scholarly journals Desensitization onset and recovery at the potassium-depolarized frog neuromuscular junction are voltage sensitive.

1978 ◽  
Vol 71 (3) ◽  
pp. 285-299 ◽  
Author(s):  
B Scubon-Mulieri ◽  
R L Parsons
Keyword(s):  
Membrane Potential ◽  
Neuromuscular Junction ◽  
Time Constant ◽  
Time Course ◽  
Voltage Dependence ◽  
Onset Time ◽  
Control Voltage ◽  
Frog Neuromuscular Junction ◽  
End Plate ◽  
Voltage Dependent

The influence of voltage on the time-course of desensitization onset and recovery has been studied at the frog neuromuscular junction. The activation-desensitization sequence was determined from carbachol-induced end-plate currents in potassium-depolarized fibers voltage-clamped either to -40 mV or +40 mV. The time-course of both desensitization onset and recovery developed exponentially, with onset occurring more rapidly than recovery. Desensitization onset was voltage dependent, the onset time constant being 8.3 +/- 1.3 s (11 fibers) at -40 mV and 19.3 +/- 3.4 s (15 fibers) at +40 mV. Recovery from desensitization was also influenced by voltage. The extent of recovery after 2 min was 80.4 +/- 6.3% in those fibers voltage-clamped to -40 mV and 57.4 +/- 3.6% in those fibers voltage-clamped to +40 mV. The voltage dependence of desenistization onset and recovery did not result from a difference in ability to control voltage at these two levels of membrane potential. These results demonstrate that in the potassium-depolarized preparation the processes controlling both desensitization onset and recovery of sensitivity from the desensitivity from the desensitized state are influenced by membrane voltage.

Voltage Dependence of the Glycine Receptor–Channel Kinetics in the Zebrafish Hindbrain

1999 ◽  
Vol 82 (5) ◽  
pp. 2120-2129 ◽  
Author(s):  
Pascal Legendre
Keyword(s):  
Time Constant ◽  
Rise Time ◽  
Time Course ◽  
Voltage Dependence ◽  
Good Description ◽  
Glycine Receptor ◽  
Relative Amplitude ◽  
Time Constants ◽  
Low Concentration ◽  
Voltage Dependent

Electrophysiological recordings of outside-out patches to fast-flow applications of glycine were made on patches derived from the Mauthner cells of the 50-h-old zebrafish larva. As for glycinergic miniature inhibitory postsynaptic currents (mIPSCs), depolarizing the patch produced a broadening of the transient outside-out current evoked by short applications (1 ms) of a saturating concentration of glycine (3 mM). When the outside-out patch was depolarized from −50 to +20 mV, the peak current varied linearly with voltage. A 1-ms application of 3 mM glycine evoked currents that activated rapidly and deactivated biexponentially with time constants of ≈5 and ≈30 ms (holding potential of −50 mV). These two decay time constants were increased by depolarization. The fast deactivation time constant increased e-fold per 95 mV. The relative amplitude of the two decay components did not significantly vary with voltage. The fast component represented 64.2 ± 2.8% of the total current at −50 mV and 54.1 ± 10% at +20 mV. The 20–80% rise time of these responses did not show any voltage dependence, suggesting that the opening rate constant is insensitive to voltage. The 20–80% rise time was 0.2 ms at −70 mV and 0.22 ms at +20 mV. Responses evoked by 100–200 ms application of a low concentration of glycine (0.1 mM) had a biphasic rising phase reflecting the complex gating behavior of the glycine receptor. The time constant of these two components and their relative amplitude did not change with voltage, suggesting that modal shifts in the glycine-activated channel gating mode are not sensitive to the membrane potential. Using a Markov model to simulate glycine receptor gating behavior, we were able to mimic the voltage-dependent change in the deactivation time course of the responses evoked by 1-ms application of 3 mM glycine. This kinetics model incorporates voltage-dependent closing rate constants. It provides a good description of the time course of the onset of responses evoked by the application of a low concentration of glycine at all membrane potentials tested.

Gating currents in the node of Ranvier: voltage and time dependence

1975 ◽  
Vol 270 (908) ◽  
pp. 483-492 ◽  
Keyword(s):  
Membrane Potential ◽  
Time Constant ◽  
Time Course ◽  
Voltage Dependence ◽  
Sudden Change ◽  
Node Of Ranvier ◽  
Ionic Currents ◽  
Gating Currents ◽  
Myelinated Nerve ◽  
Sodium Conductance

Like the axolemma of the giant nerve fibre of the squid, the nodal membrane of frog myelinated nerve fibres after blocking transmembrane ionic currents exhibits asymmetrical displacement currents during and after hyperpolarizing and depolarizing voltage clamp pulses of equal size. The steady-state distribution of charges as a function of membrane potential is consistent with Boltzmann’s law (midpoint potential —33.7 mV; saturation value 17200 charges/(μm 2 ). The time course of the asymmetry current and the voltage dependence of its time constant are consistent with the notion that due to a sudden change in membrane potential the charges undergo a first order transition between two configurations. Size and voltage dependence of the time constant are similar to those of the activation of the sodium conductance assuming m 2 h kinetics, The results suggest the presence of ten times more sodium channels (5000/μm2) in the node of Ranvier than in the squid giant axon with similar sodium conductance per channel (2-3 pS),

scholarly journals Desensitization and recovery at the frog neuromuscular junction.

1977 ◽  
Vol 69 (4) ◽  
pp. 431-447 ◽  
Author(s):  
B Scubon-Mulieri ◽  
R L Parsons
Keyword(s):  
Neuromuscular Junction ◽  
Intracellular Calcium ◽  
Time Constant ◽  
Time Course ◽  
Frog Neuromuscular Junction ◽  
Rate Of Development ◽  
Recovery Interval ◽  
Cyclic Model ◽  
Input Conductance ◽  
External Calcium

The time course of carbachol-induced desensitization onset and recovery of sensitivity after desenitization have been compared at the frog neuromuscular junction. The activation-desensitization sequence was determined from input conductance measurements using potassium-depolarized muscle preparations. Both desensitization onset and recovery from desensitization could be adequately described by single time constant expressions, with tauonset being considerably shorter than taurecovery. In nine experiments, tauonset was 13+/-1.3 s and taurecovery was 424+/-51 s with 1 mM carbachol. Elevating the external calcium or carbachol concentration accelerated desensitization onset without changing the recovery of sensitivity after equilibrium desensitization. Desensitization onset was accelerated by a prior activation-desensitization sequence to an extent determined by the recovery interval that followed the initial carbachol application. The time course of return of tauonset was closely parallel to, but slower than the time course of recovery of sensitivity. These results are consistent with a cyclic model in which intracellular calcium is a factor controlling the rate of development of desensitization.

Time course of miniature end-plate currents at different sites on the frog neuromuscular junction

1988 ◽  
Vol 19 (6) ◽  
pp. 566-573
Author(s):  
E. G. Bezgina ◽  
T. M. Drabkina ◽  
S. N. Zemskova ◽  
A. L. Zefirov ◽  
L. A. Kashapova ◽  
...  
Keyword(s):  
Neuromuscular Junction ◽  
Time Course ◽  
Frog Neuromuscular Junction ◽  
End Plate

Differences in presynaptic action of 4-aminopyridine and tetraethylammonium at frog neuromuscular junction

1987 ◽  
Vol 65 (5) ◽  
pp. 747-752 ◽  
Author(s):  
M. I. Glavinović
Keyword(s):  
Neuromuscular Junction ◽  
Transmitter Release ◽  
Action Potentials ◽  
Time Course ◽  
Potassium Conductance ◽  
Frog Neuromuscular Junction ◽  
Quantal Content ◽  
Low Concentrations ◽  
Voltage Dependent ◽  
Intracellular Ca

4-Aminopyridine markedly potentiates transmitter release at the frog cutaneous pectoris neuromuscular junction by increasing the quantal content even when applied at low concentrations (5–20 μM). This enhancement of transmitter release is associated with greater minimum synaptic latency, but the dispersion of the synaptic latencies does not appear much affected. This is in contrast with the action of tetraethylammonium (0.2–0.5 mM) in which case similar enhancement of transmitter release results not only in larger minimum synaptic latency but also in greater dispersion of the synaptic latencies. The time course of transmitter release associated with enhanced transmitter output is hence much more prolonged in the presence of tetraethylammonium than 4-aminopyridine, at least for low concentrations of 4-aminopyridine (5–20 μM). This indicates that their presynaptic actions differ significantly. This conclusion is further strengthened by the finding that unlike tetraethylammonium, 4-aminopyridine induces bursts of release, presumably by producing multiple action potentials in the nerve terminal. Tetraethylammonium probably acts by blocking the delayed potassium conductance, but the blockade of Ca2+-activated K+ conductance cannot be excluded. 4-Aminopyridine, however, probably blocks the fast inactivating (IA) K+ current, but it also may be acting directly on the voltage-dependent Ca2+ conductance or on the intracellular Ca2+ buffering.

scholarly journals The hyperpolarization-activated current shifts the dynamic range of a voltage-dependent electrical synapse

2021 ◽  
Author(s):  
Wolfgang Stein ◽  
Margaret DeMaegd ◽  
Lena Yolanda Braun ◽  
Andrés G Vidal-Gadea ◽  
Allison L Harris ◽  
...  
Keyword(s):  
Membrane Potential ◽  
Motor Neuron ◽  
Axon Terminal ◽  
Voltage Dependence ◽  
Dynamic Range ◽  
Complex Dynamics ◽  
Ionic Current ◽  
Electrical Synapse ◽  
Resting Membrane Potential ◽  
Voltage Dependent

Like their chemical counterparts, electrical synapses show complex dynamics such as rectification and voltage dependence that interact with other electrical processes in neurons. The consequences arising from these interactions for the electrical behavior of the synapse, and the dynamics they create, remain largely unexplored. Using a voltage-dependent electrical synapse between a descending modulatory projection neuron (MCN1) and a motor neuron (LG) in the crustacean stomatogastric ganglion, we find that the influence of the hyperpolarization-activated inward current (Ih) is critical to the function of the electrical synapse. When we blocked Ih with CsCl, the voltage dependence of the electrical synapse shifted by 18.7 mV to more hyperpolarized voltages, placing the dynamic range of the electrical synapse outside of the range of voltages used by the LG motor neuron (-60.2 mV to -44.9 mV). With dual electrode current- and voltage-clamp recordings, we demonstrate that this voltage shift is due to a sustained effect of Ih on the presynaptic MCN1 axon terminal membrane potential. Ih-induced depolarization of the axon terminal membrane potential increased the electrical postsynaptic potentials and currents. With Ih present, the axon terminal resting membrane potential depolarized, shifting the dynamic range of the electrical synapse towards the functional range of the motor neuron. We thus demonstrate that the function of an electrical synapse is critically influenced by a voltage-dependent ionic current (Ih).

Input Resistance, Time Constants, and Spike Initiation

1998 ◽  
Author(s):  
Christof Koch
Keyword(s):  
Membrane Potential ◽  
Time Constant ◽  
Action Potentials ◽  
Input Resistance ◽  
Current Injection ◽  
Membrane Conductances ◽  
Voltage Dependent ◽  
Dc Component ◽  
Definition Of ◽  
A Current

This chapter represents somewhat of a tephnical interlude. Having introduced the reader to both simplified and more complex compartmental single neuron models, we need to revisit terrain with which we are already somewhat familiar. In the following pages we reevaluate two important concepts we defined in the first few chapters: the somatic input resistance and the neuronal time constant. For passive systems, both are simple enough variables: Rin is the change in somatic membrane potential in response to a small sustained current injection divided by the amplitude of the current injection, while τm is the slowest time constant associated with the exponential charging or discharging of the neuronal membrane in response to a current pulse or step. However, because neurons express nonstationary and nonlinear membrane conductances, the measurement and interpretation of these two variables in active structures is not as straightforward as before. Having obtained a more sophisticated understanding of these issues, we will turn toward the question of the existence of a current, voltage, or charge threshold at which a biophysical faithful model of a cell triggers action potentials. We conclude with recent work that suggests how concepts from the subthreshold domain, like the input resistance or the average membrane potential, could be extended to the case in which the cell is discharging a stream of action potentials. This chapter is mainly for the cognoscendi or for those of us that need to make sense of experimental data by comparing therp to theoretical models that usually fail to reflect reality adequately. In Sec. 3.4, we defined Kii (f) for passive cable structures as the voltage change at location i in response to a sinusoidal current injection of frequency f at the same location. Its dc component is also referred to as input resistance or Rin. Three difficulties render this definition of input resistance problematic in real cells: (1) most membranes, in particular at the soma, show voltage-dependent nonlinearities, (2) the associated ionic membrane conductances are time dependent and (3) instrumental aspects, such as the effect of the impedance of the recording electrode on Rin, add uncertainty to the measuring process.

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