机构:
Institut Curie, Centre de Recherche, Université Paris 6, F75248 Paris, FranceInstitut Curie, Centre de Recherche, Université Paris 6, F75248 Paris, France
Wu-Bavouzet, F.
[1
]
Clain-Burckbuchler, J.
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机构:
Institut Curie, Centre de Recherche, Université Paris 6, F75248 Paris, FranceInstitut Curie, Centre de Recherche, Université Paris 6, F75248 Paris, France
Clain-Burckbuchler, J.
[1
]
Buguin, A.
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机构:
Institut Curie, Centre de Recherche, Université Paris 6, F75248 Paris, FranceInstitut Curie, Centre de Recherche, Université Paris 6, F75248 Paris, France
Buguin, A.
[1
]
De Gennes, P.-G.
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机构:
Institut Curie, Centre de Recherche, Université Paris 6, F75248 Paris, FranceInstitut Curie, Centre de Recherche, Université Paris 6, F75248 Paris, France
De Gennes, P.-G.
[1
]
Brochard-Wyart, F.
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机构:
Institut Curie, Centre de Recherche, Université Paris 6, F75248 Paris, FranceInstitut Curie, Centre de Recherche, Université Paris 6, F75248 Paris, France
Brochard-Wyart, F.
[1
]
机构:
[1] Institut Curie, Centre de Recherche, Université Paris 6, F75248 Paris, France
来源:
Journal of Adhesion
|
2007年
/
83卷
/
08期
关键词:
A rubber lens (polydimethylsiloxane) is pressed against silanated or bare glass plates (Johnson-Kendall-Roberts (JKR) contact). As the plate slides with a velocity U;
we measure the friction on the lens using a macro Atomic Force Microscope (AFM);
where the cantilever is a thin rectangular glass rod and the tip is the rubber lens. We observe the contact area via optical interferometry. In air for hard lenses (Young's modulus E ' MPa);
we find smooth sliding on a model substrate;
and a transition to stick-slip on a hysteretic substrate above a threshold velocity;
VM. For soft lenses (E 1MPa);
we observe Schallamach waves and stick-slip depending on normal force and the plate's velocity;
U. When immersed in a liquid (silicone oils;
water-glycerol mixtures);
the contact remains dry at low velocities;
but is invaded by a liquid film above a critical velocity;
Uc. For hard lenses we observe smooth sliding and high friction below Uc;
and low friction above Uc. For soft lenses;
we find wet Schallamach waves for U M and stick-slip instabilities at large velocities. In the stick-slip regime;
the contact is wet in the slip phase;
and dewets in the stick phase. We measure the period of the stick-slip cycle as a function of the liquid viscosity. We interpret the stick-slip process by the formation and rupture of adhesive bonds (between the rubber polymer chains and active sites on the glass). Using a recent model;
we can explain most of the data for the stick-slip period and slip threshold velocity;