Characterization of a voltage-dependent cation-channel from the plasma membrane of rye (Secale cereale L.) roots in planar lipid bilayers

Plasma-membrane vesicles were purified by aqueous-polymer two-phase partitioning of a microsomal membrane fraction from rye (Secale cereale L.) roots and incorporated into planar 1-palmitoyl-2-oleoyl phosphatidylethanolamine bilayers. A voltage-dependent cation-channel became incorporated into the bilayer with its cytoplasmic surface facing the trans compartment (which was grounded) and was characterized from single-channel recordings. The channel had a unitary conductance of 174 pS in symmetrical 100 mM KCl. The selectivity towards monovalent cations, determined from both conductance measurements in symmetrical 100 mM cation chloride and from permeability ratios in the presence of (cis: trans) 100 mM cation chloride: 100 mM KCl, was CsKRb>Na. The channel was also permeable to both Ba²⁺ and Ca²⁺. Although the unitary conductances in symmetrical 100 mM BaCl₂ and CaCl₂ were only 46 pS and 40 pS, respectively, the apparent permeabilities of the divalent cations relative to K⁺ were greater than expected (P_KP_BaP_Ca, 1.001.662.60). This anomaly might result from competition between divalent and monovalent cations for an intrapore binding site. The channel exhibited complex gating kinetics, which were modulated in response to changes in the zero-current (reversal) potential of the channel (E_rev). In symmetrical 100 mM KCl the channel inactivated at positive voltages greater than 100 mV and the activated channel exhibited a high probability of being in an open-state (P₀>0.90) at all voltages between ±100 mV. Channel P₀ approximated unity at voltages in the range -60 to +20 mV. As more-negative voltages were applied, P₀ decreased gradually. In contrast, as more positive voltages were applied, P₀ decreased initially to a local minimum (approaching P₀=0.90), then increased as the voltage was further increased before declining at extreme positive voltages. Under physiologically relevant ionic conditions, with 100 mM KCl plus contaminant Ca²⁺ on the trans (cytoplasmic) side and 1 mM KCl plus 2 mM CaCl₂ on the cis (extracellular) side of the channel, E_rev was 25.2 mV and the relative permeability P_Ca/P_K was 7.45. Thus, the channel would be activated by plasma-membrane depolarization in vivo and facilitate Ca²⁺ influx and net K⁺ efflux. A role in intracellular signalling is proposed for this channel. It could open in response to stimuli which depolarize the plasma membrane, allowing Ca²⁺ into the cytoplasm and, thereby, initiating a cellular response. The outward K⁺ current would act to stabilize the trans-plasma membrane voltage, preventing excessive depolarization during Ca²⁺ influx.Abbreviations and Symbols E_K Nernst (equilibrium) potential for potassium ions - E_rev zero-current (reversal) potential of the channel - _c apparent mean lifetime of the activated-channel closed-state - _o apparent mean lifetime of the activated-channel open-state - PE dephosphatidylethanolamine - P_O probability of finding the activated channel in an open-state This work was supported by the Agriculture and Food Research Council and by a grant from the Science and Engineering Research Council Membrane Initiative (GR/F 33971) to Prof. E.A.C. MacRobbie (University of Cambridge).     

Ion Regulation of the Kinetics of Potential-Dependent Potassium Channels

We apply a theoretical approach developed earlier. The interaction ofions that permeate a channel with slowly relaxing charged channel-forminggroups (ion-conformational interaction – ICI) is addressed by thisapproach. One can describe the ion concentration influence (ion regulation)on channel functioning in this manner. A patch-clamp method in awhole-cell configuration is used to study the ICI. For this purpose theinfluence of an external concentration of potassium ions on thepotential-dependent potassium current (I_A) in the externalmembrane of GH₃ cells was studied. The increase of[K⁺ _out] from 5 mM to 100 mM causes anon-monotonous shift of current-voltage dependencies. The dependence of bothan activation time constant tgr_n and a steady-state activation(n) on [K⁺]_out have a minimum andmaximum respectively. The analysis of the results suggests that the observedeffects are caused by ICI. A physical model is developed to describe thedependence of the potassium channel kinetics on the external concentrationof the ions and the membrane potential. The deformation of the closedstate of the gate and the corresponding energy shifts cause the observednon-monotonous dependencies due to ICI. Thus, the general theoreticalapproach has an experimental confirmation and is applied to concreteexamples. Formulas for concentrational dependencies of the channel kineticsare given for practical uses.     

Potassium channels from the plasma membrane of rye roots characterized following incorporation into planar lipid bilayers

Plasma membrane was purified from roots of rye (Secale cereale L. cv. Rheidol) by aqueous-polymer two-phase partitioning and incorporated into planar bilayers of 1-palmitoyl-2-oleoyl phosphatidylethanolamine by stirring with an osmotic gradient. Since plasmamembrane vesicles were predominantly oriented with their cytoplasmic face internal, when fused to the bilayer the cytoplasmic side of channels faced the trans chamber. In asymmetrical (cis:trans) 280100 mM KCl, five distinct K⁺-selective channels were detected with mean chord-conductances (between +30 and -30 mV; volyages cis with respect to trans) of 500 pS, 194 pS, 49 pS, 21 pS and 10 pS. The frequencies of incorporation of these K⁺ channels into the bilayer were 48, 21, 50, 10 and 9%, in the order given (data from 159 bilayers). Only the 49 pS channel was characterized further in this paper, but the remarkable diversity of K⁺ channels found in this preparation is noteworthy and is the subject of further study. In symmetrical KCl solutions, the 49 pS channel exhibited non-ohmic unitary-current/voltage relationships. The chord-conductance (between +30 and-30 mV) of the channel in symmetrical 100 mM KCl was 39 pS. The unitary current was greater at positive voltages than at corresponding negative voltages and showed considerable rectification with increasing positive and negative voltages. This would represent inward rectification in vivo. Gating of the channel was not voltage-dependent and the channel was open for approx. 80% of the time. Presumably this is not the case in vivo, but we are at present uncertain of the in vivo controls of channel gating. The distribution of channel-open times could be approximated by the sum of two negative exponential functions, yielding two open-state time constants (_o, the apparent mean lifetime of the channel-open state) of 1.0 ms and 5.7 s. The distribution of channel-closed times was best approximated by the sum of three negative exponential functions, yielding time constants (_c, the apparent mean lifetime of the channel-closed state) of 1.1 ms, 51 ms and 11 s. This indicates at least a five-state kinetic model for the activity of the channel. The selectivity of the 49 pS channel, determined from both reversal potentials under biionic conditions (100 mM KCl100 mM cation chloride) and from conductance measurements in symmetrical 100 mM cation chloride, was Rb⁺ K⁺ > Cs⁺ > Na⁺ > Li⁺ > tetraethylammonium (TEA⁺). The 49 pS channel was reversibly inhibited by quinine (1 mM) but TEA⁺ (10 mM), Ba²⁺ (3 mM), Ca²⁺ (1 mM), 4-aminopyridine (1 mM) and charybdotoxin (3 M) were without effect when applied to the extracellular (cis) surface.Abbreviations and Symbols GHK Goldman-Hodgkin-Katz - I/V current/voltage - PEG polyethyleneglycol - P_o probability o f the channel being open - TEA⁺ tetraethylammonium - _c apparent mean lifetime of the channel-closed state - _o apparent mean lifetime of the channel-open state P.J.W. was supported by a grant from the Science and Engineering Research Council Membrane Initiative (GR/F 33971) to Professor E.A.C. MacRobbie and M.T. by the Glaxo Junior Research Fellowship at Churchill College, Cambridge. We thank Dr. D.T. Cooke (AFRC, Long Ashton Research Station, University of Bristol, UK) and Ms. J. Marshall (University of York, UK) for their advice and assistance with the aqueous-polymer two-phase partitioning of plasma membrane from rye roots, Mr. J. Banfield and Miss P. Parmar (University of Cambridge, UK) for technical assistance and Professor E.A.C. MacRobbie, Dr. G. Thiel (University of Cambridge, UK), Dr. M.R. Blatt (Wye College, University of London, UK), Dr. D. Sanders and Dr. E. Johannes (University of York, UK) for helpful discussions.     

The effect of humidity and light on cellular water relations and diffusion conductance of leaves ofTradescantia virginiana L.

Turgor (_p) and osmotic potential (_s) in epidermal and mesophyll cells, in-situ xylem water potential (-xyl) and gas exchange were measured during changes of air humidity and light in leaves ofTradescantia virginiana L., Turgor of single cells was determined using the pressure probe. Sap of individual cells was collected with the probe for measuring the freezing-point depression in a nanoliter osmometer. Turgor pressure was by 0.2 to 0.4 MPa larger in mesophyll cells than in epidermal cells. A water-potential gradient, which was dependent on the rate of transpiration, was found between epidermis and mesophyll and between tip and base of the test leaf. Step changes of humidity or light resulted in changes of epidermal and mesophyll turgor (_p-epi, _p-mes) and could be correlated with the transpiration rate. Osmotic potential was not affected by a step change of humidity or light. For the humidity-step experiments, stomatal conductance (g) increased with increasing epidermal turgor.g/_p-epi appeared to be constant over a wide range of epidermal turgor pressures. In light-step experiments this type of response was not found and stomatal conductance could increase while epidermal turgor decreased.Symbols E transpiration - g leaf conductance - w leaf/air vapour concentration difference - -epi water potential of epidermal cells - -mes water potential of mesophyll cells - -xyl water potential of xylem - _p-epi turgor pressure of epidermal cells - _p-mes turgor pressure of mesophyll cells - _s-epi osmotic potential of epidermal cells - _s-mes osmotic potential of mesophyll cells     

Radial transport of water across cortical sleeves of excised roots ofZea mays L.

The stationary radial volume flows across maize (Zea mays L.) root segments without steles (sleeves) were measured under isobaric conditions. The driving force of the volume flow is an osmotic difference between the internal and external compartment of the root preparations. It is generated by differences in the concentrations of sucrose, raffinose or polyethylene glycol. The flows are linear functions of the corresponding osmotic differences ( ) up to osmotic values which cause plasmolysis. The straight lines obtained pass through the origin. No asymmetry of the osmotic barrier could be detected within the range of driving forces applied ( =±0.5 MPa), corresponding to volume-flow densities of j_{v, s}=±7·10^–8 m·s^–1. Using the literature values for the reflection coefficients of sucrose and polyethylene glycol in intact roots (E. Steudle et al. (1987) Plant Physiol.84, 1220–1234), values for the sleeve hydraulic conductivity of about 1·10^–7 m·s^–1 MPa^–1 were calculated. They are of the same order of magnitude as those reported in the literature for the hydraulic conductivity of intact root segments when hydrostatic pressure is applied.Abbreviations and symbols a _s outer surface of sleeve segment - c concentration of osmotically active solute - j _{v, s} radial volume flow density across sleeve segment - Lp_s hydraulic conductivity of sleeves - Lp_r hydraulic conductivity of intact roots - _N thickness of Nernst diffusion layer - reflection coefficient of root for solute - osmotic value of bulk phase - osmotic coefficient     

Manganese accumulation in yeast cells

Summary Manganese accumulation was studied by room-temperature electron spin resonance (ESR) spectroscopy inSaccharomyces cerevisiae grown in the presence of increasing amounts of MnSO₄. Mn²⁺ retention was nearly linear in intact cells for fractions related to both low-molecular-mass and macromolecular complexes (free and bound Mn²⁺, respectively). A deviation from linearity was observed in cell extracts between the control value and 0.1 mM Mn²⁺, indicating more efficient accumulation at low Mn²⁺ concentrations. The difference in slopes between the two straight lines describing Mn²⁺ retention at concentrations lower and higher than 0.1 mM, respectively, was quite large for the free Mn²⁺ fraction. Furthermore it was unaffected by subsequent dialyses of the extracts, showing stable retention in the form of low-molecular-mass complexes. In contrast, the slope of the line describing retention of bound Mn²⁺ at concentrations higher than 0.1 mM became less steep after subsequent dialyses of the cell extracts. This result indicates that the macromolecule-bound Mn²⁺ was essentially associated with particulate structures. In contrast to Cu²⁺, Mn²⁺ had no effect on the major enzyme activities involved in oxygen metabolism except for a slight increase of cyanide-resistant Mn-superoxide dismutase activity, due to dialyzable Mn²⁺ complexes.     

Analysis of the genotypic variation in radiocaesium uptake from soil

Young spinach (Spinacia oleracea L., cv. Subito) and wheat (Triticum aestivum, cv. Tonic) plants were hydroponically grown in eight different nutrient solutions containing ¹³⁷Cs. Ca, Mg, K and NH₄ concentrations were varied whilst anion concentrations were equal in all solutions. The large differences in potassium content between spinach and wheat were not reflected in similar differences in ¹³⁷Cs content at any nutritive treatment.Both crops were also grown in a potted podzolic soil contaminated with radiocaesium. This experiment was conducted in a phytotron at two climatic conditions (summer and winter) which differed in day length and light intensity. Wheat plants had higher ¹³⁷Cs levels than spinach at both conditions. The ¹³⁷Cs levels furthermore decreased during development. The ¹³⁷Cs plant/soil solution concentration ratio was lower at the summer than at the winter conditions.     

The αβ complexes of ATP synthase: the α3β3 oligomer and α1β1 protomer

The basic structures of the catalytic portion (F₁, ₃₃) of ATP synthase are the ₃₃ hexamer (oligomer with cooperativity) and ₁₁ heterodimer (protomer). These were reconstituted from the and subunits of thermophilic F₁ (TF₁), and the ₃₃ hexamer was crystallized. On electrophoresis, both the dimer and hexamer showed bands with ATPase activity. Using the dimer and hexamer, we studied the nucleotide-dependent rapid molecular dynamics. The formation of the hexamer required neither nucleotide nor Mg. The hexamer was dissociated into the dimer in the presence of MgADP, while the dimer was associated into the hexamer in the presence of MgATP. The hexamer, like mitochondrial F₁ and TF₁, showed two kinds of ATPase activity: one was cooperative and was inhibited by only one BzADP per hexamer, and the other was inhibited by three BzADP per hexamer.     

Diversity of amyloid beta protein fragment [1-40]-formed channels

1. The lipid bilayer technique was used to characterize the biophysical and pharmacological properties of several ion channels formed by incorporating amyloid beta protein fragment (AP) 1–40 into lipid membranes. Based on the conductance, kinetics, selectivity, and pharmacological properties, the following AP[1–40]-formed ion channels have been identified: (i) The AP[1–40]-formed bursting fast cation channel was characterized by (a) a single channel conductance of 63 pS (250/50 mM KCl cis/trans) at +140 mV, 17 pS (250/50 mM KCl cis/trans) at –160 mV, and the nonlinear current–voltage relationship drawn to a third-order polynomial, (b) selectivity sequence P _K > P _Na > P _Li = 1.0:0.60:0.47, (c) P_o of 0.22 at 0 mV and 0.55 at +120 mV, and (d) Zn²⁺-induced reduction in current amplitude, a typical property of a slow block mechanism. (ii) The AP[1–40]-formed spiky fast cation channel was characterized by (a) a similar kinetics to the bursting fast channel with exception for the absence of the long intraburst closures, (b) single channel conductance of 63 pS (250/50 KCl) at +140 mV 17 pS (250/50 KCl) at –160 mV, the current–voltage relationship nonlinear drawn to a third-order polynomial fit, and (c) selectivity sequence P _Rb > P _K > P _Cs > P _Na > P _Li = 1.3:1.0:0.46:0.40:0.27. (iii) The AP[1–40]-formed medium conductance channel was charcterized by (a) 275 pS (250/50 mM KCl cis/trans) at +140 mV and 19 pS (250/50 mM KCl cis/trans) at –160 mV and (b) inactivation at V_ms more negative than –120 and more positive than +120 mV. (iv) The AP[1–40]-formed inactivating large conductance channel was characterized by (a) fast and slow modes of opening to seven multilevel conductances ranging between 0–589 pS (in 250/50 mM KCl) at +140 mV and 0–704 pS (in 250/50 mM KCl) at –160 mV, (b) The fast mode which had a conductance of <250 pS was voltage dependent. The inactivation was described by a bell-shaped curve with a peak lag time of 7.2 s at +36 mV. The slow mode which had a conductance of >250 pS was also voltage dependent. The inactivation was described by a bell-shaped curve with a peak lag time of 7.0 s at –76 mV, (c) the value of P _K/P _choline for the fast mode was 3.9 and selectivity sequence P _K > P _Cs > P _Na > P _Li = 1.0:0.94:0.87:0.59. The value of P _K/P _choline for the slow mode was 2.7 and selectivity sequence P _K > P _Na > P _Li > P _Cs = 1.0:0.59:0.49:0.21, and (d) asymmetric blockade with 10 mM Zn²⁺-induced reduction in the large conductance state of the slow mode mediated via slow block mechanism. The fast mode of the large conductance channel was not affected by 10 mM Zn²⁺.2. It has been suggested that, although the bursting fast channel, the spiky fast channel and the inactivating medium conductance channel are distinct, it is possible that they are intermediate configurations of yet another configuration underlying the inactivating large conductance channel. It is proposed that this heterogeneity is one of the most common features of these positively-charged cytotoxic amyloid-formed channels reflecting these channels ability to modify multiple cellular functions.3. Furthermore, the formation of -sheet based oligomers could be an important common step in the formation of cytotoxic amyloid channels.     

Transport of phenylalanine into vacuoles isolated from barley mesophyll protoplasts

The energy-dependent transport of phenylalanine into isolated vacuoles of barley (Hordeum vulgare L.) mesophyll protoplasts has been studied by silicone-layer floatation filtering. The uptake of this aromatic amino acid into the vacuolar compartment is markedly increased by MgATP, showing saturation kinetics; the K _m values were 0.5 mM for MgATP and 1.2 mM for phenylalanine. V _max for phenylalanine transport was estimated to 140 nmol phenylalanine·(mg·Chl)^-1·h^-1. The transport shows a distinct pH optimum at 7.3 and is markedly inhibited by 40 mM nitrate. Azide (1 mM) and vanadate (400 M) had no or little effect on rates of transport while p-fluorophenylalanine seemed to be an effective inhibitor, indicating a possible competition at an amino-acid carrier. Ionophores such as valinomycin, nigericin or gramicidin were strong inhibitors of phenylalanine transport, indicating that this process is coupled to both the transmembrane pH gradient (pH) and the transmembrane potential ().Abbreviations and symbols BSA bovine serum albumin - Chl chlorophyll - Hepes 4-(2-hydroxyethyl)-1-piperazineethanesulfonic acid - pH transmembrane pH gradient - transmembrane potential     

Mouse–Torpedo Chimeric α-Subunit Used to Probe Channel-Gating Determinants on the Nicotinic Acetylcholine Receptor Primary Sequence

1. To determine if structural domains are important for nicotinic acetylcholine receptor (nAChr) channel function, six mouse–Torpedo chimeric -subunits were constructed (Fig. 2) and coexpressed with Torpedo californica -, -, and -subunits in Xenopus laevis oocytes.2. nAChRs containing a chimeric -subunit were examined by voltage- and patch-clamp methods to determine their functional characteristics. Dose–response curves from voltage-clamped oocytes were used to estimate EC₅₀'s and Hill coefficients. Whole-cell currents were normalized against the -bungarotoxin (-BTX) binding sites to obtain normalized responses to acetylcholine (ACh). Open time constants at 4 M ACh were used to examine single-channel behavior.3. The EC₅₀ for ACh was modulated by the N-terminal half of the -subunit. When the Torpedo subunit sequence between position 1 and position 268 was replaced by mouse sequence, the EC₅₀ shifted toward the value for the wild-type mouse subunit. Replacement of either the 1–159 or the 160–268 positions of the Torpedo sequence with the mouse sequence lowered the EC₅₀. This suggests that at least two regions play a role in determining the EC₅₀.4. When the primary sequence (160–268) of the Torpedo -subunit was introduced in the mouse -subunit (T160–268), the expressed chimeric receptor was nonfunctional. The inverse chimera (M160–268) was functional and the open time constant and EC₅₀ were similar to those of mouse but the normalized response was characteristic of Torpedo.5. The normalized macroscopic response to ACh (300 M) of the chimera containing the mouse -subunit showed a ninefold increase relative to the Torpedo wild type. Receptors which contain the C terminal of the mouse -subunit also show an increase in the maximum normalized current. Receptors with the -subunit which contain the Torpedo C-terminal sequence have a lower normalized response.6. The combined results suggest that AChR channel function is modulated by structural determinants within the primary sequence. These structural domains might modulate channel function through specific allosteric interactions. The lack of response of the T160–268 chimera suggests that a critical interaction essential for the coupling of agonist binding and channel gating was disrupted. This result suggests that the interaction of structural domains within the nAChR primary structure are essential for channel function and that these intractions could be very specific within different nAChR species.     

Inheritance of mitochondrial DNA in lentil (Lens culinaris Medik.)

Restriction fragment analysis was used to examine the inheritance of lentil mitochondrial DNA (mtDNA) in F₁ and F₅ progeny from intrasubspecific (Lens culinaris ssp. culinaris) crosses and in F₁ progeny from intersubspecific (Lens culinaris ssp. orientalis x L. culinaris ssp. culinaris) crosses. Southern blots of digested parental and progeny DNA were hybridized to heterologous maize mtDNA probes specific to coxI and atp6 genes. Two restriction fragment polymorphisms separated L.c. ssp. culinaris Laird and Eston from L.c. ssp. culinaris ILL5588, and one restriction fragment polymorphism distinguished L.c. ssp. culinaris Laird and Eston from L.c. ssp. orientalis LO4. Twelve of 13 f₁ progeny and all F₅ progeny from the intrasubspecific crosses, and all F₁ progeny from intersubspecific crosses had only maternal mtDNA restriction fragments. One f₁ plant from an Eston x ILL5588 cross inherited mtDNA fragments from both parents. Nuclear DNA inheritance was biparental in all F₁ progeny.NRCC No. 38451     

Identification of two RAPD markers tightly linked with the Nicotiana debneyi gene for resistance to black root rot of tobacco

Linkage of randomly amplified polymorphic DNA (RAPD) markers with a single dominant gene for resistance to black root rot (Chalara elegans Nag Raj and Kendrick; Syn. Thielaviopsis basicola [Berk. and Broome] Ferraris) of tobacco (Nicotiana tabacum L.), which was transferred from N. debneyi Domin, was investigated in this study. There were 2594 repeatable RAPD fragments generated by 441 primers on DNAs of Delgold tobacco, a BC₅F₈ near isogenic line (NIL) carrying the resistance gene in a Delgold background, and PB19, the donor parent of the resistance gene. Only 7 of these primers produced eight RAPD markers polymorphic between Delgold and PB19, indicating there are few RAPD polymorphisms between them despite relatively dissimilar pedigrees. Five of the eight RAPD markers were not polymorphic between Delgold and the NIL. All of these markers proved to be unlinked with the resistance gene in F₂ linkage tests. Of the remaining three RAPD markers polymorphic between Delgold and the NIL, two were shown to be strongly linked with the resistance gene; one in coupling and the other in repulsion. Application of the two RAPDs in the elimination of linkage drag associated with the N. debneyi resistance gene and marker-assisted selection for the breeding of new tobacco cultivars with the resistance gene is discussed.     

Contrasting leaf and ‘ecosystem’ CO2 and H2O exchange in Avena fatua monoculture: Growth at ambient and elevated CO2

Elevated CO₂ (ambient + 35 Pa) increased shoot dry mass production in Avena fatua by 68% at maturity. This increase in shoot biomass was paralleled by an 81% increase in average net CO₂ uptake (A) per unit of leaf area and a 65% increase in average A at the ecosystem level per unit of ground area. Elevated CO₂ also increased ecosystem A per unit of biomass. However, the products of total leaf area and light-saturated leaf A divided by the ground surface area over time appeared to lie on a single response curve for both CO₂ treatments. The approximate slope of the response suggests that the integrated light saturated capacity for leaf photosynthesis is 10-fold greater than the ecosystem rate. Ecosystem respiration (night) per unit of ground area, which includes soil and plant respiration, ranged from-20 (at day 19) to-18 (at day 40) mol m^-2 s^-1 for both elevated and ambient CO₂ Avena. Ecosystem below-ground respiration at the time of seedling emergence was -10 mol m^-2 s^-1, while that occuring after shoot removal at the termination of the experiment ranged from -5 to-6 mol m^-2 s^-1. Hence, no significant differences between elevated and ambient CO₂ treatments were found in any respiration measure on a ground area basis, though ecosystem respiration on a shoot biomass basis was clearly reduced by elevated CO₂. Significant differences existed between leaf and ecosystem water flux. In general, leaf transpiration (E) decreased over the course of the experiment, possibly in response to leaf aging, while ecosystem rates of evapotranspiration (ET) remained constant, probably because falling leaf rates were offset by an increasing total leaf biomass. Transpiration was lower in plants grown at elevated CO₂, though variation was high because of variability in leaf age and ambient light conditions and differences were not significant. In contrast, ecosystem evapotranspiration (ET) was significantly decreased by elevated CO₂ on 5 out of 8 measurement dates. Photosynthetic water use efficiencies (A/E at the leaf level, A/ET at the ecosystem level) were increased by elevated CO₂. Increases were due to both increased A at leaf and ecosystem level and decreased leaf E and ecosystem ET.     

Genetic characteristics of two genes for resistance to soybean mosaic virus in PI486355 soybean

Soybean [Glycine max (L.) Merr.] PI486355 is resistant to all the identified strains of soybean mosaic virus (SMV) and possesses two independently inherited resistance genes. To characterize the two genes, PI486355 was crossed with the susceptible cultivars Lee 68 and Essex and with cultivars Ogden and Marshall, which are resistant to SMV-G1 but systemically necrotic to SMV-G7. The F₂ populations and F₂₃ progenies from these crosses were inoculated with SMV-G7 in the greenhouse. The two resistance genes were separated in two F₃₄ lines, LR1 and LR2, derived from Essex x PI486355. F₁ individuals from the crosses of LR1 and LR2 with Lee 68, Ogden, and York were tested with SMV-G7 in the greenhouse; the F₂ populations were tested with SMV-G1 and G7. The results revealed that expression of the gene in LR1 is gene-dosage dependent, with the homozygotes conferring resistance but the heterozygotes showing systemic necrosis to SMV-G7. This gene was shown to be an allele of the Rsv1 locus and was designated as Rsv1-s. It is the only allele identified so far at the Rsv1 locus which confers resistance to SMV-G7. Rsv1-s also confers resistance to SMV-G1 through G4, but results in systemic necrosis with SMV-G5 and G6. The gene in LR2 confers resistance to strains SMV-G1 through G7 and exhibits complete dominance. It appears to be epistatic to genes at the Rsv1 locus, inhibiting the expression of the systemic necrosis conditioned by the Rsv1 alleles. SMV-G7 induced a pin-point necrotic reaction on the inoculated primary leaves in LR1 but not in LR2. The unique genetic features of the two resistance genes from PI486355 will facilitate their proper use and identification in breeding and contribute to a better understanding of the interaction of SMV strains with soybean resistance genes.     

Ion permeation through single channels activated by acetylcholine in denervated toad sartorius skeletal muscle fibers: Effects of alkali cations

Summary The gigaohm seal technique was used to study ion permeation through acetylcholine-activated channels in cell-attached patches of the extrajunctional membrane of chronically denervated, enzyme-treated cells from the sartorius muscle of the toadBufo marinus. The most frequently occurring channel type (>95% of channel openings), provisionally classified as extrajunctional, had a chord conductance of approximately 25 pS under normal conditions (–70 mV, 11°C, Normal Toad Ringer's). The less frequently observed channel type (<5% of channel openings), classified as a junctional type, had a conductance of 35 pS under the same conditions, and a similar null potential. In many patches, a small percentage (usually <2%) of openings of the extrajunctional channel displayed a lower conductance state. The shape of theI–V curves obtained for the extrajunctional channel dependend on the predominant extracellular cation. For Cs and K, theI–V curves were essentially linear over the voltage range +50 to –150 mV across the patch, suggesting that the potential independent component of the energy profile within the channel was symmetrical. For Li, theI–V curve was very nonlinear, displaying a significant sublinearity at hyperpolarized potentials. Both an electrodiffusion and a symmetrical uniform four-barrier, three-site rate-theory model provided reasonable fits to the data, whereas symmetrical two-barrier, single-site rate-theory models did not. For the alkali cations examined, the relative permeability sequence wasP _Cs>P _K>P _Na>P _Li—a proportional selectivity sequence. This was different from the single channel conductance sequence which was found to be _K> _Cs> _Na> _Li implying that ions do not move independently through the channel. The relative binding constant sequence for the channel sites was found to be a polarizability sequence, i.e.,K _Li>K _Cs>K _Na>K _K There was an inverse relationship for the cations examined. Under conditions when the single-channel conductance was relatively high, the conductance at depolarized potentials was lower than that predicted by both electrodiffusion and rate theory models, suggesting that there was a rate-limiting access step for ions, from the intracellular compartment into the channel.     

A Kdp-like,high-affinity,K+-translocating ATPase is expressed during growth of Rhodobacter sphaeroides in low potassium media

Cells of the purple non-sulphur bacterium Rhodobacter sphaeroides express a high-affinity K⁺ uptake system when grown in media with low K⁺ concentrations. Antibodies againts the catalytic KdpB protein or the whole KdpABC complex of Escherichia coli crossreact with a 70.0 kDa R. sphaeroides protein that was expressed only in cells grown in media with low K⁺ concentrations. In membranes derived from R. sphaeroides cells grown with low K⁺ concentrations (induced cells), a high ATPase activity could be detected when assayed in Tris-HCl pH 8.0 containing 1 mM MgSO₄. This ATPase activity increased upon addition of 1 mM KCl from 166 to 289 mol ATP hydrolysed x min^-1 x g protein^-1 (1.7-fold stimulation). The K⁺-stimulated ATPase activity was inhibited approximately 93% by 0.5 mM vanadate but hardly by N,N-dicyclohexylcarbo-diimide (DCCD). These results indicate that the inducible K⁺-ATPase in R. sphaeroides resembles the Kdp K⁺-translocating ATPase of Escherichia coli. This Kdp-like transport system is also expressed in R. capsulatus and Rhodospirillum rubrum during growth in media with low K⁺ concentrations suggesting a wide distribution of this transport system among phototrophic bacteria.Abbreviations electrical potential difference across the cytoplasmic membrane - pH pH difference across the cytoplasmic membrane - BSA bovine serum albumine - PAGE polyacrylamide gel electrophoresis - HEPES 4-(2-hydroxyethyl)-1-piperazine-ethanesulfonic acid - PMSF phenyl-methyl-sulfonyl fluoride - DCCD N,N-dicyclohexylcarbodiimide - AIB 2--aminoisobutyric acid - TMG methyl--d-thiogalactopyranoside     

Labdane diterpene derivatives from Holwaya mucida

Clumps of white crystals present in 40-day-old malt agar cultures of Holwaya mucida were isolated as long white needles by crystallization from ethanol following short extraction with chloroform. The levorotary compound ([] ₂₈₉ ²¹ =-193.8°) was recognized as a -lactone (C₁₇H₂₀O₅) by infrared and mass spectrometry. It was identified as 7-methoxy-3a, 10b-dimethyl-1, 2, 3, 3a, 5a, 7, 10b, 10c-octahydro-4H, 9H-furo[2, 3, 4 : 4, 5]naphtho[2, 1-c]pyran-4, 9-dione, a labdane-derived compound known as antibiotic LL-Z1271. Preparative thin-layer chromatography of the mother liquor afforded 2 minor metabolites. One was identified as LL-Z1271, the demethylated analogue of LL-Z1271. The other one named LL-Z1271, was recognized as a compound related to and : its structure could not be fully elucidated. H. mucida (anamorph: Crinula calciiformis) has no taxonomic relationship with two other LL-Z1271 producing species viz. Acrostalagmus sp. (= Acremonium cf. atrogriseum) and Oidiodendron truncatum.     

Electric field-induced breakdown of lipid bilayers and cell membranes: A thin viscoelastic film model

Summary A simple viscoelastic film model is presented, which predicts a breakdown electric potential having a dependence on the electric pulse length which approximates the available experimental data for the electric breakdown of lipid bilayers and cell membranes (summarized in the reviews of U. Zimmermann and J. Vienken, 1982,J. Membrane Biol. 67:165 and U. Zimmermann, 1982,Biochim. Biophys. Acta 694:227). The basic result is a formula for the time of membrane breakdown (up to the formation of pores): =(/C)/( _m ² ₀ ² U ⁴/24Gh ³+T ²/Gh–1), where is a proportionality coefficient approximately equal to ln(h/2₀),h being the membrane thickness and ₀ the amplitude of the initial membrane surface shape fluctuation ( is usually of the order of unity), represents the membrane shear viscosity,G the membranes shear elasticity modules, _m the membrane relative permittivity, ₀=8.85×10^–12 Fm,U the electric potential across the membrane, the membrane surface tension andT the membrane tension. This formula predicts a critical potentialU _c ;U _c =(24Gh ³/ _m ² ₀ ² )^1/4 (for = andT=0). It is proposed that the time course of the electric field-induced membrane breakdown can be divided into three stages: (i) growth of the membrane surface fluctuations, (ii) molecular rearrangements leading to membrane discontinuities, and (iii) expansion of the pores, resulting in the mechanical breakdown of the membrane.