Dynamics of electron transfer within and between PS II reaction center complexes indicated by the light-saturation curve of in vivo variable chlorophyll fluorescence emission

The dynamics of light-induced closure of the PS II reaction centers was studied in intact, dark-adapted leaves by measuring the light-irradiance (I) dependence of the relative variable chlorophyll fluorescence V which is the ratio between the amplitude of the variable fluorescence induced by a pulse of actinic light and the maximal variable fluorescence amplitude obtained with an intense, supersaturating light pulse. It is shown that the light-saturation curve of V is a hyperbola of order n. The experimental values of n ranged from around 0.75 to around 2, depending on the plant material and the environmental conditions. A simple theoretical analysis confirmed this hyperbolic relationship between V and I and suggested that n could represent the apparent number of photons necessary to close one reaction center. Thus, experimental conditions leading to n values higher than 1 could indicate that, from a macroscopic viewpoint, more than one photon is necessary to close one PS II center, possibly due to changes in the relative concentrations of the different redox states of the PS II reaction center complexes at the quasi-steady state induced by the actinic light. On the other hand, the existence of environmental conditions resulting in n noticeably lower than 1 suggests the possibility of an electron flow between PS II reaction center complexes.Abbreviations F₀ and F_m minimal and maximal levels of chlorophyll fluorescence emission, respectively - F_p peak fluorescence induced by a pulse of actinic light - I incident light irradiance (in W m^-2) - PS II Photosystem II - P₆₈₀ PS II reaction center - Q_A and Q_B primary and secondary (stable) electron acceptors of PS II - V relative variable chlorophyll fluorescence % MathType!MTEF!2!1!+-% feaafiart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGak0Jf9crFfpeea0xh9v8qiW7rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaiikaiaadA% facqGH9aqpcaGGOaGaaeOramaaBaaaleaacaqGWbaabeaakiabgkHi% TiaabAeadaWgaaWcbaGaaeimaaqabaGccaGGPaGaai4laiaacIcaca% qGgbWaaSbaaSqaaiaab2gaaeqaaOGaeyOeI0IaaeOramaaBaaaleaa% caqGWaaabeaakiaacMcacaGGPaaaaa!47BD!\[(V = ({\text{F}}_{\text{p}} - {\text{F}}_{\text{0}} )/({\text{F}}_{\text{m}} - {\text{F}}_{\text{0}} ))\]     

Heat stress induces in leaves an increase of the minimum level of chlorophyll fluorescence, Fo: A time-resolved analysis

A time-resolved study of the effects of heat stress (23 to 50°C) on F_o level of chlorophyll fluorescence of leaves having different antenna content has been performed in order to elucidate the causes of heat induced increase of F_o in vivo. The multi-exponential deconvolution of the decays after a picosecond flash at F_o have shown that the best fit in both wild-type and the mutant chlorina F2 of barley leaves is obtained with three components in the temperature range utilized (100, 400 and 1200 ps at 23°C). In intermittent light greened pea leaves, a fourth long lifetime component (4 ns at 23°C) is needed. The comparison of the three types of leaves at 23°C shows that the content of the LHCII b complex does not affect the lifetimes of the two main components (100 and 400 ps) and affects their preexponential factors. This result suggests that in the PS II unit the exciton transfer from LHC IIb to the rest of the antenna is irreversible. The effects of heat stress on individual lifetime components, T_i, included several changes. Utilizing for PS II unit an extended ‘Reversible Radical Pair’ model, having three compartments, to interpret the variations of T_i and A_i induced by temperature increases, it can be inferred that heat determines: (i) an irreversible disconnection of a monor antenna complex which is not the LHC IIb complex, this effect is induced by temperatures higher than 40°C; (ii) a decrease of the quantum efficiency of Photosystem II photochemistry which is due to several effects: a decrease of the rate of charge separation, an increase of P⁺I^- recombination rate constant and a decrease of the stabilization of charges. These effects on Photosystem II photochemistry start to occur above 30°C and are partially reversible.     

In search of a reversible stage of photoinhibition in a higher plant: No changes in the amount of functional Photosystem II accompany relaxation of variable fluorescence after exposure of lincomycin-treated Cucurbita pepo leaves to high light

Pumpkin (Cucurbita pepo L.) leaves in which chloroplast protein synthesis was inhibited with lincomycin were exposed to strong photoinhibitory light, and changes in F_O, F_M, F_V/F_M and in the amount of functional Photosystem II (O₂ evolution induced by saturating single-turnover flashes) were monitored during the high-light exposure and subsequent dark or low-light incubation. In the course of the photoinhibitory illumination, F_M, F_V/F_M and the amount of functional PS II declined continuously whereas F_O dropped rapidly to some extent and then slowly increased. If the experiments were done at room temperature, termination of the photoinhibitory illumination resulted in partial relaxation of the F_V/F_M ratio and in an increase in F_O and F_M. The relaxation was completed in 10–15 min after short-term (15 min) photoinhibitory treatment but continued 30–40 min if the exposure to high light was longer than 1 h. No changes in the amount of functional PS II accompanied the relaxation of F_V/F_M in darkness or in low light, in the presence of lincomycin. Transferring the leaves to low temperature (+4°C) after the room-temperature illumination (2 h) completely inhibited the relaxation of F_V/F_M. Low temperature did not suppress the relaxation if the photoinhibitory illumination had also been done at low temperature. The results indicate that illumination of lincomycin-poisoned pumpkin leaves at room temperature does not lead to accumulation of a reversibly photoinactivated intermediate.Abbreviations F_O, F_M chlorophyll fluorescence with all reaction centres open or closed, respectively - F_V variable fluorescence (F_V=F_M–F_O) - LHC Light-harvesting complex - PS II Photosystem II - Q_A, Q_B primary and secondary quinone electron acceptors of PS II, respectively - qN_E, qN_T, qN_I non-photochemical quenching due to high-energy state, state transition or photoinhibition, respectively     

Action of UV and visible radiation on chlorophyll fluorescence from dark-adapted grape leaves (Vitis vinifera L.)

Grapevine plants (Vitis vinifera L. cv. Silvaner) were cultivated under shaded conditions in the absence of UV radiation in a greenhouse, and subsequently placed outdoors under filters transmitting natural radiation, or screening out the UV-B (280 to 315 nm), or screening out the UV-A (315 to 400 nm) and the UV-B spectral range. All conditions decreased maximum chlorophyll fluorescence (F_M) and increased minimum chlorophyll fluorescence (F₀) from dark-adapted leaves; however, with increasing UV, F_M quenching was stimulated but increases in F₀ were reduced. The F_V/F_M ratio (where F_V=F_M-F₀) was clearly reduced by visible radiation (VIS): UV-B caused a moderate extra-reduction in F_V/F_M. Exposure of leaves (V. vinifera L. cv. Bacchus) to UV or VIS lamps quenched the F_M to similar extents; further, UV-B doses comparable to the field, quenched F₀. A model was developed to describe how natural radiation intensities affect PS II and thereby change leaf fluorescence. Fitting theory to experiment was successful when the same F_M yield for UV- and VIS-inactivated PS II was assumed, and for lower F₀ yields of UV- than for VIS-inactivated PS II. It is deduced, that natural UV can produce inactivated PS II exhibiting relatively high F_V/F_M. The presence of UV-inactivated PS II is difficult to detect by measuring F_V/F_M in leaves. Hence, relative concentrations of intact PS II during outdoor exposure were derived from F_M. These concentrations, but not F_V/F_M, correlated reasonably well with CO₂ gas exchange measurements. Consequently, PS II inhibition by natural UV could be a main factor for UV inhibition of photosynthesis.This revised version was published online in October 2005 with corrections to the Cover Date.     

Light-induced fluorescence quenching in the light-harvesting chlorophyll a/b protein complex

Summary Irradiation of the principal photosystem II light-harvesting chlorophyll-protein antenna complex, LHC II, with high light intensities brings about a pronounced quenching of the chlorophyll fluorescence. Illumination of isolated thylakoids with high light intensities generates the formation of quenching centres within LHC II in vivo, as demonstrated by fluorescence excitation spectroscopy. In the isolated complex it is demonstrated that the light-induced fluorescence quenching: a) shows a partial, biphasic reversibility in the dark; b) is approximately proportional to the light intensity; c) is almost independent of temperature in the range 0–30°C; d) is substantially insensitive to protein modifying reagents and treatments; e) occurs in the absence of oxygen. A possible physiological importance of the phenomenon is discussed in terms of a mechanism capable of dissipating excess excitation energy within the photosystem II antenna.Abbreviations chla chlorophyll a - chlb chlorophyll b - F₀ fluorescence yield with reaction centers open - F_m fluorescence yield with reaction centres closed - F_i fluorescence at the plateau level of the fast induction phase - LHC II light-harvesting chlorophyll a/b protein complex II - PS II photosystem II - PSI photosystem I - Tricine N-[2-hydroxy-1,1-bis(hydroxymethyl)ethyl]glycine     

Electron transfer in reaction centers of Rhodobacter sphaeroides and Rhodobacter capsulatus monitored by fluorescence of the bacteriochlorophyll dimer

Spectral and kinetic characteristics of fluorescence from isolated reaction centers of photosynthetic purple bacteria Rhodobacter sphaeroides and Rhodobacter capsulatus were measured at room temperature under rectangular shape of excitation at 810 nm. The kinetics of fluorescence at 915 nm reflected redox changes due to light and dark reactions in the donor and acceptor quinone complex of the reaction center as identified by absorption changes at 865 nm (bacteriochlorophyll dimer) and 450 nm (quinones) measured simultaneously with the fluorescence. Based on redox titration and gradual bleaching of the dimer, the yield of fluorescence from reaction centers could be separated into a time-dependent (originating from the dimer) and a constant part (coming from contaminating pigment (detached bacteriochlorin)). The origin was also confirmed by the corresponding excitation spectra of the 915 nm fluorescence. The ratio of yields of constant fluorescence over variable fluorescence was much smaller in Rhodobacter sphaeroides (0.15±0.1) than in Rhodobacter capsulatus (1.2±0.3). It was shown that the changes in fluorescence yield reflected the disappearance of the dimer and the quenching by the oxidized primary quinone. The redox changes of the secondary quinone did not have any influence on the yield but excess quinone in the solution quenched the (constant part of) fluorescence. The relative yields of fluorescence in different redox states of the reaction center were tabulated. The fluorescence of the dimer can be used as an effective tool in studies of redox reactions in reaction centers, an alternative to the measurements of absorption kinetics.Abbreviations Bchl bacteriochlorophyll - Bpheo bacteriopheophytin - D electron donor to P⁺ - P bacteriochlorophyll dimer - Q quinone acceptor - Q_A primary quinone acceptor - Q_B secondary quinone acceptor - RC reaction center protein - UQ₆ ubiquinone-30     

A simple model relating photoinhibitory fluorescence quenching in chloroplasts to a population of altered Photosystem II reaction centers

A model is presented describing the relationship between chlorophyll fluorescence quenching and photoinhibition of Photosystem (PS) II-dependent electron transport in chloroplasts. The model is based on the hypothesis that excess light creates a population of inhibited PS II units in the thylakoids. Those units are supposed to posses photochemically inactive reaction centers which convert excitation energy to heat and thereby quench variable fluorescence. If predominant photoinhibition of PS II and cooperativity in energy transfer between inhibited and active units are presumed, a quasi-linear correlation between PS II activity and the ratio of variable to maximum fluorescence, F_VF_M, is obtained. However, the simulation does not result in an inherent linearity of the relationship between quantum yield of PS II and F_VF_M ratio. The model is used to fit experimental data on photoinhibited isolated chloroplasts. Results are discussed in view of current hypotheses of photoinhibition.Abbreviations F_M maximum total fluorescence - F₀ initial fluorescence - F_V maximum variable fluorescence - PS Photosystem - Q_A, Q_B primary and secondary electron acceptors of Photosystem II     

Autotrophic cells of the <Emphasis Type="Italic">Synechocystis psbH</Emphasis> deletion mutant are deficient in synthesis of CP47 and accumulate inactive PS II core complexes

Cells of the psbH deletion mutant IC7 of the cyanobacterium Synechocystis PCC 6803 grown in the absence of glucose contain strongly reduced levels of chlorophyll when compared with cells grown in the presence of glucose, or compared with wild-type (WT) cells. Low-temperature fluorescence emission spectra revealed decreased content of both active PS II (Photosystem II) and PS I (Photosystem I) complexes. Analysis of thylakoid membrane complexes of IC7 by native electrophoresis showed a similar set of chlorophyll–proteins, namely a PS II core complex and trimeric and monomeric PS II complexes, as in WT. However, in contrast to WT, the ³⁵S-methionine protein labeling pattern of the mutant exhibited no preferential labeling of the D1 protein in the PS II core complexes, and the labeled D1 and D2 proteins accumulated predominantly in the PS II reaction center lacking CP47. The results show that in autotrophically grown cells of the psbH deletion mutant, selective D1 turnover is inhibited and synthesis of CP47 becomes a limiting step in the PS II assembly.     

Characterization of the photosystem II centers inactive in plastoquinone reduction by fluorescence induction

In order to characterize the photosystem II (PS II) centers which are inactive in plastoquinone reduction, the initial variable fluorescence rise from the non-variable fluorescence level F_o to an intermediate plateau level F_i has been studied. We find that the initial fluorescence rise is a monophasic exponential function of time. Its rate constant is similar to the initial rate of the fastest phase (-phase) of the fluorescence induction curve from DCMU-poisoned chloroplasts. In addition, the initial fluorescence rise and the -phase have the following common properties: their rate constants vary linearly with excitation light intensity and their fluorescence yields are lowered by removal of Mg⁺⁺ from the suspension medium. We suggest that the inactive PS II centers, which give rise to the fluorescence rise from F_o to F_i, belong to the -type PS II centers. However, since these inactive centers do not display sigmoidicity in fluorescence, they thus do not allow energy transfer between PS II units like PS II.Abbreviations DCMU 3-(3,4-dichlorophenyl)-1,1-dimethyl urea - DMQ 2,5-dimethyl-p-benzoquinone - F_o initial non-variable fluorescence yield - F_m maximum fluorescence yield - F_i intermediate fluorescence yield - PS II photosystem II - Q_A primary quinone acceptor of PS II - Q_B secondary quinone acceptor of PS II     

Acceptor side photoinhibition in PS II: On the possible effects of the functional integrity of the PS II donor side on photoinhibition of stable charge separation

Photoinhibition under aerobic and anaerobic conditions was analyzed in O₂-evolving and in Tris-treated PS II-membrane fragments from spinach by measuring laser-flash-induced absorption changes at 826 nm reflecting the transient P680⁺ formation and the chlorophyll fluorescence lifetime. It was found that anaerobic photoinhibitory treatment leads in both types of samples to the appearence of two long-lived fluorescence components with lifetimes of 7 ns and 16 ns, respectively. The extent of these fluorescence kinetics depends on the state of the reaction center (open/closed) during the fluorescence measurements: it is drastically higher in the closed state. It is concluded that this long-lived fluorescence is mainly emitted from modified reaction centers with singly reduced Q_A(Q_A ^-). This suggests that the observation of long-lived fluorescence components cannot necessarily be taken as an indicator for reaction centers with missing or doubly reduced and protonated Q_A (Q_AH₂). Time-resolved measurements of 826 nm absorption changes show that the rate of photoinhibition of the stable charge separation (P680^*Q_A P680⁺Q_A ^-), is nearly the same in O₂-evolving and in Tris-treated PS II-membrane fragments. This finding is difficult to understand within the framework of the Q_AH₂-mechanism for photoinhibition of stable charge separation because in that case the rate of photoinhibition should strongly depend on the functional integrity of the donor side of PS II. Based on the results of this study it is inferred, that several processes contribute to photoinhibition within the PS II reaction center and that a mechanism which comprises double reduction and protonation of Q_A leading to Q_AH₂ formation is only of marginal – if any – relevance for photoinhibition of PS II under both, aerobic and anaerobic, conditions.     

State 1-state 2 transition in leaves and its association with ATP-induced chlorophyll fluorescence quenching

By using chlorophyll fluorescence, a study has been made of changes in spillover of excitation energy from Photosystem (PS) II to PS I associated with the State 1–State 2 transition in intact pea and barley leaves and in isolated envelope-free chloroplasts treated with ATP. (1) In pea leaves, illumination with light preferentially absorbed by PS II (Light 2) led to a condition of maximum spillover (state 2) while light preferentially absorbed by PS I induced minimum spillover condition (State 1) as judged from the redox state of Q and low-temperature emission spectra. The State 1–State 2 transitions took several minutes to occur, with the time increasing when the temperature was lowered from 19 to 6°C. (2) In contrast to the wild type, leaves of a chlorophyll b-less mutant barley did not exhibit a State 1–State 2 transition, suggesting the involvement of the light-harvesting chlorophyll $\text{a}\text{b-}\text{protein}$ complex in spillover changes in higher plants. (3) Spillover in isolated pea chloroplasts was increased by treatment with ATP either (a) in Light 2 in the absence of an electron acceptor or (b) in the dark in the presence of NADPH and ferredoxin. These observations can be interpreted in terms of the model that a more reduced state of plastoquinone activates the protein kinase which catalyzes phosphorylation of the light-harvesting chlorophyll $\text{a}\text{b-}\text{protein}$ complex (Allen, J.F., Bennett, J., Steinback, K.E. and Arntzen, C.J. (1981). Nature 291, 25–29). This process was found to be very temperature sensitive. (4) Pea chloroplasts illuminated in the presence of ATP seemed to exhibit a slight decrease in the degree of thylakoid stacking, and an increased intermixing of the two photosystems. (5) The possible mechanism by which protein phosphorylation regulates the State 1–State 2 changes in intact leaves is presented in terms of changes in the spatial relationship of two photosystems resulting from alteration in membrane organization.     

Delayed fluorescence observed in the nanosecond time region at 77 K originates directly from the photosystem II reaction center

The excited-state dynamics of delayed fluorescence in photosystem (PS) II at 77 K were studied by time-resolved fluorescence spectroscopy and decay analysis on three samples with different antenna sizes: PS II particles and the PS II reaction center from spinach, and the PS II core complexes from Synechocystis sp. PCC 6803. Delayed fluorescence in the nanosecond time region originated from the 683-nm component in all three samples, even though a slight variation in lifetimes was detected from 15 to 25 ns. The relative amplitude of the delayed fluorescence was higher when the antenna size was smaller. Energy transfer from the 683-nm pigment responsible for delayed fluorescence to antenna pigment(s) at a lower energy level was not observed in any of the samples examined. This indicated that the excited state generated by charge recombination was not shared with antenna pigments under the low-temperature condition, and that delayed fluorescence originates directly from the PS II reaction center, either from chlorophyll a_D1 or P680. Supplemental data on delayed fluorescence from spinach PS I complexes are included.     

Light-induced quenching of chlorophyll fluorescence at 77 K in leaves,chloroplasts and Photosystem II particles

The light-induced chlorophyll (Chl) fluorescence decline at 77 K was investigated in segments of leaves, isolated thylakoids or Photosystem (PS) II particles. The intensity of chlorophyll fluorescence declines by about 40% upon 16 min of irradiation with 1000 μmol m⁻² s⁻¹ of white light. The decline follows biphasic kinetics, which can be fitted by two exponentials with amplitudes of approximately 20 and 22% and decay times of 0.42 and 4.6 min, respectively. The decline is stable at 77 K, however, it is reversed by warming of samples up to 270 K. This proves that the decline is caused by quenching of fluorescence and not by pigment photodegradation. The quantum yield for the induction of the fluorescence decline is by four to five orders lower than the quantum yield of Q_A reduction. Fluorescence quenching is only slightly affected by addition of ferricyanide or dithionite which are known to prevent or stimulate the light-induced accumulation of reduced pheophytin (Pheo). The normalised spectrum of the fluorescence quenching has two maxima at 685 and 695 nm for PS II emission and a plateau for PS I emission showing that the major quenching occurs within PS II. ‘Light-minus-dark’ difference absorbance spectra in the blue spectral region show an electrochromic shift for all samples. No absorbance change indicating Chl oxidation or Pheo reduction is observed in the blue (410–600 nm) and near infrared (730–900 nm) spectral regions. Absorbance change in the red spectral region shows a broad-band decrease at approximately 680 nm for thylakoids or two narrow bands at 677 and 670–672 nm for PS II particles, likely resulting also from electrochromism. These absorbance changes follow the slow component of the fluorescence decline. No absorbance changes corresponding to the fast component are found between 410 and 900 nm. This proves that the two components of the fluorescence decline reflect the formation of two different quenchers. The slow component of the light-induced fluorescence decline at 77 K is related to charge accumulation on a non-pigment molecule of the PS II complex. This revised version was published online in June 2006 with corrections to the Cover Date.     

Light-dependent modification of Photosystem II in spinach leaves

In dark-adapted spinach leaves approximately one third of the Photosystem II (PS II) reaction centers are impaired in their ability to transfer electrons to Photosystem I. Although these inactive PS II centers are capable of reducing the primary quinone acceptor, Q_A, oxidation of Q_A ^– occurs approximately 1000 times more slowly than at active centers. Previous studies based on dark-adapted leaves show that minimal energy transfer occurs from inactive centers to active centers, indicating that the quantum yield of photosynthesis could be significantly impaired by the presence of inactive centers. The objective of the work described here was to determine the performance of inactive PS II centers in light-adapted leaves. Measurements of PS II activity within leaves did not indicate any increase in the concentration of active PS II centers during light treatments between 10 s and 5 min, showing that inactive centers are not converted to active centers during light treatment. Light-induced modification of inactive PS II centers did occur, however, such that 75% of these centers were unable to sustain stable charge separation. In addition, the maximum yield of chlorophyll fluorescence associated with inactive PS II centers decreased substantially, despite the lack of any overall quenching of the maximum fluorescence yield. The effect of light treatment on inactive centers was reversed in the dark within 10–20 mins. These results indicate that illumination changes inactive PS II centers into a form that quenches fluorescence, but does not allow stable charge separation across the photosynthetic membrane. One possibility is that inactive centers are converted into centers that quench fluorescence by formation of a radical, such as reduced pheophytin or oxidized P680. Alternatively, it is possible that inactive PS II centers are modified such that absorbed excitation energy is dissipated thermally, through electron cycling at the reaction center.Abbreviations A518 absorbance change at 518 nm, reflecting the formation of an electric field across the thylakoid membrane - A_FL1 amplitude of the fast (<100 ms) phase of A518 induced by the first of two saturating, single-turnover flashes spaced 30 ms apart - A_FL2 amplitude of the fast (<100 ms) phase of A518 induced by the second of two saturating, single-turnover flashes spaced 50 ms apart - DCBQ 2,6-dichloro-p-benzoquinone - Fo yield of chlorophyll fluorescence when Q_A is fully oxidized - Fm yield of chlorophyll fluorescence when Q_A is fully reduced - Fx yield of chlorophyll fluorescence when Q_A is fully reduced at inactive PS II centers, but fully oxidized at active PS II centers - Pheo pheophytin - P680 the primary donor of Photosystem II - PPFD photosynthetic photon flux density - Q_A Primary quinone acceptor of PS II - Q_B secondary quinone acceptor of PS II     

遮荫下高原濒危药用植物川贝母(Fritillaria cirrhosa)光合作用和叶绿素荧光特征

测量了川贝母遮荫和全光下叶片光合生理参数和叶绿素荧光参数,探讨了其遮荫下生理生态学指标的变化和强光下的光适应机制,且对光合生理的测量过程给出了全面系统的介绍.川贝母日光合曲线呈双峰变化,遮荫后川贝母光合效率(Pmax)、细胞内CO2浓度(Ci)分别增加了31.1%、10%(p<0.01),有效光反应光强域值(PFD)增加了331.5 [μmol/(m2·s)],最大表观量子效率(AQY)和气孔导度(COND)也有所增加,暗呼吸速率(Rd)和叶片蒸汽压亏缺(Vpdl)明显降低,此均有利用光合产物的积累;F′v/F′m(光照下反应中心能量捕获效率)、qP(光化学淬灭)、ETR(电子传递效率)、Psips2(PSⅡ的效率)分别增加了14.7%(p<0.01)、8.8%(p<0.01)、10%(p<0.01)、24.2%(p>0.05),促进了川贝母叶片对光能的利用;Fv/Fm(光化学效率)变化不明显,说明"灯笼花"阶段,全光下川贝母没有受到到明显的胁迫,光合机构未遭到破坏.当自然光强超过光饱和点时,川贝母主要通过提高非化学淬灭,耗散过多吸收的热能以防止光合机构的破坏.当出现极端气候(高温干旱)时,川贝母繁育退化现象("树儿子"或"灯笼花"阶段退回到"一匹叶"生长阶段)可能是对环境适应的主要方式.另外川贝母叶片狭小、叶片倾角较大降低了强光辐射的有效面积,在形态结构上有利于避免过高光强对叶光合器官的损伤.     

Determination of the primary charge separation rate in Photosystem II reaction centers at 15 K

We have measured the rate constant for the formation of the oxidized chlorophyll a electron donor (P680⁺) and the reduced electron acceptor pheophytin a ^– (Pheo a ^–) following excitation of isolated Photosystem II reaction centers (PS II RC) at 15 K. This PS II RC complex consists of D₁, D₂, and cytochrome b-559 proteins and was prepared by a procedure which stabilizes the protein complex. Transient absorption difference spectra were measured from 450–840 nm as a function of time with 500fs resolution following 610 nm laser excitation. The formation of P680⁺-Pheo a ^– is indicated by the appearance of a band due to P680⁺ at 820 nm and corresponding absorbance changes at 490, 515 and 546 nm due to the formation of Pheo a ^–. The appearance of the 490 nm and 820 nm bands is monoexponenital with =1.4±0.2 ps. Treatment of the PS II RC with sodium dithionite and methyl viologen followed by exposure to laser excitation results in accumulation of Pheo a ^–. Laser excitation of these prereduced RCs at 15 K results in formation of a transient absorption spectrum assigned to ^1*P680. We observe wavelength-dependent kinetics for the recovery of the transient bleach of the Q_y absorption bands of the pigments in both untreated and pre-reduced PS II RCs at 15K. This result is attributed to an energy transfer process within the PS II RC at low temperature that is not connected with charge separation.Abbreviations PS I Photosystem I - PS II Photosystem II - RC reaction center - P680 primary electron donor in Photosystem II - Chl a chlorophyll a - Pheo a pheophytin a     

Measurement of gradients of absorbed light in spinach leaves from chlorophyll fluorescence profiles

Profiles of chlorophyll fluorescence were measured in spinach leaves irradiated with monochromatic light. The characteristics of the profiles within the mesophyll were determined by the optical properties of the leaf tissue and the spectral quality of the actinic light. When leaves were infiltrated with 10^?4M DCMU [3‐(3,4‐dichlorophenyl)‐1, 1‐dimethyl‐urea] or water, treatments that minimized light scattering, irradiation with 2000 μmol m^?2 s^?1 green light produced broad Gaussian‐shaped fluorescence profiles that spanned most of the mesophyll. Profiles for chlorophyll fluorescence in the red (680 ± 16 nm) and far red (λ > 710 nm) were similar except that there was elevated red fluorescence near the adaxial leaf surface relative to far red fluorescence. Fluorescence profiles were narrower in non‐infiltrated leaf samples where light scattering increased the light gradient. The fluorescence profile was broader when the leaf was irradiated on its adaxial versus abaxial surface due to the contrasting optical properties of the palisade and spongy mesophyll. Irradiation with blue, red and green monochromatic light produced profiles that peaked 50, 100 and 150 μm, respectively, beneath the irradiated surface. These results are consistent with previous measurements of the light gradient in spinach and they agree qualitatively with measurements of carbon fixation under monochromatic blue, red and green light. These results suggest that chlorophyll fluorescence profiles may be used to estimate the distribution of quanta that are absorbed within the leaf for photosynthesis.     

Drought-induced changes in chlorophyll fluorescence,photosynthetic pigments,and thylakoid membrane proteins of Vigna radiata

The effects of drought on chlorophyll fluorescence characteristics of PSII, photosynthetic pigments, thylakoid membrane protein (D1), and proline content in different varieties of mung bean plants were studied. Drought stress inhibits PSII activity and induces alterations in D1 protein. We observed a greater decline in the effective quantum yield of PSII, electron transport rate, and saturating photosynthetically active photon flux density (PPFD_sat) under drought stress in var. Anand than var. K-851 and var. RMG 268. This may possibly be due to either downregulation of photosynthesis or photoinhibition process. Withholding irrigation resulted in gradual diminution in total Chl content at Day 4 of stress. HPLC analysis revealed that the quantity of β-carotene in stressed plants was always higher reaching maxima at Day 4. Photoinactivation of PSII in var. Anand includes the loss of the D1 protein, probably from greater photosynthetic damage caused by drought stress than the other two varieties.     

Evidence for localisation of accumulated chlorophyll cation on the D1-accessory chlorophyll in the reaction centre of Photosystem II

Absorption and circular dichroism spectra of Photosystem II (PS II) reaction centres (RC) were studied and compared with spectra calculated on the basis of point-dipole approximation. Chlorophyll cation was accumulated during a light treatment of PS II RC in the presence of artificial electron acceptor silicomolybdate. Light-induced difference spectra and their calculated counterparts revealed the location of accumulated cation at the accessory chlorophyll of the D1 protein subunit.     

An instrument capable of imaging chlorophyll a fluorescence from intact leaves at very low irradiance and at cellular and subcellular levels of organization

An instrument capable of imaging chlorophyll a fluorescence, from intact leaves, and generating images of widely used fluorescence parameters is described. This instrument, which is based around a fluorescence microscope and a Peltier-cooled charge-coupled device (CCD) camera, differs from those described previously in two important ways. First, the instrument has a large dynamic range and is capable of generating images of chlorophyll a fluorescence at levels of incident irradiance as low as 0.1 μmol m^?2 s^?1. Secondly, chlorophyll fluorescence, and consequently photosynthetic performance, can be resolved down to the level of individual cells and chloroplasts. Control of the instrument, as well as image capture, manipulation, analysis and presentation, are executed through an integrated computer application, developed specifically for the task. Possible applications for this instrument include detection of early and differential responses to environmental stimuli, including various types of stress. Images illustrating the instrument's capabilities are presented.