Microstructure of iron and low-carbon steel after pulse loading
Conclusions The deformation mechanism in pulse loading differs from all other types in static and dynamic loading and consists in the formation of a mosaic structure without plastic flow of the grains.Plastic flow occurs during pulse loading when the movement of the piece is restrained or as the res...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Shishkova, A. P. [verfasserIn] |
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| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1969 |
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| Schlagwörter: |
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| Anmerkung: |
© Consultants Bureau 1969 |
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| Übergeordnetes Werk: |
Enthalten in: Metal science and heat treatment - Kluwer Academic Publishers-Plenum Publishers, 1959, 11(1969), 4 vom: Apr., Seite 325-326 |
|---|---|
| Übergeordnetes Werk: |
volume:11 ; year:1969 ; number:4 ; month:04 ; pages:325-326 |
| Links: |
|---|
| DOI / URN: |
10.1007/BF00653209 |
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OLC2047988756 |
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| 520 | |a Conclusions The deformation mechanism in pulse loading differs from all other types in static and dynamic loading and consists in the formation of a mosaic structure without plastic flow of the grains.Plastic flow occurs during pulse loading when the movement of the piece is restrained or as the result of the interaction of structurally heterogeneous zones during pulse loading.The hardening resulting from pulse loading exceeds that resulting from ordinary plastic deformation. The hardness is highest when a mosaic structure is formed and amounts to approximately 150–250% of the initial values.The principal factors influencing the structure and properties of the material after pulse loading are the loading velocity and the shape of the sample.At the critical percentage of mosaic structure, pores are formed. Fracture occurs when the propagation rate of the pores exceeds the rate at which the load is removed. | ||
| 650 | 4 | |a Iron | |
| 650 | 4 | |a Microstructure | |
| 650 | 4 | |a Plastic Deformation | |
| 650 | 4 | |a Propagation Rate | |
| 650 | 4 | |a Deformation Mechanism | |
| 700 | 1 | |a Lapidus, A. M. |4 aut | |
| 700 | 1 | |a Torgasheva, V. S. |4 aut | |
| 700 | 1 | |a Pol'dyaeva, G. P. |4 aut | |
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10.1007/BF00653209 doi (DE-627)OLC2047988756 (DE-He213)BF00653209-p DE-627 ger DE-627 rakwb eng 670 620 660 VZ Shishkova, A. P. verfasserin aut Microstructure of iron and low-carbon steel after pulse loading 1969 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Consultants Bureau 1969 Conclusions The deformation mechanism in pulse loading differs from all other types in static and dynamic loading and consists in the formation of a mosaic structure without plastic flow of the grains.Plastic flow occurs during pulse loading when the movement of the piece is restrained or as the result of the interaction of structurally heterogeneous zones during pulse loading.The hardening resulting from pulse loading exceeds that resulting from ordinary plastic deformation. The hardness is highest when a mosaic structure is formed and amounts to approximately 150–250% of the initial values.The principal factors influencing the structure and properties of the material after pulse loading are the loading velocity and the shape of the sample.At the critical percentage of mosaic structure, pores are formed. Fracture occurs when the propagation rate of the pores exceeds the rate at which the load is removed. Iron Microstructure Plastic Deformation Propagation Rate Deformation Mechanism Lapidus, A. M. aut Torgasheva, V. S. aut Pol'dyaeva, G. P. aut Enthalten in Metal science and heat treatment Kluwer Academic Publishers-Plenum Publishers, 1959 11(1969), 4 vom: Apr., Seite 325-326 (DE-627)129596981 (DE-600)240858-2 (DE-576)015090159 0026-0673 nnns volume:11 year:1969 number:4 month:04 pages:325-326 https://doi.org/10.1007/BF00653209 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_11 GBV_ILN_30 GBV_ILN_70 GBV_ILN_2015 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4319 AR 11 1969 4 04 325-326 |
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10.1007/BF00653209 doi (DE-627)OLC2047988756 (DE-He213)BF00653209-p DE-627 ger DE-627 rakwb eng 670 620 660 VZ Shishkova, A. P. verfasserin aut Microstructure of iron and low-carbon steel after pulse loading 1969 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Consultants Bureau 1969 Conclusions The deformation mechanism in pulse loading differs from all other types in static and dynamic loading and consists in the formation of a mosaic structure without plastic flow of the grains.Plastic flow occurs during pulse loading when the movement of the piece is restrained or as the result of the interaction of structurally heterogeneous zones during pulse loading.The hardening resulting from pulse loading exceeds that resulting from ordinary plastic deformation. The hardness is highest when a mosaic structure is formed and amounts to approximately 150–250% of the initial values.The principal factors influencing the structure and properties of the material after pulse loading are the loading velocity and the shape of the sample.At the critical percentage of mosaic structure, pores are formed. Fracture occurs when the propagation rate of the pores exceeds the rate at which the load is removed. Iron Microstructure Plastic Deformation Propagation Rate Deformation Mechanism Lapidus, A. M. aut Torgasheva, V. S. aut Pol'dyaeva, G. P. aut Enthalten in Metal science and heat treatment Kluwer Academic Publishers-Plenum Publishers, 1959 11(1969), 4 vom: Apr., Seite 325-326 (DE-627)129596981 (DE-600)240858-2 (DE-576)015090159 0026-0673 nnns volume:11 year:1969 number:4 month:04 pages:325-326 https://doi.org/10.1007/BF00653209 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_11 GBV_ILN_30 GBV_ILN_70 GBV_ILN_2015 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4319 AR 11 1969 4 04 325-326 |
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10.1007/BF00653209 doi (DE-627)OLC2047988756 (DE-He213)BF00653209-p DE-627 ger DE-627 rakwb eng 670 620 660 VZ Shishkova, A. P. verfasserin aut Microstructure of iron and low-carbon steel after pulse loading 1969 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Consultants Bureau 1969 Conclusions The deformation mechanism in pulse loading differs from all other types in static and dynamic loading and consists in the formation of a mosaic structure without plastic flow of the grains.Plastic flow occurs during pulse loading when the movement of the piece is restrained or as the result of the interaction of structurally heterogeneous zones during pulse loading.The hardening resulting from pulse loading exceeds that resulting from ordinary plastic deformation. The hardness is highest when a mosaic structure is formed and amounts to approximately 150–250% of the initial values.The principal factors influencing the structure and properties of the material after pulse loading are the loading velocity and the shape of the sample.At the critical percentage of mosaic structure, pores are formed. Fracture occurs when the propagation rate of the pores exceeds the rate at which the load is removed. Iron Microstructure Plastic Deformation Propagation Rate Deformation Mechanism Lapidus, A. M. aut Torgasheva, V. S. aut Pol'dyaeva, G. P. aut Enthalten in Metal science and heat treatment Kluwer Academic Publishers-Plenum Publishers, 1959 11(1969), 4 vom: Apr., Seite 325-326 (DE-627)129596981 (DE-600)240858-2 (DE-576)015090159 0026-0673 nnns volume:11 year:1969 number:4 month:04 pages:325-326 https://doi.org/10.1007/BF00653209 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_11 GBV_ILN_30 GBV_ILN_70 GBV_ILN_2015 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4319 AR 11 1969 4 04 325-326 |
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10.1007/BF00653209 doi (DE-627)OLC2047988756 (DE-He213)BF00653209-p DE-627 ger DE-627 rakwb eng 670 620 660 VZ Shishkova, A. P. verfasserin aut Microstructure of iron and low-carbon steel after pulse loading 1969 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Consultants Bureau 1969 Conclusions The deformation mechanism in pulse loading differs from all other types in static and dynamic loading and consists in the formation of a mosaic structure without plastic flow of the grains.Plastic flow occurs during pulse loading when the movement of the piece is restrained or as the result of the interaction of structurally heterogeneous zones during pulse loading.The hardening resulting from pulse loading exceeds that resulting from ordinary plastic deformation. The hardness is highest when a mosaic structure is formed and amounts to approximately 150–250% of the initial values.The principal factors influencing the structure and properties of the material after pulse loading are the loading velocity and the shape of the sample.At the critical percentage of mosaic structure, pores are formed. Fracture occurs when the propagation rate of the pores exceeds the rate at which the load is removed. Iron Microstructure Plastic Deformation Propagation Rate Deformation Mechanism Lapidus, A. M. aut Torgasheva, V. S. aut Pol'dyaeva, G. P. aut Enthalten in Metal science and heat treatment Kluwer Academic Publishers-Plenum Publishers, 1959 11(1969), 4 vom: Apr., Seite 325-326 (DE-627)129596981 (DE-600)240858-2 (DE-576)015090159 0026-0673 nnns volume:11 year:1969 number:4 month:04 pages:325-326 https://doi.org/10.1007/BF00653209 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_11 GBV_ILN_30 GBV_ILN_70 GBV_ILN_2015 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4319 AR 11 1969 4 04 325-326 |
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10.1007/BF00653209 doi (DE-627)OLC2047988756 (DE-He213)BF00653209-p DE-627 ger DE-627 rakwb eng 670 620 660 VZ Shishkova, A. P. verfasserin aut Microstructure of iron and low-carbon steel after pulse loading 1969 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Consultants Bureau 1969 Conclusions The deformation mechanism in pulse loading differs from all other types in static and dynamic loading and consists in the formation of a mosaic structure without plastic flow of the grains.Plastic flow occurs during pulse loading when the movement of the piece is restrained or as the result of the interaction of structurally heterogeneous zones during pulse loading.The hardening resulting from pulse loading exceeds that resulting from ordinary plastic deformation. The hardness is highest when a mosaic structure is formed and amounts to approximately 150–250% of the initial values.The principal factors influencing the structure and properties of the material after pulse loading are the loading velocity and the shape of the sample.At the critical percentage of mosaic structure, pores are formed. Fracture occurs when the propagation rate of the pores exceeds the rate at which the load is removed. Iron Microstructure Plastic Deformation Propagation Rate Deformation Mechanism Lapidus, A. M. aut Torgasheva, V. S. aut Pol'dyaeva, G. P. aut Enthalten in Metal science and heat treatment Kluwer Academic Publishers-Plenum Publishers, 1959 11(1969), 4 vom: Apr., Seite 325-326 (DE-627)129596981 (DE-600)240858-2 (DE-576)015090159 0026-0673 nnns volume:11 year:1969 number:4 month:04 pages:325-326 https://doi.org/10.1007/BF00653209 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_11 GBV_ILN_30 GBV_ILN_70 GBV_ILN_2015 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4319 AR 11 1969 4 04 325-326 |
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microstructure of iron and low-carbon steel after pulse loading |
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Microstructure of iron and low-carbon steel after pulse loading |
| abstract |
Conclusions The deformation mechanism in pulse loading differs from all other types in static and dynamic loading and consists in the formation of a mosaic structure without plastic flow of the grains.Plastic flow occurs during pulse loading when the movement of the piece is restrained or as the result of the interaction of structurally heterogeneous zones during pulse loading.The hardening resulting from pulse loading exceeds that resulting from ordinary plastic deformation. The hardness is highest when a mosaic structure is formed and amounts to approximately 150–250% of the initial values.The principal factors influencing the structure and properties of the material after pulse loading are the loading velocity and the shape of the sample.At the critical percentage of mosaic structure, pores are formed. Fracture occurs when the propagation rate of the pores exceeds the rate at which the load is removed. © Consultants Bureau 1969 |
| abstractGer |
Conclusions The deformation mechanism in pulse loading differs from all other types in static and dynamic loading and consists in the formation of a mosaic structure without plastic flow of the grains.Plastic flow occurs during pulse loading when the movement of the piece is restrained or as the result of the interaction of structurally heterogeneous zones during pulse loading.The hardening resulting from pulse loading exceeds that resulting from ordinary plastic deformation. The hardness is highest when a mosaic structure is formed and amounts to approximately 150–250% of the initial values.The principal factors influencing the structure and properties of the material after pulse loading are the loading velocity and the shape of the sample.At the critical percentage of mosaic structure, pores are formed. Fracture occurs when the propagation rate of the pores exceeds the rate at which the load is removed. © Consultants Bureau 1969 |
| abstract_unstemmed |
Conclusions The deformation mechanism in pulse loading differs from all other types in static and dynamic loading and consists in the formation of a mosaic structure without plastic flow of the grains.Plastic flow occurs during pulse loading when the movement of the piece is restrained or as the result of the interaction of structurally heterogeneous zones during pulse loading.The hardening resulting from pulse loading exceeds that resulting from ordinary plastic deformation. The hardness is highest when a mosaic structure is formed and amounts to approximately 150–250% of the initial values.The principal factors influencing the structure and properties of the material after pulse loading are the loading velocity and the shape of the sample.At the critical percentage of mosaic structure, pores are formed. Fracture occurs when the propagation rate of the pores exceeds the rate at which the load is removed. © Consultants Bureau 1969 |
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Microstructure of iron and low-carbon steel after pulse loading |
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Lapidus, A. M. Torgasheva, V. S. Pol'dyaeva, G. P. |
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Lapidus, A. M. Torgasheva, V. S. Pol'dyaeva, G. P. |
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10.1007/BF00653209 |
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2024-07-03T17:10:21.771Z |
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P.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Microstructure of iron and low-carbon steel after pulse loading</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1969</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">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Consultants Bureau 1969</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Conclusions The deformation mechanism in pulse loading differs from all other types in static and dynamic loading and consists in the formation of a mosaic structure without plastic flow of the grains.Plastic flow occurs during pulse loading when the movement of the piece is restrained or as the result of the interaction of structurally heterogeneous zones during pulse loading.The hardening resulting from pulse loading exceeds that resulting from ordinary plastic deformation. 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