An automated system for biocide testing on biofilms*

The paper presents and discusses a novel on-line real-time non-destructive continuous-flow system for biocide testing on industrial biofilms. This laboratory system is capable of monitoring changes in growth, accumulation and respiratory activity of biofilms in response to biocidal treatment. The system incorporates a fouling monitor for continuous measuring of the rate of biofilm accumulation (heat transfer resistance), a sensor for monitoring of microbial activity (oxygen meter for monitoring the rate of biofilm respiratory activity), and subsystems necessary for microbial life support and control of operation parameters. Examples of system operation and testing of oxidizing and non-oxidizing biocides are presented. Received 25 May 1997/ Accepted in revised form 25 November 1997     

Light Harvesting and State Transitions in Cyanobacteria

Cyanobacteria are oxygenic phototrophic prokaryotes and are considered to be the ancestors of chloroplasts. Their photosynthetic machinery is functionally equivalent in terms of primary photochemistry and photosynthetic electron transport. Fluorescence measurements and other techniques indicate that cyanobacteria, like plants, are capable of redirecting pathways of excitation energy transfer from light harvesting antennae to both photosystems. Cyanobacterial cells can reach two energetically different states, which are defined as “State 1” (obtained after preferential excitation of photosystem I) and “State 2” (preferential excitation of photosystem II). These states can be distinguished by static and time resolved fluorescence techniques. One of the most important conclusions reached so far is that the presence of both photosystems, as well as certain antenna components, are necessary for state transitions to occur. Spectroscopic evidence suggests that changes in the coupling state of the light harvesting antenna complexes (the phycobilisomes) to both photosystems occur during state transitions. The finding that the phycobilisome complexes are highly mobile on the surface of the thylakoid membrane (the mode of interaction with the thylakoid membrane is essentially unknown), has led to the proposal that they are in dynamic equilibrium with both photosystems and regulation of energy transfer is mediated by changes in affinity for either photosystem.     

应用离子注入技术对家蚕形态学及遗传学进行的初步研究(英文)

离子注入技术是将某种元素的原子进行电离,并使其在电场中加速,在获得较高的速度后射入固体材料表面。在离子注入过程中,被电离的离子在电场作用下加速运动,离子靠着本身获得的动能进入基体表面,在表层中运动的离子与基体原子作用损失能量后在一定的位置停留下来。该技术自６０年代问世以来,主要用于材料改性等方面。８０年代中期,我国学者开始将其用于农作物育种方面的研究,大大拓宽了离子注入技术的应用领域。所用实验材料的基因及表现型见Ｔａｂ３,我们将氢离子（Ｅ＝３５ＭｅＶ）注入处于胚胎发育后期的家蚕卵内（Ｔａｂ１）,观察其对家蚕形态及遗传方面的影响,结果表明：（１）在家蚕胚胎发育的已４期注入氢离子,其半致死剂量ＬＤ５０为１ｘ１０１０～１ｘ１０１１ｃｍ２这一区间之内;当剂量达到１ｘ１０１２ｃｍ２时,已全部致死（Ｆｉｇ．１＆Ｔａｂ．２）;（２）注入氢离子能够使家蚕在第１腹节上产生褐斑（Ｆｉｇ．２）的频率增高。并首次观察到因注入氢离子而导致家蚕出现非成对的褐斑（Ｆｉｇ．３＆Ｔａｂ．４）。（３）在氢离子注入剂量为１ｘ１０１０ｃｍ２时,能够诱变产生大量的嵌合体家蚕,并且诱变频率高达３８．５％（Ｆｉｇ．４＆Ｔａｂ．５）,这样高的     

Attenuation of seizure in P77PMC rats with an HSV-vector expressing IL-1ra in brain

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Protonmotive Mechanism of Heme-Copper Oxidases

The mechanism of coupling of proton and electron transfer in oxidases is reviewed and related to the structural information that is now available. A glutamate trap mechanism for proton/electron coupling is described.     

Genetic and biochemical evidence for distinct key functions of two highly divergent GAPDH genes in catabolic and anabolic carbon flow of the cyanobacterium Synechocystis sp. PCC 6803

Cyanobacterial genomes harbour two separate highly divergent glyceraldehyde-3-phosphate dehydrogenase (GAPDH) genes, gap1 and gap2, which are closely related at the sequence level to the nuclear genes encoding cytosolic and chloroplast GAPDH of higher plants, respectively. Genes gap1 and gap2 of the unicellular cyanobacterium Synechocystis sp. PCC 6803 were cloned and sequenced and subsequently inactivated by insertional mutagenesis to understand their metabolic functions. We obtained homozygous gap1^- mutants which have lost the capacity to grow on glucose under dim light while growth on organic acids as well as photosynthetic growth under CO₂ and high light is not impaired. Homozygous gap2^- mutants show the reciprocal phenotype. Under dim light they only grow on glucose but not on organic acids nor do they survive under photosynthetic conditions. Measurements of the anabolic activities (reduction of 1,3-bisphosphoglycerate) in extracts from wild type and mutant cells show that Gap2 is a major enzyme with dual cosubstrate specificity for NAD and NADP, while Gap1 displays a minor NAD-specific GAPDH activity. However, if measured in the catabolic direction (oxidation of glyceraldehyde-3-phosphate) Gap2 activity is very low and increases three- to fivefold after gel filtration of extracts over Sephadex G25. Our results suggest that enzymes Gap1 and Gap2, although coexpressed in cyanobacterial wild-type cells, play distinct key roles in catabolic and anabolic carbon flow, respectively. While Gap2 operates in the photosynthetic Calvin cycle and in non-photosynthetic gluconeogenesis, Gap1 seems to be essential only for glycolytic glucose breakdown, conditions under which the catabolic activity of Gap2 seems to be repressed by a specific low-molecular-weight inhibitor.     

Time-resolved electron transfer at the donor side of Rhodopseudomonas viridis photosynthetic reaction centers in whole cells

We have studied the electron transfer reactions from the tetraheme cytochrome of Rhodopseudomonas viridis to the oxidized primary donor in whole cells with a new high sensitivity spectrophotometer. In this apparatus the monochromatic detecting flashes are provided by a YAG pumped Optical Parametric Oscillator, allowing a 10 ns time resolution. When four hemes are reduced the observed electron transfer reaction sequence is the following: first the low-potential c552 heme (the number refers to the maximum absorption wavelength in the alpha-band region) is oxidized with a half time of 130 ns, in agreement with previous reports of measurements performed with purified reaction centers. Then, the electron hole is transferred to the low potential c554 heme with a half time of 2.6 µs. When only the two high potential hemes are reduced the observed electron transfer sequence is the following: oxidation of the high potential c559 heme in the hundreds of ns time range (410 ns), reduction of this heme by the high potential c556 heme in the µs time range (2.7 µs). This confirms the first steps of electron transfer observed in isolated reaction centers. However, in the microsecond time domain, the overall amount of oxidized hemes increases suggesting that, in vivo, the equilibrium constant between the P⁺/P and the c559^ox/c559^red couples is significantly lower than expected from the difference in their midpoint potentials.     

Chromatophore heterogeneity explains phenomena seen in Rhodobacter sphaeroides previously attributed to supercomplexes

It is generally considered that metabolic reactions are well described by homogeneous kinetic models in which the reaction phase is statistically uniform. In membranes, especially in photosynthetic systems where the protein complement is high, it has recently been recognized that effects of local heterogeneity might contribute additional factors that perturb the kinetic behavior, and require more extensive treatment. We show in this paper that statistical heterogeneity in vesicular systems can also contribute to quite marked discrepancies from the behavior expected from standard kinetic and thermodynamic models, for reactions involving free diffusion in the aqueous phase. We explain the kinetic and thermodynamic effects observed in studies of photosynthetic electron transfer in cells and chromatophores from Rhodobacter sphaeroides previously attributed to supercomplexes, in terms of a model based on heterogeneity in distribution of electron transfer components among the chromatophore population. We discuss examples of data inconsistent with the supercomplex model, but well explained by the heterogeneity model.     

ATP-synthesis in archaea: Structure-function relations of the halobacterial A-ATPase

The archaeal (A)-ATPase has been described as a chimeric energy converter with close relationship to both the vacuolar ATPase class in higher eukaryotes and the coupling factor (F)-ATPase class in eubacteria, mitochondria and chloroplasts. With respect to their structure and some inhibitor responses, A-ATPases are more closely related to the vacuolar ATPase type than to F-ATPase. Their function, ATP synthesis at the expense of an ion gradient, however, is a typical attribute of the F-ATPase class. V-type ATPases serve as generators of a proton gradient driving the accumulation of solutes within vesicles such as the vacuoles of plant cells. The three catalytic subunits (A) of the archaeal ATPases are the largest subunits of the A1-part and, like in V-ATPases, closer related to the F-ATPase -subunits, whereas B corresponds to F-ATPase . The catalytic subunits A of archaeal ATPases contain an insert of about 80 amino acids in their primary structures that may be aligned to comparable structures in V-ATPases. The location of this additional peptide in Haloferax volcanii is shown using the 2.8 Å X-ray resolution of the bovine mitochondrial F-ATPase [Abrahams et al. (1994) Nature 370: 621-628]. A three dimensional structure for the catalytic subunit of Haloferax volcanii ATPase is proposed using the Swiss-Model Automated Protein Modelling Server. The halobacterial ATPase is a halophilic protein; it contains about 20% negatively charged amino acid residues. A large portion of acidic residues is located on the outer surface of the protein as well as in the insert of subunit A. This result is discussed in terms of protein stability under high salt stress conditions.     

Oscillations of the energy gap for the initial electron-transfer step in bacterial reaction centers

Oscillations in the electrostatic energy gap [V_elec(t)] for electron transfer from the primary electron donor (P) to the adjacent bacteriochlorophyll (B) in photosynthetic bacterial reaction centers are examined by molecular-dynamics simulations. Autocorrelation functions of V_elec in the reactant state (PB) include prominent oscillations with an energy of 17 cm^–1. This feature is much weaker if the trajectory is propagated in the product state P⁺B^–. The autocorrelation functions also include oscillations in the regions of 5, 80 and 390 cm^–1 in both states, and near 25 and 48 cm^–1 in P⁺B^–. The strong 17-cm^–1 oscillation could involve motions that modulate the distance between P and B, because a similar oscillation occurs in the direct electrostatic interactions between the electron carriers.