The statistical mechanics of polymer loops entangled in the two-dimens
ional array of randomly distributed obstacles of infinite length is di
scussed. The area of the loop projected onto the plane perpendicular t
o the obstacles is used as a collective variable in order to re-expres
s a (mean-field) effective theory for the polymer conformation. It is
shown explicitly that the loop undergoes a collapse transition to a ra
ndomly branched polymer with R proportional to lN(1/4).