Epithelial action potentials inOikopleura (Tunicata: Larvacea)

Summary The passive electrical properties and initiation of action potentials have been examined in the external epithelium of oikopleurid larvacean tunicates. The epithelial cells are electrically coupled, and are polygons up to 200 m across and up to 1.4–2.8 m thick. Membrane constants determined by a 2-electrode study were forO. dioica:: 922 m; R_m: 4.3 kcm₂; R_i: 82.7 cm. Corresponding values for the largerO. longicauda were: 3350 m; 35.6 kcm²; and 104.5 cm. Mean resting potentials in both species were around 80 mV. Mechanical stimulation evokes over-shooting action potentials propagated (at 18 °C) at some 40 cm/s. These are rapid events, repolarisation being almost complete in 5 ms. There is no undershoot.When the recording electrode penetrates the epithelial cell from its inner surface distant mechanical stimulation may evoke similar action potentials arising from the stimulus site, but more often evokes graded small depolarisations which give rise to action potentials with increasing strength of mechanical stimulation. Reasons are given for considering these to be generator potentials resulting from deformation of the outer epithelial cell membrane by the tip of the recording electrode. The effects of epithelial action potentials upon the potentials recorded from the caudal muscle cells are briefly described.     

Miniature Ag−AgCl electrode for voltage clamping of theAmbystoma collecting duct

Summary We have developed a miniature silver-silver chloride electrode. The outer diameter of the electrodes averaged 22 m and the input resistance 8.8 k. Since the core of the electrode is a glass fiber, the problem of the extreme malleability of a small diameter silver fiber is circumvented. The properties of the electrode permit us to insert it into short (600 m) fragments of the amphibian collecting duct while they are being perfusedin vitro. The passage of currents in the range of 0 to 6×10^–8 amperes allowed us to voltage clamp the nephron fragment between +20 and –20 mV. The current-voltage plots are linear over this range. Two lines of evidence suggest that the voltage clamp is homogeneous. First, the voltage measured at the perfusion end during a voltage-clamp experiment of the tubule is not significantly different from that measured at the collecting end. Secondly, the specific resistance of collecting ducts estimated from the core conductor analysis is 3.3±0.8×10⁴ cm, a value not significantly different from that computed from the current-voltage plots as determined with the Ag–AgCl electrode, 3.0±0.5×10⁴ cm. This method permits precise control of both the ionic and electrical gradients across fragments of the amphibian collecting duct.     

Measurement of the electrical resistance of plasmodesmata and membranes of corn suspension-culture cells

Electrophysiological investigations of intercellular communication and membrane resistance in higher plants have been hampered by the difficulty in measuring these quantities independently. Uncertainty about the position of an electrode inserted into vacuolate tissue has further complicated such measurement. To overcome these problems sister cell pairs of a Zea mays L. Black Mexican Sweet suspension culture were used and dye was injected from the current-injecting electrode to determine the location of the electrode tip in each experiment. Of the impalements, 72% were cytoplasmic. The presence of plasmodesmata was fully incorporated into the electriccircuit model for the cell, and the resistance of the membrane of the current-injected cell was calculated, separate from the plasmodesmata resistance. This avoided some of the confusion resulting from work on multicellular tissue in which the position of the electrode and the extent of intercellular coupling is not determined. Using this technique, plasma-membrane resistivity was measured as 0.65 ·m², the resistivity of the tonoplast and plasma membrane in series was 1.35 ·m², and the resistance of a single plasmodesma was calculated to be 53 ± 11 G.Abbreviations BMS Black Mexican Sweet - PD potential difference - R_j resistance of the plasmodesmata in the junction between cells - R_m resistance of the plasma membrane of the current-injected cell - R_t resistance of the tonoplast - V₁, V₂ membrane PDs of sister cells This work was funded by an Australian Research Council grant to R.L.O. We are grateful to Dr. Maret Vesk (Electron Microscope Unit, The University of Sydney) for assistance with the preparation of EM sections, and to Dr. Richard Brettell (C.S.I.R.O. Division of Plant Industry) for assistance with the BMS culture.     

The intrinsic electrophysiological characteristics of fly lobula plate tangential cells: I. Passive membrane properties

The passive membrane properties of the tangential cells in the fly lobula plate (CH, HS, and VS cells, Fig. 1) were determined by combining compartmental modeling and current injection experiments. As a prerequisite, we built a digital base of the cells by 3D-reconstructing individual tangential cells from cobalt-stained material including both CH cells (VCH and DCH cells), all three HS cells (HSN, HSE, and HSS cells) and most members of the VS cell family (Figs. 2, 3). In a first series of experiments, hyperpolarizing and depolarizing currents were injected to determine steady-state I-V curves (Fig. 4). At potentials more negative than resting, a linear relationship holds, whereas at potentials more positive than resting, an outward rectification is observed. Therefore, in all subsequent experiments, when a sinusoidal current of variable frequency was injected, a negative DC current was superimposed to keep the neurons in a hyperpolarized state. The resulting amplitude and phase spectra revealed an average steady-state input resistance of 4 to 5 M and a cut-off frequency between 40 and 80 Hz (Fig. 5). To determine the passive membrane parameters R _m (specific membrane resistance), R _i (specific internal resistivity), and C _m (specific membrane capacitance), the experiments were repeated in computer simulations on compartmental models of the cells (Fig. 6). Good fits between experimental and simulation data were obtained for the following values: R _m = 2.5 kcm², R _i = 60 cm, and C _m = 1.5 F/cm² for CH cells; R _m = 2.0 kcm², R _i = 40 cm, and C _m = 0.9 F/cm² for HS cells; R _m = 2.0 kcm², R _i = 40 cm, and C _m = 0.8 F/cm² for VS cells. An error analysis of the fitting procedure revealed an area of confidence in the R _m -R _i plane within which the R _m -R _i value pairs are still compatible with the experimental data given the statistical fluctuations inherent in the experiments (Figs. 7, 8). We also investigated whether there exist characteristic differences between different members of the same cell class and how much the exact placement of the electrode (within ±100 m along the axon) influences the result of the simulation (Fig. 9). The membrane parameters were further examined by injection of a hyperpolarizing current pulse (Fig. 10). The resulting compartmental models (Fig. 11) based on the passive membrane parameters determined in this way form the basis of forthcoming studies on dendritic integration and signal propagation in the fly tangential cells (Haag et al., 1997; Haag and Borst, 1997).     

PEG-enhanced,electric field-induced fusion of tonoplast and plasmalemma of grape protoplasts

Cultured grape cells accumulate anthocyanins in vacuoles rather than secreting them into the nutrient medium. Therefore, grape cells that contain tonoplast segments in their plasmalemma should be capable of excreting anthocyanins rather than sequestering them in their vacuoles. In initial attempts to construct such novel cells, small vacuoles were fused with the plasmalemma of cultured plant cells. Protoplasts were isolated from grape calluses that produce and accumulate anthocyanins. Small vacuoles were formed by gently rupturing vacuoles isolated from grape protoplasts. Although small vacuoles and protoplasts became aligned in an AC field, the tonoplast and plasmalemma did not readily fuse when subjected to 3 DC pulses of 1200 V cm^–1 for 50 s each. Changes in the intensity, number and/or duration of the DC pulses had no effect on the fusion process. When 1.0% polyethylene glycol was added to the electrofusion buffer, however, small vacuoles and protoplasts fused within a few minutes after the DC pulses were applied. These novel grape cells remained viable for several hours.Abbreviations BSA bovine serum albumin - 2,4-D 2,4-dichloro-phenoxyacetic acid - DTT dithiothreitol - EGTA ethyleneglycol-bis-(-amino-ethyl ether)-N,N,N,N - MES 2-[N-Morpholino]ethanesulfonic acid - MOPS 3-[N-Morpholino]propanesulfonic acid - PVP polyvinylpyrrolidone     

Cellular and paracellular pathway resistances in the “tight” Cl−-secreting epithelium of rabbit cornea

Summary The high transverse resistance of the isolated rabbit cornea (6–12 k·cm²) is associated with the corneal epithelium, a Cl^–-secreting tissue which is modulated by -adrenergic and serotonergic receptors. Three methods were employed to determine the resistances for the apical membrane, basolateral membrane, and paracellular conductive pathways in the epithelium. In the first method, the specific resistance of the apical membrane was selectively and reversibly changed. Epinephrine was used to increase apical Cl^– conductance and Ag⁺ was used to increase apical cation permeability. The second method utilized a direct measure of the spontaneous cellular ionic current. The third method obtained estimates of shunt resistance using transepithelial electrophysiological responses to changes in apical membrane resistance. The results of the first method were largely independent of the agent used. In addition, the three methods were in general agreement, and the ranges of mean values for apical membrane, basolateral membrane, and shunt resistances were 23–33, 3–4, and 12–16 k·cm², respectively, for the normal cornea. The apical membrane was the major, physiologically-modulated barrier to ion permeation. The shunt resistance of the corneal epithelium was comparable to that found previously for other tight epithelia. Experiments using Ag⁺ in tissues that were bathed in Cl^– and HCO₃-free solutions indicated that under resting conditions the apical membrane is anion-selective.     

The solution conformation of sialyl-α(2→6)-lactose studied by modern NMR techniques and Monte Carlo simulations

Summary We present a comprehensive strategy for detailed characterization of the solution conformations of oligosaccharides by NMR spectroscopy and force-field calculations. Our experimental strategy generates a number of interglycosidic spatial constraints that is sufficiently large to allow us to determine glycosidic linkage conformations with a precision heretofore unachievable. In addition to the commonly used {¹H,¹H} NOE contacts between aliphatic protons, our constraints are: (a) homonuclear NOEs of hydroxyl protons in H₂O to other protons in the oligosaccharide, (b) heteronuclear {¹H,¹³C} NOEs, (c) isotope effects of O¹H/O²H hydroxyl groups on¹³C chemical shifts, and (d) long-range heteronuclear scalar coupling across glycosidic bonds.We have used this approach to study the trisaccharide sialyl-(26)-lactose in aqueous solution. The experimentally determined geometrical constraints were compared to results obtained from force-field calculations based on Metropolis Monte Carlo simulations. The molecule was found to exist in 2 families of conformers. The preferred conformations of the (26)-linkage of the trisaccharide are best described by an equilibrium of 2 conformers with angles at –60° or 180° and of the 3 staggered rotamers of the angle with a predominantgt conformer. Three intramolecular hydrogen bonds, involving the hydroxyl protons on C8 and C7 of the sialic acid residue and on C3 of the reducing-end glucose residue, contribute significantly to the conformational stability of the trisaccharide in aqueous solution. Supplementary material available from the corresponding author: Table containing values for the dihedral angles , , , , and for bond angles , for the six lowest-energy conformations of sialyl-(26)-lactose (1 page).     

Two useful dimensionless parameters that combine physiological, operational and bioreactor design parameters for improved control of dissolved oxygen

Two new dimensionless parameters ( and ) are proposed for calculating the proportional, integral, and derivative constants of a dissolved oxygen proportional integral-derivative (PID) feed-back control algorithm from knowledge of the growth rate, bioreactor design and operation variables. The values of and were determined for a broad range of Reynolds numbers (between 1000 to 40 000) during the exponential growth phase of two highly different processes: fermentations of recombinant Escherichia coli and cultures of human hematopoietic cells. The utility of and for use in dissolved oxygen self-tunning adaptive control algorithms is discussed.     

Thermodynamic compensation in microbial thermal death

Sixty eight Arrhenius plots of thermal death in six mesophilic yeast species, tested at various concentrations of NaCl, lacked an isokinetic temperature. Nevertheless the H ^#/S ^# plot was apparently linear with a slope corresponding to 314° K. It was concluded that linear thermodynamic compensation of thermal death is non-existent in heterogeneous groups of yeasts and is unlikely to occur in heterogeneous groups of other organisms and that H ^#/S ^# plots lack sensitivity for the detection of non-linearity over narrow temperature ranges.However, the H ^# and S ^# parameters of thermal death displayed non-linear compensation in such a way that the extrapolated Arrhenius plots of death attained nearly identical values near the respective maximum temperatures for growth.Linear thermodynamic compensation occurred in each of the six strains, when stationary populations of the same strain were tested at various NaCl concentrations. On the other hand, exponential populations of each of the strains, tested in the same way, lacked an isokinetic temperature of thermal death.The significance of linear and non-linear thermodynamic compensation in biological rate processes is discussed.     

A new electrical method for the determination of the cell membrane area in plant cells

The membrane are of giant algal cells of Valonia utricularis was determined electrically by using the charge-pulse technique. The membrane was charged to low voltages between 2 and 20 mV by injecting charge pulses of defined amplitude and very short duration (about 100 ns). The injected charge was calculated by measuring the current increment via a potential drop across a 10 resistance in the outer circuit and by considering the preselected charging time. The initial voltage across the membrane was calculated by extrapolation to time zero (=end of the charge pulse). From the values of the injected charge and the voltage built up initially across the membrane, the capacitance of the membrane could be calculated. Assuming that the specific capacity of the two membranes, tonoplast and plasmalemma, arranged in series was 0.5 F cm^-2, the membrane area could be derived from the membrane capacity. The electrically determined membrane area agrees with the geometrically determined one to within 10%.     

Electrical membrane potential and resistance in photoautotrophic suspension cells of Chenopodium rubrum L.

On photoautotrophically grown, suspension-cultured cells of Chenopodium rubrum L. the electrical potential difference V _mand the electrical resistance across plasmalemma and tonoplast have been measured using one or two intracellular micro-electrodes. In a mineral test-medium of 5.8 mM ionic strength V _mvalues between 100 and 250 mV, 40% thereof between 170 and 200 mV, and a mean value (±S.E.M.) of 180.6±3.4 mV have been recorded. The average membrane input resistance R _mwas 269±36 M, corresponding to an average membrane resistivity r _mof 3.0 m². V _mand r _mare sensitive to light, temperature, and addition of cyanide, suggesting the presence of an electrogenic hyperpolarizing ion pump, and are ascribed essentially to the plasmalemma. A hexose-specific saturable electrogenic membrane channel is identified through a decrease of V _mand r _mupon addition of hexoses. The hexoseconcentration-dependent depolarization V _msaturates at 92 mV and returns half-saturating concentrations (apparent k _mvalues) of 0.16 mM galactose, 0.28 mM glucose, and 0.48 mM fructose. The magnitude of V _mand r _mwell agrees with pertinent data from mesophyll cells in situ (where only V _mdata are available) and from photoautotrophic lower plant cells. However, V _mis markedly higher than reported for heterotrophically grown suspension cells of different higher plants (with which r _mdata have not been reported so far). It is concluded from the present study and a companion paper on water transport (Büchner et al., Planta, in press) that photoautotrophically grown Chenopodium suspension cells closely resemble mesophyll cells as to cell membrane transport properties.Abbreviations V _m membrane potential(mV) - R _o input resistance () - R _m membrane input resistance () - r _m specific resistance (resistivity) of the membrane (m²)     

Discrimination of objects through electrolocation in the weakly electric fish,Gnathonemus petersii

Summary Three weakly electric fish (Gnathonemus petersii) were force-choice trained in a two-alternative procedure to discriminate between objects differing in their electrical characteristics. The objects were carbon dipoles in plexiglass tubing (length 2.5 cm, diameter 0.6 cm). Their electrical characteristics could be changed by varying the impedance of an external circuit to which they were connected (Fig. 1). In one (the capacitance dipole) the resistance was very low(< 3 ) and the capcitance variable. In the other (the resistance dipole) the resistance was variable and the capacitance low (<50 pF).Capacitances from several hundred pF (lower thresholds, Fig. 2) to several hundred nF (upper thresholds, Fig. 3) could be discriminated from both insulators and good conductors. In all cases the reward-negative stimulus was the capacitance dipole, which was avoided by all fish spontaneously. Thresholds were defined at 70% correct choices.The fish were then tested for their ability to discriminate between one object with a given capacitance and another with resistances varying from 3 to 200 k. The capacitance dipole continued to be the negative stimulus throughout. All 3 fish avoided it in at least 80% of the trials at each stimulus combination (Fig. 4). This result suggests that Gnathonemus perceives the capacitance and the resistance of objects differentially.The effect of the dipole-objects as well as some natural objects on the local EOD was recorded differentially very close to the fish's skin (Fig. 5). The amplitude of the local EODs was affected by all types of objects as they approached the skin. However, the waveform was changed only by capacitance dipoles and some natural objects (Figs. 6 and 7). It appears that the fish perceive not only intensity changes in the local EOD but wave-form deformations as well and can thus distinguish objects of different complex impedances.Abbreviations EOD electric organ discharge - f _max maximal spectral frequency - GP Gnathonemus petersii - LFS local filtered signal - PMA probing motor act - S+ positive stimulus - S negative stimulus     

Separation of tonoplast and plasma membrane potential and resistance in cells of oat coleoptiles

Summary Membrane potential and resistance were recorded from parenchymal cells of oat (Avena) coleoptiles, using one and two intracellular electrodes. Membrane potential is largest (–100 mV) in impalements with low input resistance (2–4 M), and is less negative (–50 mV) in penetrations with high input resistance (> 20 m). The interpretation is that the electrode lodges in the vacuole which is positive to the cytoplasm (but still negative to the external solution), and that measurements of net membrane potential are compromised to varying degrees by leakage shunts introduced across the high resistance vacuolar membrane by the electrode. This conclusion is supported by several additional lines of evidence. (1) It is possible to convert large-R/small-V impalements into small-R/large-V penetrations by passing excess current through the electrode or by briefly ringing the capacitance neutralization circuit in the amplifier. The cells usually recover their resistance in a few minutes, with a concomitant decrease in the negativity of the membrane potential. (2) Changes in external [K] affect the measuree potential by an amount that is independent of the input resistance of the impalement. This is consistent with an effect of [K] _o on the potential of the plasma membrane and the occurrence of leakage shunts primarily at the tonoplast. (3) Quantitatively, the effects of a change in [K] _o on resistance indicate that nearly 90 percent of the input resistance of unshunted cells resides in the tonoplast. (4) The effects of metabolic inhibitors (DNP, CN^–) on potential are smaller in large-R than in small-R impalements. This observation suggests there are electrogenic pumps contributing to the membrane potential at both the plasmalemma and tonoplast. Finally, we conclude that with an electrode in the vacuole it is possible to record potentials that are dominated by the contribution of the plasma membrane, provided care is taken to select impalements combining both large, negative potential and low input resistance.     

Electrotonic spread of current in monolayer cultures of neonatal rat heart cells

Summary The passive electrical properties of neonatal rat heart cells grown in monolayer cultures were determined. Hyperpolarizing current pulses were injected through one microelectrode via an active bridge circuit. Membrane voltage displacements caused by the injected current pulses were measured at various distances from the first with a second microelectrode. Using a modified least-squares method the experimental results were fitted to a Bessel function, which is the steady-state solution of the differential equation describing the relation between membrane voltage caused by current injection and interelectrode distance in a very large and very thin plane cell. Best fit was obtained with a space constant of 360 m and an internal resistivity of 500 cm. From these figures, specific membrane resistance was calculated to be 1,300 cm², assuming all current to leave through the upper surface of the monolayer.The time constant of the membrane was measured from the time course of the current-induced membrane voltage displacements. From its value of 1.7 msec a membrane capacity of 1.3 F/cm² was calculated.From these results and some literature data on nexus distribution (A. W. Spira,J. Ultrastruct. Res. 34:409, 1971) specific nexus resistance was calculated to range between 0.25 and 1.25 cm², depending on the amount of folding of the intercalated discs. The results suggest that spread of activation in monolayer cultures of heart cells by means of local circuit currents is very likely.     

Electrical properties of parenchymal cell membranes in the oat coleoptile

Summary Parenchymal cells of oat (Avena sativa) coleoptiles had an osmotic concentration of 410 mM (determined by plasmolysis); of this only 22 mM was K⁺ and 1 mM Na⁺ (flame photometry). Cells were impaled with micropipette electrodes. Iontophoretic injection of the dye Niagara sky-blue from the micropipette showed that the tip of the electrode penetrated the vacuole. When sections of tissue were immersed in a solution of 22 mM KCl, 1 mM CaCl₂, and 50 mM glucose, average membrane potential was found to be 38.5 mV inside negative specific membrane resistance was 510 cm², and specific membrane capacitance, 2 f cm^-2. The cell membranes showed <25% retification and no electrical excitability. Electrotonic coupling of adjacent cells could not be demonstrated.     

The route of passive ion movement through the epithelium ofNecturus gallbladder

Summary Electrophysiological experiments were performed onNecturus gallbladder to determine whether the main route of passive ion flow was via the cells or via a paracellular shunt path. In the first approach the following values were determined: the transepithelial resistance, the ratio of the voltage deflections across the luminal and basal cell membrane during transepithelial current flow, and the voltage spread within the epithelial cell layer during intracellular application of current pulses. From these data the luminal and basal cell membrane resistances were calculated to be 4,500 and 2,900 cm², respectively, whereas the transepithelial resistance was only 310 cm², indicating that approximately 96% of the transepithelial current bypassed the cells. This result was confirmed in a second approach, in which the intracellular voltage deflections were found to remain approximately constant, when the current pulses were passed from a cell into the interstitial compartment with the luminal compartment being empty or when they were passed from the cell into both external compartments simultaneously. In the third approach current was passed through the epithelium and a voltage-scanning microelectrode was moved across the surface of the epithelium to explore the induced electrical field. Significant distortions of the field were observed in the immediate vicinity of the cell borders. This result indicated that the paracellular shunt, which carries the main part of the transepithelial current, leads through the terminal bars and that the terminal bars or tight junctions arenot tight for transepithelial movement of small ions in gallbladder epithelium.     

Resistance properties of the diluting segment ofAmphiuma kidney: Influence of potassium adaptation

Summary Chronic exposure to high potassium stimulates K⁺-secretory mechanisms in the diluting segment of the amphibian kidney (K⁺ adaptation). Since K⁺ net flux depends critically on the passive cell membrane permeabilities for K⁺ ions, cable analysis and K⁺-concentration step changes were applied in this nephron segment to assess the individual resistances of the epithelium and the K⁺ conductance of the luminal cell membrane. Experiments were performed in the isolated, doubly-perfused kidney of both control and K⁺-adaptedAmphiuma. In control animals transepithelial resistance was 290±27 cm², which decreased significantly to 199±17 cm² after K⁺ adaptation. The resistance in parallel of the luminal and peritubular cell membrane decreased from a control value of 157±14 to 108±6 cm² after chronic K⁺ treatment. This was paralleled by a decrease of the ratio of the luminal to peritubular cell membrane resistance from 2.5±0.1 to 1.9±0.1, respectively. Estimation of the individual cell membrane resistances reveals that the combined resistance of the luminal and peritubular cell membrane is in the same order of magnitude as the paracellular shunt resistance in diluting segments of both control and K⁺-adapted animals. The luminal cell membrane is K⁺ selective under both conditions, but the absolute luminal K⁺ conductance increases by some 60% with K⁺ adaptation. This leads to an increased back-leak of K⁺ from cell to lumen and may explain stimulated K⁺ net secretion found after chronic K⁺ loading.     

Intracellular sites of the synthesis of sweet potato mitochondrial F1ATPase subunits

Summary Five subunits (-, -, -, - and -subunits) of the six -and -subunits) in the F₁ portion (F₁ATPase) of sweet potato (Ipomoea batatas) mitochondrial adenosine triphosphatase were isolated by an electrophoretic method. The - and -subunits were not distinguishable immunologically but showed completely different tryptic peptide maps, indicating that they were different molecular species. In vitro protein synthesis with isolated sweet potato root mitochondria produced only the -subunit when analyzed with anti-sweet potato F₁ATPase antibody reacting with all the subunits except the -subunit. Sweet potato root poly(A)⁺RNA directed the synthesis of six polypeptides which were immunoprecipitated by the antibody: two of them immunologically related to the -subunit and the others to the - and -subunits. We conclude that the -subunit of the F₁ATPase is synthesized only in the mitochondria and the -, - and -subunits are in the cytoplasm.     

Noise measurements in squid axon membrane

Summary A small area (10^–4 to 10^–5 cm² patch) of the external surface of a squid (Loligo pealei) axon was isolated electrically by means of a pair of concentric glass pipettes and sucrose solution to achieve a low extraneous noise measurement of spontaneous fluctuations in membrane potential and current. The measured small-signal impedance function of the isolated patch in seawater was constant at low frequencies and declined monotonically at frequencies beyond 100 Hz. It is shown that the power-density spectrum (PDS) of voltage noise, which generally reflects the current-noise spectrum filtered by the membrane impedance function, is equivalent to the power spectrum of current-noise up to frequencies where the impedance decline is significant (Fishman, 1973a, Proc. Nat. Acad. Sci. USA 70:876). This result is in contrast to an impedance resonance measured under uniform constant-current (internal axial wire) conditions, for which the voltage-noise PDS reflects the impedance resonance. The overdamped resonance in the patch technique is a consequence of the relatively low resistance (1 M) pathways through the sucrose solution in the interstitial Schwann cell space which surround and shunt the high resistance (10–100 M) membrane patch. Current-noise measurements during patch voltage clamp extend observation of patch ionconductance fluctuations to 1 kHz. Various tests are presented to demonstrate the temporal and spatial adequacy of patch potential control during current-noise measurements.     

Primary structure of alpha-globin chains from river buffalo (Bubalus bubalis L.) hemoglobins

Primary structure analysis of the four river buffalo -globin chains showed that haplotypes A and B differ from each other by a substitution at codon 64 that may encode Ala or Asn. The A haplotype encodes two -globin chains, ^I1 and ^II3, which differ at positions 129 and 131: ^I1 has 64 Ala, 129 Phe, 131 Asn; ^II3 has 64 Ala, 129 Leu, 131 Ser. The B haplotype encodes two -globin chains, ^I2 and ^II4, which differ at positions 10 and 11: ^I2 has 10 Ile, 11 Gln, 64 Asn; ^II4 has 10 Val, 11 Lys, 64 Asn. Apart from the Ala/Asn polymorphism at position 64, amino acid substitutions in allelic and nonallelic -globin chains seem to have arisen by single point mutations. Detection of electrophoretically silent mutations due to neutral amino acid substitutions and their influence on the isoelectric point are discussed. Furthermore, primary structures of river buffalo -globin chains are compared to other species of the Bovidae family to suggest evolutionary events that have characterized the amino acid substitutions of river buffalo hemoglobin.