  We analyze the classical limit of kinematic loop quantum gravity in which the
diffeomorphism and hamiltonian constraints are ignored. We show that there are
no quantum states in which the primary variables of the loop approach, namely
the SU(2) holonomies along {\em all} possible loops, approximate their
classical counterparts. At most a countable number of loops must be specified.
To preserve spatial covariance, we choose this set of loops to be based on
physical lattices specified by the quasi-classical states themselves. We
construct ``macroscopic'' operators based on such lattices and propose that
these operators be used to analyze the classical limit. Thus, our aim is to
approximate classical data using states in which appropriate macroscopic
operators have low quantum fluctuations.
  Although, in principle, the holonomies of `large' loops on these lattices
could be used to analyze the classical limit, we argue that it may be simpler
to base the analysis on an alternate set of ``flux'' based operators. We
explicitly construct candidate quasi-classical states in 2 spatial dimensions
and indicate how these constructions may generalize to 3d. We discuss the less
robust aspects of our proposal with a view towards possible modifications.
Finally, we show that our proposal also applies to the diffeomorphism invariant
Rovelli model which couples a matter reference system to the Hussain Kucha{\v
r} model.
