scholarly journals Transfer of ion binding site from ether-à-go-go to Shaker: Mg2+ binds to resting state to modulate channel opening

2010 ◽  
Vol 135 (5) ◽  
pp. 415-431 ◽  
Author(s):  
Meng-chin A. Lin ◽  
Jeff Abramson ◽  
Diane M. Papazian
Keyword(s):  
Binding Site ◽  
Resting State ◽  
Ionic Current ◽  
Voltage Sensor ◽  
Ion Binding ◽  
Charge Movement ◽  
X Ray ◽  
Cation Binding Site ◽  
Channel Opening ◽  
Voltage Dependent

In ether-à-go-go (eag) K+ channels, extracellular divalent cations bind to the resting voltage sensor and thereby slow activation. Two eag-specific acidic residues in S2 and S3b coordinate the bound ion. Residues located at analogous positions are ∼4 Å apart in the x-ray structure of a Kv1.2/Kv2.1 chimera crystallized in the absence of a membrane potential. It is unknown whether these residues remain in proximity in Kv1 channels at negative voltages when the voltage sensor domain is in its resting conformation. To address this issue, we mutated Shaker residues I287 and F324, which correspond to the binding site residues in eag, to aspartate and recorded ionic and gating currents in the presence and absence of extracellular Mg2+. In I287D+F324D, Mg2+ significantly increased the delay before ionic current activation and slowed channel opening with no readily detectable effect on closing. Because the delay before Shaker opening reflects the initial phase of voltage-dependent activation, the results indicate that Mg2+ binds to the voltage sensor in the resting conformation. Supporting this conclusion, Mg2+ shifted the voltage dependence and slowed the kinetics of gating charge movement. Both the I287D and F324D mutations were required to modulate channel function. In contrast, E283, a highly conserved residue in S2, was not required for Mg2+ binding. Ion binding affected activation by shielding the negatively charged side chains of I287D and F324D. These results show that the engineered divalent cation binding site in Shaker strongly resembles the naturally occurring site in eag. Our data provide a novel, short-range structural constraint for the resting conformation of the Shaker voltage sensor and are valuable for evaluating existing models for the resting state and voltage-dependent conformational changes that occur during activation. Comparing our data to the chimera x-ray structure, we conclude that residues in S2 and S3b remain in proximity throughout voltage-dependent activation.

scholarly journals R1 in the Shaker S4 occupies the gating charge transfer center in the resting state

2011 ◽  
Vol 138 (2) ◽  
pp. 155-163 ◽  
Author(s):  
Meng-chin A. Lin ◽  
Jui-Yi Hsieh ◽  
Allan F. Mock ◽  
Diane M. Papazian
Keyword(s):  
Charge Transfer ◽  
Binding Site ◽  
Resting State ◽  
Slow Component ◽  
Maximum Amplitude ◽  
Voltage Sensor ◽  
Shaker Channels ◽  
Gating Charge ◽  
Voltage Dependent ◽  
Arginine Residues

During voltage-dependent activation in Shaker channels, four arginine residues in the S4 segment (R1–R4) cross the transmembrane electric field. It has been proposed that R1–R4 movement is facilitated by a “gating charge transfer center” comprising a phenylalanine (F290) in S2 plus two acidic residues, one each in S2 and S3. According to this proposal, R1 occupies the charge transfer center in the resting state, defined as the conformation in which S4 is maximally retracted toward the cytoplasm. However, other evidence suggests that R1 is located extracellular to the charge transfer center, near I287 in S2, in the resting state. To investigate the resting position of R1, we mutated I287 to histidine (I287H), paired it with histidine mutations of key voltage sensor residues, and determined the effect of extracellular Zn2+ on channel activity. In I287H+R1H, Zn2+ generated a slow component of activation with a maximum amplitude (Aslow,max) of ∼56%, indicating that only a fraction of voltage sensors can bind Zn2+ at a holding potential of −80 mV. Aslow,max decreased after applying either depolarizing or hyperpolarizing prepulses from −80 mV. The decline of Aslow,max after negative prepulses indicates that R1 moves inward to abolish ion binding, going beyond the point where reorientation of the I287H and R1H side chains would reestablish a binding site. These data support the proposal that R1 occupies the charge transfer center upon hyperpolarization. Consistent with this, pairing I287H with A359H in the S3–S4 loop generated a Zn2+-binding site. At saturating concentrations, Aslow,max reached 100%, indicating that Zn2+ traps the I287H+A359H voltage sensor in an absorbing conformation. Transferring I287H+A359H into a mutant background that stabilizes the resting state significantly enhanced Zn2+ binding at −80 mV. Our results strongly support the conclusion that R1 occupies the gating charge transfer center in the resting conformation.

scholarly journals Mutations in the S4 Region Isolate the Final Voltage-dependent Cooperative Step in Potassium Channel Activation

1999 ◽  
Vol 113 (3) ◽  
pp. 389-414 ◽  
Author(s):  
Jennifer L. Ledwell ◽  
Richard W. Aldrich
Keyword(s):  
Voltage Dependence ◽  
Ionic Current ◽  
Amino Acid Sequences ◽  
Total Charge ◽  
Charge Movement ◽  
Activation Pathway ◽  
Channel Opening ◽  
Voltage Dependent ◽  
Rate Limiting ◽  
Cooperative Transition

Charged residues in the S4 transmembrane segment play a key role in determining the sensitivity of voltage-gated ion channels to changes in voltage across the cell membrane. However, cooperative interactions between subunits also affect the voltage dependence of channel opening, and these interactions can be altered by making substitutions at uncharged residues in the S4 region. We have studied the activation of two mutant Shaker channels that have different S4 amino acid sequences, ILT (V369I, I372L, and S376T) and Shaw S4 (the S4 of Drosophila Shaw substituted into Shaker), and yet have very similar ionic current properties. Both mutations affect cooperativity, making a cooperative transition in the activation pathway rate limiting and shifting it to very positive voltages, but analysis of gating and ionic current recordings reveals that the ILT and Shaw S4 mutant channels have different activation pathways. Analysis of gating currents suggests that the dominant effect of the ILT mutation is to make the final cooperative transition to the open state of the channel rate limiting in an activation pathway that otherwise resembles that of Shaker. The charge movement associated with the final gating transition in ILT activation can be measured as an isolated component of charge movement in the voltage range of channel opening and accounts for 13% (∼1.8 e0) of the total charge moved in the ILT activation pathway. The remainder of the ILT gating charge (87%) moves at negative voltages, where channels do not open, and confirms the presence of Shaker-like conformational changes between closed states in the activation pathway. In contrast to ILT, the activation pathway of Shaw S4 seems to involve a single cooperative charge-moving step between a closed and an open state. We cannot detect any voltage-dependent transitions between closed states for Shaw S4. Restoring basic residues that are missing in Shaw S4 (R1, R2, and K7) rescues charge movement between closed states in the activation pathway, but does not alter the voltage dependence of the rate-limiting transition in activation.

scholarly journals The ladder-shaped polyether toxin gambierol anchors the gating machinery of Kv3.1 channels in the resting state

2013 ◽  
Vol 141 (3) ◽  
pp. 359-369 ◽  
Author(s):  
Ivan Kopljar ◽  
Alain J. Labro ◽  
Tessa de Block ◽  
Jon D. Rainier ◽  
Jan Tytgat ◽  
...  
Keyword(s):  
Binding Site ◽  
Resting State ◽  
Ionic Current ◽  
Dissociation Kinetics ◽  
Gating Currents ◽  
Voltage Range ◽  
High Affinity ◽  
Kv Channels ◽  
Channel Opening ◽  
Nav Channels

Voltage-gated potassium (Kv) and sodium (Nav) channels are key determinants of cellular excitability and serve as targets of neurotoxins. Most marine ciguatoxins potentiate Nav channels and cause ciguatera seafood poisoning. Several ciguatoxins have also been shown to affect Kv channels, and we showed previously that the ladder-shaped polyether toxin gambierol is a potent Kv channel inhibitor. Most likely, gambierol acts via a lipid-exposed binding site, located outside the K+ permeation pathway. However, the mechanism by which gambierol inhibits Kv channels remained unknown. Using gating and ionic current analysis to investigate how gambierol affected S6 gate opening and voltage-sensing domain (VSD) movements, we show that the resting (closed) channel conformation forms the high-affinity state for gambierol. The voltage dependence of activation was shifted by >120 mV in the depolarizing direction, precluding channel opening in the physiological voltage range. The (early) transitions between the resting and the open state were monitored with gating currents, and provided evidence that strong depolarizations allowed VSD movement up to the activated-not-open state. However, for transition to the fully open (ion-conducting) state, the toxin first needed to dissociate. These dissociation kinetics were markedly accelerated in the activated-not-open state, presumably because this state displayed a much lower affinity for gambierol. A tetrameric concatemer with only one high-affinity binding site still displayed high toxin sensitivity, suggesting that interaction with a single binding site prevented the concerted step required for channel opening. We propose a mechanism whereby gambierol anchors the channel’s gating machinery in the resting state, requiring more work from the VSD to open the channel. This mechanism is quite different from the action of classical gating modifier peptides (e.g., hanatoxin). Therefore, polyether toxins open new opportunities in structure–function relationship studies in Kv channels and in drug design to modulate channel function.

scholarly journals Permeation of Na+ through a delayed rectifier K+ channel in chick dorsal root ganglion neurons.

1994 ◽  
Vol 104 (4) ◽  
pp. 747-771 ◽  
Author(s):  
M J Callahan ◽  
S J Korn
Keyword(s):  
Dorsal Root Ganglion ◽  
Binding Site ◽  
Dorsal Root ◽  
Reversal Potential ◽  
Dorsal Root Ganglion Neurons ◽  
K Channel ◽  
Delayed Rectifier ◽  
Cation Binding Site ◽  
Voltage Dependent ◽  
Ganglion Neurons

In whole-cell patch clamp recordings from chick dorsal root ganglion neurons, removal of intracellular K+ resulted in the appearance of a large, voltage-dependent inward tail current (Icat). Icat was not Ca2+ dependent and was not blocked by Cd2+, but was blocked by Ba2+. The reversal potential for Icat shifted with the Nernst potential for [Na+]. The channel responsible for Icat had a cation permeability sequence of Na+ > Li+ > TMA+ > NMG+ (PX/PNa = 1:0.33:0.1:0) and was impermeable to Cl-. Addition of high intracellular concentrations of K+, Cs+, or Rb+ prevented the occurrence of Icat. Inhibition of Icat by intracellular K+ was voltage dependent, with an IC50 that ranged from 3.0-8.9 mM at membrane potentials between -50 and -110 mV. This voltage-dependent shift in IC50 (e-fold per 52 mV) is consistent with a single cation binding site approximately 50% of the distance into the membrane field. Icat displayed anomolous mole fraction behavior with respect to Na+ and K+; Icat was inhibited by 5 mM extracellular K+ in the presence of 160 mM Na+ and potentiated by equimolar substitution of 80 mM K+ for Na+. The percent inhibition produced by both extracellular and intracellular K+ at 5 mM was identical. Reversal potential measurements revealed that K+ was 65-105 times more permeant than Na+ through the Icat channel. Icat exhibited the same voltage and time dependence of inactivation, the same voltage dependence of activation, and the same macroscopic conductance as the delayed rectifier K+ current in these neurons. We conclude that Icat is a Na+ current that passes through a delayed rectifier K+ channel when intracellular K+ is reduced to below 30 mM. At intracellular K+ concentrations between 1 and 30 mM, PK/PNa remained constant while the conductance at -50 mV varied from 80 to 0% of maximum. These data suggest that the high selectivity of these channels for K+ over Na+ is due to the inability of Na+ to compete with K+ for an intracellular binding site, rather than a barrier that excludes Na+ from entry into the channel or a barrier such as a selectivity filter that prevents Na+ ions from passing through the channel.

scholarly journals Effective gating charges per channel in voltage-dependent K+ and Ca2+ channels.

1996 ◽  
Vol 108 (3) ◽  
pp. 143-155 ◽  
Author(s):  
F Noceti ◽  
P Baldelli ◽  
X Wei ◽  
N Qin ◽  
L Toro ◽  
...  
Keyword(s):  
Ionic Current ◽  
Variance Analysis ◽  
Beta Subunit ◽  
Charge Movement ◽  
Gating Currents ◽  
Open Probability ◽  
K Channels ◽  
Voltage Dependent ◽  
Pore Opening ◽  
Ca2 Channels

In voltage-dependent ion channels, the gating of the channels is determined by the movement of the voltage sensor. This movement reflects the rearrangement of the protein in response to a voltage stimulus, and it can be thought of as a net displacement of elementary charges (e0) through the membrane (z: effective number of elementary charges). In this paper, we measured z in Shaker IR (inactivation removed) K+ channels, neuronal alpha 1E and alpha 1A, and cardiac alpha 1C Ca2+ channels using two methods: (a) limiting slope analysis of the conductance-voltage relationship and (b) variance analysis, to evaluate the number of active channels in a patch, combined with the measurement of charge movement in the same patch. We found that in Shaker IR K+ channels the two methods agreed with a z congruent to 13. This suggests that all the channels that gate can open and that all the measured charge is coupled to pore opening in a strictly sequential kinetic model. For all Ca2+ channels the limiting slope method gave consistent results regardless of the presence or type of beta subunit tested (z = 8.6). However, as seen with alpha 1E, the variance analysis gave different results depending on the beta subunit used. alpha 1E and alpha 1E beta 1a gave higher z values (z = 14.77 and z = 15.13 respectively) than alpha 1E beta 2a (z = 9.50, which is similar to the limiting slope results). Both the beta 1a and beta 2a subunits, coexpressed with alpha 1E Ca2+ channels facilitated channel opening by shifting the activation curve to more negative potentials, but only the beta 2a subunit increased the maximum open probability. The higher z using variance analysis in alpha 1E and alpha 1E beta 1a can be explained by a set of charges not coupled to pore opening. This set of charges moves in transitions leading to nulls thus not contributing to the ionic current fluctuations but eliciting gating currents. Coexpression of the beta 2a subunit would minimize the fraction of nulls leading to the correct estimation of the number of channels and z.

scholarly journals An extended x-ray absorption fine structure study of the high-affinity cation-binding site in the purple membrane

1996 ◽  
Vol 70 (2) ◽  
pp. 852-856 ◽  
Author(s):  
F. Sepulcre ◽  
J. Cladera ◽  
J. García ◽  
M.G. Proietti ◽  
J. Torres ◽  
...  
Keyword(s):  
Fine Structure ◽  
Binding Site ◽  
Structure Study ◽  
Purple Membrane ◽  
Cation Binding ◽  
X Ray ◽  
High Affinity ◽  
Absorption Fine ◽  
Cation Binding Site ◽  
X Ray Absorption

scholarly journals Heme Regulates Allosteric Activation of the Slo1 BK Channel

2005 ◽  
Vol 126 (1) ◽  
pp. 7-21 ◽  
Author(s):  
Frank T. Horrigan ◽  
Stefan H. Heinemann ◽  
Toshinori Hoshi
Keyword(s):  
Divalent Cations ◽  
Ionic Currents ◽  
Bk Channels ◽  
Bk Channel ◽  
Voltage Sensor ◽  
Gating Currents ◽  
Calcium Dependent ◽  
Channel Opening ◽  
Activation Gate ◽  
Voltage Dependent

Large conductance calcium-dependent (Slo1 BK) channels are allosterically activated by membrane depolarization and divalent cations, and possess a rich modulatory repertoire. Recently, intracellular heme has been identified as a potent regulator of Slo1 BK channels (Tang, X.D., R. Xu, M.F. Reynolds, M.L. Garcia, S.H. Heinemann, and T. Hoshi. 2003. Nature. 425:531–535). Here we investigated the mechanism of the regulatory action of heme on heterologously expressed Slo1 BK channels by separating the influences of voltage and divalent cations. In the absence of divalent cations, heme generally decreased ionic currents by shifting the channel's G–V curve toward more depolarized voltages and by rendering the curve less steep. In contrast, gating currents remained largely unaffected by heme. Simulations suggest that a decrease in the strength of allosteric coupling between the voltage sensor and the activation gate and a concomitant stabilization of the open state account for the essential features of the heme action in the absence of divalent ions. At saturating levels of divalent cations, heme remained similarly effective with its influence on the G–V simulated by weakening the coupling of both Ca2+ binding and voltage sensor activation to channel opening. The results thus show that heme dampens the influence of allosteric activators on the activation gate of the Slo1 BK channel. To account for these effects, we consider the possibility that heme binding alters the structure of the RCK gating ring and thereby disrupts both Ca2+- and voltage-dependent gating as well as intrinsic stability of the open state.

scholarly journals Dynamic Modulation of Voltage-Dependent Kv7.2-7.3 Channel Opening by Voltage-Sensor Relaxation

2011 ◽  
Vol 100 (3) ◽  
pp. 428a
Author(s):  
Carlos A. Villalba-Galea ◽  
Junghoon Ha ◽  
I. Scott Ramsey
Keyword(s):  
Voltage Sensor ◽  
Dynamic Modulation ◽  
Channel Opening ◽  
Voltage Dependent

scholarly journals Allosteric binding site in a Cys-loop receptor ligand-binding domain unveiled in the crystal structure of ELIC in complex with chlorpromazine

2016 ◽  
Vol 113 (43) ◽  
pp. E6696-E6703 ◽  
Author(s):  
Mieke Nys ◽  
Eveline Wijckmans ◽  
Ana Farinha ◽  
Özge Yoluk ◽  
Magnus Andersson ◽  
...  
Keyword(s):  
Ligand Binding ◽  
Ion Channel ◽  
Binding Site ◽  
Binding Domain ◽  
Ligand Binding Domain ◽  
Channel Pore ◽  
X Ray ◽  
Electrophysiological Recordings ◽  
Channel Opening ◽  
Dynamics Simulations

Pentameric ligand-gated ion channels or Cys-loop receptors are responsible for fast inhibitory or excitatory synaptic transmission. The antipsychotic compound chlorpromazine is a widely used tool to probe the ion channel pore of the nicotinic acetylcholine receptor, which is a prototypical Cys-loop receptor. In this study, we determine the molecular determinants of chlorpromazine binding in the Erwinia ligand-gated ion channel (ELIC). We report the X-ray crystal structures of ELIC in complex with chlorpromazine or its brominated derivative bromopromazine. Unexpectedly, we do not find a chlorpromazine molecule in the channel pore of ELIC, but behind the β8–β9 loop in the extracellular ligand-binding domain. The β8–β9 loop is localized downstream from the neurotransmitter binding site and plays an important role in coupling of ligand binding to channel opening. In combination with electrophysiological recordings from ELIC cysteine mutants and a thiol-reactive derivative of chlorpromazine, we demonstrate that chlorpromazine binding at the β8–β9 loop is responsible for receptor inhibition. We further use molecular-dynamics simulations to support the X-ray data and mutagenesis experiments. Together, these data unveil an allosteric binding site in the extracellular ligand-binding domain of ELIC. Our results extend on previous observations and further substantiate our understanding of a multisite model for allosteric modulation of Cys-loop receptors.

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