When the bulk filling factor is nu=1-1/m with m odd, at. least one counterp
ropagating chiral collective mode occurs simultaneously with magnetoplasmon
s at the edge of Fractional quantum Hall samples. Initial experimental sear
ches for an additional mode were unsuccessful. In this paper, we address co
nditions under which its observation should be expected in experiments wher
e the electronic system is excited and probed by capacitive coupling. We de
rive realistic expressions for the velocity of the slow counterpropagating
mode, starting from a microscopic calculation which is simplified by a Land
au-Silin-like separation between long-range Hartree and residual interactio
ns. The microscopic calculation determines the stiffness of the edge to lon
g-wavelength neutral excitations, which fixes the slow-mode velocity, and t
he effective width of the edge region, which influences the magnetoplasmon
dispersion. [S0163-1829(98)02243-7].