Clay M. Armstrong

Currents Related to Movement of the Gating Particles of the Sodium Channels

“…IT seems difficult to escape the conclusion that the changes in ionic permeability depend on the movement of some component of the membrane which behaves as though it had a large charge or dipole moment”1. With these words Hodgkin and Huxley predicted the existence of gating currents: charge movement associated with molecular rearrangements that attend the opening and closing of the ionic channels in response to changes in the membrane field. The polarity of gating current of the sodium channels can be easily predicted: following a positive step change of membrane voltage, positively charged gating particles would move outward through the membrane field from closed to open position (or negatively charged particles would move inward), yielding an outward current. On repolarization after a voltage step that opened the channels, gating current would be inward, as particles moved from open to closed position. Hodgkin and Huxley were unable to observe gating currents experimentally, and concluded that the density of ionic channels in the membrane must be low. A later attempt by Chandler and Meves2 to detect such currents was also unsuccessful, and they estimated that there are less than 100 sodium channels μm−2, a prediction that has been borne out by later estimates of sodium channel density3,4. We report here that by use of signal averaging techniques, we have observed small transient currents which we believe are the gating currents of the sodium channels.

Ionic pores, gates, and gating currents

The current phase of axon physiology began with the invention of the voltage clamp by Cole (1949) and its use by Hodgkin & Huxley (1952 d ) to produce an astonishingly complete analysis of the ionic permeabilities that are responsible for the action potential. Their description did notcontain much in the way of molecular detail, and left open such questions as whether ions cross the membrane by way of pores or carriers, and the nature of the ‘gating‘ processes that increase ordecrease ion permeability in response to changes of the membrane potential. In the last few years our picture of the ionicchannels has grown considerably more tangible, though it still falls far short of a detailed molecular description. This article describes this sharpened picture and reviews the evidence for it. The viewpoint expressed is a very personal one, andno attempt has been made to review the literature of axonology comprehensively.

Voltage-Gated Ion Channels and Electrical Excitability

Our original research has been generously supported over many years by National Institutes of Health grants NS08174 and NS12547.

Synaptically triggered action potentials in dendrites.

We tested the hypothesis that action potentials originate in apical dendrites of pyramidal cells. Layer V somata were voltage clamped in thin slices of rat motor cortex. Fibers synapsing in unclamped regions far out on the apical dendrite caused small, slow synaptic currents, as recorded at the soma, and sometimes elicited complex, multicomponent current spikes, beginning with a small first spike. Hyperpolarization, or tetrodotoxin applied to basal dendrites and soma, blocked the later spike components without affecting the synaptic current and the first component, which was a synaptically triggered Na+ spike in the apical dendrite. Similar spikes followed voltage steps or direct stimulation. We conclude that Na+ action potentials are initiated in the apical dendrite in response to synaptic input.

Na channel inactivation from open and closed states

A sodium channel is composed of four similar domains, each containing a highly charged S4 helix that is driven outward (activates) in response to a depolarization. Functionally, the channel has two gates, called activation gate (a gate) and inactivation gate (I gate), both of which must be open for conduction to occur. The cytoplasmically located a gate opens after a depolarization has activated the S4s of (probably) all four domains. The I gate consists of a cytoplasmically located inactivation “particle” and a receptor for it in the channel. The receptor becomes available after some degree of S4 activation, and the particle diffuses in to inactivate the channel. The I gate usually closes when the a gate is open [open-state inactivation (Osi)] but also can close before the channel reaches the conducting state. This “closed-state inactivation” (Csi) is studied quantitatively in this paper to determine the degree of S4 activation required for (i) opening the a gate, and (ii) permitting the I gate to close. Csi is most prominent for small depolarizations, during which occupancy of the partially activated closed states is prolonged. Large depolarizations drive the S4s outward quickly, minimizing the duration of closed-state occupancy and making Csi small and Osi large. Based on these data and evidence in the literature, it is concluded that opening the a gate requires S4 activation in domains 1–3, with partial activation of the S4 of domain 4. Csi requires only S4 activation of domains 3 and 4, which does not open the a gate.

C-type inactivation of voltage-gated K+ channels: Pore constriction or dilation?

K+ channels have many timing and control functions throughout the body, especially in the nervous system and heart. These vital functions are made possible by several types of “gates” that govern ion flow through the channels ([Yellen, 1998][1]). KV channels (K+ selective, voltage activated),

Inositol trisphosphate and ryanodine receptors share a common functional Ca2+ pool in cerebellar Purkinje neurons

Changes in the intracellular free calcium concentration ([Ca2+]i) control many important processes in excitable and nonexcitable cells. In cerebellar Purkinje neurons, increases in [Ca2+]i modulate excitability by turning on calcium-activated potassium and chloride conductances, and modifying the synaptic efficacy of inhibitory and excitatory inputs to the cell. Calcium release from the intracellular stores plays an important role in the regulation of [Ca2+]i. Purkinje neurons contain both inositol trisphosphate (InsP3) and ryanodine (Ry) receptors. With the exception of the dendritic spines, where only InsP3 receptors are found, InsP3 and Ry receptors are present in the entire cell. The distribution of the two calcium release channels, however, is not uniform, and it has been suggested that InsP3 and Ry receptors use separate Ca2+ pools. The functional properties of InsP3 and Ry Ca2+ pools were investigated by flash photolysis and single-cell microspectrofluorimetry. It was found that depletion of ryanodine-sensitive Ca2+ stores renders InsP3 incapable of releasing more Ca2+ from the stores. Abolishing calcium-induced calcium release by blocking ryanodine receptors with ruthenium red did not have a significant effect on InsP3-evoked Ca2+ release. It is concluded that InsP3 receptors use the same functional Ca2+ pool as that utilized by Ry receptors in Purkinje neurons.

Dilated and Defunct K Channels in the Absence of K

Potassium ions are vital for maintaining functionality of K channels. In their absence, many K channel types enter a long-lasting defunct condition characterized by absence of conductance and drastic changes in gating current. We show that channels pass through a dilated condition with altered selectivity as they are becoming defunct. To characterize these abnormalities we examined gating and ionic currents generated by Shaker IR and by three nonconducting mutants, W434F, D447N, and Y445A, in 0 K+. On entering the dilated condition, Shaker IR becomes permeable to Na+ and tetramethylammonium-positive (TMA+), signaling deformation of the selectivity filter. When dilated, nearly normal closing is possible at -140 mV. At -80 mV, however, closing is very slow and channels stray from the dilated into the defunct condition. Restoration from defunct to dilated condition requires tens of seconds at 0 mV and can occur in the absence of K+. W434F and D447N are similar to Shaker IR, showing Na+ and TMA+ permeability when dilated. The defunct gating currents are similar in Shaker IR and these two mutants and are reminiscent of the early transitions of normal gating. Y445A does not become defunct and shows Na+ but not TMA+ permeability on K+ removal.

The Na/K pump, Cl ion, and osmotic stabilization of cells

An equation for membrane voltage is derived that takes into account the electrogenicity of the Na/K pump and is valid dynamically, as well as in the steady state. This equation is incorporated into a model for the osmotic stabilization of cells. The results emphasize the role of the pump and membrane voltage in lowering internal Cl− concentration, thus making osmotic room for vital substances that must be sequestered in the cell.

A Model for 4-Aminopyridine Action on K Channels: Similarities to Tetraethylammonium Ion Action

We present a model for the action of 4-aminopyridine (4AP) on K channels. The model is closely based on the gating current studies of the preceding paper and has been extended to account for ionic current data in the literature. We propose that 4AP, like tetraethylammonium ion and other quaternary ammonium ions, enters and leaves the channel only when the activation gate is open, a proposal that is strongly supported by the literature. Once in the open channel, 4APs major action is to bias the activation gate toward the closed conformation by approximately the energy of a hydrogen bond. S4 segment movement, as reflected in gating currents, is almost normal for a 4AP-occupied channel; only the final opening transition is affected. The model is qualitatively the same as the one used for many years to explain the action of quaternary ammonium ions.