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This paper proposes a simple and yet effective scheme to identify the dynamic friction region of robotic manipulators.
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The fault contains two regions with different mechanical behaviours: a strong region (asperity) with a high static friction and a velocity-weakening dynamic friction and a weak region with a negligible static friction and a velocity-strengthening dynamic friction.
The dynamic friction increases in the shallower region in order to reduce the slip-rate amplitudes (Wada and Goto, 2012), because the stopping front from the shallower edge is assumed to be less dominant in this simulation.
Additionally, the fact that the loading curve in region (III) is nearly identical to the unloading (retraction) curve in region (ii) at slightly elevated temperatures (Fig. 2c) demonstrates that the magnitude of the dynamic friction force is negligible (since this force points in opposite directions on loading and unloading) and the retraction (above ∼100 °C) is superlubric.
In technical terms, its dynamic friction must be lower than its static friction.
Su, H., Goddard III, W. A. & Zhao, Y. Dynamic friction force in a carbon peapod oscillator.
For the friction force description, the dynamic friction models were used.
The traditional style of cross-country skiing works on the same principle — the downward kick stroke requires high static friction, while the glide is possible thanks to low dynamic friction.
The traditional style of cross-country skiing works on the same principle the downward kick stroke requires high static friction, while the glide is possible thanks to low dynamic friction.
However, there is a more significant 32% reduction between the wet static friction coefficients versus the wet dynamic friction coefficient.
Monotonic shear tests indicate that the dry dynamic friction coefficient was approximately 15% smaller than the dry static friction coefficient.
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