John V. Walsh

Direct regulation of ion channels by fatty acids

A variety of fatty acids regulate the activity of specific ion channels by mechanisms not involving the enzymatic pathways that convert arachidonic acid to oxygenated metabolites. Furthermore, these actions of fatty acids occur in patches of membrane excised from the cell and are not mediated by cellular signal transduction pathways that require soluble factors such as nucleotides and calcium. Thus, fatty acids themselves appear to regulate the action of channels directly, much as they regulate the action of several purified enzymes, and might constitute a new class of first or second messengers acting on ion channels.

Both membrane stretch and fatty acids directly activate large conductance Ca2+-activated K+ channels in vascular smooth muscle cells

Large conductance Ca2+‐activated K+ channels in rabbit pulmonary artery smooth muscle cells are activated by membrane stretch and by arachidonic acid and other fatty acids. Activation by stretch appears to occur by a direct effect of stretch on the channel itself or a closely associated component. In excised inside‐out patches stretch activation was seen under conditions which precluded possible mechanisms involving cytosolic factors, release of Ca2+ from intracellular stores, or stretch induced transmembrane flux of Ca2+ or other ions potentially capable or activating the channel, Fatty acids also directly activate this channel. Like stretch activation, fatty acid activation occurs in excised inside‐out patches in the absence of cytosolic constituents. Moreover, the channel is activated by fatty acids which, unlike arachidonic acid, are not substrates for the cyclo‐oxygenase or lypoxygenase pathways, indicating that oxygenated metabolites do not mediate the response. Thus, four distinct types of stimuli (cytosolic Ca2+, membrane potential, membrane stretch, and fatty acids) can directly affect the activity of this channel.

Stretch-activated ion channels in smooth muscle: a mechanism for the initiation of stretch-induced contraction

As in many smooth muscle tissue preparations, single smooth muscle cells freshly dissociated from the stomach of the toadBufo marinus contract when stretched. Stretch-activated channels have been identified in these cells using patch-clamp techniques. In both cell-attached and excised inside-out patches, the probability of the channel being open (Po) increases when the membrane is stretched by applying negative pressure to the extracellular surface through the patch pipette. The increase inPo is mainly due to a decrease in closed time durations, but an increase in open time duration is also seen. The open-channel current-voltage relationship shows inward rectification and is not appreciably altered when K+ is substituted for Na+ as the charge-carrying cation in Ca2+-free (2 mM EGTA) pipette solutions bathing the extracellular surface of the patch. The inclusion of physiological concentrations of Ca2+ (1.8 mM) in pipette solutions (containing high concentrations of Na+ and low K+) significantly decreases the slope conductance as well as the unitary amplitude. The channel also conducts Ca2+, since inward currents were observed using pipette solutions in which Ca2+ ions were the only inorganic cations. When simulating normal physiological conditions, we find that substantial ionic current is conducted into the cell when the channel is open. These characteristics coupled with the high density of the stretch-activated channels point to a key role for them in the initiation of stretch-induced contraction.

Ca2+ sparks activate K+ and Cl− channels, resulting in spontaneous transient currents in guinea‐pig tracheal myocytes

1 Local changes in cytosolic [Ca2+] were imaged with a wide‐field, high‐speed, digital imaging system while membrane currents were simultaneously recorded using whole‐cell, perforated patch recording in freshly dissociated guinea‐pig tracheal myocytes. 2 Depending on membrane potential, Ca2+ sparks triggered ‘spontaneous’ transient inward currents (STICs), ‘spontaneous’ transient outward currents (STOCs) and biphasic currents in which the outward phase always preceded the inward (STOICs). The outward currents resulted from the opening of large‐conductance Ca2+‐activated K+ (BK) channels and the inward currents from Ca2+‐activated Cl− (ClCa) channels. 3 A single Ca2+ spark elicited both phases of a STOIC, and sparks originating from the same site triggered STOCs, STICs and STOICs, depending on membrane potential. 4 STOCs had a shorter time to peak (TTP) than Ca2+ sparks and a much shorter half‐time of decay. In contrast, STICs had a somewhat longer TTP than sparks but the same half‐time of decay. Thus, the STIC, not the STOC, more closely reflected the time course of cytosolic Ca2+ elevation during a Ca2+ spark. 5 These findings suggest that ClCa channels and BK channels may be organized spatially in quite different ways in relation to points of Ca2+ release from intracellular Ca2+ stores. The results also suggest that Ca2+ sparks may have functions in smooth muscle not previously suggested, such as a stabilizing effect on membrane potential and hence on the contractile state of the cell, or as activators of voltage‐gated Ca2+ channels due to depolarization mediated by STICs.

Spontaneous Transient Outward Currents Arise from Microdomains Where BK Channels Are Exposed to a Mean Ca2+ Concentration on the Order of 10 μM during a Ca2+ Spark

Ca2+ sparks are small, localized cytosolic Ca2+ transients due to Ca2+ release from sarcoplasmic reticulum through ryanodine receptors. In smooth muscle, Ca2+ sparks activate large conductance Ca2+-activated K+ channels (BK channels) in the spark microdomain, thus generating spontaneous transient outward currents (STOCs). The purpose of the present study is to determine experimentally the level of Ca2+ to which the BK channels are exposed during a spark. Using tight seal, whole-cell recording, we have analyzed the voltage-dependence of the STOC conductance (g(STOC)), and compared it to the voltage-dependence of BK channel activation in excised patches in the presence of different [Ca2+]s. The Ca2+ sparks did not change in amplitude over the range of potentials of interest. In contrast, the magnitude of g(STOC) remained roughly constant from 20 to −40 mV and then declined steeply at more negative potentials. From this and the voltage dependence of BK channel activation, we conclude that the BK channels underlying STOCs are exposed to a mean [Ca2+] on the order of 10 μM during a Ca2+ spark. The membrane area over which a concentration ≥10 μM is reached has an estimated radius of 150–300 nm, corresponding to an area which is a fraction of one square micron. Moreover, given the constraints imposed by the estimated channel density and the Ca2+ current during a spark, the BK channels do not appear to be uniformly distributed over the membrane but instead are found at higher density at the spark site.

Quantitative Analysis of Spontaneous Mitochondrial Depolarizations

Spontaneous transient depolarizations in mitochondrial membrane potential (DeltaPsi(m)), mitochondrial flickers, have been observed in isolated mitochondria and intact cells using the fluorescent probe, tetramethylrhodamine ethyl ester (TMRE). In theory, the ratio of [TMRE] in cytosol and mitochondrion allows DeltaPsi(m) to be calculated with the Nernst equation, but this has proven difficult in practice due to fluorescence quenching and binding of dye to mitochondrial membranes. We developed a new method to determine the amplitude of flickers in terms of millivolts of depolarization. TMRE fluorescence was monitored using high-speed, high-sensitivity three-dimensional imaging to track individual mitochondria in freshly dissociated smooth muscle cells. Resting mitochondrial fluorescence, an exponential function of resting DeltaPsi(m), varied among mitochondria and was approximately normally distributed. Spontaneous changes in mitochondrial fluorescence, indicating depolarizations and repolarizations in DeltaPsi(m), were observed. The depolarizations were reversible and did not result in permanent depolarization of the mitochondria. The magnitude of the flickers ranged from <10 mV to >100 mV with a mean of 17.6 +/- 1.0 mV (n = 360) and a distribution skewed to smaller values. Nearly all mitochondria flickered, and they did so independently of one another, indicating that mitochondria function as independent units in the myocytes employed here.

Regulation of one type of Ca2+ current in smooth muscle cells by diacylglycerol and acetylcholine.

Electrophysiological recordings from freshly dissociated smooth muscle cells from the stomach of the toad Bufo marinus revealed two types of Ca2+ currents. One has a low threshold of activation and inactivates rapidly; the other has a high threshold of activation and inactivates more slowly. Acetylcholine (ACh) increased the high‐threshold current but not the low‐threshold current. The synthetic diacylglycerol analog sn‐1,2‐dioctanoylglycerol, an activator of protein kinase C (PKC), mimicked these effects of ACh on Ca2+ currents. However, another diacylglycerol analog, 1,2‐dioctanoyl‐3‐thioglycerol, which has a closely related structure but does not activate PKC, failed to increase the Ca2+ current. The same was true of l,2‐dioctanoyl‐3‐chloropropanediol, an analog that even at high concentrations only minimally activates PKC. These results suggest that diacylglycerol may be the second messenger mediating the effects of ACh on one type of voltage‐activated Ca2+ channel, possibly by activating PKC.— Vivaudou, M. B.; Clapp, L. H.; Walsh, J. V., Jr.; Singer, J. J. Regulation of one type of Ca2+ current in smooth muscle cells by diacylglycerol and acetylcholine. FASEB J. 2: 2497‐2504; 1988.

P2X7 purinoceptor expression in Xenopus oocytes is not sufficient to produce a pore-forming P2Z-like phenotype

The purinergic rP2X7 receptor expressed in a number of heterologous systems not only functions as a cation channel but also gives rise to a P2Z‐like response, i.e. a reversible membrane permeabilization that allows the passage of molecules with molecular masses of ≥300 Da. We investigated the properties of rP2X7 receptors expressed in Xenopus oocytes. In two‐electrode voltage‐clamp experiments, ATP or BzATP caused inward currents that were abolished or greatly diminished when NMDG+ or choline+ replaced Na+ as the principal external cation. In fluorescent dye experiments, BzATP application did not result in entry of the fluorophore YO‐PRO‐12+. Thus, rP2X7 expression in Xenopus oocytes does not by itself give rise to the pore‐forming P2Z phenotype, suggesting that ancillary factors are involved.

Cholinergic agonists suppress a potassium current in freshly dissociated smooth muscle cells of the toad.

Single micro‐electrode voltage‐clamp and current‐clamp techniques were used to study cholinergic responses in single freshly isolated gastric smooth muscle cells from the toad Bufo marinus. Acetylcholine (ACh) or muscarine caused membrane depolarization, which sometimes gave rise to action potentials and contractions. The agonist‐induced depolarization is due to the suppression of a voltage‐dependent K+ conductance, a conclusion based on the following observations. Depolarization was accompanied by an apparent membrane conductance decrease, seen as the increased size of voltage deflexions in response to constant current pulses. The conductance decrease was confirmed under voltage clamp, where current deflexions in response to constant voltage jumps were smaller in the presence of cholinergic agonists. Muscarine induced net inward currents at potentials positive to the K+ equilibrium potential (EK), and net outward currents at potentials negative to EK. In experiments where external K+ concentration ([K+]o) ranged from 20 to 90 mM the reversal potentials shifted 58 mV positive per tenfold elevation of [K+]o, as expected for a K+ current. The steady‐state current‐voltage relationship revealed that the K+ current inhibited by muscarine was larger at more positive potentials than expected from driving force considerations alone. Therefore, the underlying conductance suppressed by cholinergic agonists was voltage dependent, with almost complete deactivation at potentials more negative than approximately ‐70 mV and exhibiting a sigmoidal activation curve upon depolarization. The deactivation of this voltage‐dependent K+ conductance caused slow current relaxations to occur in response to hyperpolarizing voltage commands from depolarized holding potentials. In experiments where [K+]o ranged from 3 to 30 mM, these current relaxations reversed direction at potentials near EK and the reversal potential shifted 52 mV positive per tenfold elevation of [K+]o, indicating that K ions carry most of the charge. The current relaxations that occurred in response to hyperpolarizing voltage commands were suppressed by ACh, muscarine and oxotremorine. The effects of muscarine persisted in nominally Ca2+‐free solutions containing Mn2+. Ba2+ mimicked the effects of muscarinic agonists. Thus, isolated smooth muscle cells exhibit a K+ current resembling the M‐current of sympathetic and other neurones, which is reversibly suppressed by cholinergic agonists. The existence of a cholinergic K+ conductance decrease is of interest because it has not previously been demonstrated in smooth muscle.

Ca2+ Syntillas, Miniature Ca2+ Release Events in Terminals of Hypothalamic Neurons, Are Increased in Frequency by Depolarization in the Absence of Ca2+ Influx

Localized, brief Ca2+ transients (Ca2+ syntillas) caused by release from intracellular stores were found in isolated nerve terminals from magnocellular hypothalamic neurons and examined quantitatively using a signal mass approach to Ca2+ imaging. Ca2+ syntillas (scintilla, L., spark, from a synaptic structure, a nerve terminal) are caused by release of ∼250,000 Ca ions on average by a Ca2+ flux lasting on the order of tens of milliseconds and occur spontaneously at a membrane potential of –80 mV. Syntillas are unaffected by removal of extracellular Ca2+, are mediated by ryanodine receptors (RyRs) and are increased in frequency, in the absence of extracellular Ca2+, by physiological levels of depolarization. This represents the first direct demonstration of mobilization of Ca2+ from intracellular stores in neurons by depolarization without Ca2+ influx. The regulation of syntillas by depolarization provides a new link between neuronal activity and cytosolic [Ca2+] in nerve terminals.