Neuregulin-1 Enhances Depolarization-Induced GABA Release
Ran‐Sook WooXiao-Ming LiYanmei TaoEzekiel P. Carpenter‐HylandYang Z. HuangJanet L. WeberHannah NeiswenderXian‐Ping DongJiong WuMartin GassmannCary LaiWen‐Cheng XiongTian-Ming GaoLin Mei
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Neuregulin
1. Contractile responses in short twitch-type snake muscle fibres have been studied. These fibres are sufficiently short to allow fairly uniform changes in membrane potential along their length when current is passed through an intracellular micropipette. Active sodium permeability changes were blocked with tetrodotoxin (TTX), procaine, or by using solutions low in sodium. Current and voltage micropipettes were used to voltage-clamp these fibres. Depolarization steps to about -40 mV evoked contractile responses, maximal tension being developed between -10 and 0 mV. The relation between contraction and membrane potential was sigmoid.2. Depolarization beyond a critical threshold produced an increment of outward current which inactivated with time. The threshold for this delayed rectification was normally similar to the threshold for contractile activation. Fibres exposed to high potassium showed a reversal of this inactivating current to slightly super-threshold depolarizing pulses. At membrane potentials near 0 mV, no inactivating current was noted, while stronger depolarizing pulses produced an inactivating current in the normal direction. Fibres in high potassium show the same threshold for initiation of contraction as in normal solution.3. Thiocyanate, nitrate, and caffeine shifted the relation between membrane potential and contraction toward higher levels of membrane potential. The threshold for inactivating rectifying current failed to shift to a corresponding extent, although some shift in rectification which did not inactivate was evident.4. When depolarization was maintained, contractile tension was maximal for several seconds, then gradually disappeared. The rate of this contractile inactivation depended upon the level of depolarization.
Tetrodotoxin
Tetraethylammonium
Pipette
Current clamp
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Both vertebrate and invertebrate skeletal muscle fibres have Ca2+ permeability mechanisms which are turned on by depolarization of the surface membrane. In frog muscle, Ca currents are extremely slow and will be scarcely activated during the action potential that normally elicits a twitch. This Ca permeability cannot therefore play any substantial, direct role in excitation--contraction coupling. In insect (Carausius morosus) muscle, Ca currents activate within milliseconds of depolarization, even at low temperature, and may well play at least a triggering role in excitation--contraction coupling. These Ca currents show saturation with increasing [Ca]0, while the instantaneous current--voltage relation rectifies inwards, as expected from a very low [Ca]i. The Ca channel is permeable to Sr2+ and Ba2+. Inactivation of Ca currents under a maintained depolarization depends on Ca2+ carrying inward current, however, rather than on the depolarization itself.
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Voltage-gated potassium channels play crucial roles in regulating membrane potential. They are activated by membrane depolarization, allowing the selective permeation of K+ ions across the plasma membrane, and enter a nonconducting state after lasting depolarization, a process known as inactivation. Inactivation in voltage-activated potassium channels occurs through two distinct mechanisms, N-type and C-type inactivation. C-type inactivation is caused by conformational changes in the extracellular mouth of the channel, whereas N-type inactivation is elicited by changes in the cytoplasmic mouth of the protein. The W434F-mutated Shaker channel is known as a nonconducting mutant and is in a C-type inactivation state at a depolarizing membrane potential. To clarify the structural properties of C-type inactivated protein, we performed molecular dynamics simulations of the wild-type and W366F (corresponding to W434F in Shaker) mutant of the Kv1.2-2.1 chimera channel. The W366F mutant was in a nearly nonconducting state with a depolarizing voltage and recovered from inactivation with a reverse voltage. Our simulations and three-dimensional reference interaction site model analysis suggested that structural changes in the selectivity filter upon membrane depolarization trap K+ ions around the inner mouth of the selectivity filter and prevent ion permeation. This pore restriction is involved in the molecular mechanism of C-type inactivation.
Shaker
KcsA potassium channel
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Noradrenaline (NA) in a concentration of 5 X 10(-6) M produces depolarization of smooth muscle cells of the rabbit pulmonary artery and reduction of membrane resistance followed by contraction and increased excitability of muscle cells. Experiments with repolarization of the membrane exposed to NA in normal and Ca-free Krebs solutions have shown that activation of the NA-induced contraction is mainly due to Ca++ entering the cells through NA-sensitive potential-dependent Ca-channels. The NA-induced depolarization results from an initial decrease of K-permeability of the membrane subsequent increase of the permeability of NA-sensitive potential-dependent channels for Na+ and/or Cl-, which provides further depolarization of the membrane. Depolarization ceases after becoming sufficient for activation of potential-dependent non-inactivated K-channels. Voltage clamp experiments have shown that the NA-induced increased excitability is related to a reduction of slow, particularly of fast component of outward current, whose early activation prevents the development of regenerative process of action potential generation under normal conditions.
Myogenic contraction
Reversal potential
Hyperpolarization
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Correlation between Charge Movement and Ionic Current during Slow Inactivation in Shaker K+ Channels
Prolonged depolarization induces a slow inactivation process in some K+ channels. We have studied ionic and gating currents during long depolarizations in the mutant Shaker H4-Δ(6–46) K+ channel and in the nonconducting mutant (Shaker H4-Δ(6–46)-W434F). These channels lack the amino terminus that confers the fast (N-type) inactivation (Hoshi, T., W.N. Zagotta, and R.W. Aldrich. 1991. Neuron. 7:547–556). Channels were expressed in oocytes and currents were measured with the cut-open-oocyte and patch-clamp techniques. In both clones, the curves describing the voltage dependence of the charge movement were shifted toward more negative potentials when the holding potential was maintained at depolarized potentials. The evidences that this new voltage dependence of the charge movement in the depolarized condition is associated with the process of slow inactivation are the following: (a) the installation of both the slow inactivation of the ionic current and the inactivation of the charge in response to a sustained 1-min depolarization to 0 mV followed the same time course; and (b) the recovery from inactivation of both ionic and gating currents (induced by repolarizations to −90 mV after a 1-min inactivating pulse at 0 mV) also followed a similar time course. Although prolonged depolarizations induce inactivation of the majority of the channels, a small fraction remains non–slow inactivated. The voltage dependence of this fraction of channels remained unaltered, suggesting that their activation pathway was unmodified by prolonged depolarization. The data could be fitted to a sequential model for Shaker K+ channels (Bezanilla, F., E. Perozo, and E. Stefani. 1994. Biophys. J. 66:1011–1021), with the addition of a series of parallel nonconducting (inactivated) states that become populated during prolonged depolarization. The data suggest that prolonged depolarization modifies the conformation of the voltage sensor and that this change can be associated with the process of slow inactivation.
Shaker
Reversal potential
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ABSTRACT Voltage-gated potassium channels play crucial roles in regulating membrane potential. They are activated by membrane depolarization, allowing the selective permeation of potassium ions across the plasma membrane, and enter a nonconducting state after lasting depolarization of membrane potential, a process known as inactivation. Inactivation in voltage-activated potassium channels occurs through two distinct mechanisms, N-type inactivation and C-type inactivation. C-type inactivation is caused by conformational changes in the extracellular mouth of the channel, while N-type inactivation is elicited by changes in the cytoplasmic mouth of the protein. The W434F-mutated Shaker channel is known as a nonconducting mutant and is in a C-type inactivation state at a depolarizing membrane potential. To clarify the structural properties of C-type inactivated protein, we performed molecular dynamics simulations of the wild-type and W366F (corresponding to W434F in Shaker) mutant of the Kv1.2-2.1 chimera channel. The W366F mutant was in a nearly nonconducting state with a depolarizing voltage and recovered from inactivation with a reverse voltage. Our simulations and 3D-RISM analysis suggested that structural changes in the selective filter upon membrane depolarization trap potassium ions around the entrance of the selectivity filter and prevent ion permeation. This pore restriction is involved in the molecular mechanism of C-type inactivation.
Shaker
KcsA potassium channel
Voltage-gated potassium channel
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The effects of hypoxia on K+ current (IK), resting membrane potential, and cytosolic free Ca2+ in rat pheochromocytoma (PC-12) cells were studied. Whole cell voltage- and current-clamp experiments were performed to measure IK and membrane potential, respectively. Cytosolic free Ca2+ level was measured using the Ca(2+)-sensitive fluorescent dye fura 2. Depolarizing voltage steps to +50 mV from a holding potential of -90 mV elicited a slowly inactivating, tetraethylammonium chloride-sensitive, and Ca(2+)-insensitive IK that was reversibly inhibited by reduced O2 tension. Graded reduction in PO2 (from 150 to 0 mmHg) induced a graded inhibition of O2-sensitive IK [IK(O2)] up to 46% at 0 mmHg. Moreover, hypoxia induced a 19-mV membrane depolarization and a twofold increase in cytosolic free Ca2+. In Ca(2+)-free condition, inhibition of IK(O2) induced an 8-mV depolarization, suggesting that inhibition of IK(O2) was responsible for initiating depolarization. The effect of reduced PO2 on the current-voltage relationship showed a reduction of outward current and a 14-mV shift in the reversal potential comparable with the amount of depolarization measured in current clamp experiments. Neither Ca(2+)-activated IK nor inwardly rectifying IK are responsible for the hypoxia-induced depolarization. In conclusion, PC-12 cells express an IK(O2), inhibition of which leads to membrane depolarization and increased intracellular Ca2+, making the PC-12 clonal cell line a useful model for studying the molecular and biophysical mechanisms that mediate O2 chemosensitivity.
Tetraethylammonium
Current clamp
Tetraethylammonium chloride
Fura-2
Reversal potential
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1. Two glass micro-electrodes were inserted into neighbouring cells from rat or mouse pancreatic segments, superfused in vitro. The tip of a third glass micro-electrode, filled with 2 M-AChCl, was placed just outside the acinus under investigation. Membrane potential and resistance, and changes in these parameters in response to short pulses of ACh stimulation, were recorded.2. The resting current-voltage relationship, obtained by injecting 100 msec depolarizing or hyperpolarizing current pulses through one of the intracellular micro-electrodes and recording the membrane potential with the other intracellular electrode, was linear within the range -5 to -60 mV.3. Injecting depolarizing or hyperpolarizing current (d.c.) through one of the intracellular micro-electrodes, the membrane potential (as measured with the other intracellular micro-electrode) could be set at various levels. The effect of ACh at different membrane potentials was investigated. When the acinar cell membrane was hyperpolarized, the amplitude of ACh-evoked depolarization was increased, while ACh-evoked depolarization was reduced when the membrane potential was reduced by depolarizing current, and finally changed into a hyperpolarization at very low membrane potentials. In each acinus investigated (rat and mouse), there was a linear relationship between amplitude of ACh-evoked potential change (DeltaV) (+ value or - value according to polarity) and resting membrane potential. During superfusion with control solution, the value of the membrane potential at which ACh did not evoke a potential change (E(ACh)) was about -15 mV in the mouse and about -20 mV in the rat. During superfusion with a chloride-free sulphate-containing solution (steady state), a linear relationship between DeltaV and resting membrane potential was again found but E(ACh) (mouse) was about +10 mV.4. A continuous rough estimate of E(ACh) was obtained by injecting repetitively depolarizing current pulses (100 msec) through one intracellular micro-electrode; in this way, the effect of ACh measured by the other intracellular electrode could be assessed simultaneously at the spontaneous resting level, and at a depolarized level. The direction of change in E(ACh) following acute changes in the superfusion fluid ion composition was assessed. Replacing extracellular chloride by sulphate caused an immediate change in E(ACh) in the positive direction. Re-admission of chloride, after a long period of chloride ion deprivation, caused an immediate sharp change in E(ACh) in the negative direction. Replacing extracellular sodium by Tris caused an immediate transient negative change in E(ACh). In contrast, taking away extracellular calcium changed E(ACh) in a positive direction. Augmenting extracellular potassium concentration to 40 mM caused a change in E(ACh) in the positive direction.5. At a membrane potential (V) equal to E(ACh) the sum of ionic currents evoked by the action of ACh is zero. Using the Goldman treatment, it appears that ACh increases membrane Na, K and Cl permeability. The approximate relative ion permeabilities of the pathways opened up by ACh are: P(Na)/P(K) = 2.5 and P(Cl)/P(K) = 5. At V = E(ACh), the approximate relative sizes of the ACh-evoked currents are: I(Na)/I(K) = 2.6 and I(Cl)/I(K) = 1.6 ACh, therefore, causes influx of Na and Cl and a small efflux of K.
Hyperpolarization
Acinus
Reversal potential
Membrane channel
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The ionic basis of the glucose-induced membrane potential changes in pancreatic B-cells was investigated. The results suggest that the initial depolarization of the membrane in response to a stimulation with glucose is due to a decrease of the K permeability. This depolarization seems to open a voltage-dependent Ca-channel and thereby an additional depolarization, the depolarization phase of the slow waves, is initiated. Insulin release is then triggered by the entering Ca ions. The fast spike activity may be a consequence of the exocytotic process. The polarization phase of the slow waves seems to be caused by the activity of an electrogenic Na-K-pump and a calcium-dependent increase of the K permeability. The activity of the Na-pump is considered to be regulated by the intracellular Na concentration.
Hyperpolarization
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