@article{oai:nagoya.repo.nii.ac.jp:00031252,
 author = {Imachi, Isamu},
 issue = {1},
 journal = {Memoirs of the Faculty of Engineering, Nagoya University},
 month = {Jan},
 note = {When a constant force S is applied to a mass m which is under control of the Coulomb friction µmg between the horizontal base surface (See Fig. 1), the following wellknown rule is maintained as far as no other dynamical effects are concerned. "When S>µmg, the velocity of the mass is ever accelerated, and when S<µmg, it is ever decelerated until the mass comes to standstill." However, if the base surface is in vibration in the horizontal plane, and if some condition is fulfilled, the mean velocity of the mass can be kept constant as if there exists some viscous resistance. This phenomena may be called as "Frictional Viscosity." The mean velocity thus observed has, in general, components not only in the direction of S but also in the lateral direction to it.},
 pages = {171--176},
 title = {On Frictional viscosity in vibrating systems},
 volume = {19},
 year = {1968}
}