Vasil'ev S, Bruce D
Department of Biological Sciences, Brock University, St. Catharines, Ontario, Canada.
Biochemistry. 1998 Aug 4;37(31):11046-54. doi: 10.1021/bi9806854.
Chlorophyll a fluorescence emission is widely used as a noninvasive measure of a number of parameters related to photosynthetic efficiency in oxygenic photosynthetic organisms. The most important component for the estimation of photochemistry is the relative increase in fluorescence yield between dark-adapted samples which have a maximal capacity for photochemistry and a minimal fluorescence yield (F0) and light-saturated samples where photochemistry is saturated and fluorescence yield is maximal (Fm). However, when photosynthesis is saturated with a short (less than 50 micro(s)) flash of light, which induces only one photochemical turnover of photosystem II, the maximal fluorescence yield is significantly lower (Fsat) than when saturation is achieved with a millisecond duration multiturnover flash (Fm). To investigate the origins of the difference in fluorescence yield between these two conditions, our time-resolved fluorescence apparatus was modified to allow collection of picosecond time-resolved decay kinetics over a short time window immediately following a saturating single-turnover flash (Fsat) as well as after a multiturnover saturating pulse (Fm). Our data were analyzed with a global kinetic model based on an exciton radical pair equilibrium model for photosystem II. The difference between Fm and Fsat was modeled well by changing only the rate constant for quenching of excitation energy in the antenna of photosystem II. An antenna-based origin for the quenching was verified experimentally by the observation that addition of the antenna quencher 5-hydroxy-1,4-naphthoquinone to thylakoids under Fm conditions resulted in decay kinetics and modeled kinetic parameters very similar to those observed under Fsat conditions in the absence of added quinone. Our data strongly support the origin of low fluorescence yield at Fsat to be an antenna-based nonphotochemical quenching of excitation energy in photosystem II which has not usually been considered explicitly in calculations of photochemical and nonphotochemical quenching parameters. The implications of our data with respect to kinetic models for the excited-state dynamics of photosystem II and the practical applications of the fluorescence yield parameters Fm and Fsat to calculations of photochemical yield are discussed.
叶绿素a荧光发射被广泛用作一种非侵入性手段,用于测量与含氧光合生物光合效率相关的多个参数。用于估算光化学的最重要组成部分是暗适应样品(具有最大光化学能力且荧光产量最小(F0))与光饱和样品(光化学饱和且荧光产量最大(Fm))之间荧光产量的相对增加。然而,当光合作用用短(小于50微秒)闪光饱和时,该闪光仅诱导光系统II的一次光化学周转,最大荧光产量(Fsat)明显低于用毫秒持续时间的多周转闪光实现饱和时的最大荧光产量(Fm)。为了研究这两种条件下荧光产量差异的起源,我们对时间分辨荧光装置进行了改进,以便在饱和单周转闪光(Fsat)之后以及多周转饱和脉冲(Fm)之后的短时间窗口内收集皮秒时间分辨衰减动力学。我们的数据用基于光系统II的激子自由基对平衡模型的全局动力学模型进行了分析。通过仅改变光系统II天线中激发能猝灭的速率常数,很好地模拟了Fm和Fsat之间的差异。通过观察到在Fm条件下向类囊体中添加天线猝灭剂5-羟基-1,4-萘醌导致衰减动力学和模拟动力学参数与在不添加醌的情况下在Fsat条件下观察到的非常相似,实验验证了基于天线的猝灭起源。我们的数据有力地支持了Fsat时低荧光产量的起源是光系统II中基于天线的激发能非光化学猝灭,而在光化学和非光化学猝灭参数的计算中通常没有明确考虑这一点。讨论了我们的数据对光系统II激发态动力学动力学模型的影响以及荧光产量参数Fm和Fsat在光化学产量计算中的实际应用。