Properties of photochemical reaction centers purified from Rhodopseudomonas gelatinosa

Reaction centers were isolated from a carotenoidless mutant of Rhodopseudomonas gelatinosa by hydroxyapatite chromatography of purified chromatophores treated with lauryl dimethyl amine oxide. Absorption spectra and spectra of light-induced absorbance changes are similar to those of reaction centers from Rhodopseudomonas sphaeroides. The ratio of absorbance at 280 nm to that at 799 nm was 1.8 in the purest preparations. The extinction coefficient at the 799 nm absorption maximum was estimated to be 305 ± 20 mM^?1 · cm^?1. The molecular weight based on protein and chromophore assays was found to be 1.5 · 10⁵; the reaction center protein accounted for 6% of the total membrane protein. These reaction centers contained no cytochrome and showed just two components of apparent molecular weights 33 000 and 25 000 in polyacrylamide gel electrophoresis. The chromatophores contained 42 molecules of antenna bacteriochlorophyll for each reaction center.     

Picosecond spectroscopy of the charge separation in reaction centers of Chloroflexus aurantiacus with selective excitation of the primary electron donor

Absorbance changes in the picosecond region were studied in isolated reaction centers of the green photosynthetic bacterium Chloroflexus aurantiacus upon selective excitation of the primary electron donor, P, at 870 nm. The results indicate that the first observed state is an excited state of P (P1) which appears to transfer an electron to a bacteriochlorophyll a molecule absorbing at 812 nm (B₁) in 10 ± 2 ps as indicated by a bleaching at this wavelength. This reaction is followed by a rapid electron transfer (3 ± 1 ps) from B₁⁻ to bacteriopheophytin a, so that the fraction of reaction centers in the state P⁺B₁⁻ remains small during the experiment. An apparent bleaching at 925 nm is ascribed to stimulated emission from excited P, which emission disappears upon formation of P⁺. The difference between these time constants for electron transfer and those observed for the same reactions in reaction centers of the purple photosynthetic bacterium Rhodopseudomonas (Rhodobacter) sphaeroides is discussed in terms of the energy difference between P1 and P⁺B₁⁻, which appears to be larger for C. aurantiacus.     

Regulation of photosystem stoichiometry,chlorophyll a and chlorophyll b content and relation to chloroplast ultrastructure

The structural-functional organization of higher plant chloroplasts has been investigated in relation to the particular light conditions during plant growth. (1) Light intensity variations during growth caused changes in the $\text{Chl}\text{a}\text{Chl}\text{b}$ ratio, in the light-saturated uncoupled rates of electron transport to a Hill oxidant and in the distribution of the chloroplast volume between the membrane and stroma phases. (2) Light quality differences during growth had an effect on the PS II/PS I reaction center ratio and on the chloroplast membrane phase differentiation into grana and stroma thylakoids. Plants grown under far-red-enriched (680–710 nm) illumination contained higher (20–25%) amounts of PS II and simultaneously lower (20–25%) amounts of PS I reaction centers. They also showed a higher grana density along with thicker grana stacks in their chloroplasts. (3) The size of the light-harvesting antenna pool of PS II centers was estimated from the fluorescence time course of 3-(3′,4′-dichlorophenyl)-1,1-dimethylurea-poisoned chloroplasts and was found to be fairly constant (±10%) in spite of the variable PS II/PS I reaction center ratio. The results are compatible with the hypothesis that the structural entities of grana facilitated the centralization and relative concentration increase of a certain group of PS II reaction centers.     

Catalytic properties of enzymes from Erwinia carotovora involved in transamination of phenylpyruvate

K _m for L-phenylalanine, L-glutamic acid, L-aspartic acid, and the corresponding keto acids were calculated, as well as V _max was measured for the following pairs of substrates: L-phenylalanine-2-ketoglutarate, L-phenylalanine-oxaloacetate, L-glutamic acid-phenylpyruvate, and L-aspartic acid-phenylpyruvate for aminotransferases PAT1, PAT2, and PAT3 from Erwinia carotovora catalyzing transamination of phenylpyruvate. The ping-pong bi-bi mechanism was shown for the studied aminotransferases. The substrate inhibition (K _s) of PAT3 with 2-ketoglutarate and oxaloacetate was 10.23 ± 3.20 and 3.73 ± 1.99 mM, respectively. It was shown that L-β-(N-benzylamino)alanine was a competitive inhibitor with respect to L-phenylalanine for PAT1 (K _i = 0.32 ± 0.07 mM, K _m = 0.45 ± 0.1 mM, V _max = 11. 6 ± 0.4 U/mg) at 25 mM concentration of 2-ketoglutarate in the reaction medium. L-β-(N-methylamino)alanine is a noncompetitive inhibitor with respect to L-phenylalanine for PAT3 (K _I = 138.4 ± 95.4 mM, K _m = 13.7 ±3.9 mM, V _max = 18.6 ± 4.1 U/mg) at 2 mM concentration of 2-ketoglutarate in the reaction medium. L-stereo isomers of nonprotein analogues of aromatic amino acids were studied as substrates for PAT1, PAT2, and PAT3. L-β-(2-Br-phenyl)alanine, L-β-(4-Br-phenyl)alanine, L-β-(2-F-phenyl)alanine, and L-(2-F)tryptophan were good substrates for all three aminotransferases; L-α-methyl-β-(2-Br-phenyl)alanine and L-O-benzyltyrosine were substrates only for PAT3; L-β-(4-F-phenyl)alanine was a substrate for PAT1 and PAT3. Thus, these analogues of aromatic amino acids can be stereoselectively synthesized using the studied aminotransferases in the presence of the corresponding keto acids.     

Molar extinction coefficients and other properties of an improved reaction center preparation from Rhodopseudomonas viridis

Reaction centers have been purified from chromatophores of Rhodopseudomonas viridis by treatment with lauryl dimethyl amine oxide followed by hydroxyapatite chromatography and precipitation with ammonium sulfate. The absorption spectrum at low temperature shows bands at 531 and 543 nm, assigned to two molecules of bacteriopheophytin b. The 600 nm band of bacteriochlorophyll b is resolved at low temperature into components at 601 and 606.5 nm. At room temperature the light-induced difference spectrum shows a negative band centered at 615 nm, where the absorption spectrum shows only a weak shoulder adjacent to the 600 nm band. The fluorescence spectrum shows a band at 1000 nm and no fluorescence corresponding to the 830 nm absorption band. Two molecules of cytochrome 558 and three of cytochrome 552 accompany each reaction center. The differential extinction coefficient (reduced minus oxidized) of cytochrome 558 at 558 nm was estimated as 20 ± 2 mM^?1 · cm^?1 through a coupled reaction with equine cytochrome c. The extinction coefficient of reaction centers at 960 nm was determined to be 123 ± 25 mM^?1 · cm^?1 by measuring the light-induced bleaching of P-960 and the coupled oxidation of cytochrome 558. The corresponding extinction coefficient at 830 nm is 300 ± 65 mM^?1 · cm^?1. The absorbance ratio $\text{a}{}_{\mathrm{<mtext>280</mtext><mtext>nm</mtext>}}\text{a}{}_{\mathrm{<mtext>830</mtext><mtext>nm</mtext>}}$ in our preparations was 2.1, and there was 190 kg protein per mol of reaction centers. Sodium dodecyl sulfate-polyacrylamide gel electrophoresis showed three major components of apparent molecular weights 31 000, 37 000 and 41 000.     

The effect of pressure on the electrical breakdown in the membranes of Valonia utricularis

The interpretation of electrical breakdown in terms of electro-mechanical instabilities, predicts that the breakdown potential should decrease with increasing cell turgor pressure.Experiments were conducted to test this hypothesis on cells of Valonia utricularis over a turgor pressure range of 0.5 · 10⁵–5.0 · 10⁵ N/m². Electrical breakdown was measured using intracellular electrodes and 500 μs current pulses. The pressure was monitored by an intracellular micropipette pressure transducer. The results obtained show a linear decrease in the critical breakdown potential with pressure. The effective compressive modulus of the cell membrane, γ, is calculated from the slope of this line to 69 ± 10 · 10⁵N/m² (average value of seven measurements). This is consistent with the theoretical prediction of the electromechanical model using our previously determined values of the elastic modulus of the membrane.A theoretical analysis is given of the effects of pressure on the breakdown. This includes also considerations of the indirect effect of pressure on the membrane via stretching of the cell wall with a possible coupling of such strains to the cell membrane. The results and analysis presented allow us to conclude on the basis of the experimentally determined breakdown P.D. of 959 mV that the region of membrane where electrical breakdown occurs is a dielectric with one of the following combinations of parameters: (A) a thickness δ = 7–9 nm with a dielectric constant ? = >10, e.g. a hydrated protein spanning the whole membrane. (B) δ = 4–5 nm with ? = 3–8, e.g. a lipoprotein of lipid bilayer dimensions. (C) δ ≈ 2 nm with ? = 2–3, e.g. a half lipid bilayer.If we assume that the breakdown P.D. of the tonoplast and plasmalemma are identical, that is 480 mV, then there is only one reasonable choice for the membrane thickness and the dielectric constant: δ = 2nm, ? = 3–8, e.g. a (lipo-)proteinaceous module facing a half lipid bilayer.     

Formation and decay of radical-pair state P+I− in Chloroflexus aurantiacus reaction centers

We have examined the room temperature kinetics of the absorption changes associated with the formation of state P⁺I⁻ (P⁺BPh⁻) and its subsequent decay to state P⁺Q⁻_A in reaction centers from Chloroflexus aurantiacus. Our data, acquired using 30-ps excitation flashes, strongly suggest that formation of P⁺I⁻ (P⁺BPh⁻) takes longer in Chloroflexus than in reaction centers from Rhodopseudomonas sphaeroides. The reduction of the photoactive bacteriopheophytin (BPh) could take as long as 13 ps. Absorption changes different from those due to P⁺I⁻ are observed early in the excitation flash, but the detailed identity of the transient remains unclear. We also find that the kinetics observed subsequent to P⁺I⁻ formation differ with detection wavelength. The time constant measured in the anion band (I⁻) at 655 nm is 324 ± 20 ps and probably reflects the rate of electron transfer from I⁻ (BPh⁻) to Q_A. However, the kinetics measured in the BPh ground-state absorption bands are slightly longer: 365 ± 19 and 367 ± 21 ps at 538 and 760 nm, respectively. At 810 nm, a wavelength normally associated with the monomeric bacteriochlorophyll (BChl) in the Chloroflexus reaction center, a slightly faster (281 ± 19 ps) time constant is observed. This detection-wavelength dependence of the kinetics is similar to that observed recently in Rps. sphaeroides reaction centers. Comparison of these results suggests that the kinetics observed in the ground-state absorption bands of the BPhs and BChls in Chloroflexus may contain contributions from readjustments of the pigments and/or protein in response to the charge separation process.     

Action of tannin on cellular membranes: Novel insights from concerted studies on lipid bilayers and native cells

Hydrolyzable tannin (3,6-bis-O-digalloyl-1,2,4-tri-O-galloyl-β-d-glucose) has a dual effect on the cell membrane: (1) it binds to a plasmalemmal protein of the Chara corallina cell (C₅₀ = 2.7 ± 0.3 μM) and (2) it forms ionic channels in the lipid membrane. Based on these facts, a molecular model for the interaction of tannins with the cell membrane is proposed. The model suggests that the molecules of hydrolyzable tannin bind electrostatically to the outer groups of the membrane protein responsible for the Ca²⁺-dependent chloride current and blocks it. Some tannin molecules penetrate into the hydrophobic region of the membrane, and when a particular concentration is reached, they form ion-conducting structures selective toward Cl^?.     

Serotoninergic agonists and antagonists are the modulators of α1-Adrenoceptor activity in rat brain cortical membranes

The effects of activation and inhibition of serotonin receptors by serotonin (5-HT) and mianserin on the specific nonselective α₁-antagonist [³H]prazosine binding in rat cerebral cortex membranes was studied. It was shown that the ligand-receptor interaction of α₁-adrenoceptors corresponded to the model suggesting the presence of one pool of receptors and the binding of two ligand molecules to the receptor. The parameters of [³H]prazosine binding to α₁-adrenoceptors were as follows: K _d =1.85 ± 0.16 nM, B _max = 31.1 ± 0.3 fmol/mg protein, n = 2. In case of activation of 5HT-receptors by serotonin, the character of ligand binding was different: two pools of receptors were detected with the parameters K _d1 = 0.61 ± 0.04, K _d2 = 3.82 ± 0.15 nM, B _m1 = 6.6 ± 0.7, B _m2 = 25.6 ± 0.4 fmol/mg protein, n = 2. The sensitivity of the high-affinity pool increased threefold and the sensitivity of the low-affinity pool decreased twofold as compared to the control. The value of maximal reaction (B _max) did not change. In the case of inhibition of 5HT-receptors by mianserin, radioactive ligand is bound to α₁-adrenoceptors according to the same model as in the control conditions. The affinity of α₁-adrenoceptors to [³H]prazosine decreases twofold and the concentration increases (K _d = 3.97 ± 0.12 nM, B _max = 40.0 ± 0.5 fmol/mg protein). The data suggest that α₁-adrenoceptors in rat cerebral cortex exist as a dimer. The modulatory effects of serotonin and mianserin on the specific binding of [³H]prazosine to α₁-adrenoceptors was detected, manifesting itself as changes in the binding parameters and in the general character of ligand-receptor interactions.     

Supramolecular organization of chlorosomes (chlorobium vesicles) and of their membrane attachment sites in Chlorobium Limicola

The photosynthetic green bacterium Chlorobium limicola 6230 has been examined by freeze-fracture electron microscopy to investigate the size, form, distribution and supramolecular architecture of its chlorosomes (chlorobium vesicles) as well as the chlorosome attachment sites on the cytoplasmic membrane. The oblong chlorosomes that underlie the cytoplasmic membrane show a considerable variation in size from about 40 × 70 nm to 100 × 260 nm and exhibit no particular orientation. The chlorosome core, which appears to be hydrophobic in nature, contains between 10 and 30 rod-shaped elements (approx. 10 nm in diameter) surrounded by an unetchable matrix. The rod elements are closely packed and extend the full length of the chlorosome. Separating the chlorosome core from the cytoplasm is a approx. 3 nm thick lipid-like envelope layer, which exhibits no substructure. A 5–6 nm thick, crystalline baseplate connects the chlorosome to the cytoplasmic membrane. The ridges of the baseplate lattice make an angle of between 40° and 60° with the longitudinal axis of the chlorosome and have a repeating distance of approx. 6 nm. In addition, each ridge exhibits a granular substructure with a periodicity of approx. 3.3 nm. The cytoplasmic membrane regions adjacent to the baseplates are enriched in large (greater than 9 nm) intramembrane particles, most of which belong to approx. 10 nm and approx. 12.5 nm particle size categories. Each chlorosome attachment site contains between 20 and 30 very large (greater than 12.0 nm diameter) intramembrane particles.The following interpretive model of a chlorosome is discussed in terms of biophysical, biochemical and structural information reported by others: it is proposed that the bacteriochlorophyll c (BChl c; chlorobium chlorophyll) is located in the rod elements of the core and that it is complexed with specific proteins. The cytoplasm-associated envelope layer is depicted as consisting of a monolayer of galactosyl diacylglycerol molecules. BChl a-protein complexes in a planar lattice configuration most likely make up the crystalline baseplate. The greater than 12-nm particles in the chlorosome attachment sites of the cytoplasmic membrane, finally, may correspond to complexes containing a reaction center and non-crystalline light-harvesting BChl a. The crystalline nature of the baseplate is consistent with the notion that it serves two functions: besides transferring excitation energy to the reaction centers it could also function as a distributor of this energy amongst the reaction centers.     

Structural study of modified fibrinogen microcrystals by electron microscopy

The same molecular shape of proteolytically modified fibrinogen has been identified in two different crystalline forms: orthorhombic P2₁2₁2 with a = 44.7(± 1.7) nm, b = 11.8(± 1.0) nm, c = 3.8 nm and monoclinic P2₁ with a = 17.7(± 0.6) nm, b = 16.2(± 1.0) nm, c = 4.8 nm and β = 95 °. The shape of the molecule is more detailed than has been reported. It has the commonly accepted elongated form 44.5(± 1.5) nm long with a 2-fold axis perpendicular to the major axis of the molecule. Each end domain shows a distinctive substructure and has an asymmetry similar to that reported by Williams (1981) and Mosesson et al. (1981) from single molecule observations. The ends are flattened, having overall dimensions of approximately 12 nm × 9 nm × 4 nm. The major difference between this model and previous models is the absence of a central nodule. There are, however, two small additional protein-dense regions at 5.0 nm from the centre of the rod connecting the two ends. A rough estimate of the relative heights of the different parts of the molecule was obtained using the two different projections of the molecule obtained from the two different crystalline forms. The molecule appears to be slightly bent at the centre, as predicted by Doolittle (1977).     

Photoreactions of bacteriopheophytins and bacteriochlorophylls in reaction centers of Rhodopseudomonas sphaeroides and Chloroflexus aurantiacus

A comparison of spectral properties of reaction centers from Chloroflexus aurantiacus and Rhodopseudomonas sphaeroides (R-26) is reported. Treatment of reaction centers from Rps. sphaeroides with NaBH₄ leads to a decrease of the dipole strength of the 800-nm band by factor of approx. 1.75-1.95 and to the formation of new bacteriopheophytin, BPh-715, which is almost completely removed during the purification of reaction centers. The modification of the reaction centers does not change the quantum yield of P photooxidation and the spectrum of BPh-545 (H₁) photoreduction which includes the changing of the 800-nm band. This implies the preservation of the photoactive chain P-B₁-H₁-Q_A (where B₁ is the bacteriochlorophyll (BChl)-800 molecule situated between P and H₁) and the modification of the second BChl-800 (B₂). The preparation of modified reaction centers is a mixture of at least three types of reaction centers with different contents of B₂ and of the second BPh (H₂). Some of the reaction centers (5-25%) contain the original B₂ and H₂ molecules (type I). In the CD spectrum of modified reaction centers a decrease of the 800-nm band and the appearance of a positive band at 765 nm is observed. This spectrum is similar to the CD spectrum of Chloroflexus reaction centers containing 3 BPh's and 3 BChl's. This implies that in some (approx. 40%) of the modified Rps. sphaeroides reaction centers (type II) B₂ has been replaced by BPh a which interacts with H₂. Probably some of the modified reaction centers (approx. 40%) have lost both B₂ and H₂ (type III). The modification of reaction centers leads to a considerable decrease of the CD bands at 800 (+) nm and 810 (−) nm and to a decrease of the absorbance changes near 800 nm in the difference absorption spectrum of the oxidation of P. The data are interpreted in terms of the interaction between P and B₁ molecules which gives two transitions at 790-800 and 810 nm with different orientations in modified Rps. sphaeroides as well as in Chloroflexus reaction centers. Similar transitions are observed for the interaction between P and B₂. The spectral analysis shows the existence of two chains P-B₁-H₁, and P-B₂-H₂ in which the distances between the centers of molecules are 1.3 nm or less.     

Evidence for cross-talk between atrial natriuretic peptide and nitric oxide receptors

Guanylyl cyclases (GCs), a ubiquitous family of enzymes that metabolize GTP to cyclic GMP (cGMP), are traditionally divided into membrane-bound forms (GC-A-G) that are activated by peptides and cytosolic forms that are activated by nitric oxide (NO) and carbon monoxide. However, recent data has shown that NO activated GC’s (NOGC) also may be associated with membranes. In the present study, interactions of guanylyl cyclase A (GC-A), a caveolae-associated, membrane-bound, homodimer activated by atrial natriuretic peptide (ANP), with NOGC, a heme-containing heterodimer (α/β) β1 isoform of the β subunit of NOGC (NOGCβ1) was specifically focused. NOGCβ1 co-localized with GC-A and caveolin on the membrane in human kidney (HK-2) cells. Interaction of GC-A with NOGCβ1 was found using immunoprecipitations. In a second set of experiments, the possibility that NOGCβ1 regulates signaling by GC-A in HK-2 cells was explored. ANP-stimulated membrane guanylyl cyclase activity (0.05 ± 0.006 pmol/mg protein/5 min; P < 0.01) and intra cellular GMP (18.1 ± 3.4 vs. 1.2 ± 0.5 pmol/mg protein; P < 0.01) were reduced in cells in which NOGCβ1 abundance was reduced using specific siRNA to NOGCβ1. On the other hand, ANP-stimulated cGMP formation was increased in cells transiently transfected with NOGCβ1 (530.2 ± 141.4 vs. 26.1 ± 13.6 pmol/mg protein; P < 0.01). siRNA to NOGCβ1 attenuated inhibition of basolateral Na/K ATPase activity by ANP (192 ± 22 vs. 92 ± 9 nmol phosphate/mg protein/min; P < 0.05). In summary, the results show that NOGCβ1 and GC-A interact and that NOGCβ1 regulates ANP signaling in HK-2 cells. The results raise the novel possibility of cross-talk between NOGC and GC-A signaling pathways in membrane caveolae.     

Orientation of the chromophores in the reaction center of Rhodopseudomonas viridis. Comparison of low-temperature linear dichroism spectra with a model derived from X-ray crystallography

Linear dichroism (LD) and absorption (A) spectra of reaction centers from Rhodopseudomonas viridis included in the native chromatophores or reconstituted in planar aggregates have been recorded at 10 K. The samples were oriented in squeezed polyacrylamide gels and the primary donor P was in the reduced or (chemically) oxidized state. The LD spectra of reaction centers in these two states are in favor of a dimeric model of P in which excitonic coupling between the two non-parallel Q_Y transitions leads to a main transition at 990 nm (parallel to the membrane plane) and another one of smaller oscillator strength at 850 nm (tilted at approx. 60° out of the membrane plane). These assignments are in close agreement with the ones proposed in a previous LD study at room temperature (Paillotin, G., Verméglio, A. and Breton, J. (1979) Biochim. Biophys. Acta 545, 249–264). The main Q_X excitonic component of P has a broad absorption peaking at 620 nm and it corresponds to dipoles exhibiting the same orientation as those responsible for the 850 nm transition. On the basis of the present LD study and of CD data of chemically oxidized-minus-reduced reaction centers, we proposed that the minor Q_X excitonic component of P is oriented close to the membrane plane and absorbs around 660 nm. The two monomeric bacteriochlorophylls exhibit a positive LD for both their Q_Y transitions (unresolved at 834 nm) and their Q_X transitions (resolved at 600 and 607 nm), indicating that the planes of these molecules are only slightly tilted out of the membrane plane. The two bacteriopheophytins exhibit strong negative LD with identical LD/A values for their Q_Y transitions (resolved at 790 and 805 nm) and small positive LD for their Q_X transitions (resolved at 534 and 544 nm), demonstrating that these two molecules are strongly tilted out of the membrane plane with each of the Q_Y transitions tilted at approx. 50° out of that plane. A comparison of these LD data with the structural model derived from X-ray crystallography (Deisenhofer, J., Epp, O., Miki, K., Huber, R. and Michel, H. (1984) J. Mol. Biol. 180, 385–398) clearly suggests that a good agreement exists between the results of the two techniques under the following conditions: (i) the C-2 symmetry axis of the reaction center runs along the membrane normal; (ii) excitonic coupling is present only in the primary donor special pair; and (iii) the direction of the optical transitions of the monomeric bacteriochlorophylls and of the bacteriopheophytins is not significantly perturbed by the interactions among the pigments. In addition, a carotenoid is detected in the isolated reaction center with an orientation rather perpendicular to the C-2 symmetry axis. Finally, a comparison of these data with similar ones obtained on the bacteriochlorophyll a-containing reaction center of Rhodopseudomonas sphaeroides 241 points towards a geometrical arrangement of the chromophores which is indistinguishable from the one observed in the reaction center of Rps. viridis.     

Evidence for structural distinction between PS IIα and PS IIβ reaction centers

The technique of (γ-ray) radiation inactivation has been used to estimate the functional sizes of the PS II centers (PS II_α and PS II_β) responsible for the biphasicity of the fluorescence induction curve from DCMU-inhibited spinach chloroplasts. It is found that the size of PS II_α (266 ± 5 kDa) is almost twice as large as that of PS II_β (135 ± 5 kDa). The result clearly indicates that the two types of PS II are structurally distinct and furthermore, the difference exists in the reaction center per se. Implications on the organization of PS II reaction centers are discussed.     

Solution and solid state behavior of Co2+, Ni2+ and Zn2+ tosylaminoacidate systems: Crystal and molecular structure of bis(N-tosylglycinato)tetraaquocobalt(II) and bis(N-tosyl-β-alaninato)tetraaquozinc(II) complexes

The interactions between N-tosylamino acids and cobalt(II), nickel(II) and zinc(II) ions in aqueous solution and in the solid state have been investigated. From concentrated aqueous solutions, compounds of general formula [M(II)(N-tosylaminoacidato)₂(H₂O)₄](M = Co(II), Ni(II) and N-tosylaminoacidato = N-tosylglycinate (Tsgly^?), N-tosyl-α- and -β-alaninate (Ts-α- and Ts-β-ala^?); M = Zn(II) and N-tosylaminoacidate = Tsgly^?, Ts-β-ala^?) and [Zn(II)(N- tosylaminoacidato)₂(H₂O)₂] were isolated and characterized by means of thermogravimetric, electronic and infrared spectra. For two of them: [Co(Tsgly)₂(H₂O)₄](I) and [Zn(Ts-β-ala)₂(H₂O)₄](II) the crystal and molecular structures were also determined. Both compounds crystallize in the monoclinic space group P2₁/c, with two formula units in a cell of dimensions: a = 13.007(6), b = 5.036(2), c = 18.925(7) Å, β = 102.33(3)° for (I) and a = 14.173(6), b = 5.469(2), c = 17.701(7) Å, β = 106.63(3)° for (II). The structures were solved by the heavy-atom method and refined by least-squares calculations to R = 0.031 and 0.064 for (I) and (II) respectively. The cobalt and zinc atoms lie in the centers of symmetry, each bonded to two amino- acid molecules through a carboxylic oxygen atom and four water molecules in a slightly tetragonally distorted octahedral geometry. The second carboxylic oxygen atom is not involved in metal coordination. Electronic and X ray-powder spectra suggest that the tetrahydrate complexes of Co²⁺, Ni²⁺ and Zn²⁺ ions of the same amino acids are isomorphous and isostructural. No coordinative interactions between ligand and metal ions were found in aqueous solution on varying the pH values before hydroxide precipitation.     

Reaction of cythchrome c with one-electron redox reagents. I. Reduction of ferricytochrome c by the hydrated electron produced by pulse radiolysis

Pulse radiolysis-kinetic spectrometry has been used to investigate the reaction of hydrated electrons with ferricytochrome c in dilute aqueous solution at pH 6.5–7.0. Time resolutions from 2·10^?7 to 1 s were employed. Transient spectra from 320 to 580 nm were characterized with a wavelength resolution of ±0.5 nm. 1 In neutral salt-free solution, k(ferricytochrome c+e^?_aq)=(6.0±0.9)·10¹⁰ M^?1·s^?1 and k(ferricytochrome c+H)=(1.2±0.2)·10¹⁰ M^?1·s^?1. The reaction of ferricytochrome c with hydrated electrons is sensitive to ionic strength; in 0.1 M NaClO₄, k(ferricytochrome c+e^?_aq)=(2.4±0.4)·10¹⁰ M^?1·s^?1. In contrast, k(ferricytochrome c+H) is insensitive to ionic strength. Time resolution of three spectral stages has been accomplished. The primary spectrum is the first observable spectrum detectable after irradiation and is formed in a second-order process. Its rate of formation is indisting-uishable from the rate of disappearance of the electron spectrum. The secondary spectrum is generated in a true first order intramolecular process, k(p→s)=(1.2±0.1)·10⁵ s^?1. The tertiary spectrum is also generated in a true first-order process, k(s→t)=(1.3±0.2)·10² s^?1. The specific rates of both transformations are independent of the wavelength of measurement. The tertiary spectrum, observable 50 ms after initial reaction and remaining unchanged thereafter for at least 1 s, shows that relaxed ferrocytochrome c is the only detectable product. This product is not autoxidizable, as expected for native reduced enzyme. It is more probable that the intramolecular changes responsible for the p→s and s→t spectral transformations involve the influence of conformational relaxation of ferrocytochrome c upon electronic energy states then that they are intramolecular transmission of reducing equivalents from primary sites of electron attachment.     

Time-resolved picosecond fluorescence spectra of the antenna chlorophylls in Chlorella vulgaris. Resolution of Photosystem I fluorescence

The time-resolved fluorescence emission and excitation spectra of Chlorella vulgaris cells have been measured by single-photon timing with picosecond resolution. In a three-exponential analysis the time-resolved excitation spectra recorded at 685 and 706 nm emission wavelength with closed PS II reaction centers show large variations of the preexponential factors of the different decay components as a function of wavelength. At λ_em = 685 nm the major contribution to the fluorescence decay originates from two components with life-times of 2.1–2.4 and 1.2–1.3 ns. A short-lived component with life-times of 0.1–0.16 ns of relatively small amplitude is also found. When the emission is detected at 706 nm, the short-lived component with a life-time of less than 0.1 ns predominates. Time-resolved emission spectra using λ_exc = 630 or λ_exc = 652 nm show a spectral peak of the two longer-lived components at about 680–685 nm, whereas the fast component is red-shifted as compared to the others and shows a maximum at about 690 nm. The emission spectrum observed upon excitation at 696 nm with closed PS II reaction centers shows a large increase in the amplitude of the fast component with a lifetime of 80–100 ps as compared to that at 630 nm excitation. At almost open Photosystem II (PS II) reaction centers (F₀), the life-time of the fast component decreased from 150–160 ps at 682 nm to less than 100 ps at 720 nm emission wavelength. We conclude that at least two pigment pools contribute to the fast component. One is attributed to PS II and the other to Photosystem I (PS I). They have life-times of approx. 180 ps and 80 ps, respectively. The 80 ps (PS I) contribution has a spectral maximum slightly below 700 nm, whereas the 180 ps (PS II) spectrum peaks at 680–685 nm. The spectra of the middle decay component τ_m and its sensitivity to inhibitors of PS II suggest that this component is not preferentially related to LHC II but arises mainly from Chl a pigments probably associated with a second type of PS II centers. The amplitudes of the fast (180 ps, PS II) component and the long-lived decay show an opposite dependence on the state of the PS II centers and confirm our earlier conclusion that the contribution of PS II to the fast component probably disappears at the F_max state (Haehnel W., Holzwarth, A.R. and Wendler, J. (1983) Photochem. Photobiol. 34, 435–443). Our data are discussed in terms of α,β-heterogeneity in PS II centers.     

Temperature and detection-wavelength dependence of the picosecond electron-transfer kinetics measured in Rhodopseudomonas sphaeroides reaction centers. Resolution of new spectral and kinetic components in the primary charge-separation process

We have examined the temperature dependence of the rate of electron transfer to ubiquinone from the bacteriopheophytin (BPh) that serves as an initial electron acceptor (I) in reaction centers of Rhodopseudomonas sphaeroides. The kinetics were measured from the decay of the 665-nm absorption band of the reduced BPh (BPh⁻ or I⁻) and from the recovery of the BPh band at 545 nm, following excitation of reaction centers in polyvinyl alcohol films with 30-ps flashes. The measured time constant decreases from 229 ± 25 ps at 295 K to 97 ± 8 ps near 100 K and then remains constant down to 5 K. The temperature dependence of the kinetics can be rationalized on the assumption that the reaction results in changes in the frequencies of numerous low-energy nuclear (vibrational) modes of the electron carriers and/or the protein. The kinetics measured in the absorption bands near 765 and 795 nm show essentially the same temperature dependence as those measured at 545 or 665 nm, but the time constants vary with detection wavelength. The time constant measured in the 795-nm region (70 ± 10 ps at 5 and 76 K) is shorter than that seen in the absorption bands of the BPh; the time constant measured at 758 nm is longer. Time constants measured with reaction centers in solution at 288 K also vary with the detection wavelength. These results can be explained on the assumption that the absorption changes measured at some wavelengths reflect nuclear relaxations rather than electron transfer. The absorption changes at 795 nm probably reflect a relaxation of the bacteriochlorophyll molecules that are near neighbors of the BPh and the primary electron donor (P). Those near 530 and 755 nm probably are due to the second BPh molecule, which does not appear to undergo oxidation or reduction.     

Stabilities,solubility, and kinetics and mechanism for formation and hydrolysis of some palladium(II)and platinum(II) iodo complexes in aqueous solution

Complex formation between Pd(II), Pt(II) and iodide has been studied at 25 °C for an aqueous 1.00 M perchloric acid medium. Measurements of the solubility of PdI₂(s) in aqueous mercury(II) perchlorate and of AgI(s) and PdI₂(s) in aqueous solutions of Pd²⁺(aq) and Ag⁺(aq) gave the solubility product of PdI₂(s) as K_s^o=(7±3) × 10⁻³² M³, which is much smaller than previous literature values.The stability constants β₁=[MI(H₂O)₃⁺]/([M(H₂O)₄²⁺][I⁻]) for the two systems were obtained as the ratio between rate constants for the forward and reverse reactions of (i).

The following values of k₁ (s⁻¹ M⁻¹), k₋₁ (s⁻¹) and β₁ (M⁻¹) were obtained at 25 °C: (1.14±0.11) × 10⁶, (0.92±0.18), (12±4) × 10⁵ for MPd, and (7.7±0.4), (8.0±0.7) × 10⁻⁵, (9.6±1.3) × 10⁴ for MPt. Combination with previous literature data gives the following values of log(β₁ (M⁻¹)) to log(β₄ (M⁻⁴)): 6.08, ∼22, 25.8 and 28.3 for MPd, and 4.98, ∼25, ∼28, and ∼30 for MPt. The present results show that the large overall stability constants β₄ observed for the M²⁺I⁻ systems are most likely due to a very large stability of the second complex MI₂(H₂O)₂, which is probably a cis-isomer. A distinct plateau in the formation curve for mean ligand number 2 is obtained both for MPd and Pt. The other iodo complexes are not especially stable compared to those of chloride and bromide.ΔH^≠ (kJ mol⁻¹) and ΔS^≠ (JK⁻¹ mol⁻¹) for the forward reaction of (i), MPd, are (17.3±1.7) and (−71±5), and for the reverse reaction of (i) MPd, (45±3) and (−95±6), respectively. The kinetics are compatible with associative activation (I_a). The contribution from bond-breaking in the formation of the transition state seems to be less important for Pd than for Pt.