Slow Growth of a Crack with Contacting Faces in a Viscoelastic Body
An algorithm for solving the problem of slow growth of a mode I crack with a zone of partial contact of the faces is proposed. The algorithm is based on a crack model with a cohesive zone, an iterative method of finding a solution for the elastic opening displacement, and elasto–viscoelastic analogy...
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Gespeichert in:
| Autor*in: |
Selivanov, M. F. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2017 |
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| Schlagwörter: |
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| Anmerkung: |
© Springer Science+Business Media, LLC, part of Springer Nature 2018 |
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| Übergeordnetes Werk: |
Enthalten in: International applied mechanics - Springer US, 1993, 53(2017), 6 vom: Nov., Seite 617-622 |
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| Übergeordnetes Werk: |
volume:53 ; year:2017 ; number:6 ; month:11 ; pages:617-622 |
| Links: |
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| DOI / URN: |
10.1007/s10778-018-0844-8 |
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OLC2075737991 |
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| 520 | |a An algorithm for solving the problem of slow growth of a mode I crack with a zone of partial contact of the faces is proposed. The algorithm is based on a crack model with a cohesive zone, an iterative method of finding a solution for the elastic opening displacement, and elasto–viscoelastic analogy, which makes it possible to describe the time-dependent opening displacement in Boltzmann–Volterra form. A deformation criterion with a constant critical opening displacement and cohesive strength during quasistatic crack growth is used. The algorithm was numerically illustrated for tensile loading at infinity and two concentrated forces symmetric about the crack line that cause the crack faces to contact. When the crack propagates, the contact zone disappears and its dynamic growth begins. | ||
| 650 | 4 | |a cohesive crack | |
| 650 | 4 | |a viscoelastic solids | |
| 650 | 4 | |a slow crack growth | |
| 650 | 4 | |a contact of crack faces | |
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10.1007/s10778-018-0844-8 doi (DE-627)OLC2075737991 (DE-He213)s10778-018-0844-8-p DE-627 ger DE-627 rakwb eng 530 VZ Selivanov, M. F. verfasserin aut Slow Growth of a Crack with Contacting Faces in a Viscoelastic Body 2017 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2018 An algorithm for solving the problem of slow growth of a mode I crack with a zone of partial contact of the faces is proposed. The algorithm is based on a crack model with a cohesive zone, an iterative method of finding a solution for the elastic opening displacement, and elasto–viscoelastic analogy, which makes it possible to describe the time-dependent opening displacement in Boltzmann–Volterra form. A deformation criterion with a constant critical opening displacement and cohesive strength during quasistatic crack growth is used. The algorithm was numerically illustrated for tensile loading at infinity and two concentrated forces symmetric about the crack line that cause the crack faces to contact. When the crack propagates, the contact zone disappears and its dynamic growth begins. cohesive crack viscoelastic solids slow crack growth contact of crack faces Enthalten in International applied mechanics Springer US, 1993 53(2017), 6 vom: Nov., Seite 617-622 (DE-627)131145630 (DE-600)1128258-7 (DE-576)032855141 1063-7095 nnns volume:53 year:2017 number:6 month:11 pages:617-622 https://doi.org/10.1007/s10778-018-0844-8 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 AR 53 2017 6 11 617-622 |
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10.1007/s10778-018-0844-8 doi (DE-627)OLC2075737991 (DE-He213)s10778-018-0844-8-p DE-627 ger DE-627 rakwb eng 530 VZ Selivanov, M. F. verfasserin aut Slow Growth of a Crack with Contacting Faces in a Viscoelastic Body 2017 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2018 An algorithm for solving the problem of slow growth of a mode I crack with a zone of partial contact of the faces is proposed. The algorithm is based on a crack model with a cohesive zone, an iterative method of finding a solution for the elastic opening displacement, and elasto–viscoelastic analogy, which makes it possible to describe the time-dependent opening displacement in Boltzmann–Volterra form. A deformation criterion with a constant critical opening displacement and cohesive strength during quasistatic crack growth is used. The algorithm was numerically illustrated for tensile loading at infinity and two concentrated forces symmetric about the crack line that cause the crack faces to contact. When the crack propagates, the contact zone disappears and its dynamic growth begins. cohesive crack viscoelastic solids slow crack growth contact of crack faces Enthalten in International applied mechanics Springer US, 1993 53(2017), 6 vom: Nov., Seite 617-622 (DE-627)131145630 (DE-600)1128258-7 (DE-576)032855141 1063-7095 nnns volume:53 year:2017 number:6 month:11 pages:617-622 https://doi.org/10.1007/s10778-018-0844-8 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 AR 53 2017 6 11 617-622 |
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10.1007/s10778-018-0844-8 doi (DE-627)OLC2075737991 (DE-He213)s10778-018-0844-8-p DE-627 ger DE-627 rakwb eng 530 VZ Selivanov, M. F. verfasserin aut Slow Growth of a Crack with Contacting Faces in a Viscoelastic Body 2017 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2018 An algorithm for solving the problem of slow growth of a mode I crack with a zone of partial contact of the faces is proposed. The algorithm is based on a crack model with a cohesive zone, an iterative method of finding a solution for the elastic opening displacement, and elasto–viscoelastic analogy, which makes it possible to describe the time-dependent opening displacement in Boltzmann–Volterra form. A deformation criterion with a constant critical opening displacement and cohesive strength during quasistatic crack growth is used. The algorithm was numerically illustrated for tensile loading at infinity and two concentrated forces symmetric about the crack line that cause the crack faces to contact. When the crack propagates, the contact zone disappears and its dynamic growth begins. cohesive crack viscoelastic solids slow crack growth contact of crack faces Enthalten in International applied mechanics Springer US, 1993 53(2017), 6 vom: Nov., Seite 617-622 (DE-627)131145630 (DE-600)1128258-7 (DE-576)032855141 1063-7095 nnns volume:53 year:2017 number:6 month:11 pages:617-622 https://doi.org/10.1007/s10778-018-0844-8 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 AR 53 2017 6 11 617-622 |
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An algorithm for solving the problem of slow growth of a mode I crack with a zone of partial contact of the faces is proposed. The algorithm is based on a crack model with a cohesive zone, an iterative method of finding a solution for the elastic opening displacement, and elasto–viscoelastic analogy, which makes it possible to describe the time-dependent opening displacement in Boltzmann–Volterra form. A deformation criterion with a constant critical opening displacement and cohesive strength during quasistatic crack growth is used. The algorithm was numerically illustrated for tensile loading at infinity and two concentrated forces symmetric about the crack line that cause the crack faces to contact. When the crack propagates, the contact zone disappears and its dynamic growth begins. © Springer Science+Business Media, LLC, part of Springer Nature 2018 |
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An algorithm for solving the problem of slow growth of a mode I crack with a zone of partial contact of the faces is proposed. The algorithm is based on a crack model with a cohesive zone, an iterative method of finding a solution for the elastic opening displacement, and elasto–viscoelastic analogy, which makes it possible to describe the time-dependent opening displacement in Boltzmann–Volterra form. A deformation criterion with a constant critical opening displacement and cohesive strength during quasistatic crack growth is used. The algorithm was numerically illustrated for tensile loading at infinity and two concentrated forces symmetric about the crack line that cause the crack faces to contact. When the crack propagates, the contact zone disappears and its dynamic growth begins. © Springer Science+Business Media, LLC, part of Springer Nature 2018 |
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An algorithm for solving the problem of slow growth of a mode I crack with a zone of partial contact of the faces is proposed. The algorithm is based on a crack model with a cohesive zone, an iterative method of finding a solution for the elastic opening displacement, and elasto–viscoelastic analogy, which makes it possible to describe the time-dependent opening displacement in Boltzmann–Volterra form. A deformation criterion with a constant critical opening displacement and cohesive strength during quasistatic crack growth is used. The algorithm was numerically illustrated for tensile loading at infinity and two concentrated forces symmetric about the crack line that cause the crack faces to contact. When the crack propagates, the contact zone disappears and its dynamic growth begins. © Springer Science+Business Media, LLC, part of Springer Nature 2018 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC2075737991</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230503092347.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200820s2017 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s10778-018-0844-8</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2075737991</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)s10778-018-0844-8-p</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Selivanov, M. F.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Slow Growth of a Crack with Contacting Faces in a Viscoelastic Body</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2017</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">© Springer Science+Business Media, LLC, part of Springer Nature 2018</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">An algorithm for solving the problem of slow growth of a mode I crack with a zone of partial contact of the faces is proposed. The algorithm is based on a crack model with a cohesive zone, an iterative method of finding a solution for the elastic opening displacement, and elasto–viscoelastic analogy, which makes it possible to describe the time-dependent opening displacement in Boltzmann–Volterra form. A deformation criterion with a constant critical opening displacement and cohesive strength during quasistatic crack growth is used. The algorithm was numerically illustrated for tensile loading at infinity and two concentrated forces symmetric about the crack line that cause the crack faces to contact. When the crack propagates, the contact zone disappears and its dynamic growth begins.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">cohesive crack</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">viscoelastic solids</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">slow crack growth</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">contact of crack faces</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">International applied mechanics</subfield><subfield code="d">Springer US, 1993</subfield><subfield code="g">53(2017), 6 vom: Nov., Seite 617-622</subfield><subfield code="w">(DE-627)131145630</subfield><subfield code="w">(DE-600)1128258-7</subfield><subfield code="w">(DE-576)032855141</subfield><subfield code="x">1063-7095</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:53</subfield><subfield code="g">year:2017</subfield><subfield code="g">number:6</subfield><subfield code="g">month:11</subfield><subfield code="g">pages:617-622</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/s10778-018-0844-8</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-TEC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">53</subfield><subfield code="j">2017</subfield><subfield code="e">6</subfield><subfield code="c">11</subfield><subfield code="h">617-622</subfield></datafield></record></collection>
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