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Length Changes of Unconfined Nb$_3$Sn Rutherford Cables During Reaction Heat Treatment
In order to predict volume changes of Nb$_3$Sn coils during reaction heat treatment (RHT), coefficients of thermal expansion (CTE) of the involved materials need to be known. While the CTEs of bulk materials are widely available, there is a lack of knowledge about the dimensional changes of the Nb$_...
Autores principales: | , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2019
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1109/TASC.2019.2897104 http://cds.cern.ch/record/2759038 |
_version_ | 1780970294552297472 |
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author | Michels, Matthias Lackner, Friedrich Scheuerlein, Christian Carlon Zurita, Alejandro Ferradas Troitino, Salvador Bourcey, Nicolas Savary, Frederic Tommasini, Davide |
author_facet | Michels, Matthias Lackner, Friedrich Scheuerlein, Christian Carlon Zurita, Alejandro Ferradas Troitino, Salvador Bourcey, Nicolas Savary, Frederic Tommasini, Davide |
author_sort | Michels, Matthias |
collection | CERN |
description | In order to predict volume changes of Nb$_3$Sn coils during reaction heat treatment (RHT), coefficients of thermal expansion (CTE) of the involved materials need to be known. While the CTEs of bulk materials are widely available, there is a lack of knowledge about the dimensional changes of the Nb$_3$Sn Rutherford cables. By extensometry we have measured the length changes of 11 T dipole Nb$_3$Sn Rutherford cables during the RHT. Similar to the length change behavior of multifilament wires, after an initial cable length increase the cable length decreases when the temperature exceeds about 150°C, due to relaxation of the Nb subelements when the Cu matrix is annealed. At higher temperatures the cable length increase is determined by the CTE of the unreacted Nb, before the onset of Nb$_3$Sn formation leads to an increased expansion rate. During cooling, the thermal contraction of fully reacted Nb$_3$Sn cable is similar to that of Nb$_3$Sn bulk. |
id | oai-inspirehep.net-1850484 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2019 |
record_format | invenio |
spelling | oai-inspirehep.net-18504842021-06-21T13:25:29Zdoi:10.1109/TASC.2019.2897104http://cds.cern.ch/record/2759038engMichels, MatthiasLackner, FriedrichScheuerlein, ChristianCarlon Zurita, AlejandroFerradas Troitino, SalvadorBourcey, NicolasSavary, FredericTommasini, DavideLength Changes of Unconfined Nb$_3$Sn Rutherford Cables During Reaction Heat TreatmentAccelerators and Storage RingsIn order to predict volume changes of Nb$_3$Sn coils during reaction heat treatment (RHT), coefficients of thermal expansion (CTE) of the involved materials need to be known. While the CTEs of bulk materials are widely available, there is a lack of knowledge about the dimensional changes of the Nb$_3$Sn Rutherford cables. By extensometry we have measured the length changes of 11 T dipole Nb$_3$Sn Rutherford cables during the RHT. Similar to the length change behavior of multifilament wires, after an initial cable length increase the cable length decreases when the temperature exceeds about 150°C, due to relaxation of the Nb subelements when the Cu matrix is annealed. At higher temperatures the cable length increase is determined by the CTE of the unreacted Nb, before the onset of Nb$_3$Sn formation leads to an increased expansion rate. During cooling, the thermal contraction of fully reacted Nb$_3$Sn cable is similar to that of Nb$_3$Sn bulk.In order to predict volume changes of Nb3Sn coils during reaction heat treatment (RHT), coefficients of thermal expansion (CTE) of the involved materials need to be known. While the CTEs of bulk materials are widely available, there is a lack of knowledge about the dimensional changes of the Nb3Sn Rutherford cables. By extensometry we have measured the length changes of 11 T dipole Nb3Sn Rutherford cables during the RHT. Similar to the length change behavior of multifilament wires, after an initial cable length increase the cable length decreases when the temperature exceeds about 150 °C, due to relaxation of the Nb subelements when the Cu matrix is annealed. At higher temperatures the cable length increase is determined by the CTE of the unreacted Nb, before the onset of Nb3Sn formation leads to an increased expansion rate. During cooling, the thermal contraction of fully reacted Nb3Sn cable is similar to that of Nb3Sn bulk.oai:inspirehep.net:18504842019 |
spellingShingle | Accelerators and Storage Rings Michels, Matthias Lackner, Friedrich Scheuerlein, Christian Carlon Zurita, Alejandro Ferradas Troitino, Salvador Bourcey, Nicolas Savary, Frederic Tommasini, Davide Length Changes of Unconfined Nb$_3$Sn Rutherford Cables During Reaction Heat Treatment |
title | Length Changes of Unconfined Nb$_3$Sn Rutherford Cables During Reaction Heat Treatment |
title_full | Length Changes of Unconfined Nb$_3$Sn Rutherford Cables During Reaction Heat Treatment |
title_fullStr | Length Changes of Unconfined Nb$_3$Sn Rutherford Cables During Reaction Heat Treatment |
title_full_unstemmed | Length Changes of Unconfined Nb$_3$Sn Rutherford Cables During Reaction Heat Treatment |
title_short | Length Changes of Unconfined Nb$_3$Sn Rutherford Cables During Reaction Heat Treatment |
title_sort | length changes of unconfined nb$_3$sn rutherford cables during reaction heat treatment |
topic | Accelerators and Storage Rings |
url | https://dx.doi.org/10.1109/TASC.2019.2897104 http://cds.cern.ch/record/2759038 |
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