Analysis of the spin-polarized electron spin echo of the [P700+ A1-] radical pair of photosystem I indicates that both reaction center subunits are competent in electron transfer in cyanobacteria, green algae, and higher plants

The decay of the light-induced spin-correlated radical pair [P700+ A1-] and the associated electron spin echo envelope modulation (ESEEM) have been studied in either thylakoid membranes, cellular membranes, or purified photosystem I prepared from the wild-type strains of Synechocystis sp. PCC 6803, Chlamydomonas reinhardtii, and Spinaceae oleracea. The decay of the spin-correlated radical pair is described in the wild-type membrane by two exponential components with lifetimes of 2-4 and 16-25 micros. The proportions of the two components can be altered by preillumination of the membranes in the presence of reductant at temperatures lower than 220 K, which leads to the complete reduction of the iron-sulfur electron acceptors F(A), F(B), and F(X) and partial photoaccumulation of the reduced quinone electron acceptor A1A-. The "out-of-phase" (OOP) ESEEM attributed to the [P700+ A1-] radical pair has been investigated in the three species as a function of the preillumination treatment. Values of the dipolar (D) and the exchange (J) interactions were extracted by time-domain fitting of the OOP-ESEEM. The results obtained in the wild-type systems are compared with two site-directed mutants of C. reinhardtii [Santabarbara et al. (2005) Biochemistry 44, 2119-2128], in which the spin-polarized signal on either the PsaA- or PsaB-bound electron transfer pathway is suppressed so that the radical pair formed on each electron transfer branch could be monitored selectively. This comparison indicates that when all of the iron-sulfur centers are oxidized, only the echo modulation associated with the A branch [P700+ A1A-] radical pair is observed. The reduction of the iron-sulfur clusters and the quinone A1 by preillumination treatment induces a shift in the ESEEM frequency. In all of the systems investigated this observation can be interpreted in terms of different proportions of the signal associated with the [P700+ A1A-] and [P700+ A1B-] radical pairs, suggesting that bidirectionality of electron transfer in photosystem I is a common feature of all species rather than being confined to green algae.     

Bidirectional electron transfer in photosystem I: determination of two distances between P700+ and A1- in spin-correlated radical pairs

The spin-correlated radical pair [P(700)(+)A(1)(-)] gives rise to a characteristic "out-of-phase" electron spin-echo signal. The electron spin-echo envelope modulation (ESEEM) of these signals has been studied in thylakoids prepared from the wild-type strain of Chlamydomonas reinhardtii and in two site-directed mutants, in which the methionine residue which acts as the axial ligand to the chlorin electron acceptor A(0) has been substituted with a histidine either on the PsaA (PsaA-M684H) or the PsaB (PsaB-M664H) reaction center subunits. The analysis of the time domain ESEEM provides information about the spin-spin interaction in the [P(700)(+)A(1)(-)] radical pair, and the values of the dipolar (D) and the exchange (J) interaction can be extracted. From the distance dependence of the dipolar coupling term, the distance between the unpaired electron spin density clouds of the primary donor P(700)(+) and the phyllosemiquinone A(1)(-) can be determined. The [P(700)(+)A(1)(-)] ESEEM spectrum obtained in wild-type thylakoids can be reconstructed using a linear combination of the spectra measured in the PsaA and PsaB A(0) mutants, demonstrating that electron transfer resulting in charge separation is occurring on both the PsaA and PsaB branches. The [P(700)(+)A(1B)(-)] distance in the point dipole approximation in the PsaA-M684H mutant is 24.27 +/- 0.02 A, and the [P(700)(+)A(1A)(-)] distance in the PsaB-M664H mutant is 25.43 +/- 0.01 A. An intermediate value of 25.01 +/- 0.02 A is obtained in the wild-type membranes which exhibit both spin-polarized pairs.     

Evidence for hydrogen bond formation to the PsaB chlorophyll of P700 in photosystem I mutants of Synechocystis sp. PCC 6803

P700, the primary electron donor of photosystem I, is an asymmetric dimer made of one molecule of chlorophyll a' (P(A)) and one of chlorophyll a (P(B)) that are bound to the homologous PsaA and PsaB polypeptides. While the carbonyl groups of P(A) are involved in hydrogen-bonding interactions with several surrounding amino acid side chains and a water molecule, P(B) does not engage hydrogen bonds with the protein. Notably, the residue Thr A739 is donating a strong hydrogen bond to the 9-keto C=O group of P(A) and the homologous residue Tyr B718 is free from interaction with P(B). Light-induced FTIR difference spectroscopy of the photooxidation of P700 has been combined with a site-directed mutagenesis attempt to introduce hydrogen bonds to the carbonyl groups of P(B) in Synechocystis sp. PCC 6803. The FTIR study of the Y(B718)T mutant provides evidence that the 9-keto C=O group of P(B) and P(B)(+) engages a relatively strong hydrogen-bonding interaction with the surroundings in a significant fraction (40 +/-10%) of the reaction centers. Additional mutations on the two PsaB residues homologous to those involved in the main interactions between the PsaA polypeptide and the 10a-carbomethoxy groups of P(A) affect only marginally the vibrational frequency of the 10a-ester C=O group of P(B). The FTIR data on single, double, and triple mutants at these PsaB sites indicate a plasticity of the interactions of the carbonyl groups of P(B) with the surrounding protein. However, these mutations do not perturb the hydrogen-bonding interactions assumed by the 9-keto and 10a-ester C=O groups of P(A) and P(A)(+) with the protein and have only a limited effect on the relative charge distribution between P(A)(+) and P(B)(+).     

Modelling of the electron transfer reactions in Photosystem I by electron tunnelling theory: the phylloquinones bound to the PsaA and the PsaB reaction centre subunits of PS I are almost isoenergetic to the iron-sulfur cluster F(X)

Photosystem I is a large macromolecular complex located in the thylakoid membranes of chloroplasts and in cyanobacteria that catalyses the light driven reduction of ferredoxin and oxidation of plastocyanin. Due to the very negative redox potential of the primary electron transfer cofactors accepting electrons, direct estimation by redox titration of the energetics of the system is hampered. However, the rates of electron transfer reactions are related to the thermodynamic properties of the system. Hence, several spectroscopic and biochemical techniques have been employed, in combination with the classical Marcus theory for electron transfer tunnelling, in order to access these parameters. Nevertheless, the values which have been presented are very variable. In particular, for the case of the tightly bound phylloquinone molecule A(1), the values of the redox potentials reported in the literature vary over a range of about 350 mV. Previous models of Photosystem I have assumed a unidirectional electron transfer model. In the present study, experimental evidence obtained by means of time resolved absorption, photovoltage, and electron paramagnetic resonance measurements are reviewed and analysed in terms of a bi-directional kinetic model for electron transfer reactions. This model takes into consideration the thermodynamic equilibrium between the iron-sulfur centre F(X) and the phylloquinone bound to either the PsaA (A(1A)) or the PsaB (A(1B)) subunit of the reaction centre and the equilibrium between the iron-sulfur centres F(A) and F(B). The experimentally determined decay lifetimes in the range of sub-picosecond to the microsecond time domains can be satisfactorily simulated, taking into consideration the edge-to-edge distances between redox cofactors and driving forces reported in the literature. The only exception to this general behaviour is the case of phylloquinone (A(1)) reoxidation. In order to describe the reported rates of the biphasic decay, of about 20 and 200 ns, associated with this electron transfer step, the redox potentials of the quinones are estimated to be almost isoenergetic with that of the iron sulfur centre F(X). A driving force in the range of 5 to 15 meV is estimated for these reactions, being slightly exergonic in the case of the A(1B) quinone and slightly endergonic, in the case of the A(1A) quinone. The simulation presented in this analysis not only describes the kinetic data obtained for the wild type samples at room temperature and is consistent with estimates of activation energy by the analysis of temperature dependence, but can also explain the effect of the mutations around the PsaB quinone binding pocket. A model of the overall energetics of the system is derived, which suggests that the only substantially irreversible electron transfer reactions are the reoxidation of A(0) on both electron transfer branches and the reduction of F(A) by F(X).     

Modelling of the electron transfer reactions in Photosystem I by electron tunnelling theory: The phylloquinones bound to the PsaA and the PsaB reaction centre subunits of PS I are almost isoenergetic to the iron-sulfur cluster FX

Photosystem I is a large macromolecular complex located in the thylakoid membranes of chloroplasts and in cyanobacteria that catalyses the light driven reduction of ferredoxin and oxidation of plastocyanin. Due to the very negative redox potential of the primary electron transfer cofactors accepting electrons, direct estimation by redox titration of the energetics of the system is hampered. However, the rates of electron transfer reactions are related to the thermodynamic properties of the system. Hence, several spectroscopic and biochemical techniques have been employed, in combination with the classical Marcus theory for electron transfer tunnelling, in order to access these parameters. Nevertheless, the values which have been presented are very variable. In particular, for the case of the tightly bound phylloquinone molecule A₁, the values of the redox potentials reported in the literature vary over a range of about 350 mV. Previous models of Photosystem I have assumed a unidirectional electron transfer model. In the present study, experimental evidence obtained by means of time resolved absorption, photovoltage, and electron paramagnetic resonance measurements are reviewed and analysed in terms of a bi-directional kinetic model for electron transfer reactions. This model takes into consideration the thermodynamic equilibrium between the iron-sulfur centre F_X and the phylloquinone bound to either the PsaA (A_1A) or the PsaB (A_1B) subunit of the reaction centre and the equilibrium between the iron-sulfur centres F_A and F_B. The experimentally determined decay lifetimes in the range of sub-picosecond to the microsecond time domains can be satisfactorily simulated, taking into consideration the edge-to-edge distances between redox cofactors and driving forces reported in the literature. The only exception to this general behaviour is the case of phylloquinone (A₁) reoxidation. In order to describe the reported rates of the biphasic decay, of about 20 and 200 ns, associated with this electron transfer step, the redox potentials of the quinones are estimated to be almost isoenergetic with that of the iron sulfur centre F_X. A driving force in the range of 5 to 15 meV is estimated for these reactions, being slightly exergonic in the case of the A_1B quinone and slightly endergonic, in the case of the A_1A quinone. The simulation presented in this analysis not only describes the kinetic data obtained for the wild type samples at room temperature and is consistent with estimates of activation energy by the analysis of temperature dependence, but can also explain the effect of the mutations around the PsaB quinone binding pocket. A model of the overall energetics of the system is derived, which suggests that the only substantially irreversible electron transfer reactions are the reoxidation of A₀ on both electron transfer branches and the reduction of F_A by F_X.     

Thermodynamics of electron transfer in oxygenic photosynthetic reaction centers: a pulsed photoacoustic study of electron transfer in photosystem I reveals a similarity to bacterial reaction centers in both volume change and entropy

The thermodynamic properties of electron transfer in biological systems are far less known in comparison with that of their kinetics. In this paper the enthalpy and entropy of electron transfer in the purified photosystem I trimer complexes from Synechocystis sp. PCC 6803 have been studied, using pulsed time-resolved photoacoustics on the 1 micros time scale. The volume contraction of reaction centers of photosystem I, which results directly from the light-induced charge separation forming P(700+F(A)/F(B-) from the excited-state P700*, is determined to be -26 +/- 2 A3. The enthalpy of the above electron-transfer reaction is found to be -0.39 +/- 0.1 eV. Photoacoustic estimation of the quantum yield of photochemistry in the purified photosystem I trimer complex showed it to be close to unity. Taking the free energy of the above reaction as the difference of their redox potentials in situ allows us to calculate an apparent entropy change (TDeltaS) of +0.35 +/- 0.1 eV. These values of DeltaV and TDeltaS are similar to those of bacterial reaction centers. The unexpected sign of entropy of electron transfer is tentatively assigned, as in the bacterial case, to the escape of counterions from the surface of the particles. The apparent entropy change of electron transfer in biological system is significant and cannot be neglected.     

Nanosecond electron transfer kinetics in photosystem I following substitution of quinones for vitamin K1 as studied by time resolved EPR.

Room temperature transient EPR spectra of photosystem I (PS I) particles from Synechocystis 6803 are presented. Native PS I samples and preparations depleted in the A1-acceptor site by solvent extraction and then reconstituted with the quinones (Q) vitamin K1 (VK1), duroquinone (DQ and DQd12) and naphthoquinone (NQ) have been studied. Sequential electron transfer to P700+A1- (FeS) and P700+A1 (FeS)- is recovered only with VK1. With DQ and NQ electron transfer is restored to form the radical pair P700+Q- as specified by a characteristic electron spin polarization (ESP)-pattern, but further electron transfer is either slowed down or blocked. A qualitative analysis of the K-band spectrum suggests that the orientation of reconstituted NQ in PS I is different from the native acceptor A1 = VK1.     

Variable chlorophyll a fluorescence from P-700 enriched photosystem I particles dependent on the redox state of the reaction centre.

1. Photosystem I particles enriched in P-700 prepared by Triton X-100 treatment of chloroplasts show a light-induced increase in fluorescence yield of more than 100% in the presence of dithionite but not in its absence. 2. Steady state light maintains the P-700, of these particles, in the oxidised state when ascorbate is present but in the presence of dithionite only a transient oxidation occurs. 3 EPR data show that, in these particles, the primary electron acceptor (X) is maintained in the reduced state by light at room temperature only when the dithionite is also present. In contrast, the secondary electron acceptors are reduced in the dark by dithionite. 4. Fluorescence emission and excitation spectra and fluorescence lifetime measurements for the constant and variable fluorescence indicate a heterogeneity of the chlorophyll in these particles. 5. It is concluded that the variable fluorescence comes from those chlorophylls which can transfer their energy to the reaction centre and that the states PX and P+X are more effective quenchers of chlorophyll fluorescence than PX-, where P is P-700.     

Flash-photolysis studies of the electron transfer from genetically modified spinach plastocyanin to photosystem I.

Plastocyanin (Pc) has been modified by site-directed mutagenesis at two separate electron-transfer (ET) sites: Leu-12-Glu at a hydrophobic patch, and Tyr-83-His at an acidic patch. The reduction potential at pH 7.5 is decreased by 26 mV in Pc(Leu-12-Glu) and increased by 35 mV in Pc(Tyr-83-His). The latter mutant shows a 2-fold slower intracomplex ET to photosystem I (PSI) as expected from the decreased driving force. The affinity for PSI is unaffected for this mutant but is drastically decreased for Pc(Leu-12-Glu). It is concluded that the hydrophobic patch is more important for the ET to PSI.     

Kinetics of charge separation and A0- --> A1 electron transfer in photosystem I reaction centers

The charge separation P700*A(0) --> P700(+)A(0)(-) and the subsequent electron transfer from the primary to secondary electron acceptor have been studied by subtracting absorption difference profiles for cyanobacterial photosystem I (PS I) complexes with open and closed reaction centers. Samples were excited at 660 nm, which lies toward the blue edge of the core antenna absorption spectrum. The resulting PS I kinetics were analyzed in terms of the relevant P700, P700(+), A(0), and A(0)(-) absorption spectra. In our kinetic model, the radical pair P700(+)A(0)(-) forms with 1.3 ps rise kinetics after creation of electronically excited P700*. The formation of A(1)(-) via electron transfer from A(0)(-) requires approximately 13 ps. The kinetics of the latter step are appreciably faster than previously estimated by other groups (20--50 ps).     

Investigation of B-branch electron transfer by femtosecond time resolved spectroscopy in a Rhodobacter sphaeroides reaction centre that lacks the Q(A) ubiquinone

The dynamics of electron transfer in a membrane-bound Rhodobacter sphaeroides reaction centre containing a combination of four mutations were investigated by transient absorption spectroscopy. The reaction centre, named WAAH, has a mutation that causes the reaction centre to assemble without a Q(A) ubiquinone (Ala M260 to Trp), a mutation that causes the replacement of the H(A) bacteriopheophytin with a bacteriochlorophyll (Leu M214 to His) and two mutations that remove acidic groups close to the Q(B) ubiquinone (Glu L212 to Ala and Asp L213 to Ala). Previous work has shown that the Q(B) ubiquinone is reduced by electron transfer along the so-called inactive cofactor branch (B-branch) in the WAAH reaction centre (M.C. Wakeham, M.G. Goodwin, C. McKibbin, M.R. Jones, Photo-accumulation of the P(+)Q(B)(-) radical pair state in purple bacterial reaction centres that lack the Q(A) ubiquinone, FEBS Letters 540 (2003) 234-240). In the present study the dynamics of electron transfer in the membrane-bound WAAH reaction centre were studied by femtosecond transient absorption spectroscopy, and the data analysed using a compartmental model. The analysis indicates that the yield of Q(B) reduction via the B-branch is approximately 8% in the WAAH reaction centre, consistent with results from millisecond time-scale kinetic spectroscopy. Possible contributions to this yield of the constituent mutations in the WAAH reaction centre and the membrane environment of the complex are discussed.     

The two histidine axial ligands of the primary electron donor chlorophylls (P700) in photosystem I are similarly perturbed upon P700+ formation

The extent of delocalization of the positive charge in the oxidized dimer of chlorophyll (Chl) constituting P700, the primary electron donor of photosystem I (PSI), has been investigated by analyzing the perturbation upon P700(+) formation of infrared (IR) vibrational modes of the two His axial ligands of the two P700 Chl molecules. Fourier transform IR (FTIR) difference spectra of the photooxidation of P700 in PSI core complexes isolated from Synechocystis sp. PCC 6803 isotopically labeled either globally with (15)N or more specifically with (13)C on all the His residues reveal isotopic shifts of a differential signal at 1102/1108 cm(-)(1). This signal is assigned to a downshift upon P700(+) formation of the predominantly C(5)-Ntau imidazole stretching mode of His residue(s). The amplitude of this signal is reduced by approximately half in FTIR spectra of Synechocystis mutants in which His PsaB 651, the axial ligand to one of the two Chl molecules in P700, is replaced by Cys, Gln, or Leu. These observations provide further evidence that the positive charge in P700(+) is essentially delocalized over the two Chl molecules, in agreement with a previous FTIR study in which the frequency of the vibrational modes of the 9-keto and 10a-ester C=O groups of the two Chl's in P700, P700(+), and (3)P700 were firmly established for the first time [Breton, J., et al. (1999) Biochemistry 38, 11585-11592]. Only limited perturbations of the amplitude and frequency of the 9-keto and 10a-ester C=O bands of the P700 Chl are elicited by the mutations. On the basis of comparable mutational studies of the primary electron donor in purple bacteria, these perturbations are attributed to small molecular rearrangements of the Chl macrocycle and substituents caused by the repositioning of the P700 dimer in the new protein cavity generated by the mutations. It is proposed that the perturbation of the FTIR spectra upon mutation of a His axial ligand of the P700 Chl recently reported in Chlamydomonas reinhardtii [Hastings, G., et al. (2001) Biochemistry 40, 12943-12949] can be explained by the same effect without the need for a new assignment of the C=O bands of P700. The distribution of charge/spin in P700(+) and (3)P700 determined by FTIR spectroscopy is discussed in relation with the contrasting interpretations derived from recent magnetic resonance experiments.     

FTIR study of the primary electron donor of photosystem I (P700) revealing delocalization of the charge in P700(+) and localization of the triplet character in (3)P700.

The effect of global (15)N or (2)H labeling on the light-induced P700(+)/P700 FTIR difference spectra has been investigated in photosystem I samples from Synechocystis at 90 K. The small isotope-induced frequency shifts of the carbonyl modes observed in the P700(+)/P700 spectra are compared to those of isolated chlorophyll a. This comparison shows that bands at 1749 and 1733 cm(-)(1) and at 1697 and 1637 cm(-)(1), which upshift upon formation of P700(+), are candidates for the 10a-ester and 9-keto C=O groups of P700, respectively. A broad and relatively weak band peaking at 3300 cm(-)(1), which does not shift upon global labeling or (1)H-(2)H exchange, is ascribed to an electronic transition of P700(+), indicating that at least two chlorophyll a molecules (denoted P(1) and P(2)) participate in P700(+). Comparisons of the (3)P700/P700 FTIR difference spectrum at 90 K with spectra of triplet formation in isolated chlorophyll a or in RCs from photosystem II or purple bacteria identify the bands at 1733 and 1637 cm(-)(1), which downshift upon formation of (3)P700, as the 10a-ester and 9-keto C=O modes, respectively, of the half of P700 that bears the triplet (P(1)). Thus, while the P(2) carbonyls are free from interaction, both the 10a-ester and the 9-keto C=O of P(1) are hydrogen bonded and the latter group is drastically perturbed compared to chlorophyll a in solution. The Mg atoms of P(1) and P(2) appear to be five-coordinated. No localization of the triplet on the P(2) half of P700 is observed in the temperature range of 90-200 K. Upon P700 photooxidation, the 9-keto C=O bands of P(1) and P(2) upshift by almost the same amount, giving rise to the 1656(+)/1637(-) and 1717(+)/1697(-) cm(-)(1) differential signals, respectively. The relative amplitudes of these differential signals, as well as of those of the 10a-ester C=O modes, appear to be slightly dependent on sample orientation and temperature and on the organism used to generate the P700(+)/P700 spectrum. If it is assumed that the charge density on ring V of chlorophyll a, as measured by the perturbation of the 10a-ester or 9-keto C=O IR vibrations, mainly reflects the spin density on the two halves of the oxidized P700 special pair, a charge distribution ranging from 1:1 to 2:1 (in favor of P(2)) is deduced from the measurements presented here. The extreme downshift of the 9-keto C=O group of P(1), indicative of an unusually strong hydrogen bond, is discussed in relation with the models previously proposed for the PSI special pair.     

Full replacement of the function of the secondary electron acceptor phylloquinone(= vitamin K1) by non-quinone carbonyl compounds in green plant photosystem I photosynthetic reaction centers

One-carbonyl quinonoid compounds, fluorenone (fluoren-9-one), anthrone, and their derivatives are introduced into spinach photosystem (PS) I reaction centers in place of the intrinsic secondary electron acceptor phylloquinone (= vitamin K1). Anthrone and 2-nitrofluorenone fully mediated the electron-transfer reaction between the reduced primary electron acceptor chlorophyll A0- and the tertiary electron acceptor iron-sulfur centers. It is concluded that the PS I phylloquinone-binding site has a structure that enables various compounds with different molecular structures to function as the secondary acceptor and that the reactions of incorporated compounds are mainly determined by their redox properties rather than by their molecular structure. Carbonyl groups increase the binding affinity of the quinone/quinonoid compounds but do not seem to be essential to their function. The quinonoid compounds as well as quinones incorporated into the PS I phylloquinone-binding sites are estimated to function at redox potentials more negative than in organic solvents.     

Temperature dependence of biphasic forward electron transfer from the phylloquinone(s) A1 in photosystem I: only the slower phase is activated

The temperature dependence of the biphasic electron transfer (ET) from the secondary acceptor A1 (phylloquinone) to iron-sulfur cluster F(X) was investigated by flash absorption spectroscopy in photosystem I (PS I) isolated from Synechocystis sp. PCC 6803. While the slower phase (tau=340 ns at 295 K) slowed upon cooling according to an activation energy of 110 meV, the time constant of the faster phase (tau=11 ns at 295 K) was virtually independent of temperature. Following a suggestion in the literature that the two phases arise from bidirectional ET involving two symmetrically arranged phylloquinones, Q(K)-A and Q(K)-B, it is concluded that energetic parameters (most likely the driving forces) rather than the electronic couplings are different for ET from Q(K)-A to F(X) and from Q(K)-B to F(X). Two alternative schemes of ET in PS I are presented and discussed.     

Salt-induced photosystem I cyclic electron transfer restores growth on low inorganic carbon in a type 1 NAD(P)H dehydrogenase deficient mutant of Synechocystis PCC6803

The cyanobacterium Synechocystis PCC6803 induces a photosystem I cyclic electron transfer route independent of type 1 NAD(P)H dehydrogenase. The capacity to tolerate raised salinity conditions was shown to operate in a mutant lacking functional type 1 NAD(P)H dehydrogenase. The mutant showed salt-induced enhancement of photosystem I cyclic electron transfer and respiratory capacities. Moreover, this salt-adapted energetic state also restored the capacity of the mutant to grow under inorganic carbon limitation. Uptake of the latter in these conditions became almost as efficient as in the wild-type. The acquired energetic capacities, in contrast, did not allow restoration of photoheterotrophic growth in the type 1 NAD(P)H dehydrogenase mutant.     

Temperature dependence of biphasic forward electron transfer from the phylloquinone(s) A1 in photosystem I: only the slower phase is activated

The temperature dependence of the biphasic electron transfer (ET) from the secondary acceptor A1 (phylloquinone) to iron-sulfur cluster F_X was investigated by flash absorption spectroscopy in photosystem I (PS I) isolated from Synechocystis sp. PCC 6803. While the slower phase (τ=340 ns at 295 K) slowed upon cooling according to an activation energy of 110 meV, the time constant of the faster phase (τ=11 ns at 295 K) was virtually independent of temperature. Following a suggestion in the literature that the two phases arise from bidirectional ET involving two symmetrically arranged phylloquinones, Q_K-A and Q_K-B, it is concluded that energetic parameters (most likely the driving forces) rather than the electronic couplings are different for ET from Q_K-A to F_X and from Q_K-B to F_X. Two alternative schemes of ET in PS I are presented and discussed.