Structure and Thermal Expansion of Cu−90 vol. % Graphite Composites

Copper–graphite composites are promising functional materials exhibiting application potential in electrical equipment and heat exchangers, due to their lower expansion coefficient and high electrical and thermal conductivities. Here, copper–graphite composites with 10–90 vol. % graphite were prepar...

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Autores principales: Andrej Opálek, Štefan Emmer, Roman Čička, Naďa Beronská, Peter Oslanec, Jaroslav Kováčik
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Publicado: MDPI AG 2021
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spelling oai:doaj.org-article:dfd62d18f8d1433e850a15026add9cb22021-11-25T18:16:17ZStructure and Thermal Expansion of Cu−90 vol. % Graphite Composites10.3390/ma142270891996-1944https://doaj.org/article/dfd62d18f8d1433e850a15026add9cb22021-11-01T00:00:00Zhttps://www.mdpi.com/1996-1944/14/22/7089https://doaj.org/toc/1996-1944Copper–graphite composites are promising functional materials exhibiting application potential in electrical equipment and heat exchangers, due to their lower expansion coefficient and high electrical and thermal conductivities. Here, copper–graphite composites with 10–90 vol. % graphite were prepared by hot isostatic pressing, and their microstructure and coefficient of thermal expansion (CTE) were experimentally examined. The CTE decreased with increasing graphite volume fraction, from 17.8 × 10<sup>−6</sup> K<sup>−1</sup> for HIPed pure copper to 4.9 × 10<sup>−6</sup> K<sup>−1</sup> for 90 vol. % graphite. In the HIPed pure copper, the presence of cuprous oxide was detected by SEM-EDS. In contrast, Cu–graphite composites contained only a very small amount of oxygen (OHN analysis). There was only one exception, the composite with 90 vol. % graphite contained around 1.8 wt. % water absorbed inside the structure. The internal stresses in the composites were released during the first heating cycle of the CTE measurement. The permanent prolongation and shape of CTE curves were strongly affected by composition. After the release of internal stresses, the CTE curves of composites did not change any further. Finally, the modified Schapery model, including anisotropy and the clustering of graphite, was used to model the dependence of CTE on graphite volume fraction. Modeling suggested that the clustering of graphite via van der Waals bonds (out of hexagonal plane) is the most critical parameter and significantly affects the microstructure and CTE of the Cu–graphite composites when more than 30 vol. % graphite is present.Andrej OpálekŠtefan EmmerRoman ČičkaNaďa BeronskáPeter OslanecJaroslav KováčikMDPI AGarticlemetal matrix compositeshot isostatic pressingthermal expansionSchapery modelTechnologyTElectrical engineering. Electronics. Nuclear engineeringTK1-9971Engineering (General). Civil engineering (General)TA1-2040MicroscopyQH201-278.5Descriptive and experimental mechanicsQC120-168.85ENMaterials, Vol 14, Iss 7089, p 7089 (2021)
institution DOAJ
collection DOAJ
language EN
topic metal matrix composites
hot isostatic pressing
thermal expansion
Schapery model
Technology
T
Electrical engineering. Electronics. Nuclear engineering
TK1-9971
Engineering (General). Civil engineering (General)
TA1-2040
Microscopy
QH201-278.5
Descriptive and experimental mechanics
QC120-168.85
spellingShingle metal matrix composites
hot isostatic pressing
thermal expansion
Schapery model
Technology
T
Electrical engineering. Electronics. Nuclear engineering
TK1-9971
Engineering (General). Civil engineering (General)
TA1-2040
Microscopy
QH201-278.5
Descriptive and experimental mechanics
QC120-168.85
Andrej Opálek
Štefan Emmer
Roman Čička
Naďa Beronská
Peter Oslanec
Jaroslav Kováčik
Structure and Thermal Expansion of Cu−90 vol. % Graphite Composites
description Copper–graphite composites are promising functional materials exhibiting application potential in electrical equipment and heat exchangers, due to their lower expansion coefficient and high electrical and thermal conductivities. Here, copper–graphite composites with 10–90 vol. % graphite were prepared by hot isostatic pressing, and their microstructure and coefficient of thermal expansion (CTE) were experimentally examined. The CTE decreased with increasing graphite volume fraction, from 17.8 × 10<sup>−6</sup> K<sup>−1</sup> for HIPed pure copper to 4.9 × 10<sup>−6</sup> K<sup>−1</sup> for 90 vol. % graphite. In the HIPed pure copper, the presence of cuprous oxide was detected by SEM-EDS. In contrast, Cu–graphite composites contained only a very small amount of oxygen (OHN analysis). There was only one exception, the composite with 90 vol. % graphite contained around 1.8 wt. % water absorbed inside the structure. The internal stresses in the composites were released during the first heating cycle of the CTE measurement. The permanent prolongation and shape of CTE curves were strongly affected by composition. After the release of internal stresses, the CTE curves of composites did not change any further. Finally, the modified Schapery model, including anisotropy and the clustering of graphite, was used to model the dependence of CTE on graphite volume fraction. Modeling suggested that the clustering of graphite via van der Waals bonds (out of hexagonal plane) is the most critical parameter and significantly affects the microstructure and CTE of the Cu–graphite composites when more than 30 vol. % graphite is present.
format article
author Andrej Opálek
Štefan Emmer
Roman Čička
Naďa Beronská
Peter Oslanec
Jaroslav Kováčik
author_facet Andrej Opálek
Štefan Emmer
Roman Čička
Naďa Beronská
Peter Oslanec
Jaroslav Kováčik
author_sort Andrej Opálek
title Structure and Thermal Expansion of Cu−90 vol. % Graphite Composites
title_short Structure and Thermal Expansion of Cu−90 vol. % Graphite Composites
title_full Structure and Thermal Expansion of Cu−90 vol. % Graphite Composites
title_fullStr Structure and Thermal Expansion of Cu−90 vol. % Graphite Composites
title_full_unstemmed Structure and Thermal Expansion of Cu−90 vol. % Graphite Composites
title_sort structure and thermal expansion of cu−90 vol. % graphite composites
publisher MDPI AG
publishDate 2021
url https://doaj.org/article/dfd62d18f8d1433e850a15026add9cb2
work_keys_str_mv AT andrejopalek structureandthermalexpansionofcu90volgraphitecomposites
AT stefanemmer structureandthermalexpansionofcu90volgraphitecomposites
AT romancicka structureandthermalexpansionofcu90volgraphitecomposites
AT nadaberonska structureandthermalexpansionofcu90volgraphitecomposites
AT peteroslanec structureandthermalexpansionofcu90volgraphitecomposites
AT jaroslavkovacik structureandthermalexpansionofcu90volgraphitecomposites
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