Dynamic model of surface-layer formation in friction
Abstract A model of the frictional interaction between two elastoplastic bodies as an interaction between microheterogeneities of the surface layers is considered. This interaction consists of a series of short large-amplitude impacts of random duration, occurring at random intervals. Thus, friction...
Ausführliche Beschreibung
Autor*in: |
Popov, V. L. [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
1993 |
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Schlagwörter: |
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Anmerkung: |
© Plenum Publishing Corporation 1994 |
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Übergeordnetes Werk: |
Enthalten in: Russian physics journal - Kluwer Academic Publishers-Plenum Publishers, 1992, 36(1993), 12 vom: Dez., Seite 1119-1120 |
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Übergeordnetes Werk: |
volume:36 ; year:1993 ; number:12 ; month:12 ; pages:1119-1120 |
Links: |
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DOI / URN: |
10.1007/BF00559686 |
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Katalog-ID: |
OLC2033042022 |
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520 | |a Abstract A model of the frictional interaction between two elastoplastic bodies as an interaction between microheterogeneities of the surface layers is considered. This interaction consists of a series of short large-amplitude impacts of random duration, occurring at random intervals. Thus, friction is modeled as a dynamic stochastic perturbation. Heat propagation is regarded as the process determining surface-layer formation. The penetration depth of the thermal wave in the material is determined by the frequency of the perturbation and the thermal conductivity of the material. | ||
650 | 4 | |a Thermal Conductivity | |
650 | 4 | |a Surface Layer | |
650 | 4 | |a Penetration Depth | |
650 | 4 | |a Heat Propagation | |
650 | 4 | |a Thermal Wave | |
700 | 1 | |a Soshnyanina, N. N. |4 aut | |
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10.1007/BF00559686 doi (DE-627)OLC2033042022 (DE-He213)BF00559686-p DE-627 ger DE-627 rakwb eng 530 370 VZ Popov, V. L. verfasserin aut Dynamic model of surface-layer formation in friction 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1994 Abstract A model of the frictional interaction between two elastoplastic bodies as an interaction between microheterogeneities of the surface layers is considered. This interaction consists of a series of short large-amplitude impacts of random duration, occurring at random intervals. Thus, friction is modeled as a dynamic stochastic perturbation. Heat propagation is regarded as the process determining surface-layer formation. The penetration depth of the thermal wave in the material is determined by the frequency of the perturbation and the thermal conductivity of the material. Thermal Conductivity Surface Layer Penetration Depth Heat Propagation Thermal Wave Soshnyanina, N. N. aut Enthalten in Russian physics journal Kluwer Academic Publishers-Plenum Publishers, 1992 36(1993), 12 vom: Dez., Seite 1119-1120 (DE-627)131169718 (DE-600)1138228-4 (DE-576)033029253 1064-8887 nnns volume:36 year:1993 number:12 month:12 pages:1119-1120 https://doi.org/10.1007/BF00559686 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2021 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4700 AR 36 1993 12 12 1119-1120 |
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10.1007/BF00559686 doi (DE-627)OLC2033042022 (DE-He213)BF00559686-p DE-627 ger DE-627 rakwb eng 530 370 VZ Popov, V. L. verfasserin aut Dynamic model of surface-layer formation in friction 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1994 Abstract A model of the frictional interaction between two elastoplastic bodies as an interaction between microheterogeneities of the surface layers is considered. This interaction consists of a series of short large-amplitude impacts of random duration, occurring at random intervals. Thus, friction is modeled as a dynamic stochastic perturbation. Heat propagation is regarded as the process determining surface-layer formation. The penetration depth of the thermal wave in the material is determined by the frequency of the perturbation and the thermal conductivity of the material. Thermal Conductivity Surface Layer Penetration Depth Heat Propagation Thermal Wave Soshnyanina, N. N. aut Enthalten in Russian physics journal Kluwer Academic Publishers-Plenum Publishers, 1992 36(1993), 12 vom: Dez., Seite 1119-1120 (DE-627)131169718 (DE-600)1138228-4 (DE-576)033029253 1064-8887 nnns volume:36 year:1993 number:12 month:12 pages:1119-1120 https://doi.org/10.1007/BF00559686 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2021 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4700 AR 36 1993 12 12 1119-1120 |
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10.1007/BF00559686 doi (DE-627)OLC2033042022 (DE-He213)BF00559686-p DE-627 ger DE-627 rakwb eng 530 370 VZ Popov, V. L. verfasserin aut Dynamic model of surface-layer formation in friction 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1994 Abstract A model of the frictional interaction between two elastoplastic bodies as an interaction between microheterogeneities of the surface layers is considered. This interaction consists of a series of short large-amplitude impacts of random duration, occurring at random intervals. Thus, friction is modeled as a dynamic stochastic perturbation. Heat propagation is regarded as the process determining surface-layer formation. The penetration depth of the thermal wave in the material is determined by the frequency of the perturbation and the thermal conductivity of the material. Thermal Conductivity Surface Layer Penetration Depth Heat Propagation Thermal Wave Soshnyanina, N. N. aut Enthalten in Russian physics journal Kluwer Academic Publishers-Plenum Publishers, 1992 36(1993), 12 vom: Dez., Seite 1119-1120 (DE-627)131169718 (DE-600)1138228-4 (DE-576)033029253 1064-8887 nnns volume:36 year:1993 number:12 month:12 pages:1119-1120 https://doi.org/10.1007/BF00559686 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2021 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4700 AR 36 1993 12 12 1119-1120 |
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10.1007/BF00559686 doi (DE-627)OLC2033042022 (DE-He213)BF00559686-p DE-627 ger DE-627 rakwb eng 530 370 VZ Popov, V. L. verfasserin aut Dynamic model of surface-layer formation in friction 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1994 Abstract A model of the frictional interaction between two elastoplastic bodies as an interaction between microheterogeneities of the surface layers is considered. This interaction consists of a series of short large-amplitude impacts of random duration, occurring at random intervals. Thus, friction is modeled as a dynamic stochastic perturbation. Heat propagation is regarded as the process determining surface-layer formation. The penetration depth of the thermal wave in the material is determined by the frequency of the perturbation and the thermal conductivity of the material. Thermal Conductivity Surface Layer Penetration Depth Heat Propagation Thermal Wave Soshnyanina, N. N. aut Enthalten in Russian physics journal Kluwer Academic Publishers-Plenum Publishers, 1992 36(1993), 12 vom: Dez., Seite 1119-1120 (DE-627)131169718 (DE-600)1138228-4 (DE-576)033029253 1064-8887 nnns volume:36 year:1993 number:12 month:12 pages:1119-1120 https://doi.org/10.1007/BF00559686 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2021 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4700 AR 36 1993 12 12 1119-1120 |
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10.1007/BF00559686 doi (DE-627)OLC2033042022 (DE-He213)BF00559686-p DE-627 ger DE-627 rakwb eng 530 370 VZ Popov, V. L. verfasserin aut Dynamic model of surface-layer formation in friction 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1994 Abstract A model of the frictional interaction between two elastoplastic bodies as an interaction between microheterogeneities of the surface layers is considered. This interaction consists of a series of short large-amplitude impacts of random duration, occurring at random intervals. Thus, friction is modeled as a dynamic stochastic perturbation. Heat propagation is regarded as the process determining surface-layer formation. The penetration depth of the thermal wave in the material is determined by the frequency of the perturbation and the thermal conductivity of the material. Thermal Conductivity Surface Layer Penetration Depth Heat Propagation Thermal Wave Soshnyanina, N. N. aut Enthalten in Russian physics journal Kluwer Academic Publishers-Plenum Publishers, 1992 36(1993), 12 vom: Dez., Seite 1119-1120 (DE-627)131169718 (DE-600)1138228-4 (DE-576)033029253 1064-8887 nnns volume:36 year:1993 number:12 month:12 pages:1119-1120 https://doi.org/10.1007/BF00559686 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2021 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4700 AR 36 1993 12 12 1119-1120 |
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Abstract A model of the frictional interaction between two elastoplastic bodies as an interaction between microheterogeneities of the surface layers is considered. This interaction consists of a series of short large-amplitude impacts of random duration, occurring at random intervals. Thus, friction is modeled as a dynamic stochastic perturbation. Heat propagation is regarded as the process determining surface-layer formation. The penetration depth of the thermal wave in the material is determined by the frequency of the perturbation and the thermal conductivity of the material. © Plenum Publishing Corporation 1994 |
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Abstract A model of the frictional interaction between two elastoplastic bodies as an interaction between microheterogeneities of the surface layers is considered. This interaction consists of a series of short large-amplitude impacts of random duration, occurring at random intervals. Thus, friction is modeled as a dynamic stochastic perturbation. Heat propagation is regarded as the process determining surface-layer formation. The penetration depth of the thermal wave in the material is determined by the frequency of the perturbation and the thermal conductivity of the material. © Plenum Publishing Corporation 1994 |
abstract_unstemmed |
Abstract A model of the frictional interaction between two elastoplastic bodies as an interaction between microheterogeneities of the surface layers is considered. This interaction consists of a series of short large-amplitude impacts of random duration, occurring at random intervals. Thus, friction is modeled as a dynamic stochastic perturbation. Heat propagation is regarded as the process determining surface-layer formation. The penetration depth of the thermal wave in the material is determined by the frequency of the perturbation and the thermal conductivity of the material. © Plenum Publishing Corporation 1994 |
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L.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Dynamic model of surface-layer formation in friction</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1993</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">© Plenum Publishing Corporation 1994</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract A model of the frictional interaction between two elastoplastic bodies as an interaction between microheterogeneities of the surface layers is considered. 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The penetration depth of the thermal wave in the material is determined by the frequency of the perturbation and the thermal conductivity of the material.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Thermal Conductivity</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Surface Layer</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Penetration Depth</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Heat Propagation</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Thermal Wave</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Soshnyanina, N. 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