  The main challenge faced by Higgsless models of electroweak symmetry breaking
is to reconcile the experimental constraints imposed by the precision
electroweak data and the top quark phenomenology with the unitarity constraints
imposed by longitudinal gauge boson scattering amplitudes. In this paper we
expand on previous work, giving details of how delocalized fermions can be used
to adjust the $S$ parameter to zero, while keeping the $T$ and $U$ parameters
naturally suppressed. We also show that it is possible to obtain the top quark
mass, without affecting the delay of unitarity violation of the $W^+ W^-\to
W^+W^-$ scattering amplitude, by separating the mass scales of the fermion
sector ($1/R_f$) from that of the gauge sector ($1/R_g$). The fermion sector
scale $1/R_f$ is only weakly constrained by unitarity of the $t\bar{t}\to W^+
W^-$ scattering amplitude; thus the ratio $R_g/R_f$ can be quite large, and the
top mass can be easily achieved. Anomalous right-handed couplings involving the
third generation quarks also avoid constraints from experimental data if
$1/R_f$ is sufficiently large.
