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.

The effect of temperature on the primary reaction of chloroplast Photosystem II Evidence for a temperature-dependent back reaction

The primary reaction of Photosystem II has been studied over the temperature range from −196 to −20 °C. The photooxidation of the reaction-center chlorophyll (P680) was followed by the free-radical electron paramagnetic resonance signal of P680⁺, and the photoreduction of the Photosystem II primary electron acceptor was monitored by the C-550 absorbance change.

At temperatures below −100 °C, the primary reaction of Photosystem II is irreversible. However, at temperatures between −100 and −20 °C a back reaction that is insensitive to 3-(3′,4′-dichlorophenyl)-1,1′-dimethylurea (DCMU) occurs between P680⁺ and the reduced acceptor.

The amount of reduced acceptor and P680⁺ present under steady-state illumination at temperatures between −100 and −20 °C is small unless high light intensity is used to overcome the competing back reaction. The amount of reduced acceptor present at low light intensity can be increased by adjusting the oxidation-reduction potential so that P680⁺ is reduced by a secondary electron donor (cytochrome b₅₅₉) before P680⁺ can reoxidize the reduced primary acceptor. The photooxidation of cytochrome b₅₅₉ and the accompanying photoreduction of C-550 are inhibited by DCMU. The inhibition of C-550 photoreduction by DCMU, the dependence of P680 photooxidation and C-550 photoreduction on light intensity, and the effect of the availability of reduced cytochrome b₅₅₉ on C-550 photoreduction are unique to the temperature range where the Photosystem II primary reaction is reversible and are not observed at lower temperatures.     

Effect of low temperature (−30 to −60°C) on the reoxidation of the Photosystem II primary electron acceptor in the presence and absence of 3(3,4-dichlorophenyl)-1,1-dimethylurea

The fluorescence yield has been measured on spinach chloroplasts at low temperature (−30 to −60°C) for various dark times following a short saturating flash. A decrease in the fluorescence yield linked to the reoxidation of the Photosystem II electron acceptor Q is still observed at −60°C. Two reactions participate in this reoxidation: a back reaction or charge recombination and the transfer of an electron from Q⁻ to Pool A. The relative competition between these two reactions at low temperature depends upon the oxidation state of the donor side of the Photosystem II center:

1. (1) In dark-adapted chloroplasts (i.e. in States S₀+S₁ according to Kok, B., Forbush, B. and McGloin, M. (1970) Photochem. Photobiol. 11, 457–475), Q, reduced by a flash at low temperature, is reoxidized by a secondary acceptor and the positive charge is stabilized on the Photosystem II donor Z. Although this reaction is strongly temperature dependent, it still occurs very slowly at −60°C.

2. (2) When chloroplasts are placed in the S₂+S₃ states by a two-flash preillumination at room temperature, the reoxidation of Q⁻ after a flash at low temperature is mainly due to a temperature-independent back reaction which occurs with non-exponential kinetics.

3. (3) Long continuous illumination of a frozen sample at −30°C causes 6–7 reducing equivalents to be transferred to the pool. Thus, a sufficient number of oxidizing equivalents should have been generated to produce at least one O₂ molecule.

4. (4) A study of the back reaction in the presence of 3(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) shows the superposition of two distinct non-exponential reactions one temperature dependent, the other temperature independent.

Quantum yield and rate of formation of the carotenoid triplet state in photosynthetic structures

The formation of the triplet state of carotenoids (detected by an absorption peak at 515 nm) and the photo-oxidation of the primary donor of Photosystem II, P-680 (detected by an absorption increase at 820 nm) have been measured by flash absorption spectroscopy in chloroplasts in which the oxygen evolution was inhibited by treatment with Tris. The amount of each transient form has been followed versus excitation flash intensity (at 590 or 694 nm). At low excitation energy the quantum yield of triplet formation (with the Photosystem II reaction center in the state Q⁻) is about 30% that of P-680 photo-oxidation. The yield of carotenoid triplet formation is higher in the state Q⁻ than in the state Q, in nearly the same proportion as chlorophyll a fluorescence. It is concluded that, for excited chlorophyll a, the relative rates of intersystem crossing to the triplet state and of fluorescence emission are the same in vivo as in organic solvent. At high flash intensity the signal of P-680⁺ completely saturates, whereas that of carotenoid triplet continues to increase.

The rate of triplet-triplet energy transfer from chlorophyll a to carotenoids has been derived from the rise time of the absorption change at 515 nm, in chloroplasts and in several light-harvesting pigment-protein complexes. In all cases the rate is very high, around 8 · 10⁷ s⁻¹ at 294 K. It is about 2–3 times slower at 5 K. The transitory formation of chlorophyll triplet has been verified in two pigment-protein complexes, at 5 K.     

Absorbance difference spectra upon charge transfer to secondary donors and acceptors in Photosystem II

Charge-transfer reactions to secondary electron donors (Z, M) and acceptors (Q_A, Q_B) in Photosystem II particles isolated from a thermophilic cyanobacterium Synechococcus sp. (Schatz, G.H. and Witt H.T. (1984) Photobiochem. Photobiophys. 7, 1–14) were analyzed by measurements of fluorescence yield and absorbance changes in the millisecond time domain induced by repetitive flashes. (1) The electron-transfer reaction Q⁻_AQ_B → Q_AQ⁻_B was found to occur with kinetic phases of 0.2 ± 0.1 ms and 1.5 ± 0.5 ms half-time. At 10 ms after flashes an equilibrium distribution of Q⁻_AQ_B/Q_AQ⁻_B of about 15/85 in oxygen-evolving and of about 25/75 in Tris-treated PS II particles was reached. (2) The absorbance difference spectra were determined for (Q⁻_A - Q_A), (Q⁻_B - Q_B), (Z⁺ - Z) and for (S₄ - S₀), the transition associated with oxygen evolution. In the ultraviolet region they show that these electron-acceptors and -donors are the same as in spinach PS II. In the visible region all the difference spectra contain major contributions by electrochromic bandshifts due to electrostatic interaction of the reduced acceptors or oxidized donors with nearby reaction center pigments. Upon electron transfer from Q⁻_A to Q_B electrochromic bandshifts due to interaction with pheophytin a disappeared almost completely. Bandshifts observed in the (Z⁺ - Z) and (S₄ - S₀) spectra were attributed to chlorophyll a.     

Charge accumulation at the reducing side of system 2 of photosynthesis

A study was made of the reactions between the primary and secondary electron acceptors of Photosystem 2 by measurements of the increase of chlorophyll fluorescence induced in darkness by dithionite or by 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU). The experiments were done either with chloroplasts to which hydroxylamine or carbonylcyanide-p-trifluoromethoxyphenylhydrazone (FCCP) was added, or with chloroplasts treated with tris(hydroxymethyl)aminomethane (Tris) to which phenylenediamine and ascorbate were added as donor system. Under these conditions the fluorescence increase induced by dithionite or DCMU added after illumination with short light flashes was dependent on the flash number with a periodicity of two; it was large after an uneven number of flashes, and small after a long darktime or after an even number of flashes. The results are interpreted in terms of a model which involves a hypothetical electron carrier situated between Q and plastoquinone; this electron carrier is thought to equilibrate with plastoquinone in a two-electron transfer reaction; the results obtained with DCMU are explained by assuming that its midpoint potential is lowered by this inhibitor.     

Chlorophyll a fluorescence as a monitor of nanosecond reduction of the photooxidized primary donor P-680 of Photosystem II

1. Changes in the fluorescence yield of aerobic Chlorella vulgaris have been measured in laser flashes of 15 ns, 30 ns and 350 ns half time. The kinetics after the first flash given after a 3 min dark period could be simulated on a computer using the hypothesis that the oxidized acceptor Q and primary donor P⁺ are fluorescence quenchers, and Q⁻ is a weak quencher, and that the reduction time for P⁺ is 20–35 ns.

2. The P⁺ reduction time for at least an appreciable part of the reaction centers was found to be longer after the second and subsequent flashes. In the first 5 flashes an oscillation was observed. Under steady state conditions, with a pulse separation of 3 s, a reduction time for P⁺ of about 400 ns for all reaction centers gave the best correspondence between computed and experimental fluorescence kinetics.     

pH control of the chlorophyll a fluorescence in algae

The pH of the suspension medium was found to have a remarkable influence on the “slow” (min) time course of Chlorophyll a fluorescence yield in the green alga Chlorella pyrenoidosa and in the blue-green alga Anacystis nidulans. In Chlorella, the decay of fluorescence yield, in the 1- to 5-min region, is strongly retarded at alkaline pH; this decay rate shows an optimum at pH 6–7. In Anacystis, the rise of fluorescence yield, in the same time range, is decreased optimally at pH 6–7; poisoning with 3(3,4-dichlorophenyl)-1,1-dimethylurea reverses the direction of this pH effect. These observations suggest a correlation of the H⁺ status (or the processes associated with it such as photophosphorylation and resulting conformational changes) of the chloroplast to the yield of chlorophyll a fluorescence in vivo.     

Chlorophyll a fluorescence and photochemical activities of chloroplast fragments

1. Comparative studies were made on the fluorescence characteristics of chlorophyll a at 20° and −193°, and quantum efficiencies for P 700 oxidation and NADP⁺ reduction were measured in chloroplasts and chloroplast fragments obtained after incubation with 0.5% digitonin.

2. Differences in the flurescence yield of chlorophyll a in flowing and stationary suspensions of untreated chloroplasts and of the large fragments are indicative of light-induced photoreduction of the quencher Q of chlorophyll a, associated with pigment System 2 (chlorophyll a₂). The relatively low constant fluorescence yield of chlorophyll a in the small fragments indicates the absence of fluorescent chlorophyll a₂ from these fragments and suggests that the low fluorescence is due to chlorophyll a, associated with pigmen System 1 (chlorophyll a₁). The ratio of the fluorescence yields of chlorophyll a₁ and chlorophyll a₂ is 0.45:1. In the large particles the concentration ratio of pigment System 1 and System 2 is 1:3.

3. The efficiencies of quanta absorbed at 673, 683 and 705 nm for NADP⁺ reduction and P 700 oxidation in untreated chloroplasts and chloroplast fragments indicate that digitonin treatment results in a separation of System 2 from System 1 in the small fragments. Sonication does not cause such a separation. Under the conditions used P 700 oxidation and NADP⁺ reduction in the small fragments separated after digitonin treatment, occurred with maximal efficiency of 0.7 to 1.0 and 0.7, respectively.

4. The constancy of the fluorescence yield of chlorophyll a₁ in the small fragments, under conditions at which P 700 is oxidized and NADP⁺ is reduced, is interpreted as evidence either for the hypothesis that the fluorescence of chlorophyll a₁ is controlled by the redox state of the primary photoreductant XH, or alternatively for the hypothesis that energy transfer from fluorescent chlorophyll a₁ to P 700 goes via an intrinsically weak fluorescent, still unknown, chlorophyll-like pigment.

5. The low-temperature emission band around 730 nm is argued not to be due to excitation by System 1 only; the relatively large half width of the band, as compared to the emission bands at 683 and 696 nm, suggests that it is possibly due to overlapping emission bands of different pigments.     

Effects of monovalent cations on light energy distribution between two pigment systems of photosynthesis in isolated spinach chloroplasts

The effects of monovalent cations on the light energy distribution between two pigment systems of photosynthesis were studied in isolated spinach chloroplasts by measuring chlorophyll a fluorescence and photochemical reactions.

The addition of NaCl to the chloroplast suspension produced a 40–80% increase in fluorescence yield measured at 684 nm at room temperature. The fluorescence increase was completed about 5 min after the addition. The effect saturated at 100 mM NaCl. Low-temperature fluorescence spectra showed that NaCl increased the yields of two fluorescence bands of pigment system II at 684 and 695 nm but decreased that of pigment system I at 735 nm. Similar effects on chlorophyll a fluorescence at room and at low temperatures were obtained with NaBr, NaNO₃, Na₂SO₄, LiCl, KCl, RbCl, CsCl, NH₄Cl and CH₃NH₃Cl.

NaCl suppressed the quantum efficiency of NADP⁺ reduction supported by the ascorbate-2,6-dichlorophenolindophenol (DCIP) couple as an electron donor system in the presence of 3-(3′,4′-chlorophenyl)-1,1-dimethylurea (DCMU). On the other hand, NaCl only slightly enhanced the quantum yield of photoreaction II measured by the Hill reaction with DCIP.

It is concluded that the monovalent cations tested suppressed the excitation transfer from pigment system II to pigment system I; the effects were the same as those of alkaline earth metals and Mn²⁺ (refs. 1, 2).     

Flash-induced absorption changes in Photosystem I,Radical pair or triplet state formation?

Absorption changes induced in chlorophyll protein (CP 1) particles by short laser flashes have been analyzed in order to decide whether a state lasting for a few microseconds at 21°C or 800 μs at 10 K corresponds to the biradical P-700⁺ ... A⁻₁ (A₁ being a chlorophyll a) or to a triplet state produced in a submicrosecond recombination of the preceding state. At 21°C the spectrum of the flash-induced ΔA (720–870 nm) presents a flat-topped band from 740 to 820 nm, clearly different from that of P-700⁺. A saturation curve (ΔA vs. laser energy), obtained with a 2 or 10 ns laser pulse, indicates that ΔA saturates at a value 2- or 3-times smaller than that expected on the basis of the chemical oxidation of P-700. At 21°C the size of flash-induced ΔA is slightly decreased (5–15%) when the sample is subjected to a 400 G magnetic field. The kinetics of decay are not affected; they are not affected either by the oxygen concentration. At 10 K the spectrum of the flash-induced ΔA has been measured between 650 and 1700 nm. Between 650 and 720 nm, the spectrum presents only one major negative peak at 702 nm; it is quite different from that due to the chemical oxidation of P-700 (which has additional peaks at 688 and 677 nm). Between 720 and 870 nm, the spectrum is identical to that obtained at 21°C. Above 870 nm, the spectrum includes a broad band around 1250 nm, which is absent in P-700⁺. A saturation curve leads to a maximum ΔA greater than that at 21°C and which is also greater with a 1 μs dye laser flash than with a 10 ns ruby laser flash. An analysis of the spectral data indicates that these do not fit correctly with the hypothesis of a contribution of P-700⁺ and of a chlorophyll a anion radical. They fit more closely with the hypothesis of a triplet state of P-700, a hypothesis which is discussed in relation to other experimental data.     

The reduction kinetics of chlorophyll a1 as an indicator for proton uptake between the light reactions in chloroplasts

The flash-induced oxidation kinetics of the primary acceptor of light Reaction II (X-320) and the reduction kinetics of chlorophyll a₁ (P-700) after far-red preilluination have been studied with high time resolution in spinach chloroplasts.

1. 1. The kinetics of chlorophyll a₁ exhibits a pronounced lag phase of 2–3 ms at the onset of reduction as would be expected for the final product of consecutive reactions. Because the oxidation of the plastoquinone pool is the rate-limiting step for the electron transport between the two light reactions, the lag indicates the maximal electron transfer time over all preceding reactions after light Reaction II.

2. 2. The observation that the lag phase decreases with decreasing pH is evidence of an electron transfer step coupled to a proton uptake reaction.

3. 3. Protonation of X-320 after reduction in the flash is excluded because a slight increase of the decay time is found at decreasing pH values.

4. 4. The time course of plastohydroquinone formation is deduced from the first derivative of the reduction kinetics of chlorophyll a₁. This approach covers those plastohydroquinone molecules being available to the electron carriers of System I via the rate-limiting step. Direct measurements of absorbance changes would not allow to discriminate between these and functionally different plastohydroquinone molecules.

5. 5. The derived time course of plastohydroquinone at different pH gives evidence for an additional electron transfer step with a half time of about 1 ms following the proton uptake and preceding the rate-limiting step. It is tentatively attributed to the diffusion of neutral plastohydroquinone across the hydrophobic core of the thylakoid membrane.

6. 6. The lower limit of the rate constant for proton uptake by an electron carrier, consistent with the lag of chlorophyll a₁ reduction, is estimated as > 10¹¹ M⁻¹ · s⁻¹. The value is higher than that of the fastest diffusion controlled protonations of organic molecules in solution.

Possible mechanisms of linear electron transport between light Reaction II and the rate-limiting oxidation of neutral plastohydroquinone are thoroughly discussed.     

Fluorescence yield kinetics in the microsecond-range in Chlorella pyrenoidosa and spinach chloroplasts in the presence of hydroxylamine

The kinetics of fluorescence yield inChlorella pyrenoidosa and spinach chloroplasts were studied in the time range of 0.5 μs to several hundreds of microseconds in the presence of hydroxylamine. Fluorescence was excited with a just-saturating xenon flash with a halfwidth of 13 μs (λ = 420 nm). The fast rise of the fluorescence yield which was limited by the rate of light influx, was, in the presence of 10⁻³–10⁻² M hydroxylamine, replaced by a slow component which had a half risetime of 25 μs in essence independent of light intensity. This slow fluorescence yield increase reflects a dark reaction on the watersplitting side of Photosystem II. Simultaneous oxygen evolution measurements suggested that a fast fluorescence component is only present in organisms with intact O₂-evolving system, whereas a slow rise predominantly occurs in organisms with the watersplitting system irreversibly inhibited by hydroxylamine.

The results can be explained by the following hypotheses: (a) The primary donor of Photosystem II in its oxidized state, P⁺, is a fluorescence quencher. (b) Hydroxylamine prevents the secondary electron donor Z from reducing the oxidized reaction center pigment P⁺ rapidly. This inhibition is dependent on hydroxylamine concentration and is complete at a concentration of 10⁻² M. (c) A second donor (not transporting electrons from water) transfers electrons to P⁺ with a half time of roughly 25 μs.     

The back reaction in the primary electron transfer couple of photosystem II of photosynthesis

Changes of C-550, cytochrome b₅₅₉ and fluorescence yield induced in chloroplasts by single saturating flashes were studied at low temperature. A single saturating flash at −196°C was quite ineffective in reducing C-550, oxidizing cytochrome b₅₅₉ or increasing the fluorescence yield, presumably because most of the charge separation induced by the flash was dissipated by a direct back reaction in the primary electron transfer couple. The back reaction, which competes with the dark reduction of the oxidized primary electron donor by a secondary electron donor, becomes increasingly important as the temperature is lowered because of the temperature coefficient of the reaction with the secondary donor. The effect of the back reaction is to lower the quantum yield for the production of stable photochemical products by steady irradiation. Assuming a quantum yield of unity for the photoreduction of C-550 at room temperature, the quantum yield for the reaction is about 0.40 at −100°C and 0.27 at −196°C.     

Transfer and trapping of excitation energy in Photosystem II as studied by chlorophyll a2 fluorescence quenching by dinitrobenzene and carotenoid triplet. The matrix model

1. The curves representing the reciprocal fluorescence yield of chlorophyll a of Photosystem II (PS II) in Chlorella vulgaris as a function of the concentration of m-dinitrobenzene in the states P Q and P Q^-, are found to be straight parallel lines; P is the primary donor and Q the primary acceptor of PS II. In the weakly trapping state P Q^- the half-quenching of dinitrobenzene is about 0.2 mM, in vitro it is of the order of 10 mM. The fluorescence yield as a function of the concentration of a quencher is described for three models for the structure of pigment systems: the model of separate units, the model of limited energy transfer between the units, and the matrix model. If it is assumed that the rate constant of quenching by dinitrobenzene is high and thus the number of dinitrobenzene molecules per reaction center low, it can be concluded that the pigment system of PS II in C. vulgaris is a matrix of chlorophyll molecules in which the reaction centers are embedded. Theoretical and experimental evidence is consistent with such an assumption.

For Cyanidium caldarium the zero fluorescence yield Ф₀ and its quenching by dinitrobenzene were found to be much smaller than the corresponding quantities for C. vulgaris. Nevertheless, our measurements on C. caldarium could be interpreted by the assumption that the essential properties (rate constants, dinitrobenzene quenching) of PS II are the same for these two species belonging to such widely different groups.

2. The measured dinitrobenzene concentrations required for half-quenching in vivo and other observations are explained by (non-rate-limiting) energy transfer between the chlorophyll a molecules of PS II and by the assumptions that dinitrobenzene is approximately distributed at random in the membrane and does not diffuse during excitation.

3. The fluorescence kinetics of C. vulgaris during a 350 ns laser flash of variable intensity could be simulated on a computer using the matrix model. From the observed fluorescence quenching by the carotenoid triplet (C^T) and the measurement of the number of C^T per reaction center via difference absorption spectroscopy, the rate constant for quenching of C^T is calculated to be k_T = 3.3 · 10¹¹ s⁻¹ which is almost equal to the rate constant of trapping by an open reaction center (Duysens, L.N.M. (1979) CIBA Foundation Symposium 61 (New Series), pp. 323–340).

4. The fluorescence quenching by C^T in non-treated spinach chloroplasts after a 500 ns laser flash (Breton, J., Geacintov, N.E. and Swenberg, C.E. (1979) Biochim. Biophys. Acta 548, 616–635) could be explained within the framework of the matrix model when the value for k_T is used as given in point 3.

5. The observations mentioned under point 1 indicate that the fluorescence yield Ф₀ for centers in trapping state P Q is probably for a fraction exceeding 0.8 emitted by PS II.     

Photosynthetic response of Myriophyllum salsugineum A.E. orchard to photon irradiance, temperature and external free CO2

The photosynthetic capacity of Myriophyllum salsugineum A.E. Orchard was measured, using plants collected from Lake Wendouree, Ballarat, Victoria and grown subsequently in a glasshouse pond at Griffith, New South Wales. At pH 7.00, under conditions of constant total alkalinity of 1.0 meq dm⁻³ and saturating photon irradiance, the temperature optimum was found to be 30–35°C with rates of 140 μmol mg⁻¹ chlorophyll a h⁻¹ for oxygen production and 149 μmol mg⁻¹ chlorophyll a h⁻¹ for consumption of CO₂. These rates are generally higher than those measured by other workers for the noxious Eurasian water milfoil, Myriophyllum spicatum L., of which Myriophyllum salsugineum is a close relative. The light-compensation point and the photon irradiance required to saturate photosynthetic oxygen production were exponentially dependent on water temperature. Over the temperature range 15–35°C the light-compensation point increased from 2.4 to 16.9 μmol (PAR) m⁻² s⁻¹ for oxygen production while saturation photon irradiance increased from 41.5 to 138 μmol (PAR) m⁻² s⁻¹ for oxygen production and from 42.0 to 174 μmol (PAR) m⁻² s⁻¹ for CO₂ consumption. Respiration rates increased from 27.1 to 112.3 μmol (oxygen consumed) g⁻¹ dry weight h⁻¹ as temperature was increased from 15 to 35°C. The optimum temperature for productivity is 30°C.     

Quenching of fluorescence by triplet excited states in chloroplasts

The fluorescence quantum yield in spinach chloroplasts at room temperature has been studied utilizing a 0.5–4.0 μs duration dye laser flash of varying intensities as an excitation source. The yield (Ф) and carotenoid triplet concentration were monitored both during and following the laser flash. The triplet concentration was monitored by transient absorption spectroscopy at 515 nm, while the yield Ф following the laser was probed with a low intensity xenon flash. The fluorescence is quenched by factors of up to 10–12, depending on the intensity of the flash and the time interval following the onset of the flash. This quenching is attributed to a quencher Q whose concentration is denoted by Q. The relative instantaneous concentration of Q was calculated from Ф utilizing the Stern-Volmer equation, and its buildup and decay kinetics were compared to those of carotenoid triplets. At high flash intensities (10¹⁶ photon · cm⁻²) the decay kinetics of Q are slower than those of the carotenoid triplets, while at lower flash intensities they are similar. Q is sensitive to oxygen and it is proposed that Q, at the higher intensities, is a trapped chlorophyll triplet. This hypothesis accounts well for the continuing rise of the carotenoid triplet concentration for 1–2 μs after the cessation of the laser pulse by a slow detrapping mechanism, and the subsequent capture of the triplet energy by carotenoid molecules.

At the maximum laser intensities, the carotenoid triplet concentration is about one per 100 chlorophyll molecules. The maximum chlorophyll ion concentration generated by the laser pulses was estimated to be below 0.8 ions/100 chlorophyll molecules. None of the observations described here were altered when a picosecond pulse laser train was substituted for the microsecond pulse.

A simple kinetic model describing the generation of singlets and triplets (by intersystem crossing), and their subsequent interaction leading to fluorescence quenching, accounts well for the observations. The two coupled differential equations describing the time dependent evolution of singlet and triplet excited states are solved numerically. Using a singlet-triplet bimolecular rate constant of γ_st = 10⁻⁸ cm³ · s⁻¹, the following observations can be accounted for: (1) the rapid initial drop in Ф and its subsequent levelling off with increasing time during the laser pulse, (2) the buildup of the triplets during the pulse, and (3) the integrated yield of triplets per pulse as a function of the energy of the flash.     

Biochemical and biophysical studies on cytochrome c oxidase XIV. The reaction with cytochrome c as studied by pulse radiolysis

1. The reduction of cytochrome c oxidase by hydrated electrons was studied in the absence and presence of cytochrome c.

2. Hydrated electrons do not readily reduce the heme of cytochrome c oxidase. This observation supports our previous conclusion that heme a is not directly exposed to the solvent.

3. In a mixture of cytochrome c and cytochrome c oxidase, cytochrome c is first reduced by hydrated electrons (k = 4 · 10¹⁰ M⁻¹ · s⁻¹ at 22 °C and pH 7.2) after which it transfers electrons to cytochrome c oxidase with a rate constant of 6 · 10⁷ M⁻¹ · s⁻¹ at 22 °C and pH 7.2.

4. It was found that two equivalents of cytochrome c are oxidized initially per equivalent of heme a reduced, showing that one electron is accepted by a second electron acceptor, probably one of the copper atoms of cytochrome c oxidase.

5. After the initial reduction, redistribution of electrons takes place until an equilibrium is reached similar to that found in redox experiments of Tiesjema, R. H., Muijsers, A. O. and Van Gelder, B. F. (1973) Biochim. Biophys. Acta 305, 19–28.     

Rapid delayed luminescence from chloroplasts: Kinetic analysis of components; The relationship to the O2 evolving system

Delayed luminescence from saturating flashes given to isolated chloroplasts was measured in the time range of 65–800 μsec with the following results:

1. 1. Three distinct components having decay half times of approx. 10, 35 and 200 μsec could be detected.

2. 2. The yields of both the 35- and 200-μsec delayed luminescence components oscillate with a period of four, in phase with oscillations of O₂ yield; no large oscillations of fluorescence paralleling those of luminescence or O₂ were observed.

3. 3. 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) abolished the 10- and 200-μsec components and the oscillatory behavior of the 35-μsec component.

4. 4. The 35- and 200-μsec components are not directly influenced by System I.

The DCMU isolated 35-μsec component showed the following properties:

1. 1. The decay is first order and the emission spectrum is essentially identical to that of chloroplast fluorescence;

2. 2. The yield saturates with a total emission of about 10^-4 quanta/trap.

3. 3. The temperature dependence indicates an activation energy of about 250 mV for the yield and 200 mV for the decay.

4. 4. Maximal emission was obtained when Q, the acceptor of System II, was oxidized prior to the flash.

The results are discussed in terms of possible mechanisms concerning the production and behavior of the luminescence.     

Evidence for a double hit process in Photosystem II based on fluorescence studies

1. The amplitudes of the fast (0–20 μs) and slow (20 μs–2 ms) fluorescence rise induced by a 2 μs flash have been measured as a function of the energy of the flash in chloroplasts inhibited by 3(3,4-dichlorophenyl)-1,1-dimethylurea. The saturation curve for the slow rise shows a characteristic lag which is not observed for the fast fluorescence rise. This lag indicates that Photosystem II centers undergo a double hit process which implies that (a), each photocenter includes two acceptors Q₁ and Q₂; (b), after the first hit, oxidized chlorophyll Chl⁺ is reduced by a secondary acceptor Y in a time short compared to the duration of the flash; (c), after the second hit, Chl⁺ is reduced by another secondary donor, D.

2. According to Den Haan et al. ((1974) Biochim. Biophys. Acta 368, 409–421), hydroxylamine destroys the secondary donor responsible for the fast reduction of Chl⁺. In the presence of 3 mM hydroxylamine, only the secondary donor D is functional and a flash induces mainly a single hit process.

3. The saturation curves for the fast and the slow rises have been studied in the presence of 3(3,4-dichlorophenyl)-1,1-dimethylurea for a second actinic flash given 2.5 s after a first saturating one. The large decrease in the half-saturating energy indicates the existence of efficient energy transfer occuring between photosynthetic units.

4. Two alternate hypotheses are discussed (a) in which D is an auxiliary donor and (b) in which D is included in the main electron transfer chain.