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N Moran

Publications and source records attributed to N Moran.

51 records · Page 3Linked to original sources
PubMed1990

Interaction of the Depolarization-Activated K Channel of Samanea saman with Inorganic Ions: A Patch-Clamp Study.

A depolarization-activated K(+) channel capable of carrying the large K(+) currents that flow from shrinking cells during movements of Samanea saman leaflets has been described in the plasmalemma of Samanea motor cell protoplasts (N Moran et al [1988] Plant Physiol 88:643-648). We now characterize this channel in greater detail. It is selective for K(+) over other monovalent ions, with the following order of relative permeability: K(+) > Rb(+) > Na(+) approximately Cs(+) approximately Li(+). It is blocked by Cs(+) and by Ba(2+) in a voltage dependent manner, exhibiting a ;long-pore' behavior, similarly to various types of K(+) channels in animal systems. Cadmium, known for its blockage of Ca(2+) channels in animal systems, and Gd(3+), closely related to La(3+), which also blocks Ca(2+) channels in animal cells, both block K(+) currents in Samanea in a voltage-independent manner, and without interfering with the kinetics of the currents. The suggested mechanism of block is either (a) by a direct interaction with the K(+) channel, but external to its lumen, or, alternatively, (b) by blocking putative Ca(2+) channels, and preventing the influx of Ca(2+), on which the activation of the K(+) channels may be dependent.

Journal Article↗
PubMed1989

Equilibrium binding analysis of neural cell adhesion molecule binding to heparin.

The kinetics of neural cell adhesion molecule (NCAM) binding to heparin were studied in a heparin-Sepharose-based solid-phase binding assay. The observed binding is time dependent and saturable. A binding constant of 5.2 +/- 1.4 X 10(-8) M is observed for binding of newborn rat NCAM to heparin. This is approximately 25 times lower than the binding constant determined for newborn rat NCAM homophilic binding. Both Scatchard and Hill plot analyses suggest the presence of only one binding site. Fab' fragments of antibodies to rat NCAM significantly inhibit binding, a result indicating that a specific site on NCAM is involved in binding to heparin. The binding is inhibited by heparin (IC50, approximately 5 micrograms/ml), whereas chondroitin sulfate is a less potent inhibitor (IC50, approximately 15 micrograms/ml).

Animals↗
PubMed1988

Characterization of the kinetics of neural cell adhesion molecule homophilic binding.

A solid-phase assay has been developed for the investigation of the kinetics of neural cell adhesion molecule (NCAM) binding. Using this assay we can show that NCAM binds to itself in a time-dependent and saturable manner. Binding constants (KB values) of 6.9 x 10(-8) M and 1.23 x 10(-6) M, respectively, were obtained for adult and newborn rat NCAM homophilic binding. Binding is specifically inhibited by Fab' fragments of polyclonal anti-NCAM antibodies but is unaffected by heparin or chondroitin sulphate. This indicates that the NCAM homophilic binding site is separate from and independent of the heparin-binding site and that a developmental modification, probably polysialation, gives rise to marked differences in the adhesive properties of NCAM.

Animals↗
PubMed1988

Potassium Channels in Motor Cells of Samanea saman: A Patch-Clamp Study.

Leaflet movements in Samanea saman are driven by the shrinking and swelling of cells in opposing (extensor and flexor) regions of the motor organ (pulvinus). Changes in cell volume, in turn, depend upon large changes in motor cell content of K(+), Cl(-) and other ions. We performed patch-clamp experiments on extensor and flexor protoplasts, to determine whether their plasma membranes contain channels capable of carrying the large K(+) currents that flow during leaflet movement. Recordings in the "whole-cell" mode reveal depolarization-activated K(+) currents in extensor and flexor cells that increase slowly (t((1/2)) = ca. 2 seconds) and remain active for minutes. Recordings from excised patches reveal a single channel conductance of ca. 20 picosiemens in both cell types. The magnitude of the K(+) currents is adequate to account quantitatively for K(+) loss, previously measured in vivo during cell shrinkage. The K(+) channel blockers tetraethylammonium (5 millimolar) or quinine (1 millimolar) blocked channel opening and decreased light- and dark-promoted movements of excised leaflets. These results provide evidence for the role of potassium channels in leaflet movement.

Journal Article↗
PubMed1986

Evidence for interactions between batrachotoxin-modified channels in hybrid neuroblastoma cells.

Current records from voltage-clamped membrane patches containing two batrachotoxin-modified sodium channels were analyzed to determine whether these channels are identical and independent. In most two-channel patches, the experimentally observed probabilities that zero, one, or two channels are open differ from the binomial distribution, demonstrating that the two channels are nonidentical or nonindependent or both. From the same current records, we also determined the rate for the transition from two open channels to one open channel and for the transition from one open channel to zero open channels. These data are consistent with closing rates for the two channels that are equal and independent. Both probability and closing rate data can be fit by a model wherein the channels are identical, the closing rates are independent, and the opening rate is greater when the other channel is closed than when it is open. The implications of this model for analyzing noise spectra and current variance are examined.

Animals↗
PubMed1985

Significant potassium ion accumulation at the external surface of Myxicola giant axons.

Potassium accumulation associated with outward membrane potassium current was investigated experimentally in Myxicola giant axon. During prolonged voltage-clamp pulses to positive transmembrane potentials, the K+ equilibrium potential may approach zero mV, suggesting massive K+ accumulation outside the axonal membrane to concentrations many-fold higher than those in the bathing medium. The potassium accumulation can be satisfactorily described by a three-compartment model, consisting of the nerve fiber, a restricted physiological periaxonal space and the bulk solution. The average thickness, theta, of the periaxonal space is calculated as 177 +/- 59 A, i.e., comparable to that in the squid, while the permeability coefficient of the external barrier, PKs, was calculated to be (1.4 +/- 0.4) X 10(-4) cm/s. These conclusions are well supported by morphological study.

Animals↗
PubMed1984

Ion channels in plasmalemma of wheat protoplasts.

The patch-clamp technique was used to study passive movements of ions through the plasmalemma of wheat leaf protoplasts. This method overcomes the problems inherent in conventional electrophysiological study of plant cells. Changes in conductance were recorded in patches excised from the plasmalemma. Two types of patches were observed: (i) regions of low channel density, where discrete single-channel currents could be resolved and conductance ranged from 10 to 200 picosiemens and (ii) regions of high channel density, where single-channel currents could not be resolved and conductance was on the order of a few nanosiemens. The results indicate a striking similarity between animal and plant cell membranes in the basic phenomena of transport. Moreover, the approach used constitutes a new degree of refinement in the study of processes of regulation, pathology, and toxicity in plants.

Calcium Chloride↗
PubMed1984

Gating kinetics of batrachotoxin-modified sodium channels in neuroblastoma cells determined from single-channel measurements.

We have observed the opening and closing of single batrachotoxin (BTX)-modified sodium channels in neuroblastoma cells using the patch-clamp method. The conductance of a single BTX-modified channel is approximately 10 pS. At a given membrane potential, the channels are open longer than are normal sodium channels. As is the case for normal sodium channels, the open dwell times become longer as the membrane is depolarized. For membrane potentials more negative than about -70 mV, histograms of both open-state dwell times and closed-state dwell times could be fit by single exponentials. For more depolarized potentials, although the open-state histograms could still be fit by single exponentials, the closed-state histograms required two exponentials. This data together with macroscopic voltage clamp data on the same system could be accounted for by a three-state closed-closed-open model with transition rates between these states that are exponential functions of membrane potential. One of the implications of this model, in agreement with experiment, is that there are always some closed BTX-modified sodium channels, regardless of membrane potential.

Animals↗
PubMed1982

Batrachotoxin modifies the gating kinetics of sodium channels in internally perfused neuroblastoma cells.

We have studied the effects of batrachotoxin (BTX) on sodium channels in hybrid mouse neuroblastoma cells NG108-15 by using the suction pipet voltage clamp method. BTX-modified sodium channels activate with first-order kinetics and, over most of the potential range, activate more slowly than normal sodium channels. The peak conductance-voltage curve and the time constant of activation-versus-voltage curve for BTX-modified sodium channels are shifted about 50 mV in the hyperpolarizing direction compared to the corresponding curves for normal sodium channels. There is no change in the slope of the conductance-voltage curve. These results suggest that BTX slows down one of the steps leading to channel opening, which consequently becomes rate-limiting. In addition, BTX eliminates both fast and slow inactivation.

Animals↗
PubMed1980

Potassium ion accumulation at the external surface of the nodal membrane in frog myelinated fibers.

Potassium accumulation associated with outward membrane potassium current was investigated experimentally in myelinated fibers and analyzed in terms of two models-three-compartment and diffusion in an unstirred layer. In the myelinated fibers, as in squid giant axons, the three-compartment model satisfactorily describes potassium accumulation. Within this framework the average space thickness, theta, in frog was 5,900 +/- 700 A, while the permeability coefficient of the external barrier, PK, was (1.5 +/- 0.1) X 10(-2) cm/s. The model of ionic diffusion in an unstirred aqueous layer adjacent to the axolemma, as an alternative explanation for ion accumulation, was also consistent with the experimental data, provided that D, the diffusion constant, was (1.8 +/- 0.2) X 10(-6) cm/s and l, the unstirred layer thickness, was 1.4 +/- 0.1 micron, i.e., similar to the depth of the nodal gap. An empirical equation relating the extent of potassium accumulation to the amplitude and duration of depolarization is given.

Animals↗
PubMed1980

Potassium currents and conductance. Comparison between motor and sensory myelinated fibers.

The potassium conductance system of sensory and motor fibers from the frog Rana esculenta were studied and compared by means of the voltage clamp. The potassium ion accumulation was first estimated from the currents and reversal potentials within the framework of both a three-compartment model and diffusion-in-an-unstirred-layer model. The potassium conductance parameters were then computed using the measured currents and corrected ionic driving forces. It was found that the potassium accumulation is faster and more pronounced in sensory fibers, the voltage dependency of the potassium conductance is steeper in sensory fibers, the maximal potassium conductance, corrected for accumulation, is approximately 1.1 S/cm2 in sensory and 0.55 S/cm2 in motor fibers, and that the conductance time constants, tau n, are smaller in sensory than in motor fibers. These differences, which increase progressively with depolarization, are not detectable for depolarization of 50 mV or smaller. The interpretation of these findings in terms of different types of potassium channels as well as their implications with regard to the differences between the excitability phenomena in motor and sensory fibers are discussed.

Animals↗