Influence of Histidine-198 of the D1 subunit on the properties of the primary electron donor, P680, of photosystem II in Thermosynechococcus elongatus

The influence of the histidine axial ligand to the P_D1 chlorophyll of photosystem II on the redox potential and spectroscopic properties of the primary electron donor, P_680, was investigated in mutant oxygen-evolving photosystem II (PSII) complexes purified from the thermophilic cyanobacterium Thermosynechococcus elongatus. To achieve this aim, a mutagenesis system was developed in which the psbA₁ and psbA₂ genes encoding D1 were deleted from a His-tagged CP43 strain (to generate strain WT^?) and mutations D1-H198A and D1-H198Q were introduced into the remaining psbA₃ gene. The O₂-evolving activity of His-tagged PSII isolated from WT^? was found to be significantly higher than that measured from His-tagged PSII isolated from WT in which psbA₁ is expected to be the dominantly expressed form. PSII purified from both the D1-H198A and D1-H198Q mutants exhibited oxygen-evolving activity as high as that from WT^?. Surprisingly, a variety of kinetic and spectroscopic measurements revealed that the D1-H198A and D1-H198Q mutations had little effect on the redox and spectroscopic properties of P₆₈₀, in contrast to the earlier results from the analysis of the equivalent mutants constructed in Synechocystis sp. PCC 6803 [B.A. Diner, E. Schlodder, P.J. Nixon, W.J. Coleman, F. Rappaport, J. Lavergne, W.F. Vermaas, D.A. Chisholm, Site-directed mutations at D1-His198 and D2-His197 of photosystem II in Synechocystis PCC 6803: sites of primary charge separation and cation and triplet stabilization, Biochemistry 40 (2001) 9265-9281]. We conclude that the nature of the axial ligand to P_D1 is not an important determinant of the redox and spectroscopic properties of P₆₈₀ in T. elongatus.     

Cationic state distribution over the chlorophyll d-containing PD1/PD2 pair in photosystem II

Most of the chlorophyll (Chl) cofactors in photosystem II (PSII) from Acaryochloris marina are Chld, although a few Chla molecules are also present. To evaluate the possibility that Chla may participate in the P_D1/P_D2 Chl pair in PSII from A. marina, the P_D1^?+/P_D2^?+ charge ratio was investigated using the PSII crystal structure analyzed at 1.9-Å resolution, while considering all possibilities for the Chld-containing P_D1/P_D2 pair, i.e., Chld/Chld, Chla/Chld, and Chld/Chla pairs. Chld/Chld and Chla/Chld pairs resulted in a large P_D1^?+ population relative to P_D2^?+, as identified in Chla/Chla homodimer pairs in PSII from other species, e.g., Thermosynechococcus elongatus PSII. However, the Chld/Chla pair possessed a P_D1^?+/P_D2^?+ ratio of approximately 50/50, which is in contrast to previous spectroscopic studies on A. marina PSII. The present results strongly exclude the possibility that the Chld/Chla pair serves as P_D1/P_D2 in A. marina PSII. This article is part of a Special Issue entitled: Photosynthesis Research for Sustainability: from Natural to Artificial.     

Function of two β-carotenes near the D1 and D2 proteins in photosystem II dimers

The antenna proteins in photosystem II (PSII) not only promote energy transfer to the photosynthetic reaction center (RC) but provide also an efficient cation sink to re-reduce chlorophyll a if the electron transfer (ET) from the Mn-cluster is inhibited. Using the newest PSII dimer crystal structure (3.0 Å resolution), in which 11 β-carotene molecules (Car) and 14 lipids are visible in the PSII monomer, we calculated the redox potentials (E_m) of one-electron oxidation for all Car (E_m(Car)) by solving the Poisson-Boltzmann equation. In each PSII monomer, the D1 protein harbors a previously unlocated Car (Car_D1) in van der Waals contact with the chlorin ring of Chl_Z(D1). Each Car_D1 in the PSII dimer complex is located in the interface between the D1 and CP47 subunits, together with another four Car of the other PSII monomer and several lipid molecules. The proximity of Car bridging between Car_D1 and plastoquinone/Q_A may imply a direct charge recombination of Car⁺Q_A⁻. The calculated E_m(Car_D1) and E_m(Chl_Z(D1)) are, respectively, 83 and 126 mV higher than E_m(Car_D2) and E_m(Chl_Z(D2)), which could explain why Car_D2⁺ and Chl_Z(D2)⁺ are observed rather than the corresponding Car_D1⁺ and Chl_Z(D1)⁺.     

Using site-directed mutagenesis to probe the role of the D2 carotenoid in the secondary electron-transfer pathway of photosystem II

Secondary electron transfer in photosystem II (PSII), which occurs when water oxidation is inhibited, involves redox-active carotenoids (Car), as well as chlorophylls (Chl), and cytochrome b ₅₅₉ (Cyt b ₅₅₉), and is believed to play a role in photoprotection. Car_D2 may be the initial point of secondary electron transfer because it is the closest cofactor to both P₆₈₀, the initial oxidant, and to Cyt b ₅₅₉, the terminal secondary electron donor within PSII. In order to characterize the role of Car_D2 and to determine the effects of perturbing Car_D2 on both the electron-transfer events and on the identity of the redox-active cofactors, it is necessary to vary the properties of Car_D2 selectively without affecting the ten other Car per PSII. To this end, site-directed mutations around the binding pocket of Car_D2 (D2-G47W, D2-G47F, and D2-T50F) have been generated in Synechocystis sp. PCC 6803. Characterization by near-IR and EPR spectroscopy provides the first experimental evidence that Car_D2 is one of the redox-active carotenoids in PSII. There is a specific perturbation of the Car^?+ near-IR spectrum in all three mutated PSII samples, allowing the assignment of the spectral signature of Car _D2 ^?+ ; Car _D2 ^?+ exhibits a near-IR peak at 980 nm and is the predominant secondary donor oxidized in a charge separation at low temperature in ferricyanide-treated wild-type PSII. The yield of secondary donor radicals is substantially decreased in PSII complexes isolated from each mutant. In addition, the kinetics of radical formation are altered in the mutated PSII samples. These results are consistent with oxidation of Car_D2 being the initial step in secondary electron transfer. Furthermore, normal light levels during mutant cell growth perturb the shape of the Chl^?+ near-IR absorption peak and generate a dark-stable radical observable in the EPR spectra, indicating a higher susceptibility to photodamage further linking the secondary electron-transfer pathway to photoprotection.     

Altered structure of the Mn4Ca cluster in the oxygen-evolving complex of photosystem II by a histidine ligand mutation

The effect of replacing a histidine ligand on the properties of the oxygen-evolving complex (OEC) and the structure of the Mn₄Ca cluster in Photosystem II (PSII) is studied by x-ray absorption spectroscopy using PSII core complexes from the Synechocystis sp. PCC 6803 D1 polypeptide mutant H332E. In the x-ray crystallographic structures of PSII, D1-His³³² has been assigned as a direct ligand of a manganese ion, and the mutation of this histidine ligand to glutamate has been reported to prevent the advancement of the OEC beyond the S₂Yz^• intermediate state. The manganese K-edge (1s core electron to 4p) absorption spectrum of D1-H332E shifts to a lower energy compared with that of the native WT samples, suggesting that the electronic structure of the manganese cluster is affected by the presence of the additional negative charge on the OEC of the mutant. The extended x-ray absorption spectrum shows that the geometric structure of the cluster is altered substantially from that of the native WT state, resulting in an elongation of manganese-ligand and manganese-manganese interactions in the mutant. The strontium-H332E mutant, in which calcium is substituted by strontium, confirms that strontium (calcium) is a part of the altered cluster. The structural perturbations caused by the D1-H332E mutation are much larger than those produced by any biochemical treatment or mutation examined previously with x-ray absorption spectroscopy. The substantial structural changes provide an explanation not only for the altered properties of the D1-H332E mutant but also the importance of the histidine ligand for proper assembly of the Mn₄Ca cluster.     

Radiative and non-radiative charge recombination pathways in Photosystem II studied by thermoluminescence and chlorophyll fluorescence in the cyanobacterium Synechocystis 6803

The mechanism of charge recombination was studied in Photosystem II by using flash induced chlorophyll fluorescence and thermoluminescence measurements. The experiments were performed in intact cells of the cyanobacterium Synechocystis 6803 in which the redox properties of the primary pheophytin electron acceptor, Phe, the primary electron donor, P₆₈₀, and the first quinone electron acceptor, Q_A, were modified. In the D1Gln130Glu or D1His198Ala mutants, which shift the free energy of the primary radical pair to more positive values, charge recombination from the S₂Q_A⁻ and S₂Q_B⁻ states was accelerated relative to the wild type as shown by the faster decay of chlorophyll fluorescence yield, and the downshifted peak temperature of the thermoluminescence Q and B bands. The opposite effect, i.e. strong stabilization of charge recombination from both the S₂Q_A⁻ and S₂Q_B⁻ states was observed in the D1Gln130Leu or D1His198Lys mutants, which shift the free energy level of the primary radical pair to more negative values, as shown by the retarded decay of flash induced chlorophyll fluorescence and upshifted thermoluminescence peak temperatures. Importantly, these mutations caused a drastic change in the intensity of thermoluminescence, manifested by 8- and 22-fold increase in the D1Gln130Leu and D1His198Lys mutants, respectively, as well as by a 4- and 2.5-fold decrease in the D1Gln130Glu and D1His198Ala mutants, relative to the wild type, respectively. In the presence of the electron transport inhibitor bromoxynil, which decreases the redox potential of Q_A/Q_A⁻ relative to that observed in the presence of DCMU, charge recombination from the S₂Q_A⁻ state was accelerated in the wild type and all mutant strains. Our data confirm that in PSII the dominant pathway of charge recombination goes through the P₆₈₀⁺Phe⁻ radical pair. This indirect recombination is branched into radiative and non-radiative pathways, which proceed via repopulation of P₆₈₀^* from ¹[P₆₈₀⁺Ph⁻] and direct recombination of the ³[P₆₈₀⁺Ph⁻] and ¹[P₆₈₀⁺Ph⁻] radical states, respectively. An additional non-radiative pathway involves direct recombination of P₆₈₀⁺Q_A⁻. The yield of these charge recombination pathways is affected by the free energy gaps between the Photosystem II electron transfer components in a complex way: Increase of ΔG(P₆₈₀^* ↔ P₆₈₀⁺Phe⁻) decreases the yield of the indirect radiative pathway (in the 22-0.2% range). On the other hand, increase of ΔG(P₆₈₀⁺Phe⁻ ↔ P₆₈₀⁺Q_A⁻) increases the yield of the direct pathway (in the 2-50% range) and decreases the yield of the indirect non-radiative pathway (in the 97-37% range).     

Neutralization of the Charge on Asp369 of Na+,K+-ATPase Triggers E1 ? E2 Conformational Changes

This work investigates the role of charge of the phosphorylated aspartate, Asp³⁶⁹, of Na⁺,K⁺-ATPase on E₁ ↔ E₂ conformational changes. Wild type (porcine α₁/His₁₀-β₁), D369N/D369A/D369E, and T212A mutants were expressed in Pichia pastoris, labeled with fluorescein 5′-isothiocyanate (FITC), and purified. Conformational changes of wild type and mutant proteins were analyzed using fluorescein fluorescence (Karlish, S. J. (1980) J. Bioenerg. Biomembr. 12, 111–136). One central finding is that the D369N/D369A mutants are strongly stabilized in E₂ compared with wild type and D369E or T212A mutants. Stabilization of E₂(Rb) is detected by a reduced K_0.5Rb for the Rb⁺-induced E₁ ↔ E₂(2Rb) transition. The mechanism involves a greatly reduced rate of E₂(2Rb) → E₁Na with no effect on E₁ → E₂(2Rb). Lowering the pH from 7.5 to 5.5 strongly stabilizes wild type in E₂ but affects the D369N mutant only weakly. Thus, this “Bohr” effect of pH on E₁ ↔ E₂ is due largely to protonation of Asp³⁶⁹. Two novel effects of phosphate and vanadate were observed with the D369N/D369A mutants as follows. (a) E₁ → E₂·P is induced by phosphate without Mg²⁺ ions by contrast with wild type, which requires Mg²⁺. (b) Both phosphate and vanadate induce rapid E₁ → E₂ transitions compared with slow rates for the wild type. With reference to crystal structures of Ca²⁺-ATPase and Na⁺,K⁺-ATPase, negatively charged Asp³⁶⁹ favors disengagement of the A domain from N and P domains (E₁), whereas the neutral D369N/D369A mutants favor association of the A domain (TGES sequence) with P and N domains (E₂). Changes in charge interactions of Asp³⁶⁹ may play an important role in triggering E₁P(3Na) ↔ E₂P and E₂(2K) → E₁Na transitions in native Na⁺,K⁺-ATPase.     

Influence of histidine-198 of the D1 subunit on the properties of the primary electron donor, P680, of photosystem II in Thermosynechococcus elongatus

The influence of the histidine axial ligand to the PD1 chlorophyll of photosystem II on the redox potential and spectroscopic properties of the primary electron donor, P680, was investigated in mutant oxygen-evolving photosystem II (PSII) complexes purified from the thermophilic cyanobacterium Thermosynechococcus elongatus. To achieve this aim, a mutagenesis system was developed in which the psbA1 and psbA2 genes encoding D1 were deleted from a His-tagged CP43 strain (to generate strain WT*) and mutations D1-H198A and D1-H198Q were introduced into the remaining psbA3 gene. The O2-evolving activity of His-tagged PSII isolated from WT* was found to be significantly higher than that measured from His-tagged PSII isolated from WT in which psbA1 is expected to be the dominantly expressed form. PSII purified from both the D1-H198A and D1-H198Q mutants exhibited oxygen-evolving activity as high as that from WT*. Surprisingly, a variety of kinetic and spectroscopic measurements revealed that the D1-H198A and D1-H198Q mutations had little effect on the redox and spectroscopic properties of P680, in contrast to the earlier results from the analysis of the equivalent mutants constructed in Synechocystis sp. PCC 6803 [B.A. Diner, E. Schlodder, P.J. Nixon, W.J. Coleman, F. Rappaport, J. Lavergne, W.F. Vermaas, D.A. Chisholm, Site-directed mutations at D1-His198 and D2-His197 of photosystem II in Synechocystis PCC 6803: sites of primary charge separation and cation and triplet stabilization, Biochemistry 40 (2001) 9265-9281]. We conclude that the nature of the axial ligand to PD1 is not an important determinant of the redox and spectroscopic properties of P680 in T. elongatus.     

Improving the Activity and Stability of GL-7-ACA Acylase CA130 by Site-Directed Mutagenesis

In the present study, glutaryl-7-amino cephalosporanic acid acylase from Pseudomonas sp. strain 130 (CA130) was mutated to improve its enzymatic activity and stability. Based on the crystal structure of CA130, two series of amino acid residues, one from those directly involved in catalytic function and another from those putatively involved in surface charge, were selected as targets for site-directed mutagenesis. In the first series of experiments, several key residues in the substrate-binding pocket were substituted, and the genes were expressed in Escherichia coli for activity screening. Two of the mutants constructed, Y151αF and Q50βN, showed two- to threefold-increased catalytic efficiency (k_cat/K_m) compared to wild-type CA130. Their K_m values were decreased by ca. 50%, and the k_cat values increased to 14.4 and 16.9 s⁻¹, respectively. The ability of these mutants to hydrolyze adipoyl 6-amino penicillinic acid was also improved. In the second series of mutagenesis, several mutants with enhanced stabilities were identified. Among them, R121βA and K198βA had a 30 to 58% longer half-life than wild-type CA130, and K198βA and D286βA showed an alkaline shift of optimal pH by about 1.0 to 2.0 pH units. To construct an engineered enzyme with the properties of both increased activity and stability, the double mutant Q50βN/K198βA was expressed. This enzyme was purified and immobilized for catalytic analysis. The immobilized mutant enzyme showed a 34.2% increase in specific activity compared to the immobilized wild-type CA130.     

Benzene-1,2-dithiolate-induced assembly of reactive iridium fragments into tetranuclear octahydride complexes

The tetrametallic compound [Ir₄(μ-1,2-S₂C₆H₄)₂(μ-H)₂H₆(PⁱPr₃)₄(NCMe)] (1) has been obtained by treatment of the reactive cationic complex [IrH₂(PⁱPr₃)(NCMe)₃]BF₄ with the benzene-1,2-dithiolate anion. In the solid state, this tetrametallic compound exhibits an irregular nearly planar metal skeleton with the two dithiolate anions bridging the four metal centres from the same side of the tetrametallic plane. Even though all iridium atoms coordinate one PⁱPr₃ ligand, two bridging S atoms and, at least, two hydrides, they show different electronic and coordination environments. This unusual structure is maintained in solution, even after substitution of the labile acetonitrile ligand by other Lewis bases such as ethylene or carbon monoxide.     

Energetics and proton release in photosystem II from Thermosynechococcus elongatus with a D1 protein encoded by either the psbA2 or psbA3 gene

In the cyanobacterium Thermosynechococcus elongatus, there are three psbA genes coding for the Photosystem II (PSII) D1 subunit that interacts with most of the main cofactors involved in the electron transfers. Recently, the 3D crystal structures of both PsbA2-PSII and PsbA3-PSII have been solved [Nakajima et al., J. Biol. Chem. 298 (2022) 102668.]. It was proposed that the loss of one hydrogen bond of Phe_D1 due to the D1-Y147F exchange in PsbA2-PSII resulted in a more negative E_m of Phe_D1 in PsbA2-PSII when compared to PsbA3-PSII. In addition, the loss of two water molecules in the Cl-1 channel was attributed to the D1-P173M substitution in PsbA2-PSII. This exchange, by narrowing the Cl-1 proton channel, could be at the origin of a slowing down of the proton release. Here, we have continued the characterization of PsbA2-PSII by measuring the thermoluminescence from the S₂Q_A⁻/DCMU charge recombination and by measuring proton release kinetics using time-resolved absorption changes of the dye bromocresol purple. It was found that i) the E_m of Phe_D1^–/Phe_D1 was decreased by ∼30 mV in PsbA2-PSII when compared to PsbA3-PSII and ii) the kinetics of the proton release into the bulk was significantly slowed down in PsbA2-PSII in the S₂Tyr_Z^• to S₃Tyr_Z and S₃Tyr_Z^• → (S₃Tyr_Z^•)’ transitions. This slowing down was partially reversed by the PsbA2/M173P mutation and induced by the PsbA3/P173M mutation thus confirming a role of the D1-173 residue in the egress of protons trough the Cl-1 channel.     

Spectroscopic properties of reaction center pigments in photosystem II core complexes: revision of the multimer model

Absorbance difference spectra associated with the light-induced formation of functional states in photosystem II core complexes from Thermosynechococcus elongatus and Synechocystis sp. PCC 6803 (e.g., ) are described quantitatively in the framework of exciton theory. In addition, effects are analyzed of site-directed mutations of D1-His¹⁹⁸, the axial ligand of the special-pair chlorophyll P_D1, and D1-Thr¹⁷⁹, an amino-acid residue nearest to the accessory chlorophyll Chl_D1, on the spectral properties of the reaction center pigments. Using pigment transition energies (site energies) determined previously from independent experiments on D1-D2-cytb559 complexes, good agreement between calculated and experimental spectra is obtained. The only difference in site energies of the reaction center pigments in D1-D2-cytb559 and photosystem II core complexes concerns Chl_D1. Compared to isolated reaction centers, the site energy of Chl_D1 is red-shifted by 4 nm and less inhomogeneously distributed in core complexes. The site energies cause primary electron transfer at cryogenic temperatures to be initiated by an excited state that is strongly localized on Chl_D1 rather than from a delocalized state as assumed in the previously described multimer model. This result is consistent with earlier experimental data on special-pair mutants and with our previous calculations on D1-D2-cytb559 complexes. The calculations show that at 5 K the lowest excited state of the reaction center is lower by ∼10 nm than the low-energy exciton state of the two special-pair chlorophylls P_D1 and P_D2 which form an excitonic dimer. The experimental temperature dependence of the wild-type difference spectra can only be understood in this model if temperature-dependent site energies are assumed for Chl_D1 and P_D1, reducing the above energy gap from 10 to 6 nm upon increasing the temperature from 5 to 300 K. At physiological temperature, there are considerable contributions from all pigments to the equilibrated excited state P*. The contribution of Chl_D1 is twice that of P_D1 at ambient temperature, making it likely that the primary charge separation will be initiated by Chl_D1 under these conditions. The calculations of absorbance difference spectra provide independent evidence that after primary electron transfer the hole stabilizes at P_D1, and that the physiologically dangerous charge recombination triplets, which may form under light stress, equilibrate between Chl_D1 and P_D1.     

Energy dependent changes in the cytochromes of the mitochondrial respiratory chain

In intact mitochondria a stoichiometric coupling exists between cytochrome a₃ and the hydrolysis of adenosine triphosphate (ATP). In each case the modification of one cytochrome a₃ (measured as a spectral change) is coupled to the hydrolysis of one ATP molecule. When both cytochromes a₃ and a are reduced the measured equilibrium constant is 0.06 m^?1 but this constant is 10³ M^?1 when both cytochromes are oxidized. When the sixth ligand for cytochrome a₃ is an externally added ligand (HCN, H₂S, CO, NO) the equilibrium constant is different for each ligand, suggesting that the ATP induced modification is of the fifth ligand but that it is energetically dependent on the chemical nature of the sixth ligand. The measured half-reduction potentials for cytochromes a₃ and b_T are dependent on the concentrations of added ATP, adenosine diphosphate (ADP), and orthophosphate. The relationship is consistent with a ligand exchange mechanism in which the ligand on the cytochrome is dependent on the phosphate potential ($\text{ATP}\text{ADP}$ × P_i). The equilibrium constants obtained by the ligand exchange treatment of the E_m values for cytochrome a₃ are consistent with those obtained by direct measurement of the equilibrium constants for the spectrally measured changes.     

Structure and electrochemistry of the bridging-ligand mono-substituted diruthenium compound, [Ru2(II,III)(O2CCH3)3(admpym)(Cl)(MeOH)] (Hadmpym=2-amino-4,6-dimethylpyrimidine)

The ligand substitution reaction of Ru₂(O₂CCH₃)₄Cl with 2-amino-4,6-dimethylpyrimidine (Hadmpym) under gentle refluxing conditions in methanol led to the formation of a bridging-ligand mono-substituted compound, [Ru₂(O₂CCH₃)₃(admpym)(Cl)(MeOH)] (1). Compound 1 crystallized in monoclinic space group P2₁/n (no. 14) with a=8.3074(8) Å, b=12.3722(8) Å, c=18.913(1) Å, β=95.559(3)°, V=1934.8(3) ų, and Z=4. Temperature dependence of the magnetic susceptibility of 1 revealed it to be in a spin ground state S=3/2 arising from the electronic configuration of σ²π⁴δ²(δ*π*)³. Compound 1 undergoes three metal-centered redox reactions in electrochemistry: E_1/2 ^(ox)=+0.72 V (I_a/I_c<1, ΔE_p=0.17 V); E_1/2 ^(1,red)=−0.65 V (I_a/I_c≈1, ΔE_p=0.10 V); and E_1/2 ^(2,red)=−1.80 V (I_a/I_c?1, ΔE_p=0.16 V). Then, the redox species produced by electrolysis were characterized by spectroscopic studies.     

pH dependent stabilization of S2QA − and S2QB − charge pairs studied by thermoluminescence

The pH dependence of emission peak temperature and decay time of thermoluminescence arising from S₂Q_B ^– and S₂Q_A ^– recombinations demonstrates that a stabilization of S₂Q_B ^– occurs at low pH whereas stabilization of S₂Q_A ^– occurs at high pH. Based on comparative analysis of thermoluminescence parameters of the two types of recombination, we suggest that in the pH range between 5.3 and 7.5, E_m(S₂/S₁) and E_m(Q_A/Q_A ^–) are constant, but E_m(Q_B/Q_B ^–) gradually increases with decreasing pH, while in the pH range between 7.5 and 8.5, an unusual change occurs on S₂Q_A ^– charge pair, which is interpreted as either a decrease in E_m(S₂/S₁) or an increase in E_m(Q_A/Q_A ^–).     

Stabilisation of the iminooxo tautomer of 1-methylcytosine in Pt complexes: Role of the ancillary ligands

Reaction of cis-[L₂Pt(μ-OH)]₂(NO₃)₂ (L = PPh₃) with 1-methylthymine (1-MeTy), in DMF, leads to the formation of the mononuclear neutral adduct cis-L₂Pt{1-MeTy(-H)}(ONO₂) (1) whose structure in the solid state has been obtained by single crystal X-ray diffraction. The deprotonated nucleobase is bounded at the N(3) site, with the pyrimidinic ring almost perpendicular (78.0(1)°) to the metal coordination plane. The fourth ligand is a monodentate nitrate group. Addition of 1 equiv. of 1-methylcytosine (1-MeCy) causes the immediate replacement of the nitrato ligand to form the cationic complex cis-[L₂Pt{1-MeTy(-H)}(1-MeCy,N³)]NO₃ (2) in which both the nucleobases are N(3)-platinated. In CD₂Cl₂ at −40 °C 2 exists as a mixture of two conformers (2:1 molar ratio) arising from the different orientation of the nucleobases with respect to the metal coordination plane.In solution of DMSO, DMF or chlorinated solvents, 2 slowly converts into the isomer cis-[L₂Pt{1-MeTy(-H)}(1-MeCy,N⁴)]NO₃ (3), containing the tautomeric form of the cytosine stabilised through the coordination at the N(4) atom, as a mixture of conformers whose relative abundance is dependent on the solvent and the temperature.In contrast, the analogous complex of 2 containing the phosphine PMe₃, cis-[(PMe₃)₂Pt{1-MeTy(-H)}(1-MeCy,N³)]NO₃ (4), also isolated as pure compound, in DMSO solution slowly rearranges leading to the elimination of the neutral 1-MeTy, with the formation of the dinuclear cytosinate complex cis-[(PMe₃)₂Pt{1-MeCy(-H),N³N⁴}]₂(NO₃)₂, previously characterised by us.     

Electronic absorption and MCD spectra for octacyanometallate complexes M(CN)8, M=Mo(IV), W(IV), n=4 and Mo(V), W(V), n=3

Electronic absorption and 8.0 T magnetic circular dichroism (MCD) spectra are reported for M(CN)₈ ⁴⁻, M=Mo(IV) and W(IV), in aqueous solution and M(CN)₈ ³⁻, M=Mo(V) and W(V), in acetonitrile solutions. In addition some absorption and MCD spectra are reported for the M(CN)₈ ³⁻ ions embedded in thin poly methyl methacrylate (PMMA) plastic films at temperatures from 295 to 10 K. The temperature dependence of the MCD spectra confirms the presence of C terms. The solution and PMMA spectra for the both Mo and W complexes in either the IV or V oxidation states are remarkably similar to each other for the same oxidation state and are interpreted within a D_2d structural framework for the isotropic environment. The weak bands below 3.0 μm⁻¹ (1 μm⁻¹=10⁴ cm⁻¹) for the M(IV) complexes are assigned as metal-localized ligand field (LF) transitions. LF transitions are also suggested for weaker unresolved absorption between 3.0 and 3.6 μm⁻¹ for the M(V) ions. The intense bands above 3.6 μm⁻¹ for M(IV) and 4.6 μm⁻¹ for M(V) complexes are interpreted as metal to ligand charge transfer (MLCT) from the metal b₁(x²−y²) HOMO to CN⁻-based π * orbitals. The prominent intense bands observed below 4.5 μm⁻¹for the M(V) complexes are assigned as ligand to metal charge transfer (LMCT) from occupied non-bonding or weakly π bonding CN⁻ orbitals to the half-filled b₁(x²−y²) HOMO.     

Theoretical studies on the conformations of aldohexopyranose pentaacetates

The net charges on various atoms of aldohexopyranose pentaacetates were computed by using the MO-LCAO method of Del Re for σ-charges and the Hückel MO method for π-charges. The potential and free energies of sixteen aldohexopyranose pentaacetates in the C1(D) and 1C(D) conformations were estimated. Minimization of the energies of these conformations was studied by suitably tilting the axial CC and CO bonds. As with the free sugars, considerable release of strain is achieved when tilts of 4.5 and 2° are given to the axial CH₂OAc and the axial OAc groups, respectively, involved in the Hassel—Ottar effect in the 1C(D) conformations. In the case of C1(D) conformations, the ideal models have the minimum energy even when the acetate groups are involved in syn-axial interactions, indicating that strain induced by axial acetate groups is less than that of axial hydroxyl groups. The calculated free-energies agree well with the experimental values after adding a value of 0.9 kcal.mole^-1 for the anomeric effect of the acetoxyl group. The free-energy calculations also predict that α-D-idohexopyranose pentaacetate and α-D-altrose pentaacetate favour the C1(D) conformation and β-D-idose pentaacetate a C1?1C equilibrium in solution, in agreement with n.m.r. studies.     

Active transport of chloride by the giant neuron of the Aplysia abdominal ganglion

Internal chloride activity, aⁱ _Cl, and membrane potential, E_m, were measured simultaneously in 120 R2 giant neurons of Aplysia californica. aⁱ _Cl was 37.0 ± 0.8 mM, E_m was -49.3 ± 0.4 mv, and E _Cl calculated using the Nernst equation was -56.2 ± 0.5 mv. Such values were maintained for as long as 6 hr of continuous recording in untreated neurons. Cooling to 1°–4°C caused aⁱ _Cl to increase at such a rate that 30–80 min after cooling began, E _Cl equalled E_m. The two then remained equal for as long as 6 hr. Rewarming to 20°C caused aⁱ _Cl to decline, and E _Cl became more negative than E_m once again. Exposure to 100 mM K⁺-artificial seawater caused a rapid increase of aⁱ _Cl. Upon return to control seawater, aⁱ _Cl declined despite an unfavorable electrochemical gradient and returned to its control values. Therefore, we conclude that chloride is actively transported out of this neuron. The effects of ouabain and 2,4-dinitrophenol were consistent with a partial inhibitory effect. Chloride permeability calculated from net chloride flux using the constant field equation ranged from 4.0 to 36 x 10^-8 cm/sec.     

Synthesis, spectroscopy, tandem mass spectrometry, and electrochemistry of the linearly bridged μ-{trans-1,4-bis[2-(4-pyridyl)ethenyl]-benzene}-{Ru3O(CH3COO)6(py)2}2 cluster

The novel polynuclear [{Ru₃O(CH₃COO)₆(py)₂}₂(BPEB)](PF₆)₂ species containing the linear bridging trans-1,4-bis[2-(4-pyridyl)ethenyl]-benzene ligand (BPEB) was synthesized and its structural characterization carried out by means of positive ion electrospray (ESI-MS) and tandem mass (ESI-MS/MS) spectrometry, as well as by ¹H NMR spectroscopy. The doubly charged cation [{Ru₃O(CH₃COO)₆(py)₂}₂(BPEB)]²⁺ was detected in the ESI-MS mass spectrum as a multiple-component isotopomeric ionic cluster centered at m/z 974, which ion abundance and m/z distribution matched perfectly the isotopic pattern calculated for this multiple isotope Ru₃-containing ion. The tandem mass spectrum of [{Ru₃O(CH₃COO)₆(py)₂}₂(BPEB)]²⁺ provided a structural diagnostic dissociation behavior, on the basis of the characteristic charge splitting and sequential ligand loss steps. The cyclic voltammograms of the complex exhibited a quasi-reversible multistep redox behavior, displaying three waves at 1.14, 0.08, and −1.21 V ascribed to the [Ru₃O]^2+/1+/0/1− processes and two waves at −1.56 and −1.78 V ascribed to the BPEB^0/1−/2− redox processes which are also observed in the free ligand, at −1.48 and 1.61 V, respectively. In spite of the conducting nature of the bridging ligand, the electrochemical and spectroelectrochemical results indicated a weak electronic coupling between the triangular cluster centers.