Ion permeation mechanism of the potassium channel

Ion-selective channels enable the specific permeation of ions through cell membranes and provide the basis of several important biological functions; for example, electric signalling in the nervous system. Although a large amount of electrophysiological data is available, the molecular mechanisms by which these channels can mediate ion transport remain a significant unsolved problem. With the recently determined crystal structure of the representative K+ channel (KcsA) from Streptomyces lividans, it becomes possible to examine ion conduction pathways on a microscopic level. K+ channels utilize multi-ion conduction mechanisms, and the three-dimensional structure also shows several ions present in the channel. Here we report results from molecular dynamics free energy perturbation calculations that both establish the nature of the multiple ion conduction mechanism and yield the correct ion selectivity of the channel. By evaluating the energetics of all relevant occupancy states of the selectivity filter, we find that the favoured conduction pathway involves transitions only between two main states with a free difference of about 5 kcal mol(-1). Other putative permeation pathways can be excluded because they would involve states that are too high in energy.     

Control of ion selectivity in potassium channels by electrostatic and dynamic properties of carbonyl ligands

Potassium channels are essential for maintaining a normal ionic balance across cell membranes. Central to this function is the ability of such channels to support transmembrane ion conduction at nearly diffusion-limited rates while discriminating for K+ over Na+ by more than a thousand-fold. This selectivity arises because the transfer of the K+ ion into the channel pore is energetically favoured, a feature commonly attributed to a structurally precise fit between the K+ ion and carbonyl groups lining the rigid and narrow pore. But proteins are relatively flexible structures that undergo rapid thermal atomic fluctuations larger than the small difference in ionic radius between K+ and Na+. Here we present molecular dynamics simulations for the potassium channel KcsA, which show that the carbonyl groups coordinating the ion in the narrow pore are indeed very dynamic ('liquid-like') and that their intrinsic electrostatic properties control ion selectivity. This finding highlights the importance of the classical concept of field strength. Selectivity for K+ is seen to emerge as a robust feature of a flexible fluctuating pore lined by carbonyl groups.     

Ion conduction pore is conserved among potassium channels.

Potassium channels, a group of specialized membrane proteins, enable K+ ions to flow selectively across cell membranes. Transmembrane K+ currents underlie electrical signalling in neurons and other excitable cells. The atomic structure of a bacterial K+ channel pore has been solved by means of X-ray crystallography. To the extent that the prokaryotic pore is representative of other K+ channels, this landmark achievement has profound implications for our general understanding of K+ channels. But serious doubts have been raised concerning whether the prokaryotic K+ channel pore does actually represent those of eukaryotes. Here we have addressed this fundamental issue by substituting the prokaryotic pore into eukaryotic voltage-gated and inward-rectifier K+ channels. The resulting chimaeras retain the respective functional hallmarks of the eukaryotic channels, which indicates that the ion conduction pore is indeed conserved among K+ channels.     

Energetic optimization of ion conduction rate by the K+ selectivity filter.

The K+ selectivity filter catalyses the dehydration, transfer and rehydration of a K+ ion in about ten nanoseconds. This physical process is central to the production of electrical signals in biology. Here we show how nearly diffusion-limited rates are achieved, by analysing ion conduction and the corresponding crystallographic ion distribution in the selectivity filter of the KcsA K+ channel. Measurements with K+ and its slightly larger analogue, Rb+, lead us to conclude that the selectivity filter usually contains two K+ ions separated by one water molecule. The two ions move in a concerted fashion between two configurations, K+-water-K+-water (1,3 configuration) and water-K+-water-K+ (2,4 configuration), until a third ion enters, displacing the ion on the opposite side of the queue. For K+, the energy difference between the 1,3 and 2,4 configurations is close to zero, the condition of maximum conduction rate. The energetic balance between these configurations is a clear example of evolutionary optimization of protein function.     

在Gramicidin膜通道中碱金属离子与多肽基团之间的相互作用

以Grimicidin A做为生物膜金属离子通道模型,在给定的通道结构参数条件下,用量子化学ASED-MO法研究了K~+,Na~+离子在通道内沿中心轴移动时,能量剖面,金属离子与肽骨架上各原子的相互作用规律。发现(1)Na~+离子在通道中总能量的下降较K~+离子情况的低,但受到周围的排斥作用较前者大;(2)金属离子与通道上原子的排斥能在中间区域表现为小波动变化,与前人结论是一致的。着重分析骨架原子的净电荷分布及其受金属离子的影响,讨论了金属离子与骨架原子排斥能周期性变化的原因。     

Crystal structure and mechanism of a calcium-gated potassium channel

Ion channels exhibit two essential biophysical properties; that is, selective ion conduction, and the ability to gate-open in response to an appropriate stimulus. Two general categories of ion channel gating are defined by the initiating stimulus: ligand binding (neurotransmitter- or second-messenger-gated channels) or membrane voltage (voltage-gated channels). Here we present the structural basis of ligand gating in a K(+) channel that opens in response to intracellular Ca(2+). We have cloned, expressed, analysed electrical properties, and determined the crystal structure of a K(+) channel (MthK) from Methanobacterium thermoautotrophicum in the Ca(2+)-bound, opened state. Eight RCK domains (regulators of K(+) conductance) form a gating ring at the intracellular membrane surface. The gating ring uses the free energy of Ca(2+) binding in a simple manner to perform mechanical work to open the pore.     

Na0.54Bi0.46Ti0.96Al0.04O2.94氧离子导体制备与性能研究

采用传统的固相反应法合成Na0.54Bi0.46Ti0.96Al0.04O2.94氧离子导体,借助于交流阻抗谱和介电弛豫谱分别研究了钠和铝的双掺杂对Na0.5Bi0.5TiO3材料电学性能及氧离子扩散的影响。在400℃时,Na0.54Bi0.46Ti0.96Al0.04O2.94材料的晶粒电导率可以达到1.51×10-3 S/cm,是Na0.5Bi0.5TiO3材料电导率的5.5倍。在Na0.54Bi0.46Ti0.96Al0.04O2.94材料中观察到一个与氧离子弛豫相关的介电弛豫峰,弛豫参数为E= 0.80 eV和t0= 6.12×10-13 s,氧离子在Na0.54Bi0.46Ti0.96Al0.04O2.94材料中主要通过Na-Bi-Ti的路径进行扩散迁移的。结合结构参数容忍因子及自由体积的分析,钠和铝的双掺杂改善了氧离子在Na0.5Bi0.5TiO3材料中的扩散通道,但是铝的引入一定程度上提高了氧空位扩散的能量壁垒。     

Conformational changes associated with ion permeation in L-type calcium channels

The mechanism by which ions deliver their message to effector proteins involves a change in the protein conformation which is induced by the specific interaction of the ion with its binding site on the protein. In the case of an ion-channel protein, conformational changes induced by permeant ions and the consequences for channel function have received little attention. Here we report that binding of permeant cations to an intra-channel binding site of the dihydropyridine (DHP)-sensitive (L-type) Ca2+ channel leads to a conformational change which destabilizes the protonated state of a group on the external channel surface, and can shift its apparent pK value by more than 2 pH units. The lifetime of the protonated state correlates with the occupancy of an intra-channel binding site by the permeant cation. The demonstration of such conformational changes in a channel protein induced by the permeant ion has important implications for realistic models of the mechanism of ion permeation.     

Structure of a potentially open state of a proton-activated pentameric ligand-gated ion channel

The X-ray structure of a pentameric ligand-gated ion channel from Erwinia chrysanthemi (ELIC) has recently provided structural insight into this family of ion channels at high resolution. The structure shows a homo-pentameric protein with a barrel-stave architecture that defines an ion-conduction pore located on the fivefold axis of symmetry. In this structure, the wide aqueous vestibule that is encircled by the extracellular ligand-binding domains of the five subunits narrows to a discontinuous pore that spans the lipid bilayer. The pore is constricted by bulky hydrophobic residues towards the extracellular side, which probably serve as barriers that prevent the diffusion of ions. This interrupted pore architecture in ELIC thus depicts a non-conducting conformation of a pentameric ligand-gated ion channel, the thermodynamically stable state in the absence of bound ligand. As ligand binding promotes pore opening in these ion channels and the specific ligand for ELIC has not yet been identified, we have turned our attention towards a homologous protein from the cyanobacterium Gloebacter violaceus (GLIC). GLIC was shown to form proton-gated channels that are activated by a pH decrease on the extracellular side and that do not desensitize after activation. Both prokaryotic proteins, ELIC and GLIC form ion channels that are selective for cations over anions with poor discrimination among monovalent cations, characteristics that resemble the conduction properties of the cation-selective branch of the family that includes acetylcholine and serotonin receptors. Here we present the X-ray structure of GLIC at 3.1 A resolution. The structure reveals a conformation of the channel that is distinct from ELIC and that probably resembles the open state. In combination, both structures suggest a novel gating mechanism for pentameric ligand-gated ion channels where channel opening proceeds by a change in the tilt of the pore-forming helices.     

The role of protein surface charges in ion binding

Protein engineering is a means of probing the role of electrostatic interactions in protein functions; this elegant technique has been applied to the elucidation of electrostatic effects in enzyme catalysis. Here we show how the use of mutant proteins allows the determination of the contributions of individual charges to the free energy of ion binding to proteins. We have investigated the importance of three negatively charged side chains in the binding of Ca2+ to bovine calbindin D9K (ref.2): these are clustered around the calcium sites but are not directly involved as ligands. Each of these charges is found to contribute approximately 7 kJ mol-1 to the free energy of binding of two Ca2+ ions and to affect the cooperativity of Ca2+ binding. The influence of surface charges on ion binding to proteins may be more common than generally supposed and could have important consequences for protein function.     

Mechanism of ion permeation through calcium channels

Calcium channels carry out vital functions in a wide variety of excitable cells but they also face special challenges. In the medium outside the channel, Ca2+ ions are vastly outnumbered by other ions. Thus, the calcium channel must be extremely selective if it is to allow Ca2+ influx rather than a general cation influx. In fact, calcium channels show a much greater selectivity for Ca2+ than sodium channels do for Na+ despite the high flux that open Ca channels can support. Relatively little is known about the mechanism of ion permeation through Ca channels. Earlier models assumed ion independence or single-ion occupancy. Here we present evidence for a novel hypothesis of ion movement through Ca channels, based on measurements of Ca channel activity at the level of single cells or single channels. Our results indicate that under physiological conditions, the channel is occupied almost continually by one or more Ca2+ ions which, by electrostatic repulsion, guard the channel against permeation by other ions. On the other hand, repulsion between Ca2+ ions allows high throughput rates and tends to prevent saturation with calcium.     

The twisted ion-permeation pathway of a resting voltage-sensing domain

Proteins containing voltage-sensing domains (VSDs) translate changes in membrane potential into changes in ion permeability or enzymatic activity. In channels, voltage change triggers a switch in conformation of the VSD, which drives gating in a separate pore domain, or, in channels lacking a pore domain, directly gates an ion pathway within the VSD. Neither mechanism is well understood. In the Shaker potassium channel, mutation of the first arginine residue of the S4 helix to a smaller uncharged residue makes the VSD permeable to ions ('omega current') in the resting conformation ('S4 down'). Here we perform a structure-guided perturbation analysis of the omega conductance to map its VSD permeation pathway. We find that there are four omega pores per channel, which is consistent with one conduction path per VSD. Permeating ions from the extracellular medium enter the VSD at its peripheral junction with the pore domain, and then plunge into the core of the VSD in a curved conduction pathway. Our results provide a model of the resting conformation of the VSD.     

Atomic structure of a Na+- and K+-conducting channel

Ion selectivity is one of the basic properties that define an ion channel. Most tetrameric cation channels, which include the K+, Ca2+, Na+ and cyclic nucleotide-gated channels, probably share a similar overall architecture in their ion-conduction pore, but the structural details that determine ion selection are different. Although K+ channel selectivity has been well studied from a structural perspective, little is known about the structure of other cation channels. Here we present crystal structures of the NaK channel from Bacillus cereus, a non-selective tetrameric cation channel, in its Na+- and K+-bound states at 2.4 A and 2.8 A resolution, respectively. The NaK channel shares high sequence homology and a similar overall structure with the bacterial KcsA K+ channel, but its selectivity filter adopts a different architecture. Unlike a K+ channel selectivity filter, which contains four equivalent K+-binding sites, the selectivity filter of the NaK channel preserves the two cation-binding sites equivalent to sites 3 and 4 of a K+ channel, whereas the region corresponding to sites 1 and 2 of a K+ channel becomes a vestibule in which ions can diffuse but not bind specifically. Functional analysis using an 86Rb flux assay shows that the NaK channel can conduct both Na+ and K+ ions. We conclude that the sequence of the NaK selectivity filter resembles that of a cyclic nucleotide-gated channel and its structure may represent that of a cyclic nucleotide-gated channel pore.     

Chemistry of ion coordination and hydration revealed by a K+ channel-Fab complex at 2.0 A resolution.

Ion transport proteins must remove an ion's hydration shell to coordinate the ion selectively on the basis of its size and charge. To discover how the K+ channel solves this fundamental aspect of ion conduction, we solved the structure of the KcsA K+ channel in complex with a monoclonal Fab antibody fragment at 2.0 A resolution. Here we show how the K+ channel displaces water molecules around an ion at its extracellular entryway, and how it holds a K+ ion in a square antiprism of water molecules in a cavity near its intracellular entryway. Carbonyl oxygen atoms within the selectivity filter form a very similar square antiprism around each K+ binding site, as if to mimic the waters of hydration. The selectivity filter changes its ion coordination structure in low K+ solutions. This structural change is crucial to the operation of the selectivity filter in the cellular context, where the K+ ion concentration near the selectivity filter varies in response to channel gating.     

Alteration of ionic selectivity of a K+ channel by mutation of the H5 region

The high ionic selectivity of K+ channels is a unifying feature of this diverse class of membrane proteins. Though K+ channels differ widely in regulation and kinetics, physiological studies have suggested a common structure: a single file pore containing multiple ion-binding sites and having broader vestibules at both ends. We have used site-directed mutagenesis and single-channel recordings to identify a molecular region that influences ionic selectivity in a cloned A-type K+ channel from Drosophila. Single amino-acid substitutions in H5, the fifth hydrophobic region, enhanced the passage of NH4+ and Rb+, ions with diameters larger than K+, without compromising the ability of the channel to exclude the smaller cation, Na+. The mutations that substantially altered selectivity had little effect on the gating properties of the channel. We conclude that the H5 region is likely to line the pore of the K+ channel.     

From molecule to malady

Ion channels are membrane proteins, found in virtually all cells, that are of crucial physiological importance. In the past decade, an explosion in the number of crystal structures of ion channels has led to a marked increase in our understanding of how ion channels open and close, and select between permeant ions. There has been a parallel advance in research on channelopathies (diseases resulting from impaired channel function), and mutations in over 60 ion-channel genes are now known to cause human disease. Characterization of their functional consequences has afforded unprecedented and unexpected insights into ion-channel mechanisms and physiological roles.     

基于微观机理的页岩气运移分析

认识气体在页岩孔隙中的运移机理对页岩气开采具有重要的科学意义.页岩作为一种致密岩石,孔隙尺寸分布主要集中在几纳米到百纳米之间,小孔隙尺寸与气体的平均分子自由程在同一个数量级,气体与孔隙边壁的碰撞对流动起到控制作用.本文针对页岩气开采过程中孔隙中气体流动过程,建立了考虑气体滑移、Knudsen扩散、Langmuir等温吸附、孔隙压缩等过程的多场耦合控制方程.分析了流态变化对滑移效应的影响,得到了考虑滑移效应的临界孔径,并针对实际中不同页岩储层有机质含量的差异,分析了解吸机制对页岩气产气率、产气量的贡献.研究还表明孔隙压缩性对产气率影响显著,通过考虑开采过程中孔隙压缩,可以更真实地反映页岩气运移过程.     

Aggregation and vesiculation of membrane proteins by curvature-mediated interactions

Membrane remodelling plays an important role in cellular tasks such as endocytosis, vesiculation and protein sorting, and in the biogenesis of organelles such as the endoplasmic reticulum or the Golgi apparatus. It is well established that the remodelling process is aided by specialized proteins that can sense as well as create membrane curvature, and trigger tubulation when added to synthetic liposomes. Because the energy needed for such large-scale changes in membrane geometry significantly exceeds the binding energy between individual proteins and between protein and membrane, cooperative action is essential. It has recently been suggested that curvature-mediated attractive interactions could aid cooperation and complement the effects of specific binding events on membrane remodelling. But it is difficult to experimentally isolate curvature-mediated interactions from direct attractions between proteins. Moreover, approximate theories predict repulsion between isotropically curving proteins. Here we use coarse-grained membrane simulations to show that curvature-inducing model proteins adsorbed on lipid bilayer membranes can experience attractive interactions that arise purely as a result of membrane curvature. We find that once a minimal local bending is realized, the effect robustly drives protein cluster formation and subsequent transformation into vesicles with radii that correlate with the local curvature imprint. Owing to its universal nature, curvature-mediated attraction can operate even between proteins lacking any specific interactions, such as newly synthesized and still immature membrane proteins in the endoplasmic reticulum.     

离子匹配精细水驱提高采收率机理研究

水驱是油田开发的主要技术,但常规水驱只是通过向地层补充能量的方式提高采收率,而离子匹配水驱技术则是基于油藏介质中固液微界面作用强的特点,通过对注入水离子类型和强度的精确离子匹配实现剥离残余油膜提高驱油效率。以西峰油田为例,结合室内驱油实验、Zeta电位测量、原子力显微分析和界面作用力数值计算等方法,系统研究了离子匹配精细水驱技术提高低渗油藏采收率的主控因素。结果表明,随着注入水离子类型的调整和离子浓度的改变,在二次采油和在三次采油模式下,离子匹配精细水驱分别比模拟地层水驱提高采出程度15.6和9.8个百分点。其中,界面的Zeta电位和分离压的大小与离子匹配精细水的离子类型关系密切。相同离子浓度情况下,数值计算与原子力显微分析实验所得结果均表明,Na⁺比Ca²⁺和Mg²⁺的分离压高,从而表现出了更有利于从岩石表面剥离油膜的能力;同时,随着注入水离子浓度的降低,盐水原油岩石界面的Zeta电位负值和分离压均呈增大的趋势,油和岩石表面之间的斥力增大,致使残余油更容易从岩石表面剥落,离子匹配精细水驱有助于提高水驱油藏的开发效果。     

ATP-sensitive K+ channel in the mitochondrial inner membrane.

Mitochondria take up and extrude various inorganic and organic ions, as well as larger substances such as proteins. The technique of patch clamping should provide real-time information on such transport and on energy transduction in oxidative phosphorylation. It has been applied to detect microscopic currents from mitochondrial membranes and conductances of ion channels in the 5-1,000 pS range in the outer and inner membranes. These pores are not, however, selective for particular ions. Here we use fused giant mitoplasts prepared from rat liver mitochondria to identify a small conductance channel highly selective for K+ in the inner mitochondrial membrane. This channel can be reversibly inactivated by ATP applied to the matrix side under inside-out patch configuration; it is also inhibited by 4-aminopyridine and by glybenclamide. The slope conductance of the unitary currents measured at negative membrane potentials was 9.7 +/- 1.0 pS (mean +/- s.d., n = 6) when the pipette solution contained 100 mM K+ and the bathing solution 33.3 mM K+. Our results indicate that mitochondria depolarize by generating a K+ conductance when ATP in the matrix is deficient.