5 (i.e., ΔI/I = 5.45 × 10−3 GS-4997 for 1 e − per PS II). For example, the initial slope of ΔI/(I × Δt) × 10−3 = 554 s−1 measured 9.5 s after light-on is equivalent to 102 e − per PS II and s. It should be noted that this “PS II-related selleckchem charge flux” does not correspond to the actual PS II charge separation rate occurring

in the given example at 9.5 s after light-on, but rather to the overall rate of photochemical charge separation in PS I and PS II (R ph, see definition above). If it were assumed that the rates of PS I and PS II are equal in a quasi-stationary state, the actual PS II charge separation rate would be 50 % of the “PS II-related charge flux”. However, electron flux rate via PS II would be less, if cyclic PS I would contribute to charge flux. In the context of this technical report it is essential that almost identical charge flux rates are obtained with the point-by-point DIRKECS PHA-848125 and the continuous P515 flux methods, with the latter having the obvious advantage of being less time consuming and more simple in practical applications. As the flux signal is quasi-continuous, its measurement does not disturb other continuously measured signals, like oxygen evolution or CO2 uptake. In the following sections simultaneous measurements of CO2 uptake

and P515 indicated charge flux are presented. Comparison of CO2 uptake Rapamycin nmr and charge flux: light response Simultaneously measured changes of P515, P515 indicated charge flux and CO2 uptake induced by stepwise lowering of light intensity, are shown in Fig. 8a. P515

indicated charge flux is presented in units of ΔI/(I × Δt) s−1, i.e., without information on PS II density, PS II/PS I and a possible contribution of cyclic PS I, no attempt was made to compare the rates of charge flux and CO2 uptake in absolute terms. The charge flux and CO2 uptake signals were scaled such that the responses in the low-intensity range were close to identical. At the same time the observed flux responses in the high-intensity range were relatively smaller, thus suggesting an earlier light saturation of charge flux compared with CO2 uptake, as evident in the light intensity plots (Fig. 8b). When plotted against each other (Fig. 8c), a curvi-linear relationship was apparent, with the deviation from linearity being small, at least up to about 200 μmol m−2 s−1. Fig. 8 Simultaneously measured CO2 uptake (A + Resp) and P515 indicated charge flux in a dandelion leaf during the course of stepwise decrease of light intensity. Before start of measurement the leaf had been extensively pre-illuminated: 30 min at slowly increasing PAR up to 1,120 μmol m−2 s−1 at 380 μmol CO2, followed by 50 min at 1,120 μmol m−2 s−1, for stomatal opening and accumulation of zeaxanthin. 2.1 % O2 and 380 μmol mol−1 CO2 in nitrogen. 5 ms light/dark intervals.