Electron microscopic serial section analysis of nodes of Ranvier in lumbar spinal roots of the cat: a morphometric study of nodal compartments in fibres of different sizes

Computational models of compound nerve action potentials: Efficient filter-based methods to quantify effects of tissue conductivities, conduction distance, and nerve fiber parameters

BACKGROUND

Peripheral nerve recordings can enhance the efficacy of neurostimulation therapies by providing a feedback signal to adjust stimulation settings for greater efficacy or reduced side effects. Computational models can accelerate the development of interfaces with high signal-to-noise ratio and selective recording. However, validation and tuning of model outputs against in vivo recordings remains computationally prohibitive due to the large number of fibers in a nerve.

METHODS

We designed and implemented highly efficient modeling methods for simulating electrically evoked compound nerve action potential (CNAP) signals. The method simulated a subset of fiber diameters present in the nerve using NEURON, interpolated action potential templates across fiber diameters, and filtered the templates with a weighting function derived from fiber-specific conduction velocity and electromagnetic reciprocity outputs of a volume conductor model. We applied the methods to simulate CNAPs from rat cervical vagus nerve.

RESULTS

Brute force simulation of a rat vagal CNAP with all 1,759 myelinated and 13,283 unmyelinated fibers in NEURON required 286 and 15,860 CPU hours, respectively, while filtering interpolated templates required 30 and 38 seconds on a desktop computer while maintaining accuracy. Modeled CNAP amplitude could vary by over two orders of magnitude depending on tissue conductivities and cuff opening within experimentally relevant ranges. Conduction distance and fiber diameter distribution also strongly influenced the modeled CNAP amplitude, shape, and latency. Modeled and in vivo signals had comparable shape, amplitude, and latency for myelinated fibers but not for unmyelinated fibers.

CONCLUSIONS

Highly efficient methods of modeling neural recordings quantified the large impact that tissue properties, conduction distance, and nerve fiber parameters have on CNAPs. These methods expand the computational accessibility of neural recording models, enable efficient model tuning for validation, and facilitate the design of novel recording interfaces for neurostimulation feedback and understanding physiological systems.

Pathophysiology of the Different Clinical Phenotypes of Chronic Inflammatory Demyelinating Polyradiculoneuropathy (CIDP)

Chronic inflammatory demyelinating polyneuropathy (CIDP) is the most common form of autoimmune polyneuropathy. It is a chronic disease and may be monophasic, progressive or recurrent with exacerbations and incomplete remissions, causing accumulating disability. In recent years, there has been rapid progress in understanding the background of CIDP, which allowed us to distinguish specific phenotypes of this disease. This in turn allowed us to better understand the mechanism of response or non-response to various forms of therapy. On the basis of a review of the relevant literature, the authors present the current state of knowledge concerning the pathophysiology of the different clinical phenotypes of CIDP as well as ongoing research in this field, with reference to key points of immune-mediated processes involved in the background of CIDP.

Small and large cutaneous fibers display different excitability properties to slowly increasing ramp pulses

The excitability of large nerve fibers is reduced when their membrane potential is slowly depolarizing, i.e., the fibers display accommodation. The aim of this study was to assess accommodation in small (mainly Aδ) and large (Aβ) cutaneous sensory nerve fibers using the perception threshold tracking (PTT) technique. Linearly increasing ramp currents (1 ms-200 ms) were used to assess the excitability of the nerve fibers by cutaneous electrical stimulation. To investigate the PPT technique's ability to preferentially activate different fiber types, topical application of lidocaine/prilocaine (EMLA) or a placebo cream was applied. By means of computational modeling, the underlying mechanisms governing the perception threshold in the two fiber types was studied. The axon models included the voltage-gated ion channels: transient TTX-sensitive sodium current, transient TTX-resistant sodium current (Na_TTXr), persistent sodium current, delayed rectifier potassium channel (K_Dr), slow potassium channel, and hyperpolarization-activated current. Large fibers displayed accommodation, whereas small fibers did not display accommodation (P < 0.05). For the pin electrode, a significant interaction was observed between cream (EMLA or placebo) and pulse duration (P < 0.05); for the patch electrode, there was no significant interaction between cream and duration, which supports the pin electrode's preferential activation of small fibers. The results from the computational model suggested that differences in accommodation between the two fiber types may originate from selective expression of voltage-gated ion channels, particularly the transient Na_TTXr and/or K_Dr. The PTT technique could assess the excitability changes during accommodation in different nerve fibers. Therefore, the PTT technique may be a useful tool for studying excitability in nerve fibers in both healthy and pathological conditions.NEW & NOTEWORTHY When large nerve fibers are stimulated by long, slowly increasing electrical pulses, interactive mechanisms counteract the stimulation, which is called accommodation. The perception threshold tracking technique was able to assess accommodation in both small and large fibers. The novelty of this study is that large fibers displayed accommodation, whereas small fibers did not. Additionally, the difference in accommodation between the fiber could be linked to expression of voltage-gated ion channels by means of computational modeling.

From Perception Threshold to Ion Channels-A Computational Study

Small-surface-area electrodes have successfully been used to preferentially activate cutaneous nociceptors, unlike conventional large area-electrodes, which preferentially activate large non-nociceptor fibers. Assessments of the strength-duration relationship, threshold electrotonus, and slowly increasing pulse forms have displayed different perception thresholds between large and small surface electrodes, which may indicate different excitability properties of the activated cutaneous nerves. In this study, the origin of the differences in perception thresholds between the two electrodes was investigated. It was hypothesized that different perception thresholds could be explained by the varying distributions of voltage-gated ion channels and by morphological differences between peripheral nerve endings of small and large fibers. A two-part computational model was developed to study activation of peripheral nerve fibers by different cutaneous electrodes. The first part of the model was a finite-element model, which calculated the extracellular field delivered by the cutaneous electrodes. The second part of the model was a detailed multicompartment model of an Aδ-axon as well as an Aβ-axon. The axon models included a wide range of voltage-gated ion channels: Na_TTXs, Na_TTXr, Na_p, K_dr, K_M, K_A, and HCN channel. The computational model reproduced the experimentally assessed perception thresholds for the three protocols, the strength-duration relationship, the threshold electrotonus, and the slowly increasing pulse forms. The results support the hypothesis that voltage-gated ion channel distributions and morphology differences between small and large fibers were sufficient to explain the difference in perception thresholds between the two electrodes. In conclusion, assessments of perception thresholds using the three protocols may be an indirect measurement of the membrane excitability, and computational models may have the possibility to link voltage-gated ion channel activation to perception threshold measurements.

Local Acceleration of Neurofilament Transport at Nodes of Ranvier

Myelinated axons are constricted at nodes of Ranvier. These constrictions are important physiologically because they increase the speed of saltatory nerve conduction, but they also represent potential bottlenecks for the movement of axonally transported cargoes. One type of cargo are neurofilaments, which are abundant space-filling cytoskeletal polymers that function to increase axon caliber. Neurofilaments move bidirectionally along axons, alternating between rapid movements and prolonged pauses. Strikingly, axon constriction at nodes is accompanied by a reduction in neurofilament number that can be as much as 10-fold in the largest axons. To investigate how neurofilaments navigate these constrictions, we developed a transgenic mouse strain that expresses a photoactivatable fluorescent neurofilament protein in neurons. We used the pulse-escape fluorescence photoactivation technique to analyze neurofilament transport in mature myelinated axons of tibial nerves from male and female mice of this strain ex vivo Fluorescent neurofilaments departed the activated region more rapidly in nodes than in flanking internodes, indicating that neurofilament transport is faster in nodes. By computational modeling, we showed that this nodal acceleration can be explained largely by a local increase in the duty cycle of neurofilament transport (i.e., the proportion of the time that the neurofilaments spend moving). We propose that this transient acceleration functions to maintain a constant neurofilament flux across nodal constrictions, much as the current increases where a river narrows its banks. In this way, neurofilaments are prevented from piling up in the flanking internodes, ensuring a stable neurofilament distribution and uniform axonal morphology across these physiologically important axonal domains.SIGNIFICANCE STATEMENT Myelinated axons are constricted at nodes of Ranvier, resulting in a marked local decrease in neurofilament number. These constrictions are important physiologically because they increase the efficiency of saltatory nerve conduction, but they also represent potential bottlenecks for the axonal transport of neurofilaments, which move along axons in a rapid intermittent manner. Imaging of neurofilament transport in mature myelinated axons ex vivo reveals that neurofilament polymers navigate these nodal axonal constrictions by accelerating transiently, much as the current increases where a river narrows its banks. This local acceleration is necessary to ensure a stable axonal morphology across nodal constrictions, which may explain the vulnerability of nodes of Ranvier to neurofilament accumulations in animal models of neurotoxic neuropathies and neurodegenerative diseases.

The effects of paranodal myelin damage on action potential depend on axonal structure

Biophysical computational models of axons provide an important tool for quantifying the effects of injury and disease on signal conduction characteristics. Several studies have used generic models to study the average behavior of healthy and injured axons; however, few studies have included the effects of normal structural variation on the simulated axon's response to injury. The effects of variations in physiological characteristics on axonal function were mapped by altering the structure of the nodal, paranodal, and juxtaparanodal regions across reported values in three different caliber axons (1, 2, and 5.7 μm). Myelin detachment and retraction were simulated to quantify the effects of each injury mechanism on signal conduction. Conduction velocity was most affected by axonal fiber diameter (89%), while membrane potential amplitude was most affected by nodal length (86%) in healthy axons. Postinjury axonal functionality was most affected by myelin detachment in the paranodal and juxtaparanodal regions when retraction and detachment were modeled simultaneously. The efficacy of simulated potassium channel blockers on restoring membrane potential and velocity varied with axonal caliber and injury type. The structural characteristics of axons affect their functional response to myelin retraction and detachment and their subsequent response to potassium channel blocker treatment.

Node of Ranvier length as a potential regulator of myelinated axon conduction speed

Myelination speeds conduction of the nerve impulse, enhancing cognitive power. Changes of white matter structure contribute to learning, and are often assumed to reflect an altered number of myelin wraps. We now show that, in rat optic nerve and cerebral cortical axons, the node of Ranvier length varies over a 4.4-fold and 8.7-fold range respectively and that variation of the node length is much less along axons than between axons. Modelling predicts that these node length differences will alter conduction speed by ~20%, similar to the changes produced by altering the number of myelin wraps or the internode length. For a given change of conduction speed, the membrane area change needed at the node is >270-fold less than that needed in the myelin sheath. Thus, axon-specific adjustment of node of Ranvier length is potentially an energy-efficient and rapid mechanism for tuning the arrival time of information in the CNS.

DOI:http://dx.doi.org/10.7554/eLife.23329.001

Information is transmitted around the nervous system as electrical signals passing along nerve cells. A fatty substance called myelin, which is wrapped around the nerve cells, increases the speed with which the signals travel along the nerve cells. This allows us to think and move faster than we would otherwise be able to do.

The electrical signals start at small “nodes” between areas of myelin wrapping. Originally it was thought that we learn things mainly as a result of changes in the strength of connections between nerve cells, but recently it has been proposed that changes in myelin wrapping could also contribute to learning.

Arancibia-Cárcamo, Ford, Cossell et al. investigated how much node structure varies in rat nerve cells, and whether differences in the length of nodes can fine-tune the activity of the nervous system. The experiments show that rat nerve cells do indeed have nodes with a range of different lengths. Calculations show that this could result in electrical signals moving at different speeds through different nerve cells.

These findings raise the possibility that nerve cells actively alter the length of their nodes in order to alter their signal speed. The next step is to try to show experimentally that this happens during learning in animals.

DOI:http://dx.doi.org/10.7554/eLife.23329.002

Analyzing the tradeoff between electrical complexity and accuracy in patient-specific computational models of deep brain stimulation

OBJECTIVE

Deep brain stimulation (DBS) is an adjunctive therapy that is effective in treating movement disorders and shows promise for treating psychiatric disorders. Computational models of DBS have begun to be utilized as tools to optimize the therapy. Despite advancements in the anatomical accuracy of these models, there is still uncertainty as to what level of electrical complexity is adequate for modeling the electric field in the brain and the subsequent neural response to the stimulation.

APPROACH

We used magnetic resonance images to create an image-based computational model of subthalamic DBS. The complexity of the volume conductor model was increased by incrementally including heterogeneity, anisotropy, and dielectric dispersion in the electrical properties of the brain. We quantified changes in the load of the electrode, the electric potential distribution, and stimulation thresholds of descending corticofugal (DCF) axon models.

MAIN RESULTS

Incorporation of heterogeneity altered the electric potentials and subsequent stimulation thresholds, but to a lesser degree than incorporation of anisotropy. Additionally, the results were sensitive to the choice of method for defining anisotropy, with stimulation thresholds of DCF axons changing by as much as 190%. Typical approaches for defining anisotropy underestimate the expected load of the stimulation electrode, which led to underestimation of the extent of stimulation. More accurate predictions of the electrode load were achieved with alternative approaches for defining anisotropy. The effects of dielectric dispersion were small compared to the effects of heterogeneity and anisotropy.

SIGNIFICANCE

The results of this study help delineate the level of detail that is required to accurately model electric fields generated by DBS electrodes.

Minimizing the caliber of myelinated axons by means of nodal constrictions

In myelinated axons, most of the voltage-gated ion channels are concentrated at the nodes of Ranvier, which are short gaps in the myelin sheath. This arrangement leads to saltatory conduction and a larger conduction velocity than in nonmyelinated axons. Intriguingly, axons in the peripheral nervous system that exceed about 2 μm in diameter exhibit a characteristic narrowing of the axon at nodes that results in a local reduction of the axonal cross-sectional area. The extent of constriction increases with increasing internodal axonal caliber, reaching a threefold reduction in diameter for the largest axons. In this paper, we use computational modeling to investigate the effect of nodal constrictions on axonal conduction velocity. For a fixed number of ion channels, we find that there is an optimal extent of nodal constriction which minimizes the internodal axon caliber that is required to achieve a given target conduction velocity, and we show that this is sensitive to the precise geometry of the axon and myelin sheath in the flanking paranodal regions. Thus axonal constrictions at nodes of Ranvier appear to be a biological adaptation to minimize axonal volume, thereby maximizing the spatial and metabolic efficiency of these processes, which can be a significant evolutionary constraint. We show that the optimal nodal morphologies are relatively insensitive to changes in the number of nodal sodium channels.

Axon-somatic back-propagation in detailed models of spinal alpha motoneurons

Antidromic action potentials following distal stimulation of motor axons occasionally fail to invade the soma of alpha motoneurons in spinal cord, due to their passing through regions of high non-uniformity. Morphologically detailed conductance-based models of cat spinal alpha motoneurons have been developed, with the aim to reproduce and clarify some aspects of the electrophysiological behavior of the antidromic axon-somatic spike propagation. Fourteen 3D morphologically detailed somata and dendrites of cat spinal alpha motoneurons have been imported from an open-access web-based database of neuronal morphologies, NeuroMorpho.org, and instantiated in neurocomputational models. An axon hillock, an axonal initial segment and a myelinated axon are added to each model. By sweeping the diameter of the axonal initial segment (AIS) and the axon hillock, as well as the maximal conductances of sodium channels at the AIS and at the soma, the developed models are able to show the relationships between different geometric and electrophysiological configurations and the voltage attenuation of the antidromically traveling wave. In particular, a greater than usually admitted sodium conductance at AIS is necessary and sufficient to overcome the dramatic voltage attenuation occurring during antidromic spike propagation both at the myelinated axon-AIS and at the AIS-soma transitions.

The energetics of CNS white matter

The energetics of CNS white matter are poorly understood. We derive a signaling energy budget for the white matter (based on data from the rodent optic nerve and corpus callosum) which can be compared with previous energy budgets for the gray matter regions of the brain, perform a cost-benefit analysis of the energetics of myelination, and assess mechanisms for energy production and glucose supply in myelinated axons. We show that white matter synapses consume ≤0.5% of the energy of gray matter synapses and that this, rather than more energy-efficient action potentials, is the main reason why CNS white matter uses less energy than gray matter. Surprisingly, while the energetic cost of building myelin could be repaid within months by the reduced ATP cost of neuronal action potentials, the energetic cost of maintaining the oligodendrocyte resting potential usually outweighs the saving on action potentials. Thus, although it dramatically speeds action potential propagation, myelination need not save energy. Finally, we show that mitochondria in optic nerve axons could sustain measured firing rates with a plausible density of glucose transporters in the nodal membrane, without the need for energy transfer from oligodendrocytes.

Breakdown of accommodation in nerve: a possible role for persistent sodium current

Background

Accommodation and breakdown of accommodation are important elements of information processing in nerve fibers, as they determine how nerve fibers react to natural slowly changing stimuli or electrical stimulation. The aim of the present study was to elucidate the biophysical mechanism of breakdown of accommodation, which at present is unknown.

Results

A model of a space-clamped motor nerve fiber was developed. It was found that this new model could reproduce breakdown of accommodation when it included a low-threshold, rapidly activating, persistent sodium current. However, the phenomenon was not reproduced when the persistent sodium current did not have fast activation kinetics or a low activation threshold.

Conclusion

The present modeling study suggests that persistent, low-threshold, rapidly activating sodium currents have a key role in breakdown of accommodation, and that breakdown of accommodation can be used as a tool for studying persistent sodium current under normal and pathological conditions.

Modeling the excitability of mammalian nerve fibers: influence of afterpotentials on the recovery cycle

Human nerve fibers exhibit a distinct pattern of threshold fluctuation following a single action potential known as the recovery cycle. We developed geometrically and electrically accurate models of mammalian motor nerve fibers to gain insight into the biophysical mechanisms that underlie the changes in axonal excitability and regulate the recovery cycle. The models developed in this study incorporated a double cable structure, with explicit representation of the nodes of Ranvier, paranodal, and internodal sections of the axon as well as a finite impedance myelin sheath. These models were able to reproduce a wide range of experimental data on the excitation properties of mammalian myelinated nerve fibers. The combination of an accurate representation of the ion channels at the node (based on experimental studies of human, cat, and rat) and matching the geometry of the paranode, internode, and myelin to measured morphology (necessitating the double cable representation) were needed to match the model behavior to the experimental data. Following an action potential, the models generated both depolarizing (DAP) and hyperpolarizing (AHP) afterpotentials. The model results support the hypothesis that both active (persistent Na(+) channel activation) and passive (discharging of the internodal axolemma through the paranodal seal) mechanisms contributed to the DAP, while the AHP was generated solely through active (slow K(+) channel activation) mechanisms. The recovery cycle of the fiber was dependent on the DAP and AHP, as well as the time constant of activation and inactivation of the fast Na(+) conductance. We propose that experimentally documented differences in the action potential shape, strength-duration relationship, and the recovery cycle of motor and sensory nerve fibers can be attributed to kinetic differences in their nodal Na(+) conductances.

Modelling the effects of electric fields on nerve fibres: influence of the myelin sheath

The excitation and conduction properties of computer-based cable models of mammalian motor nerve fibres, incorporating three different myelin representations, are compared. The three myelin representations are a perfectly insulating single cable (model A), a finite impedance single cable (model B) and a finite impedance double cable (model C). Extracellular stimulation of the three models is used to study their strength-duration and current-distance (I-X) relationships, conduction velocity (CV) and action potential shape. All three models have a chronaxie time that is within the experimental range. Models B and C have increased threshold currents compared with model A, but each model has slope to the I-X relationship that matches experimental results. Model B has a CV that matches experimental data, whereas the CV of models A and C are above and below the experimental range, respectively. Model C is able to produce a depolarising afterpotential (DAP), whereas models A and B exhibit hyperpolarising afterpotentials. Models A and B are determined to be the preferred models when low-frequency stimulation (< approximately 25 Hz) is used, owing to their efficiency and accurate excitation and conduction properties. For high frequency stimulation (approximately 25 Hz and greater), model C, with its ability to produce a DAP, is necessary accurately to simulate excitation behaviour.

Computational analysis of action potential initiation in mitral cell soma and dendrites based on dual patch recordings

In olfactory mitral cells, dual patch recordings show that the site of action potential initiation can shift between soma and distal primary dendrite and that the shift is dependent on the location and strength of electrode current injection. We have analyzed the mechanisms underlying this shift, using a model of the mitral cell that takes advantage of the constraints available from the two recording sites. Starting with homogeneous Hodgkin-Huxley-like Na(+)-K(+) channel distribution in the soma-dendritic region and much higher sodium channel density in the axonal region, the model's channel kinetics and density were adjusted by a fitting algorithm so that the model response was virtually identical to the experimental data. The combination of loading effects and much higher sodium channel density in the axon relative to the soma-dendritic region results in significantly lower "voltage threshold" for action potential initiation in the axon; the axon therefore fires first unless the voltage gradient in the primary dendrite is steep enough for it to reach its higher threshold. The results thus provide a quantitative explanation for the stimulus strength and position dependence of the site of action potential initiation in the mitral cell.

Development of nodes of Ranvier in feline nerves: an ultrastructural presentation

The ultrastructure of developing nodes of Ranvier and adjacent paranodes of future large myelinated fibers in feline lumbar spinal roots is described. The development starts before birth concurrent with myelination and is finished at the end of the first postnatal month when the nodal regions of future large fibers, now 4-5 microns of diameter, for the first time appear like miniatures of those of their 4 times thicker and fully mature counterparts. At this stage the fibers also begin to show mature functional properties. The latent maturation process is denoted "nodalization" and includes two major events: (1) the formation of a narrow node gap bordered by compact myelin segments and filled with Schwann cell microvilli that interconnect an undercoated nodal axolemma with rapidly increasing accumulations of mitochondria lodging in the longitudinal cords of Schwann cell cytoplasm that is distributed outside a more and more crenated paranodal myelin sheath; (2) the setting of a fixed number of nodes along the axons; an event that includes segmental axonal and myelin sheath degeneration and is concluded by the elimination of supernumerary Schwann cells.

Axonal constriction at Ranvier's node increases during development

We have studied the ratio between the nodal and the internodal diameter (the dn/d(in) ratio) of large myelinated axons in the L7 ventral spinal root of the cat during pre- and postnatal development using light and electron microscopy. A substantial nodal constriction, dn/d(in) = 0.6, was found at the beginning of myelination, about 2 weeks before birth. The ratio decreased during the subsequent 10 weeks and approached the adult value of 0.47 (SE 0.01, N = 45) in the 8 weeks old kitten. The observations are discussed with respect to the maturation of the nodal region and to our earlier idea that the constricted nodal axon segments of large peripheral myelinated nerve fibres of adult cats and kittens 2 months and more of age are sites capable of interacting with and perhaps even controlling the passage of axonally transported materials.

Axoplasmic organelles at nodes of Ranvier. II. Occurrence and distribution in large myelinated spinal cord axons of the adult cat

The occurrence and distribution of axoplasmic organelles in large myelinated axons of the ventral, the lateral and the dorsal funiculi of L7 spinal cord segments of the cat have been studied using electron microscopy (EM). Most organelles were found to be concentrated to the paranode-node-paranode (pnp)-regions and they showed their highest relative concentration in the constricted part of these regions, i.e. at the nodes of Ranvier. In the paranode-node-paranode-regions of the lateral and dorsal funiculi, large dense bodies predominated distal to the nodal mid-level and vesiculo-tubular membranous organelles proximal to it. This pattern of organelle distribution, a proximo-distal (with reference to the neuron soma) segregation of the organelles, was only faintly indicated in the paranode-node-paranode-regions of the alpha motor axons of the ventral funiculus. These paranode-node-paranode-regions were, apart from a weak proximo-distal segregation of a few organelles, characterized by deposits of electron dense granules and clusters of large round mitochondria. We conclude that there are two types of organelle accumulation and distribution in the paranode-node-paranode-regions of large spinal cord nerve fibres of the cat. One type is found in the lateral and dorsal funiculi, i.e. in axons with terminal (synaptic) fields inside the blood-brain-barrier. The other type is found in the alpha motor axons of the ventral funiculus, i.e. in axons with their terminal field in the PNS and thus outside the blood-brain barrier. It should be noted that retrogradely transported material in the alpha motor axons has passed through a long sequence of paranode-node-paranode-regions equipped with Schwann cells before it reaches the CNS, while material transported retrogradely in the axons of the dorsal and lateral funiculi has not. The following discussion includes a comparison of the organelle accumulation and distribution in these two types of CNS paranode-node-paranode-regions with the organelle accumulation and distribution observed in the paranode-node-paranode-regions of PNS axons.

Axoplasmic organelles at nodes of Ranvier. I. Occurrence and distribution in large myelinated spinal root axons of the adult cat

Using light microscopy (LM) and electron microscopy (EM) we have examined the occurrence and distribution of axoplasmic organelles in large myelinated nerve fibres of the L7 ventral and dorsal spinal roots of the cat with special reference to the paranode-node-paranode (pnp)-regions. Ninety-eight percent of the 550 Toluidine Blue-stained paranode-node-paranode-regions examined in the light microscope contained dark-blue bodies accumulated distal to the midlevel of the paranode-node-paranode-region. Further, a veil of Toluidine Blue positive material was observed in about 50% of the paranode-node paranode-regions. In about 25% of these paranode-node-paranode-regions the veil lay distal to the midlevel of the paranode-node-paranode-region and in the remainder it lay proximally. Electron microscopy suggested that the ultrastructural equivalents of the dark-blue bodies and of the veil were dense lamellar bodies and a diffuse granular material, respectively. Our calculations indicate that from 70% to more than 90% of some organelles (dense lamellar bodies, multivesicular bodies and vesiculo-tubular membranous organelles) present in an axon are accumulated in the paranode-node-paranode-regions. The occurrence of these organelles in the individual paranode-node-paranode-regions varied within wide limits also in adjacent fibres. The dense lamellar and multivesicular bodies dominated the distal part of the paranode-node-paranode-regions while the vesiculo-tubular membranous organelles dominated the proximal part, i.e. the organelles showed a mutual proximo-distal segregation with reference to the midlevel of the paranode-node-paranode-region. Of seventeen paranode-node-paranode-regions analyzed ultrastructurally, seven were classified as 'fully segregated', that is 67% or more of the lamellar and multivescular bodies, present in the whole paranode-node-paranode-region, lay distal to the mid-level, and 67% or more of the vesiculo-tubular membranous organelles lay proximal to it.

Nodes of Ranvier and myelin sheath dimensions along exceptionally thin myelinated vertebrate PNS axons

The trigeminal alveolar branch in the lower jaw of the cichlid Tilapia mariae was examined by light and electron microscopy on single and serial sections, and by light microscopy on teased fibre preparations. The principal purpose was to find out if the exceptionally thin myelinated axons (d < 1 micron) present in this nerve possess true nodes of Ranvier, and to determine the dimensions of their myelin sheaths. This necessitated analysis of the whole size range of myelinated fibres, with respect to nodal and internodal morphology. The results show that the exceptionally thin myelinated fibres exhibit primitive nodal regions, with patches of axolemmal undercoating, and few Schwann cell processes in the node gap. This contrasts with the more complex nodal organization seen in larger trigeminal alveolar branch fibres. For the whole population of myelinated fibres the number of myelin lamellae increases rectilinearly with axon diameter, and sheath length increases with fibre diameter according to a logarithmic expression. The myelin sheaths of the exceptionally thin trigeminal alveolar branch fibres are composed of 10-20 lamellae, and extend 35-50 microns along the axon. These results show that the structural complexity of nodal regions in the trigeminal alveolar branch decreases with decreasing fibre size, that the exceptionally thin myelinated trigeminal alveolar branch fibres possess primitive nodes and that they have very short myelin sheaths. Our crude theoretical calculations suggest that these fibres might be capable of saltatory conduction.

Three types of sodium channels in adult rat dorsal root ganglion neurons

Several types of Na+ currents have previously been demonstrated in dorsal root ganglion (DRG) neurons isolated from neonatal rats, but their expression in adult neurons has not been studied. Na+ current properties in adult dorsal root ganglion (DRG) neurons of defined size class were investigated in isolated neurons maintained in primary culture using a combination of microelectrode current clamp, patch voltage clamp and immunocytochemical techniques. Intracellular current clamp recordings identified differing relative contributions of TTX-sensitive and -resistant inward currents to action potential waveforms in DRG neuronal populations of defined size. Patch voltage clamp recordings identified three distinct kinetic types of Na+ current differentially distributed among these size classes of DRG neurons. 'Small' DRG neurons co-express two types of Na+ current: (i) a rapidly-inactivating, TTX-sensitive 'fast' current and (ii) a slowly-activating and -inactivating, TTX-resistant 'slow' current. The TTX-sensitive Na+ current in these cells was almost completely inactivated at typical resting potentials. 'Large' cells expressed a single TTX-sensitive Na+ current identified as 'intermediate' by its inactivation rate constants. 'Medium'-sized neurons either co-expressed 'fast' and 'slow' current or expressed only 'intermediate' current. Na+ channel expression in these size classes was also measured by immunocytochemical techniques. An antibody against brain-type Na+ channels (Ab7493)10 labeled small and large neurons with similar intensity. These results demonstrate that three types of Na+ currents can be detected which correlate with electrogenic properties of physiologically and anatomically distinct populations of adult rat DRG neurons.

Axonal cytoskeleton at the nodes of Ranvier

The relationship between the degree of nodal narrowing and the changes in the structure of the axonal cytoskeleton was studied in 53 fibres of mouse sciatic nerve. Nodal narrowing increased with increasing fibre calibre to reach about 20% of the internodal area in the thicker fibres. The narrowing corresponded quantitatively to a decreased number of nodal neurofilaments. Nodal microtubule numbers varied greatly, and a majority of fibres had considerably (approximately 55%) more microtubules in their nodal profile than in the internode. Nodal profiles of different calibre showed an increase in the number of filaments and of microtubules with nodal calibre, although at rates different from those in the internode. The degree of observed axon non-circularities had no discernible effect on the restructuring of the axonal cytoskeleton at the node. A transnodal transport of the axonal cytoskeleton can occur with: (1) accelerated transnodal transport of filaments, (2) stationary internodal fraction of filaments, (3) depolymerization of filaments proximal to the node and repolymerization distally, or (4) different nodal and internodal polymerization equilibria.

Sodium channels in the cytoplasm of Schwann cells

Immunoblotting, ultrastructural immunocytochemistry, and tritiated saxitoxin ([3H]STX) binding experiments were used to study sodium channel localization in Schwann cells. Polyclonal antibody 7493, which is directed against purified sodium channels from rat brain, specifically recognizes a 260-kDa protein corresponding to the alpha subunit of the sodium channel in immunoblots of crude glycoproteins from rat sciatic nerve. Electron microscopic localization of sodium channel immunoreactivity within adult rat sciatic nerves reveals heavy staining of the axon membrane at the node of Ranvier, in contrast to the internodal axon membrane, which does not stain. Schwann cells including perinodal processes also exhibit antibody 7493 immunoreactivity, localized within both the cytoplasm and the plasmalemma of the Schwann cell. To examine further the possibility that sodium channels are localized within Schwann cell cytoplasm, [3H]STX binding was studied in cultured rabbit Schwann cells, both intact and after homogenization. Saturable binding of STX was significantly higher in homogenized Schwann cells (410 +/- 37 fmol/mg of protein) than in intact Schwann cells (214 +/- 21 fmol/mg of protein). Moreover, the equilibrium dissociation constant was higher for homogenized preparations (1.77 +/- 0.37 nM) than for intact Schwann cells (1.06 +/- 0.29 nM). These data suggest the presence of an intracellular pool of sodium channels or channel precursors in Schwann cells.

Voltage-sensitive Na+ channels in mammalian peripheral nerves detected using scorpion toxins

The localization of voltage-sensitive sodium channels was investigated in mouse, rat and rabbit sciatic nerves using iodinated alpha- and beta-Scorpion toxins (ScTx) as specific probes. Saturable specific binding for a beta-ScTx was detected in mouse sciatic nerve homogenates (Kd = 90 pM, binding site capacity = 90 fmol mg-1 protein). LM autoradiographic studies demonstrated that the two types of ScTx stained the Ranvier nodes of the myelinated fibres, and also showed a clear but weaker labelling of the unmyelinated Remak bundles. In the sciatic nerve, which is widely considered as a model 'myelinated nerve', the nodal membrane represented only a small fraction of the total axonal membranes (0.2% and 0.05% for mouse and rabbit sciatic nerves respectively). Therefore, despite their high channel density, nodal membranes contribute only a small proportion of the total labelling by beta-ScTx (15% and 2.3% for mouse and rabbit sciatic nerves respectively), with the major contribution to labelling arising from unmyelinated axons. The distribution of specific binding sites for a beta-Scorpion toxin was then analysed in cross-sections of rabbit sciatic nerve at the EM level. The quantitative analysis of autoradiograms involved three methods, the 50% probability circle method, and two cross-fire analyses using either systematically distributed hypothetical sources or hypothetical sources only located on the plasma membranes of axons and of Schwann cells associated with unmyelinated Remak bundles. No specific beta-Scorpion toxin binding sites were detected at the plasma membrane of Schwann cells from either myelinated fibres or unmyelinated bundles, or at the internodal surface of myelinated axons. Sites were only detected at the surface of unmyelinated axons and at nodal axolemma. Their density in unmyelinated axons was found to be in the range of 1-6 per micron2 of plasma membrane surface area by combining quantitative EM autoradiography and stereological measurements.

Sodium currents in Schwann cells from myelinated and non-myelinated nerves of neonatal and adult rabbits

1. Patch-clamp methods were used to study sodium channels in Schwann cells obtained from four different tissue sources. Primary cultures of Schwann cells were prepared from the sciatic nerve and from the vagus nerve of neonatal and of adult rabbits. In the adult, the sciatic is predominantly myelinated whereas the vagus is predominantly non-myelinated. Whole-cell currents, and single-channel currents in outside-out membrane patches, were analysed. 2. No substantial differences were noted in the passive electrical properties (input resistance, cell capacitance, resting membrane potential) of the four groups of cells. Similarly, no substantial differences were found in the average properties of sodium currents (maximum current, maximum conductance, time-to-peak current, current-voltage relation, h infinity relation) recorded from each type of cell in cultures less than 8 days old. At 10-17 days a fall in the size of the sodium currents recorded from cells in the vagal cultures was found. 3. Exposure of the cells to proteolytic enzymes or collagenase, under conditions similar to those used when the cells were put in culture initially, substantially reduced the size of the peak sodium currents recorded from the cells 24 h later. 4. The results of experiments on Schwann cells with retracted processes indicated that sodium channels are present in the processes extending from each pole of the cell soma and that the plasmalemmal density of these channels in the processes is about the same as it is at the soma. 5. Recordings from outside-out patches revealed no apparent differences in the properties of single-channel sodium currents in patches from cells obtained from the four different sources. The single-channel conductance was about 20 pS for each of the four groups. Ensemble currents from single-channel records were similar in time course to those of whole-cell currents. 6. Saxitoxin reduced the maximum sodium conductance in Schwann cells and bound to the cells with equally high affinity. The equilibrium dissociation constant was about 2 nM at 20-22 degrees C. 7. It is argued that the expression of sodium channels in myelinating Schwann cells does not differ substantially from that of non-myelinating Schwann cells.

The action of pyrethroids on sodium channels in myelinated nerve fibres and spinal ganglion cells of the frog

The interaction of pyrethroids with the voltage-dependent sodium channel was studied in voltage-clamped nodes of Ranvier and isolated spinal ganglion neurons of the clawed frog, Xenopus laevis. In the node, pyrethroids prolonged the sodium tail current associated with a step repolarization of the membrane. It was found that the amplitude of the slow, pyrethroid-induced, sodium tail current (PIT) first increased and then decreased as a function of the duration of membrane depolarization (to -5 mV). This decrease of the PIT amplitude was absent when depolarizations to the sodium equilibrium potential (+40 mV) were used. Measurements of changes in sodium reversal potential indicated that sodium ion depletion in the perinodal space is largely responsible for the inactivation of the pyrethroid-modified sodium current. Inactivation is not completely abolished by pyrethroid treatment since the probability of channel opening, measured in membrane patches excised from spinal ganglion cells, decreased slowly during prolonged depolarization. Analysis of unitary currents indicated that both activation and inactivation are retarded by pyrethroids. The arrival of sodium channels in the pyrethroid-modified open state followed a time course that was slower than both activation and inactivation of unmodified sodium channels. Our findings indicate that sodium channels are modified when in the closed resting state and that both opening and closing kinetics are delayed by pyrethroids.

The perinodal astrocyte

Several studies have demonstrated the presence of perinodal astrocyte processes at nodes of Ranvier in the central nervous system, suggesting that, in addition to the axon and oligodendrocyte, astrocytes participate in the formation of mature central nodes. The specific association between perinodal astrocyte processes and nodal membrane develops at the time of, or soon after, the appearance of relatively differentiated nodes of Ranvier. This interaction is likely to be mediated by cell adhesion molecules. J1 is a member of a family of glycoproteins that share a common carbohydrate epitope, designated L2/HNK-1, and that have been implicated in cell-cell interactions. This glycoprotein is concentrated at the interface between perinodal astrocyte processes and the nodal region of the axon. Moreover, N-CAM, which is a member of the same family as J1, and cytotactin, an extracellular matrix component produced by glia, are localized at the interface between the axon and perinodal astrocyte processes at nodes of Ranvier. The association of perinodal astrocyte processes with nodal membrane in the central nervous system is similar to that exhibited by perinodal Schwann cell processes at peripheral nodes, and similar functional properties have been suggested for these two glial cell processes, including production of nodal gap substance, buffering of perinodal extracellular ion concentration, and development and/or maintenance of nodal specializations in the axon membrane. Perinodal astrocyte and Schwann cell processes may also function as extraneuronal sites for the synthesis of voltage-sensitive sodium channels, to complement neuronal perikaryal synthesis and axonal transport. Ultrastructural studies on specialized patches of axon membrane within some unmyelinated, demyelinated, and dysmyelinated axons support the hypothesis of a specific role for perinodal astrocyte processes in the assembly, stabilization, and/or maintenance of axolemma with nodal characteristics. These observations suggest a multiplicity of functions for perinodal astrocyte processes at central nodes and implicate the astrocyte as an important component of the node of Ranvier.

Macromolecular structure of the Schwann cell membrane. Perinodal microvilli

The macromolecular structure of perinodal Schwann cell membrane was examined with freeze-fracture electron microscopy. Perinodal microvillous-like processes of Schwann cells exhibit an asymmetrical partitioning of intramembranous particles (IMPs), with a moderate (approximately 900/microns2) density of particles on P-faces and a lower (approximately 300/microns2) density of IMPs on E-faces. The densities of IMPs observed on the fracture faces of perinodal processes are similar to those within the outer membrane of the Schwann cell proper. On both fracture faces of the perinodal processes and the Schwann cell membrane proper, a high (approximately 45%) percentage of the IMPs displayed a large (greater than or equal to 9.6 nm) diameter. Specialized junctions (i.e., gap junctions, tight junctions) between adjacent perinodal Schwann cell processes or between perinodal processes and nodal axolemmal were not observed.

Progressive axonopathy: an inherited neuropathy of boxer dogs. 3. The peripheral axon lesion with special reference to the nerve roots

Progressive axonopathy is an autosomal recessive inherited neuropathy of Boxer dogs with lesions in the CNS and PNS. This paper describes the axonal changes in the lumbar and cervical nerve roots and tibial nerve. By 2 months of age the proximal paranodal areas of many larger diameter fibres show small axonal swellings, sometimes with attenuation or loss of the associated myelin sheath. Axoplasmic changes within swollen and non-swollen fibres include disorganization of the peripheral neurofilaments and small accumulations of vesicles and vesiculo-tubular profiles, particularly in the sub-axolemmal area. Occasional fibres, more often in the cervical roots, are massively distended with disorganized neurofilaments. The frequency of the membranous accumulations decreases with progression of the disease. Many axons show a markedly irregular or corrugated outline and are surrounded by an attenuated sheath. The peripheral axonal cytoskeleton is disorganized and misaligned, whereas the central structures maintain a more normal arrangement. Regenerating axonal clusters are common in the cervical ventral roots but occur infrequently in the lumbar roots. Similar axonal changes occur in the peripheral nerves but at a much lower frequency. Any membranous accumulations or cytoskeletal disorganization are more probable in the proximal tibial nerves, while the frequency of axonal degeneration and regeneration increases distally. The morphological appearances indicate gross disturbances in axon-sheath cell relationships and suggest that abnormalities in the transport of various axoplasmic organelles may be involved in the pathogenesis of the axonal lesion.

The axon tree of rat motor fibres: morphometry and fine structure

A quantitative light and electron microscopic study of the axon tree of rat motor fibres was undertaken to supply data relevant to the understanding of the spread of excitation. Continuous proximodistal foreshortening of internode length and dwindling of fibre calibre were statistically verified. Internodes had progressively foreshortened geometric proportions (length/diameter quotient). The postbranching internodes were significantly shorter than would correspond to the general trend, but no such foreshortening was evident for the prebranching internodes. Relative sheath thickness (g-ratio, i.e. quotient axon diameter/fibre diameter) of filial fibres did not differ from the stem. Increase in axon area in filial fibres versus stem fibre averaged 1.3. The total proximodistal increase in axoplasmic area from the stem fibre to the distal branches was less than two since increases at branch points were compensated by the proximodistal dwindling of fibres. Nodal membrane area of branch points was greater than in nonbranching fibres, and there were larger than normal microvillar spaces. The majority of branches were approximately symmetric, but asymmetric branchings were also found. The thinner branches of these had wider nodal gaps than the thick branches. The observed changes were interpreted as adaptations to facilitate uniform spread of excitation along the axon tree; asymmetric branchings, however, may permit routing of impulses.

Organization of ion channels in the myelinated nerve fiber

The functional organization of the mammalian myelinated nerve fiber is complex and elegant. In contrast to nonmyelinated axons, whose membranes have a relatively uniform structure, the mammalian myelinated axon exhibits a high degree of regional specialization that extends to the location of voltage-dependent ion channels within the axon membrane. Sodium and potassium channels are segregated into complementary membrane domains, with a distribution reflecting that of the overlying Schwann or glial cells. This complexity of organization has important implications for physiology and pathophysiology, particularly with respect to the development of myelinated fibers.

A note on the mechanism of resistance to anoxia and ischaemia in pathophysiological mammalian myelinated nerve

Computer simulation of the action potential in myelinated nerve fibres show that the metabolic cost of conduction of an impulse is less than normal in a slightly depolarised fibre. This would account, at least in part, for the greater resistance to ischaemia and anoxia of nerves from diabetics and other pathophysiological conditions.

Sodium channels in the axolemma of normal and degenerating rabbit optic nerve

Section of a rabbit peripheral nerve leads to axonal degeneration and a proliferation of Schwann cells, and it is known to lead to a profound increase in the saxitoxin binding capacity of its distal portion, suggesting that Schwann cells may bind this marker for sodium channels. The present study shows, however, that crush with subsequent axonal degeneration of the central axons of the rabbit optic nerve leads to a slow monotonic fall in the saxitoxin binding capacity, which by 100 days after crush is not significantly different from zero. This suggests that central glial cells (astrocytes and oligodendrocytes) do not bind saxitoxin, and that the saturable binding of saxitoxin to this nerve is entirely to the axolemma. On this basis, the value for total saxitoxin binding capacity of the normal rabbit optic nerve, taken together with the morphometric data of D. I. Vaney & A. Hughes (J. comp. Neurol. 80, 241-252 (1976)), yields a sodium channel density of about 400-700 channels per square micrometre nodal axolemma.

Freeze-fracture ultrastructure of the perinodal astrocyte and associated glial junctions

Freeze-fracture examination of nodes of Ranvier from adult rat optic nerve demonstrates the presence of astrocytic processes at the majority of nodes of Ranvier. Astrocytic processes often run along the entire length of the nodal gap, although they do not necessarily encircle the entire nodal circumference. The E- and P-fracture faces and the cross-fractured cytoplasm of these astrocytes (termed 'perinodal astrocytes') were examined. The cytoplasm of perinodal astrocytes contains 10-nm filaments. The P-faces of perinodal astrocytic membranes are characterized by orthogonal arrays of intramembranous particles ('assemblies'), with a center-to-center periodicity of approximately equal to 6 nm. Complementary orthogonally arranged pits are observed on the E-faces of the astrocytic membranes. The density of these arrays in perinodal astrocytic membranes is similar to that in parenchymal astrocytic membranes, but is substantially lower than that at pericapillary astrocytic membranes. In addition, gap junctions are present between astrocytes, and between astrocytes and paranodal oligodendroglial layers. These findings indicate that astrocytic processes comprise an important structural component of central nodes of Ranvier, and provide a morphological basis for a possible astrocytic role in nodal function.

Current-dependent inactivation induced by sodium depletion in normal and batrachotoxin-treated frog node of Ranvier

In batrachotoxin (BTX)-treated frog node of Ranvier, in spite of a marked reduction in Na inactivation, the Na current still presents a time- and voltage-dependent inactivation that could induce a 50-60% decrease in the current. The inactivation was found to be modified by changing the amplitude of a conditioning pulse, adding tetrodotoxin in the external solution, or replacing NaCl with KCl in the external solution. Conditioning pulses were able to alter the reversal potential of the BTX-modified Na current (Vrev). Vrev was shifted toward negative values for inward conditioning currents and was shifted toward positive values for outward conditioning currents. The change in Vrev was proportional to the conditioning current amplitude. Large inward currents induced 15-25 mV shifts of Vrev. During a 10-20-ms depolarizing pulse, the inactivation and change in Vrev were proportional to the time integral of the current. For longer depolarizations, Vrev reached a steady state level proportional to the current amplitude. The conductance, as calculated from the current and the actual Vrev, showed an inactivation proportional to exp(Vrev F/RT). These observations suggest that the BTX-modified Na current induces a decrease in local Na concentrations, which results in an alteration of the driving force and the conductance. During a pulse that induced a large inward current, the Na space concentration [( Na]s) changed from 114 to 50-60 mM. In normal fibers, the reversal potential of Na current was also shifted toward negative values by a prepulse that induced a large inward current. The change in Vrev reached 5-15 mV, which corresponded to a decrease in [Na]s of 20-50 mM. This change in Vrev slightly altered the time course of Na current. On the basis of a three-compartment model (axoplasm-perinodal space-bulk solution), a Na permeability of the barrier between the space and the bulk solution (PNa,s) and a mean thickness of the space (theta) were calculated. The mean value of PNa,s was 0.0051 cm X s-1 in both normal and BTX-treated fibers, whereas the value of theta was 0.29 micron in BTX-treated fibers and 0.05 micron in normal fibers. When compared with the values calculated during K accumulation, PNa,s was 10 times smaller than PK,s and theta Na-BTX was equal to theta K.(ABSTRACT TRUNCATED AT 400 WORDS)

Membrane specialization and axo-glial association in the rat retinal nerve fibre layer: freeze-fracture observations

The ultrastructure of non-myelinated ganglion cell axolemma within the retinal nerve fibre layer of adult rats was examined by thin section and freeze-fracture electron microscopy. Most of the axolemma within the nerve fibre layer does not exhibit any membrane specializations; intramembranous particles are partitioned with a density of approximately 1750 microns-2 on the P-fracture face and approximately 225 microns-2 on the E-face of the non-specialized axolemma. The nerve fibres also exhibit specialized foci of axolemma, at which the axons are abutted by the tips of blunt, radially oriented processes from Müller cells. At such sites of axo-glial association, an electron-dense undercoating is present beneath the axon membrane. Freeze-fracture analysis revealed a substantial increase in the density of E-face particles (greater than 500 microns-2) at sites of association between the tips of blunt glial processes and the axon. These findings demonstrate that non-myelinated axolemma of the retinal nerve fibre layer can exhibit spatial heterogeneity, with patches of node-like membrane at regions of specialized association with glial cell processes. On the basis of their morphological similarity to nodes of Ranvier, we suggest that these specialized axon regions represent foci of inward ionic current.

On the physiological role of internodal potassium channels and the security of conduction in myelinated nerve fibres

A theoretical analysis of the passive electrical properties of normal myelinated nerve suggests that the function of the voltage-dependent potassium channels in the internodal axolemma under the myelin sheath is to permit the generation of an internodal resting potential. Calculation shows that if this internodal potential were not present, the nodal potential would be reduced (by electrotonic short-circuiting) thus impairing the security of conduction. This impairment is particularly pronounced with smaller diameter fibres.

Electron microscopic serial section analysis of nodes of Ranvier in lumbosacral spinal roots of the cat: ultrastructural organization of nodal compartments in fibres of different sizes

The general ultrastructural organization of nodes of Ranvier in peripheral nerve fibres from 2 to 20 microns in diameter (D) was investigated in the adult cat using serially sectioned ventral and dorsal spinal roots. The study was performed in order to collect and systematize information considered necessary for a morphometric analysis of the node of Ranvier. In all cases a node of Ranvier could be divided into a central nodal axon segment and a surrounding nodal Schwann cell compartment. The latter included a nodal gap matrix substance, more or less overlapping nodal Schwann cell collars and, as a rule, also a Schwann cell brush-border emanating from the nodal Schwann cell collars and occupying the nodal gap. The relative size and the organization level of the nodal Schwann cell compartment increased with increasing fibre size up to a fibre diameter of 8-10 microns. At this fibre size the nodal gap was of a fairly even height (1 micron) all around the nodal axon and contained a thick brush-border of densely packed, more or less radially arranged Schwann cell microvilli. In very small fibres (D less than 3 microns) the nodal gap was low (less than 0.1 microns) and contained no or few microvilli. In fibres greater than 10 microns in diameter the relative size and the degree of structural order of the nodal Schwann cell compartment decreased with increasing fibre size. Drastic sectorial variations in nodal gap height and local thinning-out of the brush-border became prominent features in the largest fibres. The possible in vivo organization of the nodal Schwann cell compartment is discussed. Preliminary calculations indicate that the extracellular space directly surrounding the nodal axon might be quite small and that the area open for free communication between this extracellular space and the endoneurial space might be very much restricted, measuring as little as 2% of the area of the nodal axolemma. Algorithms for calculating various nodal structural parameters are discussed.