Dry friction distributed over a contact patch between a rigid body and a visco-elastic plane
We consider the dynamics of an absolutely rigid body moving along a rough horizontal plane. We assume that the plane deforms during the motion so that the contact patch is non-planar and has non-zero, but comparatively small area. In the contact patch, the vertical reactions are proportional to the...
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Published in | Multibody system dynamics Vol. 45; no. 2; pp. 203 - 222 |
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Main Author | |
Format | Journal Article |
Language | English |
Published |
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15.02.2019
Springer Nature B.V |
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Abstract | We consider the dynamics of an absolutely rigid body moving along a rough horizontal plane. We assume that the plane deforms during the motion so that the contact patch is non-planar and has non-zero, but comparatively small area. In the contact patch, the vertical reactions are proportional to the vertical deformations and their rates, that is, we consider Kelvin–Voigt model. The tangent forces are assumed to be classic Coulomb dry friction in sliding regime (no stiction in contact patch). Due to the viscous part of Kelvin–Voigt law, the contact patch, the plane’s normal reaction, friction force and torque depend on the position, orientation, velocity of the center of mass and the angular velocity of the body. The model does not involve any additional dynamic parameter and gives the friction force and torque directly for any given state of the body. To show the advances of the model, we recall the analytical solution of Cauchy’s initial problem with general initial conditions of ODE governing the dynamics of the homogeneous sphere on a horizontal plane (results of Zobova and Treschev in Proc. Steklov Inst. Math. 281:91–118,
2013
). Here we generalize the model for arbitrary convex bodies and study its main properties. The model is compared to the continuous velocity-base friction model for pure sliding (Brown and McPhee in ASME J. Comput. Nonlinear Dyn. 11(5):054502,
2016
) and to the combined dry friction (Awrejcewicz and Kudra in Multibody Syst. Dyn.,
2018
,
https://doi.org/10.1007/s11044-018-9624-9
) in case of sliding with spinning. We illustrate the model considering the results of numerical integration of the Cauchy problem for a controlled differential-drive vehicle on a horizontal plane. |
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AbstractList | We consider the dynamics of an absolutely rigid body moving along a rough horizontal plane. We assume that the plane deforms during the motion so that the contact patch is non-planar and has non-zero, but comparatively small area. In the contact patch, the vertical reactions are proportional to the vertical deformations and their rates, that is, we consider Kelvin–Voigt model. The tangent forces are assumed to be classic Coulomb dry friction in sliding regime (no stiction in contact patch). Due to the viscous part of Kelvin–Voigt law, the contact patch, the plane’s normal reaction, friction force and torque depend on the position, orientation, velocity of the center of mass and the angular velocity of the body. The model does not involve any additional dynamic parameter and gives the friction force and torque directly for any given state of the body. To show the advances of the model, we recall the analytical solution of Cauchy’s initial problem with general initial conditions of ODE governing the dynamics of the homogeneous sphere on a horizontal plane (results of Zobova and Treschev in Proc. Steklov Inst. Math. 281:91–118, 2013). Here we generalize the model for arbitrary convex bodies and study its main properties. The model is compared to the continuous velocity-base friction model for pure sliding (Brown and McPhee in ASME J. Comput. Nonlinear Dyn. 11(5):054502, 2016) and to the combined dry friction (Awrejcewicz and Kudra in Multibody Syst. Dyn., 2018, https://doi.org/10.1007/s11044-018-9624-9) in case of sliding with spinning. We illustrate the model considering the results of numerical integration of the Cauchy problem for a controlled differential-drive vehicle on a horizontal plane. We consider the dynamics of an absolutely rigid body moving along a rough horizontal plane. We assume that the plane deforms during the motion so that the contact patch is non-planar and has non-zero, but comparatively small area. In the contact patch, the vertical reactions are proportional to the vertical deformations and their rates, that is, we consider Kelvin–Voigt model. The tangent forces are assumed to be classic Coulomb dry friction in sliding regime (no stiction in contact patch). Due to the viscous part of Kelvin–Voigt law, the contact patch, the plane’s normal reaction, friction force and torque depend on the position, orientation, velocity of the center of mass and the angular velocity of the body. The model does not involve any additional dynamic parameter and gives the friction force and torque directly for any given state of the body. To show the advances of the model, we recall the analytical solution of Cauchy’s initial problem with general initial conditions of ODE governing the dynamics of the homogeneous sphere on a horizontal plane (results of Zobova and Treschev in Proc. Steklov Inst. Math. 281:91–118, 2013 ). Here we generalize the model for arbitrary convex bodies and study its main properties. The model is compared to the continuous velocity-base friction model for pure sliding (Brown and McPhee in ASME J. Comput. Nonlinear Dyn. 11(5):054502, 2016 ) and to the combined dry friction (Awrejcewicz and Kudra in Multibody Syst. Dyn., 2018 , https://doi.org/10.1007/s11044-018-9624-9 ) in case of sliding with spinning. We illustrate the model considering the results of numerical integration of the Cauchy problem for a controlled differential-drive vehicle on a horizontal plane. |
Author | Zobova, Alexandra A. |
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Cites_doi | 10.1016/j.jappmathmech.2009.08.016 10.1016/S0021-8928(98)00090-2 10.1115/1.4033658 10.1134/S1560354715050020 10.1007/s11044-017-9572-9 10.1007/s11044-017-9605-4 10.1007/978-94-015-9048-8 10.1016/j.jappmathmech.2009.04.003 10.1109/MCS.2008.929279 10.1134/S0081543813040093 10.1134/S1995080217060051 10.1016/j.jappmathmech.2016.06.008 10.3103/S0025654413020039 10.1007/s11071-015-2485-3 10.1109/9.376053 10.1115/1.1454112 10.1007/s11044-018-9624-9 10.1155/2008/561280 |
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Keywords | Differential-drive vehicle Wheel dynamic Dry friction Distributed friction Visco-elastic contact |
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References | Borisov, Karavaev, Mamaev, Erdakova, Ivanova, Tarasov (CR7) 2015; 20 Al-Bender, Swevers (CR17) 2008; 28 Ivanov (CR15) 2009; 73 Awrejcewicz, Kudra (CR3) 2018 Kalker (CR14) 2000 Karapetyan, Zobova (CR23) 2017; 38 Zhuravlev (CR20) 1998; 62 Contensou (CR10) 1963 de Wit, Olsson, Astrom, Lischinsky (CR19) 1995; 40 Karapetyan (CR21) 2009; 73 Brown, McPhee (CR6) 2018; 42 Nikolić, Borovac, Raković (CR5) 2018; 42 Zobova (CR12) 2013; 48 Pennestrì, Rossi, Salvini, Valentini (CR8) 2016; 83 Zobova (CR16) 2016; 80 Brown, McPhee (CR2) 2016; 11 De Moerlooze, Al-Bender (CR4) 2008; 2008 Leine, Glocker (CR11) 2003 Goryacheva (CR13) 1998 Al-Bender, De Moerlooze (CR18) 2008; 2008 MacMillan (CR22) 1936 Zobova, Treschev (CR1) 2013; 281 Brogliato, ten Dam, Paoli, Génot, Abadie (CR9) 2002; 55 A. Zobova (9637_CR12) 2013; 48 A. Zobova (9637_CR16) 2016; 80 E. Pennestrì (9637_CR8) 2016; 83 P. Contensou (9637_CR10) 1963 J. Awrejcewicz (9637_CR3) 2018 P. Brown (9637_CR2) 2016; 11 F. Al-Bender (9637_CR18) 2008; 2008 C.C. Wit de (9637_CR19) 1995; 40 I.G. Goryacheva (9637_CR13) 1998 A.V. Karapetyan (9637_CR23) 2017; 38 A.A. Zobova (9637_CR1) 2013; 281 B. Brogliato (9637_CR9) 2002; 55 A. Karapetyan (9637_CR21) 2009; 73 K. Moerlooze De (9637_CR4) 2008; 2008 P. Brown (9637_CR6) 2018; 42 R.I. Leine (9637_CR11) 2003 M. Nikolić (9637_CR5) 2018; 42 F. Al-Bender (9637_CR17) 2008; 28 V. Zhuravlev (9637_CR20) 1998; 62 W. MacMillan (9637_CR22) 1936 A. Ivanov (9637_CR15) 2009; 73 A.V. Borisov (9637_CR7) 2015; 20 J. Kalker (9637_CR14) 2000 |
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Zobova – volume-title: Contact Mechanics in Tribology year: 1998 ident: 9637_CR13 doi: 10.1007/978-94-015-9048-8 contributor: fullname: I.G. Goryacheva – volume: 83 start-page: 1785 year: 2016 ident: 9637_CR8 publication-title: Nonlinear Dyn. doi: 10.1007/s11071-015-2485-3 contributor: fullname: E. Pennestrì – volume: 2008 year: 2008 ident: 9637_CR18 publication-title: Adv. Tribol. contributor: fullname: F. Al-Bender – volume: 11 issue: 5 year: 2016 ident: 9637_CR2 publication-title: ASME J. Comput. Nonlinear Dyn. doi: 10.1115/1.4033658 contributor: fullname: P. Brown – volume: 42 start-page: 447 issue: 4 year: 2018 ident: 9637_CR6 publication-title: Multibody Syst. Dyn. doi: 10.1007/s11044-017-9605-4 contributor: fullname: P. Brown – volume: 40 start-page: 419 year: 1995 ident: 9637_CR19 publication-title: IEEE Trans. Autom. Control doi: 10.1109/9.376053 contributor: fullname: C.C. Wit de – volume: 62 start-page: 705 issue: 5 year: 1998 ident: 9637_CR20 publication-title: J. Appl. Math. Mech. doi: 10.1016/S0021-8928(98)00090-2 contributor: fullname: V. Zhuravlev – year: 2018 ident: 9637_CR3 publication-title: Multibody Syst. Dyn. doi: 10.1007/s11044-018-9624-9 contributor: fullname: J. Awrejcewicz – volume: 2008 year: 2008 ident: 9637_CR4 publication-title: Adv. Tribol. doi: 10.1155/2008/561280 contributor: fullname: K. Moerlooze De – volume-title: Dynamics of Rigid Bodies year: 1936 ident: 9637_CR22 contributor: fullname: W. MacMillan – volume: 73 start-page: 367 issue: 4 year: 2009 ident: 9637_CR21 publication-title: J. Appl. Math. Mech. doi: 10.1016/j.jappmathmech.2009.08.016 contributor: fullname: A. Karapetyan – volume-title: 19th Biennial Conference on Mechanical Vibration and Noise, Parts A, B, and C year: 2003 ident: 9637_CR11 contributor: fullname: R.I. Leine – volume: 73 start-page: 134 issue: 2 year: 2009 ident: 9637_CR15 publication-title: J. Appl. Math. Mech. doi: 10.1016/j.jappmathmech.2009.04.003 contributor: fullname: A. Ivanov – volume: 20 start-page: 518 year: 2015 ident: 9637_CR7 publication-title: Regul. Chaotic Dyn. doi: 10.1134/S1560354715050020 contributor: fullname: A.V. Borisov – volume-title: Couplage entre frottement de glissement et frottement de pivotement dans la teorie de la toupie year: 1963 ident: 9637_CR10 contributor: fullname: P. Contensou – volume: 28 start-page: 64 year: 2008 ident: 9637_CR17 publication-title: IEEE Control Syst. doi: 10.1109/MCS.2008.929279 contributor: fullname: F. Al-Bender – volume: 42 start-page: 197 year: 2018 ident: 9637_CR5 publication-title: Multibody Syst. Dyn. doi: 10.1007/s11044-017-9572-9 contributor: fullname: M. Nikolić – volume-title: Rolling Contact Phenomena—Linear Elasticity year: 2000 ident: 9637_CR14 contributor: fullname: J. Kalker |
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Snippet | We consider the dynamics of an absolutely rigid body moving along a rough horizontal plane. We assume that the plane deforms during the motion so that the... |
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SubjectTerms | Angular velocity Automotive Engineering Automotive parts Cauchy problems Control Deformation Dry friction Dynamical Systems Electrical Engineering Engineering Friction Initial conditions Mathematical models Mechanical Engineering Numerical integration Optimization Repair & maintenance Rigid structures Rigid-body dynamics Sliding Stiction Torque Vibration Viscoelasticity |
Title | Dry friction distributed over a contact patch between a rigid body and a visco-elastic plane |
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