Department of Biology, St. Francis Xavier University, P.O. Box 5000, B2G 2W5, Antigonish, Nova Scotia, Canada.
Photosynth Res. 1996 Sep;49(3):251-62. doi: 10.1007/BF00034786.
Previous work has shown that the maximum fluorescence yield from PS 2 of Synechococcus PCC 7942 occurs when the cells are at the CO2 compensation point. The addition of inorganic carbon (Ci), as CO2 or HCO3 (-), causes a lowering of the fluorescence yield due to both photochemical (qp) and non-photochemical (qN) quenching. In this paper, we characterize the qN that is induced by Ci addition to cells grown at high light intensities (500 μmol photons m(-2) s(-1)). The Ci-induced qN was considerably greater in these cells than in cells grown at low light intensities (50 μmol photons m(-2) s(-1)), when assayed at a white light (WL) intensity of 250 μmol photons m(-2) s(-1). In high-light grown cells we measured qN values as high as 70%, while in low-light grown cells the qN was about 16%. The qN was relieved when cells regained the CO2 compensation point, when cells were illuminated by supplemental far-red light (FRL) absorbed mainly by PS 1, or when cells were illuminated with increased WL intensities. These characteristics indicate that the qN was not a form of energy quenching (qE). Supplemental FRL illumination caused significant enhancement of photosynthetic O2 evolution that could be correlated with the changes in qp and qN. The increases in qp induced by Ci addition represent increases in the effective quantum yield of PS 2 due to increased levels of oxidized QA. The increase in qN induced by Ci represents a decrease in PS 2 activity related to decreases in the potential quantum yield. The lack of diagnostic changes in the 77 K fluorescence emission spectrum argue against qN being related to classical state transitions, in which the decrease in potential quantum yield of PS 2 is due either to a decrease in absorption cross-section or by increased 'spill-over' of excitation energy to PS 1. Both the Ci-induced qp (t 0.5<0.5 s) and qN (t 0.5≃1.6 s) were rapidly relieved by the addition of DCMU. The two time constants give further support for two separate quenching mechanisms. We have thus characterized a novel form of qN in cyanobacteria, not related to state transitions or energy quenching, which is induced by the addition of Ci to cells at the CO2-compensation point.
先前的工作表明,当 PS2 的细胞处于二氧化碳补偿点时,最大荧光产量来自聚球藻 PCC 7942 的 PS2。添加无机碳(Ci),如 CO2 或 HCO3(-),由于光化学(qp)和非光化学(qN)猝灭,会降低荧光产量。在本文中,我们描述了在高光强(500 μmol 光子 m(-2) s(-1))下生长的细胞中,由于 Ci 的添加而引起的 qN。当在 250 μmol 光子 m(-2) s(-1)的白光(WL)强度下进行测定时,与在低光强(50 μmol 光子 m(-2) s(-1))下生长的细胞相比,Ci 诱导的 qN 在这些细胞中要大得多。在高光强生长的细胞中,我们测量到高达 70%的 qN 值,而在低光强生长的细胞中,qN 值约为 16%。当细胞恢复二氧化碳补偿点时,当细胞被补充远红光(FRL)照射时,主要被 PS1 吸收,或者当细胞被增加的 WL 强度照射时,qN 被缓解。这些特征表明,qN 不是一种能量猝灭(qE)形式。补充的 FRL 照射导致光合作用 O2 演化的显著增强,这可以与 qp 和 qN 的变化相关联。Ci 添加引起的 qp 增加代表由于氧化 QA 水平增加而导致 PS2 的有效量子产率增加。Ci 诱导的 qN 增加代表与 PS2 活性相关的降低,这与潜在量子产率的降低有关。在 77 K 荧光发射光谱中缺乏诊断变化表明 qN 与经典状态转变无关,其中 PS2 的潜在量子产率降低要么是由于吸收截面的减小,要么是由于激发能量的“溢出”增加到 PS1。Ci 诱导的 qp(t0.5<0.5 s)和 qN(t0.5≃1.6 s)都可以通过添加 DCMU 迅速缓解。两个时间常数为两种独立的猝灭机制提供了进一步的支持。因此,我们在蓝细菌中描述了一种新型的 qN,它与状态转变或能量猝灭无关,而是由 Ci 在二氧化碳补偿点添加到细胞中引起的。