Department of Biophysics, Biology Faculty of the M.V. Lomonosov Moscow State University, 119234, Moscow, Russia.
Photosynth Res. 2020 Dec;146(1-3):259-278. doi: 10.1007/s11120-020-00774-3. Epub 2020 Jul 30.
Measurements of OJIP-SMT patterns of fluorescence induction (FI) in Synechocystis sp. PCC 6803 (Synechocystis) cells on a time scale up to several minutes were mathematically treated within the framework of thylakoid membrane (T-M) model (Belyaeva et al., Photosynth Res 140:1-19, 2019) that was renewed to account for the state transitions effects. Principles of describing electron transfer in reaction centers of photosystems II and I (PSII and PSI) and cytochrome bf complex remained unchanged, whereas parameters for dissipative reactions of non-radiative charge recombination were altered depending on the oxidation state of Q-site (neutral, reduced by one electron, empty, reduced by two electrons). According to our calculations, the initial content of plastoquinol (PQH) in the total quinone pool of Synechocystis cells adapted to darkness for 10 min ranged between 20 and 40%. The results imply that the PQ pool mediates photosynthetic and respiratory charge flows. The redistribution of PBS antenna units responsible for the increase of Chl fluorescence in cyanobacteria (qT) upon state 2 → 1 transition or the fluorescence lowering (qT) due to state 1 → 2 transition were described in the model by exponential functions. Parameters of dynamically changed effective cross section were found by means of simulations of OJIP-SMT patterns observed on Synechocystis cells upon strong (3000 μmol photons ms) and moderate (1000 μmol photons ms) actinic light intensities. The corresponding light constant values kL = 1.2 ms and 0.4 ms define the excitation of total antenna pool dynamically redistributed between PSII and PSI reaction centers. Although the OCP-induced quenching of antenna excitation is not involved in the model, the main features of the induction signals have been satisfactorily explained. In the case of strong illumination, the effective cross section decreases by approximately 33% for irradiated Synechocystis cells as compared to untreated cells. Under moderate light, the irradiated Synechocystis cells showed in simulations the same cross section as the untreated cells. The thylakoid model renewed with state transitions description allowed simulation of fluorescence induction OJIP-SMT curves detected on time scale from microseconds to minutes.
在藻胆体膜(T-M)模型的框架内对 Synechocystis sp. PCC 6803(集胞藻)细胞的荧光诱导(FI)OJIP-SMT 模式的测量结果进行了长达数分钟的时间尺度的数学处理(Belyaeva 等人,Photosynth Res 140:1-19, 2019),该模型进行了更新以考虑状态转变的影响。描述光系统 II 和 I(PSII 和 PSI)反应中心电子转移以及细胞色素 bf 复合物的原则保持不变,而取决于 Q 位的氧化状态(中性、被一个电子还原、空、被两个电子还原),非辐射电荷复合耗散反应的参数发生了变化。根据我们的计算,适应黑暗 10 分钟的集胞藻细胞总醌库中质体醌(PQH)的初始含量在 20%至 40%之间。结果表明,PQ 库介导光合作用和呼吸电荷流动。在状态 2→1 转变或由于状态 1→2 转变导致的荧光降低(qT)时,负责增加蓝细菌 Chl 荧光的 PBS 天线单元的再分配(qT)在模型中用指数函数描述。通过模拟在强(3000 μmol 光子 ms)和中等(1000 μmol 光子 ms)光强下集胞藻细胞上观察到的 OJIP-SMT 模式,找到了动态变化的有效截面的参数。相应的光常数值 kL=1.2 ms 和 0.4 ms 定义了在 PSII 和 PSI 反应中心之间动态重新分配的总天线池的激发。尽管模型中不涉及 OCP 诱导的天线激发猝灭,但诱导信号的主要特征得到了令人满意的解释。在强光照下,与未处理的细胞相比,辐照的集胞藻细胞的有效截面减少了约 33%。在中等光照下,模拟的辐照集胞藻细胞的截面与未处理的细胞相同。带有状态转变描述的更新的类囊体模型允许模拟在从微秒到分钟的时间尺度上检测到的荧光诱导 OJIP-SMT 曲线。