Membrane tension, lipid adaptation, conformational changes, and energetics in MscL gating

This study aims to explore gating mechanisms of mechanosensitive channels in terms of membrane tension, membrane adaptation, protein conformation, and energetics. The large conductance mechanosensitive channel from Mycobacterium tuberculosis (Tb-MscL) is used as a model system; Tb-MscL acts as a safety valve by releasing small osmolytes through the channel opening under extreme hypoosmotic conditions. Based on the assumption that the channel gating involves tilting of the transmembrane (TM) helices, we have performed free energy simulations of Tb-MscL as a function of TM helix tilt angle in a dimyristoylphosphatidylcholine bilayer. Based on the change in system dimensions, TM helix tilting is shown to be essentially equivalent to applying an excess surface tension to the membrane, causing channel expansion, lipid adaptation, and membrane thinning. Such equivalence is further corroborated by the observation that the free energy cost of Tb-MscL channel expansion is comparable to the work done by the excess surface tension. Tb-MscL TM helix tilting results in an expanded water-conducting channel of an outer dimension similar to the proposed fully open MscL structure. The free energy decomposition indicates a possible expansion mechanism in which tilting and expanding of TM2 facilitates the iris-like motion of TM1, producing an expanded Tb-MscL.     

Ion conduction in substates of the batrachotoxin-modified Na+ channel from toad skeletal muscle.

Batrachotoxin-modified Na+ channels from toad muscle were inserted into planar lipid bilayers composed of neutral phospholipids. Single-channel conductances were measured for [Na+] ranging between 0.4 mM and 3 M. When membrane preparations were made in the absence of protease inhibitors, two open conductance states were identified: a fully open state (16.6 pS in 200 mM symmetrical NaCl) and a substate that was 71% of the full conductance. The substate was predominant at [Na+] > 65 mM, whereas the presence of the fully open state was predominant at [Na+] < 15 mM. Addition of protease inhibitors during membrane preparation stabilized the fully open state over the full range of [Na+] studied. In symmetrical Na+ solutions and in biionic conditions, the ratio of amplitudes remained constant and the two open states exhibited the same permeability ratios of PLi/PNa and PCs/PNa. The current-voltage relations for both states showed inward rectification only at [Na+] < 10 mM, suggesting the presence of asymmetric negative charge densities at both channel entrances, with higher charge density in the external side. An energy barrier profile that includes double ion occupancy and asymmetric charge densities at the channel entrances was required to fit the conductance-[Na+] relations and to account for the rectification seen at low [Na+]. Energy barrier profiles differing only in the energy peaks can give account of the differences between both conductance states. Estimation of the surface charge density at the channel entrances is very dependent on the ion occupancy used and the range of [Na+] tested. Independent evidence for the existence of a charged external vestibule was obtained at low external [Na+] by identical reduction of the outward current induced by micromolar additions of Mg2+ and Ba2+.     

Relative Movements of Transmembrane Regions at the Outer Mouth of the Cystic Fibrosis Transmembrane Conductance Regulator Channel Pore during Channel Gating

Multiple transmembrane (TM) segments line the pore of the cystic fibrosis transmembrane conductance regulator Cl(-) channel; however, the relative alignment of these TMs and their relative movements during channel gating are unknown. To gain three-dimensional structural information on the outer pore, we have used patch clamp recording to study the proximity of pairs of cysteine side chains introduced into TMs 6 and 11, using both disulfide cross-linking and Cd(2+) coordination. Following channel activation, disulfide bonds could apparently be formed between three cysteine pairs (of 15 studied): R334C/T1122C, R334C/G1127C, and T338C/S1118C. To examine the state dependence of cross-linking, we combined these cysteine mutations with a nucleotide-binding domain mutation (E1371Q) that stabilizes the channel open state. Investigation of the effects of the E1371Q mutation on disulfide bond formation and Cd(2+) coordination suggests that although R334C/T1122C and T338C/S1118C are closer together in the channel open state, R334C/G1127C are close together and can form disulfide bonds only when the channel is closed. These results provide important new information on the three-dimensional structure of the outer mouth of the cystic fibrosis transmembrane conductance regulator channel pore: TMs 6 and 11 are close enough together to form disulfide bonds in both open and closed channels. Moreover, the altered relative locations of residues in open and in closed channels that we infer allow us to propose that channel opening and closing may be associated with a relative translational movement of TMs 6 and 11, with TM6 moving "down" (toward the cytoplasm) during channel opening.     

Sodium channel subconductance levels measured with a new variance-mean analysis

The currents through single Na+ channels were recorded from dissociated cells of the flexor digitorum brevis muscle of the mouse. At 15 degrees C the prolonged bursts of Na+ channel openings produced by application of the drug DPI 201-106 had brief sojourns to subconductance levels. The subconductance events were relatively rare and brief, but could be identified using a new technique that sorts amplitude estimates based on their variance. The resulting "levels histogram" had a resolution of the conductance levels during channel activity that was superior to that of standard amplitude histograms. Cooling the preparation to 0 degrees C prolonged the subconductance events, and permitted further quantitative analysis of their amplitudes, as well as clear observations of single-channel subconductance events from untreated Na+ channels. In all cases the results were similar: a subconductance level, with an amplitude of roughly 35% of the fully open conductance and similar reversal potential, was present in both drug-treated and normal Na+ channels. Drug-treated channels spent approximately 3-6% of their total open time in the subconductance state over a range of potentials that caused the open probability to vary between 0.1 and 0.9. The summed levels histograms from many channels had a distinctive form, with broader, asymmetrical open and substate distributions compared with those of the closed state. Individual subconductance events to levels other than the most common 35% were also observed. I conclude that subconductance events are a normal subset of the open state of Na+ channels, whether or not they are drug treated. The subconductance events may represent a conformational alteration of the channel that occurs when it conducts ions.     

Regulation of ROMK by extracellular cations

The effect of external potassium (K) and cesium (Cs) on the inwardly rectifying K channel ROMK2 (K(ir)1.1b) was studied in Xenopus oocytes. Elevating external K from 1 to 10 mM increased whole-cell outward conductance by a factor of 3.4 +/- 0.4 in 15 min and by a factor of 5.7 +/- 0.9 in 30 min (n = 22). Replacing external Na by Cs blocked inward conductance but increased whole-cell conductance by a factor of 4.5 +/- 0.5 over a period of 40 min (n = 15). In addition to this slow increase in conductance, there was also a small, rapid increase in conductance that occurred as soon as ROMK was exposed to external cesium or 10 mM K. This rapid increase could be explained by the observed increase in ROMK single-channel conductance from 6.4 +/- 0.8 pS to 11.1 +/- 0.8 pS (10 mM K, n = 8) or 11.7 +/- 1.2 pS (Cs, n = 8). There was no effect of either 10 mM K or cesium on the high open probability (P(o) = 0.97 +/- 0.01; n = 12) of ROMK outward currents. In patch-clamp recordings, the number of active channels increased when the K concentration at the outside surface was raised from 1 to 50 mM K. In cell-attached patches, exposure to 50 mM external K produced one or more additional channels in 9/16 patches. No change in channel number was observed in patches continuously exposed to 50 mM external K. Hence, the slow increase in whole-cell conductance is interpreted as activation of pre-existing ROMK channels that had been inactivated by low external K. This type of time-dependent channel activation was not seen with IRK1 (K(ir)2.1) or in ROMK2 mutants in which any one of 6 residues, F129, Q133, E132, V121, L117, or K61, were replaced by their respective IRK1 homologs. These results are consistent with a model in which ROMK can exist in either an activated mode or an inactivated mode. Within the activated mode, individual channels undergo rapid transitions between open and closed states. High (10 mM) external K or Cs stabilizes the activated mode, and low external K stabilizes the inactivated mode. Mutation of a pH-sensing site (ROMK2-K61) prevents transitions from activated to inactivated modes. This is consistent with a direct effect of external K or Cs on the gating of ROMK by internal pH.     

Mechanosensitive membrane channels in action

The tension-driven gating process of MscL from Mycobacterium tuberculosis, Tb-MscL, has been addressed at near-atomic detail using coarse-grained molecular dynamics simulations. To perform the simulations, a novel coarse-grained peptide model based on a thermodynamic parameterization of the amino-acid side chains has been applied. Both the wild-type Tb-MscL and its gain-of-function mutant V21D embedded in a solvated lipid bilayer have been studied. To mimic hypoosmotic shock conditions, simulations were performed at increasing levels of membrane tension approaching the rupture threshold of the lipid bilayer. Both the wild-type and the mutant channel are found to undergo significant conformational changes in accordance with an irislike expansion mechanism, reaching a conducting state on a microsecond timescale. The most pronounced expansion of the pore has been observed for the V21D mutant, which is consistent with the experimentally shown gain-of-function phenotype of the V21D mutant.     

Energetic and spatial parameters for gating of the bacterial large conductance mechanosensitive channel, MscL

MscL is multimeric protein that forms a large conductance mechanosensitive channel in the inner membrane of Escherichia coli. Since MscL is gated by tension transmitted through the lipid bilayer, we have been able to measure its gating parameters as a function of absolute tension. Using purified MscL reconstituted in liposomes, we recorded single channel currents and varied the pressure gradient (P) to vary the tension (T). The tension was calculated from P and the radius of curvature was obtained using video microscopy of the patch. The probability of being open (Po) has a steep sigmoidal dependence on T, with a midpoint (T1/2) of 11.8 dyn/cm. The maximal slope sensitivity of Po/Pc was 0.63 dyn/cm per e-fold. Assuming a Boltzmann distribution, the energy difference between the closed and fully open states in the unstressed membrane was DeltaE = 18.6 kBT. If the mechanosensitivity arises from tension acting on a change of in-plane area (DeltaA), the free energy, TDeltaA, would correspond to DeltaA = 6.5 nm2. MscL is not a binary channel, but has four conducting states and a closed state. Most transition rates are independent of tension, but the rate-limiting step to opening is the transition between the closed state and the lowest conductance substate. This transition thus involves the greatest DeltaA. When summed over all transitions, the in-plane area change from closed to fully open was 6 nm2, agreeing with the value obtained in the two-state analysis. Assuming a cylindrical channel, the dimensions of the (fully open) pore were comparable to DeltaA. Thus, the tension dependence of channel gating is primarily one of increasing the external channel area to accommodate the pore of the smallest conducting state. The higher conducting states appear to involve conformational changes internal to the channel that don't involve changes in area.     

Patch clamp analysis of a partially purified ion channel from rat liver mitochondria.

A protein fraction isolated from detergent-solubilized mitochondrial membranes by affinity chromatography on immobilized quinine was reconstituted into phospholipid vesicles by detergent dialysis. Vesicles were fused to a diameter of 10 microns or larger by dehydration and rehydration. Patch clamp recordings carried out in detached mode with a symmetrical solution of 150 mM KCl, 5 mM HEPES, and 0.1 mM CaCl2 revealed conductance increments of 140 pS. Transitions of 40 pS were less frequently observed. Control vesicles which lacked protein showed no channel activity. The probability for the 140 pS channel to be open increased with increasing voltage in the range from 20 to 80 mV (positive potentials relative to what was the vesicle interior prior to excision), while the single channel conductance remained essentially constant. The 140 pS channel did not open at negative voltages. The voltage dependence suggests asymmetric incorporation of the 140 pS channel into vesicle membranes during reconstitution.     

Subconductance states of Cx30 gap junction channels: data from transfected HeLa cells versus data from a mathematical model

Human HeLa cells expressing mouse connexin30 were used to study the electrical properties of gap junction channel substates. Experiments were performed on cell pairs using a dual voltage-clamp method. Single-channel currents revealed discrete levels attributable to a main state, a residual state, and five substates interposed, suggesting the operation of six subgates provided by the six connexins of a gap junction hemichannel. Substate conductances, gamma(j,substate), were unevenly distributed between the main-state and the residual-state conductance (gamma(j,main state) = 141 pS, gamma(j,residual state) = 21 pS). Activation of the first subgate reduced the channel conductance by approximately 30%, and activation of subsequent subgates resulted in conductance decrements of 10-15% each. Current transitions between the states were fast (<2 ms). Substate events were usually demarcated by transitions from and back to the main state; transitions among substates were rare. Hence, subgates are recruited simultaneously rather than sequentially. The incidence of substate events was larger at larger gradients of V(j). Frequency and duration of substate events increased with increasing number of synchronously activated subgates. Our mathematical model, which describes the operation of gap junction channels, was expanded to include channel substates. Based on the established V(j)-sensitivity of gamma(j,main state) and gamma(j,residual state), the simulation yielded unique functions gamma(j,substate) = f(V(j)) for each substate. Hence, the spacing of subconductance levels between the channel main state and residual state were uneven and characteristic for each V(j).     

Molecular dynamics simulations of wild-type and mutant forms of the Mycobacterium tuberculosis MscL channel

The crystal structure of the Mycobacterium tuberculosis homolog of the bacterial mechanosensitive channel of large conductance (Tb-MscL) provides a unique opportunity to consider mechanosensitive signal transduction at the atomic level. Molecular dynamics simulations of the Tb-MscL channel embedded in an explicit lipid bilayer and of its C-terminal helical bundle alone in aqueous solvent were performed. C-terminal calculations imply that although the helix bundle structure is relatively unstable at physiological pH, it may have been stabilized under low pH conditions such as those used in the crystallization of the channel. Specific mutations to the C-terminal region, which cause a similar conservation of the crystal structure conformation, have also been identified. Full channel simulations were performed for the wild-type channel and two experimentally characterized gain-of-function mutants, V21A and Q51E. The wild-type Tb-MscL trajectory gives insight into regions of relative structural stability and instability in the channel structure. Channel mutations led to observable changes in the trajectories, such as an alteration of intersubunit interactions in the Q51E mutant. In addition, interesting patterns of protein-lipid interactions, such as hydrogen bonding, arose in the simulations. These and other observations from the simulations are relevant to previous and ongoing experimental studies focusing on characterization of the channel.     

Volume-dependent ATP-conductive large-conductance anion channel as a pathway for swelling-induced ATP release

In mouse mammary C127i cells, during whole-cell clamp, osmotic cell swelling activated an anion channel current, when the phloretin-sensitive, volume-activated outwardly rectifying Cl(-) channel was eliminated. This current exhibited time-dependent inactivation at positive and negative voltages greater than around +/-25 mV. The whole-cell current was selective for anions and sensitive to Gd(3)+. In on-cell patches, single-channel events appeared with a lag period of approximately 15 min after a hypotonic challenge. Under isotonic conditions, cell-attached patches were silent, but patch excision led to activation of currents that consisted of multiple large-conductance unitary steps. The current displayed voltage- and time-dependent inactivation similar to that of whole-cell current. Voltage-dependent activation profile was bell-shaped with the maximum open probability at -20 to 0 mV. The channel in inside-out patches had the unitary conductance of approximately 400 pS, a linear current-voltage relationship, and anion selectivity. The outward (but not inward) single-channel conductance was suppressed by extracellular ATP with an IC(50) of 12.3 mM and an electric distance (delta) of 0.47, whereas the inward (but not outward) conductance was inhibited by intracellular ATP with an IC(50) of 12.9 mM and delta of 0.40. Despite the open channel block by ATP, the channel was ATP-conductive with P(ATP)/P(Cl) of 0.09. The single-channel activity was sensitive to Gd(3)+, SITS, and NPPB, but insensitive to phloretin, niflumic acid, and glibenclamide. The same pharmacological pattern was found in swelling-induced ATP release. Thus, it is concluded that the volume- and voltage-dependent ATP-conductive large-conductance anion channel serves as a conductive pathway for the swelling-induced ATP release in C127i cells.     

Gain-of-function mutations reveal expanded intermediate states and a sequential action of two gates in MscL

The tension-driven gating transition in the large mechanosensitive channel MscL proceeds through detectable states of intermediate conductance. Gain-of-function (GOF) mutants with polar or charged substitutions in the main hydrophobic gate display altered patterns of subconducting states, providing valuable information about gating intermediates. Here we present thermodynamic analysis of several GOF mutants to clarify the nature and position of low-conducting conformations in the transition pathway. Unlike wild-type (WT) MscL, which predominantly occupies the closed and fully open states with very brief substates, the mild V23T GOF mutant frequently visits a multitude of short-lived subconducting states. Severe mutants V23D and G22N open in sequence: closed (C) --> low-conducting substate (S) --> open (O), with the first subtransition occurring at lower tensions. Analyses of equilibrium state occupancies as functions of membrane tension show that the C-->S subtransition in WT MscL is associated with only a minor conductance increment, but the largest in-plane expansion and free energy change. The GOF substitutions strongly affect the first subtransition by reducing area ((Delta)A) and energy ((Delta)E) changes between C and S states commensurably with the severity of mutation. GOF mutants also exhibited a considerably larger (Delta)E associated with the second (S-->O) subtransition, but a (Delta)A similar to WT. The area changes indicate that closed conformations of GOF mutants are physically preexpanded. The tension dependencies of rate constants for channel closure (k(off)) predict different positions of rate-limiting barriers on the energy-area profiles for WT and GOF MscL. The data support the two-gate mechanism in which the first subtransition (C-->S) can be viewed as opening of the central (M1) gate, resulting in an expanded water-filled "leaky" conformation. Strong facilitation of this step by polar GOF substitutions suggests that separation of M1 helices associated with hydration of the pore in WT MscL is the major energetic barrier for opening. Mutants with a stabilized S1 gate demonstrate impeded transitions from low-conducting substates to the fully open state, whereas extensions of S1-M1 linkers result in a much higher probability of reverse O-->S transitions. These data strongly suggest that the bulk of conductance gain in the second subtransition (S-->O) occurs through the opening of the NH2-terminal (S1) gate and the linkers are coupling elements between the M1 and S1 gates.     

Ryanodine stabilizes multiple conformational states of the skeletal muscle calcium release channel.

Nanomolar to micromolar ryanodine alters the gating kinetics of the Ca2+ release channel from skeletal sarcoplasmic reticulum (SR) fused with bilayer lipid membranes (BLM). In the presence of asymmetric CsCl and 100 microM CaCl2 cis, ryanodine (RY) (5-40 nM) activates the channel, increasing the open probability (po; maximum 300% of control) without changing unitary conductance (468 picosiemens (pS)). Statistical analyses of gating kinetics reveal that open and closed dwell times exhibit biexponential distributions and are significantly modified by nanomolar RY. Altered channel gating kinetics with low nanomolar RY is fully reversible and correlates well with binding kinetics of nanomolar [3H]RY with its high affinity site (Kd1 = 0.7 nM) under identical experimental conditions. RY (20-50 nM) induces occasional 1/2 conductance fluctuations which correlate with [3H]RY binding to a second site having lower affinity (Kd2 = 23 nM). RY (5-50 nM) in the presence of 500 mM CsCl significantly enhances Ca(2+)-induced Ca2+ release from actively loaded SR vesicles. Ryanodine > or = 50 nM stabilizes the channel in a 234-pS subconductance which is not readily reversible. RY (> or = 70 microM) produces a unidirectional transition from the 1/2 to a 1/4 conductance fluctuation, whereas RY > or = 200 microM causes complete closure of the channel. The RY required for stabilizing 1/4 conductance transitions and channel closure do not quantitatively correlate with [3H]RY equilibrium binding constants and is attributed to significant reduction in association kinetics with > 200 nM [3H]RY in the presence of 500 mM CsCl. These results demonstrate that RY stabilizes four discrete states of the SR release channel and supports the existence of multiple interacting RY effector sites on the channel protein.     

Adenophostin A and imipramine are two activators of the olfactory inositol 1,4,5-trisphosphate-gated channel in fish olfatory cilia

Binding of an odorant to its receptor activates the cAMP-dependent pathway, and also leads to inositol 1,4,5-trisphosphate (InsP(3)) production. This induces opening of a plasma membrane channel in olfactory receptor cells (ORCs). We investigated single-channel properties of this channel in the presence of a phospholipase C (PLC) activator (imipramine) and of a potent activator of the InsP(3)/Ca(2+) release channel (adenophostin A) by reconstituting carp olfactory cilia into planar lipid bilayers. In the presence of 53 mM barium as a charge carrier, the addition of 50 microM imipramine induced a current of 1.53+/-0.05 pA at 0 mV. There were two different mean open times (6.0+/-0.6 ms and 49.6+/-6.4 ms). The I/ V curve displayed a slope conductance of 50+/-2 pS. Channel activity was transient and was blocked by neomycin (50 microM). These observations suggest that imipramine may activate the olfactory InsP(3)-gated channel through PLC. Using the same ionic conditions, the application of 0.5 microM adenophostin A triggered a current of 1.47+/-0.04 pA at 0 mV. The I/ V curve displayed a slope conductance of 60+/-2 pS. This channel showed only a single mean open time (15.0+/-0.3 ms) and was strongly inhibited by ruthenium red (30 microM) and heparin (10 microg/mL). These results indicate that adenophostin A and imipramine may act on the ciliary InsP(3)-gated channel and are potentially valuable pharmacological tools for studying olfactory transduction mechanisms.     

Epithelial sodium channels: characterization by using the patch-clamp technique

The patch-clamp technique was used to resolve currents through individual Na-selective ion channels in the apical membrane of the rat cortical collecting tubule. The channels had a single unit conductance of 5 pS under control conditions (cell-attached patches, room temperature, 140 mM NaCl in the pipette). They appeared to be highly selective for Na, as K conduction through them was not measurable in inside-out patches. The channels underwent spontaneous transitions between open and closed states, both states being long-lived. At physiological temperature (37C) the conductance increased to 9 pS and the spontaneous transitions became more rapid. In the presence of amiloride on the luminal side of the membrane, the channel flickered rapidly between open and blocked states. The size of the current transitions did not change. This channel activity was observed only in rats that were fed a low-Na diet to elevate aldosterone secretion. In addition to mineralocorticoid control, the activity of the channels in inside-out patches were modulated by the pH on the cytoplasmic side of the membrane. Alkalinization from pH 6.4 to 7.4 increased the probability of channels' being open by eightfold. Changes in Ca concentration on the cytoplasmic side of the membrane did not directly affect the channels. However, addition of ionomycin, a Ca ionophore, to the bath resulted in a decrease in channel activity measured in cell-attached patches. This suggests that high cytoplasmic Ca may indirectly down-regulate Na channels in this tissue.     

Phosphorylation of connexin 50 by protein kinase A enhances gap junction and hemichannel function

Phosphorylation of connexins is an important mechanism regulating gap junction channels. However, the role(s) of connexin (Cx) phosphorylation in vivo are largely unknown. Here, we showed by mass spectrometry that Ser-395 in the C terminus of chicken Cx50 was phosphorylated in the lens. Ser-395 is located within a PKA consensus site. Analyses of Cx50 phosphorylation by two-dimensional thin layer chromatography tryptic phosphopeptide profiles suggested that Ser-395 was targeted by PKA in vivo. PKA activation increased both gap junction dye coupling and hemichannel dye uptake in a manner not involving increases in total Cx50 expression or relocation to the cell surface or gap junctional plaques. Single channel recordings indicated PKA enhanced transitions between the closed and ～200-pS open state while simultaneously reducing transitions between this open state and a ～65-pS subconductance state. The mutation of Ser-395 to alanine significantly attenuated PKA-induced increases in dye coupling and uptake by Cx50. However, channel records indicated that phosphorylation at this site was unnecessary for enhanced transitions between the closed and ～200-pS conductance state. Together, these results suggest that Cx50 is phosphorylated in vivo by PKA at Ser-395 and that this event, although unnecessary for PKA-induced alterations in channel conductance, promotes increased dye permeability of Cx50 channels, which plays an important role in metabolic coupling and transport in lens fibers.     

Characterization of a calcium-activated potassium channel in human fibroblasts

The cell-attached and inside-out patch clamp techniques were used to record single-channel currents from human epidermal fibroblasts. A large-conductance channel (320 pS in symmetric 140 mM KCl) with high potassium selectivity was observed in many patches, particularly those located at the borders of the cells. The channel exhibited both voltage and calcium sensitivity and, therefore, was regarded as a variety of the large-conductance calcium-activated potassium channels reported in many preparations. Probability density functions, fitted to histograms of open and closed time durations at 35 degrees C, usually displayed a minimum of one open state and two closed states. However, kinetic analysis by the fractal method suggested more complicated behavior, particularly for the closed condition. It was not uncommon to observe several channels in one patch. This was distinguishable from the presence of subconductances, which were also observed. Although this channel could have many roles, it seems likely to mediate the calcium-activated conductance that underlies the hyperpolarizing response of fibroblasts to mechanical, electrical, or chemical stimuli.     

Hidden Markov analysis of mechanosensitive ion channel gating

Patch clamp data from the large conductance mechanosensitive channel (MscL) in E. coli was studied with the aim of developing a strategy for statistical analysis based on hidden Markov models (HMMs) and determining the number of conductance levels of the channel, together with mean current, mean dwell time and equilibrium probability of occupancy for each level. The models incorporated state-dependent white noise and moving average adjustment for filtering, with maximum likelihood parameter estimates obtained using an EM (expectation-maximisation) based iteration. Adjustment for filtering was included as it could be expected that the electronic filter used in recording would have a major effect on obviously brief intermediate conductance level sojourns. Preliminary data analysis revealed that the brevity of intermediate level sojourns caused difficulties in assignment of data points to levels as a result of over-estimation of noise variances. When reasonable constraints were placed on these variances using the better determined noise variances for the closed and fully open levels, idealisation anomalies were eliminated. Nevertheless, simulations suggested that mean sojourn times for the intermediate levels were still considerably over-estimated, and that recording bandwidth was a major limitation; improved results were obtained with higher bandwidth data (10 kHz sampled at 25 kHz). The simplest model consistent with these data had four open conductance levels, intermediate levels being approximately 20%, 51% and 74% of fully open. The mean lifetime at the fully open level was about 1 ms; estimates for the three intermediate levels were 54-92 micros, probably still over-estimates.     

Gating properties of gap junction channels assembled from connexin43 and connexin43 fused with green fluorescent protein.

We used cell lines expressing wild-type connexin43 (Cx43) and Cx43 fused with enhanced green fluorescent protein (Cx43-EGFP) to examine mechanisms of gap junction channel gating. Previously it was suggested that each hemichannel in a cell-cell channel possesses two gates, a fast gate that closes channels to a nonzero conductance or residual state via fast (< approximately 2 ms) transitions and a slow gate that fully closes channels via slow transitions (> approximately 10 ms). Here we demonstrate that transjunctional voltage (V(j)) regulates both gates and that they are operating in series and in a contingent manner in which the state of one gate affects gating of the other. Cx43-EGFP channels lack fast V(j) gating to a residual state but show slow V(j) gating. Both Cx43 and Cx43-EGFP channels exhibit slow gating by chemical uncouplers such as CO(2) and alkanols. Chemical uncouplers do not induce obvious changes in Cx43-EGFP junctional plaques, indicating that uncoupling is not caused by dispersion or internalization of junctional plaques. Similarity of gating transitions during chemical gating and slow V(j) gating suggests that both gating mechanisms share common structural elements. Cx43/Cx43-EGFP heterotypic channels showed asymmetrical V(j) gating with fast transitions between open and residual states only when the Cx43 side was relatively negative. This result indicates that the fast V(j) gate of Cx43 hemichannels closes for relative negativity at its cytoplasmic end.     

Effect of ATP concentration on CFTR Cl- channels: a kinetic analysis of channel regulation.

Phosphorylated cystic fibrosis transmembrane conductance regulator (CFTR) Cl- channels require nucleoside triphosphates, such as ATP, to open. As the concentration of intracellular ATP increases, the probability of the channel being open (Po) increases. To better understand how ATP regulates the channel, we studied excised inside-out membrane patches that contained single, phosphorylated CFTR Cl- channels and examined the kinetics of gating at different concentrations of ATP. As the ATP concentration increased from 0.1 to 3 mM the mean closed time decreased, but mean open time did not change. Analysis of the data using histograms of open- and closed-state durations, the maximum likelihood method, and the log-likelihood ratio test suggested that channel behavior could be described by a model containing one open and two closed states (C1<==>C2<==>O). ATP regulated phosphorylated channels at the transition between the closed states C1 and C2: as the concentration of ATP increased, the rate of transition from C1 to C2 (C1-->C2) increased. In contrast, transitions from C2 to C1 and between C2 and the open state (O) were not significantly altered by ATP. Addition of ADP in the presence of ATP decreased the transition rate from C1 to C2 without affecting other transition rates. These data suggest that ATP regulates CFTR Cl- channels through an interaction that increases the rate of transition from the closed state to a bursting state in which the channel flickers back and forth between an open and a closed state (C2). This transition may reflect ATP binding or perhaps a step subsequent to binding.