Dislocation Structure Evolution in Low-Stability States of Solid Solutions of Alloys Under Their Deformation
The results of a study of the dislocation structure evolution in polycrystals of homogeneous solid solutions in low-stability states in Cu-Mn-based alloys with FCC crystal lattice are presented. It is found out that each stage is characterized by its own deformation carrier in the form of a certain...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Potekaev, A. I. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2022 |
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| Schlagwörter: |
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| Anmerkung: |
© Springer Science+Business Media, LLC, part of Springer Nature 2022 |
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| Übergeordnetes Werk: |
Enthalten in: Russian physics journal - New York, NY [u.a.] : Consultants Bureau, 1965, 65(2022), 1 vom: Mai, Seite 114-122 |
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| Übergeordnetes Werk: |
volume:65 ; year:2022 ; number:1 ; month:05 ; pages:114-122 |
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| DOI / URN: |
10.1007/s11182-022-02613-5 |
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SPR047808721 |
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| 520 | |a The results of a study of the dislocation structure evolution in polycrystals of homogeneous solid solutions in low-stability states in Cu-Mn-based alloys with FCC crystal lattice are presented. It is found out that each stage is characterized by its own deformation carrier in the form of a certain dislocation substructure (DSS), whose volume fraction has a maximum in this stage. At the same time, the deformation carrier of the previous stage gradually disappears as the strain degree (ε) increases in the current stage, and there appears a deformation carrier of the subsequent stage. In a certain range of ε values, the deformation carriers characteristic of the previous, current and subsequent stages coexist. It is shown that there are transitions from some types of DSS to other types in certain strain degree ε intervals. It is revealed that each deformation stage has its own DSS – deformation carriers. The stage-to-stage transition is accompanied by the formation of new deformation carriers, which is a characteristic feature of low-stability states of the system. Logically, this situation is observed because the study is carried out at a grain size involving a possibility of implementing a low-stability structural-phase state of the alloy, since in this case the grain size acts as a kind of a governing parameter. | ||
| 650 | 4 | |a dislocation structures |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a low-stability states |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a deformation carriers |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a dislocation substructures |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Cu-Mn alloys |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Klopotov, A. A. |4 aut | |
| 700 | 1 | |a Trishkina, L. I. |4 aut | |
| 700 | 1 | |a Cherkasova, T. V. |4 aut | |
| 700 | 1 | |a Kulagina, V. V. |4 aut | |
| 700 | 1 | |a Tazin, I. D. |4 aut | |
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10.1007/s11182-022-02613-5 doi (DE-627)SPR047808721 (SPR)s11182-022-02613-5-e DE-627 ger DE-627 rakwb eng Potekaev, A. I. verfasserin aut Dislocation Structure Evolution in Low-Stability States of Solid Solutions of Alloys Under Their Deformation 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2022 The results of a study of the dislocation structure evolution in polycrystals of homogeneous solid solutions in low-stability states in Cu-Mn-based alloys with FCC crystal lattice are presented. It is found out that each stage is characterized by its own deformation carrier in the form of a certain dislocation substructure (DSS), whose volume fraction has a maximum in this stage. At the same time, the deformation carrier of the previous stage gradually disappears as the strain degree (ε) increases in the current stage, and there appears a deformation carrier of the subsequent stage. In a certain range of ε values, the deformation carriers characteristic of the previous, current and subsequent stages coexist. It is shown that there are transitions from some types of DSS to other types in certain strain degree ε intervals. It is revealed that each deformation stage has its own DSS – deformation carriers. The stage-to-stage transition is accompanied by the formation of new deformation carriers, which is a characteristic feature of low-stability states of the system. Logically, this situation is observed because the study is carried out at a grain size involving a possibility of implementing a low-stability structural-phase state of the alloy, since in this case the grain size acts as a kind of a governing parameter. dislocation structures (dpeaa)DE-He213 low-stability states (dpeaa)DE-He213 deformation carriers (dpeaa)DE-He213 dislocation substructures (dpeaa)DE-He213 Cu-Mn alloys (dpeaa)DE-He213 Klopotov, A. A. aut Trishkina, L. I. aut Cherkasova, T. V. aut Kulagina, V. V. aut Tazin, I. D. aut Enthalten in Russian physics journal New York, NY [u.a.] : Consultants Bureau, 1965 65(2022), 1 vom: Mai, Seite 114-122 (DE-627)325572518 (DE-600)2037572-4 1573-9228 nnns volume:65 year:2022 number:1 month:05 pages:114-122 https://dx.doi.org/10.1007/s11182-022-02613-5 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 65 2022 1 05 114-122 |
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10.1007/s11182-022-02613-5 doi (DE-627)SPR047808721 (SPR)s11182-022-02613-5-e DE-627 ger DE-627 rakwb eng Potekaev, A. I. verfasserin aut Dislocation Structure Evolution in Low-Stability States of Solid Solutions of Alloys Under Their Deformation 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2022 The results of a study of the dislocation structure evolution in polycrystals of homogeneous solid solutions in low-stability states in Cu-Mn-based alloys with FCC crystal lattice are presented. It is found out that each stage is characterized by its own deformation carrier in the form of a certain dislocation substructure (DSS), whose volume fraction has a maximum in this stage. At the same time, the deformation carrier of the previous stage gradually disappears as the strain degree (ε) increases in the current stage, and there appears a deformation carrier of the subsequent stage. In a certain range of ε values, the deformation carriers characteristic of the previous, current and subsequent stages coexist. It is shown that there are transitions from some types of DSS to other types in certain strain degree ε intervals. It is revealed that each deformation stage has its own DSS – deformation carriers. The stage-to-stage transition is accompanied by the formation of new deformation carriers, which is a characteristic feature of low-stability states of the system. Logically, this situation is observed because the study is carried out at a grain size involving a possibility of implementing a low-stability structural-phase state of the alloy, since in this case the grain size acts as a kind of a governing parameter. dislocation structures (dpeaa)DE-He213 low-stability states (dpeaa)DE-He213 deformation carriers (dpeaa)DE-He213 dislocation substructures (dpeaa)DE-He213 Cu-Mn alloys (dpeaa)DE-He213 Klopotov, A. A. aut Trishkina, L. I. aut Cherkasova, T. V. aut Kulagina, V. V. aut Tazin, I. D. aut Enthalten in Russian physics journal New York, NY [u.a.] : Consultants Bureau, 1965 65(2022), 1 vom: Mai, Seite 114-122 (DE-627)325572518 (DE-600)2037572-4 1573-9228 nnns volume:65 year:2022 number:1 month:05 pages:114-122 https://dx.doi.org/10.1007/s11182-022-02613-5 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 65 2022 1 05 114-122 |
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10.1007/s11182-022-02613-5 doi (DE-627)SPR047808721 (SPR)s11182-022-02613-5-e DE-627 ger DE-627 rakwb eng Potekaev, A. I. verfasserin aut Dislocation Structure Evolution in Low-Stability States of Solid Solutions of Alloys Under Their Deformation 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2022 The results of a study of the dislocation structure evolution in polycrystals of homogeneous solid solutions in low-stability states in Cu-Mn-based alloys with FCC crystal lattice are presented. It is found out that each stage is characterized by its own deformation carrier in the form of a certain dislocation substructure (DSS), whose volume fraction has a maximum in this stage. At the same time, the deformation carrier of the previous stage gradually disappears as the strain degree (ε) increases in the current stage, and there appears a deformation carrier of the subsequent stage. In a certain range of ε values, the deformation carriers characteristic of the previous, current and subsequent stages coexist. It is shown that there are transitions from some types of DSS to other types in certain strain degree ε intervals. It is revealed that each deformation stage has its own DSS – deformation carriers. The stage-to-stage transition is accompanied by the formation of new deformation carriers, which is a characteristic feature of low-stability states of the system. Logically, this situation is observed because the study is carried out at a grain size involving a possibility of implementing a low-stability structural-phase state of the alloy, since in this case the grain size acts as a kind of a governing parameter. dislocation structures (dpeaa)DE-He213 low-stability states (dpeaa)DE-He213 deformation carriers (dpeaa)DE-He213 dislocation substructures (dpeaa)DE-He213 Cu-Mn alloys (dpeaa)DE-He213 Klopotov, A. A. aut Trishkina, L. I. aut Cherkasova, T. V. aut Kulagina, V. V. aut Tazin, I. D. aut Enthalten in Russian physics journal New York, NY [u.a.] : Consultants Bureau, 1965 65(2022), 1 vom: Mai, Seite 114-122 (DE-627)325572518 (DE-600)2037572-4 1573-9228 nnns volume:65 year:2022 number:1 month:05 pages:114-122 https://dx.doi.org/10.1007/s11182-022-02613-5 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 65 2022 1 05 114-122 |
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10.1007/s11182-022-02613-5 doi (DE-627)SPR047808721 (SPR)s11182-022-02613-5-e DE-627 ger DE-627 rakwb eng Potekaev, A. I. verfasserin aut Dislocation Structure Evolution in Low-Stability States of Solid Solutions of Alloys Under Their Deformation 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2022 The results of a study of the dislocation structure evolution in polycrystals of homogeneous solid solutions in low-stability states in Cu-Mn-based alloys with FCC crystal lattice are presented. It is found out that each stage is characterized by its own deformation carrier in the form of a certain dislocation substructure (DSS), whose volume fraction has a maximum in this stage. At the same time, the deformation carrier of the previous stage gradually disappears as the strain degree (ε) increases in the current stage, and there appears a deformation carrier of the subsequent stage. In a certain range of ε values, the deformation carriers characteristic of the previous, current and subsequent stages coexist. It is shown that there are transitions from some types of DSS to other types in certain strain degree ε intervals. It is revealed that each deformation stage has its own DSS – deformation carriers. The stage-to-stage transition is accompanied by the formation of new deformation carriers, which is a characteristic feature of low-stability states of the system. Logically, this situation is observed because the study is carried out at a grain size involving a possibility of implementing a low-stability structural-phase state of the alloy, since in this case the grain size acts as a kind of a governing parameter. dislocation structures (dpeaa)DE-He213 low-stability states (dpeaa)DE-He213 deformation carriers (dpeaa)DE-He213 dislocation substructures (dpeaa)DE-He213 Cu-Mn alloys (dpeaa)DE-He213 Klopotov, A. A. aut Trishkina, L. I. aut Cherkasova, T. V. aut Kulagina, V. V. aut Tazin, I. D. aut Enthalten in Russian physics journal New York, NY [u.a.] : Consultants Bureau, 1965 65(2022), 1 vom: Mai, Seite 114-122 (DE-627)325572518 (DE-600)2037572-4 1573-9228 nnns volume:65 year:2022 number:1 month:05 pages:114-122 https://dx.doi.org/10.1007/s11182-022-02613-5 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 65 2022 1 05 114-122 |
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10.1007/s11182-022-02613-5 doi (DE-627)SPR047808721 (SPR)s11182-022-02613-5-e DE-627 ger DE-627 rakwb eng Potekaev, A. I. verfasserin aut Dislocation Structure Evolution in Low-Stability States of Solid Solutions of Alloys Under Their Deformation 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2022 The results of a study of the dislocation structure evolution in polycrystals of homogeneous solid solutions in low-stability states in Cu-Mn-based alloys with FCC crystal lattice are presented. It is found out that each stage is characterized by its own deformation carrier in the form of a certain dislocation substructure (DSS), whose volume fraction has a maximum in this stage. At the same time, the deformation carrier of the previous stage gradually disappears as the strain degree (ε) increases in the current stage, and there appears a deformation carrier of the subsequent stage. In a certain range of ε values, the deformation carriers characteristic of the previous, current and subsequent stages coexist. It is shown that there are transitions from some types of DSS to other types in certain strain degree ε intervals. It is revealed that each deformation stage has its own DSS – deformation carriers. The stage-to-stage transition is accompanied by the formation of new deformation carriers, which is a characteristic feature of low-stability states of the system. Logically, this situation is observed because the study is carried out at a grain size involving a possibility of implementing a low-stability structural-phase state of the alloy, since in this case the grain size acts as a kind of a governing parameter. dislocation structures (dpeaa)DE-He213 low-stability states (dpeaa)DE-He213 deformation carriers (dpeaa)DE-He213 dislocation substructures (dpeaa)DE-He213 Cu-Mn alloys (dpeaa)DE-He213 Klopotov, A. A. aut Trishkina, L. I. aut Cherkasova, T. V. aut Kulagina, V. V. aut Tazin, I. D. aut Enthalten in Russian physics journal New York, NY [u.a.] : Consultants Bureau, 1965 65(2022), 1 vom: Mai, Seite 114-122 (DE-627)325572518 (DE-600)2037572-4 1573-9228 nnns volume:65 year:2022 number:1 month:05 pages:114-122 https://dx.doi.org/10.1007/s11182-022-02613-5 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 65 2022 1 05 114-122 |
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Potekaev, A. I. @@aut@@ Klopotov, A. A. @@aut@@ Trishkina, L. I. @@aut@@ Cherkasova, T. V. @@aut@@ Kulagina, V. V. @@aut@@ Tazin, I. D. @@aut@@ |
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I.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Dislocation Structure Evolution in Low-Stability States of Solid Solutions of Alloys Under Their Deformation</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2022</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Springer Science+Business Media, LLC, part of Springer Nature 2022</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">The results of a study of the dislocation structure evolution in polycrystals of homogeneous solid solutions in low-stability states in Cu-Mn-based alloys with FCC crystal lattice are presented. 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Potekaev, A. I. |
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Potekaev, A. I. misc dislocation structures misc low-stability states misc deformation carriers misc dislocation substructures misc Cu-Mn alloys Dislocation Structure Evolution in Low-Stability States of Solid Solutions of Alloys Under Their Deformation |
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Dislocation Structure Evolution in Low-Stability States of Solid Solutions of Alloys Under Their Deformation dislocation structures (dpeaa)DE-He213 low-stability states (dpeaa)DE-He213 deformation carriers (dpeaa)DE-He213 dislocation substructures (dpeaa)DE-He213 Cu-Mn alloys (dpeaa)DE-He213 |
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dislocation structure evolution in low-stability states of solid solutions of alloys under their deformation |
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Dislocation Structure Evolution in Low-Stability States of Solid Solutions of Alloys Under Their Deformation |
| abstract |
The results of a study of the dislocation structure evolution in polycrystals of homogeneous solid solutions in low-stability states in Cu-Mn-based alloys with FCC crystal lattice are presented. It is found out that each stage is characterized by its own deformation carrier in the form of a certain dislocation substructure (DSS), whose volume fraction has a maximum in this stage. At the same time, the deformation carrier of the previous stage gradually disappears as the strain degree (ε) increases in the current stage, and there appears a deformation carrier of the subsequent stage. In a certain range of ε values, the deformation carriers characteristic of the previous, current and subsequent stages coexist. It is shown that there are transitions from some types of DSS to other types in certain strain degree ε intervals. It is revealed that each deformation stage has its own DSS – deformation carriers. The stage-to-stage transition is accompanied by the formation of new deformation carriers, which is a characteristic feature of low-stability states of the system. Logically, this situation is observed because the study is carried out at a grain size involving a possibility of implementing a low-stability structural-phase state of the alloy, since in this case the grain size acts as a kind of a governing parameter. © Springer Science+Business Media, LLC, part of Springer Nature 2022 |
| abstractGer |
The results of a study of the dislocation structure evolution in polycrystals of homogeneous solid solutions in low-stability states in Cu-Mn-based alloys with FCC crystal lattice are presented. It is found out that each stage is characterized by its own deformation carrier in the form of a certain dislocation substructure (DSS), whose volume fraction has a maximum in this stage. At the same time, the deformation carrier of the previous stage gradually disappears as the strain degree (ε) increases in the current stage, and there appears a deformation carrier of the subsequent stage. In a certain range of ε values, the deformation carriers characteristic of the previous, current and subsequent stages coexist. It is shown that there are transitions from some types of DSS to other types in certain strain degree ε intervals. It is revealed that each deformation stage has its own DSS – deformation carriers. The stage-to-stage transition is accompanied by the formation of new deformation carriers, which is a characteristic feature of low-stability states of the system. Logically, this situation is observed because the study is carried out at a grain size involving a possibility of implementing a low-stability structural-phase state of the alloy, since in this case the grain size acts as a kind of a governing parameter. © Springer Science+Business Media, LLC, part of Springer Nature 2022 |
| abstract_unstemmed |
The results of a study of the dislocation structure evolution in polycrystals of homogeneous solid solutions in low-stability states in Cu-Mn-based alloys with FCC crystal lattice are presented. It is found out that each stage is characterized by its own deformation carrier in the form of a certain dislocation substructure (DSS), whose volume fraction has a maximum in this stage. At the same time, the deformation carrier of the previous stage gradually disappears as the strain degree (ε) increases in the current stage, and there appears a deformation carrier of the subsequent stage. In a certain range of ε values, the deformation carriers characteristic of the previous, current and subsequent stages coexist. It is shown that there are transitions from some types of DSS to other types in certain strain degree ε intervals. It is revealed that each deformation stage has its own DSS – deformation carriers. The stage-to-stage transition is accompanied by the formation of new deformation carriers, which is a characteristic feature of low-stability states of the system. Logically, this situation is observed because the study is carried out at a grain size involving a possibility of implementing a low-stability structural-phase state of the alloy, since in this case the grain size acts as a kind of a governing parameter. © Springer Science+Business Media, LLC, part of Springer Nature 2022 |
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Dislocation Structure Evolution in Low-Stability States of Solid Solutions of Alloys Under Their Deformation |
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https://dx.doi.org/10.1007/s11182-022-02613-5 |
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Klopotov, A. A. Trishkina, L. I. Cherkasova, T. V. Kulagina, V. V. Tazin, I. D. |
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Klopotov, A. A. Trishkina, L. I. Cherkasova, T. V. Kulagina, V. V. Tazin, I. D. |
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| score |
7.399289 |