Torsional vibrations in systems with combined dry friction
Abstract We consider an example of torsional vibrations of a vertically located cylindrical rod one of whose ends is elastically fixed and the other end rests on an infinite band moving at a constant velocity. We compare the main models of dry friction, such as “pure” dry friction and “viscous” fric...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Kireenkov, A. A. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2009 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Mechanics of solids - New York, NY : Allerton, 2007, 44(2009), 3 vom: Juni, Seite 361-365 |
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| Übergeordnetes Werk: |
volume:44 ; year:2009 ; number:3 ; month:06 ; pages:361-365 |
| Links: |
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| DOI / URN: |
10.3103/S0025654409030042 |
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| Katalog-ID: |
SPR023255684 |
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| 520 | |a Abstract We consider an example of torsional vibrations of a vertically located cylindrical rod one of whose ends is elastically fixed and the other end rests on an infinite band moving at a constant velocity. We compare the main models of dry friction, such as “pure” dry friction and “viscous” friction, and the models based on the Padé expansions of the corresponding order. We show that the model based on linear-fractional Padé expansions of the exact integral model, which is written under the assumption that the Coulomb law in differential form is true, is the simplest form of the model of combined dry friction, which gives correct results, while the models of pure dry and viscous friction cannot provide correct descriptions of the effects of combined dry friction. | ||
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10.3103/S0025654409030042 doi (DE-627)SPR023255684 (SPR)S0025654409030042-e DE-627 ger DE-627 rakwb eng 600 ASE Kireenkov, A. A. verfasserin aut Torsional vibrations in systems with combined dry friction 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We consider an example of torsional vibrations of a vertically located cylindrical rod one of whose ends is elastically fixed and the other end rests on an infinite band moving at a constant velocity. We compare the main models of dry friction, such as “pure” dry friction and “viscous” friction, and the models based on the Padé expansions of the corresponding order. We show that the model based on linear-fractional Padé expansions of the exact integral model, which is written under the assumption that the Coulomb law in differential form is true, is the simplest form of the model of combined dry friction, which gives correct results, while the models of pure dry and viscous friction cannot provide correct descriptions of the effects of combined dry friction. Friction Model (dpeaa)DE-He213 Torsional Vibration (dpeaa)DE-He213 Viscous Friction (dpeaa)DE-He213 Contact Spot (dpeaa)DE-He213 Normal Contact Stress (dpeaa)DE-He213 Enthalten in Mechanics of solids New York, NY : Allerton, 2007 44(2009), 3 vom: Juni, Seite 361-365 (DE-627)535186789 (DE-600)2375720-6 1934-7936 nnns volume:44 year:2009 number:3 month:06 pages:361-365 https://dx.doi.org/10.3103/S0025654409030042 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 44 2009 3 06 361-365 |
| spelling |
10.3103/S0025654409030042 doi (DE-627)SPR023255684 (SPR)S0025654409030042-e DE-627 ger DE-627 rakwb eng 600 ASE Kireenkov, A. A. verfasserin aut Torsional vibrations in systems with combined dry friction 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We consider an example of torsional vibrations of a vertically located cylindrical rod one of whose ends is elastically fixed and the other end rests on an infinite band moving at a constant velocity. We compare the main models of dry friction, such as “pure” dry friction and “viscous” friction, and the models based on the Padé expansions of the corresponding order. We show that the model based on linear-fractional Padé expansions of the exact integral model, which is written under the assumption that the Coulomb law in differential form is true, is the simplest form of the model of combined dry friction, which gives correct results, while the models of pure dry and viscous friction cannot provide correct descriptions of the effects of combined dry friction. Friction Model (dpeaa)DE-He213 Torsional Vibration (dpeaa)DE-He213 Viscous Friction (dpeaa)DE-He213 Contact Spot (dpeaa)DE-He213 Normal Contact Stress (dpeaa)DE-He213 Enthalten in Mechanics of solids New York, NY : Allerton, 2007 44(2009), 3 vom: Juni, Seite 361-365 (DE-627)535186789 (DE-600)2375720-6 1934-7936 nnns volume:44 year:2009 number:3 month:06 pages:361-365 https://dx.doi.org/10.3103/S0025654409030042 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 44 2009 3 06 361-365 |
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10.3103/S0025654409030042 doi (DE-627)SPR023255684 (SPR)S0025654409030042-e DE-627 ger DE-627 rakwb eng 600 ASE Kireenkov, A. A. verfasserin aut Torsional vibrations in systems with combined dry friction 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We consider an example of torsional vibrations of a vertically located cylindrical rod one of whose ends is elastically fixed and the other end rests on an infinite band moving at a constant velocity. We compare the main models of dry friction, such as “pure” dry friction and “viscous” friction, and the models based on the Padé expansions of the corresponding order. We show that the model based on linear-fractional Padé expansions of the exact integral model, which is written under the assumption that the Coulomb law in differential form is true, is the simplest form of the model of combined dry friction, which gives correct results, while the models of pure dry and viscous friction cannot provide correct descriptions of the effects of combined dry friction. Friction Model (dpeaa)DE-He213 Torsional Vibration (dpeaa)DE-He213 Viscous Friction (dpeaa)DE-He213 Contact Spot (dpeaa)DE-He213 Normal Contact Stress (dpeaa)DE-He213 Enthalten in Mechanics of solids New York, NY : Allerton, 2007 44(2009), 3 vom: Juni, Seite 361-365 (DE-627)535186789 (DE-600)2375720-6 1934-7936 nnns volume:44 year:2009 number:3 month:06 pages:361-365 https://dx.doi.org/10.3103/S0025654409030042 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 44 2009 3 06 361-365 |
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10.3103/S0025654409030042 doi (DE-627)SPR023255684 (SPR)S0025654409030042-e DE-627 ger DE-627 rakwb eng 600 ASE Kireenkov, A. A. verfasserin aut Torsional vibrations in systems with combined dry friction 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We consider an example of torsional vibrations of a vertically located cylindrical rod one of whose ends is elastically fixed and the other end rests on an infinite band moving at a constant velocity. We compare the main models of dry friction, such as “pure” dry friction and “viscous” friction, and the models based on the Padé expansions of the corresponding order. We show that the model based on linear-fractional Padé expansions of the exact integral model, which is written under the assumption that the Coulomb law in differential form is true, is the simplest form of the model of combined dry friction, which gives correct results, while the models of pure dry and viscous friction cannot provide correct descriptions of the effects of combined dry friction. Friction Model (dpeaa)DE-He213 Torsional Vibration (dpeaa)DE-He213 Viscous Friction (dpeaa)DE-He213 Contact Spot (dpeaa)DE-He213 Normal Contact Stress (dpeaa)DE-He213 Enthalten in Mechanics of solids New York, NY : Allerton, 2007 44(2009), 3 vom: Juni, Seite 361-365 (DE-627)535186789 (DE-600)2375720-6 1934-7936 nnns volume:44 year:2009 number:3 month:06 pages:361-365 https://dx.doi.org/10.3103/S0025654409030042 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 44 2009 3 06 361-365 |
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10.3103/S0025654409030042 doi (DE-627)SPR023255684 (SPR)S0025654409030042-e DE-627 ger DE-627 rakwb eng 600 ASE Kireenkov, A. A. verfasserin aut Torsional vibrations in systems with combined dry friction 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We consider an example of torsional vibrations of a vertically located cylindrical rod one of whose ends is elastically fixed and the other end rests on an infinite band moving at a constant velocity. We compare the main models of dry friction, such as “pure” dry friction and “viscous” friction, and the models based on the Padé expansions of the corresponding order. We show that the model based on linear-fractional Padé expansions of the exact integral model, which is written under the assumption that the Coulomb law in differential form is true, is the simplest form of the model of combined dry friction, which gives correct results, while the models of pure dry and viscous friction cannot provide correct descriptions of the effects of combined dry friction. Friction Model (dpeaa)DE-He213 Torsional Vibration (dpeaa)DE-He213 Viscous Friction (dpeaa)DE-He213 Contact Spot (dpeaa)DE-He213 Normal Contact Stress (dpeaa)DE-He213 Enthalten in Mechanics of solids New York, NY : Allerton, 2007 44(2009), 3 vom: Juni, Seite 361-365 (DE-627)535186789 (DE-600)2375720-6 1934-7936 nnns volume:44 year:2009 number:3 month:06 pages:361-365 https://dx.doi.org/10.3103/S0025654409030042 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 44 2009 3 06 361-365 |
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Enthalten in Mechanics of solids 44(2009), 3 vom: Juni, Seite 361-365 volume:44 year:2009 number:3 month:06 pages:361-365 |
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Kireenkov, A. A. |
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Kireenkov, A. A. ddc 600 misc Friction Model misc Torsional Vibration misc Viscous Friction misc Contact Spot misc Normal Contact Stress Torsional vibrations in systems with combined dry friction |
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600 ASE Torsional vibrations in systems with combined dry friction Friction Model (dpeaa)DE-He213 Torsional Vibration (dpeaa)DE-He213 Viscous Friction (dpeaa)DE-He213 Contact Spot (dpeaa)DE-He213 Normal Contact Stress (dpeaa)DE-He213 |
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Torsional vibrations in systems with combined dry friction |
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torsional vibrations in systems with combined dry friction |
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Torsional vibrations in systems with combined dry friction |
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Abstract We consider an example of torsional vibrations of a vertically located cylindrical rod one of whose ends is elastically fixed and the other end rests on an infinite band moving at a constant velocity. We compare the main models of dry friction, such as “pure” dry friction and “viscous” friction, and the models based on the Padé expansions of the corresponding order. We show that the model based on linear-fractional Padé expansions of the exact integral model, which is written under the assumption that the Coulomb law in differential form is true, is the simplest form of the model of combined dry friction, which gives correct results, while the models of pure dry and viscous friction cannot provide correct descriptions of the effects of combined dry friction. |
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Abstract We consider an example of torsional vibrations of a vertically located cylindrical rod one of whose ends is elastically fixed and the other end rests on an infinite band moving at a constant velocity. We compare the main models of dry friction, such as “pure” dry friction and “viscous” friction, and the models based on the Padé expansions of the corresponding order. We show that the model based on linear-fractional Padé expansions of the exact integral model, which is written under the assumption that the Coulomb law in differential form is true, is the simplest form of the model of combined dry friction, which gives correct results, while the models of pure dry and viscous friction cannot provide correct descriptions of the effects of combined dry friction. |
| abstract_unstemmed |
Abstract We consider an example of torsional vibrations of a vertically located cylindrical rod one of whose ends is elastically fixed and the other end rests on an infinite band moving at a constant velocity. We compare the main models of dry friction, such as “pure” dry friction and “viscous” friction, and the models based on the Padé expansions of the corresponding order. We show that the model based on linear-fractional Padé expansions of the exact integral model, which is written under the assumption that the Coulomb law in differential form is true, is the simplest form of the model of combined dry friction, which gives correct results, while the models of pure dry and viscous friction cannot provide correct descriptions of the effects of combined dry friction. |
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