Fluorescence detected magnetic resonance (FDMR) of green sulfur photosynthetic bacteria Chlorobium sp.

Fluorescence Detected Magnetic Resonance (FDMR) spectra have been measured for whole cells and isolated chlorosomal fractions for the green photosyntheic bacteria Chlorobium phaeobacteroides (containing bacteriochlorophyll e, and isorenieratene as major carotenoid) and Chlorobium limicola (containing bacteriochlorophyll c, and chlorobactene as major carotenoid). The observed transition at 237 MHz (identical in both bacteria) and > 1100 MHz can be assigned, by analogy with published data on other carotenoids, to the 2E and D + E transitions, respectively, of Chlorobium carotenoids. Their zero field splitting (ZFS) parameters are estimated to be: |D|=0.0332 cm^–1 and |E|=0.0039 cm^–1 (chlorobactene), and |D|=0.0355 cm^–1 and |E|=0.0039 cm^–1 (isorenieratene). In the intermediate frequency range 300–1000 MHz the observed transitions can be assigned to chlorosomal bacteriochlorophylls c and e, and to bacteriochlorophyll a located in the chlorosome envelope and water-soluble protein. The bacteriochlorophyll e triplet state measured in 750 nm fluorescence (aggregated chlorosomal BChl e) is characterised by the ZFS parameters: |D|=0.0251 cm^–1 and |E|=0.0050 cm^–1.Abbreviations BChl - bacteriochlorophyll - BPh - bacteriopheophytin - Chl. - Chlorobium - F(A)(O)DMR - fluorescence (absorption) (optical) detected magnetic resonance - FF - fluorescence fading - ISC - intramolecular intersystem crossing - RC - reaction center - ZFS - zero field splitting     

Fluorescence detected magnetic resonance of the primary donor and inner core antenna chlorophyll in Photosystem I reaction centre protein: Sign inversion and energy transfer

The Photosystem I reaction centre protein CP1, isolated from barley using polyacrylamide gel electrophoresis showed an EPR (Electron Paramgnetic Resonance) spectrum with the polarisation pattern AEEAAE, typical of the primary donor triplet state ³P700, created via radical pair formation and recombination. ³P700 could also be detected by Fluorescence Detected Magnetic Resonance (FDMR) at _f > 700 nm even in the presence of a large number of chlorophyll antennae. Its zero field splitting parameters, D=282.5×10^-4 cm^-1 and E=38.5×10^-4 cm^-1, were independent of the detection wavelength, and agreed with ADMR (Absorption Detected Magnetic Resonance) and EPR values. The signs of the ³P700 D+E and D-E transitions were positive (increase in fluorescence intensity on applying a resonance microwave field). In contrast, in the emission band 685 < _f < 700 nm FDMR spectra with negative D+E and D-E transitions were detected, and the D value was wavelength-dependent. These FDMR results support an excitation energy transfer model for CP1, derived from time-resolved fluorescence studies, in which two chlorophyll antenna forms are distinguished, with fluorescence at 685 < _f < 700 nm (inner core antennae, F690), and _f > 700 nm (low energy antenna sites, F720), in addition to the P700. The FDMR spectrum in F690 emission can be interpreted as that of ³P700, observed via reverse singlet excitation energy transfer and added to the FDMR spectrum of the antenna triplet states generated via intramolecular intersystem crossing. This would indicate that reversible energy transfer between F690 and P700 occurs even at 4.2 K.Abbreviations Chl chlorophyll - CP1 core chlorophyll protein of Photosystem I - EPR electron paramagnetic resonance - F690, F720 chlorophyll forms having fluorescence maximum at 690–695 and 720 nm, respectively - F(A)(O)DMR fluorescence (absorption) (optical) detected magnetic resonance - FF fluorescence fading - ISC intramolecular intersystem crossing - _f fluorescence emission wave-length - LHC I light harvesting chlorophyll a/b protein of Photosystem I - P700 primary donor of Photosystem I - PS I Photosystem I - RC reaction centre - RP radical pair - SDS sodium dodecyl sulphate - ZFS zero field splitting     

Study of the long-wavelength fluorescence band at 920 nm of isolated reaction centers of the photosynthetic bacterium Rhodopseudomonas spaeroides R-26 with fluorescence-detected magnetic resonance in zero field

The triplet state of isolated reaction centers of Rhodopseudomonas sphaeroides R-26 has been studied by fluorescence-detected electron spin resonance in zero magnetic field (FDMR) at 4.2 K. The sign of the FDMR resonance monitored at the long-wavelength fluorescence band is positive (fluorescence increase); this confirms the earlier interpretation (Hoff, A.J. and Gorter de Vries, H. (1978) Biochim. Biophys. Acta 503, 94–106) that the negative sign of the FDMR resonance of the reaction center triplet state in whole bacterial cells is caused by resonant transfer of the singlet excitations from the antenna pigments to the trap. By monitoring the FDMR response as a function of the wavelength of fluorescence, we have recorded microwave-induced fluorescence spectra. In addition to the positive microwave-induced fluorescence band peaking at 935 nm, at 905 nm a negative band was found. The resonant microwave frequencies for these two bands, i.e., the values of the zero-field splitting parameters |D| and |E| of the triplet state being monitored, were different, those of the 905 nm microwave-induced fluorescence band being identical to the resonant microwave frequencies measured with absorption-detected zero-field resonance (Den Blanken, H.J., Van der Zwet, G.P. and Hoff, A.J. (1982) Chem. Phys. Lett. 85, 335–338), a technique that monitors the bulk properties of the sample. From this result and its negative sign, we tentatively attribute the 905 nm microwave-induced fluorescence band to a small (possibly less than 1%) fraction of antenna bacteriochlorophylls that are in close contact with the trap. The positive 935 nm microwave-induced fluorescence band with resonant microwave frequencies deviating from the bulk material is ascribed to a minority of primary donor bacteriochlorophyll dimers, which have a higher than normal fluorescence yield because of a somewhat slower charge-separation reaction. Is it likely that practically all long-wavelength fluorescence of isolated reaction centers stems from such impaired reaction centers.     

The triplet exciton of chlorophyll a and carotenoid in solution and in photosynthetic antenna proteins

We have observed the development and decay of triplet excitons formed in the ‘antenna’ chlorophyll $\text{a}\text{b}$ protein complex by high-intensity laser excitation. The carotenoid triplet (³Car) appeared 5 ns after excitation in the protein isolation, commonly termed CP-II; the risetime in a larger antenna particle, called LHC (light-harvesting complex) was 12 ns. The quantum yield of ³Car in CP-II decreased 11-fold as intensity was increased from 10¹⁶ to 2 · 10¹⁷ photons/cm² per pulse. The effect is attributed to exciton annihilation during the initial period of triplet formation. Above 5 · 10¹⁶ photons/cm² per s, the ³Car lifetime decreases substantially from its low intensity value of 8.7 μs. A comparison of the transient absorption spectrum of CP-II with those of chlorophyll and carotenoid in vitro indicates that ‘trapped’ chlorophyll triplets formed at high intensities. We present a simple model of destructive interaction between ³Car and chlorophyll triplets which is compatible with the observed increased rate of ³Car decay. Indirect evidence suggests similar effects occur in LHC.     

Quantum yield and rate of formation of the carotenoid triplet state in photosynthetic structures

The formation of the triplet state of carotenoids (detected by an absorption peak at 515 nm) and the photo-oxidation of the primary donor of Photosystem II, P-680 (detected by an absorption increase at 820 nm) have been measured by flash absorption spectroscopy in chloroplasts in which the oxygen evolution was inhibited by treatment with Tris. The amount of each transient form has been followed versus excitation flash intensity (at 590 or 694 nm). At low excitation energy the quantum yield of triplet formation (with the Photosystem II reaction center in the state Q⁻) is about 30% that of P-680 photo-oxidation. The yield of carotenoid triplet formation is higher in the state Q⁻ than in the state Q, in nearly the same proportion as chlorophyll a fluorescence. It is concluded that, for excited chlorophyll a, the relative rates of intersystem crossing to the triplet state and of fluorescence emission are the same in vivo as in organic solvent. At high flash intensity the signal of P-680⁺ completely saturates, whereas that of carotenoid triplet continues to increase.

The rate of triplet-triplet energy transfer from chlorophyll a to carotenoids has been derived from the rise time of the absorption change at 515 nm, in chloroplasts and in several light-harvesting pigment-protein complexes. In all cases the rate is very high, around 8 · 10⁷ s⁻¹ at 294 K. It is about 2–3 times slower at 5 K. The transitory formation of chlorophyll triplet has been verified in two pigment-protein complexes, at 5 K.     

Time-dependent nanomechanics of cartilage

In this study, atomic force microscopy-based dynamic oscillatory and force-relaxation indentation was employed to quantify the time-dependent nanomechanics of native (untreated) and proteoglycan (PG)-depleted cartilage disks, including indentation modulus E_ind, force-relaxation time constant τ, magnitude of dynamic complex modulus |E^∗|, phase angle δ between force and indentation depth, storage modulus E′, and loss modulus E″. At ∼2 nm dynamic deformation amplitude, |E^∗| increased significantly with frequency from 0.22 ± 0.02 MPa (1 Hz) to 0.77 ± 0.10 MPa (316 Hz), accompanied by an increase in δ (energy dissipation). At this length scale, the energy dissipation mechanisms were deconvoluted: the dynamic frequency dependence was primarily governed by the fluid-flow-induced poroelasticity, whereas the long-time force relaxation reflected flow-independent viscoelasticity. After PG depletion, the change in the frequency response of |E^∗| and δ was consistent with an increase in cartilage local hydraulic permeability. Although untreated disks showed only slight dynamic amplitude-dependent behavior, PG-depleted disks showed great amplitude-enhanced energy dissipation, possibly due to additional viscoelastic mechanisms. Hence, in addition to functioning as a primary determinant of cartilage compressive stiffness and hydraulic permeability, the presence of aggrecan minimized the amplitude dependence of |E^∗| at nanometer-scale deformation.     

Long-Term Temperature Acclimation of Photosynthesis in Steady-State Cultures of the Polar Diatom <Emphasis Type="Italic">Fragilariopsis cylindrus</Emphasis>

Cultures of the obligate psychrophilic diatom Fragilariopsis cylindrus (Grunow) were grown for 4 months under steady-state conditions at −1 °C and +7 °C (50 μmol photons m⁻² s⁻¹) prior to measurements in order to investigate long-term acclimation of photosynthesis to both temperatures. No differences in maximum intrinsic quantum yield of PS II (F_V/F_M) and relative electron transport rates could be detected at either temperature after 4 months of acclimation. Measurements of photosynthesis (relative electron transport rates) vs. irradiance (P vs. E curves) revealed similar values for relative light utilization efficiency (α = 0.57 at −1 °C, α = 0.60 at +7 °C) but higher values for irradiance levels at which photosynthesis saturates (E_K) at −1 °C and, therefore, higher maximum photosynthesis (P_MAX = 54 (relative units) at −1 °C, P_MAX = 49 at +7 °C). Nonphotochemical quenching (NPQ) measurements at 385 μmol photons m⁻² s⁻¹ indicated higher (37%) NPQ for diatoms grown at −1 °C compared to +7 °C, which was possibly related to a 2-fold increase in the concentration of the pigment diatoxanthin and a 9-fold up-regulation of a gene encoding a fucoxanthin chlorophyll a,c-binding protein. Expression of the D1 protein encoding gene psbA was ca. 1.5-fold up-regulated at −1 °C, whereas expression levels of other genes from Photosystem II (psbC, psbU, psbO), as well as rbcL, the gene encoding the Rubisco large subunit were similar at both temperatures. However, a 2-fold up-regulation of a plastid glyceraldehyde-P dehydrogenase at −1 °C indicated enhanced Calvin cycle activity. This study revealed for the first time that a polar diatom could efficiently acclimate photosynthesis over a wide range of polar temperatures given enough time. Acclimation of photosynthesis at −1 °C was probably regulated similarly to high light acclimation.     

Transepithelial Taurine Transport in Caco-2 Cell Monolayers

Here we characterized transepithelial taurine transport in monolayers of cultured human intestinal Caco-2 cells by analyzing kinetic apical and basolateral uptake and efflux parameters. Basolateral uptake was Na⁺- and Cl⁻- dependent and was inhibited by β-amino acids. Uptake by this membrane showed properties similar to those of the apical TauT system. In both membranes, taurine uptake fitted a model consisting of a non-saturable plus a saturable component, with a higher half-saturation constant and transport capacity at the apical membrane (K_m, 17.1 μmol/L; V_max, 28.4 pmol·cm⁻²·5 min⁻¹) than in the basolateral domain (K_m, 9.46 μmol/L; V_max, 5.59 pmol·cm⁻²·5 min⁻¹). The non-saturable influx component, estimated in the absence of Na⁺ and Cl⁻, showed no significant differences between apical and basolateral membranes (K_D, 89.2 and 114.7 nL·cm⁻² · 5 min⁻¹, respectively). Taurine efflux from the cells is a diffusive process, as shown in experiments using preloaded cells and in trans-stimulation studies (apical K_D,72.7 and basolateral K_D, 50.1 nL·cm⁻²·5 min⁻¹). Basolateral efflux rates were significantly lower than passive influx rates. We conclude that basolateral taurine uptake in Caco-2 cells is mediated by a transport mechanism that shares some properties with the apical system TauT. Moreover, calculation of unidirectional and transepithelial taurine fluxes reveals that apical influx of this amino acid is higher than basolateral efflux rates, thereby enabling epithelial cells to accumulate taurine against a concentration gradient.     

Esterification and Spectral Shifts of Chlorophyll(ide) in Wildtype and Mutant Seedlings Developed in Darkness

Spectral changes and esterification (presumably with phytol) of newly formed chlorophyllide a in dark-grown leaves of wildtype bean (Phaseolus vulgaris) and barley (Hordeum vulgare) and a number of chloroplast mutants in barley, were studied by spectrofluorimetry on leaves and on solvent extracts. The shift of the fluorescence emission maximum from 692–694 to 678 nm (excitation shift: 682–684 to 672 nm) and esterification of chlorophyllide a have a similar time course, and both processes are temperature dependent in a similar manner. After completion of the spectral shift and esterification, the fluorescence efficiency of chlorophyll a increases with a subsequent reaccumulation of protochlorophyllide. In leaves of mutants where the shift of fluorescence from 692 to 678 nm is lacking, esterification and the subsequent processes are also blocked. In leaves of mutants with a rapid shift of the fluorescence from 692 to 678 nm, or with direct photoconversion to chlorophyllide a with the fluorescence at 678 nm, esterification is also rapid. The results are interpreted as a sequence of molecular events involving a conformational relaxation of the chlorophyllide holochrome and a translocation of chlorophyll a to reaction centers of the photosystems.     

The effect of norflurazon on protein composition and chlorophyll organization in pigment–protein complex of Photosystem II

The pyridazinone-type herbicide norflurazon SAN 9789 inhibiting the biosynthesis of long-chain carotenoids results in significant decrease in PS II core complexes and content of light-harvesting complex (LHC) polypeptides in the 29.5–21 kDa region. The Chl a forms at 668, 676, and 690 nm that belong to LHC and antenna part of PS I disappear completely after treatment. The intensity of the Chl b form at 648 nm is sharply decreased in treated seedlings grown under 30 or 100 lx light intensity. The bands of carotenoid absorption at 421, 448 (Chl a), 452, 480, 492, 496 (β-carotene), and 508 nm also disappear. The band shift from 740 to 720 nm and decrease in its intensity relative to the 687 nm emission peak in the low-temperature fluorescence spectrum (77 K) suggests a disturbance of energy transfer from LHC to the Chla form at 710–712 nm.     

EPR characterisation of the triplet state in photosystem II reaction centers with singly reduced primary acceptor QA

The triplet states of photosystem II core particles from spinach were studied using time-resolved cw EPR technique at different reduction states of the iron-quinone complex of the reaction center primary electron acceptor. With doubly reduced primary acceptor, the well-known photosystem II triplet state characterised by zero-field splitting parameters |D| = 0.0286 cm⁻¹, |E| = 0.0044 cm⁻¹ was detected. When the primary acceptor was singly reduced either chemically or photochemically, a triplet state of a different spectral shape was observed, bearing the same D and E values and characteristic spin polarization pattern arising from RC radical pair recombination. The latter triplet state was strongly temperature dependent disappearing at T = 100 K, and had a much faster decay than the former one. Based on its properties, this triplet state was also ascribed to the photosystem II reaction center. A sequence of electron-transfer events in the reaction centers is proposed that explains the dependence of the triplet state properties on the reduction state of the iron-quinone primary acceptor complex.     

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

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

Determination of the primary charge separation rate in Photosystem II reaction centers at 15 K

We have measured the rate constant for the formation of the oxidized chlorophyll a electron donor (P680⁺) and the reduced electron acceptor pheophytin a ^– (Pheo a ^–) following excitation of isolated Photosystem II reaction centers (PS II RC) at 15 K. This PS II RC complex consists of D₁, D₂, and cytochrome b-559 proteins and was prepared by a procedure which stabilizes the protein complex. Transient absorption difference spectra were measured from 450–840 nm as a function of time with 500fs resolution following 610 nm laser excitation. The formation of P680⁺-Pheo a ^– is indicated by the appearance of a band due to P680⁺ at 820 nm and corresponding absorbance changes at 490, 515 and 546 nm due to the formation of Pheo a ^–. The appearance of the 490 nm and 820 nm bands is monoexponenital with =1.4±0.2 ps. Treatment of the PS II RC with sodium dithionite and methyl viologen followed by exposure to laser excitation results in accumulation of Pheo a ^–. Laser excitation of these prereduced RCs at 15 K results in formation of a transient absorption spectrum assigned to ^1*P680. We observe wavelength-dependent kinetics for the recovery of the transient bleach of the Q_y absorption bands of the pigments in both untreated and pre-reduced PS II RCs at 15K. This result is attributed to an energy transfer process within the PS II RC at low temperature that is not connected with charge separation.Abbreviations PS I Photosystem I - PS II Photosystem II - RC reaction center - P680 primary electron donor in Photosystem II - Chl a chlorophyll a - Pheo a pheophytin a     

Modification of excitation energy distribution to photosystem I by protein phosphorylation and cation depletion during thylakoid biogenesis in wheat

The effects of protein phosphorylation and cation depletion on the electron transport rate and fluorescence emission characteristics of photosystem I at two stages of chloroplast development in light-grown wheat leaves are examined. The light-harvesting chlorophyll a/b protein complex associated with photosystem I (LHC I) was absent from the thylakoids at the early stage of development, but that associated with photosystem II (LHC II) was present. Protein phosphorylation produced an increase in the light-limited rate of photosystem I electron transport at the early stage of development when chlorophyll b was preferentially excited, indicating that LHC I is not required for transfer of excitation energy from phosphorylated LHC II to the core complex of photosystem I. However, no enhancement of photosystem I fluorescence at 77 K was observed at this stage of development, demonstrating that a strict relationship between excitation energy density in photosystem I pigment matrices and the long-wavelength fluorescence emission from photosystem I at 77 K does not exist. Depletion of Mg²⁺ from the thylakoids produced a stimulation of photosystem I electron transport at both stages of development, but a large enhancement of the photosystem I fluorescence emission was observed only in the thylakoids containing LHC I. It is suggested that the enhancement of PS I electron transport by Mg²⁺-depletion and phosphorylation of LHC II is associated with an enhancement of fluorescence at 77 K from LHC I and not from the core complex of PS I.     

Tryptophan residue is essential for immunoreactivity of a diagnostically relevant peptide epitope of A. fumigatus

The role of tryptophan (Trp¹⁷) in immunoreactivity of P1, the diagnostically relevant peptide from a major allergen/antigen of Aspergillus fumigatus, was evaluated by chemically modifying tryptophanyl residue of P1. In BIAcore kinetic studies, unmodified P1 showed a 100-fold higher binding with ABPA (Allergic Bronchopulmonary Aspergillosis) patients’ IgG [K_D (equilibrium dissociation constant) = 2.74 e⁻⁸ ± 0.13 M] than the controls’ IgG (K_D = 2.97 e⁻⁶± 0.14 M), whereas chemically-modified P1 showed similar binding [K_D patients’ IgG = 3.25 e⁻⁷± 0.16 M, K_D controls’ IgG = 3.86 e⁻⁷± 0.19 M] indicating loss of specific immunoreactivity of P1 on tryptophan modification. Modified P1 showed loss of specific binding to IgE and IgG antibodies of ABPA patients in ELISA (Enzyme-Linked Immunosorbent Assay). The study infers that tryptophan residue (Trp¹⁷) is essential for immunoreactivity of P1.     

Chlorophyll triplet states associated with Photosystem I and Photosystem II in thylakoids of the green alga Chlamydomonas reinhardtii

The analysis of FDMR spectra, recorded at multiple emission wavelengths, by a global decomposition technique, has allowed us to characterise the triplet populations associated with Photosystem I and Photosystem II of thylakoids in the green alga Chlamydomonas reinhardtii. Three triplet populations are observed at fluorescence emissions characteristic of Photosystem II, and their zero field splitting parameters have been determined. These are similar to the zero field parameters for the three Photosystem II triplets previously reported for spinach thylakoids, suggesting that they have a widespread occurrence in nature. None of these triplets have the zero field splitting parameters characteristic of the Photosystem II recombination triplet observed only under reducing conditions. Because these triplets are generated under non-reducing redox conditions, when the recombination triplet is undetectable, it is suggested that they may be involved in the photoinhibition of Photosystem II. At emission wavelengths characteristic of Photosystem I, three triplet populations are observed, two of which are attributed to the P₇₀₀ recombination triplet frozen in two different conformations, based on the microwave-induced fluorescence emission spectra and the triplet minus singlet difference spectra. The third triplet population detected at Photosystem I emission wavelengths, which was previously unresolved, is proposed to originate from the antenna chlorophyll of the core or the unusually blue-shifted outer antenna complexes of this organism.     

Resonant Raman quantification of zeaxanthin production from Flavobacterium multivorum

Resonant Raman scattering was used as a novel, rapid, non-destructive optical technique to measure zeaxanthin levels in Flavobacterium multivorum ATCC 55238. Culture broth, after bacterial growth for 40 h, exhibited characteristic resonance Raman vibrational modes at 1159 cm^–1 (C-C stretch) and 1525 cm^–1 (C=C stretch) upon excitation at 488 nm. A striking correlation was observed between the carotenoid level as estimated by HPLC and by resonance Raman spectroscopy.     

Synthesis and magnetic properties of bis(μ-hydroxo)bis[(2,2 ′-bipyridyl)copper(II)] squarate. Crystal structure of bis(μ-hydroxo)bis[(2,2′-bipyridyl)copper(II)] squarate tetrahydrate

The compound [Cu₂(bipy)₂(OH)₂](C₄O₄)·5.5H₂O, where bipy and C₄O₄²⁻ correspond to 2,2′-bipyridyl and squarate (dianion of 3,4-dihydroxy-3-cyclo- butene-1,3-dione) respectively, has been synthesized. Its magnetic properties have been investigated in the 2–300 K temperature range. The ground state is a spin-triplet state, with a singlet-triplet separation of 145 cm⁻¹. The EPR powder spectrum confirms the nature of the ground state.Well-formed single crystals of the tetrahydrate, [Cu₂(bipy)₂(OH)₂](C₄O₄)·4H₂O, were grown from aqueous solutions and characterized by X-ray diffraction. The system is triclinic, space group P , with a = 9.022(2), b = 9.040(2), c = 8.409(2) Å, α = 103.51(2), β = 103.42(3), γ = 103.37(2)°, V = 642.9(3) ų, Z = 1, D_x = 1.699 g cm⁻³, μ(Mo Kα) = 17.208 cm⁻¹, F(000) = 336 and T= 295 K. A total of 2251 data were collected over the range 1θ25°; of these, 1993 (independent and with I3σ(I)) were used in the structural analysis. The final R and R_w residuals were 0.034 and 0.038 respectively. The structure contains squarato-O¹, O³-bridged bis(μ-hydroxo)bis[(2,2′-bipyridyl)copper(II)] units forming zigzag one-dimensional chains. Each copper atom is in a square-pyramidal environment with the two nitrogen atoms of 2,2′-bipyridyl and the two oxygen atoms of the hydroxo groups building the basal plane and another oxygen atom of the squarate lying in the apical position.The magnetic properties are discussed in the light of spectral and structural data and compared with the reported ones for other bis(μ-hydroxo)bis[(2,2′-bipyridyl)copper(II)] complexes.     

Physico-chemical characterization of exomannan from <Emphasis Type="Italic">Rhodotorula acheniorum</Emphasis> MC

The batch fermentation of Rhodotorula acheniorum MC on a culture medium containing 5% sucrose, mineral salts and yeast extract at 26 °C for 96 h, with aeration at 0.75 v/v/m and agitation at 500 rev min ⁻¹ resulted in the synthesis of an exopolysaccharide (6.2 g l ⁻¹) which formed two fractions upon precipitation. The fractions were purified to a carbohydrate content of 98.2% for fraction I and 87.3% for fraction II. Mannose was the main monosaccharide component in a 92.8% concentration in fraction I and a 90.6% concentration in Fraction II. The exopolysaccharide was thus a mannan. The gel chromatograms confirmed the chemical composition of both fractions. The molecular weight of mannan I was 310 kD, whereas that of mannan II was 249 kD. The mannan I intrinsic viscosity [η]=6.23 dl g⁻¹ was higher than that of mannan II [η]=2.73 dl g⁻¹. The water-binding capacity of the mannan samples was established within the 1.2–3.5 g g⁻¹ range. The multiplicative model [η]=387.22. D_r^−0.1913. T^−1.095. C^1.814 describing the effect of the velocity gradient D_r, the exomannan concentration C and the temperature T on the dynamic viscosity values η of polymer solutions was obtained.     

Conformational change of core particles studied by quasielastic light scattering

The diffusion translational coefficient D_T of core particles in monodisperse solutions has been measured by the quasielastic light scattering method in a large scale of salinities over the range 6.10⁻⁴ to 2M Na⁺ or K⁺. The observed values of D_T are independent of particle concentration in the range 0.1–2 mg/ml and do not vary with the scattering vector q corresponding to scattering angles between 40°–120°. When the salinity is progressively raised an increase of D_T from 1.9.10⁻⁷ cm²s⁻¹ to 3.2.10⁻⁷ cm²s⁻¹ was observed at about 2.10⁻³ M NaCl followed by a decrease of D_T beyond 0.6 M NaCl.The various possible causes of the changes of D_T such as interactions between particles or between particles and salt ions are discussed. We show that the single low ionic strength change is due to a conformational transition of the core particles, while the second variation of D_T accompanies the disorganization of the core particles.