnetron Sputtered Al-CuO Nanolaminates: Effect of Stoichiometry and Layers Thickness on Energy Release and Burning Rate

This paper reports on the reaction characteristic of Al/CuO reactive nanolaminates for different stoichiometries and bilayer thicknesses. Al/CuO nanolaminates are deposited by a DC reactive magnetron sputtering method. Pure Al and Cu targets are used in argon‐oxygen gas mixture plasma and an oxygen...

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Veröffentlicht in:Propellants, explosives, pyrotechnics explosives, pyrotechnics, 2014-06, Vol.39 (3), p.365-373
Hauptverfasser: Bahrami, Mehdi, Taton, Guillaume, Conédéra, Véronique, Salvagnac, Ludovic, Tenailleau, Christophe, Alphonse, Pierre, Rossi, Carole
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container_end_page 373
container_issue 3
container_start_page 365
container_title Propellants, explosives, pyrotechnics
container_volume 39
creator Bahrami, Mehdi
Taton, Guillaume
Conédéra, Véronique
Salvagnac, Ludovic
Tenailleau, Christophe
Alphonse, Pierre
Rossi, Carole
description This paper reports on the reaction characteristic of Al/CuO reactive nanolaminates for different stoichiometries and bilayer thicknesses. Al/CuO nanolaminates are deposited by a DC reactive magnetron sputtering method. Pure Al and Cu targets are used in argon‐oxygen gas mixture plasma and an oxygen partial pressure of 0.13 Pa. This process produces low stress multilayered materials, each layer being in the range of 25 nanometers to one micrometer. Their structural, morphological, and chemical properties were characterized by high resolution transmission electron microscopy (HR‐TEM), X‐ray Diffraction (XRD), and X‐ray photoelectron spectroscopy (XPS). The heat of reaction and onset temperature were measured using differential scanning calorimetry (DSC). Under stoichiometric conditions, the reactivity quickly increases with the decrease of Al/CuO bilayer thickness. The burning rate is 2 m s−1 for bilayer thickness of 1.5 μm and reaches 80 m s−1 for bilayer thickness of 150 nm. At constant heating rate, the Al/CuO heat of reaction depends on both stoichiometry and bilayer thickness. When the bilayer thickness exceeds 300 nm, the heat of reaction decreases; it seems that only the region near the interface reacts. The best nanolaminate configuration was obtained for Al/CuO bilayer thickness of 150 nm.
doi_str_mv 10.1002/prep.201300080
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Al/CuO nanolaminates are deposited by a DC reactive magnetron sputtering method. Pure Al and Cu targets are used in argon‐oxygen gas mixture plasma and an oxygen partial pressure of 0.13 Pa. This process produces low stress multilayered materials, each layer being in the range of 25 nanometers to one micrometer. Their structural, morphological, and chemical properties were characterized by high resolution transmission electron microscopy (HR‐TEM), X‐ray Diffraction (XRD), and X‐ray photoelectron spectroscopy (XPS). The heat of reaction and onset temperature were measured using differential scanning calorimetry (DSC). Under stoichiometric conditions, the reactivity quickly increases with the decrease of Al/CuO bilayer thickness. The burning rate is 2 m s−1 for bilayer thickness of 1.5 μm and reaches 80 m s−1 for bilayer thickness of 150 nm. At constant heating rate, the Al/CuO heat of reaction depends on both stoichiometry and bilayer thickness. When the bilayer thickness exceeds 300 nm, the heat of reaction decreases; it seems that only the region near the interface reacts. 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When the bilayer thickness exceeds 300 nm, the heat of reaction decreases; it seems that only the region near the interface reacts. 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Al/CuO nanolaminates are deposited by a DC reactive magnetron sputtering method. Pure Al and Cu targets are used in argon‐oxygen gas mixture plasma and an oxygen partial pressure of 0.13 Pa. This process produces low stress multilayered materials, each layer being in the range of 25 nanometers to one micrometer. Their structural, morphological, and chemical properties were characterized by high resolution transmission electron microscopy (HR‐TEM), X‐ray Diffraction (XRD), and X‐ray photoelectron spectroscopy (XPS). The heat of reaction and onset temperature were measured using differential scanning calorimetry (DSC). Under stoichiometric conditions, the reactivity quickly increases with the decrease of Al/CuO bilayer thickness. The burning rate is 2 m s−1 for bilayer thickness of 1.5 μm and reaches 80 m s−1 for bilayer thickness of 150 nm. At constant heating rate, the Al/CuO heat of reaction depends on both stoichiometry and bilayer thickness. When the bilayer thickness exceeds 300 nm, the heat of reaction decreases; it seems that only the region near the interface reacts. The best nanolaminate configuration was obtained for Al/CuO bilayer thickness of 150 nm.</abstract><cop>Weinheim</cop><pub>WILEY-VCH Verlag</pub><doi>10.1002/prep.201300080</doi><tpages>9</tpages><orcidid>https://orcid.org/0000-0001-8862-5889</orcidid><orcidid>https://orcid.org/0000-0003-3864-7574</orcidid><oa>free_for_read</oa></addata></record>
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1521-4087
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subjects Al/CuO
Aluminum
Argon
Bilayers
Burning rate
CALORIMETRY
CHEMICAL PROPERTIES
Chemical Sciences
COPPER OXIDE
Copper oxides
Differential scanning calorimetry
Engineering Sciences
Gas mixtures
Heat of reaction
Heating rate
LAMINATES
Magnetron sputtering
Material chemistry
Materials
MICROSTRUCTURES
Nanoenergetics
Nanostructure
Nanothermites
Organic chemistry
Partial pressure
Photoelectrons
Reactive material
SPUTTERING
STOICHIOMETRY
Thickness
Transmission electron microscopy
X ray photoelectron spectroscopy
X RAY SPECTROSCOPY
X RAYS
X-ray diffraction
title Magnetron Sputtered Al-CuO Nanolaminates: Effect of Stoichiometry and Layers Thickness on Energy Release and Burning Rate
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