Abstract
Recent measurements (Honig et al., 1984; Gayeski, Connett and Honig, 1985; Gayeski and Honig, 1986) and mathematical models (Hellums, 1977; Clark et al., 1985; Federspiel and Popel, in press; Groebe and Thews, 1986) indicate that the principal resistance to O2 mass transfer is at the capillary under conditions of high O2 flux. Federspiel and Popel (in press) have described this behaviour by relating the transcapillary O2 flux to a driving force. The factor of proportionality is a mass transfer coefficient homologous to a conductance: 1 $$J=C\times\left[Pcap{{O}_{2}}-Pcell{{O}_{2}}\right]$$