Resealing of the proximal and distal cut ends of transected axons: Electrophysiological and ultrastructural analysis

The fates of the proximal and distal segments of transected axons differ. Whereas the proximal segment usually recovers from injury and regenerates, the distal segment degenerates. In the present report we studied the kinetics of the recovery processes of both proximal and distal axonal segment following axotomy and its temporal relations to the alterations in the cytoarchitecture of the injured neuron. The experiments were performed on primary cultured metacerebral neurons (MCn) isolated from Aplysia. We transected axons while monitoring the changes in transmembrane potential and input resistance (Rn) by inserting intracellular microelectrodes into the soma and axon. Correlation between the electrophysiological status of the injured axon and its ultrastructure was provided by rapid fixation of the neuron at selected times postaxotomy. Axotomy leads to membrane depolarization from a mean of ?55.7 S.D. 12.8 mV to ?12.7 S.D. 3.3 mV and decreased Rn from tens of MΩ to 1–3 MΩ. The transected axons remained depolarized for a period of 10–260 s for as long as the axoplasm was in direct contact with the bathing solution. Rapid repolarization and partial recovery of Rn was associated with the formation of a membrane seal over the cut ends by the constriction and subsequent fusion of the axolema. Prior to the formation of a membraneous barrier, electron-dense deposits aggregate at the tip of the cut axon and appear to form an axoplasmic “plug.” Electrophysiological analysis revealed that this “plug” does not provide resistance for current flow and that the axoplasmic resistance is homogenously distributed. The kinetics of injury and recovery processes as well as the ultrastructural changes of the proximal and distal segments are cannot be attributed to differences in the immediated response of the segments to axotomy. © 1993 John Wiley & Sons, Inc.     

Barrier permeability at cut axonal ends progressively decreases until an ionic seal is formed

After axonal severance, a barrier forms at the cut ends to rapidly restrict bulk inflow and outflow. In severed crayfish axons we used the exclusion of hydrophilic, fluorescent dye molecules of different sizes (0.6-70 kDa) and the temporal decline of ionic injury current to levels in intact axons to determine the time course (0-120 min posttransection) of barrier formation and the posttransection time at which an axolemmal ionic seal had formed, as confirmed by the recovery of resting and action potentials. Confocal images showed that the posttransection time of dye exclusion was inversely related to dye molecular size. A barrier to the smallest dye molecule formed more rapidly (<60 min) than did the barrier to ionic entry (>60 min). These data show that axolemmal sealing lacks abrupt, large changes in barrier permeability that would be expected if a seal were to form suddenly, as previously assumed. Rather, these data suggest that a barrier forms gradually and slowly by restricting the movement of molecules of progressively smaller size amid injury-induced vesicles that accumulate, interact, and form junctional complexes with each other and the axolemma at the cut end. This process eventually culminates in an axolemmal ionic seal, and is not complete until ionic injury current returns to baseline levels measured in an undamaged axon.     

Injury-induced vesiculation and membrane redistribution in squid giant axon

Injury of isolated squid giant axons in sea water by cutting or stretching initiates the following unreported processes: (i) vesiculation in the subaxolemmal region extending along the axon several mm from the site of injury, followed by (ii) vesicular fusions that result in the formation of large vesicles (20-50 micron diameter), 'axosomes', and finally (iii) axosomal migration to and accumulation at the injury site. Some axosomes emerge from a cut end, attaining sizes up to 250 microns in diameter. Axosomes did not form after axonal injury unless divalent cations (Ca2+ or Mg2+) were present (10mM) in the external solution. The requirement for Ca2+ and the action of other ions are similar to that for cut-end cytoskeletal constriction in transected squid axons (Gallant, P.E. (1988) J. Neurosci. 8, 1479-1484) and for electrical sealing in transected axons of the cockroach (Yawo, H. and Kuno, M. (1985) J. Neurosci. 5, 1626-1632). Axosomes probably consist of membrane from different sources (e.g., axolemma, organelles and Schwann cells); however, localization of axosomal formation to the inner region of the axolemma and the formation dependence on divalent cations suggest principal involvement of cisternae of endoplasmic reticulum. Patch clamp of excised patches from axosomes liberated spontaneously from cut ends of transected axons showed a 12-pS K+ channel and gave indications of other channel types. Injury-induced vesiculation and membrane redistribution seem to be fundamental processes in the short-term (minutes to hours) that precede axonal degeneration or repair and regeneration. Axosomal formation provides a membrane preparation for the study of ion channels and other membrane processes from inaccessible organelles.     

Regeneration restores some of the altered electrical properties of axotomized bullfrog B-cells

In bullfrog B-type sympathetic neurones axon injury produces substantial changes in somal membrane properties. These include a shortening of action potential afterhyperpolarization (AHP) and an increase in action potential (AP) duration. In the present experiments we compared two injury situations: nerve crush, which was followed by regeneration, and nerve cut, after which regeneration to the original target was prevented, to investigate whether these electrophysiological changes were related to axon regeneration. Both crush and cut injuries produced a similar maximum decrease in AHP duration (to 33 and 30%) by 14 days after axotomy. After nerve crush, AHP duration recovered to within control values by 42 days, while after cut it remained depressed. AHP amplitude decreased to the same extent after nerve crush or cut (to 62 and 58%), but the rate of decrease was slower following crush when compared with cut, and following both types of injury it still remained depressed at 42 and 49 days. Changes in AP duration also took longer to occur following nerve crush, reaching maximal values at 35-42 days, at which time AHP duration had returned to within the normal range. The early reduction in AHP duration and its rapid recovery in regenerating neurones suggests that the current underlying this membrane property is regulated by events associated with axon outgrowth and peripheral reconnection. In contrast, changes in AHP amplitude and AP repolarization appeared to be independent of the occurrence of axon regeneration and remained abnormal at 49 days despite the recovery of AHP duration. These results imply that the electrophysiological changes seen in B-cells following injury are differentially regulated during subsequent regeneration.     

Computer simulation of the effect of the nodal gap resistance on ionic current measurements in the Ranvier node membrane.

Results are presented of a computer simulation of the effect of the irreducible resistance introduced by the nodal gap, in series with the impedance of the axon membrane. A clamp potential is applied to a structure modeled as an electric circuit composed of a resistance in series with the membrane impedance, and modified nerve equations describing membrane currents are solved to predict the effect of nodal series resistance on these currents. These studies reveal changes in the absolute values and kinetics of the ionic currents (errors greater than 10-20%) for selected values of series resistance.     

Voltage-dependent block of the cystic fibrosis transmembrane conductance regulator Cl- channel by two closely related arylaminobenzoates

The gene defective in cystic fibrosis encodes a Cl- channel, the cystic fibrosis transmembrane conductance regulator (CFTR). CFTR is blocked by diphenylamine-2-carboxylate (DPC) when applied extracellularly at millimolar concentrations. We studied the block of CFTR expressed in Xenopus oocytes by DPC or by a closely related molecule, flufenamic acid (FFA). Block of whole-cell CFTR currents by bath-applied DPC or by FFA, both at 200 microM, requires several minutes to reach full effect. Blockade is voltage dependent, suggesting open-channel block: currents at positive potentials are not affected but currents at negative potentials are reduced. The binding site for both drugs senses approximately 40% of the electric field across the membrane, measured from the inside. In single-channel recordings from excised patches without blockers, the conductance was 8.0 +/- 0.4 pS in symmetric 150 mM Cl-. A subconductance state, measuring approximately 60% of the main conductance, was often observed. Bursts to the full open state lasting up to tens of seconds were uninterrupted at depolarizing membrane voltages. At hyperpolarizing voltages, bursts were interrupted by brief closures. Either DPC or FFA (50 microM) applied to the cytoplasmic or extracellular face of the channel led to an increase in flicker at Vm = -100 mV and not at Vm = +100 mV, in agreement with whole-cell experiments. DPC induced a higher frequency of flickers from the cytoplasmic side than the extracellular side. FFA produced longer closures than DPC; the FFA closed time was roughly equal (approximately 1.2 ms) at -100 mV with application from either side. In cell-attached patch recordings with DPC or FFA applied to the bath, there was flickery block at Vm = -100 mV, confirming that the drugs permeate through the membrane to reach the binding site. The data are consistent with the presence of a single binding site for both drugs, reached from either end of the channel. Open-channel block by DPC or FFA may offer tools for use with site-directed mutagenesis to describe the permeation pathway.     

Properties of internally perfused, voltage-clamped, isolated nerve cell bodies

The membrane properties of isolated neurons from Helix aspersa were examined by using a new suction pipette method. The method combines internal perfusion with voltage clamp of nerve cell bodies separated from their axons. Pretreatment with enzymes such as trypsin that alter membrane function is not required. A platinized platinum wire which ruptures the soma membrane allows low resistance access directly to the cell's interior improving the time resolution under voltage clamp by two orders of magnitude. The shunt resistance of the suction pipette was 10-50 times the neuronal membrane resistance, and the series resistance of the system, which was largely due to the tip diameter, was about 10(5) omega. However, the peak clamp currents were only about 20 nA for a 60-mV voltage step so that measurements of membrane voltage were accurate to within at least 3%. Spatial control of voltage was achieved only after somal separation, and nerve cell bodies isolated in this way do not generate all-or-none action potentials. Measurements of membrane potential, membrane resistance, and membrane time constant are equivalent to those obtained using intracellular micropipettes, the customary method. With the axon attached, comparable all-or-none action potentials were also measured by either method. Complete exchange of Cs+ for K+ was accomplished by internal perfusion and allowed K+ currents to be blocked. Na+ currents could then be blocked by TTX or suppressed by Tris-substituted snail Ringer solution. Ca2+ currents could be blocked using Ni2+ and other divalent cations as well as organic Ca2+ blockers. The most favorable intracellular anion was aspartate-, and the sequence of favorability was inverted from that found in squid axon.     

Effects of cytosolic Ca2+ on membrane voltage and conductance of cultured mesangial cells from stroke-prone spontaneously hypertensive rats and WKY rats

Mesangial cells (MC) are considered to play an important role in the development of hypertension. The purpose of this study was to characterize the effects of cytosolic Ca2+ on membrane voltage and conductance of MC using stroke-prone spontaneously hypertensive rats (SHRSP) and Wistar Kyoto rats (WKY). We applied the patch-clamp technique in the whole-cell configuration to measure membrane potential (Vm) and ion currents. There was no significant difference in resting Vm values between MC from WKY and SHRSP. The cytosolic Ca2+ increase induced membrane depolarization and the increase of Cl- currents in MC from WKY but not in MC from SHRSP. On the other hand, the Ca2+ increase induced membrane hyperpolarization and the increase of K+ currents in MC from SHRSP but not in MC from WKY. Such differences between MC from two rat strains may play an important role in the alterations in renal hemodynamics observed in hypertension.     

4℃预处理对人中性粒细胞膜电流和极性的影响

对急性分离的人中性粒细胞采用4℃预处理是进行膜片钳实验前经常采取的步骤,但这一步骤对电生理记录结果有何影响尚无文献报道。本实验探讨这一步骤对电生理记录过程和实验结果的影响。结果显示,4℃预处理可以显著提高细胞的封接率,有利于对中性粒细胞进行电生理记录;封接率提高的原因与4℃预处理降低细胞的极性活动有关,但记录到的电压依赖性钾通道全细胞电流和大电导Ca^2＋依赖性K^＋单通道电流动力学没有显著的变化。这些结果表明,4℃预处理可能影响到细胞膜上与极性有关的脂膜变化,但对细胞膜上蛋白的功能影响较少。     

The Resting Potential of Mouse Leydig Cells: Role of an Electrogenic Na+/K+ Pump

Resting potentials (Vm) were measured in mouse Leydig cells, using the whole-cell patch-clamp technique. In contrast to conventional microelectrode measurements, where a biphasic potential was observed, we recorded a stable Vm around -32.2 +/- 1.2 mV (mean +/- SEM, n = 159), at 25 degrees C, and an input resistance larger than 2.7 x 109 W. Although Vm is sensitive to changes in the extracellular concentrations of potassium and chloride, the relationship between Vm and these ions' concentrations cannot be described by either the Goldman-Hodgkin-Katz or the Nernst equation. Perifusing cells with potassium-free solution or 10?3 M ouabain induced a marked depolarization averaging 20.1 +/- 3.2 mV (n = 9) and 23.1 +/- 2.8 mV, (n = 7), respectively. Removal of potassium or addition of ouabain with the cell voltage-clamped at its Vm, resulted in an inwardly directed current, due to inhibition of the Na+K+ATPase. The pump current increased with temperature with a Q10 coefficient of 2.3 and had an average value of -6.5 +/- 0.4 pA (n = 21) at 25 degrees C. Vm also varied strongly with temperature, reaching values as low as -9.2 +/- 1.2 mV (n = 22) at 15 degrees C. Taking the pump current at 25 degrees C and a minimum estimate for the membrane input resistance, we can see that the Na+K+ATPase could directly contribute with 17.7 mV to the Vm of Leydig cells, which is a major fraction of the ?32.2 +/- 1.2 mV (n = 159) observed.     

Currents recorded through small areas of squid axon membrane with an internal virtual ground voltage clamp.

A new voltage-clamp apparatus for the squid axon has been implemented to enable recording of currents through small areas of axon membrane. The performance of this clamp was tested by recording total sodium currents from perfused axons (I total) and sodium currents from small membrane patches (I patch), which were recorded from inside the axon with an L-shaped pipette. The I patch records, although four orders of magnitude smaller than I total, were stable and showed normal kinetics and voltage dependence, and appeared to reflect the activation of a small population of normal sodium channels. The size of the current recorded from the patch was mainly a function of the tip diameter of the L-shaped pipette and of the shunt resistance between inside the pipette and the axoplasm.     

Temperature effects on a slow-crustacean neuromuscular system

The membrane potential of the E2 axon and the bender muscle fibers increased with temperature. The input resistance of the axon, the spike amplitude and time course declined with temperature. Excitatory junctional potentials (ejps) exhibited maximum amplitudes and minimum facilitation at about the same temperature. Ejp time course and muscle membrane input resistance declined with temperature. Tension produced by the muscle also declined but then increased when additional spikes were generated in the periphery of the E2 axon.     

Modeling ion channels in the gigaseal

The ability to form gigaseals is essential for patch-clamp electrophysiology; however, ion channels located in the seal can produce measureable currents. To explore the expected properties of channels in the seal (i.e., rim channels), we created a mathematical model. The seal was a two-dimensional cable filled with saline and bounded on one side by membrane (with resistance and capacitance) and on the other side by glass (nonconductive and noncapacitive). We included ion depletion/accumulation around the channels. The channels were ohmic with a conductance that increased with the concentration of permeant ions. The aqueous seal thickness was set nominally to 1 nm. Imaging with fluorescent dyes in the pipette showed that the hydrophilic dye Alexa 488 is impermeant, but lipophilic FM1-43 labels the seal. The model showed that to obtain high-resistance seals, the conductivity of the seal media has to be <10% that of the bath. Stimulus voltages decreased with distance down the seal. In agreement with results in the literature, channels in the seal can produce currents similar to those in the pipette-spanning dome. The transition times of currents are slower due to membrane capacitance. If channel densities are uniform, patch currents are dominated by channels in the dome.     

A localized zone of increased conductance progresses over the surface of the sea urchin egg during fertilization

Although activation of a sea urchin egg by sperm leads to three phases of membrane conductance increase in the egg, the mechanism by which the sperm causes these conductance changes is not known. We used the loose patch clamp technique to localize the conductance changes in voltage clamped eggs. A patch of the egg's membrane was isolated from the bath by pressing the loose patch clamp pipette against the egg surface. Sperm added to the bath attached to the surface of the egg in a region other than at the isolated membrane patch. During phase 1 of the activation current, no changes of the membrane conductance were detected. At the time of, and subsequent to the onset of phase 2, large currents recorded between the interior of the patch pipette and the bath were attributed to changes of the seal resistance between the surface of the egg and the pipette. A local change of membrane conductance was observed during phase 2 despite the changes of seal resistance. During phase 2, the large amplitude and short duration of the local membrane conductance increase relative to the membrane, conductance increase for the whole egg during phase 2 indicated that the conductance increase occurred over the entire surface of the egg, but not simultaneously. The time when the peak conductance for the membrane patch occurred, relative to the time of onset for phase 2 in the whole egg, depended on the distance, measured in a straight line, between the site of sperm attachment and the tip of the pipette. These data indicate that the localized conductance increase progressed over the surface of the egg from the site of sperm attachment to the opposite pole of the egg. It is proposed that the local conductance increase, the cortical reaction, and the change of seal resistance are all evoked by a common cytoplasmic message that progresses throughout the cytoplasm of the egg from the site of sperm attachment to the opposite pole of the egg.     

Intracellular Ca dynamics in ventricular fibrillation

In the heart, membrane voltage (Vm) and intracellular Ca (Cai) are bidirectionally coupled, so that ionic membrane currents regulate Cai cycling and Cai affects ionic currents regulating action potential duration (APD). Although Cai reliably and consistently tracks Vm at normal heart rates, it is possible that at very rapid rates, sarcoplasmic reticulum Cai cycling may exhibit intrinsic dynamics. Non-voltage-gated Cai release might cause local alternations in APD and refractoriness that influence wavebreak during ventricular fibrillation (VF). In this study, we tested this hypothesis by examining the extent to which Cai is associated with Vm during VF. Cai transients were mapped optically in isolated arterially perfused swine right ventricles using the fluorescent dye rhod 2 AM while intracellular membrane potential was simultaneously recorded either locally with a microelectrode (5 preparations) or globally with the voltage-sensitive dye RH-237 (5 preparations). Mutual information (MI) is a quantitative statistical measure of the extent to which knowledge of one variable (Vm) predicts the value of a second variable (Cai). MI was high during pacing and ventricular tachycardia (VT; 1.13 +/- 0.21 and 1.69 +/- 0.18, respectively) but fell dramatically during VF (0.28 +/- 0.06, P < 0.001). Cai at sites 4-6 mm apart also showed decreased MI during VF (0.63 +/- 0.13) compared with pacing (1.59 +/- 0.34, P < 0.001) or VT (2.05 +/- 0.67, P < 0.001). Spatially, Cai waves usually bore no relationship to membrane depolarization waves during nonreentrant fractionated waves typical of VF, whereas they tracked each other closely during pacing and VT. The dominant frequencies of Vm and Cai signals analyzed by fast Fourier transform were similar during VT but differed significantly during VF. Cai is closely associated with Vm closely during pacing and VT but not during VF. These findings suggest that during VF, non-voltage-gated Cai release events occur and may influence wavebreak by altering Vm and APD locally.     

Transmembrane currents in frog olfactory cilia

Summary We have measured transmembrane currents in intact single cilia from frog olfactory receptor neurons. A single cilium on a neuron was sucked into a patch pipette, and a high-resistance seal was formed near the base of the cilium. Action potentials could be induced by applying suction or a voltage ramp to the ciliary membrane. A transient current was seen in some cells on stimulation with odorants. After excision from the cell, most of the cilia showed increased conductance in a bath containing cAMP, indicating that the cytoplasmic face of the ciliary membrane was accessible to the bath. The estimated resistance of a single cilium was surprisingly low.     

Microscopical and electrophysiological studies on the healing-over of striated fibers of cremaster muscle of the guinea pig

In previous works it has been shown that the striated fibers of the cremaster muscle undergo a calcium-dependent healing-over reaction after transection and that the fibers of the diaphragm under the same conditions do not recover. In the present work striated fibers of the cremaster and diaphragm are studied, using electrophysiological techniques, light and electron microscopy, 15, 30, 45 and 60 min after transection in an attempt to clarify the process leading to the recovery of the fibers of the cremaster muscle. The recording of membrane potentials at different times after the lesion in the immediate vicinity of the cut end demonstrates that the new diffusion barrier is formed at the damaged surface. Light microscopy of fibers of cremaster transected in vitro indicates the existence of a rapid process preventing the outflow of particulate constituents of the cytoplasm 1 min after the lesion. Electron microscopy shows that this hindrance is due to a compact disposition of filaments derived from altered myofibrils near the cut end. This filamentary plug does not exist in the diaphragm. Cell membrane closing is a slow phenomenon which is completed between 30 and 60 min after the lesion in different fibers. No reconstitution of the cell membrane was found in the fibers of the diaphragm. Rapid and slow responses are interpreted as particular cases of the surface precipitation reaction known in several cell types for more than 40 years.     

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 μm 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. © 1997 John Wiley & Sons, Inc. J Neurobiol 33: 945–960, 1997     

Alterations in striatal synaptic transmission are consistent across genetic mouse models of Huntington's disease

Since the identification of the gene responsible for HD (Huntington''s disease), many genetic mouse models have been generated. Each employs a unique approach for delivery of the mutated gene and has a different CAG repeat length and background strain. The resultant diversity in the genetic context and phenotypes of these models has led to extensive debate regarding the relevance of each model to the human disorder. Here, we compare and contrast the striatal synaptic phenotypes of two models of HD, namely the YAC128 mouse, which carries the full-length huntingtin gene on a yeast artificial chromosome, and the CAG140 KI (knock-in) mouse, which carries a human/mouse chimaeric gene that is expressed in the context of the mouse genome, with our previously published data obtained from the R6/2 mouse, which is transgenic for exon 1 mutant huntingtin. We show that striatal MSNs (medium-sized spiny neurons) in YAC128 and CAG140 KI mice have similar electrophysiological phenotypes to that of the R6/2 mouse. These include a progressive increase in membrane input resistance, a reduction in membrane capacitance, a lower frequency of spontaneous excitatory postsynaptic currents and a greater frequency of spontaneous inhibitory postsynaptic currents in a subpopulation of striatal neurons. Thus, despite differences in the context of the inserted gene between these three models of HD, the primary electrophysiological changes observed in striatal MSNs are consistent. The outcomes suggest that the changes are due to the expression of mutant huntingtin and such alterations can be extended to the human condition.     

Formation of microtubule-based traps controls the sorting and concentration of vesicles to restricted sites of regenerating neurons after axotomy

Transformation of a transected axonal tip into a growth cone (GC) is a critical step in the cascade leading to neuronal regeneration. Critical to the regrowth is the supply and concentration of vesicles at restricted sites along the cut axon. The mechanisms underlying these processes are largely unknown. Using online confocal imaging of transected, cultured Aplysia californica neurons, we report that axotomy leads to reorientation of the microtubule (MT) polarities and formation of two distinct MT-based vesicle traps at the cut axonal end. Approximately 100 microm proximal to the cut end, a selective trap for anterogradely transported vesicles is formed, which is the plus end trap. Distally, a minus end trap is formed that exclusively captures retrogradely transported vesicles. The concentration of anterogradely transported vesicles in the former trap optimizes the formation of a GC after axotomy.