Subregion generalized variational principles for elastic thick plates
Abstract In this paper, the subregion generalized variational principle for elastic thick plates is proposed. Its main points may be stated as follows:Each subregion may be assigned arbitrarily as a potential region or complementary region. The subregion variational principles of potential energy, c...
Ausführliche Beschreibung
Autor*in: |
Yu-Chiu, Long [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
1983 |
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Schlagwörter: |
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Anmerkung: |
© Techmodern Business Promotion 1983 |
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Übergeordnetes Werk: |
Enthalten in: Ying yong shu xue he li xue / English edition - Kluwer Academic Publishers, 1980, 4(1983), 2 vom: Apr., Seite 175-184 |
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Übergeordnetes Werk: |
volume:4 ; year:1983 ; number:2 ; month:04 ; pages:175-184 |
Links: |
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DOI / URN: |
10.1007/BF01895442 |
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Katalog-ID: |
OLC2042828807 |
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520 | |a Abstract In this paper, the subregion generalized variational principle for elastic thick plates is proposed. Its main points may be stated as follows:Each subregion may be assigned arbitrarily as a potential region or complementary region. The subregion variational principles of potential energy, complementary energy and mixed energy represent three special forms of this principle.The number of independent variational variables in each subregion may be assigned arbitrarily. Any one of the subregions may be assigned, as a one-variable-region, two-variable-region or three-variable-region.The conjunction conditions of displacements and stresses on each interline of neighbouring subregions may be relaxed. On the basis of this principle the finite element analysis of non-conforming elements for thick plates can be formulated. Different finite element models for thick plates can be obtained by different applications of this principle. In particular, the subregion mixed variational principle for thick plates may be applied to formulating the subregion mixed finite element method for thick plates. | ||
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10.1007/BF01895442 doi (DE-627)OLC2042828807 (DE-He213)BF01895442-p DE-627 ger DE-627 rakwb eng 510 VZ Yu-Chiu, Long verfasserin aut Subregion generalized variational principles for elastic thick plates 1983 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Techmodern Business Promotion 1983 Abstract In this paper, the subregion generalized variational principle for elastic thick plates is proposed. Its main points may be stated as follows:Each subregion may be assigned arbitrarily as a potential region or complementary region. The subregion variational principles of potential energy, complementary energy and mixed energy represent three special forms of this principle.The number of independent variational variables in each subregion may be assigned arbitrarily. Any one of the subregions may be assigned, as a one-variable-region, two-variable-region or three-variable-region.The conjunction conditions of displacements and stresses on each interline of neighbouring subregions may be relaxed. On the basis of this principle the finite element analysis of non-conforming elements for thick plates can be formulated. Different finite element models for thick plates can be obtained by different applications of this principle. In particular, the subregion mixed variational principle for thick plates may be applied to formulating the subregion mixed finite element method for thick plates. Finite Element Method Potential Energy Element Model Finite Element Analysis Finite Element Model Enthalten in Ying yong shu xue he li xue / English edition Kluwer Academic Publishers, 1980 4(1983), 2 vom: Apr., Seite 175-184 (DE-627)130523747 (DE-600)770632-7 (DE-576)016095987 0253-4827 nnns volume:4 year:1983 number:2 month:04 pages:175-184 https://doi.org/10.1007/BF01895442 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-MAT SSG-OPC-MAT GBV_ILN_11 GBV_ILN_20 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2006 GBV_ILN_2088 GBV_ILN_4310 AR 4 1983 2 04 175-184 |
spelling |
10.1007/BF01895442 doi (DE-627)OLC2042828807 (DE-He213)BF01895442-p DE-627 ger DE-627 rakwb eng 510 VZ Yu-Chiu, Long verfasserin aut Subregion generalized variational principles for elastic thick plates 1983 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Techmodern Business Promotion 1983 Abstract In this paper, the subregion generalized variational principle for elastic thick plates is proposed. Its main points may be stated as follows:Each subregion may be assigned arbitrarily as a potential region or complementary region. The subregion variational principles of potential energy, complementary energy and mixed energy represent three special forms of this principle.The number of independent variational variables in each subregion may be assigned arbitrarily. Any one of the subregions may be assigned, as a one-variable-region, two-variable-region or three-variable-region.The conjunction conditions of displacements and stresses on each interline of neighbouring subregions may be relaxed. On the basis of this principle the finite element analysis of non-conforming elements for thick plates can be formulated. Different finite element models for thick plates can be obtained by different applications of this principle. In particular, the subregion mixed variational principle for thick plates may be applied to formulating the subregion mixed finite element method for thick plates. Finite Element Method Potential Energy Element Model Finite Element Analysis Finite Element Model Enthalten in Ying yong shu xue he li xue / English edition Kluwer Academic Publishers, 1980 4(1983), 2 vom: Apr., Seite 175-184 (DE-627)130523747 (DE-600)770632-7 (DE-576)016095987 0253-4827 nnns volume:4 year:1983 number:2 month:04 pages:175-184 https://doi.org/10.1007/BF01895442 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-MAT SSG-OPC-MAT GBV_ILN_11 GBV_ILN_20 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2006 GBV_ILN_2088 GBV_ILN_4310 AR 4 1983 2 04 175-184 |
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10.1007/BF01895442 doi (DE-627)OLC2042828807 (DE-He213)BF01895442-p DE-627 ger DE-627 rakwb eng 510 VZ Yu-Chiu, Long verfasserin aut Subregion generalized variational principles for elastic thick plates 1983 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Techmodern Business Promotion 1983 Abstract In this paper, the subregion generalized variational principle for elastic thick plates is proposed. Its main points may be stated as follows:Each subregion may be assigned arbitrarily as a potential region or complementary region. The subregion variational principles of potential energy, complementary energy and mixed energy represent three special forms of this principle.The number of independent variational variables in each subregion may be assigned arbitrarily. Any one of the subregions may be assigned, as a one-variable-region, two-variable-region or three-variable-region.The conjunction conditions of displacements and stresses on each interline of neighbouring subregions may be relaxed. On the basis of this principle the finite element analysis of non-conforming elements for thick plates can be formulated. Different finite element models for thick plates can be obtained by different applications of this principle. In particular, the subregion mixed variational principle for thick plates may be applied to formulating the subregion mixed finite element method for thick plates. Finite Element Method Potential Energy Element Model Finite Element Analysis Finite Element Model Enthalten in Ying yong shu xue he li xue / English edition Kluwer Academic Publishers, 1980 4(1983), 2 vom: Apr., Seite 175-184 (DE-627)130523747 (DE-600)770632-7 (DE-576)016095987 0253-4827 nnns volume:4 year:1983 number:2 month:04 pages:175-184 https://doi.org/10.1007/BF01895442 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-MAT SSG-OPC-MAT GBV_ILN_11 GBV_ILN_20 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2006 GBV_ILN_2088 GBV_ILN_4310 AR 4 1983 2 04 175-184 |
allfieldsGer |
10.1007/BF01895442 doi (DE-627)OLC2042828807 (DE-He213)BF01895442-p DE-627 ger DE-627 rakwb eng 510 VZ Yu-Chiu, Long verfasserin aut Subregion generalized variational principles for elastic thick plates 1983 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Techmodern Business Promotion 1983 Abstract In this paper, the subregion generalized variational principle for elastic thick plates is proposed. Its main points may be stated as follows:Each subregion may be assigned arbitrarily as a potential region or complementary region. The subregion variational principles of potential energy, complementary energy and mixed energy represent three special forms of this principle.The number of independent variational variables in each subregion may be assigned arbitrarily. Any one of the subregions may be assigned, as a one-variable-region, two-variable-region or three-variable-region.The conjunction conditions of displacements and stresses on each interline of neighbouring subregions may be relaxed. On the basis of this principle the finite element analysis of non-conforming elements for thick plates can be formulated. Different finite element models for thick plates can be obtained by different applications of this principle. In particular, the subregion mixed variational principle for thick plates may be applied to formulating the subregion mixed finite element method for thick plates. Finite Element Method Potential Energy Element Model Finite Element Analysis Finite Element Model Enthalten in Ying yong shu xue he li xue / English edition Kluwer Academic Publishers, 1980 4(1983), 2 vom: Apr., Seite 175-184 (DE-627)130523747 (DE-600)770632-7 (DE-576)016095987 0253-4827 nnns volume:4 year:1983 number:2 month:04 pages:175-184 https://doi.org/10.1007/BF01895442 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-MAT SSG-OPC-MAT GBV_ILN_11 GBV_ILN_20 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2006 GBV_ILN_2088 GBV_ILN_4310 AR 4 1983 2 04 175-184 |
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10.1007/BF01895442 doi (DE-627)OLC2042828807 (DE-He213)BF01895442-p DE-627 ger DE-627 rakwb eng 510 VZ Yu-Chiu, Long verfasserin aut Subregion generalized variational principles for elastic thick plates 1983 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Techmodern Business Promotion 1983 Abstract In this paper, the subregion generalized variational principle for elastic thick plates is proposed. Its main points may be stated as follows:Each subregion may be assigned arbitrarily as a potential region or complementary region. The subregion variational principles of potential energy, complementary energy and mixed energy represent three special forms of this principle.The number of independent variational variables in each subregion may be assigned arbitrarily. Any one of the subregions may be assigned, as a one-variable-region, two-variable-region or three-variable-region.The conjunction conditions of displacements and stresses on each interline of neighbouring subregions may be relaxed. On the basis of this principle the finite element analysis of non-conforming elements for thick plates can be formulated. Different finite element models for thick plates can be obtained by different applications of this principle. In particular, the subregion mixed variational principle for thick plates may be applied to formulating the subregion mixed finite element method for thick plates. Finite Element Method Potential Energy Element Model Finite Element Analysis Finite Element Model Enthalten in Ying yong shu xue he li xue / English edition Kluwer Academic Publishers, 1980 4(1983), 2 vom: Apr., Seite 175-184 (DE-627)130523747 (DE-600)770632-7 (DE-576)016095987 0253-4827 nnns volume:4 year:1983 number:2 month:04 pages:175-184 https://doi.org/10.1007/BF01895442 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-MAT SSG-OPC-MAT GBV_ILN_11 GBV_ILN_20 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2006 GBV_ILN_2088 GBV_ILN_4310 AR 4 1983 2 04 175-184 |
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Abstract In this paper, the subregion generalized variational principle for elastic thick plates is proposed. Its main points may be stated as follows:Each subregion may be assigned arbitrarily as a potential region or complementary region. The subregion variational principles of potential energy, complementary energy and mixed energy represent three special forms of this principle.The number of independent variational variables in each subregion may be assigned arbitrarily. Any one of the subregions may be assigned, as a one-variable-region, two-variable-region or three-variable-region.The conjunction conditions of displacements and stresses on each interline of neighbouring subregions may be relaxed. On the basis of this principle the finite element analysis of non-conforming elements for thick plates can be formulated. Different finite element models for thick plates can be obtained by different applications of this principle. In particular, the subregion mixed variational principle for thick plates may be applied to formulating the subregion mixed finite element method for thick plates. © Techmodern Business Promotion 1983 |
abstractGer |
Abstract In this paper, the subregion generalized variational principle for elastic thick plates is proposed. Its main points may be stated as follows:Each subregion may be assigned arbitrarily as a potential region or complementary region. The subregion variational principles of potential energy, complementary energy and mixed energy represent three special forms of this principle.The number of independent variational variables in each subregion may be assigned arbitrarily. Any one of the subregions may be assigned, as a one-variable-region, two-variable-region or three-variable-region.The conjunction conditions of displacements and stresses on each interline of neighbouring subregions may be relaxed. On the basis of this principle the finite element analysis of non-conforming elements for thick plates can be formulated. Different finite element models for thick plates can be obtained by different applications of this principle. In particular, the subregion mixed variational principle for thick plates may be applied to formulating the subregion mixed finite element method for thick plates. © Techmodern Business Promotion 1983 |
abstract_unstemmed |
Abstract In this paper, the subregion generalized variational principle for elastic thick plates is proposed. Its main points may be stated as follows:Each subregion may be assigned arbitrarily as a potential region or complementary region. The subregion variational principles of potential energy, complementary energy and mixed energy represent three special forms of this principle.The number of independent variational variables in each subregion may be assigned arbitrarily. Any one of the subregions may be assigned, as a one-variable-region, two-variable-region or three-variable-region.The conjunction conditions of displacements and stresses on each interline of neighbouring subregions may be relaxed. On the basis of this principle the finite element analysis of non-conforming elements for thick plates can be formulated. Different finite element models for thick plates can be obtained by different applications of this principle. In particular, the subregion mixed variational principle for thick plates may be applied to formulating the subregion mixed finite element method for thick plates. © Techmodern Business Promotion 1983 |
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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">OLC2042828807</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230502204034.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200820s1983 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/BF01895442</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2042828807</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)BF01895442-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">510</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Yu-Chiu, Long</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Subregion generalized variational principles for elastic thick plates</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1983</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">© Techmodern Business Promotion 1983</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract In this paper, the subregion generalized variational principle for elastic thick plates is proposed. Its main points may be stated as follows:Each subregion may be assigned arbitrarily as a potential region or complementary region. The subregion variational principles of potential energy, complementary energy and mixed energy represent three special forms of this principle.The number of independent variational variables in each subregion may be assigned arbitrarily. Any one of the subregions may be assigned, as a one-variable-region, two-variable-region or three-variable-region.The conjunction conditions of displacements and stresses on each interline of neighbouring subregions may be relaxed. On the basis of this principle the finite element analysis of non-conforming elements for thick plates can be formulated. Different finite element models for thick plates can be obtained by different applications of this principle. In particular, the subregion mixed variational principle for thick plates may be applied to formulating the subregion mixed finite element method for thick plates.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Finite Element Method</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Potential Energy</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Element Model</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Finite Element Analysis</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Finite Element Model</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Ying yong shu xue he li xue / English edition</subfield><subfield code="d">Kluwer Academic Publishers, 1980</subfield><subfield code="g">4(1983), 2 vom: Apr., Seite 175-184</subfield><subfield code="w">(DE-627)130523747</subfield><subfield code="w">(DE-600)770632-7</subfield><subfield code="w">(DE-576)016095987</subfield><subfield code="x">0253-4827</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:4</subfield><subfield code="g">year:1983</subfield><subfield code="g">number:2</subfield><subfield code="g">month:04</subfield><subfield code="g">pages:175-184</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/BF01895442</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-MAT</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OPC-MAT</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_11</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2006</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2088</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4310</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">4</subfield><subfield code="j">1983</subfield><subfield code="e">2</subfield><subfield code="c">04</subfield><subfield code="h">175-184</subfield></datafield></record></collection>
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