Tokyo Research Laboratories, Kao Corporation, 2-1-3 Bunka, Sumida-ku, Tokyo 131-8501, Japan.
J Chem Phys. 2009 Nov 14;131(18):184708. doi: 10.1063/1.3261732.
The static friction (stiction) of the molecularly thin films of an irregularly shaped molecule 1,3-dimethylbutyl octyl ether (DBOE) confined between mica surfaces was investigated using the surface forces apparatus. Stop-start experiments were carried out and the stiction spike was measured as a function of surface stopping (aging) time t and applied pressure P. The results show two relaxation processes, one on stopping and one on starting, where each process has a fast and a slow time constant. For stopping mode, there is no stiction spike when t is shorter than a characteristic nucleation time, tau(n) (fast time constant). When t exceeds tau(n), stiction spike appears whose height increases logarithmically with t. With regard to starting, the relaxation behavior was evaluated by a double exponential fit of the slipping regime (force decay) of the spike and two time constants (tau(1) and tau(2)) were obtained. The fast time constant on starting tau(1) is almost equal to that on stopping tau(n). To the best of our knowledge, this is the first direct observation of the agreement of the time constant on stopping and that on starting, indicative of a reversible structural transition (solid-liquid transition) in the stop-start stiction dynamics. The two fast time constants exhibit exponential dependence on P, which implies a glasslike nature of the transition. Comparison with the stick-slip friction reveals that the solid-liquid transition involved in stiction and that in stick-slip dynamics is different for DBOE; first-order-like discontinuous transition is suggested for stick-slip friction. Origins of the different solid-liquid transition dynamics in stiction and in stick-slip friction are discussed by comparing with the dynamics of other confined liquid systems.
使用表面力仪器研究了在云母表面之间受限的形状不规则分子 1,3-二甲基丁基辛基醚(DBOE)的分子薄膜的静态摩擦力(粘性)。进行了停止-启动实验,并测量了作为表面停止(老化)时间 t 和施加压力 P 的函数的粘性尖峰。结果表明存在两个弛豫过程,一个在停止时,一个在启动时,每个过程都具有快和慢时间常数。对于停止模式,当 t 短于特征成核时间 tau(n)(快时间常数)时,没有粘性尖峰。当 t 超过 tau(n)时,会出现粘性尖峰,其高度随 t 呈对数增长。对于启动,通过对尖峰的滑动区(力衰减)进行双指数拟合来评估弛豫行为,并获得两个时间常数(tau(1)和 tau(2))。启动时的快时间常数 tau(1)几乎与停止时的快时间常数 tau(n)相等。据我们所知,这是首次直接观察到停止和启动时的时间常数一致,表明在停止-启动粘性动力学中存在可逆的结构转变(固-液转变)。两个快时间常数表现出对 P 的指数依赖性,这意味着转变具有玻璃状性质。与粘滑摩擦的比较表明,粘性中涉及的固-液转变与粘滑动力学中的固-液转变不同;对于粘滑摩擦,建议存在类似一阶的不连续转变。通过与其他受限液体系统的动力学进行比较,讨论了粘性和粘滑摩擦中不同固-液转变动力学的起源。