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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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. |
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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.</description><identifier>ISSN: 0721-3115</identifier><identifier>EISSN: 1521-4087</identifier><identifier>DOI: 10.1002/prep.201300080</identifier><language>eng</language><publisher>Weinheim: WILEY-VCH Verlag</publisher><subject>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</subject><ispartof>Propellants, explosives, pyrotechnics, 2014-06, Vol.39 (3), p.365-373</ispartof><rights>2014 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim</rights><rights>2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim</rights><rights>Copyright Wiley Subscription Services, Inc. Jun 2014</rights><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c4900-65b567b1a48cf3cbc45e71419f972e6c17432d752eeeffec925bbee29587e9b33</citedby><cites>FETCH-LOGICAL-c4900-65b567b1a48cf3cbc45e71419f972e6c17432d752eeeffec925bbee29587e9b33</cites><orcidid>0000-0001-8862-5889 ; 0000-0003-3864-7574</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2Fprep.201300080$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2Fprep.201300080$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>230,314,780,784,885,1417,27924,27925,45574,45575</link.rule.ids><backlink>$$Uhttps://hal.science/hal-03464968$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Bahrami, Mehdi</creatorcontrib><creatorcontrib>Taton, Guillaume</creatorcontrib><creatorcontrib>Conédéra, Véronique</creatorcontrib><creatorcontrib>Salvagnac, Ludovic</creatorcontrib><creatorcontrib>Tenailleau, Christophe</creatorcontrib><creatorcontrib>Alphonse, Pierre</creatorcontrib><creatorcontrib>Rossi, Carole</creatorcontrib><title>Magnetron Sputtered Al-CuO Nanolaminates: Effect of Stoichiometry and Layers Thickness on Energy Release and Burning Rate</title><title>Propellants, explosives, pyrotechnics</title><addtitle>Propellants, Explosives, Pyrotechnics</addtitle><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.</description><subject>Al/CuO</subject><subject>Aluminum</subject><subject>Argon</subject><subject>Bilayers</subject><subject>Burning rate</subject><subject>CALORIMETRY</subject><subject>CHEMICAL PROPERTIES</subject><subject>Chemical Sciences</subject><subject>COPPER OXIDE</subject><subject>Copper oxides</subject><subject>Differential scanning calorimetry</subject><subject>Engineering Sciences</subject><subject>Gas mixtures</subject><subject>Heat of reaction</subject><subject>Heating rate</subject><subject>LAMINATES</subject><subject>Magnetron sputtering</subject><subject>Material chemistry</subject><subject>Materials</subject><subject>MICROSTRUCTURES</subject><subject>Nanoenergetics</subject><subject>Nanostructure</subject><subject>Nanothermites</subject><subject>Organic chemistry</subject><subject>Partial pressure</subject><subject>Photoelectrons</subject><subject>Reactive material</subject><subject>SPUTTERING</subject><subject>STOICHIOMETRY</subject><subject>Thickness</subject><subject>Transmission electron microscopy</subject><subject>X ray photoelectron spectroscopy</subject><subject>X RAY SPECTROSCOPY</subject><subject>X RAYS</subject><subject>X-ray diffraction</subject><issn>0721-3115</issn><issn>1521-4087</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNqFkUuP0zAURiPESJSBLWtLbGCR4mecsCtVmQF1HnQGjcTGctyb1jOpE-wEyL_HIahCLGBlyzrn-rv6kuQFwXOCMX3TemjnFBOGMc7xo2RGBCUpx7l8nMywjHdGiHiSPA3hHuOoYDJLhgu9c9D5xqGbtu868LBFizpd9lfoUrum1gfrdAfhLVpVFZgONRW66Rpr9rY5RHFA2m3RWg_gA7rdW_PgIAQU560c-N2ANlCDDvALe9d7Z90ObeLEZ8lJpesAz3-fp8nn96vb5Xm6vjr7sFysU8MLjNNMlCKTJdE8NxUzpeECJOGkqApJITNEcka3UlAAGAMWVJQlAC1ELqEoGTtNXk9z97pWrbcH7QfVaKvOF2s1vmHGM15k-TcS2VcT2_rmaw-hUwcbDNS1dtD0QREhCI5_kSyiL_9C75u4XdxEUYoLTokk-b8oIhgXnGfZGHE-UcY3IXiojjkJVmO3auxWHbuNQjEJ320Nw39odb1ZXf_pppNrQwc_jq72DyqTTAp1d3mm7vIv9BP_yFXOfgJ6y7W_</recordid><startdate>201406</startdate><enddate>201406</enddate><creator>Bahrami, Mehdi</creator><creator>Taton, Guillaume</creator><creator>Conédéra, Véronique</creator><creator>Salvagnac, Ludovic</creator><creator>Tenailleau, Christophe</creator><creator>Alphonse, Pierre</creator><creator>Rossi, Carole</creator><general>WILEY-VCH Verlag</general><general>WILEY‐VCH Verlag</general><general>Wiley Subscription Services, Inc</general><general>Wiley-VCH Verlag</general><scope>BSCLL</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7TB</scope><scope>8FD</scope><scope>FR3</scope><scope>H8D</scope><scope>L7M</scope><scope>7QF</scope><scope>H8G</scope><scope>JG9</scope><scope>1XC</scope><scope>VOOES</scope><orcidid>https://orcid.org/0000-0001-8862-5889</orcidid><orcidid>https://orcid.org/0000-0003-3864-7574</orcidid></search><sort><creationdate>201406</creationdate><title>Magnetron Sputtered Al-CuO Nanolaminates: Effect of Stoichiometry and Layers Thickness on Energy Release and Burning Rate</title><author>Bahrami, Mehdi ; Taton, Guillaume ; Conédéra, Véronique ; Salvagnac, Ludovic ; Tenailleau, Christophe ; Alphonse, Pierre ; Rossi, Carole</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c4900-65b567b1a48cf3cbc45e71419f972e6c17432d752eeeffec925bbee29587e9b33</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Al/CuO</topic><topic>Aluminum</topic><topic>Argon</topic><topic>Bilayers</topic><topic>Burning rate</topic><topic>CALORIMETRY</topic><topic>CHEMICAL PROPERTIES</topic><topic>Chemical Sciences</topic><topic>COPPER OXIDE</topic><topic>Copper oxides</topic><topic>Differential scanning calorimetry</topic><topic>Engineering Sciences</topic><topic>Gas mixtures</topic><topic>Heat of reaction</topic><topic>Heating rate</topic><topic>LAMINATES</topic><topic>Magnetron sputtering</topic><topic>Material chemistry</topic><topic>Materials</topic><topic>MICROSTRUCTURES</topic><topic>Nanoenergetics</topic><topic>Nanostructure</topic><topic>Nanothermites</topic><topic>Organic chemistry</topic><topic>Partial pressure</topic><topic>Photoelectrons</topic><topic>Reactive material</topic><topic>SPUTTERING</topic><topic>STOICHIOMETRY</topic><topic>Thickness</topic><topic>Transmission electron microscopy</topic><topic>X ray photoelectron spectroscopy</topic><topic>X RAY SPECTROSCOPY</topic><topic>X RAYS</topic><topic>X-ray diffraction</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Bahrami, Mehdi</creatorcontrib><creatorcontrib>Taton, Guillaume</creatorcontrib><creatorcontrib>Conédéra, Véronique</creatorcontrib><creatorcontrib>Salvagnac, Ludovic</creatorcontrib><creatorcontrib>Tenailleau, Christophe</creatorcontrib><creatorcontrib>Alphonse, Pierre</creatorcontrib><creatorcontrib>Rossi, Carole</creatorcontrib><collection>Istex</collection><collection>CrossRef</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Aluminium Industry Abstracts</collection><collection>Copper Technical Reference Library</collection><collection>Materials Research Database</collection><collection>Hyper Article en Ligne (HAL)</collection><collection>Hyper Article en Ligne (HAL) (Open Access)</collection><jtitle>Propellants, explosives, pyrotechnics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bahrami, Mehdi</au><au>Taton, Guillaume</au><au>Conédéra, Véronique</au><au>Salvagnac, Ludovic</au><au>Tenailleau, Christophe</au><au>Alphonse, Pierre</au><au>Rossi, Carole</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Magnetron Sputtered Al-CuO Nanolaminates: Effect of Stoichiometry and Layers Thickness on Energy Release and Burning Rate</atitle><jtitle>Propellants, explosives, pyrotechnics</jtitle><addtitle>Propellants, Explosives, Pyrotechnics</addtitle><date>2014-06</date><risdate>2014</risdate><volume>39</volume><issue>3</issue><spage>365</spage><epage>373</epage><pages>365-373</pages><issn>0721-3115</issn><eissn>1521-4087</eissn><abstract>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.</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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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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