Matches in SemOpenAlex for { <https://semopenalex.org/work/W2091226489> ?p ?o ?g. }
- W2091226489 endingPage "280" @default.
- W2091226489 startingPage "264" @default.
- W2091226489 abstract "The main component of rubber friction is known to be of hysteretic nature, i.e. it is due to viscoelastic energy dissipation taking place in the bulk of the material as a result of the pulsating forces induced by the surface asperities whenever rubber slides on a rough substrate, such as in the case of a car tire on a road surface. This implies that the observed macroscopic friction depends upon the constitutive behavior of the rubber and the characteristics of the rough surface profile. In contrast to analytical models, numerical approaches can fully account for geometric and material non-linearities arising in the rubber behavior, especially at small scales. However, explicit numerical modeling of rough surface features spanning a wide range of significant length scales would result prohibitively expensive, which motivates the need for a computational multiscale framework. As shown by previous related research, fractal surface profiles can be decomposed into a finite number of sinusoidal terms, so that a central ingredient of a multiscale approach becomes the homogenization of rubber friction on a sinusoidal surface. This work proposes a computational homogenization procedure where a macroscale coefficient of friction for rubber is derived from the solution of a microscale boundary-value problem. The latter considers contact of a representative volume element (RVE) with a sinusoidal rigid surface, which is assumed to represent the smallest length scale of a fractal rough surface. The numerical model is developed within the isogeometric framework and features a mortar formulation for the unilateral contact problem in the discretized setting. Numerical aspects related to the choice of the RVE, the setup of the test parameters and the convergence rate of different discretizations are discussed. Physically relevant observations concern the role of the macroscopic applied pressure and sliding velocity on the homogenized friction coefficient. Some comparisons with analytical results as well as dimensional analysis considerations are further reported." @default.
- W2091226489 created "2016-06-24" @default.
- W2091226489 creator A5016987095 @default.
- W2091226489 creator A5086471469 @default.
- W2091226489 date "2013-09-01" @default.
- W2091226489 modified "2023-10-13" @default.
- W2091226489 title "Computational homogenization of rubber friction on rough rigid surfaces" @default.
- W2091226489 cites W1971990676 @default.
- W2091226489 cites W1979668890 @default.
- W2091226489 cites W1979701617 @default.
- W2091226489 cites W1979759113 @default.
- W2091226489 cites W1981981246 @default.
- W2091226489 cites W1989386553 @default.
- W2091226489 cites W1995072869 @default.
- W2091226489 cites W1996313806 @default.
- W2091226489 cites W2000425991 @default.
- W2091226489 cites W2005566098 @default.
- W2091226489 cites W2007490740 @default.
- W2091226489 cites W2008413953 @default.
- W2091226489 cites W2019955567 @default.
- W2091226489 cites W2026375664 @default.
- W2091226489 cites W2027341162 @default.
- W2091226489 cites W2040680185 @default.
- W2091226489 cites W2046909490 @default.
- W2091226489 cites W2053168980 @default.
- W2091226489 cites W2071909989 @default.
- W2091226489 cites W2072637867 @default.
- W2091226489 cites W2078541865 @default.
- W2091226489 cites W2086732613 @default.
- W2091226489 cites W2087271212 @default.
- W2091226489 cites W2090167367 @default.
- W2091226489 cites W2092333079 @default.
- W2091226489 cites W2093333193 @default.
- W2091226489 cites W2111678256 @default.
- W2091226489 cites W2115224307 @default.
- W2091226489 cites W2147291198 @default.
- W2091226489 cites W2163821354 @default.
- W2091226489 cites W2164947120 @default.
- W2091226489 cites W2567124175 @default.
- W2091226489 doi "https://doi.org/10.1016/j.commatsci.2013.04.049" @default.
- W2091226489 hasPublicationYear "2013" @default.
- W2091226489 type Work @default.
- W2091226489 sameAs 2091226489 @default.
- W2091226489 citedByCount "38" @default.
- W2091226489 countsByYear W20912264892014 @default.
- W2091226489 countsByYear W20912264892015 @default.
- W2091226489 countsByYear W20912264892016 @default.
- W2091226489 countsByYear W20912264892017 @default.
- W2091226489 countsByYear W20912264892018 @default.
- W2091226489 countsByYear W20912264892019 @default.
- W2091226489 countsByYear W20912264892020 @default.
- W2091226489 countsByYear W20912264892021 @default.
- W2091226489 countsByYear W20912264892022 @default.
- W2091226489 countsByYear W20912264892023 @default.
- W2091226489 crossrefType "journal-article" @default.
- W2091226489 hasAuthorship W2091226489A5016987095 @default.
- W2091226489 hasAuthorship W2091226489A5086471469 @default.
- W2091226489 hasConcept C104779481 @default.
- W2091226489 hasConcept C121332964 @default.
- W2091226489 hasConcept C130217890 @default.
- W2091226489 hasConcept C134306372 @default.
- W2091226489 hasConcept C135402231 @default.
- W2091226489 hasConcept C135628077 @default.
- W2091226489 hasConcept C145420912 @default.
- W2091226489 hasConcept C159985019 @default.
- W2091226489 hasConcept C160635147 @default.
- W2091226489 hasConcept C176933379 @default.
- W2091226489 hasConcept C179428855 @default.
- W2091226489 hasConcept C179909247 @default.
- W2091226489 hasConcept C182310444 @default.
- W2091226489 hasConcept C186541917 @default.
- W2091226489 hasConcept C18903297 @default.
- W2091226489 hasConcept C192562407 @default.
- W2091226489 hasConcept C2778722038 @default.
- W2091226489 hasConcept C33923547 @default.
- W2091226489 hasConcept C37167619 @default.
- W2091226489 hasConcept C40636538 @default.
- W2091226489 hasConcept C57879066 @default.
- W2091226489 hasConcept C73000952 @default.
- W2091226489 hasConcept C86803240 @default.
- W2091226489 hasConcept C87976508 @default.
- W2091226489 hasConcept C97355855 @default.
- W2091226489 hasConceptScore W2091226489C104779481 @default.
- W2091226489 hasConceptScore W2091226489C121332964 @default.
- W2091226489 hasConceptScore W2091226489C130217890 @default.
- W2091226489 hasConceptScore W2091226489C134306372 @default.
- W2091226489 hasConceptScore W2091226489C135402231 @default.
- W2091226489 hasConceptScore W2091226489C135628077 @default.
- W2091226489 hasConceptScore W2091226489C145420912 @default.
- W2091226489 hasConceptScore W2091226489C159985019 @default.
- W2091226489 hasConceptScore W2091226489C160635147 @default.
- W2091226489 hasConceptScore W2091226489C176933379 @default.
- W2091226489 hasConceptScore W2091226489C179428855 @default.
- W2091226489 hasConceptScore W2091226489C179909247 @default.
- W2091226489 hasConceptScore W2091226489C182310444 @default.
- W2091226489 hasConceptScore W2091226489C186541917 @default.
- W2091226489 hasConceptScore W2091226489C18903297 @default.
- W2091226489 hasConceptScore W2091226489C192562407 @default.