scholarly journals Distribution and kinetics of membrane dielectric polarization. 1. Long-term inactivation of gating currents.

1982 ◽  
Vol 79 (1) ◽  
pp. 21-40 ◽  
Author(s):  
F Bezanilla ◽  
R E Taylor ◽  
J M Fernández
Keyword(s):  
Total Charge ◽  
Linear Component ◽  
Slow Inactivation ◽  
Gating Current ◽  
Dielectric Polarization ◽  
Gating Currents ◽  
Gating Charge ◽  
The One ◽  
Kinetics Of

Gating currents were measured by subtracting the linear component of the capacitative current recorded at very positive or very negative potentials. When the membrane is depolarized for a few minutes, repolarized to the usual holding potential (HP) of --70 mV for 1 ms, and then pulsed to 0 mV, the charge transferred in 2--4 ms is approximately 50% of that which was transferred during the same pulse holding at --70 mV. This charge decrease, called slow inactivation of the gating current, was found to be consistent with a shift of the charge vs. potential (Q-V) curve to more hyperpolarized potentials. When the HP is 0 mV, the total charge available to move is the same as the total charge available when the HP is --70 mV. The time constants of the fast component of the ON gating current are smaller at depolarized holding potentials than at --70 mV. When the HP is --70 mV and a prepulse of 50 ms duration is given to 0 mV, the Q-V curve is also shifted to more hyperpolarized potentials (charge immobilization), but the effect is not as pronounced as the one obtained by holding at 0 mV. When the HP is 0 mV, a prepulse to --70 mV for 50 ms partially shifts back the Q-V curve, indicating that fast inactivation of the gating charge may be recovered in the presence of slow inactivation. A physical model consisting of a gating particle that interacts with a fast inactivating particle, and a slow inactivating particle, reproduces most of the experimental results.

scholarly journals Fast Inactivation in Shaker K+ Channels

1998 ◽  
Vol 111 (5) ◽  
pp. 625-638 ◽  
Author(s):  
Michel J. Roux ◽  
Riccardo Olcese ◽  
Ligia Toro ◽  
Francisco Bezanilla ◽  
Enrico Stefani
Keyword(s):  
Time Course ◽  
Ionic Current ◽  
Fast Inactivation ◽  
Gating Current ◽  
Gating Currents ◽  
Current Decay ◽  
Gating Charge ◽  
External Potassium ◽  
Kinetics Of ◽  
Full Charge

Fast inactivating Shaker H4 potassium channels and nonconducting pore mutant Shaker H4 W434F channels have been used to correlate the installation and recovery of the fast inactivation of ionic current with changes in the kinetics of gating current known as “charge immobilization” (Armstrong, C.M., and F. Bezanilla. 1977. J. Gen. Physiol. 70:567–590.). Shaker H4 W434F gating currents are very similar to those of the conducting clone recorded in potassium-free solutions. This mutant channel allows the recording of the total gating charge return, even when returning from potentials that would largely inactivate conducting channels. As the depolarizing potential increased, the OFF gating currents decay phase at −90 mV return potential changed from a single fast component to at least two components, the slower requiring ∼200 ms for a full charge return. The charge immobilization onset and the ionic current decay have an identical time course. The recoveries of gating current (Shaker H4 W434F) and ionic current (Shaker H4) in 2 mM external potassium have at least two components. Both recoveries are similar at −120 and −90 mV. In contrast, at higher potentials (−70 and −50 mV), the gating charge recovers significantly more slowly than the ionic current. A model with a single inactivated state cannot account for all our data, which strongly support the existence of “parallel” inactivated states. In this model, a fraction of the charge can be recovered upon repolarization while the channel pore is occupied by the NH2-terminus region.

scholarly journals Phosphorylation modulates potassium conductance and gating current of perfused giant axons of squid.

1990 ◽  
Vol 95 (2) ◽  
pp. 245-271 ◽  
Author(s):  
C K Augustine ◽  
F Bezanilla
Keyword(s):  
Steady State ◽  
Voltage Dependence ◽  
Potassium Conductance ◽  
Charge Movement ◽  
Gating Current ◽  
Gating Currents ◽  
Internal Solution ◽  
Giant Axons ◽  
Gating Charge ◽  
Phosphorylation Reaction

The presence of internal Mg-ATP produced a number of changes in the K conductance of perfused giant axons of squid. For holding potentials between -40 and -50 mV, steady-state K conductance increased for depolarizations to potentials more positive than approximately -15 mV and decreased for smaller depolarizations. The voltage dependencies of both steady-state activation and inactivation also appears shifted toward more positive potentials. Gating kinetics were affected by internal ATP, with the activation time constant slowed and the characteristic delay in K conductance markedly enhanced. The rate of deactivation also was hastened during perfusion with ATP. Internal ATP affected potassium channel gating currents in similar ways. The voltage dependence of gating charge movement was shifted toward more positive potentials and the time constants of ON and OFF gating current also were slowed and hastened, respectively, in the presence of ATP. These effects of ATP on the K conductance occurred when no exogenous protein kinases were added to the internal solution and persisted even after removing ATP from the internal perfusate. Perfusion with a solution containing exogenous alkaline phosphatase reversed the effects of ATP. These results provide further evidence that the effects of ATP on the K conductance are a consequence of a phosphorylation reaction mediated by a kinase present and active in perfused axons. Phosphorylation appears to alter the K conductance of squid giant axons via a minimum of two mechanisms. First, the voltage dependence of gating parameters are shifted toward positive potentials. Second, there is an increase in the number of functional closed states and/or a decrease in the rates of transition between these states of the K channels.

scholarly journals The Voltage Sensor in Voltage-Dependent Ion Channels

2000 ◽  
Vol 80 (2) ◽  
pp. 555-592 ◽  
Author(s):  
Francisco Bezanilla
Keyword(s):  
Membrane Potential ◽  
Conformational Changes ◽  
Structural Information ◽  
Noise Analysis ◽  
Voltage Sensor ◽  
Fluorescence Labeling ◽  
Gating Current ◽  
Gating Currents ◽  
Gating Charge ◽  
Voltage Dependent

In voltage-dependent Na, K, or Ca channels, the probability of opening is modified by the membrane potential. This is achieved through a voltage sensor that detects the voltage and transfers its energy to the pore to control its gate. We present here the theoretical basis of the energy coupling between the electric field and the voltage, which allows the interpretation of the gating charge that moves in one channel. Movement of the gating charge constitutes the gating current. The properties are described, along with macroscopic data and gating current noise analysis, in relation to the operation of the voltage sensor and the opening of the channel. Structural details of the voltage sensor operation were resolved initially by locating the residues that make up the voltage sensor using mutagenesis experiments and determining the number of charges per channel. The changes in conformation are then analyzed based on the differential exposure of cysteine or histidine-substituted residues. Site-directed fluorescence labeling is then analyzed as another powerful indicator of conformational changes that allows time and voltage correlation of local changes seen by the fluorophores with the global change seen by the electrophysiology of gating currents and ionic currents. Finally, we describe the novel results on lanthanide-based resonance energy transfer that show small distance changes between residues in the channel molecule. All of the electrophysiological and the structural information are finally summarized in a physical model of a voltage-dependent channel in which a change in membrane potential causes rotation of the S4 segment that changes the exposure of the basic residues from an internally connected aqueous crevice at hyperpolarized potentials to an externally connected aqueous crevice at depolarized potentials.

Sequential gating in the human heart K+ channel Kv1.5 incorporatesQ 1 andQ 2 charge components

1999 ◽  
Vol 277 (5) ◽  
pp. H1956-H1966 ◽  
Author(s):  
J. Christian Hesketh ◽  
David Fedida
Keyword(s):  
K Channel ◽  
Delayed Rectifier ◽  
Potential Range ◽  
Charge Movement ◽  
Gating Current ◽  
Gating Currents ◽  
Charge Voltage ◽  
Hek 293 ◽  
Gating Charge ◽  
State Dependent

On-gating current from the Kv1.5 cardiac delayed rectifier K+ channel expressed in HEK-293 cells was separated into two distinct charge systems, Q 1 and Q 2, obtained from double Boltzmann fits to the charge-voltage relationship. Q 1 and Q 2 had characteristic voltage dependence and sensitivity with half-activation potentials of −29.6 ± 1.6 and −2.19 ± 2.09 mV and effective valences of 1.87 ± 0.15 and 5.53 ± 0.27 e −, respectively. The contribution to total gating charge was 0.20 ± 0.04 for Q 1 and 0.80 ± 0.04 ( n = 5) for Q 2. At intermediate depolarizations, heteromorphic gating current waveforms resulted from relatively equal contributions from Q 1 and Q 2, but with widely different kinetics. Prepulses to −20 mV moved only Q 1, simplified on-gating currents, and allowed rapid Q 2 movement. Voltage-dependent on-gating current recovery in the presence of 4-aminopyridine (1 mM) suggested a sequentially coupled movement of the two charge systems during channel activation. This allowed the construction of a linear five-state model of Q 1 and Q 2 gating charge movement, which predicted experimental on-gating currents over a wide potential range. Such models are useful in determining state-dependent mechanisms of open and closed channel block of cardiac K+ channels.

ω-Conotoxin GVIA Alters Gating Charge Movement of N-Type (CaV2.2) Calcium Channels

2009 ◽  
Vol 101 (1) ◽  
pp. 332-340 ◽  
Author(s):  
Viktor Yarotskyy ◽  
Keith S. Elmslie
Keyword(s):  
Hek293 Cells ◽  
Charge Movement ◽  
Gating Current ◽  
Gating Currents ◽  
Current Time ◽  
Gating Charge ◽  
Channel Inhibition ◽  
Significant Difference ◽  
Human Use ◽  
Gating Modulation

ω-conotoxin GVIA (ωCTX) is a specific blocker of N-type calcium (CaV2.2) channels that inhibits neuropathic pain. While the toxin appears to be an open channel blocker, we show that N-channel gating charge movement is modulated. Gating currents were recorded from N-channels expressed along with ß2a and α2δ subunits in HEK293 cells in external solutions containing either lanthanum and magnesium (La-Mg) or 5 mM Ca2+ plus ωCTX (ωCTX-Ca). A comparison showed that ωCTX induced a 10-mV right shift in the gating charge versus voltage ( Q- V) relationship, smaller off-gating current time constant (τ QOff), a lower τ QOff voltage dependence, and smaller on-gating current ( QOn) τ. We also examined gating current in La-Mg plus ωCTX and found no significant difference from that in ωCTX-Ca; this demonstrates that the modulation was induced by the toxin. A model with strongly reduced open-state occupancy reproduced the ωCTX effect on gating current and showed that the gating modulation alone would inhibit N-current by 50%. This mechanism of N-channel inhibition could be exploited to develop novel analgesics that induce only a partial block of N-current, which may limit some of the side effects associated with the toxin analgesic currently approved for human use (i.e., Prialt).

scholarly journals Distribution and kinetics of membrane dielectric polarization. II. Frequency domain studies of gating currents.

1982 ◽  
Vol 79 (1) ◽  
pp. 41-67 ◽  
Author(s):  
J M Fernández ◽  
F Bezanilla ◽  
R E Taylor
Keyword(s):  
Giant Axon ◽  
Pulse Method ◽  
Dielectric Polarization ◽  
Gating Currents ◽  
Maximum Change ◽  
Dependent Part ◽  
Ionic Conductances ◽  
Voltage Dependent ◽  
Kinetics Of ◽  
Bell Shaped Curve

We have studied the admittance of the membrane of squid giant axon under voltage clamp in the absence of ionic conductances in the range of 0-12 kHz for membrane potentials (V) between --130 and 70 mV. The admittance was measured at various holding potentials (HP) or 155 ms after pulsing from a given holding potential. Standard P/4 procedure was used to study gating currents in the same axons. We found that the membrane capacity Cm (omega) is voltage as well as frequency dependent. For any given V, the voltage-dependent part of the membrane capacitance has a maximum as the frequency approaches zero and requires at least a two-time constant equivalent circuit to be described. When the holding potential is varied, the voltage-dependent capacitance follows a bell-shaped curve with a maximum change of 0.15 muF/cm2 at about --60 mV. With the pulse method, the maximum is at --40 mV for HP = --70 and it shifts to --70 mV for HP = 0. The shift in the maximum of the voltage-dependent capacitance is consistent with the shift in the charge (Q) vs. V curve observed in our experiments with regular P/4 procedure when the HP is varied. Our data can be explained qualitatively by a four-state model for the sodium channel gating, where a charged particle can move within the field and interact with another particle not affected by the field.

scholarly journals Voltage-dependent open-state inactivation of cardiac sodium channels: gating current studies with Anthopleurin-A toxin.

1995 ◽  
Vol 106 (4) ◽  
pp. 617-640 ◽  
Author(s):  
M F Sheets ◽  
D A Hanck
Keyword(s):  
Time Course ◽  
Voltage Dependence ◽  
Na Channel ◽  
Total Charge ◽  
Na Channels ◽  
Gating Currents ◽  
Gating Charge ◽  
Cardiac Purkinje Cells ◽  
Voltage Dependent ◽  
Cardiac Sodium Channels

The gating charge and voltage dependence of the open state to the inactivated state (O-->I) transition was measured for the voltage-dependent mammalian cardiac Na channel. Using the site 3 toxin, Anthopleurin-A (Ap-A), which selectively modifies the O-->I transition (see Hanck, D. A., and M. F. Sheets. 1995. Journal of General Physiology. 106:601-616), we studied Na channel gating currents (Ig) in voltage-clamped single canine cardiac Purkinje cells at approximately 12 degrees C. Comparison of Ig recorded in response to step depolarizations before and after modification by Ap-A toxin showed that toxin-modified gating currents decayed faster and had decreased initial amplitudes. The predominate change in the charge-voltage (Q-V) relationship was a reduction in gating charge at positive potentials such that Qmax was reduced by 33%, and the difference between charge measured in Ap-A toxin and in control represented the gating charge associated with Na channels undergoing inactivation by O-->I. By comparing the time course of channel activation (represented by the gating charge measured in Ap-A toxin) and gating charge associated with the O-->I transition (difference between control and Ap-A charge), the influence of activation on the time course of inactivation could be accounted for and the inherent voltage dependence of the O-->I transition determined. The O-->I transition for cardiac Na channels had a valence of 0.75 e-. The total charge of the cardiac voltage-gated Na channel was estimated to be 5 e-. Because charge is concentrated near the opening transition for this isoform of the channel, the time constant of the O-->I transition at 0 mV could also be estimated (0.53 ms, approximately 12 degrees C). Prediction of the mean channel open time-voltage relationship based upon the magnitude and valence of the O-->C and O-->I rate constants from INa and Ig data matched data previously reported from single Na channel studies in heart at the same temperature.

scholarly journals Gating of the Bacterial Sodium Channel, NaChBac

2004 ◽  
Vol 124 (4) ◽  
pp. 349-356 ◽  
Author(s):  
Alexey Kuzmenkin ◽  
Francisco Bezanilla ◽  
Ana M. Correa
Keyword(s):  
Sodium Channel ◽  
Mammalian Cells ◽  
Ionic Current ◽  
Bacillus Halodurans ◽  
Kinetic Properties ◽  
Charge Movement ◽  
Gating Current ◽  
Gating Currents ◽  
Charge Voltage ◽  
Gating Charge

The bacterial sodium channel, NaChBac, from Bacillus halodurans provides an excellent model to study structure–function relationships of voltage-gated ion channels. It can be expressed in mammalian cells for functional studies as well as in bacterial cultures as starting material for protein purification for fine biochemical and biophysical studies. Macroscopic functional properties of NaChBac have been described previously (Ren, D., B. Navarro, H. Xu, L. Yue, Q. Shi, and D.E. Clapham. 2001. Science. 294:2372–2375). In this study, we report gating current properties of NaChBac expressed in COS-1 cells. Upon depolarization of the membrane, gating currents appeared as upward inflections preceding the ionic currents. Gating currents were detectable at −90 mV while holding at −150 mV. Charge–voltage (Q–V) curves showed sigmoidal dependence on voltage with gating charge saturating at −10 mV. Charge movement was shifted by −22 mV relative to the conductance–voltage curve, indicating the presence of more than one closed state. Consistent with this was the Cole-Moore shift of 533 μs observed for a change in preconditioning voltage from −160 to −80 mV. The total gating charge was estimated to be 16 elementary charges per channel. Charge immobilization caused by prolonged depolarization was also observed; Q–V curves were shifted by approximately −60 mV to hyperpolarized potentials when cells were held at 0 mV. The kinetic properties of NaChBac were simulated by simultaneous fit of sodium currents at various voltages to a sequential kinetic model. Gating current kinetics predicted from ionic current experiments resembled the experimental data, indicating that gating currents are coupled to activation of NaChBac and confirming the assertion that this channel undergoes several transitions between closed states before channel opening. The results indicate that NaChBac has several closed states with voltage-dependent transitions between them realized by translocation of gating charge that causes activation of the channel.

scholarly journals Allosteric Voltage Gating of Potassium Channels II

1999 ◽  
Vol 114 (2) ◽  
pp. 305-336 ◽  
Author(s):  
Frank T. Horrigan ◽  
Richard W. Aldrich
Keyword(s):  
Preceding Paper ◽  
Voltage Sensor ◽  
Voltage Gating ◽  
Total Charge ◽  
Charge Movement ◽  
Gating Currents ◽  
Open Probability ◽  
K Channels ◽  
Virtual Absence ◽  
Gating Charge

Large-conductance Ca2+-activated K+ channels can be activated by membrane voltage in the absence of Ca2+ binding, indicating that these channels contain an intrinsic voltage sensor. The properties of this voltage sensor and its relationship to channel activation were examined by studying gating charge movement from mSlo Ca2+-activated K+ channels in the virtual absence of Ca2+ (<1 nM). Charge movement was measured in response to voltage steps or sinusoidal voltage commands. The charge–voltage relationship (Q–V) is shallower and shifted to more negative voltages than the voltage-dependent open probability (G–V). Both ON and OFF gating currents evoked by brief (0.5-ms) voltage pulses appear to decay rapidly (τON = 60 μs at +200 mV, τOFF = 16 μs at −80 mV). However, QOFF increases slowly with pulse duration, indicating that a large fraction of ON charge develops with a time course comparable to that of IK activation. The slow onset of this gating charge prevents its detection as a component of IgON, although it represents ∼40% of the total charge moved at +140 mV. The decay of IgOFF is slowed after depolarizations that open mSlo channels. Yet, the majority of open channel charge relaxation is too rapid to be limited by channel closing. These results can be understood in terms of the allosteric voltage-gating scheme developed in the preceding paper (Horrigan, F.T., J. Cui, and R.W. Aldrich. 1999. J. Gen. Physiol. 114:277–304). The model contains five open (O) and five closed (C) states arranged in parallel, and the kinetic and steady-state properties of mSlo gating currents exhibit multiple components associated with C–C, O–O, and C–O transitions.

scholarly journals Gating charge displacement in a monomeric voltage-gated proton (Hv1) channel

2018 ◽  
Vol 115 (37) ◽  
pp. 9240-9245 ◽  
Author(s):  
Emerson M. Carmona ◽  
H. Peter Larsson ◽  
Alan Neely ◽  
Osvaldo Alvarez ◽  
Ramon Latorre ◽  
...  
Keyword(s):  
Conformational Changes ◽  
Time Course ◽  
Voltage Sensor ◽  
Total Charge ◽  
Gating Currents ◽  
Voltage Gated ◽  
Central Transition ◽  
Physiological Processes ◽  
Gating Charge ◽  
Voltage Dependent

The voltage-gated proton (Hv1) channel, a voltage sensor and a conductive pore contained in one structural module, plays important roles in many physiological processes. Voltage sensor movements can be directly detected by measuring gating currents, and a detailed characterization of Hv1 charge displacements during channel activation can help to understand the function of this channel. We succeeded in detecting gating currents in the monomeric form of the Ciona-Hv1 channel. To decrease proton currents and better separate gating currents from ion currents, we used the low-conducting Hv1 mutant N264R. Isolated ON-gating currents decayed at increasing rates with increasing membrane depolarization, and the amount of gating charges displaced saturates at high voltages. These are two hallmarks of currents arising from the movement of charged elements within the boundaries of the cell membrane. The kinetic analysis of gating currents revealed a complex time course of the ON-gating current characterized by two peaks and a marked Cole–Moore effect. Both features argue that the voltage sensor undergoes several voltage-dependent conformational changes during activation. However, most of the charge is displaced in a single central transition. Upon voltage sensor activation, the charge is trapped, and only a fast component that carries a small percentage of the total charge is observed in the OFF. We hypothesize that trapping is due to the presence of the arginine side chain in position 264, which acts as a blocking ion. We conclude that the movement of the voltage sensor must proceed through at least five states to account for our experimental data satisfactorily.

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