Assignment of a kinetic component to electron transfer between iron-sulfur clusters FX and FA/B of Photosystem I

We studied the kinetics of reoxidation of the phylloquinones in Chlamydomonas reinhardtii Photosystem I using site-directed mutations in the PhQ_A-binding site and of the residues serving as the axial ligand to ec3_A and ec3_B chlorophylls. In wild type PS I, these kinetics are biphasic, and mutations in the binding region of PhQ_A induced a specific slowing down of the slow component. This slowing allowed detection of a previously unobserved 180-ns phase having spectral characteristics that differ from electron transfer between phylloquinones and F_X. The new kinetic phase thus reflects a different reaction that we ascribe to oxidation of F_X⁻ by the F_A/B FeS clusters. These absorption changes partly account for the differences between the spectra associated with the two kinetic components assigned to phylloquinone reoxidation. In the mutant in which the axial ligand to ec3_A (PsaA-Met688) was targeted, about 25% of charge separations ended in P₇₀₀⁺A₀⁻ charge recombination; no such recombination was detected in the B-side symmetric mutant. Despite significant changes in the amplitude of the components ascribed to phylloquinone reoxidation in the two mutants, the overall nanosecond absorption changes were similar to the wild type. This suggests that these absorption changes are similar for the two different phylloquinones and that part of the differences between the decay-associated spectra of the two components reflect a contribution from different electron acceptors, i.e. from an inter-FeS cluster electron transfer.     

A kinetic assessment of the sequence of electron transfer from F(X) to F(A) and further to F(B) in photosystem I: the value of the equilibrium constant between F(X) and F(A)

The x-ray structure analysis of photosystem I (PS I) crystals at 4-A resolution (Schubert et al., 1997, J. Mol. Biol. 272:741-769) has revealed the distances between the three iron-sulfur clusters, labeled F(X), F(1), and F(2), which function on the acceptor side of PS I. There is a general consensus concerning the assignment of the F(X) cluster, which is bound to the PsaA and PsaB polypeptides that constitute the PS I core heterodimer. However, the correspondence between the acceptors labeled F(1) and F(2) on the electron density map and the F(A) and F(B) clusters defined by electron paramagnetic resonance (EPR) spectroscopy remains controversial. Two recent studies (Diaz-Quintana et al., 1998, Biochemistry. 37:3429-3439;, Vassiliev et al., 1998, Biophys. J. 74:2029-2035) provided evidence that F(A) is the cluster proximal to F(X), and F(B) is the cluster that donates electrons to ferredoxin. In this work, we provide a kinetic argument to support this assignment by estimating the rates of electron transfer between the iron-sulfur clusters F(X), F(A), and F(B). The experimentally determined kinetics of P700(+) dark relaxation in PS I complexes (both F(A) and F(B) are present), HgCl(2)-treated PS I complexes (devoid of F(B)), and P700-F(X) cores (devoid of both F(A) and F(B)) from Synechococcus sp. PCC 6301 are compared with the expected dependencies on the rate of electron transfer, based on the x-ray distances between the cofactors. The analysis, which takes into consideration the asymmetrical position of iron-sulfur clusters F(1) and F(2) relative to F(X), supports the F(X) --> F(A) --> F(B) --> Fd sequence of electron transfer on the acceptor side of PS I. Based on this sequence of electron transfer and on the observed kinetics of P700(+) reduction and F(X)(-) oxidation, we estimate the equilibrium constant of electron transfer between F(X) and F(A) at room temperature to be approximately 47. The value of this equilibrium constant is discussed in the context of the midpoint potentials of F(X) and F(A), as determined by low-temperature EPR spectroscopy.     

Effects of selective destruction of iron-sulfur center B on electron transfer and charge recombination in Photosystem I

Incubation of spinach thylakoids with HgCl₂ selectively destroys Fe–S center B (F_B). The function of electron acceptors in F_B-less PS I particles was studied by following the decay kinetics of P700⁺ at room temperature after multiple flash excitation in the absence of a terminal electron acceptor. In untreated particles, the decay kinetics of the signal after the first and the second flashes were very similar (t _1/22.5 ms), and were principally determined by the concentration of the artificial electron donor added. The decay after the third flash was fast (t _1/20.25 ms). In F_B-less particles, although the decay after the first flash was slow, fast decay was observed already after the second flash. We conclude that in F_B-less particles, electron transfer can proceed normally at room temperature from F_X to F_A and that the charge recombination between P700⁺ and F_X ^-/A₁ ^- predominated after the second excitation. The rate of this recombination process is not significantly affected by the destruction of F_B. Even in the presence of 60% glycerol, F_B-less particles can transfer electrons to F_A at room temperature as efficiently as untreated particles.Abbreviations DCIP 2, 6-dichlorophenol indophenol - F_A, F_B, F_X iron-sulfur center A, B and X, respectively - PMS phenazine methosulfate     

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).     

Electrometrical study of electron transfer from the terminal FA/FB iron-sulfur clusters to external acceptors in photosystem I

An electrometrical technique was used to investigate electron transfer between the terminal iron-sulfur centers F(A)/F(B) and external electron acceptors in photosystem I (PS I) complexes from the cyanobacterium Synechococcus sp. PCC 6301 and from spinach. The increase of the relative contribution of the slow components of the membrane potential decay kinetics in the presence of both native (ferredoxin, flavodoxin) and artificial (methyl viologen) electron acceptors indicate the effective interaction between the terminal 14Fe-4S] cluster and acceptors. The finding that FA fails to donate electrons to flavodoxin in F(B)-less (HgCl2-treated) PS I complexes suggests that F(B) is the direct electron donor to flavodoxin. The lack of additional electrogenicity under conditions of effective electron transfer from the F(B) redox center to soluble acceptors indicates that this reaction is electrically silent.     

Spectral and kinetic characterization of electron acceptor A1 in a Photosystem I core devoid of iron-sulfur centers FX,FB and FA

The kinetic and spectroscopic properties of the secondary electron acceptor A₁ were determined by flash absorption spectroscopy at room and cryogenic temperatures in a Photosystem I (PS I) core devoid of the iron-sulfur clusters F_X, F_B and F_A. It was shown earlier (Warren, P.V., Golbeck, J.H. and Warden, J.T. (1993) Biochemistry 32: 849–857) that the majority of the flash-induced absorbance increase at 820 nm, reflecting formation of P700⁺, decays with a t_1/2 of 10 s due to charge recombination between P700⁺ and A₁ ^–. Following A₁ ^– directly around 380 nm, where absorbance changes due to the formation of P700⁺ are negligible, two major decay components were resolved in this study with t_1/2 of 10 s and 110 s at an amplitude ratio of 2.5:1. The difference spectra between 340 and 490 nm of the two kinetic phases are highly similar, showing absorbance increases from 340 to 400 nm characteristic of the one-electron reduction of the phylloquinone A₁. When measured at 10 K, the flash-induced absorbance changes around 380 nm can be fitted with two decay phases of t_1/2 15 s and 150 s at an amplitude ratio 1:1. The difference spectra of both kinetic phases from 340 to 400 nm are similar to those determined at 298 K and are therefore attributed to charge recombination in the pair P700⁺A₁ ^–. These results indicate that the backreaction between P700⁺ and A₁ ^– is multiphasic when F_X, F_B and F_A are removed, and only slightly temperature dependent in the range of 298 K to 10 K.Abbreviations Chl chlorophyll - D pathlength for the measuring light through the sample - DPIP 2,6-dichlorophenolindophenol - EPR electron paramagnetic resonance - IR infrared - PS I Photosystem I - Tris Tris(hydroxymethyl)aminomethane - UV ultraviolet Published as Journal Series #10890 of the University of Nebraska Agricultural Research Division and supported by a grant from the National Science Foundation (MCB-9205756).     

Stabilization of iron-sulfur cluster F(X) by intra-subunit interactions unraveled by suppressor and second site-directed mutations in PsaB of Photosystem I

Intra-subunit interactions in the environment of the iron-sulfur cluster F(X) in Photosystem I (PS I) of Synechocystis sp. PCC 6803 were studied by site-directed and second site suppressor mutations. In subunit PsaB, the cysteine ligand (C565) of F(X) and a conserved aspartate (D566) adjacent to C565 were modified. The resulting mutants D566E, C556S/D566E, C556H/D566E and C565H/D566E did not assemble PS I in the thylakoids of the cyanobacterium. Yet, this is the first report of cells of the second site-suppressor mutant (D566E/L416P) and of second site-directed mutant (C565S/D566E) in PsaB that could grow autotrophically in light and were found to assemble a stable functional PS I containing all three iron-sulfur centers, F(X) and F(A/B). The newly resolved structure of PS I (PDB 1JB0) was used to interpret the functional interactions among the amino acid residues. It is suggested that the stability of F(X) is supported by a salt bridge formed between D566, which is adjacent to the cysteine ligand C565 of the iron-sulfur cluster located on loop hi, and R703 located at the start of loop jk. Hydrogen bond between R703 and D571 at the start of loop hi further stabilizes the arginine. Lengthening of the side by 1.2 A chain in mutation D566E caused destabilization of F(X). The extended side-chain was compensated for by the Fe-O, which is 0.3 A shorter than the Fe-S bond resulting in stabilization of the F(X) in the double mutations C565S/D566E. The suppressor mutation D566E/L416P allowed greater freedom for the salt bridge E566-R703, thus relieving the pressure introduced by the D566E replacement and enabling the formation of F(X). F(X) and R703 are therefore stabilized through short- and long-range interactions of the inter-helical loops between h-i, j-k and f-g, respectively.     

Kinetic identification of component X as P430: a primary electron acceptor of Photosystem I

Kinetics of dark recoveries of Component X, Center A, and Center B at 20 and 0 °C after a 30-s illumination were studied in membrane fragments from a blue-green alga by using low temperature electron paramagnetic resonance spectroscopy in combination with a quick-freeze method. These kinetics were compared with those obtained by spectrophotometry under the same conditions. Contrary to the currently popular view, the result strongly suggests that Component X, rather than Center A or Center B, is P430.     

Diazonium modification of Photosystem I. A specific effect on iron-sulfur Center B

Modification of chloroplast membranes with diazonium benzene sulfonate (DABS) leads to a loss of Photosystem I-dependent ferredoxin reduction but not methyl viologen reduction. EPR studies of DABS-modified membranes show no inhibition of P-700⁺ formation at cryogenic temperatures, but iron-sulfur Center A photoreduction is markedly inhibited. Iron-sulfur Center B photoreduction at physiological temperatures in DABS-modified membranes is also markedly inhibited and little Center B can be detected after dark chemical reduction. These results indicate DABS specifically modifies iron-sulfur Center B of the spinach chloroplast Photosystem I electron acceptor complex and that Center B is obligately required for the reduction of Center A at cryogenic temperatures. Possible electron transport pathways at physiological temperatures are also considered.     

Flavodoxin: A compromise between efficiency and versatility in the electron transfer from Photosystem I to Ferredoxin-NADP reductase

Under iron-deficient conditions Flavodoxin (Fld) replaces Ferredoxin in Anabaena as electron carrier from Photosystem I (PSI) to Ferredoxin-NADP⁺ reductase (FNR). Several residues modulate the Fld interaction with FNR and PSI, but no one appears as specifically critical for efficient electron transfer (ET). Fld shows a strong dipole moment, with its negative end directed towards the flavin ring. The role of this dipole moment in the processes of interaction and ET with positively charged surfaces exhibited by PSI and FNR has been analysed by introducing single and multiple charge reversal mutations on the Fld surface. Our data confirm that in this system interactions do not rely on a precise complementary surface of the reacting molecules. In fact, they indicate that the initial orientation driven by the alignment of dipole moment of the Fld molecule with that of the partner contributes to the formation of a bunch of alternative binding modes competent for the efficient ET reaction. Additionally, the fact that Fld uses different interaction surfaces to dock to PSI and to FNR is confirmed.     

PsaC subunit of photosystem I is oriented with iron-sulfur cluster F(B) as the immediate electron donor to ferredoxin and flavodoxin.

The PsaC subunit of photosystem I (PS I) binds two [4Fe-4S] clusters, F(A) and F(B), functioning as electron carriers between F(X) and soluble ferredoxin. To resolve the issue whether F(A) or F(B) is proximal to F(X), we used single-turnover flashes to promote step-by-step electron transfer between electron carriers in control (both F(A) and F(B) present) and HgCl2-treated (F(B)-less) PS I complexes from Synechococcus sp. PCC 6301 and analyzed the kinetics of P700+ reduction by monitoring the absorbance changes at 832 nm in the presence of a fast electron donor (phenazine methosulfate (PMS)). In control PS I complexes exogenously added ferredoxin, or flavodoxin could be photoreduced on each flash, thus allowing P700+ to be reduced from PMS. In F(B)-less complexes, both in the presence and in the absence of ferredoxin or flavodoxin, P700+ was reduced from PMS only on the first flash and was reduced from F(X)- on the following flashes, indicating lack of electron transfer to ferredoxin or flavodoxin. In the F(B)-less complexes, a normal level of P700 photooxidation was detected accompanied by a high yield of charge recombination between P700+ and F(A)- in the presence of a slow donor, 2,6-dichlorophenol-indophenol. This recombination remained the only pathway of F(A)- reoxidation in the presence of added ferredoxin, consistent with the lack of forward electron transfer. F(A)- could be reoxidized by methyl viologen in F(B)-less PS I complexes, although at a concentration two orders of magnitude higher than is required in wild-type PS I complexes, thus implying the presence of a diffusion barrier. The inhibition of electron transfer to ferredoxin and flavodoxin was completely reversed after reconstituting the F(B) cluster. Using rate versus distance estimates for electron transfer rates from F(X) to ferredoxin for two possible orientations of PsaC, we conclude that the kinetic data are best compatible with PsaC being oriented with F(A) as the cluster proximal to F(X) and F(B) as the distal cluster that donates electrons to ferredoxin.     

Evidence that the intermediate electron acceptor,A2, in Photosystem I is a bound iron-sulfur protein

Absorption changes accompanying the formation of light-induced P-700⁺ were investigated in a highly enriched Photosystem I preparation where an intermediate electron acceptor preceding P-430 could be detected. In an enriched Photosystem I particle, light-induced reversible absorption changes observed at 700 nm in the presence of dithionite resembled those previously seen at 703 nm and 820 nm [9], thus indicating the presence of a backreaction between P-700⁺ and A^?₂. After this same Photosystem I particle was treated to denature the bound iron-sulfur centers, the photochemical changes that could be attributed to P-700 A₂ were completely lost. These results provide evidence that the intermediate electron acceptor, A₂, is a bound iron-sulfur protein. Additional studies in the 400–500 nm region with Photosystem I particles prepared by sonication indicate that the spectrum of A₂ is different from that of P-430.     

Evidence for the interaction of the Photosystem I secondary electron acceptor X with chlorophyll a in spinach Photosystem I particles

Ether extraction of antenna pigments from PS I particles (Ikegami, I. and Katoh, S. (1975) Biochim. Biophys. Acta 376, 588–592) led to the change of EPR signal of the PS I secondary electron acceptor ‘X’. The g_x value of the EPR signal of X, which was 1.77 in the PS I particles, remained unchanged as far as the pigment extracted was less than 50%. However, further extraction of pigments shifted it to the higher value; it came up to 1.80 in the particles containing about 5% chlorophyll a. g_y and g_z values of the EPR signal of X were less sensitive to the pigment extraction. The g_x signal intensity of the EPR signal of X remained almost constant through the pigment extraction. The re-incorporation of the purified chlorophyll a to the pigment-extracted particles resulted in a partial recovery of the g_x value. On the other hand, vitamin K-1 had no significant effect on the recovery of the g_x value. The results suggest the close location of the component X to chlorophyll a in the vicinity of PS I reaction center.     

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.     

Characterization by electron paramagnetic resonance of the role of the Escherichia coli nitrate reductase (NarGHI) iron-sulfur clusters in electron transfer to nitrate and identification of a semiquinone radical intermediate.

We have used Escherichia coli cytoplasmic membrane preparations enriched in wild-type and mutant (NarH-C16A and NarH-C263A) nitrate reductase (NarGHI) to study the role of the [Fe-S] clusters of this enzyme in electron transfer from quinol to nitrate. The spectrum of dithionite-reduced membrane bound NarGHI has major features comprising peaks at g = 2.04 and g = 1.98, a peak-trough at g = 1.95, and a trough at g = 1.87. The oxidized spectrum of NarGHI in membranes comprises an axial [3Fe-4S] cluster spectrum with a peak at g = 2.02 (g(z)) and a peak-trough at g = 1.99 (g(xy)). We have shown that in two site-directed mutants of NarGHI which lack the highest potential [4Fe-4S] cluster (B. Guigliarelli, A. Magalon, P. Asso, P. Bertrand, C. Frixon, G. Giordano, and F. Blasco, Biochemistry 35:4828-4836, 1996), NarH-C16A and NarH-C263A, oxidation of the NarH [Fe-S] clusters is inhibited compared to the wild type. During enzyme turnover in the mutant enzymes, a distinct 2-n-heptyl-4-hydroxyquinoline-N-oxide-sensitive semiquinone radical species which may be located between the hemes of NarI and the [Fe-S] clusters of NarH is observed. Overall, these studies indicate (i) the importance of the highest-potential [4Fe-4S] cluster in electron transfer from NarH to the molybdenum cofactor of NarG and (ii) that a semiquinone radical species is an important intermediate in electron transfer from quinol to nitrate.     

Asymmetric electron transfer in cyanobacterial Photosystem I: charge separation and secondary electron transfer dynamics of mutations near the primary electron acceptor A0

Point mutations were introduced near the primary electron acceptor sites assigned to A0 in both the PsaA and PsaB branches of Photosystem I in the cyanobacterium Synechocystis sp. PCC 6803. The residues Met688PsaA and Met668PsaB, which provide the axial ligands to the Mg2+ of the eC-A3 and eC-B3 chlorophylls, were changed to leucine and asparagine (chlorophyll notation follows Jordan et al., 2001). The removal of the ligand is expected to alter the midpoint potential of the A0/A0- redox pair and result in a change in the intrinsic charge separation rate and secondary electron transfer kinetics from A0- to A1. The dynamics of primary charge separation and secondary electron transfer were studied at 690 nm and 390 nm in these mutants by ultrafast optical pump-probe spectroscopy. The data reveal that mutations in the PsaB branch do not alter electron transfer dynamics, whereas mutations in the PsaA branch have a distinct effect on electron transfer, slowing down both the primary charge separation and the secondary electron transfer step (the latter by a factor of 3-10). These results suggest that electron transfer in cyanobacterial Photosystem I is asymmetric and occurs primarily along the PsaA branch of cofactors.     

Electron-spin resonance studies of the bound iron-sulfur centers in Photosystem I II. Correlation of P-700 triplet production with urea/ferricyanide inactivation of the iron-sulfur clusters

Photosystem I charge separation in a subchloroplast particle isolated from spinach was investigated by electron spin resonance (ESR) spectroscopy following graduated inactivation of the bound iron-sulfur centers by urea-ferricyanide treatment. Previous work demonstrated a differential decrease in iron-sulfur centers A, B and X which indicated that center X serves as a branch point for parallel electron flow through centers A and B (Golbeck, J.H. and Warden, J.T. (1982) Biochim. Biophys. Acta 681, 77–84). We now show that during inactivation the disappearance of iron-sulfur centers A, B, and X correlates with the appearance of a spin-polarized triplet ESR signal with |D| = 279·10⁻⁴ cm⁻¹ and |E| = 39·10⁻⁴ cm⁻¹. The triplet resonances titrate with a midpoint potential of +380 ± 10 mV. Illumination of the inactivated particles results in the generation of an asymmetric ESR signal with g = 2.0031 and ΔH_pp = 1.0 mT. Deconvolution of the P-700⁺ contribution to this composite resonance reveals the spectrum of the putative primary acceptor species, A₀, which is characterized by g = 2.0033 ± 0.0004 and ΔH_pp = 1.0 ± 0.2 mT. The data presented in this report do not substantiate the participation of the electron acceptor A₁ in PS I electron transport, following destruction of the iron-sulfur cluster corresponding to center X. We suggest that A₁ is closely associated with center X and that this component is decoupled from the electron-transport path upon destruction of center X. The inability to photoreduce A₁ in reaction centers lacking a functional center X may result from alteration of the reaction center tertiary structure by the urea-ferricyanide treatment or from displacement of A₁ from its binding site.     

Evidence that the low-potential (−700 mV) electron acceptor (X) in Photosystem I has two iron-sulphur centres

The Photosystem I reaction centre contains two groups of iron-sulphur centres: Fe-S_A and Fe-S_B with redox potentials between ?510 and ?590 mV, and Fe-S_X with redox potential about ?700 mV. Spin quantitation (Heathcote, P., Williams-Smith, D.L. and Evans, M.C.W. (1978) Biochem. J. 170, 373–378) and Mössbauer spectroscopy (Evans, E.H., Dickson, D.P.E., Johnson, C.E., Rush, J.D. and Evans, M.C.W. (1981) Eur. J. Biochem. 118, 81–84) did not show unequivocally whether Fe-S_X has one or two centres. Experiments are described which support the proposal that Fe-S_X has two centres. Fe-S_X can be photoreduced irreversibly by 210 K illumination of dithionite-reduced samples or reversibly by 7.5 K illumination of these samples. The amplitude of the Fe-S_X signal reversibly induced by illumination at 7.5 K is never more than 50% of the amplitude of the signal when Fe-S_X is prereduced by room temperature illumination or by 210 K illumination. Approx. half of the Fe-S_X is rapidly reduced by 210 K illumination, the remainder more slowly. The extent of reversible Fe-S_X reduction and P-700 photooxidation is little affected by the fast reduction of about half of the Fe-S_X. Subsequent reduction of the remaining Fe-S_X is paralleled by loss of the reversible photoreaction.     

pH-induced intramolecular electron transfer between the iron-sulfur protein and cytochrome c(1) in bovine cytochrome bc(1) complex

Structural analysis of the bc(1) complex suggests that the extra membrane domain of iron-sulfur protein (ISP) undergoes substantial movement during the catalytic cycle. Binding of Qo site inhibitors to this complex affects the mobility of ISP. Taking advantage of the difference in the pH dependence of the redox midpoint potentials of cytochrome c(1) and ISP, we have measured electron transfer between the [2Fe-2S] cluster and heme c(1) in native and inhibitor-treated partially reduced cytochrome bc(1) complexes. The rate of the pH-induced cytochrome c(1) reduction can be estimated by conventional stopped-flow techniques (t1/2, 1-2 ms), whereas the rate of cytochrome c(1) oxidation is too high for stopped-flow measurement. These results suggest that oxidized ISP has a higher mobility than reduced ISP and that the movement of reduced ISP may require an energy input from another component. In the 5-n-undecyl-6-hydroxy-4,7-dioxobenzothiazole (UHDBT)-inhibited complex, the rate of cytochrome c(1) reduction is greatly decreased to a t1/2 of approximately 2.8 s. An even lower rate is observed with the stigmatellin-treated complex. These results support the idea that UHDBT and stigmatellin arrest the [2Fe-2S] cluster at a fixed position, 31 A from heme c(1), making electron transfer very slow.     

Electron-spin resonance studies of the bound iron-sulfur centers in Photosystem I. II. Correlation of P-700 triplet production with urea/ferricyanide inactivation of the iron-sulfur clusters

Photosystem I charge separation in a subchloroplast particle isolated from spinach was investigated by electron spin resonance (ESR) spectroscopy following graduated inactivation of the bound iron-sulfur centers by urea-ferricyanide treatment. Previous work demonstrated a differential decrease in iron-sulfur centers A, B and X which indicated that center X serves as a branch point for parallel electron flow through centers A and B (Golbeck, J.H. and Warden, J.T. (1982) Biochim. Biophys. Acta 681, 77-84). We now show that during inactivation the disappearance of iron-sulfur centers A, B, and X correlates with the appearance of a spin-polarized triplet ESR signal with [D] = 279 X 10(-4) cm-1 and [E] = 39 X 10(-4) cm-1. The triplet resonances titrate with a midpoint potential of +380 +/- 10 mV. Illumination of the inactivated particles results in the generation of an asymmetric ESR signal with g = 2.0031 and delta Hpp = 1.0 mT. Deconvolution of the P-700+ contribution to this composite resonance reveals the spectrum of the putative primary acceptor species A0, which is characterized by g = 2.0033 +/- 0.0004 and delta Hpp = 1.0 +/- 0.2 mT. The data presented in this report do not substantiate the participation of the electron acceptor A1 in PS I electron transport, following destruction of the iron-sulfur cluster corresponding to center X. We suggest that A1 is closely associated with center X and that this component is decoupled from the electron-transport path upon destruction of center X. The inability to photoreduce A1 in reaction centers lacking a functional center X may result from alteration of the reaction center tertiary structure by the urea-ferricyanide treatment or from displacement of A1 from its binding site.