Ultrastructure and permeability of the Schwann cell layer surrounding the giant axon of the squid

Axonal morphological changes following impulse activity in mouse peripheral nerve in vivo: the return pathway for sodium ions

KEY POINTS

Conduction in myelinated axons involves substantial ion movements that must be reversed to restore homeostasis. The pathway taken by sodium ions returning to their original location and the potential osmotic consequences are currently unknown. We report striking morphological changes in axons following sustained impulse conduction that appear to result from osmosis and to indicate accumulation of ions in the periaxonal space followed by their release at the paranode. We conclude that the morphological changes illustrate a hitherto unrecognized part of normal axonal physiology that may also indicate the return pathway for the sodium ions involved in impulse formation.

ABSTRACT

Myelinated axons can conduct sustained trains of impulses at high frequency, but this involves substantial ion movements that must be reversed to restore homeostasis. Little attention has been paid to the potential osmotic consequences of the ion movements or to the pathway taken by sodium ions returning to their original endoneurial location, given that the axolemmal Na(+)-K(+)-ATPase extrudes these ions into the periaxonal space beneath the myelin rather than into the endoneurium. Serial confocal imaging of fluorescent axons conducting at sustained physiological frequencies in vivo has revealed surprising morphological changes that may illuminate these problems. Saphenous nerves and spinal roots of anaesthetized transgenic mice expressing axoplasmic yellow fluorescent protein were stimulated electrically or pharmacologically (veratridine). Within 2 h, the axon herniated on one or both sides of the nodal membrane, displacing the paranodal myelin and widening the nodal gap. The herniated axoplasm became directed back towards the internode, forming a 'cap' up to 30 μm long. Concurrently, the fluid in the expanded periaxonal space accumulated into droplets that appeared to travel to the paranode, where they escaped. No such alterations occurred in axons treated with sodium channel or Na(+)-K(+)-ATPase inhibitors. Remarkably, impulse conduction continued throughout, and all these changes reversed spontaneously over hours or days. The morphological changes were verified ultrastructurally, and occurred in virtually all myelinated axons. The findings appear to reveal an overlooked part of the physiological repertoire of nerve fibres, and here they are interpreted in terms of osmotic changes that may illuminate the pathway by which sodium ions return to the endoneurial space after they have entered the axon during impulse conduction.

Ion channels in key marine invertebrates; their diversity and potential for applications in biotechnology

Of the intra-membrane proteins, the class that comprises voltage and ligand-gated ion channels represents the major substrate whereby signals pass between and within cells in all organisms. It has been presumed that vertebrate and particularly mammalian ion channels represent the apex of evolutionary complexity and diversity and much effort has been focused on understanding their function. However, the recent availability of cheap high throughput genome sequencing has massively broadened and deepened the quality of information across phylogeny and is radically changing this view. Here we review current knowledge on such channels in key marine invertebrates where physiological evidence is backed up by molecular sequences and expression/functional studies. As marine invertebrates represent a much greater range of phyla than terrestrial vertebrates and invertebrates together, we argue that these animals represent a highly divergent, though relatively underused source of channel novelty. As ion channels are exquisitely selective sensors for voltage and ligands, their potential and actual applications in biotechnology are manifold.

Myelin sheaths are formed with proteins that originated in vertebrate lineages

All vertebrate nervous systems, except those of agnathans, make extensive use of the myelinated fiber, a structure formed by coordinated interplay between neuronal axons and glial cells. Myelinated fibers, by enhancing the speed and efficiency of nerve cell communication allowed gnathostomes to evolve extensively, forming a broad range of diverse lifestyles in most habitable environments. The axon-covering myelin sheaths are structurally and biochemically novel as they contain high portions of lipid and a few prominent low molecular weight proteins often considered unique to myelin. Here we searched genome and EST databases to identify orthologs and paralogs of the following myelin-related proteins: (1) myelin basic protein (MBP), (2) myelin protein zero (MPZ, formerly P0), (3) proteolipid protein (PLP1, formerly PLP), (4) peripheral myelin protein-2 (PMP2, formerly P2), (5) peripheral myelin protein-22 (PMP22) and (6) stathmin-1 (STMN1). Although widely distributed in gnathostome/vertebrate genomes, neither MBP nor MPZ are present in any of nine invertebrate genomes examined. PLP1, which replaced MPZ in tetrapod CNS myelin sheaths, includes a novel 'tetrapod-specific' exon (see also Möbius et al., 2009). Like PLP1, PMP2 first appears in tetrapods and like PLP1 its origins can be traced to invertebrate paralogs. PMP22, with origins in agnathans, and STMN1 with origins in protostomes, existed well before the evolution of gnathostomes. The coordinated appearance of MBP and MPZ with myelin sheaths and of PLP1 with tetrapod CNS myelin suggests interdependence - new proteins giving rise to novel vertebrate structures.

Diffusion in brain extracellular space

Diffusion in the extracellular space (ECS) of the brain is constrained by the volume fraction and the tortuosity and a modified diffusion equation represents the transport behavior of many molecules in the brain. Deviations from the equation reveal loss of molecules across the blood-brain barrier, through cellular uptake, binding, or other mechanisms. Early diffusion measurements used radiolabeled sucrose and other tracers. Presently, the real-time iontophoresis (RTI) method is employed for small ions and the integrative optical imaging (IOI) method for fluorescent macromolecules, including dextrans or proteins. Theoretical models and simulations of the ECS have explored the influence of ECS geometry, effects of dead-space microdomains, extracellular matrix, and interaction of macromolecules with ECS channels. Extensive experimental studies with the RTI method employing the cation tetramethylammonium (TMA) in normal brain tissue show that the volume fraction of the ECS typically is approximately 20% and the tortuosity is approximately 1.6 (i.e., free diffusion coefficient of TMA is reduced by 2.6), although there are regional variations. These parameters change during development and aging. Diffusion properties have been characterized in several interventions, including brain stimulation, osmotic challenge, and knockout of extracellular matrix components. Measurements have also been made during ischemia, in models of Alzheimer's and Parkinson's diseases, and in human gliomas. Overall, these studies improve our conception of ECS structure and the roles of glia and extracellular matrix in modulating the ECS microenvironment. Knowledge of ECS diffusion properties is valuable in contexts ranging from understanding extrasynaptic volume transmission to the development of paradigms for drug delivery to the brain.

Activity-dependent change in morphology of the glial tubular lattice of the crayfish medial giant nerve fiber

An evaluation of electron micrographs of stimulated nerve fibers used to investigate the effect of action potential generation on the structure-function relationship between axons and its associated glial cells revealed that what was at first thought to be stimulation-induced damage to the glia was, in fact, limited to volume expansion and disaggregation of the glial tubular lattice. All other structures appeared well preserved and otherwise normal. Using a 4-point subjective scale for evaluation by two investigators, 50-Hz stimulation for 2 min was observed to cause a volume expansion and disaggregation of the tubular lattice. Quantitatively, the internal diameter of the stimulated tubular lattice increased 65% above the unstimulated control (50.96 +/- 2.09 nm and 30.81 +/- 0.87 nm, respectively, P < or = 0.001). Stimulation had its greatest effect on tubular lattice volume and organization in the adaxonal glial layer and a decreasing effect as distance from the giant axon increased. These effects are reversible since the tubular lattice diameter and degree of disaggregation preserved 10 min after the cessation of stimulation were not found to be different from their unstimulated paired controls. Axons injected with TEA, a voltage-gated potassium channel blocker, prevented stimulation-induced volume expansion and disaggregation of tubular lattice structure. These results are consistent with an active uptake of K+ with obligated water or, alternatively, hyperosmotic K+ uptake and a fixation-induced increase in water permeation. Either mechanism of K+ uptake would result in tubular lattice volume expansion and disaggregation and suggests that the tubular lattice serves a larger role than a simple trans-glial diffusion pathway.

Ionic currents in isolated and in situ squid Schwann cells

Ionic currents from Schwann cells isolated enzymatically from the giant axons of the squids Loligo forbesi, Loligo vulgaris and Loligo bleekeri were compared with those obtained in situ. Macroscopic and single channel ionic currents were recorded using whole-cell voltage and patch clamp. In the whole-cell configuration, depolarisation from negative holding potentials evoked two voltage-dependent currents, an inward current and a delayed outward current. The outward current resembled an outwardly rectifying K+ current and was activated at -40 mV after a latent period of 5-20 ms following a step depolarisation. The current was reduced by externally applied nifedipine, Co2+ or quinine, was not blocked by addition of apamin or charibdotoxin and was insensitive to externally applied L-glutamate or acetylcholine. The voltage-gated inward current was activated at -40 mV and was identified as an L-type calcium current sensitive to externally applied nifedipine. Schwann cells were impaled in situ in split-open axons and voltage clamped using discontinuous single electrode voltage clamp. Voltage dependent outward currents were recorded that were kinetically identical to those seen in isolated cells and that had similar current-voltage relations. Single channel currents were recorded from excised inside-out patches. A single channel type was observed with a reversal potential close to the equilibrium potential for K+ (E(K)) and was therefore identified as a K+ channel. The channel conductance was 43.6 pS when both internal and external solutions contained 150 mM K+. Activity was weakly dependent on membrane voltage but sensitive to the internal Ca2+ concentration. Activity was insensitive to externally or internally applied L-glutamate or acetylcholine. The results suggest that calcium channels and calcium-activated K+ channels play an important role in the generation of the squid Schwann cell membrane potential, which may be controlled by the resting intracellular Ca2+ level.

Excitability of the squid giant axon revisited

The electrical properties of the giant axon from the common squid Loligo pealei have been reexamined. The primary motivation for this work was the observation that the refractoriness of the axon was significantly greater than the predictions of the standard model of nerve excitability. In particular, the axon fired only once in response to a sustained, suprathreshold stimulus. Similarly, only a single action potential was observed in response to the first pulse of a train of 1-ms duration current pulses, when the pulses were separated in time by approximately 10 ms. The axon was refractory to all subsequent pulses in the train. The underlying mechanisms for these results concern both the sodium and potassium ion currents INa and IK. Specifically, Na+ channel activation has long been known to be coupled to inactivation during a depolarizing voltage-clamp step. This feature appears to be required to simulate the pulse train results in a revised model of nerve excitability. Moreover, the activation curve for IK has a significantly steeper voltage dependence, especially near its threshold (approximately -60 mV), than in the standard model, which contributes to reduced excitability, and the fully activated current-voltage relation for IK has a nonlinear, rather than a linear, dependence on driving force. An additional aspect of the revised model is accumulation/depeletion of K+ in the space between the axon and the glial cells surrounding the axon, which is significant even during a single action potential and which can account for the 15-20 mV difference between the potassium equilibrium potential EK and the maximum afterhyperpolarization of the action potential. The modifications in IK can also account for the shape of voltage changes near the foot of the action potential.

Endocytotic formation of vesicles and other membranous structures induced by Ca2+ and axolemmal injury

Vesicles and/or other membranous structures that form after axolemmal damage have recently been shown to repair (seal) the axolemma of various nerve axons. To determine the origin of such membranous structures, (1) we internally dialyzed isolated intact squid giant axons (GAs) and showed that elevation of intracellular Ca2+ >100 microM produced membranous structures similar to those in axons transected in Ca2+-containing physiological saline; (2) we exposed GA axoplasm to Ca2+-containing salines and observed that membranous structures did not form after removing the axolemma and glial sheath but did form in severed GAs after >99% of their axoplasm was removed by internal perfusion; (3) we examined transected GAs and crayfish medial giant axons (MGAs) with time-lapse confocal fluorescence microscopy and showed that many injury-induced vesicles formed by endocytosis of the axolemma; (4) we examined the cut ends of GAs and MGAs with electron microscopy and showed that most membranous structures were single-walled at short (5-15 min) post-transection times, whereas more were double- and multi-walled and of probable glial origin after longer (30-150 min) post-transection times; and (5) we examined differential interference contrast and confocal images and showed that large and small lesions evoked similar injury responses in which barriers to dye diffusion formed amid an accumulation of vesicles and other membranous structures. These and other data suggest that Ca2+ inflow at large or small axolemmal lesions induces various membranous structures (including endocytotic vesicles) of glial or axonal origin to form, accumulate, and interact with each other, preformed vesicles, and/or the axolemma to repair the axolemmal damage.

Delaminating myelin membranes help seal the cut ends of severed earthworm giant axons

Transected axons are often assumed to seal by collapse and fusion of the axolemmal leaflets at their cut ends. Using photomicroscopy and electronmicroscopy of fixed tissues and differential interference contrast and confocal fluorescence imaging of living tissues, we examined the proximal and distal cut ends of the pseudomyelinated medial giant axon of the earthworm, Lumbricus terrestris, at 5-60 min post-transection in physiological salines and Ca2+-free salines. In physiological salines, the axolemmal leaflets at the cut ends do not completely collapse, much less fuse, for at least 60 min post-transection. In fact, the axolemma is disrupted for 20-100 microm from the cut end at 5-60 min post-transection. However, a barrier to dye diffusion is observed when hydrophilic or styryl dyes are placed in the bath at 15-30 min post-transection. At 30-60 min post-transection, this barrier to dye diffusion near the cut end is formed amid an accumulation of some single-layered and many multilayered vesicles and other membranous material, much of which resembles delaminated pseudomyelin of the glial sheath. In Ca2+-free salines, this single and multilayered membranous material does not accumulate, and a dye diffusion barrier is not observed. These and other data are consistent with the hypothesis that plasmalemmal damage in eukaryotic cells is repaired by Ca2+-induced vesicles arising from invaginations or evaginations of membranes of various origin which form junctional contacts or fuse with each other and/or the plasmalemma.

K+ accumulation and K+ conductance inactivation during action potential trains in giant axons of the squid Sepioteuthis

1. During action potential trains in giant axons from the squid Sepioteuthis, decline of the peak level of the undershoot potential was observed. The time course of the decline of the undershoot could be fitted with a three-exponential function with time constants of approximately 25, approximately 400 and approximately 7,000 ms, respectively. 2. When the osmolarity of the external solution was doubled by adding glucose (1.2 M), the fast component of undershoot decline, but not the medium and slow components, was significantly reduced. 3. Under voltage clamp in high osmolarity solutions where K+ accumulation was completely removed, repeated depolarizing pulses at 40 Hz (designed to mimic a train of action potentials) elicited K+ currents whose peak value declined. The decline is consistent with inactivation of the K+ conductance (gK). The decline of gK was fitted by a two-exponential function with time constants of approximately 400 and approximately 7,000 ms, respectively. 4. Interventions designed to modify Schwann cell physiology, such as high frequency stimulation (100 Hz, 2 min), externally applied ouabain (100-500 microM), L-glutamate (100 microM), ACh (100 microM), Co2+ (5mM), Ba2+ (2mM), or removal of external Ca2+ by EGTA, had no significant effects on the fast, medium or slow components of undershoot decline. 5. The results suggest that the fast component of undershoot decline represents K+ accumulation in the space between Schwann cell and axolemma. The medium and slow components are the result of axonal gK inactivation. Schwann cells appear to be involved in K+ clearance only to the extent that they provide an efficient physical pathway for the clearance of K+ by extracellular diffusion.

Coupling between giant axon Schwann cells in the squid

The nature of dye and electrical coupling between Schwann cells from the the squid giant axon, determined with microelectrodes, is described. Dye coupling (sensitive to dissection in sea water containing Ca 2+ ) and electrical coupling exists between Schwann cells. The electrical length constant of the Schwann-cell sheath is 25 µm and 100 µm along the axon circumference and long axis respectively. Schwann-cell membrane resistance is ~ 500 Ω cm 2 (corrected for coupling between cells). The coupling ratio between cells is 1:0.3, and is reduced by 2 mm octanol (1:0.03) and increased by 2 mm Ba 2+ (1:0.45). We conclude that as Schwann cells are weakly coupled and have a relatively low membrane resistance they are unlikely to be involved in the spatial buffering of axonally released K + .

Glia-to-axon communication: enrichment of glial proteins transferred to the squid giant axon

The transfer of newly synthesized proteins from the glial sheath into the axon is a well-documented process for the squid giant axon. In this study, we used a novel approach to separate the transferred glial proteins (TGPs) from the endogenous axoplasmic proteins of the squid giant axon. Axoplasm, containing radiolabelled TGPs, was extruded as a cylinder and immersed in an intracellular buffer. After 1-30 min, the TGPs were enriched in the intracellular buffer, because they were eluted from the axoplasm into the intracellular buffer much faster than the endogenous axoplasmic proteins. Most of the TGPs enriched in the intracellular buffer did not pellet when centrifuged at 24,000 g for 20 min and were susceptible to protease digestion without the addition of Triton X-100. Additionally, transmission electron microscopic autoradiography of intact axons, containing radiolabelled TGPs, suggested that most TGPs were not associated with vesicular organelles within the axon. We conclude that most of the TGPs are not contained within vesicles in the axoplasm of the squid giant axon, as would be expected if the mechanism of glia-to-axon transfer were conventional exocytosis-endocytosis or microphagocytosis.