Removal of the PsaF polypeptide biases electron transfer in favor of the PsaB branch of cofactors in Triton X-100 photosystem I complexes from Synechococcus sp. PCC 7002.

Continuous wave (CW) and transient electron paramagnetic resonance studies have implied that when PsaF is removed genetically, the double reduction of A1A is facile, the lifetime of A1A(-) is shorter and the ratio of fast to slow kinetic phases increases in PS I complexes isolated with Triton X-100 (Van der Est, A., A. I. Valieva, Y. E. Kandrashkin, G. Shen, D. A. Bryant and J. H. Golbeck [2004] Biochemistry43, 1264-1275). Changes in the lifetimes of A1A(-) and A1B(-) are characteristic of mutants involving the quinone binding sites, but changes in the relative amplitudes of A1A(-) and A1B(-) are characteristic of mutants involving the primary electron acceptors, A0A and A0B. Here, we measured the fast and slow phases of electron transfer from A1B(-) and A1A(-) to FX in psaF and psaE psaF null mutants using time-resolved CW and pump-probe optical absorption spectroscopy. The lifetime of the fast kinetic phase was found to be unaltered, but the lifetime of the slow kinetic phase was shorter in the psaF null mutant and even more so in the psaE psaF null mutant. Concomitantly, the amplitude of the fast kinetic phase increased by a factor of 1.8 and 2.0 in the psaF and psaE psaF null mutants, respectively, at the expense of the slow kinetic phase. The change in ratio of the fast to slow kinetic phases is explained as either a redirection of electron transfer through A1B at the expense of A1A, or a shortening of the lifetime of A1A(-) to become identical to that of A1B(-). The constant lifetime and the characteristics of the near-UV spectrum of the fast kinetic phase favor the former explanation. A unified hypothesis is presented of a displacement of the A-jk1 alpha-helix and switchback loop, which would weaken the H-bond from Leu722 to A1A, accounting for the acceleration of the slow kinetic phase, as well as weaken the H-bond from Tyr696 to A0A, accounting for the bias of electron transfer in favor of the PsaB branch of cofactors.

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.

Contributions of the protein environment to the midpoint potentials of the A1 phylloquinones and the Fx iron-sulfur cluster in photosystem I.

Electrostatic calculations have predicted that the partial negative charge associated with D575PsaB plays a significant role in modulating the midpoint potentials of the A1A and A1B phylloquinones in photosystem I. To test this prediction, the side chain of residue 575PsaB was changed from negatively charged (D) to neutral (A) and to positively charged (K). D566PsaB, which is located at a considerable distance from either A1A or A1B, and should affect primarily the midpoint potential of FX, was similarly changed. In the 575PsaB variants, the rate of electron transfer from A1A to FX is observed to decrease slightly according to the sequence D/A/K. In the 566PsaB variants, the opposite effect of a slight increase in the rate is observed according to the same sequence D/A/K. These results are consistent with the expectation that changing these residues will shift the midpoint potentials of nearby cofactors to more positive values and that the magnitude of this shift will depend on the distance between the cofactors and the residues being changed. Thus, the midpoint potentials of A1A and A1B should experience a larger shift than will FX in the 575PsaB variants, while FX should experience a larger shift than will either A1A or A1B in the 566PsaB variants. As a result, the driving energy for electron transfer from A1A and A1B to FX will be decreased in the former and increased in the latter. This rationalization of the changes in kinetics is compared with the results of electrostatic calculations. While the altered amino acids shift the midpoint potentials of A1A, A1B, and FX by different amounts, the difference in the shifts between A1A and FX or between A1B and FX is small so that the overall effect on the electron transfer rate between A1A and FX or between A1B and FX is predicted to be small. These conclusions are borne out by experiment.

Identification of FX in the heliobacterial reaction center as a [4Fe-4S] cluster with an S = 3/2 ground spin state.

Type I homodimeric reaction centers, particularly the class present in heliobacteria, are not well understood. Even though the primary amino acid sequence of PshA in Heliobacillus mobilis has been shown to contain an F(X) binding site, a functional Fe-S cluster has not been detected by EPR spectroscopy. Recently, we reported that PshB, which contains F(A)- and F(B)-like Fe-S clusters, could be removed from the Heliobacterium modesticaldum reaction center (HbRC), resulting in 15 ms lifetime charge recombination between P798(+) and an unidentified electron acceptor [Heinnickel, M., Shen, G., Agalarov, R., and Golbeck, J. H. (2005) Biochemistry 44, 9950-9960]. We report here that when a HbRC core is incubated with sodium dithionite in the presence of light, the 15 ms charge recombination is replaced with a kinetic transient in the sub-microsecond time domain, consistent with the reduction of this electron acceptor. Concomitantly, a broad and intense EPR signal arises around g = 5 along with a minor set of resonances around g = 2 similar to the spectrum of the [4Fe-4S](+) cluster in the Fe protein of Azotobacter vinelandii nitrogenase, which exists in two conformations having S = (3)/(2) and S = (1)/(2) ground spin states. The Mössbauer spectrum in the as-isolated HbRC core shows that all of the Fe is present in the form of a [4Fe-4S](2+) cluster. After reduction with sodium dithionite in the presence of light, approximately 65% of the Fe appears in the form of a [4Fe-4S](+) cluster; the remainder is in the [4Fe-4S](2+) state. Analysis of the non-heme iron content of HbRC cores indicates an antenna size of 21.6 +/- 1.1 BChl g molecules/P798. The evidence indicates that the HbRC contains a [4Fe-4S] cluster identified as F(X) that is coordinated between the PshA homodimer; in contrast to F(X) in other type I reaction centers, this [4Fe-4S] cluster exhibits an S = (3)/(2) ground spin state.

Resolution and reconstitution of a bound Fe-S protein from the photosynthetic reaction center of Heliobacterium modesticaldum.

The photosynthetic reaction center of Heliobacterium modesticaldum (HbRC) was isolated from membranes using n-dodecyl beta-D-maltopyranoside followed by sucrose density ultracentrifugation. The low-temperature EPR spectra of whole cells, isolated membranes, and HbRC complexes are similar, showing a single Fe-S cluster with g values of 2.067, 1.933, and 1.890 after illumination at 20 K, and a complex spectrum attributed to exchange interaction from two Fe-S clusters after illumination during freezing. The protein containing the Fe-S clusters was removed from the HbRC by washing it with 1.0 M NaCl and purified by ultrafiltration over a 30 kDa cutoff membrane. Analysis of the filtrate by SDS-PAGE showed a major band at approximately 8 kDa that was weakly stained with Coomassie Brilliant Blue and strongly stained with silver. The optical spectrum of the oxidized Fe-S protein shows a maximum at 410 nm, and the EPR spectrum of the reduced Fe-S protein shows a complex set of resonances similar to those found in 2[4Fe-4S] ferredoxins. The HbRC core was purified by DEAE ion-exchange chromatography and resolved by SDS-PAGE. The purified HbRC was composed of a band at ca. 40 kDa, which is identified as PshA, and several additional proteins. The isolated Fe-S protein rebinds spontaneously to purified HbRC cores, and the light-induced EPR signals of the Fe-S clusters are recovered. The flash-induced kinetics of the HbRC complex show two kinetic phases at room temperature, one with a lifetime of 75 ms and the other with a lifetime of 15 ms. The 75 ms component is lost when the Fe-S protein is removed from the HbRC complex, and it is regained when the Fe-S protein is rebound to HbRC cores. Thus, the 75 ms kinetic phase is derived from recombination of a terminal Fe-S cluster with P798(+), and the 15 ms kinetic phase is derived from recombination with an earlier acceptor, probably F(X). We suggest that the bound Fe-S protein present in the HbRC be designated PshB.

Control of electron transport in photosystem I by the iron-sulfur cluster FX in response to intra- and intersubunit interactions.

Photosystem I (PS I) is a transmembranal multisubunit complex that mediates light-induced electron transfer from plactocyanine to ferredoxin. The electron transfer proceeds from an excited chlorophyll a dimer (P700) through a chlorophyll a (A0), a phylloquinone (A1), and a [4Fe-4S] iron-sulfur cluster FX, all located on the core subunits PsaA and PsaB, to iron-sulfur clusters FA and FB, located on subunit PsaC. Earlier, it was attempted to determine the function of FX in the absence of FA/B mainly by chemical dissociation of subunit PsaC. However, not all PsaC subunits could be removed from the PS I preparations by this procedure without partially damaging FX. We therefore removed subunit PsaC by interruption of the psaC2 gene of PS I in the cyanobacterium Synechocystis sp. PCC 6803. Cells could not grow under photosynthetic conditions when subunit PsaC was deleted, yet the PsaC-deficient mutant cells grew under heterotrophic conditions and assembled the core subunits of PS I in which light-induced electron transfer from P700 to A1 occurred. The photoreduction of FX was largely inhibited, as seen from direct measurement of the extent of electron transfer from A1 to FX. From the crystal structure it can be seen that the removal of subunits PsaC, PsaD, and PsaE in the PsaC-deficient mutant resulted in the braking of salt bridges between these subunits and PsaB and PsaA and the formation of a net of two negative surface charges on PsaA/B. The potential induced on FX by these surface charges is proposed to inhibit electron transport from the quinone. In the complete PS I complex, replacement of a cysteine ligand of FX by serine in site-directed mutation C565S/D566E in subunit PsaB caused an approximately 10-fold slow down of electron transfer from the quinone to FX without much affecting the extent of this electron transfer compared with wild type. Based on these and other results, we propose that FX might have a major role in controlling electron transfer through PS I.