TEA(+)-sensitive KCNQ1 constructs reveal pore-independent access to KCNE1 in assembled I(Ks) channels

I(Ks), a slowly activating delayed rectifier K(+) current through channels formed by the assembly of two subunits KCNQ1 (KvLQT1) and KCNE1 (minK), contributes to the control of the cardiac action potential duration. Coassembly of the two subunits is essential in producing the characteristic and physiologically critical kinetics of assembled channels, but it is not yet clear where or how these subunits interact. Previous investigations of external access to the KCNE1 protein in assembled I(Ks) channels relied on occlusion of the pore by extracellular application of TEA(+), despite the very low TEA(+) sensitivity (estimated EC(50) > 100 mM) of channels encoded by coassembly of wild-type KCNQ1 with the wild type (WT) or a series of cysteine-mutated KCNE1 constructs. We have engineered a high affinity TEA(+) binding site into the h-KCNQ1 channel by either a single (V319Y) or double (K318I, V319Y) mutation, and retested it for pore-delimited access to specific sites on coassembled KCNE1 subunits. Coexpression of either KCNQ1 construct with WT KCNE1 in Chinese hamster ovary cells does not alter the TEA(+) sensitivity of the homomeric channels (IC(50) approximately 0.4 mM [TEA(+)](out)), providing evidence that KCNE1 coassembly does not markedly alter the structure of the outer pore of the KCNQ1 channel. Coexpression of a cysteine-substituted KCNE1 (F54C) with V319Y significantly increases the sensitivity of channels to external Cd(2+), but neither the extent of nor the kinetics of the onset of (or the recovery from) Cd(2+) block was affected by [TEA(+)](o) at 10x the IC(50) for channel block. These data strongly suggest that access of Cd(2+) to the cysteine-mutated site on KCNE1 is independent of pore occlusion caused by TEA(+) binding to the outer region of the KCNE1/V319Y pore, and that KCNE1 does not reside within the pore region of the assembled channels.     

MinK endows the I(Ks) potassium channel pore with sensitivity to internal tetraethylammonium

I(Ks) channels are heteromeric complexes of pore-forming KvLQT1 subunits and pore-associated MinK subunits. Channels formed only of KvLQT1 subunits vary from I(Ks) channels in their gating kinetics, single-channel conductance, and ion selectivity. Here we show that I(Ks) channels are more sensitive to blockade by internal tetraethylammonium ion (TEA) than KvLQT1 channels. Inhibition by internal TEA is shown to proceed by a simple bimolecular interaction in the I(Ks) conduction pathway. Application of a noise-variance strategy suggests that MinK enhances blockade by increasing the dwell time of TEA on its pore site from approximately 70 to 370 micros. Mutation of consecutive residues across the single transmembrane segment of MinK identifies positions that alter TEA blockade of I(Ks) channels. MinK is seen to determine the pharmacology of I(Ks) channels in addition to establishing their biophysical attributes.     

Identification of specific pore residues mediating KCNQ1 inactivation. A novel mechanism for long QT syndrome

KCNQ1 inactivation bears electrophysiological characteristics different from classical N- and C-type inactivation in Shaker-like potassium channels. However, the molecular site of KCNQ1 inactivation has not yet been determined. KCNQ2 channels do not exert a fast inactivation in contrast to KCNQ1 channels. By expressing functional chimeras between KCNQ1 and KCNQ2 in Xenopus oocytes, we mapped the region of this inactivation to transmembrane domain S5 and the pore loop H5 and finally narrowed down the site to positions Gly(272) and Val(307) in KCNQ1. Exchanging these two amino acids individually with the analogous KCNQ2 residue abolished inactivation. Furthermore, a KCNQ1-like inactivation was introduced into KCNQ2 by mutagenesis in the corresponding region, confirming its relevance for the inactivation process. As KCNQ1 inactivation involves the regions S5 and H5, it exhibits a geography distinct from N- or C-type inactivation. Native cardiac I(Ks) channels comprising KCNQ1 and accessory MinK subunits do not inactivate because of the functional interaction of KCNQ1 with MinK. Mutations in KCNQ1 can lead to long QT1 syndrome, an inherited form of arrhythmia. The long QT1 mutant KCNQ1(L273F) displays a pronounced KCNQ1 inactivation. Here we show that when expressing mutant I(Ks) channels formed from KCNQ1(L273F) and MinK, MinK association no longer eliminates KCNQ1 inactivation. This results in smaller repolarizing currents in the heart and therefore represents a novel mechanism leading to long QT syndrome.     

Location and orientation of minK within the I(Ks) potassium channel complex

The slowly activating cardiac potassium current (I(Ks)) is generated by a heteromultimeric potassium channel complex consisting of pore-forming (KvLQT1) and accessory (minK) subunits belonging to the KCNQ and KCNE gene families, respectively. Evidence indicating that minK residues line the I(Ks) pore originates from the observation that two minK cysteine mutants (G55C and F54C) render I(Ks) Cd2+-sensitive. We have identified a single cysteine residue in the KvLQT1 S6 segment (Cys-331) that contributes to Cd2+ coordination in conjunction with cysteine residues engineered into the minK transmembrane domain. This observation indicates that minK resides in close proximity to S6 in the I(Ks) channel complex. On the basis of homology modeling that compares the KvLQT1 S6 segment with the structure of the bacterial potassium channel KcsA, we predict that the sulfhydryl side chain of Cys-331 projects away from the central axis of the KvLQT1 pore and suggest that minK resides outside of the permeation pathway. A preliminary model illustrating the orientation of minK with S6 was validated by successful prediction of a novel Cd2+ binding site created within the I(Ks) channel complex by engineering additional cysteine residues into both subunits. Our results indicate the location and orientation of minK within the I(Ks) channel complex and further suggest that Cd2+ exerts its effect on I(Ks) through an allosteric mechanism rather than direct pore blockade.     

Charybdotoxin binding in the I(Ks) pore demonstrates two MinK subunits in each channel complex

I(Ks) voltage-gated K(+) channels contain four pore-forming KCNQ1 subunits and MinK accessory subunits in a number that has been controversial. Here, I(Ks) channels assembled naturally by monomer subunits are compared to those with linked subunits that force defined stoichiometries. Two strategies that exploit charybdotoxin (CTX)-sensitive subunit variants are applied. First, CTX on rate, off rate, and equilibrium affinity are found to be the same for channels of monomers and those with a fixed 2:4 MinK:KCNQ1 valence. Second, 3H-CTX and an antibody are used to directly quantify channels and MinK subunits, respectively, showing 1.97 +/- 0.07 MinK per I(Ks) channel. Additional MinK subunits do not enter channels of monomeric subunits or those with fixed 2:4 valence. We conclude that two MinK subunits are necessary, sufficient, and the norm in I(Ks) channels. This stoichiometry is expected for other K(+) channels that contain MinK or MinK-related peptides (MiRPs).     

External barium affects the gating of KCNQ1 potassium channels and produces a pore block via two discrete sites

The pore properties and the reciprocal interactions between permeant ions and the gating of KCNQ channels are poorly understood. Here we used external barium to investigate the permeation characteristics of homomeric KCNQ1 channels. We assessed the Ba(2+) binding kinetics and the concentration and voltage dependence of Ba(2+) steady-state block. Our results indicate that extracellular Ba(2+) exerts a series of complex effects, including a voltage-dependent pore blockade as well as unique gating alterations. External barium interacts with the permeation pathway of KCNQ1 at two discrete and nonsequential sites. (a) A slow deep Ba(2+) site that occludes the channel pore and could be simulated by a model of voltage-dependent block. (b) A fast superficial Ba(2+) site that barely contributes to channel block and mostly affects channel gating by shifting rightward the voltage dependence of activation, slowing activation, speeding up deactivation kinetics, and inhibiting channel inactivation. A model of voltage-dependent block cannot predict the complex impact of Ba(2+) on channel gating in low external K(+) solutions. Ba(2+) binding to this superficial site likely modifies the gating transitions states of KCNQ1. Both sites appear to reside in the permeation pathway as high external K(+) attenuates Ba(2+) inhibition of channel conductance and abolishes its impact on channel gating. Our data suggest that despite the high degree of homology of the pore region among the various K(+) channels, KCNQ1 channels display significant structural and functional uniqueness.     

KCNE peptides differently affect voltage sensor equilibrium and equilibration rates in KCNQ1 K+ channels

KCNQ1 voltage-gated K(+) channels assemble with the family of KCNE type I transmembrane peptides to afford membrane-embedded complexes with diverse channel gating properties. KCNQ1/KCNE1 complexes generate the very slowly activating cardiac I(Ks) current, whereas assembly with KCNE3 produces a constitutively conducting complex involved in K(+) recycling in epithelia. To determine whether these two KCNE peptides influence voltage sensing in KCNQ1 channels, we monitored the position of the S4 voltage sensor in KCNQ1/KCNE complexes using cysteine accessibility experiments. A panel of KCNQ1 S4 cysteine mutants was expressed in Xenopus oocytes, treated with the membrane-impermeant cysteine-specific reagent 2-(trimethylammonium) ethyl methanethiosulfonate (MTSET), and the voltage-dependent accessibility of each mutant was determined. Of these S4 cysteine mutants, three (R228C, G229C, I230C) were modified by MTSET only when KCNQ1 was depolarized. We then employed these state-dependent residues to determine how assembly with KCNE1 and KCNE3 affects KCNQ1 voltage sensor equilibrium and equilibration rates. In the presence of KCNE1, MTSET modification rates for the majority of the cysteine mutants were approximately 10-fold slower, as was recently reported to indicate that the kinetics of the KCNQ1 voltage sensor are slowed by KCNE1 (Nakajo, K., and Y. Kubo. 2007 J. Gen. Physiol. 130:269-281). Since MTS modification rates reflect an amalgam of reagent accessibility, chemical reactivity, and protein conformational changes, we varied the depolarization pulse duration to determine whether KCNE1 slows the equilibration rate of the voltage sensors. Using the state-dependent cysteine mutants, we determined that MTSET modification rates were essentially independent of depolarization pulse duration. These results demonstrate that upon depolarization the voltage sensors reach equilibrium quickly in the presence of KCNE1 and the slow gating of the channel complex is not due to slowly moving voltage sensors. In contrast, all cysteine substitutions in the S4 of KCNQ1/KCNE3 complexes were freely accessible to MTSET independent of voltage, which is consistent with KCNE3 shifting the voltage sensor equilibrium to favor the active state at hyperpolarizing potentials. In total, these results suggest that KCNE peptides differently modulate the voltage sensor in KCNQ1 K(+) channels.     

The role of S4 charges in voltage-dependent and voltage-independent KCNQ1 potassium channel complexes

Voltage-gated potassium (Kv) channels extend their functional repertoire by coassembling with MinK-related peptides (MiRPs). MinK slows the activation of channels formed with KCNQ1 alpha subunits to generate the voltage-dependent I(Ks) channel in human heart; MiRP1 and MiRP2 remove the voltage dependence of KCNQ1 to generate potassium "leak" currents in gastrointestinal epithelia. Other Kv alpha subunits interact with MiRP1 and MiRP2 but without loss of voltage dependence; the mechanism for this disparity is unknown. Here, sequence alignments revealed that the voltage-sensing S4 domain of KCNQ1 bears lower net charge (+3) than that of any other eukaryotic voltage-gated ion channel. We therefore examined the role of KCNQ1 S4 charges in channel activation using alanine-scanning mutagenesis and two-electrode voltage clamp. Alanine replacement of R231, at the N-terminal side of S4, produced constitutive activation in homomeric KCNQ1 channels, a phenomenon not observed with previous single amino acid substitutions in S4 of other channels. Homomeric KCNQ4 channels were also made constitutively active by mutagenesis to mimic the S4 charge balance of R231A-KCNQ1. Loss of single S4 charges at positions R231 or R237 produced constitutively active MinK-KCNQ1 channels and increased the constitutively active component of MiRP2-KCNQ1 currents. Charge addition to the CO2H-terminal half of S4 eliminated constitutive activation in MiRP2-KCNQ1 channels, whereas removal of homologous charges from KCNQ4 S4 produced constitutively active MiRP2-KCNQ4 channels. The results demonstrate that the unique S4 charge paucity of KCNQ1 facilitates its unique conversion to a leak channel by ancillary subunits such as MiRP2.     

Serial perturbation of MinK in IKs implies an alpha-helical transmembrane span traversing the channel corpus

I(Ks) channels contain four pore-forming KCNQ1 subunits and two accessory MinK subunits. MinK influences surface expression, voltage-dependence of gating, conduction, and pharmacology to yield the attributes characteristic of native channels in heart. The structure and location of the MinK transmembrane domain (TMD) remains a matter of scrutiny. As perturbation of gating analysis has correctly inferred the peripheral location and alpha-helical nature of TMDs in pore-forming subunits, the method is applied here to human MinK. Tryptophan and Asparagine substitution at 23 consecutive sites yields perturbation with alpha-helical periodicity (residues 44-56) followed by an alternating impact pattern (residues 56-63). Arginine substitution across the span suggests that as few as eight sites are occluded from aqueous solution (residues 50-57). We favor a TMD model that is alpha-helical with the external portion of the span at a lipid-protein boundary and the inner portion within the channel corpus in complex interactions.     

Evidence for a deep pore activation gate in small conductance Ca2+-activated K+ channels

Small conductance calcium-gated potassium (SK) channels share an overall topology with voltage-gated potassium (K(v)) channels, but are distinct in that they are gated solely by calcium (Ca(2+)), not voltage. For K(v) channels there is strong evidence for an activation gate at the intracellular end of the pore, which was not revealed by substituted cysteine accessibility of the homologous region in SK2 channels. In this study, the divalent ions cadmium (Cd(2+)) and barium (Ba(2+)), and 2-aminoethyl methanethiosulfonate (MTSEA) were used to probe three sites in the SK2 channel pore, each intracellular to (on the selectivity filter side of) the region that forms the intracellular activation gate of voltage-gated ion channels. We report that Cd(2+) applied to the intracellular side of the membrane can modify a cysteine introduced to a site (V391C) just intracellular to the putative activation gate whether channels are open or closed. Similarly, MTSEA applied to the intracellular side of the membrane can access a cysteine residue (A384C) that, based on homology to potassium (K) channel crystal structures (i.e., the KcsA/MthK model), resides one amino acid intracellular to the glycine gating hinge. Cd(2+) and MTSEA modify with similar rates whether the channels are open or closed. In contrast, Ba(2+) applied to the intracellular side of the membrane, which is believed to block at the intracellular end of the selectivity filter, blocks open but not closed channels when applied to the cytoplasmic face of rSK2 channels. Moreover, Ba(2+) is trapped in SK2 channels when applied to open channels that are subsequently closed. Ba(2+) pre-block slows MTSEA modification of A384C in open but not in closed (Ba(2+)-trapped) channels. The findings suggest that the SK channel activation gate resides deep in the vestibule of the channel, perhaps in the selectivity filter itself.     

KCNE2 confers background current characteristics to the cardiac KCNQ1 potassium channel

Mutations in HERG and KCNQ1 (or KVLQT1) genes cause the life-threatening Long QT syndrome. These genes encode K(+) channel pore-forming subunits that associate with ancillary subunits from the KCNE family to underlie the two components, I(Kr) and I(Ks), of the human cardiac delayed rectifier current I(K). The KCNE family comprises at least three members. KCNE1 (IsK or MinK) recapitulates I(Ks) when associated with KCNQ1, whereas it augments the amplitude of an I(Kr)-like current when co-expressed with HERG. KCNE3 markedly changes KCNQ1 as well as HERG current properties. So far, KCNE2 (MirP1) has only been shown to modulate HERG current. Here we demonstrate the interaction of KCNE2 with the KCNQ1 subunit, which results in a drastic change of KCNQ1 current amplitude and gating properties. Furthermore, KCNE2 mutations also reveal their specific functional consequences on KCNQ1 currents. KCNQ1 and HERG appear to share unique interactions with KCNE1, 2 and 3 subunits. With the exception of KCNE3, mutations in all these partner subunits have been found to lead to an increased propensity for cardiac arrhythmias.     

Effect of Na(+) flow on Cd(2+) block of tetrodotoxin-resistant Na(+) channels

Tetrodotoxin-resistant (TTX-R) Na(+) channels are 1,000-fold less sensitive to TTX than TTX-sensitive (TTX-S) Na(+) channels. On the other hand, TTX-R channels are much more susceptible to external Cd(2+) block than TTX-S channels. A cysteine (or serine) residue situated just next to the aspartate residue of the presumable selectivity filter "DEKA" ring of the TTX-R channel has been identified as the key ligand determining the binding affinity of both TTX and Cd(2+). In this study we demonstrate that the binding affinity of Cd(2+) to the TTX-R channels in neurons from dorsal root ganglia has little intrinsic voltage dependence, but is significantly influenced by the direction of Na(+) current flow. In the presence of inward Na(+) current, the apparent dissociation constant of Cd(2+) ( approximately 200 microM) is approximately 9 times smaller than that in the presence of outward Na(+) current. The Na(+) flow-dependent binding affinity change of Cd(2+) block is true no matter whether the direction of Na(+) current is secured by asymmetrical chemical gradient (e.g., 150 mM Na(+) vs. 150 mM Cs(+) on different sides of the membrane, 0 mV) or by asymmetrical electrical gradient (e.g., 150 mM Na(+) on both sides of the membrane, -20 mV vs. 20 mV). These findings suggest that Cd(2+) is a pore blocker of TTX-R channels with its binding site located in a multiion, single-file region near the external pore mouth. Quantitative analysis of the flow dependence with the flux-coupling equation reveals that at least two Na(+) ions coexist with the blocking Cd(2+) ion in this pore region in the presence of 150 mM ambient Na(+). Thus, the selectivity filter of the TTX-R Na(+) channels in dorsal root ganglion neurons might be located in or close to a multiion single-file pore segment connected externally to a wide vestibule, a molecular feature probably shared by other voltage-gated cationic channels, such as some Ca(2+) and K(+) channels.     

Pore determinants of KCNQ3 K+ current expression

KCNQ3 homomeric channels yield very small macroscopic currents compared with other KCNQ channels or KCNQ2/3 heteromers. Two disparate regions of the channels--the C-terminus and the pore region--have been implicated in governing KCNQ current amplitudes. We previously showed that the C-terminus plays a secondary role compared with the pore region. Here, we confirm the critical role of the pore region in determining KCNQ3 currents. We find that mutations at the 312 position in the pore helix of KCNQ3 (I312E, I312K, and I312R) dramatically decreased KCNQ3 homomeric currents as well as heteromeric KCNQ2/3 currents. Evidence that these mutants were expressed in the heteromers includes shifted TEA sensitivity compared with KCNQ2 homomers. To test for differential membrane protein expression, we performed total internal reflection fluorescence imaging, which revealed only small differences that do not underlie the differences in macroscopic currents. To determine whether this mechanism generalizes to other KCNQ channels, we tested the effects of analogous mutations at the conserved I273 position in KCNQ2, with similar results. Finally, we performed homology modeling of the pore region of wild-type and mutant KCNQ3 channels to investigate the putative structural mechanism mediating these results. The modeling suggests that the lack of current in I312E, I312K, and I312R KCNQ3 channels is due to pore helix-selectivity filter interactions that lock the selectivity filter in a nonconductive conformation.     

Epithelial sodium channel pore region. structure and role in gating

Epithelial sodium channels (ENaC) have a crucial role in the regulation of extracellular fluid volume and blood pressure. To study the structure of the pore region of ENaC, the susceptibility of introduced cysteine residues to sulfhydryl-reactive methanethiosulfonate derivatives ((2-aminoethyl)methanethiosulfonate hydrobromide (MTSEA) and [(2-(trimethylammonium)ethyl]methanethiosulfonate bromide (MTSET)) and to Cd(2+) was determined. Selected mutants within the amino-terminal portion (alphaVal(569)-alphaTrp(582)) of the pore region responded to MTSEA, MTSET, or Cd(2+) with stimulation or inhibition of whole cell Na(+) current. The reactive residues were not contiguous but were separated by 2-3 residues where substituted cysteine residues did not respond to the reagents and line one face of an alpha-helix. The activation of alphaS580Cbetagamma mENaC by MTSET was associated with a large increase in channel open probability. Within the carboxyl-terminal portion (alphaSer(583)-alphaSer(592)) of the pore region, only one mutation (alphaS583C) conferred a rapid, nearly complete block by MTSEA, MTSET, and Cd(2+), whereas several other mutant channels were partially blocked by MTSEA or Cd(2+) but not by MTSET. Our data suggest that the outer pore of ENaC is formed by an alpha-helix, followed by an extended region that forms a selectivity filter. Furthermore, our data suggest that the pore region participates in ENaC gating.     

Ionic permeation and conduction properties of neuronal KCNQ2/KCNQ3 potassium channels

Heteromeric KCNQ2/3 potassium channels are thought to underlie the M-current, a subthreshold potassium current involved in the regulation of neuronal excitability. KCNQ channel subunits are structurally unique, but it is unknown whether these structural differences result in unique conduction properties. Heterologously expressed KCNQ2/3 channels showed a permeation sequence of while showing a conduction sequence of A differential contribution of component subunits to the properties of heteromeric KCNQ2/3 channels was demonstrated by studying homomeric KCNQ2 and KCNQ3 channels, which displayed contrasting ionic selectivities. KCNQ2/3 channels did not exhibit an anomalous mole-fraction effect in mixtures of K(+) and Rb(+). However, extreme voltage-dependence of block by external Cs(+) was indicative of multi-ion pore behavior. Block of KCNQ2/3 channels by external Ba(2+) ions was voltage-independent, demonstrating unusual ionic occupation of the outer pore. Selectivity properties and block of KCNQ2 were altered by mutation of outer pore residues in a manner consistent with the presence of multiple ion-binding sites. KCNQ2/3 channel deactivation kinetics were slowed exclusively by Rb(+), whereas activation of KCNQ2/3 channels was altered by a variety of external permeant ions. These data indicate that KCNQ2/3 channels are multi-ion pores which exhibit distinctive mechanisms of ion conduction and gating.     

Interaction between the cardiac rapidly (IKr) and slowly (IKs) activating delayed rectifier potassium channels revealed by low K+-induced hERG endocytic degradation

Cardiac repolarization is controlled by the rapidly (I(Kr)) and slowly (I(Ks)) activating delayed rectifier potassium channels. The human ether-a-go-go-related gene (hERG) encodes I(Kr), whereas KCNQ1 and KCNE1 together encode I(Ks). Decreases in I(Kr) or I(Ks) cause long QT syndrome (LQTS), a cardiac disorder with a high risk of sudden death. A reduction in extracellular K(+) concentration ([K(+)](o)) induces LQTS and selectively causes endocytic degradation of mature hERG channels from the plasma membrane. In the present study, we investigated whether I(Ks) compensates for the reduced I(Kr) under low K(+) conditions. Our data show that when hERG and KCNQ1 were expressed separately in human embryonic kidney (HEK) cells, exposure to 0 mM K(+) for 6 h completely eliminated the mature hERG channel expression but had no effect on KCNQ1. When hERG and KCNQ1 were co-expressed, KCNQ1 significantly delayed 0 mM K(+)-induced hERG reduction. Also, hERG degradation led to a significant reduction in KCNQ1 in 0 mM K(+) conditions. An interaction between hERG and KCNQ1 was identified in hERG+KCNQ1-expressing HEK cells. Furthermore, KCNQ1 preferentially co-immunoprecipitated with mature hERG channels that are localized in the plasma membrane. Biophysical and pharmacological analyses indicate that although hERG and KCNQ1 closely interact with each other, they form distinct hERG and KCNQ1 channels. These data extend our understanding of delayed rectifier potassium channel trafficking and regulation, as well as the pathology of LQTS.     

Electrostatic interaction of internal Mg2+ with membrane PIP2 Seen with KCNQ K+ channels

Activity of KCNQ (Kv7) channels requires binding of phosphatidylinositol 4,5-bisphosphate (PIP(2)) from the plasma membrane. We give evidence that Mg(2+) and polyamines weaken the KCNQ channel-phospholipid interaction. Lowering internal Mg(2+) augmented inward and outward KCNQ currents symmetrically, and raising Mg(2+) reduced currents symmetrically. Polyvalent organic cations added to the pipette solution had similar effects. Their potency sequence followed the number of positive charges: putrescine (+2) < spermidine (+3) < spermine (+4) < neomycin (+6) < polylysine (>+6). The inhibitory effects of Mg(2+) were reversible with sequential whole-cell patching. Internal tetraethylammonium ion (TEA) gave classical voltage-dependent block of the pore with changes of the time course of K(+) currents. The effect of polyvalent cations was simpler, symmetric, and without changes of current time course. Overexpression of phosphatidylinositol 4-phosphate 5-kinase Igamma to accelerate synthesis of PIP(2) attenuated the sensitivity to polyvalent cations. We suggest that Mg(2+) and other polycations reduce the currents by electrostatic binding to the negative charges of PIP(2), competitively reducing the amount of free PIP(2) available for interaction with channels. The dose-response curves could be modeled by a competition model that reduces the pool of free PIP(2). This mechanism is likely to modulate many other PIP(2)-dependent ion channels and cellular processes.     

Voltage-controlled gating at the intracellular entrance to a hyperpolarization-activated cation channel.

Hyperpolarization-activated cation (HCN) channels regulate pacemaking activity in cardiac cells and neurons. Our previous work using the specific HCN channel blocker ZD7288 provided evidence for an intracellular activation gate for these channels because it appears that ZD7288, applied from the intracellular side, can enter and leave HCN channels only at voltages where the activation gate is opened (Shin, K.S., B.S. Rothberg, and G. Yellen. 2001. J. Gen. Physiol. 117:91-101). However, the ZD7288 molecule is larger than the Na(+) or K(+) ions that flow through the open channel. In the present study, we sought to resolve whether the voltage gate at the intracellular entrance to the pore for ZD7288 also can be a gate for permeant ions in HCN channels. Single residues in the putative pore-lining S6 region of an HCN channel (cloned from sea urchin; spHCN) were substituted with cysteines, and the mutants were probed with Cd(2+) applied to the intracellular side of the channel. One mutant, T464C, displayed rapid irreversible block when Cd(2+) was applied to opened channels, with an apparent blocking rate of approximately 3 x 10(5) M(-1)s(-1). The blocking rate was decreased for channels held at more depolarized voltages that close the channels, which is consistent with the Cd(2+) access to this residue being gated from the intracellular side of the channel. 464C channels could be recovered from Cd(2+) inhibition in the presence of a dithiol applied to the intracellular side. The rate of this recovery also was reduced when channels were held at depolarized voltages. Finally, Cd(2+) could be trapped inside channels that were composed of WT/464C tandem-linked subunits, which could otherwise recover spontaneously from Cd(2+) inhibition. Thus, Cd(2+) escape is also gated at the intracellular side of the channel. Together, these results are consistent with a voltage-controlled structure at the intracellular side of the spHCN channel that can gate the flow of cations through the pore.     

A comparison of electrophysiological properties of the CNGA1, CNGA1tandem and CNGA1cys-free Channels

Three constructs are used for the analysis of biophysical properties of CNGA1 channels: the WT CNGA1 channel, a CNGA1 channel where all endogenous cysteines were removed (CNGA1(cys-free)) and a construct composed of two CNGA1 subunits connected by a small linker (CNGA1(tandem)). So far, it has been assumed, but not proven, that the molecular structure of these ionic channels is almost identical. The I/V relations, ionic selectivity to alkali monovalent cations, blockage by tetracaine and TMA(+) were not significantly different. The cGMP dose response and blockage by TEA(+) and Cd(2+) were instead significantly different in CNGA1 and CNGA1(cys-free) channels, but not in CNGA1 and CNGA1(tandem) channels. Cd(2+) blocked irreversibly the mutant channel A406C in the absence of cGMP. By contrast, Cd(2+) did not block the mutant channel A406C in the CNGA1(cys-free) background (A406C(cys-free)), but an irreversible and almost complete blockage was observed in the presence of the cross-linker M-4-M. Results obtained with different MTS cross-linkers and reagents suggest that the 3D structure of the CNGA1(cys-free) differs from that of the CNGA1 channel and that the distance between homologous residues at position 406 in CNGA1(cys-free) is longer than in the WT CNGA1 by several Angstroms.