Hydrophobic interactions as key determinants to the KCa3.1 channel closed configuration. An analysis of KCa3.1 mutants constitutively active in zero Ca2+

In this study we present evidence that residue Val282 in the S6 transmembrane segment of the calcium-activated KCa3.1 channel constitutes a key determinant of channel gating. A Gly scan of the S6 transmembrane segment first revealed that the substitutions A279G and V282G cause the channel to become constitutively active in zero Ca2+. Constitutive activity was not observed when residues extending from Cys276 to Ala286, other than Ala279 and Val282, were substituted to Gly. The accessibility of Cys engineered at Val275 deep in the channel cavity was next investigated for the ion-conducting V275C/V282G mutant and closed V275C channel in zero Ca2+ using Ag+ as probe. These experiments demonstrated that internal Ag+ ions have free access to the channel cavity independently of the channel conducting state, arguing against an activation gate located at the S6 segment C-terminal end. Experiments were also conducted where Val282 was substituted by residues differing in size and/or hydrophobicity. We found a strong correlation between constitutive activity in zero Ca2+ and the hydrophobic energy for side chain burial. Single channel recordings showed finally that constitutive activation in zero Ca2+ is better explained by a model where the channel is locked in a low conducting state with a high open probability rather than resulting from a change in the open/closed energy balance that would favor channel openings to a full conducting state in the absence of Ca2+. We conclude that hydrophobic interactions involving Val282 constitute key determinants to KCa3.1 gating by modulating the ion conducting state of the selectivity filter through an effect on the S6 transmembrane segment.     

Structural and functional characteristics of the cellular reaction of the bladder epithelium in the frog to calcium extraction from the apical and basolateral membranes

Extraction of Ca++ ions from cells of the frog urinary bladder serosa side is followed by an increase in the bladder wall permeability for water and inulin. Ultrastructural changes were observed, such as destruction of cell junctions, swelling of the cell and their organelles, reconstruction of the cytoskeleton elements. The free calcium Ringer solution injected in the bladder lumen does not change the permeability of the wall for water and sodium ions. In this case the cell response to the antidiuretic hormone decreases; the ultrastructure of cells and intercellular junctions is not disturbed; the distribution of intramembrane particles on the P- and E-faces of the apical membrane is normal. The above results indicate that there are qualitative differences in the cell response towards the extraction of Ca++-ions between the serosal and mucosal membranes. This also suggests that on the external surface of the apical membrane Ca++ ions may play a very important role in redistribution of intramembrane particles under the action of the antidiuretic hormone.     

Allosteric linkage between voltage and Ca(2+)-dependent activation of BK-type mslo1 K(+) channels

The activation of BK type Ca(2+)-activated K(+) channels depends on both voltage and Ca(2+). We studied three point mutations in the putative voltage sensor S4 or S4-S5 linker regions in the mslo1 BK channels to explore the relationship between voltage and Ca(2+) in activating the channel. These mutations reduced the steepness of the open probability - voltage (P(o) - V) relation and increased the shift of the P(o) - V relations on the voltage axis in response to increases in the calcium concentration. It is striking that these two effects were reciprocally related for all three mutations, despite different effects of the mutations on other aspects of the voltage dependence of channel gating. This reciprocal relationship suggests strongly that the free energy contributions to channel activation provided by voltage and by calcium binding are simply additive. We conclude that the Ca(2+) binding sites and the voltage sensors do not directly interact. Rather they both affect the mslo1 channel opening through an allosteric mechanism, by influencing the conformational change between the closed and open conformations. The mutations changed the channel's voltage dependence with little effect on its Ca(2+) affinitiy.     

Tuning the mechanosensitivity of a BK channel by changing the linker length

Some large-conductance Ca(2+) and voltage-activated K(+)(BK) channels are activated by membrane stretch. However, the mechanism of mechano-gating of the BK channels is still not well understood. Previous studies have led to the proposal that the linker-gating ring complex functions as a passive spring, transducing the force generated by intracellular Ca(2+) to the gate to open the channel. This raises the question as to whether membrane stretch is also transmitted to the gate of mechanosensitive (MS) BK channels via the linker-gating complex. To study this, we changed the linker length in the stretch-activated BK channel (SAKCaC), and examined the effect of membrane stretch on the gating of the resultant mutant channels. Shortening the linker increased, whereas extending the linker reduced, the channel mechanosensitivity both in the presence and in the absence of intracellular Ca(2+). However, the voltage and Ca(2+) sensitivities were not significantly altered by membrane stretch. Furthermore, the SAKCaC became less sensitive to membrane stretch at relatively high intracellular Ca(2+) concentrations or membrane depolarization. These observations suggest that once the channel is in the open-state conformation, tension on the spring is partially released and membrane stretch is less effective. Our results are consistent with the idea that membrane stretch is transferred to the gate via the linker-gating ring complex of the MS BK channels.     

The NH2 terminus of RCK1 domain regulates Ca2+-dependent BK(Ca) channel gating

Large conductance, voltage- and Ca2+-activated K+ (BK(Ca)) channels regulate blood vessel tone, synaptic transmission, and hearing owing to dual activation by membrane depolarization and intracellular Ca2+. Similar to an archeon Ca2+-activated K+ channel, MthK, each of four alpha subunits of BK(Ca) may contain two cytosolic RCK domains and eight of which may form a gating ring. The structure of the MthK channel suggests that the RCK domains reorient with one another upon Ca2+ binding to change the gating ring conformation and open the activation gate. Here we report that the conformational changes of the NH2 terminus of RCK1 (AC region) modulate BK(Ca) gating. Such modulation depends on Ca2+ occupancy and activation states, but is not directly related to the Ca2+ binding sites. These results demonstrate that AC region is important in the allosteric coupling between Ca2+ binding and channel opening. Thus, the conformational changes of the AC region within each RCK domain is likely to be an important step in addition to the reorientation of RCK domains leading to the opening of the BK(Ca) activation gate. Our observations are consistent with a mechanism for Ca2+-dependent activation of BK(Ca) channels such that the AC region inhibits channel activation when the channel is at the closed state in the absence of Ca2+; Ca2+ binding and depolarization relieve this inhibition.     

Extracellular Ba2+ and voltage interact to gate Ca2+ channels at the plasma membrane of stomatal guard cells

Ca2+ channels at the plasma membrane of stomatal guard cells contribute to increases in cytosolic free [Ca2+] ([Ca2+](i)) that regulate K+ and Cl- channels for stomatal closure in higher-plant leaves. Under voltage clamp, the initial rate of increase in [Ca2+](i) in guard cells is sensitive to the extracellular divalent concentration, suggesting a close interaction between the permeant ion and channel gating. To test this idea, we recorded single-channel currents across the Vicia guard cell plasma membrane using Ba2+ as a charge carrying ion. Unlike other Ca2+ channels characterised to date, these channels activate at hyperpolarising voltages. We found that the open probability (P(o)) increased strongly with external Ba2+ concentration, consistent with a 4-fold cooperative action of Ba2+ in which its binding promoted channel opening in the steady state. Dwell time analyses indicated the presence of a single open state and at least three closed states of the channel, and showed that both hyperpolarising voltage and external Ba2+ concentration prolonged channel residence in the open state. Remarkably, increasing Ba2+ concentration also enhanced the sensitivity of the open channel to membrane voltage. We propose that Ba2+ binds at external sites distinct from the permeation pathway and that divalent binding directly influences the voltage gate.     

"Calcium antagonists": a class of drugs with a bright future. Part I. Cellular calcium homeostasis and calcium as a coupling messenger

The aim of this series of minireviews is to present material from multidisciplinary sources to facilitate the understanding of the pharmacology and the ample clinical potential of a class of drugs that were originally designated as "calcium antagonists" and more recently have been referred to as "calcium entry blockers", "calcium slow channel blockers" or "calcium modulators". In this first report our attention will be focussed on the pivotal role of Ca++ as a messenger linking stimuli of extracellular origin to the intracellular environment. Eucaryotic cells have a number of powerful means to control their cytosolic Ca++ concentration. Firstly, in a cell at rest the cellular membrane is relatively impermeable to passive Ca++ movements. This property of the plasmalemma prevents the high free Ca++ concentration (approximately 1 mM) of the extracellular compartment from invading the cytosol (approximately 0.1 microM). However, extracellular Ca++ can reach the cytosol through the Na+/Ca++ exchange mechanism and the plasmalemma possesses special Ca++ channels the conductance of which is controlled by gates that are opened by critical changes in cellular polarization (voltage-operated channels: VOC) or by receptor activation (receptor-operated channel: ROC). The Ca++ entering via VOC or ROC can subsequently trigger the liberation of Ca++ from the sarcoplasmic reticulum or from calcium stores located in the inner side of the plasmalemma. The intracellular message generated by external stimuli is transferred to the response mechanism by several cytosolic proteins that require Ca++ as activator. Finally, the termination of the response is the result of a reduction in the cytosolic Ca++ concentration that is accomplished by the Na+/Ca++ exchange mechanism or by energy-dependent pumps which extrude Ca++ from the cell or store it in subcellular organelles. Therefore, any of the numerous steps of the excitation-response coupling which employ Ca++ as a messenger or as a protein activator can be the site of action of a pharmacological agent. In the follow-up minireview, some methods to determine the basic pharmacological profile of compounds interfering with cellular Ca++-dependent functions will be described.     

Ion flow through biomembranes. Physical theory explains its high sensitivity.

Numerous biomembranes exhibit a sensitivity to changes in electrical potential greater than predicted as possible from the classical application of the Boltzmann relation, a phenomenon which has long defied explanation, the actual sensitivity of some Na+ channels being many times greater than the classical limit. This paper explains, using a minimum of mathematics, how the very rapid gating effect of adsorbed Ca2+ (or other impermeable divalent cations) can directly affect the conductance of channels, and thus interact with the electric field within the channel to produce a change in the potential across the channel's gate much greater than the change in the membrane potential, with a corresponding change in the fraction of open conformational gates and change in conductance. These results are not in conflict with the Boltzmann relation, the necessary energy being made available from the total potential difference across the membrane by a long unrecognized stochastic process; the full mathematical theory is given in cited references.     

Gap junction channel gating

Over the last two decades, the view of gap junction (GJ) channel gating has changed from one with GJs having a single transjunctional voltage-sensitive (V(j)-sensitive) gating mechanism to one with each hemichannel of a formed GJ channel, as well as unapposed hemichannels, containing two, molecularly distinct gating mechanisms. These mechanisms are termed fast gating and slow or 'loop' gating. It appears that the fast gating mechanism is solely sensitive to V(j) and induces fast gating transitions between the open state and a particular substate, termed the residual conductance state. The slow gating mechanism is also sensitive to V(j), but there is evidence that this gate may mediate gating by transmembrane voltage (V(m)), intracellular Ca(2+) and pH, chemical uncouplers and GJ channel opening during de novo channel formation. A distinguishing feature of the slow gate is that the gating transitions appear to be slow, consisting of a series of transient substates en route to opening and closing. Published reports suggest that both sensorial and gating elements of the fast gating mechanism are formed by transmembrane and cytoplamic components of connexins among which the N terminus is most essential and which determines gating polarity. We propose that the gating element of the slow gating mechanism is located closer to the central region of the channel pore and serves as a 'common' gate linked to several sensing elements that are responsive to different factors and located in different regions of the channel.     

Laser-induced spreading arrest of Mytilus gill cilia

Using a "slit camera" recording technique, we have examined the effects of local laser irradiation of cilia of the gill epithelium of Mytilus edulis. The laser produces a lesion which interrupts epithelial integrity. In artificial sea water that contains high K+ or is effectively Ca++ free, metachronism of the lateral cilia continues to either side of the lesion with only minor perturbations in frequency synchronization and wave velocity, such as would be expected if metachronal wave coordination is mechanical. However, in normal sea water and other appropriate ionic conditions (i.e., where Ca++ concentration is elevated), in addition to local damage, the laser induces distinct arrest responses of the lateral cilia. Arrest is not mechanically coordinated, since cilia stop in sequence depending on stroke position as well as distance from the lesion. The velocity of arrest under standard conditions is about 3 mm/s, several orders of magnitude faster than spreading velocities associated with diffusion of materials from the injured region. Two responses can be distinguished on the basis of the kinetics of recovery of the arrested regions. These are (a) a nondecremental response that resembles spontaneous ciliary stoppage in the gills, and (b) a decremental response, where arrest nearer the stimulus point is much longer lasting. The slower recovery is often periodic, with a step size approximating lateral cell length. Arrest responses with altered kinetics also occur in laterofrontal cilia. The responses of Mytilus lateral cilia resemble the spreading ciliary arrest seen in Elliptio and arrest induced by electrical and other stimuli, and the decremental response may depend upon electrotonic spread of potential change produced at the stimulus site. If this were coupled to transient changes in Ca++ permeability of the cell membrane, a local rise in Ca++ concentration might inhibit ciliary beat at a sensitive point in the stroke cycle to produce the observed arrest.     

Effects of intracellular K+ and Rb+ on gating of embryonic rat telencephalon Ca(2+)-activated K+ channels.

We have investigated the effects of intracellular K+ and Rb+ on single-channel currents recorded from the large-conductance Ca(2+)-activated K+ (BK) channel of the embryonic rat telencephalon using the inside-out patch-clamp technique. Our novel observation concerns the effects of these ions on rapid flickering of channel openings. Specifically, flicker gating was voltage dependent, i.e., it was reduced by depolarization in the -60 to -10 mV range with equimolar concentrations of K+ ions (150 Ko+/150 Ki+). Removal of Ki+ resulted in significant flickering at all potentials in this voltage range. In other words, the voltage dependence of flicker gating was effectively eliminated by the removal of Ki+. This suggests that a K+ ion entering the channel from the intracellular medium binds, in a voltage-dependent manner, at a site that locks the flicker gate in its open position. No effects of changes in Ki+ were observed on the primary, voltage-dependent gate of the channel. The change in flickering did not cause a change in the mean burst duration, which indicates that the primary gate is stochastically independent of the flicker gate. Intracellular Rb+ can substitute for--and is even more effective than--Ki+ with regard to suppression of flickering. Substitution of Rbi+ for Ki+ also increased the mean burst duration for V > or = -30 mV. Both effects of Rbi+ were removed by membrane hyperpolarization.     

Hydrostatic pressures developed by osmotically swelling vesicles bound to planar membranes

When phospholipid vesicles bound to a planar membrane are osmotically swollen, they develop a hydrostatic pressure (delta P) and fuse with the membrane. We have calculated the steady-state delta P, from the equations of irreversible thermodynamics governing water and solute flows, for two general methods of osmotic swelling. In the first method, vesicles are swollen by adding a solute to the vesicle-containing compartment to make it hyperosmotic. delta P is determined by the vesicle membrane's permeabilities to solute and water. If the vesicle membrane is devoid of open channels, then delta P is zero. When the vesicle membrane contains open channels, then delta P peaks at a channel density unique to the solute permeability properties of both the channel and the membrane. The solute enters the vesicle through the channels but leaks out through the region of vesicle-planar membrane contact. delta P is largest for channels having high permeabilities to the solute and for solutes with low membrane permeabilities in the contact region. The model predicts the following order of solutes producing pressures of decreasing magnitude: KCl greater than urea greater than formamide greater than or equal to ethylene glycol. Differences between osmoticants quantitatively depend on the solute permeability of the channel and the density of channels in the vesicle membrane. The order of effectiveness is the same as that experimentally observed for solutes promoting fusion. Therefore, delta P drives fusion. When channels with small permeabilities are used, coupling between solute and water flows within the channel has a significant effect on delta P. In the second method, an impermeant solute bathing the vesicles is isosmotically replaced by a solute which permeates the channels in the vesicle membrane. delta P resulting from this method is much less sensitive to the permeabilities of the channel and membrane to the solute. delta P approaches the theoretical limit set by the concentration of the impermeant solute.     

Rapid increases in inositol trisphosphate and intracellular Ca++ after heat shock

Heat shock (45 degrees C) caused a rapid (less than 1 min) release of inositol trisphosphate from the membranes of HA-1 CHO fibroblasts. The rise in inositol trisphosphate concentration was followed by an increase in intracellular free Ca++. In addition to the heat induced rise in intracellular free Ca++, we observed an increase in 45Ca++ influx following nonlethal heat shock (45 degrees C/10 min). The heat-induced increase in 45Ca++ influx was linearly related to membrane accumulation of phosphatidic acid, phosphoinositide metabolite that may be involved in Ca++ gating. These results suggest that the membrane may be the proximal target of heat shock; stimulation of rapid breakdown of polyphosphoinositides and subsequent increases in intracellular free Ca++ may provide a mechanistic insight into the pleiotropic effects of heat. In addition, the large increases in Ca++ influx could initiate a Ca++ dependent mechanism of thermal cell killing.     

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.     

Stabilizing the closed S6 gate in the Shaker Kv channel through modification of a hydrophobic seal

The primary activation gate in K+ channels is thought to reside near the intracellular entrance to the ion conduction pore. In a previous study of the S6 activation gate in Shaker (Hackos et al., 2002), we found that mutation of V478 to W results in a channel that cannot conduct ions even though the voltage sensors are competent to translocate gating charge in response to membrane depolarization. In the present study we explore the mechanism underlying the nonconducting phenotype in V478W and compare it to that of W434F, a mutation located in an extracellular region of the pore that is nonconducting because the channel is predominantly found in an inactivated state. We began by examining whether the intracellular gate moves using probes that interact with the intracellular pore and by studying the inactivation properties of heterodimeric channels that are competent to conduct ions. The results of these experiments support distinct mechanisms underlying nonconduction in W434F and V478W, suggesting that the gate in V478W either remains closed, or that the mutation has created a large barrier to ion permeation in the open state. Single channel recordings for heterodimeric and double mutant constructs in which ion conduction is rescued suggest that the V478W mutation does not dramatically alter unitary conductance. Taken together, our results suggest that the V478W mutation causes a profound shift of the closed to open equilibrium toward the closed state. This mechanism is discussed in the context of the structure of this critical region in K+ channels.     

Properties of the FhuA channel in the Escherichia coli outer membrane after deletion of FhuA portions within and outside the predicted gating loop.

Escherichia coli transports Fe3+ as a ferrichrome complex through the outer membrane in an energy-dependent process mediated by the FhuA protein. A FhuA deletion derivative lacking residues 322 to 355 (FhuA delta322-355) forms a permanently open channel through which ferrichrome diffused. This finding led to the concept that the FhuA protein forms a closed channel that is opened by input of energy derived from the electrochemical potential across the cytoplasmic membrane, mediated by the Ton system. In this study, we constructed various FhuA derivatives containing deletions inside and outside the gating loop. FhuA delta322-336 bound ferrichrome and displayed a residual Ton-dependent ferrichrome transport activity. FhuA delta335-355 no longer bound ferrichrome but supported ferrichrome diffusion through the outer membrane in the absence of the Ton system. FhuA delta335-355 rendered cells sensitive to sodium dodecyl sulfate and supported diffusion of maltotetraose and maltopentaose in a lamB mutant lacking the maltodextrin-specific channel in the outer membrane. Cells expressing FhuA delta70-223, which has a large deletion outside the gating loop, were highly sensitive to sodium dodecyl sulfate and grew on maltodextrins but showed only weak ferrichrome uptake, suggesting formation of a nonspecific pore through the outer membrane. FhuA delta457-479 supported Ton-dependent uptake of ferrichrome. None of these FhuA deletion derivatives formed pores in black lipid membranes with a stable single-channel conductance. Rather, the conductance displayed a high degree of current noise, indicating a substantial influence of the deletions on the conformation of the FhuA protein. FhuA also supports infection by the phages T1, T5, and phi80 and renders cells sensitive to albomycin and colicin M. Cells expressing FhuA delta322-336 were sensitive to albomycin and colicin M but were only weakly sensitive to T5 and phi480 and insensitive to T1. Cells expressing FhuA delta335-355 were resistant to all FhuA ligands. These results indicate different structural requirements within the gating loop for the various FhuA ligands. Cells expressing FhuA delta457-479 displayed a strongly reduced sensitivity to all FhuA ligands, while cells expressing FhuA delta70-223 were rather sensitive to all FhuA ligands except albomycin, to which they were nearly resistant. It is concluded that residues 335 to 355 mainly determine the properties of the gate with regard to FhuA permeability and ligand binding.     

Parathyroid hormone secretion in the absence of extracellular free Ca2+ and transmembrane Ca2+ influx

The involvement of extracellular Ca2+ and Ca2+ influx across the plasma membrane in parathyroid hormone (PTH) secretion was investigated in vitro using a new preparation of bovine parathyroid cells. Incubation of these cells in the presence of 25 microM or 2.5 microM free ambient Ca2+ induced a maximal rate of PTH secretion. Low free Ca2+ secretion is not associated with changes in membrane permeability, requires metabolic energy, and is reversible. The Ca2+ channel blocker D600 had no effect on either 45Ca-influx or PTH secretion in these cells. These results, showing that extracellular Ca2+ and Ca2+ influx across the plasma membrane are not required for PTH secretion by parathyroid cells, emphasize the differences in the cellular mechanisms underlying the secretion of PTH vs that of other secretory cells.     

Control of mitochondrial Mg++-efflux]

Inorganic phosphate stimulates the release of Mg++ from liver mitochondria, depending on concentration; a concentration as low as 0.1 mM phosphate is already effective. The process is dependent on the electron transfer of the respiratory chain, and its rate is highest under conditions of endogenous respiration and with ascorbate and TMPD as substrates, respectively. The phosphate stimulated release of Mg++ is followed, with a pronounced delay, by a Ca++ efflux and a swelling of mitochondria. Addition of EGTA strongly reduced the rate of Mg++ liberation in the presence and absence of inorganic phosphate. Exogenous Ca++ is able to abolish the EGTA effect. ADP and ATP inhibit the phosphate stimulated release of Mg++. Phosphoenol pyruvate and free fatty acids enhance the rate of Mg++ and Ca++ efflux from the mitochondria. The results permit the conclusion that inorganic phosphate, Ca++ and various metabolites of the cell metabolism influence the Mg++ distribution between the extra- and intramitochondrial space, thus controlling the permeability of the mitochondrial inner membrane for monovalent cations.     

Electrical nature of the taxis signal in cyanobacteria

Electrical events after a light-dark stimulus were studied in the multicellular organism Phormidium uncinatum. Normally, such a stimulus causes the gliding trichome to reverse direction. By directing a large light spot on the end of a batch of trichomes and then switching it off, we achieved synchronization of the trichomes, since the "head" is much more sensitive than the "tail." The abrupt disappearance of a uniform light produced a depolarization wave which initiated at the head, as registered by externally applied electrodes. The second stimulus produced a depolarization of the opposite direction, reflecting the reorientation of the trichomes. No electrical response was observed at Ca2+ concentrations less than or equal to 10(-8) M. Factors causing oscillatory reversals, i.e., a combination of Ca2+ and A23187, or a viscous environment also abolished the electrical signal. Changes in an externally applied electrical field (4 V/cm2) had little effect on the motile behavior of P. uncinatum or Oscillatoria princeps. However, in the presence of 5 microM Ca2+-1 microM A23187, all the trichomes reversed synchronously to the anode after a change in polarity of an externally applied electrical field. We suggest that an increased Ca2+ concentration together with a change in delta psi (or delta mu H+) represents the taxis signal in cyanobacteria.     

Permeable ions differentially affect gating kinetics and unitary conductance of L-type calcium channels

Although ion permeation and gating of L-type Ca(2+) channels are generally considered separate processes controlled by distinct components of the channel protein, ion selectivity can vary with the kinetic state. To test this possibility, we studied single-channel currents (cell-attached) of recombinant L-type channels (Ca(V)1.2, beta(2a), and alpha(2)delta) transiently expressed in tsA201 cells in the presence of the channel agonist BayK 8644 which promotes long channel openings (Mode 2 openings). We found that both the brief (Mode 1) and long (Mode 2) mean open times in the presence of Ca(2+) were relatively longer than those with Ba(2+). The unitary slope conductance with Ba(2+) was significantly larger (p<0.05) in Mode 2 openings than for brief Mode 1 openings, whereas the conductance with Ca(2+) did not vary with mode gating. Consequently, the gamma(Ba):gamma(Ca) ratio was greater for Mode 2 than Mode 1 openings. Our findings indicate that both ion permeation and gating kinetics of the L-type channel are differentially modulated by permeable ions. Ca(2+) binding to the L-type channel may stabilize the alteration of channel ion permeability mediated by gating kinetics, and thus, play a role in preventing excessive ion entry when the activation gating of the channel is promoted to the prolonged open state.