Cardiac channel gating charge movements: recovery from inactivation

1995 ◽  
Vol 430 (5) ◽  
pp. 682-689 ◽  
Author(s):  
Ira R. Josephson ◽  
Yong Cui
1983 ◽  
Vol 82 (5) ◽  
pp. 679-701 ◽  
Author(s):  
D T Campbell

Charge movements similar to those attributed to the sodium channel gating mechanism in nerve have been measured in frog skeletal muscle using the vaseline-gap voltage-clamp technique. The time course of gating currents elicited by moderate to strong depolarizations could be well fitted by the sum of two exponentials. The gating charge exhibits immobilization: at a holding potential of -90 mV the proportion of charge that returns after a depolarizing prepulse (OFF charge) decreases with the duration of the prepulse with a time course similar to inactivation of sodium currents measured in the same fiber at the same potential. OFF charge movements elicited by a return to more negative holding potentials of -120 or -150 mV show distinct fast and slow phases. At these holding potentials the total charge moved during both phases of the gating current is equal to the ON charge moved during the preceding prepulse. It is suggested that the slow component of OFF charge movement represents the slower return of charge "immobilized" during the prepulse. A slow mechanism of charge immobilization is also evident: the maximum charge moved for a strong depolarization is approximately doubled by changing the holding potential from -90 to -150 mV. Although they are larger in magnitude for a -150-mV holding potential, the gating currents elicited by steps to a given potential have similar kinetics whether the holding potential is -90 or -150 mV.


1977 ◽  
Vol 70 (5) ◽  
pp. 567-590 ◽  
Author(s):  
C M Armstrong ◽  
F Bezanilla

Gating current (Ig) has been studied in relation to inactivation of Na channels. No component of Ig has the time course of inactivation; apparently little or no charge movement is associated with this step. Inactivation nonetheless affects Ig by immobilizing about two-thirds of gating charge. Immobilization can be followed by measuring ON charge movement during a pulse and comparing it to OFF charge after the pulse. The OFF:ON ratio is near 1 for a pulse so short that no inactivation occurs, and the ratio drops to about one-third with a time course that parallels inactivation. Other correlations between inactivation and immobilization are that: (a) they have the same voltage dependence; (b) charge movement recovers with the time coures of recovery from inactivation. We interpret this to mean that the immobilized charge returns slowly to "off" position with the time course of recovery from inactivation, and that the small current generated is lost in base-line noise. At -150 mV recover is very rapid, and the immobilized charge forms a distinct slow component of current as it returns to off position. After destruction of inactivation by pronase, there is no immobilization of charge. A model is presented in which inactivation gains its voltage dependence by coupling to the activation gate.


1989 ◽  
Vol 94 (1) ◽  
pp. 65-93 ◽  
Author(s):  
B P Bean ◽  
E Rios

Intramembrane charge movement was recorded in rat and rabbit ventricular cells using the whole-cell voltage clamp technique. Na and K currents were eliminated by using tetraethylammonium as the main cation internally and externally, and Ca channel current was blocked by Cd and La. With steps in the range of -110 to -150 used to define linear capacitance, extra charge moves during steps positive to approximately -70 mV. With holding potentials near -100 mV, the extra charge moving outward on depolarization (ON charge) is roughly equal to the extra charge moving inward on repolarization (OFF charge) after 50-100 ms. Both ON and OFF charge saturate above approximately +20 mV; saturating charge movement is approximately 1,100 fC (approximately 11 nC/muF of linear capacitance). When the holding potential is depolarized to -50 mV, ON charge is reduced by approximately 40%, with little change in OFF charge. The reduction of ON charge by holding potential in this range matches inactivation of Na current measured in the same cells, suggesting that this component might arise from Na channel gating. The ON charge remaining at a holding potential of -50 mV has properties expected of Ca channel gating current: it is greatly reduced by application of 10 muM D600 when accompanied by long depolarizations and it is reduced at more positive holding potentials with a voltage dependence similar to that of Ca channel inactivation. However, the D600-sensitive charge movement is much larger than the Ca channel gating current that would be expected if the movement of channel gating charge were always accompanied by complete opening of the channel.


2004 ◽  
Vol 123 (5) ◽  
pp. 555-571 ◽  
Author(s):  
Dmytro Isaev ◽  
Karisa Solt ◽  
Oksana Gurtovaya ◽  
John P. Reeves ◽  
Roman Shirokov

Both intracellular calcium and transmembrane voltage cause inactivation, or spontaneous closure, of L-type (CaV1.2) calcium channels. Here we show that long-lasting elevations of intracellular calcium to the concentrations that are expected to be near an open channel (≥100 μM) completely and reversibly blocked calcium current through L-type channels. Although charge movements associated with the opening (ON) motion of the channel's voltage sensor were not altered by high calcium, the closing (OFF) transition was impeded. In two-pulse experiments, the blockade of calcium current and the reduction of gating charge movements available for the second pulse developed in parallel during calcium load. The effect depended steeply on voltage and occurred only after a third of the total gating charge had moved. Based on that, we conclude that the calcium binding site is located either in the channel's central cavity behind the voltage-dependent gate, or it is formed de novo during depolarization through voltage-dependent rearrangements just preceding the opening of the gate. The reduction of the OFF charge was due to the negative shift in the voltage dependence of charge movement, as previously observed for voltage-dependent inactivation. Elevation of intracellular calcium concentration from ∼0.1 to 100–300 μM sped up the conversion of the gating charge into the negatively distributed mode 10–100-fold. Since the “IQ-AA” mutant with disabled calcium/calmodulin regulation of inactivation was affected by intracellular calcium similarly to the wild-type, calcium/calmodulin binding to the “IQ” motif apparently is not involved in the observed changes of voltage-dependent gating. Although calcium influx through the wild-type open channels does not cause a detectable negative shift in the voltage dependence of their charge movement, the shift was readily observable in the Δ1733 carboxyl terminus deletion mutant, which produces fewer nonconducting channels. We propose that the opening movement of the voltage sensor exposes a novel calcium binding site that mediates inactivation.


1996 ◽  
Vol 107 (2) ◽  
pp. 183-194 ◽  
Author(s):  
S Ji ◽  
A L George ◽  
R Horn ◽  
R L Barchi

Mutations in the gene encoding the voltage-gated sodium channel of skeletal muscle (SkMl) have been identified in a group of autosomal dominant diseases, characterized by abnormalities of the sarcolemmal excitability, that include paramyotonia congenita (PC) and hyperkalemic periodic paralysis (HYPP). We previously reported that PC mutations cause in common a slowing of inactivation in the human SkMl sodium channel. In this investigation, we examined the molecular mechanisms responsible for the effects of L1433R, located in D4/S3, on channel gating by creating a series of additional mutations at the 1433 site. Unlike the R1448C mutation, found in D4/S4, which produces its effects largely due to the loss of the positive charge, change of the hydropathy of the side chain rather than charge is the primary factor mediating the effects of L1433R. These two mutations also differ in their effects on recovery from inactivation, conditioned inactivation, and steady state inactivation of the hSkMl channels. We constructed a double mutation containing both L1433R and R1448C. The double mutation closely resembled R1448C with respect to alterations in the kinetics of inactivation during depolarization and voltage dependence, but was indistinguishable from L1433R in the kinetics of recovery from inactivation and steady state inactivation. No additive effects were seen, suggesting that these two segments interact during gating. In addition, we found that these mutations have different effects on the delay of recovery from inactivation and the kinetics of the tail currents, raising a question whether this delay is a reflection of the deactivation process. These results suggest that the S3 and S4 segments play distinct roles in different processes of hSkM1 channel gating: D4/S4 is critical for the deactivation and inactivation of the open channel while D4/S3 has a dominant role in the recovery of inactivated channels. However, these two segments interact during the entry to, and exit from, inactivation states.


Sign in / Sign up

Export Citation Format

Share Document