Accounting for the shapes and size distributions of miniature endplate currents.

The current model does not account adequately for the characteristics of miniature endplate currents (MEPCs). We do not understand their relatively slow rise, the shape of their rise, their variable and sometimes prolonged decay, and the correlation between amplitude and decay time. If we assume that ACh is released from the vesicle through a pore and that the vesicle enlarges as it takes on additional transmitter, the predictions are more like MEPCs. However, previous measurements showed that after quantal size was increased the vesicles in the terminal were not enlarged. This need not be a problem, because some of the ACh is added to vesicles positioned at the active zones, a process known as second-stage loading. By using the false transmitter precursor monoethylcholine we provide additional evidence for second-stage loading. The distribution of quantal sizes at the junction usually does not follow a normal probability distribution; it is skewed to the right. The skew can be accounted for by a model incorporating second-stage loading in which the vesicles are released randomly, without regard to their ACh content. If the vesicles increase in size when they contain more transmitter, only vesicles at the active zone need swell.     

Butyrylcholinesterase and the control of synaptic responses in acetylcholinesterase knockout mice

At the neuromuscular junction (NMJ) acetylcholinesterase (AChE) and butyrylcholinesterase (BChE) can hydrolyze acetylcholine (ACh). Released ACh quanta are known to diffuse rapidly across the narrow synaptic cleft and pairs of ACh molecules cooperate to open endplate channels. During their diffusion through the cleft, or after being released from muscle nicotinic ACh receptors (nAChRs), most ACh molecules are hydrolyzed by AChE highly concentrated at the NMJ. Advances in mouse genomics offered new approaches to assess the role of specific cholinesterases involved in synaptic transmission. AChE knockout mice (AChE-KO) provide a valuable tool for examining the complete abolition of AChE activity and the role of BChE. AChE-KO mice live to adulthood, and exhibit an increased sensitivity to BChE inhibitors, suggesting that BChE activity facilitated their survival and compensated for AChE function. Our results show that BChE is present at the endplate region of wild-type and AChE-KO mature muscles. The decay time constant of focally recorded miniature endplate currents was 1.04 +/- 0.06 ms in wild-type junctions and 5.4 ms +/- 0.3 ms in AChE-KO junctions, and remained unaffected by BChE-specific inhibitors, indicating that BChE is not limiting ACh duration on endplate nAChRs. Inhibition of BChE decreased evoked quantal ACh release in AChE-KO NMJs. This reduction in ACh release can explain the greatest sensitivity of AChE-KO mice to BChE inhibitors. BChE is known to be localized in perisynaptic Schwann cells, and our results strongly suggest that BChE's role at the NMJ is to protect nerve terminals from an excess of ACh.     

Properties of single cardiac Na channels at 35 degrees C

Single Na channel currents were recorded in cell-attached patches of mouse ventricular myocytes with an improved patch clamp technique. Using patch pipettes with a pore diameter in the range of 200 nm, seals with a resistance of up to 4 T omega were obtained. Under those conditions, total noise could be reduced to levels as low as 0.590 pA rms at 20 kHz band width. At this band width, properties of single- channel Na currents were studied at 35 degrees C. Six out of a total of 23 patches with teraohm seals contained channel activity and five of these patches contained one and only one active channel. Amplitude histograms excluding transition points showed heterogenous distributions of levels. In one patch, part of the openings was approximately Gaussian distributed at different potentials yielding a slope conductance of 27 pS. The respective peak open probability at -10 mV was 0.26. The mean open time was determined at voltages between -60 and -10 mV by evaluation of the distribution of the event-related gaps in the center of the baseline noise to be approximately 40 microseconds at -60 mV and 50-74 microseconds between -50 and -10 mV. It is concluded that single cardiac Na channels open at 35 degrees C frequently with multiple levels and with open times in the range of several tens of microseconds.     

Localization effects of acetylcholine release from a synaptic vesicle at the neuromuscular junction.

A two-dimensional compartment model devised for the appropriate representation of the transient process of the spontaneous generation of miniature endplate current (MEPC) at the neuromuscular junction is applied for clarifying the biochemical significance of the quantal release mechanism of acetylcholine (ACh), a typical neurotransmitter, in the synaptic chemical transmission process. The simulation analysis with the model demonstrates that the localization of the ACh release due to the fusion of a synaptic vesicle with the presynaptic membrane has significant effects on the amplitude of MEPC and that the stronger effects are caused with the smaller diffusion coefficients of ACh in the cleft. The sharpest and highest response of MEPC is achieved when the release area is about 4 times to the natural release through the narrow pore. On the other hand, the actual localization corresponding to the natural release of ACh makes the amplitude of MEPC higher by a factor about 2.5 compared with that in the most extended release of ACh examined, implying that the natural release mechanism works as an amplifier of the MEPC with the fixed amount of ACh available.     

Effects of ammonium ions on endplate channels

Miniature endplate currents, recorded from voltage-clamped toad sartorius muscle fibers in solutions containing ammonium ions substituted for sodium ions, were increased in amplitude and decayed exponentially with a slower time constant than in control (Na) solution. The peak conductance of miniature endplate currents was also greater in ammonium solutions. The acetylcholine null potential was - 2.8 +/- 0.8 mV in control solution, and shifted to 0.9 +/- 1.6 mV in solutions in which NH4Cl replaced half the NaCl. In solutions containing NH4Cl substituted for all the NaCl, the null potential was 6.5 +/- 1.3 mV. Single channel conductance and average channel lifetime were both increased in solutions containing ammonium ions. The exponential relationship between the time constant of decay of miniature endplate currents or channel lifetime and membrane potential was unchanged in ammonium solutions. A slight but consistent increase in peak conductance during miniature endplate currents and single channel conductance was seen as membrane potential became more positive (depolarized) in both control and ammonium solutions. Net charge transfer was greater in ammonium solutions than in control solution, whether measured during a miniature endplate current or through a single channel. The results presented here are consistent with an endplate channel model containing high field strength, neutral sites.     

Effects of vinblastine and colchicine on the postsynaptic membrane at the frog neuromuscular junction

The possible effects of the alkaloids vinblastine and colchicine on the postsynaptic membrane of the frog neuromuscular junction were investigated using voltage-clamp techniques. Concentrations of vinblastine and colchicine which had been shown to exert no effect on the amplitude and duration of miniature endplate currents (MEPC) and the current-voltage relationship of low-quantal endplate currents (EPC) together with the coefficient of voltage-dependent EPC decay did produce a considerable rise in the amplitude of response to iontophoretically applied acetylcholine (ACh). In addition, vinblastine and colchicine accelerate MEPC and EPC during acetylcholine esterase inhibition while further depressing the amplitude of multi-quantal EPC succeeding at the rate of 10 Hz as well as response to regular (5–10 Hz) application of ACh from a micropipet. The dosage-frequency effects of vinblastine and colchicine on the postsynaptic membrane (as described) are presumed to be unconnected with the action of these agents on muscle fiber cytoskeleton but the results of accelerated desensitization of cholinoreceptors.S. V. Kurashov Medical Institute, Kazan. Translated from Neirofiziologiya, Vol. 20, No. 1, pp. 75–81, January–February, 1988.     

The amplitude distribution of release events through a fusion pore

Neurotransmitters, hormones, or dyes may be released from vesicles via a fusion pore, rather than by full fusion of the vesicle with the plasma membrane. If the lifetime of the fusion pore is comparable to the time required for the substance to exit the vesicle, only a fraction of the total vesicle content may be released during a single pore opening. Assuming 1), fusion pore lifetimes are exponentially distributed (tauP), as expected for simple single channel openings, and 2), vesicle contents are lost through the fusion pore with an exponential time course (tauD), we derive an analytical expression for the probability density function of the fraction of vesicle content released (F): dP/dF=A (1-F)(A-1), where A=tauD/tauP. If A>1, the maximum of the distribution is at F=0; if A<1, the maximum is at F=1; if A=1, the distribution is perfectly flat. Thus, the distribution never has a peak in the middle (0相似文献   

Constitutive secretion of exogenous neurotransmitter by nonneuronal cells: implications for neuronal secretion.

Fibroblasts in cell culture were loaded with exogenous neurotransmitter acetylcholine (ACh). ACh secretion from loaded cells was detected by whole-cell patch clamp recordings from Xenopus myocytes manipulated into contact with ACh-loaded cells. Two different approaches were used for ACh loading. In the first approach, fibroblasts were incubated in the culture medium containing ACh. Recordings from myocytes revealed fast inward currents that resemble miniature endplate currents found at neuromuscular synapses. The currents observed in recordings from myocytes were due to exocytosis of ACh-containing vesicles. Although exogenous ACh penetrated through the plasma membrane of fibroblasts during incubation and was present in the cytoplasm at detectable levels, cytoplasmic ACh did not contribute to the quantal ACh secretion. In the second approach, exogenous ACh was loaded into the cytoplasm of fibroblasts by microinjection. Under these experimental conditions, fibroblasts also exhibited spontaneous quantal ACh secretion. Analysis of the exocytotic events in fibroblasts following two different protocols of ACh loading revealed that the vesicular compartments responsible for uptake of exogenous ACh are associated with the endocytic recycling pathway. Extrapolation of our results to neuronal cells suggest that in cholinergic neurons, in addition to genuine synaptic vesicles, ACh can be secreted by the vesicles participating in endosomal membrane recycling.     

Quantal transmitter release at somatic motor-nerve terminals: stochastic analysis of the subunit hypothesis.

Here we analyze the problem of determining whether experimentally measured spontaneous miniature end-plate currents (MEPCs) indicate that quanta are composed of subunits. The properties of MEPCs at end plates with or without secondary clefts at the neuromuscular junction are investigated, using both stochastic and deterministic models of the action of a quantum of transmitter. It is shown that as the amount of transmitter in a quantum is increased above about 4000 acetylcholine (ACh) molecules there is a linear increase in the size of the MEPC. It is possible to then use amplitude-frequency histograms of such MEPCs to detect a subunit structure, as there is little potentiation effect above 4000 ACh molecules. Autocorrelation and power spectral analyses of such histograms establish that their subunit structure can be detected if the coefficient of variation of the subunit size is less than about 0.12 or, if electrical noise is added, about 0.1. Positive gradients relate the rise time and half-decay times of MEPCs to their amplitude, even in the absence of potentiating effects; these gradients are shallower at motor nerve terminals that possess secondary clefts. The effect of asynchronous release of subunits is also investigated. The criteria determined by this analysis for identifying a subunit composition in the quantum are applied to an amplitude-frequency histogram of MEPCs recorded from a small group of active zones at a visualized amphibian motor-nerve terminal. This did not provide evidence for a subunit structure.     

The Role of Endogenous Calcitonin Gene-Related Peptide in the Neurotransmitter Quantal Size Increase in Mouse Neuromuscular Junctions

Changes in parameters of spontaneous acetylcholine (ACh) quantal secretion caused by prolonged high-frequency burst activity of neuromuscular junctions and possible involvement of endogenous calcitonin gene-related peptide (CGRP) and its receptors in these changes were studied. With this purpose, miniature endplate potentials (MEPPs) were recorded using standard microelectrode technique in isolated neuromuscular preparations of m. EDL–n. peroneus after a prolonged high-frequency nerve stimulation (30 Hz for 2 min). An increase in the MEPP amplitudes and time course was observed in the postactivation period that reached maximum 20–30 min after nerve stimulation and progressively faded in the following 30 min of recording. Inhibition of vesicular ACh transporter with vesamicol (1 μM) fully prevented this “wave” of the MEPP enhancement. This indicates the presynaptic origin of the MEPP amplitude increase, possibly mediated via intensification of synaptic vesicle loading with ACh and subsequent increase of the quantal size. Competitive antagonist of the CGRP receptor, truncated peptide isoform CGRP_8–37 (1 μM), had no effect on spontaneous secretion parameters by itself but was able to prevent the appearance of enhanced MEPPs in the postactivation period. This suggests the involvement of endogenous CGRP and its receptors in the observed MEPP enhancement after an intensive nerve stimulation. Ryanodine in high concentration (1 μM) that blocks ryanodine receptors and stored calcium release did not influence spontaneous ACh secretion but prevented the increase of the MEPP parameters in the postactivation period. Altogether, the data indicate that an intensive nerve stimulation, which activates neuromuscular junctions and muscle contractions, leads to a release of endogenous CGRP into synaptic cleft and this release strongly depends on the efflux of stored calcium. The released endogenous CGRP is able to exert an acute presynaptic effect on nerve terminals, which involves its specific receptor action and intracellular cascades leading to intensification of ACh loading into synaptic vesicles and an increase in the ACh quantal size.     

In vitro formation of neuromuscular junctions between adult Rana muscle fibres and embryonic Xenopus neurons

Adult muscle fibres of the frog Rana temporaria were cultured with neurons from embryos of the frog Xenopus laevis. Electron microscopical and electro-physiological examination of the cultures showed that hetero-specific (Xenopus-Rana) neuromuscular junctions were formed in vitro. Nerve processes, without any Schwann cell covering, made contacts anywhere along a muscle fibre, and the junctions resembled those seen during early regeneration of neuromuscular synapses in situ. Functional contacts, as inferred by the presence of spontaneous miniature endplate potentials, or currents, were more common if the muscle fibres were denervated prior to culturing with neurons. Miniature endplate currents (m.e.p.cs) had a skewed amplitude distribution, with many small events lost in the recording noise, and their mean amplitude was much smaller than that of m.e.p.cs in the original lumbricalis muscle. The time constant of decay of m.e.p.cs in the hetero-specific junctions formed in vitro was several times longer than the decay of m.e.p.cs in the original muscle. Analysis of membrane current noise elicited by ionophoretically applied acetylcholine (ACh) suggests that the slower decay of m.e.p.cs in the junctions formed in vitro is due to a prolonged lifetime of the channels opened by ACh and to repetitive activation of ACh-receptors, which becomes possible because of a comparative lack of cholinesterase in the junctions.     

Na channel distribution in vertebrate skeletal muscle

The loose patch voltage clamp has been used to map Na current density along the length of snake and rat skeletal muscle fibers. Na currents have been recorded from (a) endplate membrane exposed by removal of the nerve terminal, (b) membrane near the endplate, (c) extrajunctional membrane far from both the endplate and the tendon, and (d) membrane near the tendon. Na current densities recorded directly on the endplate were extremely high, exceeding 400 mA/cm2 in some patches. The membrane adjacent to the endplate has a current density about fivefold lower than that of the endplate, but about fivefold higher than the membrane 100-200 micron from the endplate. Small local variations in Na current density are recorded in extrajunctional membrane. A sharp decrease in Na current density occurs over the last few hundred micrometers from the tendon. We tested the ability of tetrodotoxin to block Na current in regions close to and far from the endplate and found no evidence for toxin-resistant channels in either region. There was also no obvious difference in the kinetics of Na current in the two regions. On the basis of the Na current densities measured with the loose patch clamp, we conclude that Na channels are abundant in the endplate and near-endplate membrane and are sparse close to the tendon. The current density at the endplate is two to three orders of magnitude higher than at the tendon.     

Gating current kinetics in Myxicola giant axons. Order of the back transition rate constants.

Gating current, Ig, was recorded in Myxicola axons with series resistance compensation and higher time resolution than in previous studies. Ig at ON decays as two exponentials with time constants, tau ON-F and tau ON-S, very similar to squid values. No indication of an additional very fast relaxation was detected, but could be still unresolved. Ig at OFF also displays two exponentials, neither reflecting recovery from charge immobilization. Deactivation of the two I(ON) components may proceed with well-separated exponentials at -100 mV. INa tail currents at OFF also display two exponentials plus a third very slow relaxation of 5-9% of the total tail current. The very slow component is probably deactivation of a very small subpopulation of TTX sensitive channels. A -100 mV, means for INa tail component time constants (four axons) are 76 microseconds (range: 53-89 microseconds) and 344 microseconds (range: 312-387 microseconds), and for IOFF (six axons) 62 microseconds (range: 34-87 microseconds) and 291 microseconds (range: 204-456 microseconds) in reasonable agreement. INa ON activation time constant, tau A, is clearly slower than tau ON-F at all potentials. Except for the interval -30 to -15 mV, tau A is clearly faster than tau ON-S, and has a different dependency on potential. tau ON-S is several fold smaller than tau h. Computations with a closed2----closed1----open activation model indicated Na tail currents are consistent with a closed1----open rate constant greater than the closed2----closed1.     

Three types of transmitter release from embryonic neurons

Prior to the contact with their target muscle cells in culture, growth cones of many isolated Xenopus embryonic neurons release acetylcholine (ACh) spontaneously. Using patch clamp techniques, this release can be detected by an outside-out patch of muscle membrane placed near the growth cone. Intracellular recording from innervated muscle cells showed spontaneous miniature endplate potentials (MEPPs) of varying amplitudes. Amplitude histograms showed a skewed distribution with multiple peaks, suggesting the existence of subunits in either the quantal packages of ACh released by the nerve terminal or in the postsynaptic muscle response. In addition to the quantal ACh release reflected by MEPPs, nerve terminal also release a large amount of ACh in a non-quantal fashion. This non-quantal ACh release is revealed by the hyperpolarization of the muscle membrane following extracellular application of curare or alpha-bungarotoxin, as well as by denervation of the muscle cell.     

The permeability of the endplate channel to organic cations in frog muscle

The relative permeability of endplate channels to many organic cations was determined by reversal-potential criteria. Endplate currents induced by iontophoretic "puffs" of acetylcholine were studied by a Vaseline gap, voltage clamp method in cut muscle fibers. Reversal potential changes were measured as the NaCl of the bathing medium was replaced by salts of organic cations, and permeability ratios relative to Na+ ions were calculated from the Goldman-Hodgkin-Katz equation. 40 small monovalent organic cations had permeability ratios larger than 0.1. The most permeant including NH4+, hydroxylamine, hydrazine, methylamine, guanidine, and several relatives of guanidine had permeability ratios in the range 1.3--2.0. However, even cations such as imidazole, choline, tris(hydroxymethyl)aminomethane, triethylamine, and glycine methylester were appreciably permeant with permeability ratios of 0.13--0.95. Four compounds with two charged nitrogen groups were also permeant. Molecular models of the permeant ions suggest that the smallest cross-section of the open pore must be at least as large as a square, 6.5 A x 6.5 A. Specific chemical factors seem to be less important than access or friction in determining the ionic selectivity of the endplate channel.     

Monte Carlo Simulation of Release of Vesicular Content in Neuroendocrine Cells

The release of transmitter from the vesicle, its diffusion through the fusion pore, and the cleft and its interaction with the carbon electrode were simulated using the Monte Carlo method. According to the simulation the transmitter release is largely determined by geometric factors – the ratio of the fusion pore cross-sectional and vesicular areas, if the diffusion constant is as in the aqueous solution – but the speed of transmitter dissociation from the gel matrix plays an important role during the rise phase of release. Transmitter is not depleted near the entrance to the fusion pore and there is no cleft-to-vesicle feedback, but the depletion becomes evident if the diffusion constant is reduced, especially if the pore is wide. In general, the time course of amperometric currents closely resembles the time course of the simulated transmitter concentration in the cleft and the time course of release. Surprisingly, even a tenfold change of the electrode efficiency has only a marginal effect on the amplitude or the time course of amperometric currents. Greater electrode efficiency however lowers the cleft concentration, but only if the cleft is narrow. As the cleft widens the current amplitudes diminish and rise times lengthen, but the decay times are less affected. Moreover, the amplitude dependence of the rise and decay times becomes steeper as the cleft widens and/or as the release kinetics slows. Finally, lower diffusion constant of transmitter in the narrow cleft does not further prolong the amperometric currents, whose slow time course reflects slow release kinetics.     

Single-channel and whole-cell currents evoked by acetylcholine in dissociated sympathetic neurons of the rat

Single acetylcholine-activated channels have been recorded from neurons dissociated from the sympathetic chain of 17-21 day old rats. The mean single channel conductance is 35 pS in normal medium containing 1 mM calcium, and 51 pS in the absence of calcium. The measured current amplitudes are about five times more variable than at the frog endplate, at least in part because the current, while the channel is open, is much noisier than when it is shut. Single activations of the receptor by acetylcholine (ACh) produce a burst of openings; the distribution of the burst length has two components, the longer of which is of primary importance in synaptic transmission. Whole-cell currents, in response to ACh (up to 30 microM), show strong inward rectification with no outward current being detectable. This phenomenon is similar whether the intracellular ion is sodium or cesium, whether or not divalent cations are present, and whether or not atropine is present. Nevertheless, outward single-channel currents (of normal conductance) are detectable in isolated outside-out patches.     

Estimates of quantal content during 'chemical potentiation' of transmitter release.

The number of quantal transmitter packets (m), released from motor nerve terminals in response to a single stimulus, has been estimated from the ratio of the amplitudes of endplate currents (e.p.c.) to spontaneous miniature endplate currents (m.e.p.c.), in voltage-clamped endplates of the frog. At 6 degrees C, the average value of m at normal nerve-muscle junctions was about 300. If allowance is made for the temporal dispersion of quantal transmitter release during the e.p.c., this value is increased by about 30%. After treatment with diaminopyridine or tetraethylammonium, transmitter release in response to a nerve stimulus is greatly enhanced and values of m exceeding 10(4) are frequently found. Moreover, the duration of the e.p.c. becomes much longer than that of the m.e.p.cs. The number of packets then liberated during the e.p.c. is much larger than the number of 'active zones' of the endplate and may even exceed the total number of vesicles lined up in twin-files adjacent to the presynaptic membrane.     

Dependence of Miniature Endplate Current on Kinetic Parameters of Acetylcholine Receptors Activation: A Model Study

Mathematical modeling was applied to study the dependence of miniature endplate current (MEPC) amplitude and temporal parameters on the values of the rate constants of acetylcholine binding to receptors (k₊) when cholinesterase was either active or inactive. The simulation was performed under two different sets of parameters describing acetylcholine receptor activation–one with high and another with low probability (Po_high and Po_low) of receptor transition into the open state after double ligand binding. The dependence of model MEPC amplitudes, rise times, and decay times on k₊ differs for set Po_low and set Po_high. The main outcome is that for set Po_high, the rise time is significantly longer at low values of k₊ because of the prolongation of ACh diffusion time to the receptor. For the set Polow, the rise time is shorter at low values of k1, which can be explained by the small probability of AChR forward isomerization after ACh binding and faster MEPC's peak formation.     

The unitary evoked potential at the frog nerve-muscle junction results from synchronous gating of fusion pores at docked vesicles

Exocytosis of a single vesicle has been proposed as the mechanism which determines quantal size by releasing a prepackaged and standard amount of acetylcholine. As first described by del Castillo and Katz (1954) the endplate potential is composed of 100 unitary events and the small variance suggests a binomial release from 100 "discrete patches of membrane". However, exocytosis of 100 vesicles selected randomly from 5000 docked vesicles would yield a variance that is 7 times greater than observed values. We propose that the presynaptic ridge with its compliment of docked vesicles functions as the "discrete patch of membrane" such that arrays of calcium activated fusion pores meter transmitter to form the unit of release. A model based on the synchronous flicker of a large number of fusion pores produces the small variance of both miniature end plate potentials and unitary end plate potentials. Release from a single locus (fusion pore) would generate the sub-MEPP. This model permits vesicle trafficking and vesicular content depletion during tetanic stimulation and explains the frequency dependency of MEPP amplitudes and changes in sub-MEPP to bell-MEPP class ratios.