Ploughing friction

2020-08-18  本文已影响0人  边路乙拉

Lafaye 2006 TribologyLetters

  1. scratching of a rigid perfectly plastic material
  2. 1958 Sabey [5] proposed taking into account a lost energy ratio b

I would probably start with this ref

  1. A model that takes into account the elastic recovery defined by a rear angle x as shown in figure 1, was proposed by Bucaille et al. [6] and further developed by Lafaye et al. [7] for a perfectly conical tip.
  2. \mu _{ploughing} = S_t/S_n this article uses this assumption directly, which is kind of strange.
  3. this leads to the "model for a conical tip with a blunted spherical extremity" with assumption #4 and elastic recovery \omega from #3. The result of this article shows that the increase of the COF during initial stage of a scratch is caused by the blunted spherical extremity.

Carreon 2018 TribologyInternational

  1. Starts with Lafaye's work with the assumption of elastic recovery \omega and a blunted spherical tip. Which requires three input parameters:
    • nanoindenter half-angle θ,
    • nanoindenter spherical tip radius R,
    • elastic recovery parameter ω.
  2. The ductile-to-brittle transition depth, h_{DBT}, may also contribute to this behavior by causing ω to be a function of penetration depth, ω = f(h).
  3. overall the PAVER model takes 1 more parameter into account, which is the ductile-brittle transition depth, h_{DBT}.

Chamani 2016 TI

  1. berkovch, nanoscratch, FEM,
  2. \mu _{apparent}=\mu _p+ \mu _a=\mu _p +f(\mu _s), \mu _s is the COF in the simulation.
  3. ff(60\degree) has the biggest \mu _p as it has a maximum pile up.
  4. the result is based on FEA, so the only conclusion you can use is that the pile up affects the COF heavily.
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