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While in the presence of lubricant SMJH-1, a boundary lubricant film exhibits relatively weak friction force compared with the lubricant-free systems.
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Hence, their track deflections are closer to our simulations with weak surface friction than moderate friction.
If the arc is made of a weaker 'continental-like' material or contains a weak layer/low friction interface, it is completely or partially scraped off even if it is small.
Because of weak surface friction, the southward deflection and the slowdown of the vortex are small, and the vortex remains almost circular, although two excessive relative velocity maxima with Vʹ = 5.55 m s−1 (( {text{V}^{*prime}} )= 27.8 m s−1) show up on the front and rear of the vortex.
The case of C10 in Fig. 10d has the same parameters as D4 except a weaker surface friction (i.e., α = 3.5 × 10−5 cyan line in Fig. 5c).
If this outstanding high-attenuation property was caused by weaker fault friction based on the previous laboratory measurement (Nagata et al. 2008), the faults A and B may be interpreted more active than the others at present.
Our experimental observations require a substantial modification of the model of interaction between benzene molecules and graphite surfaces: in contrast to recent studies we find only weak kinetic surface friction, but a substantial dissipative interaction during inter-molecular collisions.
Kramers considered separately the cases of weak and strong friction.
We interpret the fault parallel σ1 and fault normal σ3 acting around the Çınarcık fault area as evidence of a low coefficient of friction or weak crust.
A shallow weak layer, velocity-strengthening friction, or off-fault dissipation, can help inhibit the supershear transition near the free surface (Kaneko and Lapusta, 2010).
The relationships among the structural parameters, compositions of the weak layers, dry sliding friction and wear behavior of the materials are investigated in this study.
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