Catalogus

We compared photosynthetic parameters derived from RLCs of Ulva sp. measured during winter and summer, and show large differences in a when electron transport rates (ETR) were plotted against incident irradiance (I_i) [a = 0.26 ± 0.00 versus 0.08 ± 0.01 during the winter (November–December) and summer (July–August), respectively], as is usually done. On the other hand, no differences in the initial slopes of the RLCs were apparent when plotting ETR versus the absorbed irradiance (I_a) (initial slope = 0.75 ± 0.01 versus 0.62 ± 0.12 during the winter and summer, respectively); this is called for since also ETR is calculated using I_a. Using the I_a based RLCs, it was also found that the values of the initial slopes equalled those of the first Y-value measurements of the RLCs (Y₀) (t-test, p > 0.05, r² = 0.85). Therefore, when using PAM fluorometry, we suggest (a) to present the x-axis of RLCs as I_a (I_i × AF × 0.5), and ETR on the y-axis as Y × I_a, and (b) that Y₀ can be taken as a correct measure of the maximal quantum yield instead of estimating it from an RLC.