Potassium channels: complete and undistorted

The recently determined structure of a mammalian voltage-gated potassium channel has important implications for our understanding of voltage-sensing and gating mechanisms in channels. It is also the first crystal structure of an overexpressed eukaryotic membrane protein.     

Potassium channels

The atomic structures of K+ channels have added a new dimension to our understanding of K+ channel function. I will briefly review how structures have influenced our views on ion conduction, gating of the pore, and voltage sensing.     

Potassium channels and uterine function

Ion channels are effector proteins that mediate uterine excitability throughout gestation. This review will focus primarily on the role of potassium channels in regulating myometrial tone in pregnancy and labor contractions. During gestation, potassium channels maintain the uterus in a state of quiescence by contributing to the resting membrane potential and counteracting contractile stimuli. This review summarizes the current knowledge about the significance of the potassium channels in maintaining a normal gestational period and initiating labor contractions at term.     

Components of gating charge movement and S4 voltage-sensor exposure during activation of hERG channels

The human ether-á-go-go–related gene (hERG) K⁺ channel encodes the pore-forming α subunit of the rapid delayed rectifier current, I_Kr, and has unique activation gating kinetics, in that the α subunit of the channel activates and deactivates very slowly, which focuses the role of I_Kr current to a critical period during action potential repolarization in the heart. Despite its physiological importance, fundamental mechanistic properties of hERG channel activation gating remain unclear, including how voltage-sensor movement rate limits pore opening. Here, we study this directly by recording voltage-sensor domain currents in mammalian cells for the first time and measuring the rates of voltage-sensor modification by [2-(trimethylammonium)ethyl] methanethiosulfonate chloride (MTSET). Gating currents recorded from hERG channels expressed in mammalian tsA201 cells using low resistance pipettes show two charge systems, defined as Q₁ and Q₂, with V_1/2’s of −55.7 (equivalent charge, z = 1.60) and −54.2 mV (z = 1.30), respectively, with the Q₂ charge system carrying approximately two thirds of the overall gating charge. The time constants for charge movement at 0 mV were 2.5 and 36.2 ms for Q₁ and Q₂, decreasing to 4.3 ms for Q₂ at +60 mV, an order of magnitude faster than the time constants of ionic current appearance at these potentials. The voltage and time dependence of Q₂ movement closely correlated with the rate of MTSET modification of I521C in the outermost region of the S4 segment, which had a V_1/2 of −64 mV and time constants of 36 ± 8.5 ms and 11.6 ± 6.3 ms at 0 and +60 mV, respectively. Modeling of Q₁ and Q₂ charge systems showed that a minimal scheme of three transitions is sufficient to account for the experimental findings. These data point to activation steps further downstream of voltage-sensor movement that provide the major delays to pore opening in hERG channels.     

Interaction between extracellular Hanatoxin and the resting conformation of the voltage-sensor paddle in Kv channels

In voltage-activated potassium (Kv) channels, basic residues in S4 enable the voltage-sensing domain to move in response to membrane depolarization and thereby trigger the activation gate to open. In the X-ray structure of the KvAP channel, the S4 helix is located near the intracellular boundary of the membrane where it forms a "voltage-sensor paddle" motif with the S3b helix. It has been proposed that the paddle is lipid-exposed and that it translocates through the membrane as it activates. We studied the interaction of externally applied Hanatoxin with the voltage-sensor paddle in Kv channels and show that the toxin binds tightly even at negative voltages where the paddle is resting and the channel is closed. Moreover, measurements of gating charge movement suggest that Hanatoxin interacts with and stabilizes the resting paddle. These findings point to an extracellular location for the resting conformation of the voltage-sensor paddle and constrain its transmembrane movements during activation.     

Potassium channels: the importance of transport signals

The number, type and distribution of ion channels on a neuron's surface determine its electrical response to stimulation. One way that a cell determines how many molecules of each channel type are sent to the surface has been eludicated in a recent study of intrinsic protein transport signals within potassium channels.     

Potassium channels in Eremosphaera viridis

To characterize the assumed potassium channels in the plasma membrane of the green alga Eremosphaera viridis (Köhler et al. 1985), current-voltage (I/V)-curves under resting conditions and during an action-potential-like response (CAP) were constructed using voltage- and current-clamp techniques. Under resting conditions the I/V-curves of Eremosphaera showed a distinct upward bending when approaching zero mV, a nearly straight line in the medium part and a downward bending during strong hyperpolarization. Measurements in light and darkness frequently displayed a parallel shift of the I/V-curve in the middle part, indicating a current source which is slowed down by light-off. Using the voltage-clamp technique, N-shaped I/V-curves were sometimes observed. The potassium concentration outside influenced the downward-bending part of the I/V-curve whereas the tetraethylammonium cation, known to block potassium channels, reduced the upward-bending part in particular. A change in external pH, either to pH 7 or pH 3.1 from a standard pH 5.5, caused an increase in conductivity. Chemically induced action potentials were released in Eremosphaera under voltage-clamp conditions by light-off and there was both a current flow and an increase in conductivity during the CAP. Clamping the membrane potential at a value more negative than Nernst potential of potassium revealed an inward current, whereas clamping at a more-positive value revealed an outward current. The experiments demonstrate that there is no threshold potential in releasing a CAP. The I/V-curves performed under current clamp at the peak of CAP verify a previously found increased conductivity with hyper- or depolarization depending on the external potassium concentration. These experiments provide further evidence that in Eremosphaera potassium channels are involved in the CAP caused by a light-off signal. Additional experiments indicate that after light-off a transient acidification of the cytoplasm takes place in correlation with the CAP and the opening of potassium channels. A preliminary battery model is discussed to understand the role of potassium channels during a CAP in pH-regulation of the cytoplasm.Abbreviations AP classical action potential - CAP chemically induced action potential - E_k Nernst potential of potassium - I/V-curve current-voltage curve - TEA tetraethylammonium For part I see Planta 166, 490–499     

Potassium channels in Eremosphaera viridis

The dependence of the membrane potential of Eremosphaera viridis on different external concentrations of potassium, sodium, calcium, and protons was compared with the diffusion potential measured in the dark and in the presence of NaN₃. In contrast to some other algae, the membrane potential in the light as well as in the dark seemed to be predominantly determined by the calculated diffusion potential and less by an electrogenic pump which, however, seemed to be involved at potassium concentrations >1 mol·m^-3 and at higher pH_os (>pH 6). Furthermore, some characteristics of an action-potential-like response (CAP) triggered by light-off, and independent of the membrane-potential threshold value, were determined. The CAP had a delay period of 5.4 s and needed 4.5 s for polarization to a plateau. On average, the plateau held for 8.8 s and the CAP lasted 37.7 s. The peak amplitudes of CAP (P_AP) exactly followed the Nernst potential of potassium. Other cations like sodium, calcium and protons did not appreciably affect the peak amplitudes of CAP. From these and other results it can be assumed that the CAP is caused by a temporary opening of potassium channels in the plasma membrane of Eremosphaera (Köhler et al., 1983, Planta 159, 165–171). The release of a CAP by light-off has been partly explained by the participation of a transient increase of proton concentration in the cytoplasm. It was possible to trigger a CAP by external pH changes and by the addition of sodium acetate, thus supporting the hypothesis that a pH decrease in the cytoplasm may be one element of the signal transfer from the photosynthetic system to the potassium channels in the plasmalemma. Calcium also seemed to have an influence on triggering the CAP.Abbreviations and symbols CAP chemical-induced action-potential-like response - E_D calculated diffusion potential (mV) - E_D^* measured diffusion potential (mV) - E_K potassium equilibrium potential (mV) - E_m membrane potential (mV) - P_AP peak of action potential (mV)Part II will appear in Planta, Vol. 167, No. 1, 1986     

Potassium channels in plant cells

Potassium (K(+) ) is the most abundant inorganic cation in plant cells. Unlike animals, plants lack sodium/potassium exchangers. Instead, plant cells have developed unique transport systems for K(+) accumulation and release. An essential role in potassium uptake and efflux is played by potassium channels. Since the first molecular characterization of K(+) channels from Arabidopsis thaliana in 1992, a large number of studies on plant potassium channels have been conducted. Potassium channels are considered to be one of the best characterized class of membrane proteins in plants. Nevertheless, knowledge on plant potassium channels is still incomplete. This minireview focuses on recent developments in the research of potassium transport in plants with a strong focus on voltage-gated potassium channels.     

Potassium channels along the nephron

The K+ channels that are present in three different nephron segments, the Necturus proximal, Amphiuma early distal (diluting segment), and rabbit collecting tubule have been examined. Ca2+-sensitive K+ channels were present in the apical membranes of the cells lining all these segments. The channels were all voltage-sensitive and their open probability increased with membrane depolarization. Because of the ubiquitous distribution, it is suggested that this channel is responsible for K+ secretion by the nephron and that the same intracellular regulators act throughout the various segments. Basolateral K+ channels have been examined only in Necturus proximal tubules. This channel is apparently insensitive to Ca2+; the voltage dependence is exactly opposite to that of the apical K+ channels; that is, hyperpolarizing potentials caused an increase in open probability. These differences in regulatory factors permit the independent regulation of apical and basolateral membrane K+ permeabilities that must occur in renal cells.     

Potassium channels as tumour markers

An increasing number of ion channels are being found to be causally involved in diseases, giving rise to the new field of "channelopathies". Cancer is no exception, and several ion channels have been linked to tumour progression. Among them is the potassium channel EAG (Ether-a-go-go). Over 75% of tumours have been tested positive using a monoclonal antibody specific for EAG, while inhibition of this channel decreased the proliferation of EAG expressing cells. The inhibition of EAG is accomplished using RNA interference, functional anti-EAG1 antibodies, or (unspecific) EAG channel blockers. Fluorescently labelled recombinant Fab fragments recognizing EAG allow the distribution of EAG to be visualized in an in vivo mouse tumour model.     

Domain IV voltage-sensor movement is both sufficient and rate limiting for fast inactivation in sodium channels

Voltage-gated sodium channels are critical for the generation and propagation of electrical signals in most excitable cells. Activation of Na⁺ channels initiates an action potential, and fast inactivation facilitates repolarization of the membrane by the outward K⁺ current. Fast inactivation is also the main determinant of the refractory period between successive electrical impulses. Although the voltage sensor of domain IV (DIV) has been implicated in fast inactivation, it remains unclear whether the activation of DIV alone is sufficient for fast inactivation to occur. Here, we functionally neutralize each specific voltage sensor by mutating several critical arginines in the S4 segment to glutamines. We assess the individual role of each voltage-sensing domain in the voltage dependence and kinetics of fast inactivation upon its specific inhibition. We show that movement of the DIV voltage sensor is the rate-limiting step for both development and recovery from fast inactivation. Our data suggest that activation of the DIV voltage sensor alone is sufficient for fast inactivation to occur, and that activation of DIV before channel opening is the molecular mechanism for closed-state inactivation. We propose a kinetic model of sodium channel gating that can account for our major findings over a wide voltage range by postulating that DIV movement is both necessary and sufficient for fast inactivation.     

The voltage-sensor structure in a voltage-gated channel

A recent electron paramagnetic resonance study of KvAP, a prokaryotic voltage-gated channel, in its lipid native environment has revealed the location of the transmembrane segments, the connecting loops and the relative position of the voltage-sensing charges. The results confirm that the previously reported crystal structure does not represent a native conformation and give us structural constraints that will help in determining the molecular structure of the voltage sensor.     

Potassium channels in human and avian fibroblasts

The cell-attached and excised inside-out patch-clamp techniques were used to study single-channel characteristics of potassium channels in cultured human and avian fibroblasts. Six different potassium channels were distinguished with conductances of 235 +/- 25, 190 +/- 57, 114 +/- 27, 77 +/- 14, 40 +/- 6 and 21 +/- 4 pS in symmetric 140 mM potassium solutions. The channels were separable by their conductances, ion-selectivities, voltage-sensitivities and kinetic properties. All six channels were found in both fully differentiated human skin fibroblasts and primary cultures of 72 h chick sclerotome. The largest channel (235 pS) had a steep bimodal voltage dependence, being open only around the resting membrane potential. It was imperfectly selective for potassium, having a relative sodium:potassium permeability of 0.3. The 190 pS channel was very potassium-selective, had an S-shaped voltage sensitivity and was calcium-dependent. The two intermediate-size channels (114 and 77 pS) had open probabilities of less than 0.5 under all of the conditions we used. They were not completely selective for potassium and were not voltage-sensitive. The two smallest channels (40 and 21 pS) were not well characterized. They both had open probabilities of less than 0.2 and showed no evidence of voltage-sensitivity. The 40 pS channel seemed highly potassium-selective. A suction stimulus was used to test all observed channels for mechanosensitivity but none of the six potassium channels was mechanosensitive. Another small channel, with very clear mechanical sensitivity, was seen on a few occasions; this channel has not yet been characterized.     

Potassium channels as multi-ion single-file pores

A literature review reveals many lines of evidence that both delayed rectifier and inward rectifier potassium channels are multi-ion pores. These include unidirectional flux ratios given by the 2--2.5 power of the electrochemical activity ratio, very steeply voltage-dependent block with monovalent blocking ions, relief of block by permeant ions added to the side opposite from the blocking ion, rectification depending on E--EK, and a minimum in the reversal potential or conductance as external K+ ions are replaced by an equivalent concentration of T1+ ions. We consider a channel with a linear sequence of energy barriers and binding sites. The channel can be occupied by more than one ion at a time, and ions hop in single file into vacant sites with rate constants that depend on barrier heights, membrane potential, and interionic repulsion. Such multi-ion models reproduce qualitatively the special flux properties of potassium channels when the barriers for hopping out of the pore are larger than for hopping between sites within the pore and when there is repulsion between ions. These conditions also produce multiple maxima in the conductance-ion activity relationship. In agreement with Armstrong's hypothesis (1969. J. Gen. Physiol. 54:553--575), inward rectification may be understood in terms of block by an internal blocking cation. Potassium channels must have at least three sites and often contain at least two ions at a time.     

Potassium channels from chick lens epithelium

The technique of patch-voltage clamp has been used to demonstrate several different kinds of K+ channels in the apical membrane of the chick lens epithelium. These include a 200- to 250-ps Ca2+-activated channel, a 200- to 250-ps non-Ca2+-activated channel whose probability of being open increases with hyperpolarization, a 35-ps flickery channel, and a 30-ps inward rectifier, all characterized in symmetrical 150 mM K+. The inward rectifier allows little if any outward current. The probability that the channel is open increases as the membrane patch is depolarized, whereas the mean open and closed times of the channel decrease with depolarization. It is proposed that the rectification is a property of the open channel rather than of its gating. External Cs+ at micromolar concentrations produces a flickery block that increases with hyperpolarization and blocker concentration. The mean open time inside bursts decreases with increasing blocker concentration, whereas the mean intraburst closed time is unaffected. Thus, Cs+ blocks the open channel. The steepness of the voltage dependence of the block suggests that multiple occupancy of the channel is possible.     

Potassium ion channels in the plasmalemma

The potassium ion is an indispensible cytosolic component of living cells and a key osmolyte of plant cells, crossing the plasmalemma to drive physiological processes like cell growth and motor cell activity. K⁺ transport across the plasmalemma may be passive through channels, driven by the electrochemical gradient, K⁺ equilibrium potential (E_K) – membrane potential (V_m), or secondary active by coupling through a carrier to the inward driving force of H⁺ or Na⁺. Known K⁺ channels are permeable to monovalent cations, a permeability order being K⁺ > Rb⁺ > NH₄⁺ > Na⁺≥ Li⁺ > Cs⁺. The macroscopic K⁺ currents across a cell or protoplast surface commonly show rectification, i.e. a V^m-dependent conductance which in turn, may be controlled by the cytosolic activity of Ca²⁺, of K⁺, of H⁺, or by the K⁺ driving force. Analysis by the patch clamp technique reveals that plant K⁺ channels are similar to animal channels in their single channel conductance (4 to 100 pS), but different in that a given channel population slowly activates and may not inactivate at all. Single-channel kinetics reveal a broad range of open times (ms to s) and closed times (up to 100 s). Further progress in elucidating plant K⁺ channels will critically depend on molecular cloning, and the availability of channel-specific (phyto)toxins.