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.     

Insertional inactivation of the menG gene, encoding 2-phytyl-1,4-naphthoquinone methyltransferase of Synechocystis sp. PCC 6803, results in the incorporation of 2-phytyl-1,4-naphthoquinone into the A(1) site and alteration of the equilibrium constant between A(1) and F(X) in photosystem I.

A gene encoding a methyltransferase (menG) was identified in Synechocystis sp. PCC 6803 as responsible for transferring the methyl group to 2-phytyl-1,4-naphthoquinone in the biosynthetic pathway of phylloquinone, the secondary electron acceptor in photosystem I (PS I). Mass spectrometric measurements showed that targeted inactivation of the menG gene prevented the methylation step in the synthesis of phylloquinone and led to the accumulation of 2-phytyl-1,4-naphthoquinone in PS I. Growth rates of the wild-type and the menG mutant strains under photoautotrophic and photomixotrophic conditions were virtually identical. The chlorophyll a content of the menG mutant strain was similar to that of wild type when the cells were grown at a light intensity of 50 microE m(-2) s(-1) but was slightly lower when grown at 300 microE m(-2) s(-1). Chlorophyll fluorescence emission measurements at 77 K showed a larger increase in the ratio of PS II to PS I in the menG mutant strain relative to the wild type as the light intensity was elevated from 50 to 300 microE m(-2) s(-1). CW EPR studies at 34 GHz and transient EPR studies at multiple frequencies showed that the quinone radical in the menG mutant has a similar overall line width as that for the wild type, but consistent with the presence of an aromatic proton at ring position 2, the pattern of hyperfine splittings showed two lines in the low-field region. The spin polarization pattern indicated that 2-phytyl-1,4-naphthoquinone is in the same orientation as phylloquinone, and out-of-phase, spin-echo modulation spectroscopy shows the same P700(+) to Q(-) center-to-center distance as in wild-type PS I. Transient EPR studies indicated that the lifetime for forward electron transfer from Q(-) to F(X) is slowed from 290 ns in the wild type to 600 ns in the menG mutant. The redox potential of 2-phytyl-1,4-naphthoquinone is estimated to be 50 to 60 mV more oxidizing than phylloquinone in the A(1) site, which translates to a lowering of the equilibrium constant between Q(-)/Q and F(X)(-)/F(X) by a factor of ca. 10. The lifetime of the P700(+) [F(A)/F(B)](-) backreaction decreased from 80 ms in the wild type to 20 ms in the menG mutant strain and is evidence for a thermally activated, uphill electron transfer through the quinone rather than a direct charge recombination between [F(A)/F(B)](-) and P700(+).     

Temperature dependence and polarization of fluorescence from Photosystem I in the cyanobacterium Synechocystis sp. PCC 6803

To determine the fluorescence properties of cyanobacterial Photosystem I (PS I) in relatively intact systems, fluorescence emission from 20 to 295 K and polarization at 77 K have been measured from phycobilisomes-less thylakoids of Synechocystis sp. PCC 6803 and a mutant strain lacking Photosystem II (PS II). At 295 K, the fluorescence maxima are 686 nm in the wild type from PS I and PS II and at 688 nm from PS I in the mutant. This emission is characteristic of bulk antenna chlorophylls (Chls). The 690-nm fluorescence component of PS I is temperature independent. For wild-type and mutant, 725-nm fluorescence increases by a factor of at least 40 from 295 to 20 K. We model this temperature dependence assuming a small number of Chls within PS I, emitting at 725 nm, with an energy level below that of the reaction center, P700. Their excitation transfer rate to P700 decreases with decreasing temperature increasing the yield of 725-nm fluorescence.Fluorescence excitation spectra of polarized emission from low-energy Chls were measured at 77 and 295 K on the mutant lacking PS II. At excitation wavelengths longer than 715 nm, 760-nm emission is highly polarized indicating either direct excitation of the emitting Chls with no participation in excitation transfer or total alignment of the chromophores. Fluorescence at 760 nm is unpolarized for excitation wavelengths shorter than 690 nm, inferring excitation transfer between Chls before 760-nm fluorescence occurs.Our measurements illustrate that: 1) a single group of low-energy Chls (F725) of the core-like PS I complex in cyanobacteria shows a strongly temperature-dependent fluorescence and, when directly excited, nearly complete fluorescence polarization, 2) these properties are not the result of detergent-induced artifacts as we are examining intact PS I within the thylakoid membrane of S. 6803, and 3) the activation energy for excitation transfer from F725 Chls to P700 is less than that of F735 Chls in green plants; F725 Chls may act as a sink to locate excitations near P700 in PS I.Abbreviations Chl chlorophyll - BChl bacteriochlorophyll - PS Photosystem - S. 6803 Synechocystis sp. PCC 6803 - PGP potassium glycerol phosphate     

Recruitment of a foreign quinone into the A1 site of photosystem I. Consecutive forward electron transfer from A0 TO A1 to FX with anthraquinone in the A1 site as studied by transient EPR

In photosystem I (PS I), phylloquinone (PhQ) acts as a low potential electron acceptor during light-induced electron transfer (ET). The origin of the very low midpoint potential of the quinone is investigated by introducing anthraquinone (AQ) into PS I in the presence and absence of the iron-sulfur clusters. Solvent extraction and reincubation is used to obtain PS I particles containing AQ and the iron-sulfur clusters, whereas incubation of the menB rubA double mutant yields PS I with AQ in the PhQ site but no iron-sulfur clusters. Transient electron paramagnetic resonance spectroscopy is used to investigate the orientation of AQ in the binding site and the ET kinetics. The low temperature spectra suggest that the orientation of AQ in all samples is the same as that of PhQ in native PS I. In PS I containing the iron sulfur clusters, (i) the rate of forward electron transfer from the AQ*- to F(X) is found to be faster than from PhQ*- to F(X), and (ii) the spin polarization patterns provide indirect evidence that the preceding ET step from A0*- to quinone is slower than in the native system. The changes in the kinetics are in accordance with the more negative reduction midpoint potential of AQ. Moreover, a comparison of the spectra in the presence and absence of the iron-sulfur clusters suggests that the midpoint potential of AQ is more negative in the presence of F(X). The electron transfer from the AQ- to F(X) is found to be thermally activated with a lower apparent activation energy than for PhQ in native PS I. The spin polarization patterns show that the triplet character in the initial state of P700)*+AQ*- increases with temperature. This behavior is rationalized in terms of a model involving a distribution of lifetimes/redox potentials for A0 and related competition between charge recombination and forward electron transfer from the radical pair P700*+A0*-.     

Electron transfer in cyanobacterial photosystem I: II. Determination of forward electron transfer rates of site-directed mutants in a putative electron transfer pathway from A0 through A1 to FX

The directionality of electron transfer in Photosystem I (PS I) is investigated using site-directed mutations in the phylloquinone (QK) and FX binding regions of Synnechocystis sp. PCC 6803. The kinetics of forward electron transfer from the secondary acceptor A1 (phylloquinone) were measured in mutants using time-resolved optical difference spectroscopy and transient EPR spectroscopy. In whole cells and PS I complexes of the wild-type both techniques reveal a major, slow kinetic component of tau approximately 300 ns while optical data resolve an additional minor kinetic component of tau approximately 10 ns. Whole cells and PS I complexes from the W697FPsaA and S692CPsaA mutants show a significant slowing of the slow kinetic component, whereas the W677FPsaB and S672CPsaB mutants show a less significant slowing of the fast kinetic component. Transient EPR measurements at 260 K show that the slow phase is approximately 3 times slower than at room temperature. Simulations of the early time behavior of the spin polarization pattern of P700+A1-, in which the decay rate of the pattern is assumed to be negligibly small, reproduce the observed EPR spectra at 260 K during the first 100 ns following laser excitation. Thus any spin polarization from P700+FX- in this time window is very weak. From this it is concluded that the relative amplitude of the fast phase is negligible at 260 K or its rate is much less temperature-dependent than that of the slow component. Together, the results demonstrate that the slow kinetic phase results from electron transfer from QK-A to FX and that this accounts for at least 70% of the electrons. Although the assignment of the fast kinetic phase remains uncertain, it is not strongly temperature dependent and it represents a minor fraction of the electrons being transferred. All of the results point toward asymmetry in electron transfer, and indicate that forward transfer in cyanobacterial PS I is predominantly along the PsaA branch.     

The bound electron acceptors in green sulfur bacteria: resolution of the g-tensor for the F(X) iron-sulfur cluster in Chlorobium tepidum

The photosynthetic reaction center (RC) of green sulfur bacteria contains two [4Fe-4S] clusters named F(A) and F(B), by analogy with photosystem I (PS I). PS I also contains an interpolypeptide [4Fe-4S] cluster named F(X); however, spectroscopic evidence for an analogous iron-sulfur cluster in green sulfur bacteria remains equivocal. To minimize oxidative damage to the iron-sulfur clusters, we studied the sensitivity of F(A) and F(B) to molecular oxygen in whole cells of Chlorobium vibrioforme and Chlorobium tepidum and obtained highly photoactive membranes and RCs from Cb. tepidum by adjusting isolation conditions to maximize the amplitude of the F(A)(-)/F(B)(-) electron paramagnetic resonance signal at g = 1.89 (measured at 126 mW of microwave power and 14 K) relative to the P840(+) signal at g = 2.0028 (measured at 800 microW of microwave power and 14 K). In these optimized preparations we were able to differentiate F(X)(-) from F(A)(-)/F(B)(-) by their different relaxation properties. At temperatures between 4 and 9 K, isolated membranes and RCs of Cb. tepidum show a broad peak at g = 2.12 and a prominent high-field trough at g = 1.76 (measured at 126 mW of microwave power). The complete g-tensor of F(X)(-), extracted by numerical simulation, yields principal values of 2.17, 1.92, and 1. 77 and is similar to F(X) in PS I. An important difference from PS I is that because the bound cytochrome is available as a fast electron donor in Chlorobium, it is not necessary to prereduce F(A) and F(B) to photoaccumulate F(X)(-).     

Assembly of photosystem I. II. Rubredoxin is required for the in vivo assembly of F(X) in Synechococcus sp. PCC 7002 as shown by optical and EPR spectroscopy

The rubA gene was insertionally inactivated in Synechococcus sp. PCC 7002, and the properties of photosystem I complexes were characterized spectroscopically. X-band EPR spectroscopy at low temperature shows that the three terminal iron-sulfur clusters, F(X), F(A), and F(B), are missing in whole cells, thylakoids, and photosystem (PS) I complexes of the rubA mutant. The flash-induced decay kinetics of both P700(+) in the visible and A(1)- in the near-UV show that charge recombination occurs between P700(+) and A(1)- in both thylakoids and PS I complexes. The spin-polarized EPR signal at room temperature from PS I complexes also indicates that forward electron transfer does not occur beyond A(1). In agreement, the spin-polarized X-band EPR spectrum of P700(+) A(1)- at low temperature shows that an electron cycle between A(1)- and P700(+) occurs in a much larger fraction of PS I complexes than in the wild-type, wherein a relatively large fraction of the electrons promoted are irreversibly transferred to [F(A)/F(B)]. The electron spin polarization pattern shows that the orientation of phylloquinone in the PS I complexes is identical to that of the wild type, and out-of-phase, spin-echo modulation spectroscopy shows the same P700(+) to A(1)- center-to-center distance in photosystem I complexes of wild type and the rubA mutant. In contrast to the loss of F(X), F(B), and F(A), the Rieske iron-sulfur protein and the non-heme iron in photosystem II are intact. It is proposed that rubredoxin is specifically required for the assembly of the F(X) iron-sulfur cluster but that F(X) is not required for the biosynthesis of trimeric P700-A(1) cores. Since the PsaC protein requires the presence of F(X) for binding, the absence of F(A) and F(B) may be an indirect result of the absence of F(X).     

Double reduction of plastoquinone to plastoquinol in photosystem 1

In Photosystem 1 (PS1), phylloquinone (PhQ) acts as a secondary electron acceptor from chlorophyll ec(3) and also as an electron donor to the iron-sulfur cluster F(X). PS1 possesses two virtually equivalent branches of electron transfer (ET) cofactors from P(700) to F(X), and the lifetime of the semiquinone intermediate displays biphasic kinetics, reflecting ET along the two different branches. PhQ in PS1 serves only as an intermediate in ET and is not normally fully reduced to the quinol form. This is in contrast to PS2, in which plastoquinone (PQ) is doubly reduced to plastoquinol (PQH(2)) as the terminal electron acceptor. We purified PS1 particles from the menD1 mutant of Chlamydomonas reinhardtii that cannot synthesize PhQ, resulting in replacement of PhQ by PQ in the quinone-binding pocket. The magnitude of the stable flash-induced P(700)(+) signal of menD1 PS1, but not wild-type PS1, decreased during a train of laser flashes, as it was replaced by a ~30 ns back-reaction from the preceding radical pair (P(700)(+)A(0)(-)). We show that this process of photoinactivation is due to double reduction of PQ in the menD1 PS1 and have characterized the process. It is accelerated at lower pH, consistent with a rate-limiting protonation step. Moreover, a point mutation (PsaA-L722T) in the PhQ(A) site that accelerates ET to F(X) ~2-fold, likely by weakening the sole H-bond to PhQ(A), also accelerates the photoinactivation process. The addition of exogenous PhQ can restore activity to photoinactivated PS1 and confer resistance to further photoinactivation. This process also occurs with PS1 purified from the menB PhQ biosynthesis mutant of Synechocystis PCC 6803, demonstrating that it is a general phenomenon in both prokaryotic and eukaryotic PS1.     

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.     

Low-temperature electron transfer from cytochrome to the special pair in Rhodopseudomonas viridis: role of the L162 residue.

Electron transfer from the tetraheme cytochrome c to the special pair of bacteriochlorophylls (P) has been studied by flash absorption spectroscopy in reaction centers isolated from seven strains of the photosynthetic purple bacterium Rhodopseudomonas viridis, where the residue L162, located between the proximal heme c-559 and P, is Y (wild type), F, W, G, M, T, or L. Measurements were performed between 294 K and 8 K, under redox conditions in which the two high-potential hemes of the cytochrome were chemically reduced. At room temperature, the kinetics of P+ reduction include two phases in all of the strains: a dominant very fast phase (VF), and a minor fast phase (F). The VF phase has the following t(1/2): 90 ns (M), 130 ns (W), 135 ns (F), 189 ns (Y; wild type), 200 ns (G), 390 ns (L), and 430 ns (T). These data show that electron transfer is fast whatever the nature of the amino acid at position L162. The amplitudes of both phases decrease suddenly around 200 K in Y, F, and W. The effect of temperature on the extent of fast phases is different in mutants G, M, L, and T, in which electron transfer from c-559 to P+ takes place at cryogenic temperatures in a substantial fraction of the reaction centers (T, 48%; G, 38%; L, 23%, at 40 K; and M, 28%, at 60 K), producing a stable charge separated state. In these nonaromatic mutants the rate of VF electron transfer from cytochrome to P+ is nearly temperature-independent between 294 K and 8 K, remaining very fast at very low temperatures (123 ns at 60 K for M; 251 ns at 40 K for L; 190 ns at 8 K for G, and 458 ns at 8 K for T). In all cases, a decrease in amplitudes of the fast phases is paralleled by an increase in very slow reduction of P+, presumably by back-reaction with Q(A)-. The significance of these results is discussed in relation to electron transfer theories and to freezing at low temperatures of cytochrome structural reorganization.     

Resolution of low-energy chlorophylls in Photosystem I of Synechocystis sp. PCC 6803 at 77 and 295 K through fluorescence excitation anisotropy

Fluorescence excitation spectra of highly anisotropic emission from Photosystem I (PS I) were measured at 295 and 77 K on a PS II-less mutant of the cyanobacterium Synechocystis sp. PCC 6803 (S. 6803). When PS I was excited with light at wavelengths greater than 715 nm, fluorescence observed at 745 nm was highly polarized with anisotropies of 0.32 and 0.20 at 77 and 295 K, respectively. Upon excitation at shorter wavelengths, the 745-nm fluorescence had low anisotropy. The highly anisotropic emission observed at both 77 and 295 K is interpreted as evidence for low-energy chlorophylls (Chls) in cyanobacteria at room temperature. This indicates that low-energy Chls, defined as Chls with first excited singlet-state energy levels below or near that of the reaction center, P700, are not artifacts of low-temperature measurements.If the low-energy Chls are a distinct subset of Chls and a simple two-pool model describes the excitation transfer network adequately, one can take advantage of the low-energy Chls' high anisotropy to approximate their fluorescence excitation spectra. Maxima at 703 and 708 nm were calculated from 295 and 77 K data, respectively. Upper limits for the number of low-energy Chls per P700 in PS I from S. 6803 were calculated to be 8 (295 K) and 11 (77 K).Abbreviations Chl - chlorophyll - BChl - bacteriochlorophyll - LHC - light-harvesting chlorophyll - PS - Photosystem - RC - reaction center - S. 6803 - Synechocystis sp. PCC 6803     

Nitrite regulates distribution of excitation energy between the two photosystems by causing state transition.

The mechanism of distribution of absorbed excitation energy between the two photosystems in the presence of nitrite has been investigated in spinach (Spinacia oleracea L.) thylakoid membranes. Nitrite inhibited PS II activity (H(2)O --> DCPIP reaction) and enhanced PS I activity (DCPIPH(2) --> MV reaction). Nitrite decreased the F(v)/F(m) ratio measured at room temperature and increased the F(730)/F(685) ratio measured at low temperature (77 K). These results suggested that nitrite caused a decrease in the excitation energy available to PS II and transferred more energy to PS I by the mechanism of state transition. Measurement of fluorescence excitation spectra at 77 K showed that nitrite increased the absorption cross-section of PS I antenna at the expense of chlorophyll b and LHC II. Based on these observations we have suggested a role of nitrite in causing state transition.     

Functional role of vitamin K in photosystem I of the cyanobacterium Synechocystis 6803

The function of vitamin K1 in the primary electron-transfer processes of photosystem I (PS I) was investigated in the cyanobacterium Synechocystis 6803. A preparation of purified PS I was found to contain two vitamin K1's per reaction center. One vitamin K1 was removed by extraction with hexane, and further extraction using hexane including 0.3% methanol resulted in a preparation devoid of vitamin K1. The hexane-extracted PS I was functional in the photoreduction of NADP+, but the PS I after extraction using hexane-methanol was totally inactive. Activity was restored by using exogenous vitamin K1 plus the hexane extract. Vitamin K3 would not substitute. The room temperature recombination kinetics of the PS I extracted with hexane were not significantly modified. However, following the removal of both vitamin K1's, the 20-ms recombination between P-700+ and P-430- was replaced by a dominant relaxation (t 1/2 = 30 ns) due to recombination of the primary biradical P-700+ A0- and a slower component originating from the P-700 triplet. This kinetic behavior was consistent with an interruption of forward electron transfer to the acceptor A1. Addition of either vitamin K1 or vitamin K3 to such preparations resulted in restoration of the slow kinetic phase (greater than 2 ms), indicating significant competition by the two exogenous quinones for electron transfer from A0-. In the case of vitamin K3, this change in the kinetics induced by vitamin K1, suggesting successful reconstitution of the acceptor site A1. These data support the hypothesis that acceptor A1 is vitamin K1 and is a component of the electron-transfer pathway for NADP+ reduction.     

In vivo analysis of the electron transfer within photosystem I: are the two phylloquinones involved?

Electron transfer within PS I reaction centers has been analyzed in vivo in a mutant of Chlorella sorokiniana which lacks most of the PS II and of the peripheric antennae, using a new spectrophotometric technique with a time resolution of approximately 5 ns. Absorption changes associated with the oxidation of semiphylloquinone (acceptor A(1)(-)) have been characterized in the 371-545 nm spectral range. The oxidation of A(1)(-) and the reduction of an iron-sulfur cluster (F(X), F(A)F(B)) is monitored by an absorption decrease at 377 nm (semiphylloquinone absorption band) and by the decrease of two positive absorption bands around 480 and 515 nm, respectively, very likely associated with a local electrochromic shift induced by A(1)(-) on a carotenoid molecule localized in its vicinity. A(1)(-) undergoes a two-phase oxidation of about equal amplitude with half-times of approximately 18 and approximately 160 ns, respectively. Two hypotheses are proposed to interpret these data: (1) Photosystem I reaction centers are present under two conformational states which differ by the reoxidation rate of A(1)(-). (2) The two phylloquinones corresponding to the two branches of the PS I heterodimer are involved in the electron transfer. The similar amplitude of the two phases implies that the rates of electron transfer from P700 to each of the phylloquinones are about equal. The two different rate constants measured for A(1)(-) oxidation suggests some asymmetry in the relative position of the two phylloquinones with respect to F(X).     

ATP consumption by uncoupled mitochondria activates sarcolemmal K(ATP) channels in cardiac myocytes

We tested whether close coupling exists between mitochondria and sarcolemma by monitoring whole cell ATP-sensitive K(+) (K(ATP)) current (I(K,ATP)) as an index of subsarcolemmal energy state during mitochondrial perturbation. In rabbit ventricular myocytes, either pinacidil or the mitochondrial uncoupler dinitrophenol (DNP), which rapidly switches mitochondria from net ATP synthesis to net ATP hydrolysis, had little immediate effect on I(K,ATP). In contrast, in the presence of pinacidil, exposure to 100 microM DNP rapidly activated I(K,ATP) with complex kinetics consisting of a quick rise [time constant of I(K,ATP) increase (tau) = 0.13 +/- 0.01 min], an early partial recovery (tau = 0.43 +/- 0.04 min), and then a more gradual increase. This DNP-induced activation of I(K,ATP) was reversible and accompanied by mitochondrial flavoprotein oxidation. The F(1)F(0)-ATPase inhibitor oligomycin abolished the DNP-induced activation of I(K,ATP). The initial rapid rise in I(K,ATP) was blunted by atractyloside (an adenine nucleotide translocator inhibitor), leaving only a slow increase (tau = 0.66 +/- 0.17 min, P < 0.01). 2,4-Dinitrofluorobenzene (a creatine kinase inhibitor) slowed both the rapid rise (tau = 0.20 +/- 0.01 min, P < 0.05) and the subsequent declining phase (tau = 0.88 +/- 0.19 min, P < 0.05). From single K(ATP) channel recordings, we excluded a direct effect of DNP on K(ATP) channels. Taken together, these results indicate that rapid changes in F(1)F(0)-ATPase function dramatically alter subsarcolemmal energy charge, as reported by pinacidil-primed K(ATP) channel activity, revealing cross-talk between mitochondria and sarcolemma. The effects of mitochondrial ATP hydrolysis on sarcolemmal K(ATP) channels can be rationalized by reversal of F(1)F(0)-ATPase and the facilitation of coupling by the creatine kinase system.     

A new fluorescence band F689 in photosystem II revealed by picosecond analysis at 4-77 K: Function of two terminal energy sinks F689 and F695 in PS II

We performed picosecond time-resolved fluorescence spectroscopy in spinach photosystem II (PS II) particles at 4, 40, and 77 K and identified a new fluorescence band, F689. F689 was identified in addition to the well-known F685 and F695 bands in both analyses of decay-associated spectra and global Gaussian deconvolution of time-resolved spectra. Its fast decay suggests the energy transfer directly from F689 to the reaction center chlorophyll P680. The contribution of F689, which increases only at low temperature, explains the unusually broad and variable bandwidth of F695 at low temperature. Global analysis revealed the three types of excitation energy transfer/dissipation processes: (1) energy transfer from the peripheral antenna to the three core antenna bands F685, F689, and F695 with time constants of 29 and 171 ps at 77 and 4 K, respectively; (2) between the three core bands (0.18 and 0.82 ns); and (3) the decays of F689 (0.69 and 3.02 ns) and F695 (2.18 and 4.37 ns). The retardations of these energy transfer rates and the slow F689 decay rate produced the strong blue shift of the PS II fluorescence upon the cooling below 77 K.     

Conformational changes of cholesteryl palmitoleate in the crystal structure at low temperature

At 123 K, crystals of cholesteryl cis-9-hexadecenoate (cholesteryl palmitoleate, C45H74O2) are monoclinic, space group P2(1) with cell dimensions a = 12.917(7), b = 8.910(5), c = 34.04(1) A, beta = 94.95(7) degrees [lambda(CuK alpha) = 1.5424 A] having two independent molecules (A and B) per unit cell. The crystal structure has been determined from 6178 reflections with sin theta/lambda less than or equal to 0.56 A-1, of which 3406 gave [F] greater than 3 sigma. Structure refinement by alternating cycles of Fourier syntheses and block diagonal least squares gave R = 0.24 for all reflections, R = 0.13 for reflections [F] greater than 3 sigma. At 123 K, the crystal structure consists of closely packed layers very similar to those at 295 K. However, there are major conformational differences in the layer interface region, which affect the ester chain of molecule B and the C(17) tail of molecule A. Although the electron density is diffuse in this region, the B-chain, which is bent, appears to be ordered at 123 K and has a different conformation from the disordered B-chains at 295 K. The change in the A-tail, which is twisted at 123 K and extended at 295 K, is very similar to that which occurs in two of the molecules when anhydrous cholesterol undergoes phase transition. Measurements of the unit cell dimensions at twelve temperatures (295 K to 123 K) indicate that the major changes in the crystal structure of cholesteryl palmitoleate occur in a 10 K range near 173 K.     

A new fluorescence band F689 in photosystem II revealed by picosecond analysis at 4-77 K: function of two terminal energy sinks F689 and F695 in PS II

We performed picosecond time-resolved fluorescence spectroscopy in spinach photosystem II (PS II) particles at 4, 40, and 77 K and identified a new fluorescence band, F689. F689 was identified in addition to the well-known F685 and F695 bands in both analyses of decay-associated spectra and global Gaussian deconvolution of time-resolved spectra. Its fast decay suggests the energy transfer directly from F689 to the reaction center chlorophyll P680. The contribution of F689, which increases only at low temperature, explains the unusually broad and variable bandwidth of F695 at low temperature. Global analysis revealed the three types of excitation energy transfer/dissipation processes: (1) energy transfer from the peripheral antenna to the three core antenna bands F685, F689, and F695 with time constants of 29 and 171 ps at 77 and 4 K, respectively; (2) between the three core bands (0.18 and 0.82 ns); and (3) the decays of F689 (0.69 and 3.02 ns) and F695 (2.18 and 4.37 ns). The retardations of these energy transfer rates and the slow F689 decay rate produced the strong blue shift of the PS II fluorescence upon the cooling below 77 K.     

Decay kinetics and quantum yields of fluorescence in photosystem I from Synechococcus elongatus with P700 in the reduced and oxidized state: are the kinetics of excited state decay trap-limited or transfer-limited?

Transfer and trapping of excitation energy in photosystem I (PS I) trimers isolated from Synechococcus elongatus have been studied by an approach combining fluorescence induction experiments with picosecond time-resolved fluorescence measurements, both at room temperature (RT) and at low temperature (5 K). Special attention was paid to the influence of the oxidation state of the primary electron donor P700. A fluorescence induction effect has been observed, showing a approximately 12% increase in fluorescence quantum yield upon P700 oxidation at RT, whereas at temperatures below 160 K oxidation of P700 leads to a decrease in fluorescence quantum yield ( approximately 50% at 5 K). The fluorescence quantum yield for open PS I (with P700 reduced) at 5 K is increased by approximately 20-fold and that for closed PS I (with P700 oxidized) is increased by approximately 10-fold, as compared to RT. Picosecond fluorescence decay kinetics at RT reveal a difference in lifetime of the main decay component: 34 +/- 1 ps for open PS I and 37 +/- 1 ps for closed PS I. At 5 K the fluorescence yield is mainly associated with long-lived components (lifetimes of 401 ps and 1.5 ns in closed PS I and of 377 ps, 1.3 ns, and 4.1 ns in samples containing approximately 50% open and 50% closed PS I). The spectra associated with energy transfer and the steady-state emission spectra suggest that the excitation energy is not completely thermally equilibrated over the core-antenna-RC complex before being trapped. Structure-based modeling indicates that the so-called red antenna pigments (A708 and A720, i.e., those with absorption maxima at 708 nm and 720 nm, respectively) play a decisive role in the observed fluorescence kinetics. The A720 are preferentially located at the periphery of the PS I core-antenna-RC complex; the A708 must essentially connect the A720 to the reaction center. The excited-state decay kinetics turn out to be neither purely trap limited nor purely transfer (to the trap) limited, but seem to be rather balanced.