The adsorption of phospholipids at interfaces determines many biological phenomena, from cell life to lung-surfactant dynamics. The lung surfactant reduces the surface tension in the alveoli and ensures normal breathing. Although the dynamic adsorption and interfacial rheology of dipalmitoylphosphatidylcholine (DPPC), the main component of the native lung surfactant, has been extensively investigated to understand the mechanism of respiration, [1][2][3][4][5][6][7][8] this quest has met some serious difficulties.Many studies have focused on DPPC monolayers spread as insoluble films on water. [9][10][11][12] One serious limitation of these studies is that the DPPC monolayer was not in contact with DPPC vesicles and/or aggregates in the aqueous phase. These studies thus overlook the role that the vesicles present in the mucus that lines the alveoli do play in the relaxation processes. It was shown indeed that phospholipid aggregates released from the alveolar type II cells diffuse to, come in contact with, and spread on the interface, thereby resulting in surface-associated phospholipid reservoirs. [13] The attempts made so far to investigate DPPC films adsorbed at the air/water interface while in coexistence with dispersions of vesicles, by using the Langmuir balance, [14] Wilhelmy plate, [15] or static captive bubble methods, [16,17] met another severe shortcoming: the equilibrium interfacial tension g eq could not be attained owing to exceedingly slow phospholipid adsorption. Further studies, using a pulsating bubble surfactometer, submitted DPPC bubbles to large surface variations (typically 50 %), and hence to very strong constraint, [16,18,19] preventing linear responses. The lowest interfacial tension values were only collected when the surface of the bubble was minimum, and hence when constraint was the largest. These tensions increased again