Light-induced changes of fluorescence and absorbance in spinach chloroplasts at −40 °C

1. 1. Spinach chloroplasts were stored in the dark for at least 1 h, rapidly cooled to −40 °C, and illuminated with continuous light or short saturating flashes. In agreement with the measurements of Joliot and Joliot, chloroplasts that had been preilluminated with one or two flashes just before cooling showed a less efficient increase in the yield of chlorophyll a fluorescence upon illumination at −40 °C than dark-adapted chloroplasts. The effect disappeared below −150 °C, but reappeared again upon warming to −40 °C. Little effect was seen at room temperature in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU), added after the preillumination.

2. 2. Light-induced absorbance difference spectra at −40 °C in the region 500–560 nm indicated the participation of two components, the socalled 518-nm change (P518) and C-550. After preillumination with two flashes the absorbance change at 518 nm was smaller, and almost no C-550 was observed. After four flashes, the bands of C-550 were clearly visible again.

3. 3. The fluorescence increase and the absorbance change at 518 nm showed the same type of flash pattern with a minimum after the second and a maximum at the fourth flash. In the presence of 100 μM hydroxylamine, the fluorescence response was low after the fourth and high again after the sixth flash, which confirmed the hypothesis that the flash effect was related to the so-called S-state of the electron transport pathway from water to Photosystem 2.

4. 4. The kinetics of the light-induced absorbance changes were the same at each wavelength, and, apart from the size of the deflection, they were independent of preillumination. Flash experiments indicated that the absorbance changes were a one-quantum reaction. This was also true for the fluorescence increase in dark-adapted chloroplasts, but with preilluminated chloroplasts several flashes were needed to approximately saturate the fluorescence yield.

5. 5. The results are discussed in terms of a mechanism involving two electron donors and two electron acceptors for System 2 of photosynthesis.

Phototransformation of the Red-Light-Absorbing Form to the Far-Red-Light-Absorbing Form of Phytochrome in Pea Epicotyl Tissue Measured by a Multichannel Transient Spectrum Analyser

Phototransformation of the red-light-absorbing form (P_R) tothe far-red-light-absorbing form (P_FR) of phytochrome in 7-day-oldetiolated pea epicotyl hook segments was examined at 0.5C aftera red laser flash excitation using a multichannel transientspectra analyser with electrically gated photomultiplier. Effectsof a red laser pulse on the induction of phototransformationfrom P_R to P_FR were saturated at Ca. 15 mJ for flash wavelengthsof both 640 and 655 nm. The amount of P_FR induced by a saturatinglaser pulse was ca. 50% of that obtained at the photostationaryequilibrium. A difference spectrum measured 15 µs afterthe flash showed an absorbance increase at 697 nm and a decreaseat 663 nm. A difference spectrum determined 200 ms after theflash showed no such major absorbance increase. Kinetic analysisof the rapid absorbance decrease at 700 and 710 nm gave onesimple first-order reaction component having a rate constantof 2,500 s^–1. Kinetics of P_FR appearance measured by absorbanceincrease at 750 nm was resolved into three first-order reactionshaving rate constants of 5, 1.8 and 0.4 s^–1. The secondflash light of 710 nm given 2 µs and 2 ms after the firstred flash irradiation on P_R resulted in the formation of P_Rrather than P_FR. (Received February 8, 1985; Accepted April 11, 1985)     

Light-induced absorbance changes due to Photosystems 1 and 2 in spinach chloroplasts at −50 °C

Absorbance changes in the region 500–565 nm and at 702 nm, brought about by excitation of Photosystems 1 and 2, respectively, were measured in spinach chloroplasts at ?50 °C. Either dark-adapted chloroplasts were used or chloroplasts preilluminated with a number of short saturating flashes just before cooling.Both photosystems were found to cause a light-induced increase of absorbance at 518 nm (due to “P518”). The System 1-induced change was not affected by preillumination. It decayed within 1 s in the dark and showed similar kinetics as P700. Experiments in the presence of external electron acceptors (methylviologen or Fe(CN)₆^3?) suggested that P518 was not affected by the redox state of the primary electron acceptor of System 1. The absorbance increase at 518 nm due to System 2 decayed in the dark with a half-time of several min. The kinetics were similar to those of C-550, the presumed indicator of the primary electron acceptor of System 2. After two flashes preillumination the changes due to P518 and C-550 were reduced by about 40%, and a relatively slow, System 2-induced oxidation of cytochrome b₅₅₉ occurred which proceeded at a similar rate as the increase in yield of chlorophyll a fluorescence. The results indicate that at ?50°C two different photoreactions of System 2 occur. One consists of a photoreduction of the primary electron acceptor associated with C-550, accompanied by the oxidation of an unknown electron donor; the other is less efficient and results in the photooxidation of cytochrome b₅₅₉.     

The mechanism of reduction of the ubiquinone pool in photosynthetic bacteria at different redox potentials.

(1) A flash number dependency of flash-induced absorbance changes was observed with whole cells of Rhodospirillum rubrum and chromatophores of R. rubrum and Rhodopseudomonas sphaeroides wild type and the G1C mutant. The oscillatory behavior was dependent on the redox potential; it was observed under oxidizing conditions only. Absorbance difference spectra measured after each flash in the 275--500 nm wavelength region showed that a molecule of ubiquinone, R, is reduced to the semiquinone (R-) after odd-numbered flashes and reoxidized after even-numbered flashes. The amount of R reduced was approximately one molecule per reaction center. (2) The flash number dependency of the electrochromic shift of the carotenoid spectrum was studied with chromatophores of Rps. sphaeroides wild type and the G1C mutant. At higher values of the ambient redox potential a relatively slow phase with a rise time of 30 ms was observed after even-numbered flashes, in addition to the fast phase (completed within 0.2 ms) occurring after each flash. Evidence was obtained that the slow phase represents the formation of an additional membrane potential during a dark reaction that occurs after flashes with an even number. This reaction is inhibited by antimycin A, whereas the oscillations of the R/R- absorbance changes remain unaffected. At low potentials (E = 100 mV) no oscillations of the carotenoid shift were observed: a fast phase was followed by a slow phase (antimycin-sensitive) with a half-time of 3 ms after each flash. (3) The results are discussed in terms of a model for the cyclic electron flow as described by Prince and Dutton (Prince, R.C. and Dutton, P.L. (1976) Bacterial Photosynthesis Conference, Brussels, Belgium, September 6--9, Abstr. TB4) employing the so-called Q-cycle.     

Effects of light flashes on the dark closure of Albizzia julibrissin pinnules

An electronic flash unit is used to deliver, at the beginning of a 10 min dark period and within a few ms, large doses of light to Albizzia julibrissin pinnules, to ascertain their effects on the rate of pinnule closing. In a series of alternating light flashes at 710 and 550 nm, the first 710 nm light flash significantly retards closing. A following light flash at 550 nm negates the far-red induced delay. The second 710 nm light flash delays closing less effectively than the first when given within 4 s after the green flash, but is just as effective when given after 30 s. The delay brought about by the second 710 nm light flash is again abolished by a light flash at 550 nm. A light flash at 660 nm has no effect on pinnule closing by itself and is also ineffective in reversing the far-red induced delay. A series of ten 710 nm light flashes becomes most effective in delaying closure when there is a dark interval of one min between flashes. The closing delay induced by a 710 nm light flash escapes reversal by a 550 nm light flash when the dark interval between the two flashes exceeds 2–3 min. A 750 nm light flash has no retarding effect on pinnule closing, but it becomes effective when preceded by a 660 nm or 550 nm light flash. The results obtained are suggested to be due to light absorbed by phytochrome and an unknown photoreceptor with green, far-red photoreversal property.     

Phototransformation of the Far-red Light-absorbing Form of Large Pea Phytochrome by Laser Flash Excitation

Phototransformation of the far-red light absorbing form (P_FR)of large pea phytochrome to the red-light absorbing form (P_R)was examined at 2?C after a 715 nm laser flash excitation usinga custom-built multichannel transient spectra analyzer. Themaximum amount of phototransformation intermediates was producedby a pulse of about 50 mJ, which resulted in ca. 65% of P_R obtainedat the photostationary equilibrium. Some flash-induced intermediateswere assumed to return to P_FR in the dark. A difference spectrummeasured at 10 µsec after the flash showed an absorbanceincrease at 651 nm and a decrease at 724 nm. When the samplewas left in darkness after the flash light irradiation, absorbancein the red and far-red region gradually increased, but thatin the green region rapidly decreased. The decay curve of intermediatesmeasured at 554 nm could be resolved into three reaction componentshaving rate constants of 2,500, 590 and 48 sec^–1, respectively.Difference spectra also indicated that a small but significantincrease in absorbance between 370 and 380 nm and a decreasearound 415 nm took place 10–310 µsec after a flash. (Received February 13, 1982; Accepted April 21, 1982)     

Slow fluorescence fluctuations following high light to low light or dark transitions in Chlamydomonas reinhardi.

Slow fluorescence transients in Chlamydomonas reinhardi arise after transitions from high light intensities to low light or dark conditions. Characteristics of the newly described transient phenomena include: (a) A slow biphasic decrease in fluorescence yield occurs in the dark, followed by an even slower, hour long, increase in fluorescence. (b) A similar, but faster, fluorescence yield decrease and subsequent increase also occurs during low intensity illumination periods separating high light intervals, or after transitions from high intensity to low intensity light. (c) Short (several seconds) flashes of light given during a dark period have no effect on the dark fluorescence decay, regardless of the flash frequency. Such flash regimes accurately monitor the dark decline of the M2 level by tracing the parallel decay of flash-generated P2 (Kautsky) peaks. However, flashes during a low light illumination period do influence the decay kinetics. Frequent flashes allow decay similar to that occurring in dark, but less frequent flashes inhibit the decrease in fluorescence yield.     

Flash spectroscopic characterization of photosynthetic electron transport in isolated heterocysts

Electron transport was studied in heterocysts of the filamentous cyanobacterium Anabaena 7120 using spectral and kinetic analysis of absorbance transients elicited by single turnover flashes. Consistent photosynthetic turnovers were observed only in the presence of an exogenous source of reductant; therefore measurements were routinely made under a gas phase containing H2. Prominent absorbance changes corresponding to the oxidation of cytochrome c (554 nm) and the reduction of cytochrome b563 (563 nm) were observed. Under the most reducing conditions (99% H2/1% O2) cytochrome b563 was partially reduced between flashes in a slow, dark reaction. At 10-15% O2, the slow, dark reduction of cytochrome b563 was eliminated. Cytochrome turnover ceased entirely at high O2 concentrations (30%) but was restored by the addition of 25 microM KCN, demonstrating an interaction between the photosynthetic and respiratory electron transfer chains. Strobilurin A slowed the re-reduction of cytochrome c and eliminated the appearance of reduced cytochrome b563 by blocking electron transfer between reduced plastoquinone and the cytochrome b/f complex. Inhibition at a second site was apparent with 2-(n-heptyl)-4-hydroxyquinoline N-oxide, which blocked the reoxidation of cytochrome b563 but had little effect on cytochrome c relaxation. In uncoupled heterocysts, the rates of cytochrome c re-reduction and cytochrome b563 reduction were equal. Additional unassigned absorbance changes at 475 nm, 515 nm, and 572 nm were partially characterized. No absorbance change corresponding to an electrochromic shift was observed.     

Low Temperature Spectrophotometry on Phototransformation of PR in Pelletable Phytochrome of Pea

Phototransformation of P_R to P_FR in a 1,000–7,000 x gpelletable fraction (1–7 KP), which was extracted fromdark-grown pea shoots that had been irradiated by red then far-redlight, was studied by low temperature spectrophotometry. Redlight irradiation of P_R in 1–7 KP at –160°Cinduced an absorption increase at 695–696 nm with a concomitant,small decrease of P_R absorption at 670 nm. These changes werepartially photoreversed when the sample was irradiated subsequentlywith 700-nm light. At –55°C, red light irradiationof P_R resulted mainly in bleaching and consequently in a reductionof the P_R peak, accompanied by minor absorbance increases around695 nm. The intermediates formed at –165°C by 660-nmlight irradiation partly reverted back to P_R or formed a bleachedintermediate (probably the same bleached intermediate describedabove) in the dark, when the pellets were warmed to –60°C.The bleached intermediate was transformed to P_FR in the darkat –10°C or above. These characteristics of P_R transformation observed in the pelletablephytochrome were essentially the same as those observed in invivo or soluble phytochrome. (Received December 24, 1982; Accepted July 28, 1983)     

Light-induced absorbance changes in chloroplasts mediated by Photosystem I and Photosystem II at low temperature

Stable light-induced absorbance changes in chloroplasts at −196 °C were measured across the visible spectrum from 370 to 730 nm in an effort to find previously undiscovered absorbance changes that could be related to the primary photochemical activity of Photosystem I or Photosystem II. A Photosystem I mediated absorbance increase of a band at 690 nm and a Photosystem II mediated absorbance increase of a band at 683 nm were found. The 690-nm change accompanied the oxidation of P₇₀₀ and the 683-nm increase accompanied the reduction of C-550. No Soret band was detected for P₇₀₀.

A specific effort was made to measure the difference spectrum for the photooxidation of P₆₈₀ under conditions (chloroplasts frozen to −196 °C in the presence of ferricyanide) where a stable, Photosystem II mediated EPR signal, attributed to P₆₈₀⁺ has been reported. The difference spectra, however, did not show that P₆₈₀⁺ was stable at −196 °C under any conditions tested. Absorbance measurements induced by saturating flashes at −196 °C (in the presence or absence of ferricyanide) indicated that all of the P₆₈₀⁺ formed by the flash was reduced in the dark either by a secondary electron donor or by a backreaction with the primary electron acceptor. We conclude that P₆₈₀⁺ is not stable in the dark at −196 °C: if the normal secondary donor at −196 °C is oxidized by ferricyanide prior to freezing, P₆₈₀⁺ will oxidize other substances.     

Light and dark adaptation of halorhodopsin

Dark incubation of envelope vesicles derived from a strain of Halobacterium halobium that lacks bacteriorhodopsin but contains halorhodopsin and a third rhodopsin-like pigment caused a decrease in the flash yield [the amplitude of a transient absorbance change of flash reactive component(s) by flash] of halorhodopsin but not the rhodopsin-like pigment. The flash yield decreased to reach a low steady level after incubation for about 4 days in the dark. The flash yield of halorhodopsin at any stage of dark incubation was increased by actinic illumination of the vesicles. The flash yield at 490 nm (absorbance increase) was found to be approximately proportional to that at 590 nm (absorbance decrease). These results indicate that halorhodopsin in the envelope vesicles has two forms, dark and light adapted, and that the halorhodopsin phototransient absorbing at 490 nm is originated from the light-adapted form. A difference spectrum between these two forms of halorhodopsin shows that the light-adapted halorhodopsin was red-shifted from the dark-adapted form. The light-induced membrane potential was measured by tetraphenylphosphonium uptake. The uptake by the dark-adapted vesicles was slower than that by the light-adapted vesicles, suggesting that only the light-adapted halorhodopsin has ion-transporting activity.     

Delayed fluorescence induction in chloroplasts. Irradiance dependence

We have studied the delayed fluorescence in spinach chloroplasts produced 0.5 ms after each of a pair of (sub)-microsecond flashes. We observe an increase in the delayed fluorescence from the second flash relative to that produced by the first. This increase is proportional to the product of the first and second flash irradiances, appearing as an I² dependence if both flashes are increased together. The enhancement is observable at very weak flash levels (roughly 1 photon absorbed/100 PS II centers). If the irradiance of the first flash is increased, but the irradiance of the second held constant, the delayed fluorescence from the second flash is observed to increase, but then to saturate well below the first flash irradiance at which the delayed fluorescence from the first flash itself saturates. For most experiments, the dark time between flashes was 30 ms. If the dark time is varied, the enhancement changes, reaching a half-maximal value for a dark time of approx. 300 μs. The enhancement is stopped by hydroxylamine, but not by gramicidin, valinomycin, DCMU, or mild heating. These experiments are consistent with the notion that there are two different types of Photosystem II centers if we assume that only one type is responsible for the induction we see and has an optical cross-section about 4-times the size of the other type of center.     

Inhibition of the reoxidation of the secondary electron acceptor of Photosystem II by bicarbonate depletion

In bicarbonate-depleted chloroplasts, the chlorophyll a fluorescence decayed with a halftime of about 150 ms after the third flash, and appreciably faster after the first and second flash of a series of flashes given after a dark period. After the fourth to twentieth flashes, the decay was also slow. After addition of bicarbonate, the decay was fast after all the flashes of the sequence. This indicates that the bicarbonate depletion inhibits the reoxidation of the secondary acceptor R²⁻ by the plastoquinone pool; R is the secondary electron acceptor of pigment system II, as it accepts electrons from the reduced form of the primary electron acceptor (Q⁻). This conclusion is consistent with the measurements of the DCMU (3-(3,4-dichlorophenyl)-1,1-dimethylurea)-induced chlorophyll a fluorescence after a series of flashes in the presence and the absence of bicarbonate, if it is assumed that DCMU not only causes reduction of Q if added in the state QR⁻, but also if added in the state QR²⁻.     

On the O2 flash yields of two cyanophytes

We explored O₂ flash yield in two cyanophytes, Anacystis nidulans and Agmenellum quadruplicatum. On a rate-measuring electrode, a single flash gave a contour of O₂ evolution with a peak at about 10 ms which was maximum (100) for 680 nm background light. On 625 nm illumination the peak was smaller (62) but was followed by an increased tail of O₂ attributed to enhancement of the background. After a period of darkness, repetitive flashes (5 Hz) gave a highly damped initial oscillation in individual flash yields which finally reached steady state at 94% of the yield for 680 nm illumination. When O₂ of repetitive flashes was measured as an integrated flash yield the results was distinctive and similar to that for a continuous light 1 (680 nm). An apparent inhibition of respiration which persisted into the following dark period was taken as evidence for the Kok effect. With a concentration-measuring electrode, integrated flash yield vs. flash rate showed the same nonlinear behavior as O₂ rate vs. intensity of light 1. We draw three conclusions about the two cyanophytes. (a) The plastoquinone pool is substantially reduced in darkness. (b) Because of a high ratio of reaction centers, reaction center 1 / reaction center 2, for the two photoreactions, saturating flashes behave as light 1. (c) Because repetitive flashes are light 1, they also give a Kok effect which must be guarded against in measurements designed to count reaction centers.     

Effects of priming flash parameters and dark interval on red-induced afterpotential in Balanus photoreceptors

The sequence (a) priming flash, (b) dark interval, and (c) red light induces a long-lasting afterdepolarization (PDA) in Balanus photoreceptors. The inward flow of membrane current associated with the decay of PDA was independent of red test flashes, provided that PDA had plateaued at a particular intensity. The influence of wavelength and duration of the priming flash and their interaction with the dark interval were investigated. Increasing the duration of the priming flash produced a systematic increase in PDA duration. The dark interval plays a crucial role in PDA induction. The priming flash duration and the dark interval were reciprocally related, i.e, short flashes followed by long dark intervals induced as much PDA as long priming flashes followed by short dark intervals. The action spectrum for the priming flash was found to correspond to that of the primary photopigment (VP537).     

A seconds range component of the reoxidation of the primary Photosystem II acceptor,Q. Effects of bicarbonate depletion in chloroplasts

Broken chloroplasts depleted of bicarbonate (HCO^?₃) show 30–50% inhibition of the Hill reaction in low-intensity light. Also, photoreactions excited by repetitive flashes measured by oxygen evolution, ESR signal IIvf, and absorption changes at 680 and 334 nm show inhibition of 30–50%. An effect of HCO^?₃ was sought to explain these phenomena. The decay of chlorophyll a fluorescence yield in the millisecond and seconds range, following a single flash, was observed to be multiphasic with a very slow component of 1–2 s half-time. In HCO^?₃ -depleted samples this component is enhanced 2- or 3-fold. Since this occurs even after one flash, it is suggested that HCO^?₃ affects the Q^? B → QB^? reaction. In this work it is shown that 40% inhibition of oxygen flash yield is relieved to a great extent if the excitation flash rate is decreased from 2 to 0.33 Hz. A measurement of 520 nm absorption change in the presence of ferricyanide, which is proportional to Photosystem II charge separation, shows a similar inhibition that is dependent on flash rate. The maximum amplitude of variable fluorescence yield and 520 nm absorption change after a single flash are unaffected by HCO^?₃ depletion. The dark distribution of oxygen-evolution S-states is found to be shifted to a more reduced configuration in depleted samples. It is concluded that normal charge separation occurs in HCO^?₃ -depleted Photosystem II reaction centers but that a large fraction of Q^? decays so slowly that not all Q^? is reoxidized between flashes given at a rate of 1 or 2 Hz. Thus, a portion of the Photosystem II centers would be closed to photochemistry. There is a reversible effect of HCO^?₃ depletion on the oxygen-evolution system that is observed as a shift in the dark distribution of S-states.     

Kinetic model of the operation of a 2-electron switch in the photosynthetic reaction center of bacteria

A mathematical model, describing the binary oscillation of the concentration of semiquinone form of the secondary acceptor (ubiquinone) in photosynthetic reaction center of purple bacteria is proposed. This model takes into account both the changes of the ubiquinone state when the chromatophores are subjected to short flashes of light, and the successive dark relaxation of the semiquinone form. The model allows to calculate such characteristics as the dependence of the flash number, the stationary level of semiquinone form which is being established, when the flash number increases, the velocity which the concentration of semiquinone form is aspirating towards this stationary level and other characteristics. The model shows that the quantum yield of primary charge separation on the reaction center is higher after odd-number flashes then after even-number flashes.     

Redox transients of P680 associated with the incremental chlorophyll‐a fluorescence yield rises elicited by a series of saturating flashes in diuron‐treated photosystem II core complex of Thermosynechococcus vulcanus

Recent chlorophyll‐a fluorescence yield measurements, using single‐turnover saturating flashes (STSFs), have revealed the involvement of a rate‐limiting step in the reactions following the charge separation induced by the first flash. As also shown here, in diuron‐inhibited PSII core complexes isolated from Thermosynechococcus vulcanus the fluorescence maximum could only be reached by a train of STSFs. In order to elucidate the origin of the fluorescence yield increments in STSF series, we performed transient absorption measurements at 819 nm, reflecting the photooxidation and re‐reduction kinetics of the primary electron donor P680. Upon single flash excitation of the dark‐adapted sample, the decay kinetics could be described with lifetimes of 17 ns (～50%) and 167 ns (～30%), and a longer‐lived component (～20%). This kinetics are attributed to re‐reduction of P680^?+ by the donor side of PSII. In contrast, upon second‐flash (with Δt between 5 μs and 100 ms) or repetitive excitation, the 819 nm absorption changes decayed with lifetimes of about 2 ns (～60%) and 10 ns (～30%), attributed to recombination of the primary radical pair P680^?+Pheo^?–, and a small longer‐lived component (～10%). These data confirm that only the first STSF is capable of generating stable charge separation – leading to the reduction of Q_A; and thus, the fluorescence yield increments elicited by the consecutive flashes must have a different physical origin. Our double‐flash experiments indicate that the rate‐limiting steps, detected by chlorophyll‐a fluorescence, are not correlated with the turnover of P680.     

Oxygen Evolution from Algae Illuminated by Short and Long Flashes of Light

The oxygen produced by illuminating Ankistrodesmus braunii withsingle light flashes has been determined using the Hersch galvanicoxygen cell. Measurements were made with the cells suspendedin alkaline solution equilibrated with nitrogen containing oxygenat a partial pressure of 10^–4 mm. Hg.

1. A single light flash, if very brief (less than 5 millisec.)results in no measurable oxygen production; a longer flash (35millisec.) gave a yield of approximately 1 mole O₂/800 moleschlorophyll.
2. A pair of flashes suitably spaced gave a greateryield thanthe sum of the yields when given individually, althoughonewas so brief that by itself it produced no measurable oxygen.The yield of a long flash preceded by a short flash was twiceas great as that of the long flash given alone; when the flashorder was reversed the combined yield was smaller but stillgreater than for the long flash alone.
3. The combined yieldof a pair of flashes varies with the intervalseparating theflashes, rapidly rising to a maximum and thendecaying moreslowly. With a long and short flash the optimalinterval was0.7 sec. but some enhancement of yield was observedwhen theflashes were separated by as long as 10 or 15 sec.
4. When theflashes were superimposed on background illuminationthe yieldswere increased and were measurable even for the shortflashes.Measured with background illumination the optimal yieldfora pair of short flashes was obtained with flashes separatedby about 0.05 sec.