  In conjunction with recent numerical \hbox{$\lambda~\partial_0 A_0 +
\nabla\cdot\vec{A} =0$} ``$\lambda$-gauge'' results reported in a companion
paper, we construct an $N\to\infty$ Wilson loop picture of
$\lambda$-gaugefixing in which (I)the $\lambda$-gauge expectation value of a
link chain $C$ is the weighted sum over Wilson loops made by joining to $C$ all
selfavoiding chains $\widetilde{C}$ closing $C$. (II)Weights
$A_{\widetilde{C}}$, containing all the $\lambda$-dependence, are given by the
$\beta=0$ $\lambda$-gauge expectation value of $\widetilde{C}$.
(III)$A_{\widetilde{C}}$ equals path-products of coefficients from the trace
expansion of the gaugefixing Boltzmann weight. From (II) and (III) we deduce
formulas for $\beta =0$ quark matrix elements. We find that $M_q^{(\lambda)}$
decreases with increasing $\lambda$; the quark propagator dispersion relation
is not covariant when $\lambda\ne 1$; and $\Delta I=1/2$ matching coefficients
are $\lambda$-independent. These strong coupling features are qualitatively
consistent with numerical $\beta=5.7$ and $6.0$ results briefly described here
for comparison purposes but mainly presented in a companion paper.
