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Low pH depolarizes the voltage-dependence of cardiac voltage-gated sodium (NaV1.5) channel activation and fast inactivation and destabilizes the fast-inactivated state. The molecular basis for these changes in protein behavior has not been reported. We hypothesized that changes in the kinetics of voltage sensor movement may destabilize the fast-inactivated state in NaV1.5. To test this idea, we recorded NaV1.5 gating currents in Xenopus oocytes using a cut-open voltage-clamp with extracellular solution titrated to either pH 7.4 or pH 6.0. Reducing extracellular pH significantly depolarized the voltage-dependence of both the QON/V and QOFF/V curves, and reduced the total charge immobilized during depolarization. We conclude that destabilized fast-inactivation and reduced charge immobilization in NaV1.5 at low pH are functionally related effects., (Copyright © 2013 Biophysical Society. Published by Elsevier Inc. All rights reserved.)

Low pH depolarizes the voltage dependence of voltage-gated sodium (Na(V)) channel activation and fast inactivation. A complete description of Na(V) channel proton modulation, however, has not been reported. The majority of Na(V) channel proton modulation studies have been completed in intact tissue. Additionally, several Na(V) channel isoforms are expressed in cardiac tissue. Characterizing the proton modulation of the cardiac Na(V) channel, Na(V)1.5, will thus help define its contribution to ischemic arrhythmogenesis, where extracellular pH drops from pH 7.4 to as low as pH 6.0 within ~10 min of its onset. We expressed the human variant of Na(V)1.5 with and without the modulating β(1) subunit in Xenopus oocytes. Lowering extracellular pH from 7.4 to 6.0 affected a range of biophysical gating properties heretofore unreported. Specifically, acidic pH destabilized the fast-inactivated and slow-inactivated states, and elevated persistent I(Na). These data were incorporated into a ventricular action potential model that displayed a reduced maximum rate of depolarization as well as disparate increases in epicardial, mid-myocardial, and endocardial action potential durations, indicative of an increased heterogeneity of repolarization. Portions of these data were previously reported in abstract form., (Copyright © 2011 Biophysical Society. Published by Elsevier Inc. All rights reserved.)

We investigated structural determinants of fast inactivation and deactivation in sodium channels by comparing ionic flux and charge movement in skeletal muscle channels, using mutations of DIII-DIV linker charges. Charge altering and substituting mutations at K-1317, K-1318 depolarized the g(V) curve but hyperpolarized the h(infinity) curve. Charge reversal and substitution at this locus reduced the apparent voltage sensitivity of open- and closed-state fast inactivation. These effects were not observed with charge reversal at E-1314, E-1315. Mutations swapping or neutralizing the negative cluster at 1314, 1315 and the positive cluster at 1317, 1318 indicated that local interactions dictate the coupling of activation to fast inactivation. Gating charge was immobilized before channel entry into fast inactivation in hNa(V)1.4 but to a lesser extent in mutations at K-1317, K-1318. These results suggest that charge is preferentially immobilized in channels inactivating from the open state. Recovery of gating charge proceeded with a single, fast phase in the double mutation K-1317R, K-1318R. This mutation also partially uncoupled recovery from deactivation. Our findings indicate that charged residues near the fast inactivation "particle" allosterically interact with voltage sensors to control aspects of gating in sodium channels.

Slow inactivation determines the availability of voltage-gated sodium channels during prolonged depolarization. Slow inactivation in hNa(V)1.4 channels occurs with a higher probability than hNa(V)1.5 sodium channels; however, the precise molecular mechanism for this difference remains unclear. Using the macropatch technique we show that the DII S5-S6 p-region uniquely confers the probability of slow inactivation from parental hNa(V)1.5 and hNa(V)1.4 channels into chimerical constructs expressed in Xenopus oocytes. Site-directed mutagenesis was used to test whether a specific region within DII S5-S6 controls the probability of slow inactivation. We found that substituting V754 in hNa(V)1.4 with isoleucine from the corresponding position (891) in hNa(V)1.5 produced steady-state slow inactivation statistically indistinguishable from that in wild-type hNa(V)1.5 channels, whereas other mutations have little or no effect on slow inactivation. This result indicates that residues V754 in hNa(V)1.4 and I891in hNa(V)1.5 are unique in determining the probability of slow inactivation characteristic of these isoforms. Exchanging S5-S6 linkers between hNa(V)1.4 and hNa(V)1.5 channels had no consistent effect on the voltage-dependent slow time inactivation constants [tau(V)]. This suggests that the molecular structures regulating rates of entry into and exit from the slow inactivated state are different from those controlling the steady-state probability and reside outside the p-regions.

Skeletal and heart muscle excitability is based upon the pool of available sodium channels as determined by both fast and slow inactivation. Slow inactivation in hH1 sodium channels significantly differs from slow inactivation in hSkM1. The beta(1)-subunit modulates fast inactivation in human skeletal sodium channels (hSkM1) but has little effect on fast inactivation in human cardiac sodium channels (hH1). The role of the beta(1)-subunit in sodium channel slow inactivation is still unknown. We used the macropatch technique on Xenopus oocytes to study hSkM1 and hH1 slow inactivation with and without beta(1)-subunit coexpression. Our results indicate that the beta(1)-subunit is partly responsible for differences in steady-state slow inactivation between hSkM1 and hH1 channels. We also studied a sodium channel chimera, in which P-loops from each domain in hSkM1 sodium channels were replaced with corresponding regions from hH1. Our results show that these chimeras exhibit hH1-like properties of steady-state slow inactivation. These data suggest that P-loops are structural determinants of sodium channel slow inactivation, and that the beta(1)-subunit modulates slow inactivation in hSkM1 but not hH1. Changes in slow inactivation time constants in sodium channels coexpressed with the beta(1)-subunit indicate possible interactions among the beta(1)-subunit, P-loops, and the slow inactivation gate in sodium channels.

Using site-directed fluorescent labeling, we examined conformational changes in the S4 segment of each domain of the human skeletal muscle sodium channel (hSkM1). The fluorescence signals from S4 segments in domains I and II follow activation and are unaffected as fast inactivation settles. In contrast, the fluorescence signals from S4 segments in domains III and IV show kinetic components during activation and deactivation that correlate with fast inactivation and charge immobilization. These results indicate that in hSkM1, the S4 segments in domains III and IV are responsible for voltage-sensitive conformational changes linked to fast inactivation and are immobilized by fast inactivation, while the S4 segments in domains I and II are unaffected by fast inactivation.

The available pool of sodium channels, and thus cell excitability, is regulated by both fast and slow inactivation. In cardiac tissue, the requirement for sustained firing of long-duration action potentials suggests that slow inactivation in cardiac sodium channels may differ from slow inactivation in skeletal muscle sodium channels. To test this hypothesis, we used the macropatch technique to characterize slow inactivation in human cardiac sodium channels heterologously expressed in Xenopus oocytes. Slow inactivation was isolated from fast inactivation kinetically (by selectively recovering channels from fast inactivation before measurement of slow inactivation) and structurally (by modification of fast inactivation by mutation of IFM1488QQQ). Time constants of slow inactivation in cardiac sodium channels were larger than previously reported for skeletal muscle sodium channels. In addition, steady-state slow inactivation was only 40% complete in cardiac sodium channels, compared to 80% in skeletal muscle channels. These results suggest that cardiac sodium channel slow inactivation is adapted for the sustained depolarizations found in normally functioning cardiac tissue. Complete slow inactivation in the fast inactivation modified IFM1488QQQ cardiac channel mutant suggests that this impairment of slow inactivation may result from an interaction between fast and slow inactivation.

The skeletal muscle sodium channel mutant I1160V cosegregates with a disease phenotype producing myotonic discharges (observed as muscle stiffness) that are worsened by elevated K+ levels but unaffected by cooling. The I1160V alpha-subunit was co-expressed with the beta1-subunit in Xenopus oocytes. An electrophysiological characterization was undertaken to examine the underlying biophysical characteristics imposed by this mutation. Two abnormalities were found. 1) The voltage dependence of steady-state fast inactivation was reduced in I1160V, which resulted in faster rates of closed-state fast inactivation onset and recovery in I1160V compared with wild-type channels. 2) The rates of deactivation were slower in I1160V than in wild-type channels. Using a computer-simulated model, the combination of both defects elicited myotonic runs under conditions of elevated K+, consistent with the observed phenotype of the mutant.

Rat skeletal muscle (Skm1) sodium channel alpha and beta 1 subunits were coexpressed in Xenopus oocytes, and resulting sodium currents were recorded from on-cell macropatches. First, the kinetics and steady-state probability of both fast and slow inactivation in Skm1 wild type (WT) sodium channels were characterized. Next, we confirmed that mutation of IFM to QQQ (IFM1303QQQ) in the DIII-IV 'inactivation loop' completely removed fast inactivation at all voltages. This mutation was then used to characterize Skm1 slow inactivation without the presence of fast inactivation. The major findings of this paper are as follows: 1) Even with complete removal of fast inactivation by the IFM1303QQQ mutation, slow inactivation remains intact. 2) In WT channels, approximately 20% of channels fail to slow-inactivate after fast-inactivating, even at very positive potentials. 3) Selective removal of fast inactivation by IFM1303QQQ allows slow inactivation to occur more quickly and completely than in WT. We conclude that fast inactivation reduces the probability of subsequent slow inactivation.

Illumination of crayfish giant axons, during internal perfusion with 0.5 mM methylene blue (MB), produces photodynamic effects that include (i) reduction in total sodium conductance, (ii) shifting of the steady-state inactivation curve to the right along the voltage axis, (iii) reduction in the effective valence of steady-state inactivation and, (iv) potentially complete removal of fast inactivation. Additionally, the two kinetic components of fast inactivation in crayfish axons are differentially affected by MB+light. The intercept of the faster component (tau h1) is selectively reduced at shorter MB+light exposure times. Neither tau h1 nor the slower (tau h2) process was protected from MB+light by prior steady-state inactivation of sodium channels. However, carotenoids provide differing degrees of protection against each of the photodynamic actions listed above, suggesting that the four major effects of MB+light are mediated by changes occurring within different regions of the sodium channel molecule.

Changes in holding potential (Vh), affect both gating charge (the Q(Vh) curve) and peak ionic current (the F(Vh) curve) seen at positive test potentials. Careful comparison of the Q(Vh) and F(Vh) distributions indicates that these curves are similar, having two slopes (approximately 2.5e for Vh from -115 to -90 mV and approximately 4e for Vh from -90 to -65 mV) and very negative midpoints (approximately -86 mV). Thus, gating charge movement and channel availability appear closely coupled under fully-equilibrated conditions. The time course by which channels approach equilibration was explored using depolarizing prepulses of increasing duration. The high slope component seen in the F(Vh) and Q(Vh) curves is not evident following short depolarizing prepulses in which the prepulse duration approximately corresponds to the settling time for fast inactivation. Increasing the prepulse duration to 10 ms or longer reveals the high slope, and left-shifts the midpoint to more negative voltages, towards the F(Vh) and Q(Vh) distributions. These results indicate that a separate slow-moving voltage sensor affects the channels at prepulse durations greater than 10 ms. Charge movement and channel availability remain closely coupled as equilibrium is approached using depolarizing pulses of increasing durations. Both measures are 50% complete by 50 ms at a prepulse potential of -70 mV, with proportionately faster onset rates when the prepulse potential is more depolarized. By contrast, charge movement and channel availability dissociate during recovery from prolonged depolarizations. Recovery of gating charge is considerably faster than recovery of sodium ionic current after equilibration at depolarized potentials. Recovery of gating charge at -140 mV, is 65% complete within approximately 100 ms, whereas less than 30% of ionic current has recovered by this time. Thus, charge movement and channel availability appear to be uncoupled during recovery, although both rates remain voltage sensitive. These data suggest that channels remain inactivated due to a separate process operating in parallel with the fast gating charge. We demonstrate that this behavior can be simulated by a model in which the fast charge movement associated with channel activation is electrostatically-coupled to a separate slow voltage sensor responsible for the slow inactivation of channel conductance.

Kinetic effects of osmotic stress on sodium ionic and gating currents have been studied in crayfish giant axons after removal of fast inactivation with chloramine-T. Internal perfusion with media made hyperosmolar by addition of formamide or sucrose, reduces peak sodium current (before and after removal of fast inactivation with chloramine-T), increases the half-time for activation, but has no effect on tail current deactivation rate(s). Kinetics of ON and OFF gating currents are not affected by osmotic stress. These results confirm (and extend to sodium channels) the separation of channel gating mechanisms into voltage-sensitive and solvent-sensitive processes recently proposed by Zimmerberg J., F. Bezanilla, and V. A. Parsegian. (1990. Biophys. J. 57:1049-1064) for potassium delayed rectifier channels. Additionally, the kinetic effects produced by hyperosmolar media seem qualitatively similar to the kinetic effects of heavy water substitution in crayfish axons (Alicata, D. A., M. D. Rayner, and J. G. Starkus. 1990. Biophys. J. 57:745-758). However, our observations are incompatible with models in which voltage-sensitive and solvent-sensitive gating processes are presumed to be either (a) strictly sequential or, (b) parallel and independent. We introduce a variant of the parallel model which includes explicit coupling between voltage-sensitive and solvent-sensitive processes. Simulations of this model, in which the total coupling energy is as small as 1/10th of kT, demonstrate the characteristic kinetic changes noted in our data.

Sodium channel activations, measured as the fraction of channels open to peak conductance for different test potentials (F[V]), shows two statistically different slopes from holding potential more positive than -90 mV. A high valence of 4-6e is indicated a test potentials within 35 mV of the apparent threshold potential (circa -65 mV at -85 mV holding potential). However, for test potentials positive to -30 mV, the F(V) curve shows a 2e valence. The F(V) curve for crayfish axon sodium channels at these "depolarized" holding potentials thus closely resembles classic data obtained from other preparations at holding potentials between -80 and -60 mV. In contrast, at holding potentials more negative than -100 mV, the high slope essentially disappears and the F(V) curve follows a single Boltzmann distribution with a valence of approximately 2e at all potentials. Neither the slope of this simple distribution nor its midpoint (-20 mV) was significantly affected by removal of fast inactivation with pronase. The change in F(V) slope, when holding potential is increased from -85 to -120 mV, does not appear to be caused by the contribution of a second channel type. The simple voltage dependence of sodium current found at Vh -120 mV be used by to discriminate between models of sodium channel activation, and rules out models with three particles of equal valence.