Alveolar parenchyma comprises two interacting tensile systems: the cab
le system (a network of linear condensations of connective tissue) and
the membrane system (a network of quasiplanar alveolar septa). infere
nces can be drawn about the mechanics of this structure from its confi
guration. We reported earlier (E. H. Oldmixon, J. P. Butler, and F. G.
Hoppin, Jr. J. Appl. Physiol. 64:299-307, 1988) that the angles betwe
en alveolar septa at the common three-way junctions (J) are nearly uni
form, indicating that septal tensions are also nearly uniform. We now
report on the interseptal angles at the next most common class of sept
al junction (B), a structure where two septa meet along a segment of t
he cable system. We find, first, that the distributions of interseptal
angles at B junctions have means >120 degrees, are narrow and have fe
w, if any, angles <120 degrees. The findings of uniform 120 degrees an
gles at J junctions and a cutoff below 120 degrees at B junctions are
also characteristic of soap films supported on a frame, which follows
the physical principle of surface area minimization. We suggest that t
his principle may be operative in parenchymal development and remodeli
ng.