2011
DOI: 10.1016/j.powtec.2010.11.026
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Finite element analysis of the rolling friction of a viscous particle on a rigid plane

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Cited by 50 publications
(20 citation statements)
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“…The torque acting on particle i due to particle j includes two components: Tt,ij which is generated by the tangential force and causes particle i to rotate; and Tr,ij which, commonly known as the rolling friction torque, is generated by the asymmetric normal contact forces and slows down the relative rotation between contacting particles. 14) If particle i undergoes multiple interactions, the individual interaction forces and torques are summed up for all particles interacting with particle i. Most of the equations for determining the flows and torques have been well established as, for example, reviewed by Zhu et al 15) The equations used for the present work are the same as those used in the previous work, 16,17) as given in Table 1.…”
Section: Model Descriptionmentioning
confidence: 99%
“…The torque acting on particle i due to particle j includes two components: Tt,ij which is generated by the tangential force and causes particle i to rotate; and Tr,ij which, commonly known as the rolling friction torque, is generated by the asymmetric normal contact forces and slows down the relative rotation between contacting particles. 14) If particle i undergoes multiple interactions, the individual interaction forces and torques are summed up for all particles interacting with particle i. Most of the equations for determining the flows and torques have been well established as, for example, reviewed by Zhu et al 15) The equations used for the present work are the same as those used in the previous work, 16,17) as given in Table 1.…”
Section: Model Descriptionmentioning
confidence: 99%
“…The results for strain ߝ can be found elsewhere [10,11]; thus, the viscous stress can be obtained as…”
Section: Normal Forcementioning
confidence: 99%
“…Since the results of ߝ ௫௫ ǡ ߝ ௬௬ ǡ ߝ ௭௭ are already known [10,11], one can directly obtain the following equation for rolling friction [10] ‫ܯ‬ ൌ ‫ܨܴ߱ܣ‬…”
Section: Rolling Frictionmentioning
confidence: 99%
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“…A primeira é a dissipação de energia na interface de contato de duas partículas, devido ao microdeslizamento e fricção, irregularidades de superfície, adesão molecular, ou outras propriedades de superfície. Neste mecanismo, a energia cinética de uma partícula é dissipada, resultando na desaceleração da velocidade de rolamento da partícula, que é um fenômeno usual de atrito (ZHENG et al, 2011).…”
Section: Coeficiente De Atrito De Rolamentounclassified