Single-Channel Kinetics,Inactivation, and Spatial Distribution of Inositol Trisphosphate (IP3) Receptors in Xenopus Oocyte Nucleus

Single-channel properties of the Xenopus inositol trisphosphate receptor (IP₃R) ion channel were examined by patch clamp electrophysiology of the outer nuclear membrane of isolated oocyte nuclei. With 140 mM K⁺ as the charge carrier (cytoplasmic [IP₃] = 10 μM, free [Ca²⁺] = 200 nM), the IP₃R exhibited four and possibly five conductance states. The conductance of the most-frequently observed state M was 113 pS around 0 mV and ∼300 pS at 60 mV. The channel was frequently observed with high open probability (mean P _o = 0.4 at 20 mV). Dwell time distribution analysis revealed at least two kinetic states of M with time constants τ < 5 ms and ∼20 ms; and at least three closed states with τ ∼1 ms, ∼10 ms, and >1 s. Higher cytoplasmic potential increased the relative frequency and τ of the longest closed state. A novel “flicker” kinetic mode was observed, in which the channel alternated rapidly between two new conductance states: F₁ and F₂. The relative occupation probability of the flicker states exhibited voltage dependence described by a Boltzmann distribution corresponding to 1.33 electron charges moving across the entire electric field during F₁ to F₂ transitions. Channel run-down or inactivation (τ ∼ 30 s) was consistently observed in the continuous presence of IP₃ and the absence of change in [Ca²⁺]. Some (∼10%) channel disappearances could be reversed by an increase in voltage before irreversible inactivation. A model for voltage-dependent channel gating is proposed in which one mechanism controls channel opening in both the normal and flicker modes, whereas a separate independent mechanism generates flicker activity and voltage- reversible inactivation. Mapping of functional channels indicates that the IP₃R tends to aggregate into microscopic (<1 μm) as well as macroscopic (∼10 μm) clusters. Ca²⁺-independent inactivation of IP₃R and channel clustering may contribute to complex [Ca²⁺] signals in cells.     

Time-irreversible Subconductance Gating Associated with Ba2+ Block of Large Conductance Ca2+-activated K+ Channels

Ba²⁺ block of large conductance Ca²⁺-activated K⁺ channels was studied in patches of membrane excised from cultures of rat skeletal muscle using the patch clamp technique. Under conditions in which a blocking Ba²⁺ ion would dissociate to the external solution (150 mM N-methyl-d-glucamine⁺ _o, 500 mM K⁺ _i, 10 μM Ba²⁺ _i, +30 mV, and 100 μM Ca²⁺ _i to fully activate the channel), Ba²⁺ blocks with a mean duration of ∼2 s occurred, on average, once every ∼100 ms of channel open time. Of these Ba²⁺ blocks, 78% terminated with a single step in the current to the fully open level and 22% terminated with a transition to a subconductance level at ∼0.26 of the fully open level (preopening) before stepping to the fully open level. Only one apparent preclosing was observed in ∼10,000 Ba²⁺ blocks. Thus, the preopenings represent Ba²⁺-induced time-irreversible subconductance gating. The fraction of Ba²⁺ blocks terminating with a preopening and the duration of preopenings (exponentially distributed, mean = 0.75 ms) appeared independent of changes in [Ba²⁺]_i or membrane potential. The fractional conductance of the preopenings increased from 0.24 at +10 mV to 0.39 at +90 mV. In contrast, the average subconductance level during normal gating in the absence of Ba²⁺ was independent of membrane potential, suggesting different mechanisms for preopenings and normal subconductance levels. Preopenings were also observed with 10 mM Ba²⁺ _o and no added Ba²⁺ _i. Adding K⁺, Rb⁺, or Na⁺ to the external solution decreased the fraction of Ba²⁺ blocks with preopenings, with K⁺ and Rb⁺ being more effective than Na⁺. These results are consistent with models in which the blocking Ba²⁺ ion either induces a preopening gate, and then dissociates to the external solution, or moves to a site located on the external side of the Ba²⁺ blocking site and acts directly as the preopening gate.     

Electrophysiological Characterization of the Rat Epithelial Na+ Channel (rENaC) Expressed in MDCK Cells : Effects of Na+ and Ca2+

The epithelial Na⁺ channel (ENaC), composed of three subunits (α, β, and γ), is expressed in several epithelia and plays a critical role in salt and water balance and in the regulation of blood pressure. Little is known, however, about the electrophysiological properties of this cloned channel when expressed in epithelial cells. Using whole-cell and single channel current recording techniques, we have now characterized the rat αβγENaC (rENaC) stably transfected and expressed in Madin-Darby canine kidney (MDCK) cells. Under whole-cell patch-clamp configuration, the αβγrENaC-expressing MDCK cells exhibited greater whole cell Na⁺ current at −143 mV (−1,466.2 ± 297.5 pA) than did untransfected cells (−47.6 ± 10.7 pA). This conductance was completely and reversibly inhibited by 10 μM amiloride, with a Ki of 20 nM at a membrane potential of −103 mV; the amiloride inhibition was slightly voltage dependent. Amiloride-sensitive whole-cell current of MDCK cells expressing αβ or αγ subunits alone was −115.2 ± 41.4 pA and −52.1 ± 24.5 pA at −143 mV, respectively, similar to the whole-cell Na⁺ current of untransfected cells. Relaxation analysis of the amiloride-sensitive current after voltage steps suggested that the channels were activated by membrane hyperpolarization. Ion selectivity sequence of the Na⁺ conductance was Li⁺ > Na⁺ >> K⁺ = N-methyl-d-glucamine⁺ (NMDG⁺). Using excised outside-out patches, amiloride-sensitive single channel conductance, likely responsible for the macroscopic Na⁺ channel current, was found to be ∼5 and 8 pS when Na⁺ and Li⁺ were used as a charge carrier, respectively. K⁺ conductance through the channel was undetectable. The channel activity, defined as a product of the number of active channel (n) and open probability (P _o), was increased by membrane hyperpolarization. Both whole-cell Na⁺ current and conductance were saturated with increased extracellular Na⁺ concentrations, which likely resulted from saturation of the single channel conductance. The channel activity (nP _o) was significantly decreased when cytosolic Na⁺ concentration was increased from 0 to 50 mM in inside-out patches. Whole-cell Na⁺ conductance (with Li⁺ as a charge carrier) was inhibited by the addition of ionomycin (1 μM) and Ca²⁺ (1 mM) to the bath. Dialysis of the cells with a pipette solution containing 1 μM Ca²⁺ caused a biphasic inhibition, with time constants of 1.7 ± 0.3 min (n = 3) and 128.4 ± 33.4 min (n = 3). An increase in cytosolic Ca²⁺ concentration from <1 nM to 1 μM was accompanied by a decrease in channel activity. Increasing cytosolic Ca²⁺ to 10 μM exhibited a pronounced inhibitory effect. Single channel conductance, however, was unchanged by increasing free Ca²⁺ concentrations from <1 nM to 10 μM. Collectively, these results provide the first characterization of rENaC heterologously expressed in a mammalian epithelial cell line, and provide evidence for channel regulation by cytosolic Na⁺ and Ca²⁺.     

Subunit Composition Determines the Single Channel Kinetics of the Epithelial Sodium Channel

We have further characterized at the single channel level the properties of epithelial sodium channels formed by coexpression of α with either wild-type β or γ subunits and α with carboxy-terminal truncated β (β_T) or γ (γ_T) subunits in Xenopus laevis oocytes. αβ and αβ_T channels (9.6 and 8.7 pS, respectively, with 150 mM Li⁺) were found to be constitutively open. Only upon inclusion of 1 μM amiloride in the pipette solution could channel activity be resolved; both channel types had short open and closed times. Mean channel open probability (P _o) for αβ was 0.54 and for αβ_T was 0.50. In comparison, αγ and αγ_T channels exhibited different kinetics: αγ channels (6.7 pS in Li⁺) had either long open times with short closings, resulting in a high P _o (0.78), or short openings with long closed times, resulting in a low P _o (0.16). The mean P _o for all αγ channels was 0.48. αγ_T (6.6 pS in Li⁺) behaved as a single population of channels with distinct kinetics: mean open time of 1.2 s and closed time of 0.4 s, with a mean P _o of 0.6, similar to that of αγ. Inclusion of 0.1 μM amiloride in the pipette solution reduced the mean open time of αγ_T to 151 ms without significantly altering the closed time. We also examined the kinetics of amiloride block of αβ, αβ_T (1 μM amiloride), and αγ_T (0.1 μM amiloride) channels. αβ and αβ_T had similar blocking and unblocking rate constants, whereas the unblocking rate constant for αγ_T was 10-fold slower than αβ_T. Our results indicate that subunit composition of ENaC is a main determinant of P _o. In addition, channel kinetics and P _o are not altered by carboxy-terminal deletion in the β subunit, whereas a similar deletion in the γ subunit affects channel kinetics but not P _o.     

Imperatoxin A Induces Subconductance States in Ca2+ Release Channels (Ryanodine Receptors) of Cardiac and Skeletal Muscle

Single-channel and [³H]ryanodine binding experiments were carried out to examine the effects of imperatoxin activator (IpTx_a), a 33 amino acid peptide isolated from the venom of the African scorpion Pandinus imperator, on rabbit skeletal and canine cardiac muscle Ca²⁺ release channels (CRCs). Single channel currents from purified CRCs incorporated into planar lipid bilayers were recorded in 250 mM KCl media. Addition of IpTx_a in nanomolar concentration to the cytosolic (cis) side, but not to the lumenal (trans) side, induced substates in both ryanodine receptor isoforms. The substates displayed a slightly rectifying current–voltage relationship. The chord conductance at −40 mV was ∼43% of the full conductance, whereas it was ∼28% at a holding potential of +40 mV. The substate formation by IpTx_a was voltage and concentration dependent. Analysis of voltage and concentration dependence and kinetics of substate formation suggested that IpTx_a reversibly binds to the CRC at a single site in the voltage drop across the channel. The rate constant for IpTx_a binding to the skeletal muscle CRC increased e-fold per +53 mV and the rate constant of dissociation decreased e-fold per +25 mV applied holding potential. The effective valence of the reaction leading to the substate was ∼1.5. The IpTx_a binding site was calculated to be located at ∼23% of the voltage drop from the cytosolic side. IpTx_a induced substates in the ryanodine-modified skeletal CRC and increased or reduced [³H]ryanodine binding to sarcoplasmic reticulum vesicles depending on the level of channel activation. These results suggest that IpTx_a induces subconductance states in skeletal and cardiac muscle Ca²⁺ release channels by binding to a single, cytosolically accessible site different from the ryanodine binding site.     

Electrodiffusion,Barrier, and Gating Analysis of DIDS-insensitive Chloride Conductance in Human Red Blood Cells Treated with Valinomycin or Gramicidin

Current-voltage curves for DIDS-insensitive Cl⁻ conductance have been determined in human red blood cells from five donors. Currents were estimated from the rate of cell shrinkage using flow cytometry and differential laser light scattering. Membrane potentials were estimated from the extracellular pH of unbuffered suspensions using the proton ionophore FCCP. The width of the Gaussian distribution of cell volumes remained invariant during cell shrinkage, indicating a homogeneous Cl⁻ conductance among the cells. After pretreatment for 30 min with DIDS, net effluxes of K⁺ and Cl⁻ were induced by valinomycin and were measured in the continued presence of DIDS; inhibition was maximal at ∼65% above 1 μM DIDS at both 25°C and 37°C. The nonlinear current-voltage curves for DIDS-insensitive net Cl⁻ effluxes, induced by valinomycin or gramicidin at varied [K⁺]_o, were compared with predictions based on (1) the theory of electrodiffusion, (2) a single barrier model, (3) single occupancy, multiple barrier models, and (4) a voltage-gated mechanism. Electrodiffusion precisely describes the relationship between the measured transmembrane voltage and [K⁺]_o. Under our experimental conditions (pH 7.5, 23°C, 1–3 μM valinomycin or 60 ng/ml gramicidin, 1.2% hematocrit), the constant field permeability ratio P_K/P_Cl is 74 ± 9 with 10 μM DIDS, corresponding to 73% inhibition of P_Cl. Fitting the constant field current-voltage equation to the measured Cl⁻ currents yields P _Cl = 0.13 h⁻¹ with DIDS, compared to 0.49 h⁻¹ without DIDS, in good agreement with most previous studies. The inward rectifying DIDS-insensitive Cl⁻ current, however, is inconsistent with electrodiffusion and with certain single-occupancy multiple barrier models. The data are well described either by a single barrier located near the center of the transmembrane electric field, or, alternatively, by a voltage-gated channel mechanism according to which the maximal conductance is 0.055 ± 0.005 S/g Hb, half the channels are open at −27 ± 2 mV, and the equivalent gating charge is −1.2 ± 0.3.     

F-ATPase of Drosophila melanogaster Forms 53-Picosiemen (53-pS) Channels Responsible for Mitochondrial Ca2+-induced Ca2+ Release

Mitochondria of Drosophila melanogaster undergo Ca²⁺-induced Ca²⁺ release through a putative channel (mCrC) that has several regulatory features of the permeability transition pore (PTP). The PTP is an inner membrane channel that forms from F-ATPase, possessing a conductance of 500 picosiemens (pS) in mammals and of 300 pS in yeast. In contrast to the PTP, the mCrC of Drosophila is not permeable to sucrose and appears to be selective for Ca²⁺ and H⁺. We show (i) that like the PTP, the mCrC is affected by the sense of rotation of F-ATPase, by Bz-423, and by Mg²⁺/ADP; (ii) that expression of human cyclophilin D in mitochondria of Drosophila S₂R⁺ cells sensitizes the mCrC to Ca²⁺ but does not increase its apparent size; and (iii) that purified dimers of D. melanogaster F-ATPase reconstituted into lipid bilayers form 53-pS channels activated by Ca²⁺ and thiol oxidants and inhibited by Mg²⁺/γ-imino ATP. These findings indicate that the mCrC is the PTP of D. melanogaster and that the signature conductance of F-ATPase channels depends on unique structural features that may underscore specific roles in different species.     

Interaction of the BKCa channel gating ring with dendrotoxins

Two classes of small homologous basic proteins, mamba snake dendrotoxins (DTX) and bovine pancreatic trypsin inhibitor (BPTI), block the large conductance Ca²⁺-activated K⁺ channel (BK_Ca, KCa1.1) by production of discrete subconductance events when added to the intracellular side of the membrane. This toxin-channel interaction is unlikely to be pharmacologically relevant to the action of mamba venom, but as a fortuitous ligand-protein interaction, it has certain biophysical implications for the mechanism of BK_Ca channel gating. In this work we examined the subconductance behavior of 9 natural dendrotoxin homologs and 6 charge neutralization mutants of δ-dendrotoxin in the context of current structural information on the intracellular gating ring domain of the BK_Ca channel. Calculation of an electrostatic surface map of the BK_Ca gating ring based on the Poisson-Boltzmann equation reveals a predominantly electronegative surface due to an abundance of solvent-accessible side chains of negatively charged amino acids. Available structure-activity information suggests that cationic DTX/BPTI molecules bind by electrostatic attraction to site(s) on the gating ring located in or near the cytoplasmic side portals where the inactivation ball peptide of the β2 subunit enters to block the channel. Such an interaction may decrease the apparent unitary conductance by altering the dynamic balance of open versus closed states of BK_Ca channel activation gating.     

Selectivity Changes during Activation of Mutant Shaker Potassium Channels

Mutations of the pore-region residue T442 in Shaker channels result in large effects on channel kinetics. We studied mutations at this position in the backgrounds of NH₂-terminal–truncated Shaker H4 and a Shaker -NGK2 chimeric channel having high conductance (Lopez, G.A., Y.N. Jan, and L.Y. Jan. 1994. Nature (Lond.). 367: 179–182). While mutations of T442 to C, D, H, V, or Y resulted in undetectable expression in Xenopus oocytes, S and G mutants yielded functional channels having deactivation time constants and channel open times two to three orders of magnitude longer than those of the parental channel. Activation time courses at depolarized potentials were unaffected by the mutations, as were first-latency distributions in the T442S chimeric channel. The mutant channels show two subconductance levels, 37 and 70% of full conductance. From single-channel analysis, we concluded that channels always pass through the larger subconductance state on the way to and from the open state. The smaller subconductance state is traversed in ∼40% of activation time courses. These states apparently represent kinetic intermediates in channel gating having voltage-dependent transitions with apparent charge movements of ∼1.6 e₀. The fully open T442S chimeric channel has the conductance sequence Rb⁺ > NH₄ ⁺ > K⁺. The opposite conductance sequence, K⁺ > NH₄ ⁺ > Rb⁺, is observed in each of the subconductance states, with the smaller subconductance state discriminating most strongly against Rb⁺.     

The β1-Subunit of the MaxiK Channel Associates with the Thromboxane A2 Receptor and Reduces Thromboxane A2 Functional Effects

The large conductance voltage- and Ca²⁺-activated K⁺ channel (MaxiK, BK_Ca, BK) is composed of four pore-forming α-subunits and can be associated with regulatory β-subunits. One of the functional roles of MaxiK is to regulate vascular tone. We recently found that the MaxiK channel from coronary smooth muscle is trans-inhibited by activation of the vasoconstricting thromboxane A₂ prostanoid receptor (TP), a mechanism supported by MaxiK α-subunit (MaxiKα)-TP physical interaction. Here, we examined the role of the MaxiK β1-subunit in TP-MaxiK association. We found that the β1-subunit can by itself interact with TP and that this association can occur independently of MaxiKα. Subcellular localization analysis revealed that β1 and TP are closely associated at the cell periphery. The molecular mechanism of β1-TP interaction involves predominantly the β1 extracellular loop. As reported previously, TP activation by the thromboxane A₂ analog U46619 caused inhibition of MaxiKα macroscopic conductance or fractional open probability (FP_o) as a function of voltage. However, the positive shift of the FP_o versus voltage curve by U46619 relative to the control was less prominent when β1 was coexpressed with TP and MaxiKα proteins (20 ± 6 mV, n = 7) than in cells expressing TP and MaxiKα alone (51 ± 7 mV, n = 7). Finally, β1 gene ablation reduced the EC₅₀ of the U46619 agonist in mediating aortic contraction from 18 ± 1 nm (n = 12) to 9 ± 1 nm (n = 12). The results indicate that the β1-subunit can form a tripartite complex with TP and MaxiKα, has the ability to associate with each protein independently, and diminishes U46619-induced MaxiK channel trans-inhibition as well as vasoconstriction.     

Sodium and Calcium Inward Currents in Freshly Dissociated Smooth Myocytes of Rat Uterus

Freshly dissociated myocytes from nonpregnant, pregnant, and postpartum rat uteri have been studied with the tight-seal patch-clamp method. The inward current contains both I_Na and I_Ca that are vastly different from those in tissue-cultured material. I_Na is abolished by Na⁺-free medium and by 1 μM tetrodotoxin. It first appears at ∼−40 mV, reaches maximum at 0 mV, and reverses at 84 mV. It activates with a voltage-dependent τ of 0.2 ms at 20 mV, and inactivates as a single exponential with a τ of 0.4 ms. Na⁺ conductance is half activated at −21.5 mV, and half inactivated at −59 mV. I_Na reactivates with a τ of 20 ms. I_Ca is abolished by Ca²⁺-free medium, Co²⁺ (5 mM), or nisoldipine (2 μM), and enhanced in 30 mM Ca²⁺, Ba²⁺, or BAY-K 8644. It first appears at ∼−30 mV and reaches maximum at +10 mV. It activates with a voltage-dependent τ of 1.5 ms at 20 mV, and inactivates in two exponential phases, with τ''s of 33 and 133 ms. Ca²⁺ conductance is half activated at −7.4 mV, and half inactivated at −34 mV. I_Ca reactivates with τ''s of 27 and 374 ms. I_Na and I_Ca are seen in myocytes from nonpregnant estrus uteri and throughout pregnancy, exhibiting complex changes. The ratio of densities of peak I_Na/I_Ca changes from 0.5 in the nonpregnant state to 1.6 at term. The enhanced role of I_Na, with faster kinetics, allows more frequent repetitive spike discharges to facilitate simultaneous excitation of the parturient uterus. In postpartum, both currents decrease markedly, with I_Na vanishing from most myocytes. Estrogen-enhanced genomic influences may account for the emergence of I_Na, and increased densities of I_Na and I_Ca as pregnancy progresses. Other influences may regulate varied channel expression at different stages of pregnancy.     

Single-channel analysis of the anion channel-forming protein from the plant pathogenic bacterium Clavibacter michiganense ssp. nebraskense

The anion channel protein from Clavibacter michiganense ssp. nebraskense (Schürholz, Th. et al. 1991, J. Membrane Biol. 123: 1-8) was analyzed at different concentrations of KCl and KF. At 0.8 M KCl the conductance G(V_m) increases exponentially from 21 pS at 50 mV up to 53 pS at V_m = 200 mV, 20°C. The concentration dependence of G(V_m) corresponds to a Michaelis-Menten type saturation function at all membrane voltage values applied (0-200 mV). The anion concentration K_0.5, where G(V_m) has its half-maximum value, increases from 0.12 M at 50 mV to 0.24 M at 175 mV for channels in a soybean phospholipid bilayer. The voltage dependence of the single channel conductance, which is different for charged and neutral lipid bilayers, can be described either by a two-state flicker (2SF) model and the Nernst-Planck continuum theory, or by a two barrier, one-site (2B1S) model with asymmetric barriers. The increase in the number of open channels after a voltage jump from 50 mV to 150 mV has a time constant of 0.8 s. The changes of the single-channel conductance are much faster (<1 ms). The electric part of the gating process is characterized by the (reversible) molar electrical work ΔG^θ_el = ρZ_gFV_m ≈ -1.3 RT, which corresponds to the movement of one charge of the gating charge number |Z_g| = 1 across the fraction ρ = ΔV_m/V_m = 0.15 of the membrane voltage V_m = 200 mV. Unlike with chloride, the single channel conductance of fluoride has a maximum at about 150 mV in the presence of the buffer PIPES (≥5 mM, pH 6.8) with K_0.5 ≈ 1 M. It is shown that the decrease in conductance is due to a blocking of the channel by the PIPES anion. In summary, the results indicate that the anion transport by the Clavibacter anion channel (CAC) does not require a voltage dependent conformation change of the CAC.     

Halide Permeation in Wild-Type and Mutant Cystic Fibrosis Transmembrane Conductance Regulator Chloride Channels

Permeation of cystic fibrosis transmembrane conductance regulator (CFTR) Cl⁻ channels by halide ions was studied in stably transfected Chinese hamster ovary cells by using the patch clamp technique. In cell-attached patches with a high Cl⁻ pipette solution, the CFTR channel displayed outwardly rectifying currents and had a conductance near the membrane potential of 6.0 pS at 22°C or 8.7 pS at 37°C. The current–voltage relationship became linear when patches were excised into symmetrical, N-tris(hydroxymethyl)methyl-2-aminomethane sulfonate (TES)-buffered solutions. Under these conditions, conductance increased from 7.0 pS at 22°C to 10.9 pS at 37°C. The conductance at 22°C was ∼1.0 pS higher when TES and HEPES were omitted from the solution, suggesting weak, voltage-independent block by pH buffers. The relationship between conductance and Cl⁻ activity was hyperbolic and well fitted by a Michaelis-Menten–type function having a K _m of ∼38 mM and maximum conductance of 10 pS at 22°C. Dilution potentials measured with NaCl gradients indicated high anion selectivity (P_Na/P_Cl = 0.003–0.028). Biionic reversal potentials measured immediately after exposure of the cytoplasmic side to various test anions indicated P_I (1.8) > P_Br (1.3) > P_Cl (1.0) > P_F (0.17), consistent with a “weak field strength” selectivity site. The same sequence was obtained for external halides, although inward F⁻ flow was not observed. Iodide currents were protocol dependent and became blocked after 1–2 min. This coincided with a large shift in the (extrapolated) reversal potential to values indicating a greatly reduced I⁻/Cl⁻ permeability ratio (P_I/P_Cl < 0.4). The switch to low I⁻ permeability was enhanced at potentials that favored Cl⁻ entry into the pore and was not observed in the R347D mutant, which is thought to lack an anion binding site involved in multi-ion pore behavior. Interactions between Cl⁻ and I⁻ ions may influence I⁻ permeation and be responsible for the wide range of P_I/P_Cl ratios that have been reported for the CFTR channel. The low P_I/P_Cl ratio usually reported for CFTR only occurred after entry into an altered permeability state and thus may not be comparable with permeability ratios for other anions, which are obtained in the absence of iodide. We propose that CFTR displays a “weak field strength” anion selectivity sequence.     

Properties of an Inwardly Rectifying ATP-sensitive K+ Channel in the Basolateral Membrane of Renal Proximal Tubule

The potassium conductance of the basolateral membrane (BLM) of proximal tubule cells is a critical regulator of transport since it is the major determinant of the negative cell membrane potential and is necessary for pump-leak coupling to the Na⁺,K⁺-ATPase pump. Despite this pivotal physiological role, the properties of this conductance have been incompletely characterized, in part due to difficulty gaining access to the BLM. We have investigated the properties of this BLM K⁺ conductance in dissociated, polarized Ambystoma proximal tubule cells. Nearly all seals made on Ambystoma cells contained inward rectifier K⁺ channels (γ_{slope, in} = 24.5 ± 0.6 pS, γ_{chord, out} = 3.7 ± 0.4 pS). The rectification is mediated in part by internal Mg²⁺. The open probability of the channel increases modestly with hyperpolarization. The inward conducting properties are described by a saturating binding–unbinding model. The channel conducts Tl⁺ and K⁺, but there is no significant conductance for Na⁺, Rb⁺, Cs⁺, Li⁺, NH₄⁺, or Cl⁻. The channel is inhibited by barium and the sulfonylurea agent glibenclamide, but not by tetraethylammonium. Channel rundown typically occurs in the absence of ATP, but cytosolic addition of 0.2 mM ATP (or any hydrolyzable nucleoside triphosphate) sustains channel activity indefinitely. Phosphorylation processes alone fail to sustain channel activity. Higher doses of ATP (or other nucleoside triphosphates) reversibly inhibit the channel. The K⁺ channel opener diazoxide opens the channel in the presence of 0.2 mM ATP, but does not alleviate the inhibition of millimolar doses of ATP. We conclude that this K⁺ channel is the major ATP-sensitive basolateral K⁺ conductance in the proximal tubule.     

Voltage-Dependent Modulation of Cardiac Ryanodine Receptors (RyR2) by Protamine

It has been reported that protamine (>10 µg/ml) blocks single skeletal RyR1 channels and inhibits RyR1-mediated Ca²⁺ release from sarcoplasmic reticulum microsomes. We extended these studies to cardiac RyR2 reconstituted into planar lipid bilayers. We found that protamine (0.02–20 µg/ml) added to the cytosolic surface of fully activated RyR2 affected channel activity in a voltage-dependent manner. At membrane voltage (V_m; SR lumen - cytosol) = 0 mV, protamine induced conductance transitions to several intermediate states (substates) as well as full block of RyR2. At V_m>10 mV, the substate with the highest level of conductance was predominant. Increasing V_m from 0 to +80 mV, decreased the number of transitions and residence of the channel in this substate. The drop in current amplitude (full opening to substate) had the same magnitude at 0 and +80 mV despite the ∼3-fold increase in amplitude of the full opening. This is more similar to rectification of channel conductance induced by other polycations than to the action of selective conductance modifiers (ryanoids, imperatoxin). A distinctive effect of protamine (which might be shared with polylysines and histones but not with non-peptidic polycations) is the activation of RyR2 in the presence of nanomolar cytosolic Ca²⁺ and millimolar Mg²⁺ levels. Our results suggest that RyRs would be subject to dual modulation (activation and block) by polycationic domains of neighboring proteins via electrostatic interactions. Understanding these interactions could be important as such anomalies may be associated with the increased RyR2-mediated Ca²⁺ leak observed in cardiac diseases.     

Temperature Dependence of Voltage-gated H+ Currents in Human Neutrophils,Rat Alveolar Epithelial Cells,and Mammalian Phagocytes

H⁺ currents in human neutrophils, rat alveolar epithelial cells, and several mammalian phagocyte cell lines were studied using whole-cell and excised-patch tight-seal voltage clamp techniques at temperatures between 6 and 42°C. Effects of temperature on gating kinetics were distinguished from effects on the H⁺ current amplitude. The activation and deactivation of H⁺ currents were both highly temperature sensitive, with a Q ₁₀ of 6–9 (activation energy, E _a, ≈ 30–38 kcal/mol), greater than for most other ion channels. The similarity of E _a for channel opening and closing suggests that the same step may be rate determining. In addition, when the turn-on of H⁺ currents with depolarization was fitted by a delay and single exponential, both the delay and the time constant (τ_act) had similarly high Q ₁₀. These results could be explained if H⁺ channels were composed of several subunits, each of which undergoes a single rate-determining gating transition. H⁺ current gating in all mammalian cells studied had similarly strong temperature dependences. The H⁺ conductance increased markedly with temperature, with Q ₁₀ ≥ 2 in whole-cell experiments. In excised patches where depletion would affect the measurement less, the Q ₁₀ was 2.8 at >20°C and 5.3 at <20°C. This temperature sensitivity is much greater than for most other ion channels and for H⁺ conduction in aqueous solution, but is in the range reported for H⁺ transport mechanisms other than channels; e.g., carriers and pumps. Evidently, under the conditions employed, the rate-determining step in H⁺ permeation occurs not in the diffusional approach but during permeation through the channel itself. The large E _a of permeation intrinsically limits the conductance of this channel, and appears inconsistent with the channel being a water-filled pore. At physiological temperature, H⁺ channels provide mammalian cells with an enormous capacity for proton extrusion.     

Ca2+ Current and Charge Movements in Skeletal Myotubes Promoted by the β-Subunit of the Dihydropyridine Receptor in the Absence of Ryanodine Receptor Type 1

The β-subunit of the dihydropyridine receptor (DHPR) enhances the Ca²⁺ channel and voltage-sensing functions of the DHPR. In skeletal myotubes, there is additional modulation of DHPR functions imposed by the presence of ryanodine receptor type-1 (RyR1). Here, we examined the participation of the β-subunit in the expression of L-type Ca²⁺ current and charge movements in RyR1 knock-out (KO), β1 KO, and double β1/RyR1 KO myotubes generated by mating heterozygous β1 KO and RyR1 KO mice. Primary myotube cultures of each genotype were transfected with various β-isoforms and then whole-cell voltage-clamped for measurements of Ca²⁺ and gating currents. Overexpression of the endogenous skeletal β1a isoform resulted in a low-density Ca²⁺ current either in RyR1 KO (36 ± 9 pS/pF) or in β1/RyR1 KO (34 ± 7 pS/pF) myotubes. However, the heterologous β2a variant with a double cysteine motif in the N-terminus (C3, C4), recovered a Ca²⁺ current that was entirely wild-type in density in RyR1 KO (195 ± 16 pS/pF) and was significantly enhanced in double β1/RyR1 KO (115 ± 18 pS/pF) myotubes. Other variants tested from the four β gene families (β1a, β1b, β1c, β3, and β4) were unable to enhance Ca²⁺ current expression in RyR1 KO myotubes. In contrast, intramembrane charge movements in β2a-expressing β1a/RyR1 KO myotubes were significantly lower than in β1a-expressing β1a/RyR1 KO myotubes, and the same tendency was observed in the RyR1 KO myotube. Thus, β2a had a preferential ability to recover Ca²⁺ current, whereas β1a had a preferential ability to rescue charge movements. Elimination of the double cysteine motif (β2a C3,4S) eliminated the RyR1-independent Ca²⁺ current expression. Furthermore, Ca²⁺ current enhancement was observed with a β2a variant lacking the double cysteine motif and fused to the surface membrane glycoprotein CD8. Thus, tethering the β2a variant to the myotube surface activated the DHPR Ca²⁺ current and bypassed the requirement for RyR1. The data suggest that the Ca²⁺ current expressed by the native skeletal DHPR complex has an inherently low density due to inhibitory interactions within the DHPR and that the β1a-subunit is critically involved in process.     

Decremental Response to High-Frequency Trains of Acetylcholine Pulses but Unaltered Fractional Ca2+ Currents in a Panel of “Slow-Channel Syndrome” Nicotinic Receptor Mutants

The slow-channel congenital myasthenic syndrome (SCCMS) is a disorder of the neuromuscular junction caused by gain-of-function mutations to the muscle nicotinic acetylcholine (ACh) receptor (AChR). Although it is clear that the slower deactivation time course of the ACh-elicited currents plays a central role in the etiology of this disease, it has been suggested that other abnormal properties of these mutant receptors may also be critical in this respect. We characterized the kinetics of a panel of five SCCMS AChRs (αS269I, βV266M, εL221F, εT264P, and εL269F) at the ensemble level in rapidly perfused outside-out patches. We found that, for all of these mutants, the peak-current amplitude decreases along trains of nearly saturating ACh pulses delivered at physiologically relevant frequencies in a manner that is consistent with enhanced entry into desensitization during the prolonged deactivation phase. This suggests that the increasingly reduced availability of activatable AChRs upon repetitive stimulation may well contribute to the fatigability and weakness of skeletal muscle that characterize this disease. Also, these results emphasize the importance of explicitly accounting for entry into desensitization as one of the pathways for burst termination, if meaningful mechanistic insight is to be inferred from the study of the effect of these naturally occurring mutations on channel function. Applying a novel single-channel–based approach to estimate the contribution of Ca²⁺ to the total cation currents, we also found that none of these mutants affects the Ca²⁺-conduction properties of the AChR to an extent that seems to be of physiological importance. Our estimate of the Ca²⁺-carried component of the total (inward) conductance of wild-type and SCCMS AChRs in the presence of 150 mM Na⁺, 1.8 mM Ca²⁺, and 1.7 mM Mg²⁺ on the extracellular side of cell-attached patches turned out be in the 5.0–9.4 pS range, representing a fractional Ca²⁺ current of ∼14%, on average. Remarkably, these values are nearly identical to those we estimated for the NR1-NR2A N-methyl-d-aspartate receptor (NMDAR), which has generally been considered to be the main neurotransmitter-gated pathway of Ca²⁺ entry into the cell. Our estimate of the rat NMDAR Ca²⁺ conductance (using the same single-channel approach as for the AChR but in the nominal absence of extracellular Mg²⁺) was 7.9 pS, corresponding to a fractional Ca²⁺ current of 13%.     

Anion-Sensitive Regions of L-Type CaV1.2 Calcium Channels Expressed in HEK293 Cells

L-type calcium currents (I_Ca) are influenced by changes in extracellular chloride, but sites of anion effects have not been identified. Our experiments showed that CaV1.2 currents expressed in HEK293 cells are strongly inhibited by replacing extracellular chloride with gluconate or perchlorate. Variance-mean analysis of I_Ca and cell-attached patch single channel recordings indicate that gluconate-induced inhibition is due to intracellular anion effects on Ca²⁺ channel open probability, not conductance. Inhibition of CaV1.2 currents produced by replacing chloride with gluconate was reduced from ∼75%–80% to ∼50% by omitting β subunits but unaffected by omitting α₂δ subunits. Similarly, gluconate inhibition was reduced to ∼50% by deleting an α1 subunit N-terminal region of 15 residues critical for β subunit interactions regulating open probability. Omitting β subunits with this mutant α1 subunit did not further diminish inhibition. Gluconate inhibition was unchanged with expression of different β subunits. Truncating the C terminus at AA1665 reduced gluconate inhibition from ∼75%–80% to ∼50% whereas truncating it at AA1700 had no effect. Neutralizing arginines at AA1696 and 1697 by replacement with glutamines reduced gluconate inhibition to ∼60% indicating these residues are particularly important for anion effects. Expressing CaV1.2 channels that lacked both N and C termini reduced gluconate inhibition to ∼25% consistent with additive interactions between the two tail regions. Our results suggest that modest changes in intracellular anion concentration can produce significant effects on CaV1.2 currents mediated by changes in channel open probability involving β subunit interactions with the N terminus and a short C terminal region.