Free energy dependence of the direct charge recombination from the primary and secondary quinones in reaction centers from Rhodobacter sphaeroides

The direct charge recombination rates from the primary quinone, k _AD (D⁺Q _A ^– DQ_A) and the secondary quinone, k _BD (D⁺Q _B ^– DQ_B), in reaction centers from Rhodobacter sphaeroides were measured as a function of the free energy differences for the processes, G _AD ⁰ and G _BD ⁰ , respectively. Measurements were performed at 21 °C on a series of mutant reaction centers that have a wide range of dimer midpoint potentials and consequently a large variation in G _AD ⁰ and G _BD ⁰ . As –G _AD ⁰ varied from 0.43 to 0.78 eV, k _AD varied from 4.6 to 28.6 s^–1. The corresponding values for the wild type are 0.52 eV and 8.9 s^–1. Observation of the direct charge recombination rate k _BD was achieved by substitution of the primary quinone with naphthoquinones in samples in which ubiquinone was present at the secondary quinone site, resulting specifically in an increase in the free energy of the D⁺Q _A ^– state relative to the D⁺Q_AQ _B ^– state. As –G _BD ⁰ varied from 0.37 to 0.67 eV, k _BD varied from 0.03 to 1.4 s^–1. The corresponding values for the wild type are 0.46 eV and 0.2 s^–1. A fit of the two sets of data to the Marcus theory for electron transfer yielded significantly different reorganization energies of 0.82 and 1.3 eV for k _AD and k _BD, respectively. In contrast, the fitted values for the coupling matrix element, or equivalently the maximum possible rate, were comparable (25 s^–1) for the two charge recombination processes. These results are in accord with Q_B having more interactions with dipoles, from both the surrounding protein and bound water molecules, than Q_A and with the primary determinant of the maximal rate being the quinone-donor distance.     

Temperature dependence of the primary electron transfer reaction in pigment-modified bacterial reaction centers

The initial electron transfer steps in pigment modified reaction centers, where bacteriopheophytin is replaced by plant pheophytin (R26.Phe-a RCs) have been investigated over a wide temperature range by femtosecond time-resolved spectroscopy. The experimental data obtained in the maximum of the bacteriochlorophyll anion band at 1020 nm show the existence of a high and long-lived population of the primary acceptor P⁺B_A ^– even at 10 K. The data suggest a stepwise electron transfer mechanism with B_A as primary acceptor also in the low temperature domain. A detailed data analysis suggests that the pigment modification leads to a situation with almost isoenergetic primary and secondary acceptor levels, approximately 450 cm^–1 below P^*. A Gaussian distribution (with = 400 cm ^–1) of the G values has to be assumed to account for the strong dispersive character of the kinetics in this sample. Based on these assumptions, a model is presented that reproduces the observed kinetics, heterogeneity and temperature dependence.     

Characterization of second site mutations show that fast proton transfer to QB − is restored in bacterial reaction centers of Rhodobacter sphaeroides containing the Asp-L213 → Asn lesion

The structural basis for proton coupled electron transfer to Q_B in bacterial reaction centers (RCs) was studied by investigating RCs containing second site suppressor mutations (Asn M44 Asp, Arg M233 Cys, Arg H177 His) that complement the effects of the deleterious Asp L213 Asn mutation [DN(L213)]. The suppressor RCs all showed an increased proton coupled electron transfer rate k _AB ⁽²⁾(Q_A ^–Q_B ^– + H⁺ Q_AQ_BH^–) by at least 10³ (pH 7.5) and a recombination rate k _BD (D⁺Q_AQ_B ^– DQ_AQ_B) 15–40 times larger than the value found in DN(L213) RCs. Proton transfer was studied by measuring the dependence of k _AB ⁽²⁾ on the free energy for electron transfer (G_et). k _AB ⁽²⁾ was independent of G_et in DN(L213) RCs, but dependent on G_et in native and all suppressor RCs. This shows that proton transfer limits the k _AB ⁽²⁾ reaction with a rate of 0.1s^–1 in DN(L213) RCs but is not rate limiting and at least 10⁸-fold faster in native and 10⁵-fold faster in the suppressor RCs. The increased rate of proton transfer by the suppressor mutations are proposed to be due to: (i) a reduction in the barrier to proton transfer by providing a more negative electrostatic potential near Q_B ^–; and/or (ii) structural changes that permit fast proton transfer through the network of protonatable residues and water molecules near Q_B.     

Bubble column bioreactors

Summary The photographic and electrical conductivity methods to measure the structure of two phase flow, especially bubble size, bubble frequency, local gas hold-up and, for the latter, the bubble velocity are described.Symbols specific interfacial area - a gas/liquid interfacial area - B constant in Eq. (4) - d diameter of the bubbles - d mean diameter of the bubbles - d_S Sauter diameter - E_G relative gas hold up - I current - k_L mass transfer coefficient across the gas/liquid interface - k_L local k_L - LT^–1 - LT^–1 - 1 longitudinal distance between the start and stop sensors - 1_B pierced length of the bubble - t time - t₁ length of the square-wave signal at the start sensor - t₂ length of the square-wave signal at the stop sensor - t₁₂ time delay between start and stop signals - V volume of the bubbling layer - V_L volume of the bubble free layer - V_B bubble volume - v_B bubble velocity     

Methods for measuring the bubble size in bubble column bioreactors II

Summary Electrooptical and light scattering methods for measuring the structure of two phase flow, especially bubble size, are described and compared with photographic and electrical conductivity methods.Symbols L length - T time - M mass - d bubble diameter - mean bubble diameter - d_K inside diameter of the sensor capillary - 1 longitudinal distance between start and stop sensors - 1_B pierced length of bubble - t time - t₁ length of square-wave signal at start sensor - t₂ length of square-wave signal at stop sensor - 1₁₂ time delay between start and stop signals - V_B bubble volume - V_B bubble velocity - w_SG superficial gas velocity     

The IleL229 → Met mutation impairs the quinone binding to the QB-pocket in reaction centers of Rhodobacter sphaeroides

A spontaneous mutant (R/89) of photosynthetic purple bacterium Rhodobacter sphaeroides R-26 was selected for resistance to 200 M atrazin. It showed increased resistance to interquinone electron transfer inhibitors of o-phenanthroline (resistance factor, RF=20) in UQ_o reconstituted isolated reaction centers and terbutryne in reaction centers (RF=55) and in chromatophores (RF=85). The amino acid sequence of the Q_B binding protein of the photosynthetic reaction center (the L subunit) was determined by sequencing the corresponding pufL gene and a single mutation was found (Ile^L229 Met). The changed amino acid of the mutant strain is in van der Waals contact with the secondary quinone Q_B. The binding and redox properties of Q_B in the mutant were characterized by kinetic (charge recombination) and multiple turnover (cytochrome oxidation and semiquinone oscillation) assays of the reaction center. The free energy for stabilization of Q_AQ_B ^– with respect to Q_A ^–Q_B was G_AB=–60 meV and 0 meV in reaction centers and G_AB=–85 meV and –46 meV in chromatophores of R-26 and R/89 strains at pH 8, respectively. The dissociation constants of the quinone UQ_o and semiquinone UQ_o ^– in reaction centers from R-26 and R/89 showed significant and different pH dependence. The observed changes in binding and redox properties of quinones are interpreted in terms of differential effects (electrostatics and mesomerism) of mutation on the oxidized and reduced states of Q_B.Abbreviations BChl bacteriochlorophyll - Ile isoleucine - Met methionin - P primary donor - Q_A primary quinone acceptor - Q_B secondary quinone acceptor - RC reaction center protein - UQ_o 2,3-dimethoxy-5-methyl benzoquinone - UQ₁₀ ubiquinone 50 This work is dedicated to the memory of Randall Ross Stein (1954–1994) and is, in a small way, a testament to the impact which Randy's ideas have had on the development of the field of competitive herbicide binding.     

Changes in the Photosynthetic Apparatus of Broad Bean Leaves as Dependent on the Content of Heavy Metals in the Growth Medium

The content of chlorophyll, the rate of O₂ evolution, the slow phase of fluorescence induction, and photoinduced changes in the intensity of electron paramagnetic resonance (EPR) signal I from the reaction center of photosystem I (P⁺700) were studied in leaves of Vicia faba L. grown in 10^–7–10^–3 M aqueous solutions of CdCl₂, SnCl₂, CuCl₂, and MgCl₂. At low concentrations of heavy metal (Cd, Sn, and Cu) chlorides, the content of chlorophyll per fresh weight decreased. However, the rate of O₂ evolution calculated per chlorophyll basis, O₂/(t chlorophyll), increased. High concentrations of heavy metals significantly suppressed plant development and inhibited photosynthetic O₂ evolution. In contrast, plant treatment with MgCl₂ (10^–5–10^–3 M) resulted in an increase in the content of chlorophyll and a stimulation of leaf photosynthetic activity. A positive correlation between the F _M/F _T ratio and O₂/(t chlorophyll) (r = 0.89, P > 0.999) was found. We observed a negative correlation between the values of P/P ₀ of EPR signal I (white/far-red light) and O₂/(tchlorophyll) (r = –0.89, P > 0.999). The data obtained indicate nonspecific and nonmonotone changes in the photosynthetic apparatus of plants treated with heavy metals: low concentrations of heavy metals (10^–7–10^–6 M) stimulated photosynthetic activity, whereas high concentrations (10^–4–10^–3 M) suppressed it.     

Dependence of energization of thylakoids on frequency of exciting flashes in intact chloroplasts

We investigated the frequency-dependence of the flash-induced electrochromic absorbance change, A₅₁₅, and of the pH-indicating absorbance change of neutral red in isolated intact chloroplasts. The energization pattern of thylakoids depended strongly on the frequency (f) of the exciting flashes, tested between 0.05 and 2 s^–1. When the frequency was increased from 0.1 to 1 s^–1 the total initial change and the slow rise of A₅₁₅ decreased by about 30% and 70%, respectively, and both the slow rise and decay were considerably accelerated. These changes were fully reversible, even after prolonged excitation at 1 s^–1, if the frequency was decreased again to 0.1 s^–1. Accumulation of an appreciable transmembrane electric field strength could not be detected in any of our experiments, at high frequency, since the decay of A₅₁₅ was considerably accelerated when the frequency was increased. In contrast, pH significantly increased at higher frequencies of the exciting flashes. In the steady-state (after about 100 flashes) pH was about 0.5–0.8 pH unit higher than in the dark or at low frequencies. In the presence of nigericin or dithionite, both of which prevented accumulation of protons in the lumen, the total initial change in A₅₁₅ at f=1 s^–1 relative to that at f=0.1 s^–1 decreased to a similar extent as in the control. The proportion of the slow rise relative to the initial amplitude, however, did not decrease. Our data support the suggestion that pH controls the amplitude of the slow rise of A₅₁₅. However, contrary to a previous statement (B. Bouges-Bouquet (1981) Biochim. Biophys. Acta 535, 327–340), we show that the pH effect cannot be accounted for by variation of the rate of this kinetic component of A₅₁₅.Abbreviations DCMU 3(3,4-dichlorophenyl)-1,1-dimethylurea - f frequency of the exciting flashes - HEPES N-2-hydroxyethylpiperazine-N-2-ethanesulfonic acid - PS photosystem     

Electrogenic properties of the cloned Na+/glucose cotransporter: I. Voltage-clamp studies

Summary Cystic fibrosis (CF) is characterized by abnormal epithelial Cl^– conductance (G_Cl). In vitro studies that have shown that cAMP regulation is an intrinsic property of the CF-affected G_Cl(CF-G_Cl) have been carried out previously on cultured secretory cells and on nonepithelial cells. Even though G_Cl in absorption is defective in CF, a clear demonstration of cAMP regulation of CF-G_Cl in a purely absorptive tissue is lacking. We studied the cAMP regulation of CF-G_Cl in the microperfused intact human reabsorptive sweat duct. About 40% of the ducts responded to cAMP (responsive) while the remainder of the ducts did not. In responsive ducts, cAMP-elevating agents: -adrenergic agonist isoproterenol (IPR), CPT-cAMP, forskolin, theophylline or IBMX increased G _tby about 2.3-fold (n = no. of ducts = 8). Removal of media Cl^–, but not amiloride pretreatment (in the lumen), abolished the cAMP response, indicating exclusive activation of G_Cl. cAMP activated both apical and basolateral G_Cl. cAMP hyperpolarized gluconate: Cl^– (lumen: bath) transepithelial bionic potentials (V _t=–20.3±5.2 mV, mean ±se, n=9) and transepithelial 3 1 luminal NaCl dilution diffusion potentials (V _t=–8.8±2.9 mV, n=5). cAMP activated basolateral G_Cl as indicated by increased bi-ionic (gluconate: Cl^–, bath: lumen) diffusion potentials (by about 12 mV). The voltage divider ratio in symmetric NaCl solutions increased by 60%. Compared to responsive ducts, nonresponsive ducts were characterized by smaller spontaneous transepithelial potentials in symmetrical Ringer's solution (V _t=–6.9±0.8 mV, n=24, nonresponsive vs. –19.4±1.8 mV, n=22, responsive ducts) but larger bi-ionic potentials (–94±6 mV, n=35, nonresponsive vs. –65±5 mV, n=17, responsive ducts) and dilution diffusion potentials (–40±5 mV, n=11, nonresponsive vs. –29±3 mV, n=7, responsive ducts). These results are consistent with an inherently (prestimulus) maximal activation of G_Cl in nonresponsive ducts and submaximal activation of G_Cl in responsive ducts. We conclude that cAMP activates CF-G _Cl which is expressed and abnormal in both apical and basal membranes of this absorptive epithelium in CF.Abbreviations CF cystic fibrosis - G _t transepithelial conductance - V _b electrical potential across the basolateral membrane - V _a electrical potential across the apical membrane - V _t transepithelial potential - V _b transepithelial currentinduced voltage deflections across the basolateral membrane - V _a transepithelial current-induced voltage deflections across the apical membrane - V _t transepithelial current-induced voltage deflection across the epithelium - VDR voltage divider ratio - G_Cl transepithelial Cl^– conductance - CF-G_Cl cystic fibrosis-affected Cl^– conductance - EMF electromotive force - IPR isoproterenol - IBMX 3-isobutyl-1-methylxanthine - CPT-cAMP chlorophenylthio-adenosine 3-5 cyclic monophosphate - PGE₂ prostaglandin E₂     

Thermodynamics of the Binding of Chymotrypsin with the Black-eyed Pea Trypsin and Chymotrypsin Inhibitor (BTCI)

The binding of -chymotrypsin to black-eyed pea trypsin/chymotrypsin inhibitor (BTCI) has been studied using the inhibitory activity against the enzyme and the formation of the complex enzyme/inhibitor followed by measurements of fluorescence polarization. Apparent equilibrium constants were estimated for several temperatures and the values obtained range from 0.32 × 10⁷ to 1.36 × 10⁷ M^–1. The following values were found from van't Hoff plots: H _vh ^° = 10.8 kcal mol^-1 (from inhibitory assays) and 11.1 kcal mol^–1 (from fluorescence polarization); S° = 67.9 and = 67.8 kcal K^–1 mol^–1, respectively. Calorimetric binding enthalpy was determined (corrected for the ionization heat of the buffer) and the resulting value was H _cal ^° = 4.9 kcal mol^-1. These results indicate that the binding of chymotrypsin to BTCI is an entropically driven process.     

Electron transfer in deuterated reaction centers of Rhodobacter sphaeroides at 90 K according to femtosecond spectroscopy data

The primary act of charge separation was studied in P⁺B_A ^– and P⁺H_A ^– states (P, primary electron donor; B_A and H_A, primary and secondary electron acceptor) of native reaction centers (RCs) of Rhodobacter sphaeroides R-26 using femtosecond absorption spectroscopy at low (90 K) and room temperature. Coherent oscillations were studied in the kinetics of the stimulated emission band of P* (935 nm), of absorption band of B_A ^– (1020 nm) and of absorption band of H_A (760 nm). It was found that in native RCs kept in heavy water (D₂O) buffer the isotopic decreasing of basic oscillation frequency 32 cm ^–1 and its overtones takes place by the same factor 1.3 in the 935, 1020, and 760 nm bands in comparison with the samples in ordinary water H₂O. This suggests that the femtosecond oscillations in RC kinetics with 32 cm ^–1 frequency may be caused by rotation of hydrogen-containing groups, in particular the water molecule which may be placed between primary electron donor P_B and primary electron acceptor B_A. This rotation may appear also as high harmonics up to sixth in the stimulated emission of P*. The rotation of the water molecule may modulate electron transfer from P* to B_A. The results allow for tracing of the possible pathway of electron transfer from P* to B_A along a chain consisting of polar atoms according to the Brookhaven Protein Data Bank (1PRC): Mg(P_B)-N-C-N(His M200)-HOH-O = B_A. We assume that the role of 32-cm ^–1 modulation in electron transfer along this chain consists of a fixation of electron density at B_A ^– during a reversible electron transfer, when populations of P* and P⁺B_A ^– states are approximately equal.     

The lumenal loop connecting transmembrane helices I and II of the D1 polypeptide is important for assembly of the photosystem two complex

Current structural models indicate that the D1 and D2 polypeptides of the Photosystem two reaction center complex (PS II RC) each span the thylakoid membrane five times. In order to assess the importance of the lumenal extrinsic loop that connects transmembrane helices I and II of D1 we have constructed five deletion mutants and two double mutants in the cyanobaterium Synechocystic sp. PCC 6803. Four of the deletion mutants (59–65, 69–74, 79–86 and 109–110) are obligate photoheterotrophs unable to accumulate D1 in the membrane as assayed by immunoblotting experiments or pulse-labelling experiments using [³⁵S]-methionine. In contrast deletion mutant 100 which lacks A100 behaved very similarly to the WT control strain in terms of photoautotrophic growth rate, saturated rates of oxygen evolution, flash-induced oxygen evolution, fluorescence induction and decay, and thermoluminescence. 100 is the first example of an internal deletion on the lumenal side of the D1 polypeptide that is benign to photosystem two function. Double mutant D103G/E104A also behaves similarly to the WT control strain leading to the conclusion that residues D103 and E104 are unlikely to be involved in ligating the metal ions Mn or Ca²⁺, which are needed for photosynthetic oxygen evolution. Double mutant, G109A/G110A, was constructed to assess the significance of this GlyGly motif which is also conserved in the L subunit of purple bacterial reaction centres. The G109A/G110A mutant is able to evolve oxygen at approximately 50–70% of WT rates but is unable to grow phatoautotrophically apparently because of an enhanced sensitivity to photoinactivation than the WT control strain. A photoautotropic revertant was isolated from this strain and shown to result from a mutation that restored the WT codon at position 109. Pulse-chase experiments in cells using [³⁵S]-methionine showed that resistance to photoinhibition in the revertant correlated with an enhanced rate of incorporation of D1 into the membrane compared to mutant G109A/G110A. The sensitivity to photoinhibition shown by the G109A/G110A mutant is therefore consistent with a perturbation to the D1 repair cycle possibly at the level of D1 synthesis or incorporation of D1 into the PS II complex.Abbreviations DCMU- 3-(3,4-dichlorophenyl)-1,1-dimethylurea - Hepes- 4-(2-hydroxyethyl)-1-piperazineethanesulfonic acid - Mes- 4-morpholineethanesulfonic acid - PCR- polymerase chain reaction - PS II- Photosystem II - TL- thermoluminescence - PQ- plastoquinone - PS II^–- absence of PS II activity - PS^–- incapable of photoautotrophic growth - Q_A- primary plastoquinone electron acceptor - Q_B- secondary plastoquinone electron acceptor - SDS- sodium dodecyl sulphate     

Theoretical stability diagram of solvent-containing black lipid films

Recently, we have developed an analytical, semi-microscopic theory for the macroscopic behavior of a solvent-containing black lipid film subjected to an electric cross film voltage, . Here we employ the theoretical expressions derived for the disjoining pressure, _D, the film elasticity, _F, and the film tension, _F, to construct the stability diagram of the film, in the _D-. Depending on its state (_D, ), the film is stable or is prone to squeezing or bending deformations. For a monooleate film we show how the destruction of the plane film due to a periodic thickness fluctuation (squeezing) is facilitated by two mechanisms: i) lowering of _D at fixed ; ii) lowering of at fixed _D, provided that the film is in a stable state characterized by _D<–7.03×10³ dyne/cm² and >0 mV. Bending of a low tension film (single interface tension _s 0.025 dyne/cm¹) can be achieved only for >170 mV and _D > –8.7 × 10⁴ dyne/cm². Finally, we demonstrate the existence of a marginal state ( _D ⁰ , ⁰) where the film is predicted to exhibit strong fluctuations both in the squeezing and in the bending mode.     

Chlorophyll interference with phytochrome measurement

Measurements of phytochrome by (A_{725–815 nm}) were completely suppressed at chlorophyll concentrations of the order of 20–40 g g^-1 f.wt. in vivo and 37 g cm^-3 in vitro, and the readings were reduced by 50% at only 12 g cm^-3 in vitro. At these concentrations of chlorophyll in aqueous methanol, the loss of phytochrome signal in vitro appeared to be due to failure of phytochrome photoconversion rather than to interference with A measuremebt by chlorophyll fluorescence in the 125/815 nm measuring beam.Abbreviations Chl chlorophyll - P phytochrome - P_r and P_fr phytochrome in red absorbing and far-red absorbing forms     

Ion transport across the early chick embryo: I. Electrical measurements,ionic fluxes and regional heterogeneity

The chick blastoderm at the stage of late gastrula is a flat disc formed by three cell layers and exhibiting epithelial properties. Blastoderms were cultured in miniature chambers and their electrophysiological characteristics were determined under Ussing conditions.Under open-circuit condition and identical physiological solutions on both sides, spontaneous transblastodermal potential difference (V _oc) of –7.5±3.3 mV (ventral side positive) was measured. Under short-circuit condition (transblastodermal V = 0 mV), the blastoderm generated short-circuit current (I _sc) of 21±8 A/cm², which was entirely dependent on extracellular sodium, sensitive to ouabain applied ventrally and independent of extracellular chloride. The net transblastodermal Na⁺ flux fully accounted for the measured I _sc, both under control conditions and with ouabain. The total transblastodermal resistance (R _tot) was 390±125 cm².Frequently, the V _oc, I _sc and R _tot showed spontaneous oscillations with a period of 4–5 min. Removal of endoderm and mesoderm did not significantly affect the electrical properties, indicating that the electrogenic sodium transport is generated by the ectoderm.The V _oc and I _sc measured in the area pellucida (–1.3±0.8 mV, 9.3±4.4 A/cm²) and extraembryonic area opaca (–7.8±1.1 mV, 31.2±12.7 A/cm²) were significantly different. Such a heterogeneous distribution of electrical properties can explain the presence in the blastoderm of extracellular electrical currents found by using a vibrating probe.This work was supported by the Swiss National Research Foundation (grant. 3.418-0.86 to P.K.) and by Roche Research Foundation (grant. to U.K.). We thank Drs. E. Raddatz and Y. de Ribaupierre for helpful discussions.     

Use of 4-Thiouridine and 4-Thiothymidine in Studies on Pyrimidine Nucleoside Phosphorylases

The new substrates 4-thiouridine and 4-thiothymidine were proposed for spectrophotometric measurement of the activity of uridine (UP) and thymidine (TP) phosphorylases. At pH 7.5, 4-thiouridine has an absorbance maximum at 330 nm, and the difference in extinction coefficient () between 4-thiouridine and 4-thiouracil is 3000 ^–1cm^–1. 4-Thiouridine proved to be a good substrate for UP: the Michaelis ( ) and catalytic (k _cat) constants were estimated respectively at 130 M and 49 s^–1 at 25°C. Even a greater (5000 M^–1cm^–1 at 336 nm) was observed for the 4-thiothymidine/4-thiothymine pair.     

Mechanisms of 1,25(OH)2D3-induced rapid changes of membrane potential in proximal tubule: Role of Ca2+-dependent K+ channels

Summary Eleven different secosteroids or steroids (10^–10 to 10^–8 m) were acutely and reversibly introduced in solutions delivered to the lumen of single proximal tubules of the amphibianNecturus kidney while recording basolateral cell membrane potentialV _m. Seven of these molecules (1,25(OH)₂D₃, 25(OH)D₃, 24,25(OH)₂D₃, 5,6-trans-25(OH)D₃, 19-diol-cholesterol, estradiol and testosterone) resulted in changes ofV _m (V _m) occurring in a few seconds, the largest V _m being observed with 1,25(OH)₂D₃, +6.5±0.75 mV (n=19); these seven (seco)steroids but not the four inactive sterols (vitamin D₃, cholesterol, 1D₃ and aldosterone) possess a hydroxyl group on at least one carbon of the C₁₇ to C₂₅ lateral chain of the sterol ring. The V _m effect was present in Na⁺-free or Cl^–-free media, but it was abolished in HCO₃-free media. Depolarization of cell membrane potential by addition of glucose, 11mm, in luminal perfusion fluid abolished the 1,25(OH)₂D₃-evoked V _m effect, suggesting dependence of the latter on the absolute value of membrane potential. Barium, a blocking agent of K⁺ conductances, suppressed the 1,25(OH)₂D₃-evoked V _m effect, even when the proper effects of barium of cell membrane potential were canceled by current clamp. Pretreatment with quinine, a putative blocker of Ca²⁺-dependent K⁺ channels also abolished the 1,25(OH)₂D₃-evoked depolarization. Such observations are consistent with the presence of Ca²⁺-dependent K⁺ channels at the apical cell membrane of the proximal tubule, these channels being inactivated by 1,25(OH)₂D₃ and probably by other (seco)steroids.     

Extracellular amylolytic system of the yeast Lipomyces kononenkoae

Summary A strain of the yeast Lipomyces kononenkoae which converted starch into SCP with a high yield, produced three extracellular amylases which were purified from the culture fluid by Ficoll concentration, dialysis, isopropanol precipitation and DE-cellulose chromatography: an -amylase, a glucoamylase and a debranching transferase. The latter transferred -1,6-glucosyl units from panose to glucose forming maltose and appeared to have some debranching activity on amylopectin. The -amylase had the following properties: MW 38000 daltons; no effect of added calcium ions on activity; optimum temperature and pH for activity around 40°C and pH 5.5; H and S of heat inactivation 24360 cal mol^–1 and 29.2 cal deg^–1 mol^–1; range of pH stability pH 4–6.5; pI=7.1; final low molecular weight products of starch hydrolysis, maltose and glucose; K_m (40°C, pH 5.5) for starch 2.7 gl^–1, for maltotriose 109 gl^–1; uncompetitive inhibition by maltose with K_i (40°C, pH 5.5) 29.5 gl^–1. The glucoamylase had the following properties: MW 81500 daltons; optimum temperature and pH for activity around 50°C and pH 4.5: H and S of heat inactivation 20400 cal mol^–1 and 17.7 cal deg^–1 mol^–1; range of pH stability pH 4–6.5; pI=6.1; K_m (30°C, pH 4.5) for soluble starch 16.2 gl^–1, for maltose 0.36 gl^–1, for p-nitrophenyl--D-glucoside 0.35 gl^–1; competitive inhibition by glucose with K_i (30°C, pH 4.5) 4.7 gl^–1.     

Proton uptake upon quinone reduction in bacterial reaction centers: IR signature and possible participation of a highly polarizable hydrogen bond network

The light-induced Q _A ^– /Q_A FTIR difference spectra of Rb. sphaeroides and Rp. viridis show very broad positive bands of small amplitude peaking around 2750 cm^–1. Upon ¹H/²H exchange these bands shift to about 2150 cm^–1. Similarly, the Q _B ^– /Q_B spectra exhibit broad continuum bands at 2600 and 2800 cm^–1 shifting to 2100 and 2200 cm^–1 in ²H₂O for Rb. sphaeroides and Rp. viridis, respectively. These continuum bands are tentatively interpreted in terms of highly polarizable hydrogen bonds in a large web of polar bonds involving cofactors, amino acid residues, and structured water molecules. As a working hypothesis, we propose that the protons participating in this web redistribute upon quinone reduction, increasing their concentration around the newly formed charged species, and leading to net proton uptake. Assuming that the precise localization of the mobile protons is dependent on the local electrostatic, this model can explain the apparent discrepancies between some results of FTIR experiments and of electrostatic calculations. Notably, it could help rationalize the observation that mobile protons tend to localize on Glu L212 upon Q_B reduction in Rb. sphaeroides, while for Q_B reduction in Rp. viridis and for Q_A reduction in both Rb. sphaeroides and Rp. viridis, proton uptake by a small number of carboxylic residues is not supported by the FTIR data.     

Expression of Bacillus thuringiensis full-length and N-terminally truncated vip184 gene in an acrystalliferous strain of subspecies kurstaki

Vip3A is an 89-kDa protein secreted by Bacillus thuringiensis during vegetative growth. The 3.5 kb full-length vip184 gene was cloned from a wild-type isolate of B. thuringiensis, and the vip184S gene was constructed by deletion of the putative signal peptide encoding sequence. Both genes were expressed in the acrystalliferous strain Cry^–B of B. thuringiensis. Vip184 protein was observed mainly in the centrifuged pellets of B. thuringiensis Cry^–B(pHPT3), which contains the vip184 gene, and was less abundant in the concentrated supernatant. However, Vip184S proteins were not detected in the concentrated supernatant, but only in the pellets of Cry^–B(pHPT3S), which contains vip184S gene. This indicated that Vip184S proteins were not secreted into the culture medium and that the putative signal peptides were essential for the secretion of Vip184. The toxicity of Cry^–B(pHPT3) and Cry^–B(pHPT3S) were demonstrated against the neonate larvae of Spodoptera exigua and S. litura. Pellets and concentrated supernatant of Cry^–B(pHPT3) showed high activity against S. exigua and S. litura, but the Cry^–B(pHPT3S) strain was not toxic to either because of the deletion of N-terminal putative signal peptides. Therefore, this may suggest that the putative signal peptides are required for lethality.