Voltage Dependence Of Charge Movement Research Articles

Enzyme Domain Affects the Movement of the Voltage Sensor in Ascidian and Zebrafish Voltage-sensing Phosphatases

The ascidian voltage-sensing phosphatase (Ci-VSP) consists of the voltage sensor domain (VSD) and a cytoplasmic phosphatase region that has significant homology to the phosphatase and tensin homolog deleted on chromosome TEN (PTEN). The phosphatase activity of Ci-VSP is modified by the conformational change of the VSD. In many proteins, two protein modules are bidirectionally coupled, but it is unknown whether the phosphatase domain could affect the movement of the VSD in VSP. We addressed this issue by whole-cell patch recording of gating currents from a teleost VSP (Dr-VSP) cloned from Danio rerio expressed in tsA201 cells. Replacement of a critical cysteine residue, in the phosphatase active center of Dr-VSP, by serine sharpened both ON- and OFF-gating currents. Similar changes were produced by treatment with phosphatase inhibitors, pervanadate and orthovanadate, that constitutively bind to cysteine in the active catalytic center of phosphatases. The distinct kinetics of gating currents dependent on enzyme activity were not because of altered phosphatidylinositol 4,5-bisphosphate levels, because the kinetics of gating current did not change by depletion of phosphatidylinositol 4,5-bisphosphate, as reported by coexpressed KCNQ2/3 channels. These results indicate that the movement of the VSD is influenced by the enzymatic state of the cytoplasmic domain, providing an important clue for understanding mechanisms of coupling between the VSD and its effector.

Voltage‐sensitive prestin orthologue expressed in zebrafish hair cells

Prestin, a member of the solute carrier (SLC) family SLC26A, is the molecular motor that drives the somatic electromotility of mammalian outer hair cells (OHCs). Its closest reported homologue, zebrafish prestin (zprestin), shares approximately 70% strong amino acid sequence similarity with mammalian prestin, predicting an almost identical protein structure. Immunohistochemical analysis now shows that zprestin is expressed in hair cells of the zebrafish ear. Similar to mammalian prestin, heterologously expressed zprestin is found to generate voltage-dependent charge movements, giving rise to a non-linear capacitance (NLC) of the cell membrane. Compared with mammalian prestin, charge movements mediated by zprestin display a weaker voltage dependence and slower kinetics; they occur at more positive membrane voltages, and are not associated with electromotile responses. Given this functional dissociation of NLC and electromotility and the structural similarity with mammalian prestin, we anticipate that zprestin provides a valuable tool for tracing the molecular and evolutionary bases of prestin motor function.

Nitric oxide synthase inhibition affects sarcoplasmic reticulum Ca2+ release in skeletal muscle fibres from mouse

Nitric oxide (NO) generated by skeletal muscle is believed to regulate force production but how this is achieved remains poorly understood. In the present work we tested the effects of NO synthase (NOs) inhibitors on membrane current and intracellular calcium in isolated skeletal muscle fibres from mouse, under voltage-clamp conditions. Resting [Ca(2+)] and [Ca(2+)] transients evoked by large depolarizations exhibited similar properties in control fibres and in fibres loaded with tenth millimolar levels of the NOs inhibitor N-nitro-L-arginine (L-NNA). Yet the voltage dependence of calcium release was found to be shifted by approximately 15 mV towards negative values in the presence of L-NNA. This effect could be reproduced by the other NOs inhibitor S-methyl-L-thiocitrulline (L-SMT). Separate experiments showed that the voltage dependence of charge movement and of the slow calcium current were unaffected by the presence of L-NNA, ruling out an effect on the voltage sensor. A negative shift in the voltage dependence of calcium release with no concurrent alteration in the properties of charge movement was also observed in fibres exposed to the oxidant H(2)O(2) (1 mM). Conversely the reducing agent dithiothreitol (10 mM) had no obvious effect on Ca(2+) release. Overall, the results indicate that physiological levels of NO exert a tonic inhibitory control on the activation of the calcium release channels. Changes in the voltage dependence of Ca(2+) release activation may be a ubiquitous physiological consequence of redox-related modifications of the ryanodine receptor.

Regional Specificity of Human ether-a'-go-go-related Gene Channel Activation and Inactivation Gating

Slow activation and rapid C-type inactivation produce inward rectification of the current-voltage relationship for human ether-a'-go-go-related gene (hERG) channels. To characterize the voltage sensor movement associated with hERG activation and inactivation, we performed an Ala scan of the 32 amino acids (Gly(514)-Tyr(545)) that comprise the S4 domain and the flanking S3-S4 and S4-S5 linkers. Gating and ionic currents of wild-type and mutant channels were measured using cut-open oocyte Vaseline gap and two microelectrode voltage clamp techniques to determine the voltage dependence of charge movement, activation, and inactivation. Mapping the position of the charge-perturbing mutations (defined as |DeltaDeltaG| > 1.0 kcal/mol) on a three-dimensional S4 homology model revealed a spiral pattern. As expected, mutation of these residues also altered activation. However, mutation of residues in the S3-S4 and S4-S5 linkers and the C-terminal end of S4 perturbed activation (|DeltaDeltaG| > 1.0 kcal/mol) without altering charge movement, suggesting that the native residues in these regions couple S4 movement to the opening of the activation gate or stabilize the open or closed state of the channel. Finally, mutation of a distinct set of residues impacted inactivation and mapped to a single face of the S4 helix that was devoid of activation-perturbing residues. These results define regions on the S4 voltage sensor that contribute differentially to hERG activation and inactivation gating.

Alternative splicing in the voltage-sensing region of N-Type CaV2.2 channels modulates channel kinetics.

The CaV2.2 gene encodes the functional core of the N-type calcium channel. This gene has the potential to generate thousands of CaV2.2 splice isoforms with different properties. However, the functional significance of most sites of alternative splicing is not established. The IVS3-IVS4 region contains an alternative splice site that is conserved evolutionarily among CaValpha1 genes from Drosophila to human. In CaV2.2, inclusion of exon 31a in the IVS3-IVS4 region is restricted to the peripheral nervous system, and its inclusion slows the speed of channel activation. To investigate the effects of exon 31a in more detail, we generated four tsA201 cell lines stably expressing CaV2.2 splice isoforms. Coexpression of auxiliary CaVbeta and CaValpha2delta subunits was required to reconstitute currents with the kinetics of N-type channels from neurons. Channels including exon 31a activated and deactivated more slowly at all voltages. Current densities were high enough in the stable cell lines co-expressing CaValpha2delta to resolve gating currents. The steady-state voltage dependence of charge movement was not consistently different between splice isoforms, but on gating currents from the exon 31a-containing CaV2.2 isoform decayed with a slower time course, corresponding to slower movement of the charge sensor. Exon 31a-containing CaV2.2 is restricted to peripheral ganglia; and the slower gating kinetics of CaV2.2 splice isoforms containing exon 31a correlated reasonably well with the properties of native N-type currents in sympathetic neurons. Our results suggest that alternative splicing in the S3-S4 linker influences the kinetics but not the voltage dependence of N-type channel gating.

Modulation of the voltage sensor of L-type Ca2+ channels by intracellular Ca2+.

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

Membrane cholesterol modulates dihydropyridine receptor function in mice fetal skeletal muscle cells.

Caveolae and transverse (T-) tubules are membrane structures enriched in cholesterol and glycosphingolipids. They play an important role in receptor signalling and myogenesis. The T-system is also highly enriched in dihydropyridine receptors (DHPRs), which control excitation-contraction (E-C) coupling. Recent results have shown that a depletion of membrane cholesterol alters caveolae and T-tubules, yet detailed functional studies of DHPR expression are lacking. Here we studied electrophysiological and morphological effects of methyl-beta-cyclodextrin (MbetaCD), a cholesterol-sequestering drug, on freshly isolated fetal skeletal muscle cells. Exposure of fetal myofibres to 1-3 mM MbetaCD for 1 h at 37 degrees C led to a significant reduction in caveolae and T-tubule areas and to a decrease in cell membrane electrical capacitance. In whole-cell voltage-clamp experiments, the L-type Ca(2+) current amplitude was significantly reduced, and its voltage dependence was shifted approximately 15 mV towards more positive potentials. Activation and inactivation kinetics were slower in treated cells than in control cells and stimulation by a saturating concentration of Bay K 8644 was enhanced. In addition, intramembrane charge movement and Ca(2+) transients evoked by a depolarization were reduced without a shift of the midpoint, indicating a weakening of E-C coupling. In contrast, T-type Ca(2+) current was not affected by MbetaCD treatment. Most of the L-type Ca(2+) conductance reduction and E-C coupling weakening could be explained by a decrease of the number of DHPRs due to the disruption of caveolae and T-tubules. However, the effects on L-type channel gating kinetics suggest that membrane cholesterol content modulates DHPR function. Moreover, the significant shift of the voltage dependence of L-type current without any change in the voltage dependence of charge movement and Ca(2+) transients suggests that cholesterol differentially regulates the two functions of the DHPR.

Transition states of the high-affinity rabbit Na(+)/glucose cotransporter SGLT1 as determined from measurement and analysis of voltage-dependent charge movements.

The charge-membrane voltage (Q-V) distribution of wild-type rabbit Na(+)/glucose transporter (rSGLT1) expressed in Xenopus oocytes was investigated in the absence of glucose, using the two-electrode voltage-clamp technique. Although this distribution is generally believed to be well represented by a two-state Boltzmann equation, we recently provided evidence for the existence of at least four states (Krofchick D and Silverman M. Biophys J 84: 3690-3702, 2003), confirming an earlier finding for human SGLT1 (Chen XZ, Coady MJ, and Lapointe JY. Biophys J 71: 2544-2552, 1996). We now extend our study of rSGLT1 pre-steady-state currents, employing high-resolution measurement and analysis of the Q-V distribution. A ramp, instead of a step, voltage change was used to prevent saturation of the apparatus in the first approximately 1 ms. Transient currents were integrated out to 150 ms, instead of the standard 50-100 ms. Measurements were taken every 10 mV instead of the standard 20 mV. The Q-V distribution was fit with a two-, three-, and four-state Boltzmann equation and was described best by the three-state equation. The three-state fit produced two valences of 0.45 and 1.1 at two V(0.5) values of -48 and -7.7, respectively. Our findings are critically compared with other published studies and the differences are discussed. An implication of the three-state fit is that the turnover rate of rSGLT1 is 34 s(-1), i.e., 54% greater than previously reported (22 s(-1)). Our new findings support the concept that the sugar-free model of SGLT1 is more complex than generally accepted, most likely involving a minimum of four transition states.

Molecular action of lidocaine on the voltage sensors of sodium channels.

Block of sodium ionic current by lidocaine is associated with alteration of the gating charge-voltage (Q-V) relationship characterized by a 38% reduction in maximal gating charge (Qmax) and by the appearance of additional gating charge at negative test potentials. We investigated the molecular basis of the lidocaine-induced reduction in cardiac Na channel–gating charge by sequentially neutralizing basic residues in each of the voltage sensors (S4 segments) in the four domains of the human heart Na channel (hH1a). By determining the relative reduction in the Qmax of each mutant channel modified by lidocaine we identified those S4 segments that contributed to a reduction in gating charge. No interaction of lidocaine was found with the voltage sensors in domains I or II. The largest inhibition of charge movement was found for the S4 of domain III consistent with lidocaine completely inhibiting its movement. Protection experiments with intracellular MTSET (a charged sulfhydryl reagent) in a Na channel with the fourth outermost arginine in the S4 of domain III mutated to a cysteine demonstrated that lidocaine stabilized the S4 in domain III in a depolarized configuration. Lidocaine also partially inhibited movement of the S4 in domain IV, but lidocaine's most dramatic effect was to alter the voltage-dependent charge movement of the S4 in domain IV such that it accounted for the appearance of additional gating charge at potentials near −100 mV. These findings suggest that lidocaine's actions on Na channel gating charge result from allosteric coupling of the binding site(s) of lidocaine to the voltage sensors formed by the S4 segments in domains III and IV.

Effect of S6 Tail Mutations on Charge Movement in Shaker Potassium Channels

The cytoplasmic ends of the four S6 transmembrane segments of voltage-gated potassium channels converge in a bundle crossing that acts as the activation gate that opens in response to a depolarization. To explore whether the cytoplasmic extension of the S6 segment (the S6 tail) plays a role in coupling voltage sensor and activation gate movements, we examined the effect of cysteine substitution from residues N482 to T489 on the kinetics and voltage-dependence of S4 charge movement and on the kinetics of deactivation of ionic current. Among these mutants, F484C has the steepest voltage-dependent charge movement, the largest Q– V shift, and the fastest OFF gating currents. Further study of the residue at position 484, using mutagenesis and modification of F484C by cysteine reagents, suggests that aromaticity at this position is essential to maintain normal coupling. We used periodicity analysis to appraise the possibility that the S6 tail has an α-helical structure. Although we obtained an α-periodicity index of 2.41 for gating current parameters, a new randomization test produced an indecisive conclusion about the secondary structure of this region. Taken together, our results suggest that the tail end of S6 plays an important role in coupling between activation gating and charge movement.

Gating of the expressed Ca v3.1 calcium channel

Intramembrane charge movement originating from Ca v3.1 (T-type) channel expressed in HEK 293 cells was investigated. Ion current was blocked by 1 mM La 3+. Charge movement was detectable for depolarizations above ∼−70 mV and saturated above +60 mV. The voltage dependence of charge movement followed a single Boltzmann function with half-maximal activation voltage +12.9 mV and +12.3 mV and with slopes of 22.4 mV and 18.1 mV for the ON- and OFF-charge movement, respectively. Inactivation of I Ca by prolonged depolarization pulse did not immobilize intramembrane charge movement in the Ca v3.1 channel.

Role of Cl− in Electrogenic Na+-coupled Cotransporters GAT1 and SGLT1

We have investigated the functional role of Cl(-) in the human Na(+)/Cl(-)/gamma-aminobutyric acid (GABA) and Na(+)/glucose cotransporters (GAT1 and SGLT1, respectively) expressed in Xenopus laevis oocytes. Substrate-evoked steady-state inward currents were examined in the presence and absence of external Cl(-). Replacement of Cl(-) by gluconate or 2-(N-morpholino)ethanesulfonic acid decreased the apparent affinity of GAT1 and SGLT1 for Na(+) and the organic substrate. In the absence of substrate, GAT1 and SGLT1 exhibited charge movements that manifested as pre-steady-state current transients. Removal of Cl(-) shifted the voltage dependence of charge movements to more negative potentials, with apparent affinity constants (K(0.5)) for Cl(-) of 21 and 115 mm for SGLT1 and GAT1, respectively. The maximum charge moved and the apparent valence were not altered. GAT1 stoichiometry was determined by measuring GABA-evoked currents and the unidirectional influx of (36)Cl(-), (22)Na(+), or [(3)H]GABA. Uptake of each GABA molecule was accompanied by inward movement of 2 positive charges, which was entirely accounted for by the influx of Na(+) in the presence or absence of Cl(-). Thus, the GAT1 stoichiometry was 2Na(+):1GABA. However, Cl(-) was transported by GAT1 because the inward movement of 2 positive charges was accompanied by the influx of one Cl(-) ion, suggesting unidirectional influx of 2Na(+):1Cl(-):1GABA per transport cycle. Activation of forward Na(+)/Cl(-)/GABA transport evoked (36)Cl(-) efflux and was blocked by the inhibitor SKF 89976A. These data suggest a Cl(-)/Cl(-) exchange mechanism during the GAT1 transport cycle. In contrast, Cl(-) was not transported by SGLT1. Thus, in both GAT1 and SGLT1, Cl(-) modulates the kinetics of cotransport by altering Na(+) affinity, but does not contribute to net charge transported per transport cycle. We conclude that Cl(-) dependence per se is not a useful criterion to classify Na(+) cotransporters.

A new twist in the saga of charge movement in voltage-dependent ion channels.

Despite the many discrepancies in results and the different experimental methods used, both papers arrive at the same conclusion. S4 segments rotate when depolarized, and this rotation moves charged residues from an intracellular vestibule to an extracellular vestibule (Figure 2BFigure 2B). One reason this mechanism is so appealing is that the residues most important for charge transfer, the outermost four charged residues, lie along one face of an α helix. Note that in order for this mechanism to account for charge transfer, the direction of the electric field cannot be oriented parallel to the plane of the membrane, as implied for example by the shaded regions in Figure 1CFigure 1C, but more perpendicular to the membrane (Figure 2BFigure 2B). This reorientation of the electric field is a consequence of the topology of the aqueous vestibules surrounding the S4 segment.One prediction of these models is that the residues on the backside of this stripe of positive charge, i.e., the neutral residues between the charged residues in the primary sequence, should move in the opposite direction, from extracellular to intracellular during a depolarization. This does not occur. The residues between the second and third arginines in the primary sequence are in an intracellular compartment at hyperpolarized voltages (Figure 1CFigure 1C). This does not eliminate the possibility that S4 rotates. It means that the gating pore also undergoes conformational changes as the S4 segment moves. This fact is also apparent from accessibility studies, which suggest that the length of the gating pore changes with depolarization (Figure 1CFigure 1C).What message can we take home about S4 movement? As attractive as it is, the claim for a rotation as large as 180° is weak. Furthermore, even if a smaller rotation contributes to charge movement, it is likely to be only one of the movements of S4 and the protein surrounding it. Perhaps the most important conclusion supported by both studies is that the movements of the S4 segment are very small, as one might expect for a conformational change that has to be fast enough to underlie the gating currents.The raison d'etre of an S4 segment is not charge movement; it is the control of the activation gates at the bottom of the S6 segments. How are these movements coupled? One possibility is that movement of the S4 segment tugs or twists the linkers that connect it to S3 and S5 segments, and these segments transmit this movement to the S6 segment. Another possibility is that S4 and S6 are like entwined lovers. One cannot move without a compensatory rearrangement of the other. For example, S4 rotation may cause S6 rotation, a movement that underlies the gating of a bacterial potassium channel (Perozo et al. 1999xPerozo, E., Cortes, D.M., and Cuello, L.G. Science. 1999; 285: 73–78Crossref | PubMed | Scopus (461)See all ReferencesPerozo et al. 1999). The answers to these mysteries will surely unfold with the next episode of conformational studies of voltage-dependent gating.*E-mail: richard.horn@mail.tju.edu.

Coupling between charge movement and pore opening in vertebrate neuronal alpha 1E calcium channels.

1. Neuronal alpha 1E Ca2+ channels were expressed alone and in combination with the beta 2a subunit in Xenopus laevis oocytes. 2. The properties of ionic and gating currents of alpha 1E were investigated: ionic currents were measured in 10 mM external Ba2+; gating currents were isolated in 2 mM external Co2+. 3. Charge movement preceded channel opening. The charge movement voltage curve (Q(V)) preceded the ionic conductance voltage dependence (G(V)) by approximately 20 mV. 4. Coexpression of alpha 1E with the beta 2a subunit did not modify the voltage dependence of charge movement but shifted the G(V) curve to more negative potentials. The voltage gap between Q(V) and G(V) curves was reduced by the beta 2a subunit and both curves overlapped at potentials near 0 mV. 5. The coupling efficiency between the charge movement and pore opening was estimated by the ration between limiting conductance and maximum charge movement (Gmax/Qmax). Coexpression of the beta 2a subunit increased the Gmax/Qmax ratio from 9.2 x 10(5) +/- 1.4 x 10(5) to 21.9 x 10(5) +/- 2.8 X 10(5) S C-1 for alpha 1E and alpha 1E + beta 2a, respectively. 6. We conclude that in the neuronal alpha 1E the charge movement is tightly coupled with the pore opening and that the beta 2a subunit coexpression further improves this coupling.

Motility voltage sensor of the outer hair cell resides within the lateral plasma membrane.

The outer hair cell (OHC) from the organ of Corti is believed to be responsible for the mammal's exquisite sense of hearing. A membrane-based motile response of this cell underlies the initial processing of acoustic energy. The voltage-dependent capacitance of the OHC, possibly reflecting charge movement of the motility voltage sensor, was measured in cells during intracellular dialysis of trypsin under whole cell voltage clamp. Within 10 min after dialysis, light and electron microscopic examination revealed that the subplasmalemmal structures, including the cytoskeletal framework and subsurface cisternae, were disrupted and/or detached from adjacent plasma membrane. Dialysis of heat-inactivated trypsin produced no changes in cell structure. Simultaneous measures of linear and nonlinear membrane capacitance revealed minimal changes, indicating that contributions by subsurface structures to the generation of the nonlinear capacitance are unlikely. This study strongly suggests that voltage-dependent charge movement in the OHC reflects properties of the force generator's voltage sensor and that the sensor/motor resides solely within the lateral plasma membrane.

Charge inactivation in the membrane of intact frog striated muscle fibers.

1. Charge movements were compared in normally polarized and depolarized intact frog muscle fibres under voltage clamp. 2. The membrane capacitance was linear through positive control steps made consistently from a holding voltage of -10 mV, in agreement with earlier reports from cut fibres. 3. A shift in holding voltage from -90 to -10 mV reduced both the absolute amount and the voltage dependence of charge movement elicited by voltage steps imposed from a fixed conditioning voltage of -180 mV. The charge transferred by steps from -180 to -20 mV was 43.8 +/- 1.14 nC/microF in fully polarized fibres and 21.7 +/- 1.49 nC/microF in the same depolarized fibres (means +/- S.E. of the mean; four fibres). 4. Charge movement in response to steps from -90 to -20 mV increased from 10.4 +/- 1.60 nC/microF to 28.4 +/- 2.42 nC/microF (five fibres) within 30s of changing the holding voltage from -10 to -90 mV. 5. The same fibres also showed significant charge movement between voltages of -180 and -90 mV. However, shifts in holding voltage did not significantly alter the maximum value of this charge, around 10-11 nC/microF. 6. Membrane capacitance as measured by small steps to a voltage of -90 mV remained constant despite holding potential changes, or lidocaine (10 mM) treatment. 7. The same results were obtained whether the above procedures were applied to fibres exposed to normal extracellular [Ca2+], or in Ca(2+)-free media. In both cases tubular cable corrections did not affect the results. 8. These findings suggest independent charge I and charge II systems in which inactivation of charge I is not associated with its interconversion into charge II.

Reversible inhibition of voltage-dependent outer hair cell motility and capacitance

Outer hair cells (OHC) from the organ of Corti are capable of fast voltage-induced length changes (Santos-Sacchi and Dilger, 1988), suggesting that an associated voltage sensor should reside in the OHC plasma membrane. Voltage-dependent mechanical responses and nonlinear charge movement of isolated OHCs from the guinea pig were analyzed using the whole-cell voltage-clamp technique. Ionic currents in the cells were blocked. Nonlinear voltage-dependent charge movement or, correspondingly, voltage-dependent capacitance was measured with step or AC analysis. OHC movements were measured either from video or using a differential photodiode technique. Maximum charge movements up to 2.5 pC were measured in OHCs from the low-frequency region of the cochlea. Both AC and step analyses indicated a peak nonlinear capacitance of 16-17 pF. The voltage dependence was fit to a Boltzmann relation with the step analysis indicating a maximum nonlinear capacitance at -23 mV step potential from a holding potential of about -120 mV, and AC analysis indicating a maximum at a holding potential near -40 mV. AC analysis probably provides a more accurate evaluation of voltage dependence. Measures of OHC motility magnitude versus voltage follow the nonlinear capacitance-voltage function obtained from AC measures. Treatment of the cells with gadolinium ions (0.5-1 mM) blocked OHC motility. This treatment also produced a shift of the nonlinear capacitance function along the voltage axis in the depolarizing direction, which can be explained by membrane surface charge screening. However, maximum capacitance was reduced as well and may correspond to the reduction or abolition of OHC motility in response to gadolinium treatment. Gadolinium effects were reversible. Nonlinear capacitance is not a function of membrane deformation due to length changes, since removal of OHC cytosol via the patch pipette abolished longitudinal movement but did not reduce nonlinear charge movement. It is interesting to note that the nonlinear capacitance will dynamically influence the time constant of the OHC during acoustically evoked receptor potential generation.

Nonlinear voltage-dependent capacitance of the outer hair cell (OHC) membrane

Nonlinear, voltage-dependent charge movement within the OHC plasma membrane, presumably associated with the movement of the motility voltage sensor, was studied by ac and step analyses using the whole cell voltage clamp technique. Ionic currents in the cells were blocked. Qualitatively, the two analyses agree; however, there are some discrepancies. The ac analyses indicate a maximum nonlinear capacitance (about 18 pF) at a holding potential near −40 mV, whereas step analyses indicate a maximum capacitance (about 20 pF) at −17-mV step potential from a holding potential of about −120 mV (p/ − 4 procedure). Measures of OHC motility magnitude versus voltage indicate that half-maximal response occurs at about − 40 mV, and follows the ac nonlinear capacitance function. It is possible that step analyses may be adversely affected by the series resistance of the whole cell patch pipette. Gadolinium ion treatment (0.5 to 1 mM) produces some membrane surface charge screening; however, maximum capacitance was reduced as well, and may correspond to the simultaneous reduction or abolition of OHC motility. It is interesting to note that the nonlinear capcitance associated with the movement of the OHC motility voltage sensor will dynamically influence the time constant of the OHC during acoustic stimulation. [Work supported by an RCDA from NIDCD and NIH grant DC00273.]

The effects of tetracaine on charge movement in fast twitch rat skeletal muscle fibres.

1. The effects of tetracaine, a local anaesthetic that inhibits muscle contraction, on membrane potential and intramembrane charge movements were investigated in fast twitch rat muscle fibres (extensor digitorum longus). 2. The resting membrane potentials of surface fibres from muscles bathed in isotonic Ringer solution containing 2 mM-tetracaine were well maintained, but higher concentrations of tetracaine caused a time-dependent fall of potential. Muscle fibres bathed in hypertonic solutions containing 2 mM-tetracaine were rapidly depolarized. In both isotonic and hypertonic solutions, the depolarizing effect of tetracaine could not be reversed. 3. Charge movement measurements were made using the middle-of-the-fibre voltage clamp technique. The voltage dependence of charge movements measured in cold isotonic solutions was well fitted by a Boltzmann distribution (Q(V) = Qmax/(1 + exp(-(V-V)/k] where Qmax = 37.3 +/- 2.8 nC muF-1, V = -17.9 +/- 1.2 mV and k = 12.6 +/- 0.8 mV (n = 6, 2 degrees C; means +/- S.E. of means). Similar values were obtained when 2 mM-tetracaine was added to the isotonic bathing fluid (Qmax = 40.6 +/- 2.3 nC microF-1, V = -14.1 +/- 1.3 mV, k = 15.3 +/- 0.8 mV; n = 8, 2 degrees C). 4. Charge movements measured around mechanical threshold in muscle fibres bathed in hypertonic solutions were reduced when 2 mM-tetracaine was added to the bathing fluid. The tetracaine-sensitive component of charge was well fitted with an unconstrained Boltzmann distribution which gave: Qmax = 7.5 nC microF-1, V = -46.5 mV, k = 5.5 mV. The e-fold rise of the foot of the curve was 9.3 mV.

Effect of postnatal development on calcium currents and slow charge movement in mammalian skeletal muscle.

Single- (whole-cell patch) and two-electrode voltage-clamp techniques were used to measure transient (Ifast) and sustained (Islow) calcium currents, linear capacitance, and slow, voltage-dependent charge movements in freshly dissociated fibers of the flexor digitorum brevis (FDB) muscle of rats of various postnatal ages. Peak Ifast was largest in FDB fibers of neonatal (1-5 d) rats, having a magnitude in 10 mM external Ca of 1.4 +/- 0.9 pA/pF (mean +/- SD; current normalized by linear fiber capacitance). Peak Ifast was smaller in FDB fibers of older animals, and by approximately 3 wk postnatal, it was so small as to be unmeasurable. By contrast, the magnitudes of Islow and charge movement increased substantially during postnatal development. Peak Islow was 3.6 +/- 2.5 pA/pF in FDB fibers of 1-5-d rats and increased to 16.4 +/- 6.5 pA/pF in 45-50-d-old rats; for these same two age groups, Qmax, the total mobile charge measurable as charge movement, was 6.0 +/- 1.7 and 23.8 +/- 4.0 nC/microF, respectively. As both Islow and charge movement are thought to arise in the transverse-tubular system, linear capacitance normalized by the area of fiber surface was determined as an indirect measure of the membrane area of the t-system relative to that of the fiber surface. This parameter increased from 1.5 +/- 0.2 microF/cm2 in 2-d fibers to 2.9 +/- 0.4 microF/cm2 in 44-d fibers. The increases in peak Islow, Qmax, and normalized linear capacitance all had similar time courses. Although the function of Islow is unknown, the substantial postnatal increase in its magnitude suggests that it plays an important role in the physiology of skeletal muscle.