Influence of prestress on the velocities of plane waves propagating normally to the layers of nanocomposites
Abstract The paper is concerned with longitudinal and transverse waves propagating at a right angle to the layers of a nanocomposite material with initial (process-induced residual) stresses. The composite consists of alternating layers of two dissimilar materials. The materials are assumed nonlinea...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Zhuk, Ya. A. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2006 |
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| Schlagwörter: |
three-dimensional linearized theory of elasticity |
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| Anmerkung: |
© Springer Science+Business Media, Inc. 2006 |
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| Übergeordnetes Werk: |
Enthalten in: International applied mechanics - Kluwer Academic Publishers-Consultants Bureau, 1993, 42(2006), 7 vom: Juli, Seite 729-743 |
|---|---|
| Übergeordnetes Werk: |
volume:42 ; year:2006 ; number:7 ; month:07 ; pages:729-743 |
| Links: |
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| DOI / URN: |
10.1007/s10778-006-0141-9 |
|---|
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OLC2075728674 |
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| 520 | |a Abstract The paper is concerned with longitudinal and transverse waves propagating at a right angle to the layers of a nanocomposite material with initial (process-induced residual) stresses. The composite consists of alternating layers of two dissimilar materials. The materials are assumed nonlinearly elastic and described by the Murnaghan potential. For simulation of wave propagation, a problem is formulated within the framework of the three-dimensional linearized theory of elasticity for finite prestrains. It is established that the relative velocities of waves depend linearly on small prestresses. In some composite materials, however, the thicknesses of the layers may be in a ratio such that the wave velocities are independent of the prestress level | ||
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10.1007/s10778-006-0141-9 doi (DE-627)OLC2075728674 (DE-He213)s10778-006-0141-9-p DE-627 ger DE-627 rakwb eng 530 VZ Zhuk, Ya. A. verfasserin aut Influence of prestress on the velocities of plane waves propagating normally to the layers of nanocomposites 2006 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, Inc. 2006 Abstract The paper is concerned with longitudinal and transverse waves propagating at a right angle to the layers of a nanocomposite material with initial (process-induced residual) stresses. The composite consists of alternating layers of two dissimilar materials. The materials are assumed nonlinearly elastic and described by the Murnaghan potential. For simulation of wave propagation, a problem is formulated within the framework of the three-dimensional linearized theory of elasticity for finite prestrains. It is established that the relative velocities of waves depend linearly on small prestresses. In some composite materials, however, the thicknesses of the layers may be in a ratio such that the wave velocities are independent of the prestress level composite materials nanocomposites three-dimensional linearized theory of elasticity initial stress longitudinal and transverse waves wave velocities Guz, I. A. aut Enthalten in International applied mechanics Kluwer Academic Publishers-Consultants Bureau, 1993 42(2006), 7 vom: Juli, Seite 729-743 (DE-627)131145630 (DE-600)1128258-7 (DE-576)032855141 1063-7095 nnns volume:42 year:2006 number:7 month:07 pages:729-743 https://doi.org/10.1007/s10778-006-0141-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 AR 42 2006 7 07 729-743 |
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10.1007/s10778-006-0141-9 doi (DE-627)OLC2075728674 (DE-He213)s10778-006-0141-9-p DE-627 ger DE-627 rakwb eng 530 VZ Zhuk, Ya. A. verfasserin aut Influence of prestress on the velocities of plane waves propagating normally to the layers of nanocomposites 2006 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, Inc. 2006 Abstract The paper is concerned with longitudinal and transverse waves propagating at a right angle to the layers of a nanocomposite material with initial (process-induced residual) stresses. The composite consists of alternating layers of two dissimilar materials. The materials are assumed nonlinearly elastic and described by the Murnaghan potential. For simulation of wave propagation, a problem is formulated within the framework of the three-dimensional linearized theory of elasticity for finite prestrains. It is established that the relative velocities of waves depend linearly on small prestresses. In some composite materials, however, the thicknesses of the layers may be in a ratio such that the wave velocities are independent of the prestress level composite materials nanocomposites three-dimensional linearized theory of elasticity initial stress longitudinal and transverse waves wave velocities Guz, I. A. aut Enthalten in International applied mechanics Kluwer Academic Publishers-Consultants Bureau, 1993 42(2006), 7 vom: Juli, Seite 729-743 (DE-627)131145630 (DE-600)1128258-7 (DE-576)032855141 1063-7095 nnns volume:42 year:2006 number:7 month:07 pages:729-743 https://doi.org/10.1007/s10778-006-0141-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 AR 42 2006 7 07 729-743 |
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10.1007/s10778-006-0141-9 doi (DE-627)OLC2075728674 (DE-He213)s10778-006-0141-9-p DE-627 ger DE-627 rakwb eng 530 VZ Zhuk, Ya. A. verfasserin aut Influence of prestress on the velocities of plane waves propagating normally to the layers of nanocomposites 2006 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, Inc. 2006 Abstract The paper is concerned with longitudinal and transverse waves propagating at a right angle to the layers of a nanocomposite material with initial (process-induced residual) stresses. The composite consists of alternating layers of two dissimilar materials. The materials are assumed nonlinearly elastic and described by the Murnaghan potential. For simulation of wave propagation, a problem is formulated within the framework of the three-dimensional linearized theory of elasticity for finite prestrains. It is established that the relative velocities of waves depend linearly on small prestresses. In some composite materials, however, the thicknesses of the layers may be in a ratio such that the wave velocities are independent of the prestress level composite materials nanocomposites three-dimensional linearized theory of elasticity initial stress longitudinal and transverse waves wave velocities Guz, I. A. aut Enthalten in International applied mechanics Kluwer Academic Publishers-Consultants Bureau, 1993 42(2006), 7 vom: Juli, Seite 729-743 (DE-627)131145630 (DE-600)1128258-7 (DE-576)032855141 1063-7095 nnns volume:42 year:2006 number:7 month:07 pages:729-743 https://doi.org/10.1007/s10778-006-0141-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 AR 42 2006 7 07 729-743 |
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10.1007/s10778-006-0141-9 doi (DE-627)OLC2075728674 (DE-He213)s10778-006-0141-9-p DE-627 ger DE-627 rakwb eng 530 VZ Zhuk, Ya. A. verfasserin aut Influence of prestress on the velocities of plane waves propagating normally to the layers of nanocomposites 2006 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, Inc. 2006 Abstract The paper is concerned with longitudinal and transverse waves propagating at a right angle to the layers of a nanocomposite material with initial (process-induced residual) stresses. The composite consists of alternating layers of two dissimilar materials. The materials are assumed nonlinearly elastic and described by the Murnaghan potential. For simulation of wave propagation, a problem is formulated within the framework of the three-dimensional linearized theory of elasticity for finite prestrains. It is established that the relative velocities of waves depend linearly on small prestresses. In some composite materials, however, the thicknesses of the layers may be in a ratio such that the wave velocities are independent of the prestress level composite materials nanocomposites three-dimensional linearized theory of elasticity initial stress longitudinal and transverse waves wave velocities Guz, I. A. aut Enthalten in International applied mechanics Kluwer Academic Publishers-Consultants Bureau, 1993 42(2006), 7 vom: Juli, Seite 729-743 (DE-627)131145630 (DE-600)1128258-7 (DE-576)032855141 1063-7095 nnns volume:42 year:2006 number:7 month:07 pages:729-743 https://doi.org/10.1007/s10778-006-0141-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 AR 42 2006 7 07 729-743 |
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10.1007/s10778-006-0141-9 doi (DE-627)OLC2075728674 (DE-He213)s10778-006-0141-9-p DE-627 ger DE-627 rakwb eng 530 VZ Zhuk, Ya. A. verfasserin aut Influence of prestress on the velocities of plane waves propagating normally to the layers of nanocomposites 2006 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, Inc. 2006 Abstract The paper is concerned with longitudinal and transverse waves propagating at a right angle to the layers of a nanocomposite material with initial (process-induced residual) stresses. The composite consists of alternating layers of two dissimilar materials. The materials are assumed nonlinearly elastic and described by the Murnaghan potential. For simulation of wave propagation, a problem is formulated within the framework of the three-dimensional linearized theory of elasticity for finite prestrains. It is established that the relative velocities of waves depend linearly on small prestresses. In some composite materials, however, the thicknesses of the layers may be in a ratio such that the wave velocities are independent of the prestress level composite materials nanocomposites three-dimensional linearized theory of elasticity initial stress longitudinal and transverse waves wave velocities Guz, I. A. aut Enthalten in International applied mechanics Kluwer Academic Publishers-Consultants Bureau, 1993 42(2006), 7 vom: Juli, Seite 729-743 (DE-627)131145630 (DE-600)1128258-7 (DE-576)032855141 1063-7095 nnns volume:42 year:2006 number:7 month:07 pages:729-743 https://doi.org/10.1007/s10778-006-0141-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_70 AR 42 2006 7 07 729-743 |
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Abstract The paper is concerned with longitudinal and transverse waves propagating at a right angle to the layers of a nanocomposite material with initial (process-induced residual) stresses. The composite consists of alternating layers of two dissimilar materials. The materials are assumed nonlinearly elastic and described by the Murnaghan potential. For simulation of wave propagation, a problem is formulated within the framework of the three-dimensional linearized theory of elasticity for finite prestrains. It is established that the relative velocities of waves depend linearly on small prestresses. In some composite materials, however, the thicknesses of the layers may be in a ratio such that the wave velocities are independent of the prestress level © Springer Science+Business Media, Inc. 2006 |
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Abstract The paper is concerned with longitudinal and transverse waves propagating at a right angle to the layers of a nanocomposite material with initial (process-induced residual) stresses. The composite consists of alternating layers of two dissimilar materials. The materials are assumed nonlinearly elastic and described by the Murnaghan potential. For simulation of wave propagation, a problem is formulated within the framework of the three-dimensional linearized theory of elasticity for finite prestrains. It is established that the relative velocities of waves depend linearly on small prestresses. In some composite materials, however, the thicknesses of the layers may be in a ratio such that the wave velocities are independent of the prestress level © Springer Science+Business Media, Inc. 2006 |
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Abstract The paper is concerned with longitudinal and transverse waves propagating at a right angle to the layers of a nanocomposite material with initial (process-induced residual) stresses. The composite consists of alternating layers of two dissimilar materials. The materials are assumed nonlinearly elastic and described by the Murnaghan potential. For simulation of wave propagation, a problem is formulated within the framework of the three-dimensional linearized theory of elasticity for finite prestrains. It is established that the relative velocities of waves depend linearly on small prestresses. In some composite materials, however, the thicknesses of the layers may be in a ratio such that the wave velocities are independent of the prestress level © Springer Science+Business Media, Inc. 2006 |
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A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Influence of prestress on the velocities of plane waves propagating normally to the layers of nanocomposites</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2006</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, Inc. 2006</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The paper is concerned with longitudinal and transverse waves propagating at a right angle to the layers of a nanocomposite material with initial (process-induced residual) stresses. The composite consists of alternating layers of two dissimilar materials. The materials are assumed nonlinearly elastic and described by the Murnaghan potential. For simulation of wave propagation, a problem is formulated within the framework of the three-dimensional linearized theory of elasticity for finite prestrains. It is established that the relative velocities of waves depend linearly on small prestresses. In some composite materials, however, the thicknesses of the layers may be in a ratio such that the wave velocities are independent of the prestress level</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">composite materials</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">nanocomposites</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">three-dimensional linearized theory of elasticity</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">initial stress</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">longitudinal and transverse waves</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">wave velocities</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Guz, I. A.</subfield><subfield code="4">aut</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">Kluwer Academic Publishers-Consultants Bureau, 1993</subfield><subfield code="g">42(2006), 7 vom: Juli, Seite 729-743</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:42</subfield><subfield code="g">year:2006</subfield><subfield code="g">number:7</subfield><subfield code="g">month:07</subfield><subfield code="g">pages:729-743</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/s10778-006-0141-9</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">42</subfield><subfield code="j">2006</subfield><subfield code="e">7</subfield><subfield code="c">07</subfield><subfield code="h">729-743</subfield></datafield></record></collection>
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