Changes in the inactivation of rat Kv1.4 K(+) channels induced by varying the number of inactivation particles

N-type inactivation of rat Kv1.4 channels with one, two, or four inactivation balls was investigated using homogeneous populations of channels expressed in Xenopus oocytes. Tandem dimeric and tetrameric constructs of Kv1.4 were made. Channels encoded by tandem cDNAs Kv1. 4-Kv1.4Delta1-145 and Kv1.4-[Kv1.4Delta1-145](3) have two or only one tethered inactivation ball, respectively, whereas Kv1.4 itself encodes channels having four inactivation balls. The time constants for inactivation of macroscopic currents were increased significantly as the number of inactivation balls was decreased, whereas the time constants for recovery from inactivation were not modified. The ratios of the rate constants of inactivation (k(inact)) of Kv1.4-Kv1.4Delta1-145 and Kv1.4-[Kv1.4Delta1-145](3) channels to that of the Kv1.4 channel were 0.65 and 0.4, respectively, whereas the ratios of the rate constant of recovery (k(rec)) of these channels to that of Kv1.4 were almost unity. The rate constants k(inact) for channels having two and four inactivation balls are smaller than those that would be expected if inactivation balls on each channel are independent, suggesting some interaction occurs between inactivation balls. Furthermore, noninactivating current became apparent as the number of inactivation balls on a channel was decreased.     

The relation between ion permeation and recovery from inactivation of ShakerB K+ channels.

We have studied the relation between permeation and recovery from N-type or ball-and-chain inactivation of ShakerB K channels. The channels were expressed in the insect cell line Sf9, by infection with a recombinant baculovirus, and studied under whole cell patch clamp. Recovery from inactivation occurs in two phases. The faster of the two lasts for approximately 200 ms and is followed by a slow phase that may require seconds for completion. The fast phase is enhanced by both permeant ions (K+, Rb+) and by the blocking ion Cs+, whereas the impermeant ions (Na+, Tris+, choline+) are ineffective. The relative potencies are K+ > Rb+ > Cs+ > NH4+ >> Na+ approximately choline+ approximately Tris+. Ion permeation through the channels is not essential for recovery. The results suggest that cations influence the fast phase of recovery by binding in a site with an electrical distance greater than 0.5. Recovery from fast inactivation is voltage-dependent. With Na+, choline+, or Tris+ outside, about 15% of the channels recover in the fast phase (-80 mV), and the other 85% apparently enter a second inactivated state from which recovery is very slow. Recovery in this phase is not influenced by external ions, but is speeded by hyperpolarization.     

Functional role of the NH2-terminal cytoplasmic domain of a mammalian A- type K channel

It has been shown for a Shaker channel (H-4) that its NH2-terminal cytoplasmic domain may form a "ball and chain" structure, with the "chain" tethering the "ball" to the channel while the "ball" capable of binding to the channel in its open state and causing inactivation. Equivalent structures have not been identified in mammalian Shaker homologues. We studied the functional role of the NH2-terminal region of a fast-inactivating mammalian K channel, RHK1 (Kv1.4), by deleting different domains in this region and examining the resultant changes in channel properties at whole cell and single channel levels. Deleting the NH2-terminal hydrophobic domain (domain A) or the subsequent positive charges (domain I) from RHK1 greatly slowed the decay of whole cell currents, suggesting the existence of a ball-like structure in RHK1 similar to that in the Shaker channel. The function of the ball appeared to be abolished by deleting domain A, while modified but maintained by deleting domain I. In the latter case, the data suggest that the positive charges needed for the function of the ball can be replaced by amino acids from a following region (domain III) that has a high positive charge density. Deleting multiple domains from the NH2 terminus of RHK1 corresponding to the chain in Shaker H-4 did not induce expected changes in channel properties that might result from a shortening of a chain. A comparison of single channel kinetics of selected mutant channels with those of the wild-type channel indicated that these deletion mutations slowed whole cell currents by prolonging burst durations and by increasing the probability of reopening during depolarization. There were no changes in single channel current amplitude or latency to first opening. In conclusion, our observations indicate that the inactivation mechanism of RHK1 is similar to that of Shaker H-4 in that a positively charged cytoplasmic domain is important for such a process. The NH2-terminal domain is not involved in channel activation or ion permeation process.     

大鼠背根神经节神经元上失活 BK 通道特性的研究

大电导的电压和 Ca²⁺ 激活的 K⁺ 通道 (BK 通道 ) 在哺乳动物的组织中广泛表达,起着多种多样的作用 . 目前只有少数组织中 BK 通道的性质被深入地研究,而且鲜见有失活的 BK 通道 (BK_i) 的报道,尤其是在神经元中 . 发现在大鼠小直径的背根神经节 (DRG) 神经元中,普遍存在失活的 BK 通道 . 失活的 BK 电流成分是 Ca²⁺敏感的,可以被大电导的 BK 通道特异阻断剂 ChTX 所阻断,而且木瓜蛋白酶可以从胞外改变通道失活的特性 .     

Tyrosine phosphorylation of the inactivating peptide of the shaker B potassium channel: a structural-functional correlate

A synthetic peptide patterned after the sequence of the inactivating "ball" domain of the Shaker B K(+) channel restores fast (N-type) inactivation in mutant deletion channels lacking their constitutive ball domains, as well as in K(+) channels that do not normally inactivate. We now report on the effect of phosphorylation at a single tyrosine in position 8 of the inactivating peptide both on its ability to restore fast channel inactivation in deletion mutant channels and on the conformation adopted by the phosphorylated peptide when challenged by anionic lipid vesicles, a model target mimicking features of the inactivation site in the channel protein. We find that the inactivating peptide phosphorylated at Y8 behaves functionally as well as structurally as the noninactivating mutant carrying the mutation L7E. Moreover, it is observed that the inactivating peptide can be phosphorylated by the Src tyrosine kinase either as a free peptide in solution or when forming part of the membrane-bound protein channel as the constitutive inactivating domain. These findings suggest that tyrosine phosphorylation-dephosphorylation of this inactivating ball domain could be of physiological relevance to rapidly interconvert fast-inactivating channels into delayed rectifiers and vice versa.     

Sodium channel gating in clonal pituitary cells. The inactivation step is not voltage dependent

We have determined the time course of Na channel inactivation in clonal pituitary (GH3) cells by comparing records before and after the enzymatic removal of inactivation. The cells were subjected to whole-cell patch clamp, with papain included in the internal medium. Inactivation was slowly removed over the course of 10 min, making it possible to obtain control records before the enzyme acted. Papain caused a large (4-100x) increase in current magnitude for small depolarizations (near -40 mV), and a much smaller increase for large ones (approximately 1.5x at +40 mV). For technical reasons it was sometimes convenient to study outward INa recorded with no Na+ outside. The instantaneous I-V (IIV) curve in this condition was nonlinear before papain, and more nearly linear afterwards. The gNa-V curve after papain, obtained by dividing the INa-V curve by the IIV curve, was left-shifted by at least 20 mV and steepened. A spontaneous 5-10 mV left shift occurred in the absence of papain. The rate of the inactivation step was found to vary only slightly from -100 mV to +60 mV, based on the following evidence. (a) Before papain, inactivation rate saturated with voltage and was constant from +20 to +60 mV. (b) We activated the channels with a brief pulse, and studied the time course of the current on changing the voltage to a second, usually more negative level (Na+ present internally and externally). The time course of inactivation at each voltage was obtained by comparing control traces with those after inactivation was removed. When the 5-10-mV spontaneous shift was taken into account, inactivation rate changed by less than 10% from -100 to +60 mV. The data are considered in terms of existing models of the Na channel.     

NH2-terminal inactivation peptide binding to C-type-inactivated Kv channels

In many voltage-gated K(+) channels, N-type inactivation significantly accelerates the onset of C-type inactivation, but effects on recovery from inactivation are small or absent. We have exploited the Na(+) permeability of C-type-inactivated K(+) channels to characterize a strong interaction between the inactivation peptide of Kv1.4 and the C-type-inactivated state of Kv1.4 and Kv1.5. The presence of the Kv1.4 inactivation peptide results in a slower decay of the Na(+) tail currents normally observed through C-type-inactivated channels, an effective blockade of the peak Na(+) tail current, and also a delay of the peak tail current. These effects are mimicked by addition of quaternary ammonium ions to the pipette-filling solution. These observations support a common mechanism of action of the inactivation peptide and intracellular quaternary ammonium ions, and also demonstrate that the Kv channel inner vestibule is cytosolically exposed before and after the onset of C-type inactivation. We have also examined the process of N-type inactivation under conditions where C-type inactivation is removed, to compare the interaction of the inactivation peptide with open and C-type-inactivated channels. In C-type-deficient forms of Kv1.4 or Kv1.5 channels, the Kv1.4 inactivation ball behaves like an open channel blocker, and the resultant slowing of deactivation tail currents is considerably weaker than observed in C-type-inactivated channels. We present a kinetic model that duplicates the effects of the inactivation peptide on the slow Na(+) tail of C-type-inactivated channels. Stable binding between the inactivation peptide and the C-type-inactivated state results in slower current decay, and a reduction of the Na(+) tail current magnitude, due to slower transition of channels through the Na(+)-permeable states traversed during recovery from inactivation.     

Effects of channel cytoplasmic regions on the activation mechanisms of cardiac versus skeletal muscle Na(+) channels

Functional comparison of skeletal muscle (rSkM1) and cardiac (hH1) voltage-gated sodium channel isoforms expressed in Chinese hamster ovary cells showed rSkM1 half-activation (V(a)) and inactivation (V(i)) voltages 7 and 10 mV more depolarized than hH1 V(a) and V(i), respectively. Internal papain perfusion removed fast inactivation from each isoform and caused a 20-mV hyperpolarizing shift in hH1 V(a), with an insignificant change in rSkM1 V(a). Activation voltage of the inactivation-deficient hH1 mutant, hH1Q3, was nearly identical to wild-type hH1 V(a), both before and after papain treatment, with hH1Q3 V(a) also shifted by nearly 20 mV after internal papain perfusion. These data indicate that while papain removes both hH1 and rSkM1 inactivation, it has a second effect only on hH1 that causes a shift in activation voltage. Internal treatment with an antibody directed against the III-IV linker essentially mimicked papain treatment by removing some inactivation from each isoform and causing a 12-mV shift in hH1 V(a), while rSkM1 V(a) remained constant. This suggests that some channel segment within, near, or interacting with the III-IV linker is involved in establishing hH1 activation voltage. Together the data show that rSkM1 and hH1 activation mechanisms are different and are the first to suggest a role for a cytoplasmic structure in the voltage-dependent activation of cardiac sodium channels.     

N-type inactivation and the S4-S5 region of the Shaker K+ channel

The intracellular segment of the Shaker K+ channel between transmembrane domains S4 and S5 has been proposed to form at least part of the receptor for the tethered N-type inactivation "ball." We used the approach of cysteine substitution mutagenesis and chemical modification to test the importance of this region in N-type inactivation. We studied N-type inactivation or the block by a soluble inactivation peptide ("ball peptide") before and after chemical modification by methanethiosulfonate reagents. Particularly at position 391, chemical modification altered specifically the kinetics of ball peptide binding without altering other biophysical properties of the channel. Results with reagents that attach different charged groups at 391 C suggested that there are both electrostatic and steric interactions between this site and the ball peptide. These findings identify this site to be in or near the receptor site for the inactivation ball. At many of the other positions studied, modification noticeably inhibited channel current. The accessible cysteines varied in the state-dependence of their modification, with five- to tenfold changes in reactions rate depending on the gating state of the channel.     

On the distribution of the time required to remove white balls from an URN

Balls are removed one-at-a-time at equal time intervals from an urn initially containingw ₀ white balls and a large number b of black balls and each black or white ball is immediately replaced by a black ball. The distribution of the number of white balls remaining aftert iterations (under certain limiting operations) is taken from the literature. The problem is to use this result to find the time required to remove a fixed number of white ballsw ₁ from the urn. We then find the mean and variance of this distribution and also look at the special case whenw ₁ =w ₀.     

A voltage-dependent role for K+ in recovery from C-type inactivation.

Recovery from C-type inactivation of Kv1.3 can be accelerated by the binding of extracellular potassium to the channel in a voltage-dependent fashion. Whole-cell patch-clamp recordings of human T lymphocytes show that Ko+ can bind to open or inactivated channels. Recovery is biphasic with time constants that depend on the holding potential. Recovery is also dependent on the voltage of the depolarizing pulse that induces the inactivation, consistent with a modulatory binding site for K+ located at an effective membrane electrical field distance of 30%. This K(+)-enhanced recovery can be further potentiated by the binding of extracellular tetraethylammonium to the inactivated channel, although the tetraethylammonium does not interact directly with the K(+)-binding site. Our findings are consistent with a model in which K+ can bind and unbind slowly from a channel in the inactivated state, and inactivated channels that are bound by K+ will recover with a rate that is fast relative to unbound channels. Our data suggest that the kinetics of K+ binding to the modulatory site are slower than these recovery rates, especially at hyperpolarized voltages.     

Energetics of Shaker K channels block by inactivation peptides

A synthetic peptide of the NH2-terminal inactivation domain of the ShB channel blocks Shaker channels which have an NH2-terminal deletion and mimics many of the characteristics of the intramolecular inactivation reaction. To investigate the role of electrostatic interactions in both peptide block and the inactivation process we measured the kinetics of block of macroscopic currents recorded from the intact ShB channel, and from ShB delta 6-46 channels in the presence of peptides, at different ionic strengths. The rate of inactivation and the association rate constants (k(on)) for the ShB peptides decreased with increasing ionic strength. k(on) for a more positively charged peptide was more steeply dependent on ionic strength consistent with a simple electrostatic mechanism of enhanced diffusion. This suggests that a rate limiting step in the inactivation process is the diffusion of the NH2-terminal domain towards the pore. The dissociation rates (k(off)) were insensitive to ionic strength. The temperature dependence of k(on) for the ShB peptide was very high, (Q10 = 5.0 +/- 0.58), whereas k(off) was relatively temperature insensitive (Q10 approximately 1.1). The results suggest that at higher temperatures the proportion of time either the peptide or channel spends in the correct conformation for binding is increased. There were two components to the time course of recovery from block by the ShB peptide, indicating two distinct blocked states, one of which has similar kinetics and dependence on external K+ concentration as the inactivated state of ShB. The other is voltage- dependent and at -120 mV is very unstable. Increasing the net charge on the peptide did not increase sensitivity to knock-off by external K+. We propose that the free peptide, having fewer constraints than the tethered NH2-terminal domain binds to a similar site on the channel in at least two different conformations.     

Ultra-slow inactivation in mu1 Na+ channels is produced by a structural rearrangement of the outer vestibule

While studying the adult rat skeletal muscle Na+ channel outer vestibule, we found that certain mutations of the lysine residue in the domain III P region at amino acid position 1237 of the alpha subunit, which is essential for the Na+ selectivity of the channel, produced substantial changes in the inactivation process. When skeletal muscle alpha subunits (micro1) with K1237 mutated to either serine (K1237S) or glutamic acid (K1237E) were expressed in Xenopus oocytes and depolarized for several minutes, the channels entered a state of inactivation from which recovery was very slow, i.e., the time constants of entry into and exit from this state were in the order of approximately 100 s. We refer to this process as "ultra-slow inactivation". By contrast, wild-type channels and channels with the charge-preserving mutation K1237R largely recovered within approximately 60 s, with only 20-30% of the current showing ultra-slow recovery. Coexpression of the rat brain beta1 subunit along with the K1237E alpha subunit tended to accelerate the faster components of recovery from inactivation, as has been reported previously of native channels, but had no effect on the mutation-induced ultra-slow inactivation. This implied that ultra-slow inactivation was a distinct process different from normal inactivation. Binding to the pore of a partially blocking peptide reduced the number of channels entering the ultra-slow inactivation state, possibly by interference with a structural rearrangement of the outer vestibule. Thus, ultra-slow inactivation, favored by charge-altering mutations at site 1237 in micro1 Na+ channels, may be analogous to C-type inactivation in Shaker K+ channels.     

Probing the channel-bound shaker B inactivating peptide by stereoisomeric substitution at a strategic tyrosine residue

A synthetic peptide patterned after the sequence of the inactivating ball domain of the Shaker B K(+) channel, the ShB peptide, fully restores fast inactivation in the deletion Shaker BDelta6-46 K(+) channel, which lacks the constitutive ball domains. On the contrary, a similar peptide in which tyrosine 8 is substituted by the secondary structure-disrupting d-tyrosine stereoisomer does not. This suggests that the stereoisomeric substitution prevents the peptide from adopting a structured conformation when bound to the channel during inactivation. Moreover, characteristic in vitro features of the wild-type ShB peptide such as the marked propensity to adopt an intramolecular beta-hairpin structure when challenged by anionic phospholipid vesicles, a model target mimicking features of the inactivation site in the channel protein, or to insert into their hydrophobic bilayers, are lost in the d-tyrosine-containing peptide, whose behavior is practically identical to that of noninactivating peptide mutants. In the absence of high resolution crystallographic data on the inactivated channel/peptide complex, these latter findings suggest that the structured conformation required for the peptide to promote channel inactivation, as referred to above, is likely to be beta-hairpin.     

Electrostatic interaction between inactivation ball and T1-S1 linker region of Kv1.4 channel

Inactivation of potassium channels plays an important role in shaping the electrical signaling properties of nerve and muscle cells. The rapid inactivation of Kv1.4 has been assumed to be controlled by a "ball and chain" inactivation mechanism. Besides hydrophobic interaction between inactivation ball and the channel's inner pore, the electrostatic interaction has also been proved to participate in the "ball and chain" inactivation process of Kv1.4 channel. Based on the crystal structure of Kv1.2 channel, the acidic T1-S1 linker is indicated to be a candidate interacting with the positively charged hydrophilic region of the inactivation domain. In this study, through mutating the charged residues to amino acids of opposite polar, we identified the electrostatic interaction between the inactivation ball and the T1-S1 linker region of Kv1.4 channel. Inserting negatively charged peptide at the amino terminal of Kv1.4 channel further confirmed the electrostatic interaction between the two regions.     

Ryanoids and imperatoxin affect the modulation of cardiac ryanodine receptors by dihydropyridine receptor Peptide A

Ca²⁺-entry via L-type Ca²⁺ channels (DHPR) is known to trigger ryanodine receptor (RyR)-mediated Ca²⁺-release from sarcoplasmic reticulum (SR). The mechanism that terminates SR Ca²⁺ release is still unknown. Previous reports showed evidence of Ca²⁺-entry independent inhibition of Ca²⁺ sparks by DHPR in cardiomyocytes. A peptide from the DHPR loop II-III (PepA) was reported to modulate isolated RyRs. We found that PepA induced voltage-dependent “flicker block” and transition to substates of fully-activated cardiac RyRs in planar bilayers. Substates had less voltage-dependence than block and did not represent occupancy of a ryanoid site. However, ryanoids stabilized PepA-induced events while PepA increased RyR2 affinity for ryanodol, which suggests cooperative interactions. Ryanodol stabilized Imperatoxin A (IpTx_A) binding but when IpTx_A bound first, it prevented ryanodol binding. Moreover, IpTx_A and PepA excluded each other from their sites. This suggests that IpTx_A generates a vestibular gate (either sterically or allosterically) that prevents access to the peptides and ryanodol binding sites. Inactivating gate moieties (“ball peptides”) from K⁺ and Na⁺ channels (ShakerB and KIFMK, respectively) induced well resolved slow block and substates, which were sensitive to ryanoids and IpTx_A and allowed, by comparison, better understanding of PepA action. The RyR2 appears to interact with PepA or ball peptides through a two-step mechanism, reminiscent of the inactivation of voltage-gated channels, which includes binding to outer (substates) and inner (block) vestibular regions in the channel conduction pathway. Our results open the possibility that “ball peptide-like” moieties in RyR2-interacting proteins could modulate SR Ca²⁺ release in cells.     

Inactivation gating of Kv7.1 channels does not involve concerted cooperative subunit interactions

Inactivation is an intrinsic property of numerous voltage-gated K⁺ (Kv) channels and can occur by N-type or/and C-type mechanisms. N-type inactivation is a fast, voltage independent process, coupled to activation, with each inactivation particle of a tetrameric channel acting independently. In N-type inactivation, a single inactivation particle is necessary and sufficient to occlude the pore. C-type inactivation is a slower process, involving the outermost region of the pore and is mediated by a concerted, highly cooperative interaction between all four subunits. Inactivation of Kv7.1 channels does not exhibit the hallmarks of N- and C-type inactivation. Inactivation of WT Kv7.1 channels can be revealed by hooked tail currents that reflects the recovery from a fast and voltage-independent inactivation process. However, several Kv7.1 mutants such as the pore mutant L273F generate an additional voltage-dependent slow inactivation. The subunit interactions during this slow inactivation gating remain unexplored. The goal of the present study was to study the nature of subunit interactions along Kv7.1 inactivation gating, using concatenated tetrameric Kv7.1 channel and introducing sequentially into each of the four subunits the slow inactivating pore mutation L273F. Incorporating an incremental number of inactivating mutant subunits did not affect the inactivation kinetics but slowed down the recovery kinetics from inactivation. Results indicate that Kv7.1 inactivation gating is not compatible with a concerted cooperative process. Instead, adding an inactivating subunit L273F into the Kv7.1 tetramer incrementally stabilizes the inactivated state, which suggests that like for activation gating, Kv7.1 slow inactivation gating is not a concerted process.     

Structure of the inactivating gate from the Shaker voltage gated K+ channel analyzed by NMR spectroscopy

Rapid inactivation of voltage-gated K⁺ (K_V) channels is mediated by an N-terminal domain (inactivating ball domain) which blocks the open channel from the cytoplasmic side. Inactivating ball domains of various K_V channels are also biologically active when synthesized separately and added as a peptide to the solution. Synthetic inactivating ball domains from different K_V channels with hardly any sequence homology mediate quite similar effects even on unrelated K_V channel subtypes whose inactivation domain has been deleted. The solution structure of the inactivating ball peptide from Shaker (Sh-P22) was analyzed with NMR spectroscopy. The NMR data indicate a non-random structure in an aqueous environment. However, while other inactivating ball peptides showed well-defined three-dimensional structures under these conditions, Sh-P22 does not have a unique, compactly folded structure in solution.     

Selective open-channel block of Shaker (Kv1) potassium channels by s-nitrosodithiothreitol (SNDTT).

Large quaternary ammonium (QA) ions block voltage-gated K(+) (Kv) channels by binding with a 1:1 stoichiometry in an aqueous cavity that is exposed to the cytoplasm only when channels are open. S-nitrosodithiothreitol (SNDTT; ONSCH(2)CH(OH)CH(OH)CH(2)SNO) produces qualitatively similar "open-channel block" in Kv channels despite a radically different structure. SNDTT is small, electrically neutral, and not very hydrophobic. In whole-cell voltage-clamped squid giant fiber lobe neurons, bath-applied SNDTT causes reversible time-dependent block of Kv channels, but not Na(+) or Ca(2)+ channels. Inactivation-removed ShakerB (ShBDelta) Kv1 channels expressed in HEK 293 cells are similarly blocked and were used to study further the action of SNDTT. Dose-response data are consistent with a scheme in which two SNDTT molecules bind sequentially to a single channel, with binding of the first being sufficient to produce block. The dissociation constant for the binding of the second SNDTT molecule (K(d2) = 0.14 mM) is lower than that of the first molecule (K(d1) = 0.67 mM), indicating cooperativity. The half-blocking concentration (K(1/2)) is approximately 0.2 mM. Steady-state block by this electrically neutral compound has a voltage dependence (about -0.3 e(0)) similar in magnitude but opposite in directionality to that reported for QA ions. Both nitrosyl groups on SNDTT (one on each sulfur atom) are required for block, but transfer of these reactive groups to channel cysteine residues is not involved. SNDTT undergoes a slow intramolecular reaction (tau approximately 770 s) in which these NO groups are liberated, leading to spontaneous reversal of the SNDTT effect. Competition with internal tetraethylammonium indicates that bath-applied SNDTT crosses the cell membrane to act at an internal site, most likely within the channel cavity. Finally, SNDTT is remarkably selective for Kv1 channels. When individually expressed in HEK 293 cells, rat Kv1.1-1.6 display profound time-dependent block by SNDTT, an effect not seen for Kv2.1, 3.1b, or 4.2.     

Regulation of Kv4.3 closed state inactivation and recovery by extracellular potassium and intracellular KChIP2b

Mechanisms underlying Kv4 channel inactivation and recovery are presently unclear, although there is general consensus that the basic characteristics of these processes are not consistent with Shaker (Kv1) N- and P/C-type mechanisms. Kv4 channels also differ from Shaker in that they can undergo significant inactivation from pre-activated closed-states (closed-state inactivation, CSI), and that inactivation and recovery kinetics can be regulated by intracellular KChIP2 isoforms. To gain insight into the mechanisms regulating Kv4.3 CSI and recovery, we have analyzed the effects of increasing [K(+)](o) from 2 mM to 98 mM in the absence and in the presence of KChIP2b, the major KChIP2 isoform expressed in the mammalian ventricle. In the absence of KChIP2b, high [K(+)](o) promoted Kv4.3 inactivated closed-states and significantly slowed the kinetics of recovery from both macroscopic and closed-state inactivation. Coexpression of KChIP2b in 2 mM [K(+)](o) promoted non-inactivated closed-states and accelerated the kinetics of recovery from both macroscopic and CSI. In high [K(+)](o), KChIP2b eliminated or significantly reduced the slowing effects on recovery. Attenuation of CSI by the S4 charge-deletion mutant R302A, which produced significant stabilization of non-inactivated closed-states, effectively eliminated the opposing effects of high [K(+)](o) and KChIP2b on macroscopic recovery kinetics, confirming that these results were due to alterations of CSI. Elevated [K(+)](o) therefore slows Kv4.3 recovery by stabilizing inactivated closed-states, while KChIP2b accelerates recovery by destabilizing inactivated closed-states. Our results challenge underlying assumptions of presently popular Kv4 gating models and suggest that Kv4.3 possesses novel allosteric mechanisms, which are absent in Shaker, for coupling interactions between intracellular KChIP2b binding motifs and extracellular K(+)-sensitive regulatory sites.