Quantum yields of photosystcm I1 (PSII) charge separation (@& and oxygen production ((I) (,,) were determined by simultaneous measurements of oxygen production and variable fluorescence in four different aquatic microalgae representing three different taxonomic groups: the freshwater alga Scenedesmus protuberans (Chlorophyceae) and the marine algae Phneorystis globosa (Prymnesiophyceae), Emiliania huxleyi (Prymnesiophyceae), and Phaeodactylum tricornutum (Bacillariophyceae). In S. protuberans, P. tricornutum, and E. huxleyi, light-dependent variability was observed in the ratio of a(,,, to a,,, i.c. in the number of oxygen molecules produced per electron generated by PSII. The ratio ao,:@,, was highly variable at low light intensities (E < OSE,), and at higher light intensities (E > OSE,) @(,, : @,, showed a nonlinear decrease with increasing light intensity. In contrast, in P. globosa. a trend in a<,, : @,, could not be distinguished, and this species showed a decrease in @'o, : $ during the day, indicating a dependency of a(,, : a,, on light history. Additionally, considerable interspecific quantitative differences in a(,, : a,, were observed. Two possible interpretations to explain the variability in '.I+)! : a, are discussed. Assuming that 0, is a reliable measure of the quantum yield for charge separation at PSII, one interpretation is that net oxygen production is influenced by processes that consume oxygen or affect linear electron transport (e.g. cyclic electron transport around PSII, pseudocyclic electron transport in the Mehler reaction, Rubisco oxygenase activity, and lightdependent mitochondrial respiration). A second interpretation, however, suggests that at saturating light, changes in photosynthesis turnover time occur, such that $ does not predict the steady-state O2 yield.Quantum yields of phytoplankton photosynthesis are usually defined as the quantum yields for O? production (CacjL) or C fixation (@c,,,) (Kok 1948;Myers 1980;Babin et al. 1996). Because measurements of @oz and @'co, are laborious and time-consuming, much attention has been focused lately on the use of variable chlorophyll fluorescence as a tool to measure the quantum yield of charge separation in photosystem II (PSIl) reaction centers (Genty et al. 1989). This technique is rapid and noninvasive and may offer high temporal and spatial resolution when used in field measurements (Schreiber et al. 1986). Theoretically, the rate of noncyclic photosynthetic electron transport of a PSI1 (J) can be calculated from the quantum yield of PSI1 charge separation (a,,) according to J = @,J%s,,rwhere E is the incident light intensity and cr,,,, is the absorption cross section of PSII, which determines the fraction of the incident light intensity that is actually used by PSI1 (e.g. Kolber and Falkowski 1993; Kroon 1991; Hofstraat et al. 1994, Biehler andFock 1995). In order to use J as a measure for photosynthesis, the relationships between @,,, @coL, and @coz have to be well established. According to the stoichiometry of the Z-schem...