A comparison among Neo-Hookean model, Mooney-Rivlin model, and Ogden model for chloroprene rubber
Abstract Neo-Hookean model and Mooney-Rivlin model are hyperelastic material models where the strain energy density function is made from invariants of the left Cauchy-Green deformation tensor. Even though Ogden model is a hyperelastic material model, its strain energy density function is expressed...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Kim, Beomkeun [verfasserIn] Lee, Seong Beom [verfasserIn] Lee, Jayone [verfasserIn] Cho, Sehyun [verfasserIn] Park, Hyungmin [verfasserIn] Yeom, Sanghoon [verfasserIn] Park, Sung Han [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2012 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: International journal of precision engineering and manufacturing - Sŏul : KSPE, 2009, 13(2012), 5 vom: Mai, Seite 759-764 |
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| Übergeordnetes Werk: |
volume:13 ; year:2012 ; number:5 ; month:05 ; pages:759-764 |
| Links: |
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| DOI / URN: |
10.1007/s12541-012-0099-y |
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| Katalog-ID: |
SPR02608869X |
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| 245 | 1 | 2 | |a A comparison among Neo-Hookean model, Mooney-Rivlin model, and Ogden model for chloroprene rubber |
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| 520 | |a Abstract Neo-Hookean model and Mooney-Rivlin model are hyperelastic material models where the strain energy density function is made from invariants of the left Cauchy-Green deformation tensor. Even though Ogden model is a hyperelastic material model, its strain energy density function is expressed by principal stretch ratio. These three models have been widely used in industries. Recently, Ogden model, especially Ogden 3rd model, shows better agreement with the test data than others. In spite of the limitations to describe particular stress states, it is known that reasonable results using these models can be obtained for various structural components. In this research, three kinds of models are considered for Chloroprene rubber. Three kinds of tests (Uniaxial tension test, Biaxial tension test, and Planar shear test) are performed for Chloroprene specimen and through four kinds of test combinations (Uni+Bi, Uni+Pl, Bi+Pl, Uni+Bi+Pl), numerical simulations are carried out for Neo-Hookean model, Mooney-Rivlin model, and Ogden model. It is shown that Mooney-Rivlin model and Ogden model can be used for Chloroprene Rubber in the specific ranges for Isotropic Hyperelastic model. | ||
| 650 | 4 | |a Hyperelastic model |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Neo-Hookean model |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Mooney-Rivlin model |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Ogden model |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Chloroprene rubber |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Uniaxial test |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Biaxial test |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Planar test |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Lee, Seong Beom |e verfasserin |4 aut | |
| 700 | 1 | |a Lee, Jayone |e verfasserin |4 aut | |
| 700 | 1 | |a Cho, Sehyun |e verfasserin |4 aut | |
| 700 | 1 | |a Park, Hyungmin |e verfasserin |4 aut | |
| 700 | 1 | |a Yeom, Sanghoon |e verfasserin |4 aut | |
| 700 | 1 | |a Park, Sung Han |e verfasserin |4 aut | |
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10.1007/s12541-012-0099-y doi (DE-627)SPR02608869X (SPR)s12541-012-0099-y-e DE-627 ger DE-627 rakwb eng 600 ASE Kim, Beomkeun verfasserin aut A comparison among Neo-Hookean model, Mooney-Rivlin model, and Ogden model for chloroprene rubber 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Neo-Hookean model and Mooney-Rivlin model are hyperelastic material models where the strain energy density function is made from invariants of the left Cauchy-Green deformation tensor. Even though Ogden model is a hyperelastic material model, its strain energy density function is expressed by principal stretch ratio. These three models have been widely used in industries. Recently, Ogden model, especially Ogden 3rd model, shows better agreement with the test data than others. In spite of the limitations to describe particular stress states, it is known that reasonable results using these models can be obtained for various structural components. In this research, three kinds of models are considered for Chloroprene rubber. Three kinds of tests (Uniaxial tension test, Biaxial tension test, and Planar shear test) are performed for Chloroprene specimen and through four kinds of test combinations (Uni+Bi, Uni+Pl, Bi+Pl, Uni+Bi+Pl), numerical simulations are carried out for Neo-Hookean model, Mooney-Rivlin model, and Ogden model. It is shown that Mooney-Rivlin model and Ogden model can be used for Chloroprene Rubber in the specific ranges for Isotropic Hyperelastic model. Hyperelastic model (dpeaa)DE-He213 Neo-Hookean model (dpeaa)DE-He213 Mooney-Rivlin model (dpeaa)DE-He213 Ogden model (dpeaa)DE-He213 Chloroprene rubber (dpeaa)DE-He213 Uniaxial test (dpeaa)DE-He213 Biaxial test (dpeaa)DE-He213 Planar test (dpeaa)DE-He213 Lee, Seong Beom verfasserin aut Lee, Jayone verfasserin aut Cho, Sehyun verfasserin aut Park, Hyungmin verfasserin aut Yeom, Sanghoon verfasserin aut Park, Sung Han verfasserin aut Enthalten in International journal of precision engineering and manufacturing Sŏul : KSPE, 2009 13(2012), 5 vom: Mai, Seite 759-764 (DE-627)609403109 (DE-600)2515436-9 2005-4602 nnns volume:13 year:2012 number:5 month:05 pages:759-764 https://dx.doi.org/10.1007/s12541-012-0099-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 13 2012 5 05 759-764 |
| spelling |
10.1007/s12541-012-0099-y doi (DE-627)SPR02608869X (SPR)s12541-012-0099-y-e DE-627 ger DE-627 rakwb eng 600 ASE Kim, Beomkeun verfasserin aut A comparison among Neo-Hookean model, Mooney-Rivlin model, and Ogden model for chloroprene rubber 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Neo-Hookean model and Mooney-Rivlin model are hyperelastic material models where the strain energy density function is made from invariants of the left Cauchy-Green deformation tensor. Even though Ogden model is a hyperelastic material model, its strain energy density function is expressed by principal stretch ratio. These three models have been widely used in industries. Recently, Ogden model, especially Ogden 3rd model, shows better agreement with the test data than others. In spite of the limitations to describe particular stress states, it is known that reasonable results using these models can be obtained for various structural components. In this research, three kinds of models are considered for Chloroprene rubber. Three kinds of tests (Uniaxial tension test, Biaxial tension test, and Planar shear test) are performed for Chloroprene specimen and through four kinds of test combinations (Uni+Bi, Uni+Pl, Bi+Pl, Uni+Bi+Pl), numerical simulations are carried out for Neo-Hookean model, Mooney-Rivlin model, and Ogden model. It is shown that Mooney-Rivlin model and Ogden model can be used for Chloroprene Rubber in the specific ranges for Isotropic Hyperelastic model. Hyperelastic model (dpeaa)DE-He213 Neo-Hookean model (dpeaa)DE-He213 Mooney-Rivlin model (dpeaa)DE-He213 Ogden model (dpeaa)DE-He213 Chloroprene rubber (dpeaa)DE-He213 Uniaxial test (dpeaa)DE-He213 Biaxial test (dpeaa)DE-He213 Planar test (dpeaa)DE-He213 Lee, Seong Beom verfasserin aut Lee, Jayone verfasserin aut Cho, Sehyun verfasserin aut Park, Hyungmin verfasserin aut Yeom, Sanghoon verfasserin aut Park, Sung Han verfasserin aut Enthalten in International journal of precision engineering and manufacturing Sŏul : KSPE, 2009 13(2012), 5 vom: Mai, Seite 759-764 (DE-627)609403109 (DE-600)2515436-9 2005-4602 nnns volume:13 year:2012 number:5 month:05 pages:759-764 https://dx.doi.org/10.1007/s12541-012-0099-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 13 2012 5 05 759-764 |
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10.1007/s12541-012-0099-y doi (DE-627)SPR02608869X (SPR)s12541-012-0099-y-e DE-627 ger DE-627 rakwb eng 600 ASE Kim, Beomkeun verfasserin aut A comparison among Neo-Hookean model, Mooney-Rivlin model, and Ogden model for chloroprene rubber 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Neo-Hookean model and Mooney-Rivlin model are hyperelastic material models where the strain energy density function is made from invariants of the left Cauchy-Green deformation tensor. Even though Ogden model is a hyperelastic material model, its strain energy density function is expressed by principal stretch ratio. These three models have been widely used in industries. Recently, Ogden model, especially Ogden 3rd model, shows better agreement with the test data than others. In spite of the limitations to describe particular stress states, it is known that reasonable results using these models can be obtained for various structural components. In this research, three kinds of models are considered for Chloroprene rubber. Three kinds of tests (Uniaxial tension test, Biaxial tension test, and Planar shear test) are performed for Chloroprene specimen and through four kinds of test combinations (Uni+Bi, Uni+Pl, Bi+Pl, Uni+Bi+Pl), numerical simulations are carried out for Neo-Hookean model, Mooney-Rivlin model, and Ogden model. It is shown that Mooney-Rivlin model and Ogden model can be used for Chloroprene Rubber in the specific ranges for Isotropic Hyperelastic model. Hyperelastic model (dpeaa)DE-He213 Neo-Hookean model (dpeaa)DE-He213 Mooney-Rivlin model (dpeaa)DE-He213 Ogden model (dpeaa)DE-He213 Chloroprene rubber (dpeaa)DE-He213 Uniaxial test (dpeaa)DE-He213 Biaxial test (dpeaa)DE-He213 Planar test (dpeaa)DE-He213 Lee, Seong Beom verfasserin aut Lee, Jayone verfasserin aut Cho, Sehyun verfasserin aut Park, Hyungmin verfasserin aut Yeom, Sanghoon verfasserin aut Park, Sung Han verfasserin aut Enthalten in International journal of precision engineering and manufacturing Sŏul : KSPE, 2009 13(2012), 5 vom: Mai, Seite 759-764 (DE-627)609403109 (DE-600)2515436-9 2005-4602 nnns volume:13 year:2012 number:5 month:05 pages:759-764 https://dx.doi.org/10.1007/s12541-012-0099-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 13 2012 5 05 759-764 |
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10.1007/s12541-012-0099-y doi (DE-627)SPR02608869X (SPR)s12541-012-0099-y-e DE-627 ger DE-627 rakwb eng 600 ASE Kim, Beomkeun verfasserin aut A comparison among Neo-Hookean model, Mooney-Rivlin model, and Ogden model for chloroprene rubber 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Neo-Hookean model and Mooney-Rivlin model are hyperelastic material models where the strain energy density function is made from invariants of the left Cauchy-Green deformation tensor. Even though Ogden model is a hyperelastic material model, its strain energy density function is expressed by principal stretch ratio. These three models have been widely used in industries. Recently, Ogden model, especially Ogden 3rd model, shows better agreement with the test data than others. In spite of the limitations to describe particular stress states, it is known that reasonable results using these models can be obtained for various structural components. In this research, three kinds of models are considered for Chloroprene rubber. Three kinds of tests (Uniaxial tension test, Biaxial tension test, and Planar shear test) are performed for Chloroprene specimen and through four kinds of test combinations (Uni+Bi, Uni+Pl, Bi+Pl, Uni+Bi+Pl), numerical simulations are carried out for Neo-Hookean model, Mooney-Rivlin model, and Ogden model. It is shown that Mooney-Rivlin model and Ogden model can be used for Chloroprene Rubber in the specific ranges for Isotropic Hyperelastic model. Hyperelastic model (dpeaa)DE-He213 Neo-Hookean model (dpeaa)DE-He213 Mooney-Rivlin model (dpeaa)DE-He213 Ogden model (dpeaa)DE-He213 Chloroprene rubber (dpeaa)DE-He213 Uniaxial test (dpeaa)DE-He213 Biaxial test (dpeaa)DE-He213 Planar test (dpeaa)DE-He213 Lee, Seong Beom verfasserin aut Lee, Jayone verfasserin aut Cho, Sehyun verfasserin aut Park, Hyungmin verfasserin aut Yeom, Sanghoon verfasserin aut Park, Sung Han verfasserin aut Enthalten in International journal of precision engineering and manufacturing Sŏul : KSPE, 2009 13(2012), 5 vom: Mai, Seite 759-764 (DE-627)609403109 (DE-600)2515436-9 2005-4602 nnns volume:13 year:2012 number:5 month:05 pages:759-764 https://dx.doi.org/10.1007/s12541-012-0099-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 13 2012 5 05 759-764 |
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10.1007/s12541-012-0099-y doi (DE-627)SPR02608869X (SPR)s12541-012-0099-y-e DE-627 ger DE-627 rakwb eng 600 ASE Kim, Beomkeun verfasserin aut A comparison among Neo-Hookean model, Mooney-Rivlin model, and Ogden model for chloroprene rubber 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Neo-Hookean model and Mooney-Rivlin model are hyperelastic material models where the strain energy density function is made from invariants of the left Cauchy-Green deformation tensor. Even though Ogden model is a hyperelastic material model, its strain energy density function is expressed by principal stretch ratio. These three models have been widely used in industries. Recently, Ogden model, especially Ogden 3rd model, shows better agreement with the test data than others. In spite of the limitations to describe particular stress states, it is known that reasonable results using these models can be obtained for various structural components. In this research, three kinds of models are considered for Chloroprene rubber. Three kinds of tests (Uniaxial tension test, Biaxial tension test, and Planar shear test) are performed for Chloroprene specimen and through four kinds of test combinations (Uni+Bi, Uni+Pl, Bi+Pl, Uni+Bi+Pl), numerical simulations are carried out for Neo-Hookean model, Mooney-Rivlin model, and Ogden model. It is shown that Mooney-Rivlin model and Ogden model can be used for Chloroprene Rubber in the specific ranges for Isotropic Hyperelastic model. Hyperelastic model (dpeaa)DE-He213 Neo-Hookean model (dpeaa)DE-He213 Mooney-Rivlin model (dpeaa)DE-He213 Ogden model (dpeaa)DE-He213 Chloroprene rubber (dpeaa)DE-He213 Uniaxial test (dpeaa)DE-He213 Biaxial test (dpeaa)DE-He213 Planar test (dpeaa)DE-He213 Lee, Seong Beom verfasserin aut Lee, Jayone verfasserin aut Cho, Sehyun verfasserin aut Park, Hyungmin verfasserin aut Yeom, Sanghoon verfasserin aut Park, Sung Han verfasserin aut Enthalten in International journal of precision engineering and manufacturing Sŏul : KSPE, 2009 13(2012), 5 vom: Mai, Seite 759-764 (DE-627)609403109 (DE-600)2515436-9 2005-4602 nnns volume:13 year:2012 number:5 month:05 pages:759-764 https://dx.doi.org/10.1007/s12541-012-0099-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 13 2012 5 05 759-764 |
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Enthalten in International journal of precision engineering and manufacturing 13(2012), 5 vom: Mai, Seite 759-764 volume:13 year:2012 number:5 month:05 pages:759-764 |
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Hyperelastic model Neo-Hookean model Mooney-Rivlin model Ogden model Chloroprene rubber Uniaxial test Biaxial test Planar test |
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Kim, Beomkeun @@aut@@ Lee, Seong Beom @@aut@@ Lee, Jayone @@aut@@ Cho, Sehyun @@aut@@ Park, Hyungmin @@aut@@ Yeom, Sanghoon @@aut@@ Park, Sung Han @@aut@@ |
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Even though Ogden model is a hyperelastic material model, its strain energy density function is expressed by principal stretch ratio. These three models have been widely used in industries. Recently, Ogden model, especially Ogden 3rd model, shows better agreement with the test data than others. In spite of the limitations to describe particular stress states, it is known that reasonable results using these models can be obtained for various structural components. In this research, three kinds of models are considered for Chloroprene rubber. Three kinds of tests (Uniaxial tension test, Biaxial tension test, and Planar shear test) are performed for Chloroprene specimen and through four kinds of test combinations (Uni+Bi, Uni+Pl, Bi+Pl, Uni+Bi+Pl), numerical simulations are carried out for Neo-Hookean model, Mooney-Rivlin model, and Ogden model. 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Kim, Beomkeun |
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Kim, Beomkeun ddc 600 misc Hyperelastic model misc Neo-Hookean model misc Mooney-Rivlin model misc Ogden model misc Chloroprene rubber misc Uniaxial test misc Biaxial test misc Planar test A comparison among Neo-Hookean model, Mooney-Rivlin model, and Ogden model for chloroprene rubber |
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600 ASE A comparison among Neo-Hookean model, Mooney-Rivlin model, and Ogden model for chloroprene rubber Hyperelastic model (dpeaa)DE-He213 Neo-Hookean model (dpeaa)DE-He213 Mooney-Rivlin model (dpeaa)DE-He213 Ogden model (dpeaa)DE-He213 Chloroprene rubber (dpeaa)DE-He213 Uniaxial test (dpeaa)DE-He213 Biaxial test (dpeaa)DE-He213 Planar test (dpeaa)DE-He213 |
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ddc 600 misc Hyperelastic model misc Neo-Hookean model misc Mooney-Rivlin model misc Ogden model misc Chloroprene rubber misc Uniaxial test misc Biaxial test misc Planar test |
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A comparison among Neo-Hookean model, Mooney-Rivlin model, and Ogden model for chloroprene rubber |
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A comparison among Neo-Hookean model, Mooney-Rivlin model, and Ogden model for chloroprene rubber |
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Kim, Beomkeun |
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Kim, Beomkeun Lee, Seong Beom Lee, Jayone Cho, Sehyun Park, Hyungmin Yeom, Sanghoon Park, Sung Han |
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Kim, Beomkeun |
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10.1007/s12541-012-0099-y |
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| title_sort |
comparison among neo-hookean model, mooney-rivlin model, and ogden model for chloroprene rubber |
| title_auth |
A comparison among Neo-Hookean model, Mooney-Rivlin model, and Ogden model for chloroprene rubber |
| abstract |
Abstract Neo-Hookean model and Mooney-Rivlin model are hyperelastic material models where the strain energy density function is made from invariants of the left Cauchy-Green deformation tensor. Even though Ogden model is a hyperelastic material model, its strain energy density function is expressed by principal stretch ratio. These three models have been widely used in industries. Recently, Ogden model, especially Ogden 3rd model, shows better agreement with the test data than others. In spite of the limitations to describe particular stress states, it is known that reasonable results using these models can be obtained for various structural components. In this research, three kinds of models are considered for Chloroprene rubber. Three kinds of tests (Uniaxial tension test, Biaxial tension test, and Planar shear test) are performed for Chloroprene specimen and through four kinds of test combinations (Uni+Bi, Uni+Pl, Bi+Pl, Uni+Bi+Pl), numerical simulations are carried out for Neo-Hookean model, Mooney-Rivlin model, and Ogden model. It is shown that Mooney-Rivlin model and Ogden model can be used for Chloroprene Rubber in the specific ranges for Isotropic Hyperelastic model. |
| abstractGer |
Abstract Neo-Hookean model and Mooney-Rivlin model are hyperelastic material models where the strain energy density function is made from invariants of the left Cauchy-Green deformation tensor. Even though Ogden model is a hyperelastic material model, its strain energy density function is expressed by principal stretch ratio. These three models have been widely used in industries. Recently, Ogden model, especially Ogden 3rd model, shows better agreement with the test data than others. In spite of the limitations to describe particular stress states, it is known that reasonable results using these models can be obtained for various structural components. In this research, three kinds of models are considered for Chloroprene rubber. Three kinds of tests (Uniaxial tension test, Biaxial tension test, and Planar shear test) are performed for Chloroprene specimen and through four kinds of test combinations (Uni+Bi, Uni+Pl, Bi+Pl, Uni+Bi+Pl), numerical simulations are carried out for Neo-Hookean model, Mooney-Rivlin model, and Ogden model. It is shown that Mooney-Rivlin model and Ogden model can be used for Chloroprene Rubber in the specific ranges for Isotropic Hyperelastic model. |
| abstract_unstemmed |
Abstract Neo-Hookean model and Mooney-Rivlin model are hyperelastic material models where the strain energy density function is made from invariants of the left Cauchy-Green deformation tensor. Even though Ogden model is a hyperelastic material model, its strain energy density function is expressed by principal stretch ratio. These three models have been widely used in industries. Recently, Ogden model, especially Ogden 3rd model, shows better agreement with the test data than others. In spite of the limitations to describe particular stress states, it is known that reasonable results using these models can be obtained for various structural components. In this research, three kinds of models are considered for Chloroprene rubber. Three kinds of tests (Uniaxial tension test, Biaxial tension test, and Planar shear test) are performed for Chloroprene specimen and through four kinds of test combinations (Uni+Bi, Uni+Pl, Bi+Pl, Uni+Bi+Pl), numerical simulations are carried out for Neo-Hookean model, Mooney-Rivlin model, and Ogden model. It is shown that Mooney-Rivlin model and Ogden model can be used for Chloroprene Rubber in the specific ranges for Isotropic Hyperelastic model. |
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5 |
| title_short |
A comparison among Neo-Hookean model, Mooney-Rivlin model, and Ogden model for chloroprene rubber |
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https://dx.doi.org/10.1007/s12541-012-0099-y |
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Lee, Seong Beom Lee, Jayone Cho, Sehyun Park, Hyungmin Yeom, Sanghoon Park, Sung Han |
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| score |
7.401725 |