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Interfacial area per unit volume of the contactor, m2/m3.
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As previously described, (m_c) was mainly the effective mass of the contactor and not that of the finger pad.
Therein, the boundary of one body (contactor) is intersected with the volume of the target.
The contactor vibrates sinusoidally: begin{aligned} x_c(t) = A sin omega t end{aligned} (1 where A and (omega) are the amplitude and angular frequency, respectively, of the contactor.
Hence, the displacement of the contactor is in good agreement with that of the finger pad.
The motion of the contactor was determined by a sinusoidal function (1).
A critical factor that could influence our experiment is the surface roughness of the contactor material.
The sinusoidal vibration of the contactor was largely maintained while it was being touched.
Unlike the simulation, the sticking did not occur at every cycle of the vibration of the contactor.
The simulated friction forces, the results of the psychophysical experiments, and physical observation suggested that the transient increases in friction caused by lateral vibration of the contactor influenced friction perception for a laterally vibrating contactor.
The relative velocity is the difference between the finger velocity and that of the contactor Fig. 12 Examples of friction forces and relative velocities between the finger nail and contactor.
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