Rubber friction for tire tread compound on road surfaces
We have measured the surface topography and calculated the surface roughness power spectrum for an asphalt road surface. For the same surface we have measured the friction for a tire tread compound for velocities 10−6 m s−1 < v < 10−3 m s−1 at three different temperatures (at −8 °C, 20 °C and...
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| Published in | Journal of physics. Condensed matter Vol. 25; no. 9; p. 095007 |
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| Main Authors | , , , , |
| Format | Journal Article |
| Language | English |
| Published |
England
IOP Publishing
06.03.2013
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| Subjects | |
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| Abstract | We have measured the surface topography and calculated the surface roughness power spectrum for an asphalt road surface. For the same surface we have measured the friction for a tire tread compound for velocities 10−6 m s−1 < v < 10−3 m s−1 at three different temperatures (at −8 °C, 20 °C and 48 °C). The friction data was shifted using the bulk viscoelasticity shift factor aT to form a master curve. We have measured the effective rubber viscoelastic modulus at large strain and calculated the rubber friction coefficient (and contact area) during stationary sliding and compared it to the measured friction coefficient. We find that for the low velocities and for the relatively smooth road surface we consider, the contribution to friction from the area of real contact is very important, and we interpret this contribution as being due to shearing of a very thin confined rubber smear film. |
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| AbstractList | We have measured the surface topography and calculated the surface roughness power spectrum for an asphalt road surface. For the same surface we have measured the friction for a tire tread compound for velocities 10 super(-6) m s super(-1) < [nu] < 10 super(-3) m s super(-1) at three different temperatures (at -8 [degrees]C, 20 [degrees]C and 48 [degrees]C). The friction data was shifted using the bulk viscoelasticity shift factor a sub()Tto form a master curve. We have measured the effective rubber viscoelastic modulus at large strain and calculated the rubber friction coefficient (and contact area) during stationary sliding and compared it to the measured friction coefficient. We find that for the low velocities and for the relatively smooth road surface we consider, the contribution to friction from the area of real contact is very important, and we interpret this contribution as being due to shearing of a very thin confined rubber smear film. We have measured the surface topography and calculated the surface roughness power spectrum for an asphalt road surface. For the same surface we have measured the friction for a tire tread compound for velocities 10(-6) m s(-1) < v < 10(-3) m s(-1) at three different temperatures (at -8 °C, 20 °C and 48 °C). The friction data was shifted using the bulk viscoelasticity shift factor a(T) to form a master curve. We have measured the effective rubber viscoelastic modulus at large strain and calculated the rubber friction coefficient (and contact area) during stationary sliding and compared it to the measured friction coefficient. We find that for the low velocities and for the relatively smooth road surface we consider, the contribution to friction from the area of real contact is very important, and we interpret this contribution as being due to shearing of a very thin confined rubber smear film. We have measured the surface topography and calculated the surface roughness power spectrum for an asphalt road surface. For the same surface we have measured the friction for a tire tread compound for velocities 10−6 m s−1 < v < 10−3 m s−1 at three different temperatures (at −8 °C, 20 °C and 48 °C). The friction data was shifted using the bulk viscoelasticity shift factor aT to form a master curve. We have measured the effective rubber viscoelastic modulus at large strain and calculated the rubber friction coefficient (and contact area) during stationary sliding and compared it to the measured friction coefficient. We find that for the low velocities and for the relatively smooth road surface we consider, the contribution to friction from the area of real contact is very important, and we interpret this contribution as being due to shearing of a very thin confined rubber smear film. We have measured the surface topography and calculated the surface roughness power spectrum for an asphalt road surface. For the same surface we have measured the friction for a tire tread compound for velocities 10(-6) m s(-1) < v < 10(-3) m s(-1) at three different temperatures (at -8 °C, 20 °C and 48 °C). The friction data was shifted using the bulk viscoelasticity shift factor a(T) to form a master curve. We have measured the effective rubber viscoelastic modulus at large strain and calculated the rubber friction coefficient (and contact area) during stationary sliding and compared it to the measured friction coefficient. We find that for the low velocities and for the relatively smooth road surface we consider, the contribution to friction from the area of real contact is very important, and we interpret this contribution as being due to shearing of a very thin confined rubber smear film. |
| Author | Persson, B N J Giustiniano, M Baldoni, F Lorenz, B Fortunato, G |
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| References | 23 24 25 26 27 29 Mofidi M (16) 2008; 20 Westermann S (10) 2004; 57 Busse L (22) 2011; 64 Yang C (34) 2008; 20 Tada T (32) 2011 Pacejka H B (4) 2006 Campana C (36) 2004; 70 30 31 11 12 13 35 14 37 38 Persson B N J (17) 2005; 17 18 Persson B N J (6) 2006; 18 Persson B N J (28) 2005; 17 1 2 5 Persson B N J (19) 2011; 23 7 Persson B N J (33) 2008; 20 8 9 Persson B N J (15) 2009; 21 (3) 2006 20 21 |
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| Snippet | We have measured the surface topography and calculated the surface roughness power spectrum for an asphalt road surface. For the same surface we have measured... |
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| SubjectTerms | Condensed matter Contact Friction Mathematical analysis Roads Rubber Treads Viscoelasticity |
| Title | Rubber friction for tire tread compound on road surfaces |
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