  We present theoretical arguments, based on linear elasticity and
thermodynamics, to show that interfacial tangential stresses in sliding
adhesive contacts does not affet at all the adhesive behavior of the system,
which then follows the classical JKR solution. Our finding explains the
experimental observation of Vorvolakos and Chaudhury in 2003, who found that
the contact area of a PDMS sphere remains constant during sliding and is in
agreement with the JKR solution, at least up to velocity of 1mm/s, and of
Carpick et al. Carpick, who observed that the friction force between a
platinum-coated atomic force microscope (AFM) tip and the surface of mica in
ultrahigh vacuum (UHV) varies with load in proportion to the contact area
predicted by the Johnson-Kendall-Roberts (JKR). We show that a reduction of the
contact area, experimentlly observed at higher sliding speeds, can be caused by
a reduction of the density of adhesive bonds as the velocity is increased, or
caused by the repulsive energy term associated with the stress spatial
fluctuation at the interface. This may explain why adhesion is completely
masked at relatively large sliding velocities.
  This version of the paper follows the publication of the Corrigendum: Nicola
Menga, Giuseppe Carbone, Daniele Dini: Corrigendum to "Do uniform tangential
interfacial stresses enhance adhesion?" [Journal of the Mechanics and Physics
of Solids 112 (2018) 145--156], Journal of the Mechanics and Physics of Solids,
133, 103744, https://doi.org/10.1016/j.jmps.2019.103744, available on line
since 8 October 2019.
