Control of cation permeation through the nicotinic receptor channel

We used molecular dynamics (MD) simulations to explore the transport of single cations through the channel of the muscle nicotinic acetylcholine receptor (nAChR). Four MD simulations of 16 ns were performed at physiological and hyperpolarized membrane potentials, with and without restraints of the structure, but all without bound agonist. With the structure unrestrained and a potential of −100 mV, one cation traversed the channel during a transient period of channel hydration; at −200 mV, the channel was continuously hydrated and two cations traversed the channel. With the structure restrained, however, cations did not traverse the channel at either membrane potential, even though the channel was continuously hydrated. The overall results show that cation selective transport through the nAChR channel is governed by electrostatic interactions to achieve charge selectivity, but ion translocation relies on channel hydration, facilitated by a trans-membrane field, coupled with dynamic fluctuations of the channel structure.     

Three-dimensional structure of human voltage-gated ion channel Kv10.2 studied by electron microscopy of macromolecules and molecular modeling

Three-dimensional structure of the human voltage-gated channel Kv10.2 has been elucidated for the first time using the method of electron microscopy with 2.5 nm resolution. The molecule has a distinct domain structure. For interpretation of the structure, homology modeling was used with the cAMP-dependent channel MlotiK1 (C-subunit) structure used as a template for a membrane part of the channel, homology with the structure of the human potassium channel herg (A subunits) was used for the cytoplasmic subdomains PAS-PAC, and for the cNBD domain homology with the MloK1 channel was used. The homologous transmembrane part corresponds by size to the upper part of the three-dimensional reconstruction. Cytoplasmic domains of the Kv10.2 channel form the structure built according to the ‘hanging gondola’ type that is connected with the transmembrane part of the channel by linkers. The length of linkers suggests the possibility of contacts between the C-terminal cNBD domains and N-terminal PAS-domains.     

The dipole moment of membrane proteins: potassium channel protein and beta-subunit.

The mechanism of ion channel opening is one of the most fascinating problems in membrane biology. Based on phenomenological studies, early researchers suggested that the elementary process of ion channel opening may be the intramembrane charge movement or the orientation of dipolar proteins in the channel. In spite of the far reaching significance of these hypotheses, it has not been possible to formulate a comprehensive molecular theory for the mechanism of channel opening. This is because of the lack of the detailed knowledge on the structure of channel proteins. In recent years, however, the research on the structure of channel proteins made marked advances and, at present, we are beginning to have sufficient information on the structure of some of the channel proteins, e.g. potassium-channel protein and beta-subunits. With these new information, we are now ready to have another look at the old hypothesis, in particular, the dipole moment of channel proteins being the voltage sensor for the opening and closing of ion channels. In this paper, the dipole moments of potassium channel protein and beta-subunit, are calculated using X-ray diffraction data. A large dipole moment was found for beta-subunits while the dipole moment of K-channel protein was found to be considerably smaller than that of beta-subunits. These calculations were conducted as a preliminary study of the comprehensive research on the dipolar structure of channel proteins in excitable membranes, above all, sodium channel proteins.     

Simulation of molecular dynamics of water movement in ion channels

The motion of water molecules in a gramicidin-like channel was studied by the molecular dynamics method. Water molecules are presented in the ST2 model. The structure of the channel was presented in the form of channel's helix frame possessing mobile dipole groups. The interaction of all mobile particles with the membrane channel's walls was taken into account. The calculation consisted of 50,000 integration steps of delta t = 5 x 10(-16) s which corresponded to a total elapsed time of 25 ps. It was shown that water molecules in the channel did not possess rigid spatial structure but exhibited a structure oriented along the channel axis. The motion of water molecules in the channel occurred smoothly, i.e. all water molecules did not have any deep, stable potential wells in the channel. The distribution of water molecules along the radial coordinate of the channel was estimated. Water density was shown to be maximal near the channel axis.     

Pore Structure of the Cys-loop Ligand-gated Ion Channels

The Cys-loop receptor family of ligand-gated ion channels (LGICs) play a key role in synaptic transmission in the central nervous system of animals. Recent advances have led to the elucidation of two crystal structures of related prokaryotic LGICs and the electron micrograph derived structure of the acetylcholine receptor from Torpedo marmorata. Here, we review the structural and biochemical data that form our understanding of the structure of the channel pore. We introduce original data from the glycine receptor using the substituted-cysteine accessibility technique and show that while the helical structure of the segment that surrounds the channel pore is generally agreed, the location of the channel gate, the pore diameter and the structure that forms the entry to the channel pore are likely to differ between receptors. The fundamental structural differences between anion and cation selective receptors and how these differences are related to the pore structure are also considered.     

Channel gate! Tension, leak and disclosure.

The crystal structure of a bacterial MscL shows how this homopentameric channel protein is held tightly shut to prevent leakage whilst at rest. By inference, the structure also shows how a stretch force in the lipid bilayer causes the channel to open. We now have a concrete picture as to how a stimulus 'gates' an ion channel.     

Three-dimensional structure of human Kv10.2 ion channel studied by single particle electron microscopy and molecular modeling

Here we present a three-dimensional structure of human voltage gated Kv10.2 ion channel solved at 2.5 nm resolution. We demonstrated that Kv10.2 channel structure is subdivided into two layers. For interpretation of the structure we used the homology modeling, using the transmembrane regions of MlotiK1 channel (C subunit), and cytoplasmic PAS-PAC and cNBD domains of the N-terminal tail of hERG (A subunit) and the bacterial cyclic nucleotide-activated K+ channel binding domain as the templates. The homologous transmembrane part can be fitted into the upper part of the reconstruction. The cytoplasmic domains form the structure, similar to a "hanging gondola", which is connected to the membrane-embedded domain with linkers. The length of linkers allow contacts between C-terminal cNBD domains and N-terminal PAS domains.     

Molecular dynamics simulations of wild-type and mutant forms of the Mycobacterium tuberculosis MscL channel

The crystal structure of the Mycobacterium tuberculosis homolog of the bacterial mechanosensitive channel of large conductance (Tb-MscL) provides a unique opportunity to consider mechanosensitive signal transduction at the atomic level. Molecular dynamics simulations of the Tb-MscL channel embedded in an explicit lipid bilayer and of its C-terminal helical bundle alone in aqueous solvent were performed. C-terminal calculations imply that although the helix bundle structure is relatively unstable at physiological pH, it may have been stabilized under low pH conditions such as those used in the crystallization of the channel. Specific mutations to the C-terminal region, which cause a similar conservation of the crystal structure conformation, have also been identified. Full channel simulations were performed for the wild-type channel and two experimentally characterized gain-of-function mutants, V21A and Q51E. The wild-type Tb-MscL trajectory gives insight into regions of relative structural stability and instability in the channel structure. Channel mutations led to observable changes in the trajectories, such as an alteration of intersubunit interactions in the Q51E mutant. In addition, interesting patterns of protein-lipid interactions, such as hydrogen bonding, arose in the simulations. These and other observations from the simulations are relevant to previous and ongoing experimental studies focusing on characterization of the channel.     

Potassium and sodium binding to the outer mouth of the K+ channel.

Molecular dynamics simulations of the K+ channel from Streptomyces lividans (KcsA channel) were performed in a membrane-mimetic environment with Na+ and K+ in different initial locations. The structure of the channel remained stable and well preserved for simulations lasting up to 1.5 ns. Salt bridges between Asp80 and Arg89 of neighboring subunits, not detected in the X-ray structure, enhanced the stability of the tetrameric structure. Na+ or K+ ions located in the channel vestibule lost part of their hydration shell and diffused into the channel inner pore in less than a few hundred picoseconds. This powerful catalytic action was caused by strong electrostatic interactions with Asp80 and Glu71. The hydration state of the metal ions turned out to depend significantly on the conformational flexibility of the channel. Furthermore, Na+ entered the channel inner pore bound to more water molecules than K+. The different hydration state of the two ions may be a determinant factor in the ion selectivity of the channel.     

Functional architecture of the CFTR chloride channel

Cystic fibrosis is caused by mutations in the cystic fibrosis transmembrane conductance regulator (CFTR), a member of the ATP-binding cassette (ABC) family of membrane transport proteins. CFTR is unique among ABC proteins in that it functions not as an active transporter but as an ATP-gated Cl^? channel. As an ion channel, the function of the CFTR transmembrane channel pore that mediates Cl^? movement has been studied in great detail. On the other hand, only low resolution structural data is available on the transmembrane parts of the protein. The structure of the channel pore has, however, been modeled on the known structure of active transporter ABC proteins. Currently, significant barriers exist to building a unified view of CFTR pore structure and function. Reconciling functional data on the channel with indirect structural data based on other proteins with very different transport functions and substrates has proven problematic. This review summarizes current structural and functional models of the CFTR Cl^? channel pore, including a comprehensive review of previous electrophysiological investigations of channel structure and function. In addition, functional data on the three-dimensional arrangement of pore-lining helices, as well as contemporary hypotheses concerning conformational changes in the pore that occur during channel opening and closing, are discussed. Important similarities and differences between different models of the pore highlight current gaps in our knowledge of CFTR structure and function. In order to fill these gaps, structural and functional models of the membrane-spanning pore need to become better integrated.     

Potassium channels: life in the post-structural world

More than three years have passed since the first structure of a potassium channel protein revealed fundamental molecular details of a platform for ion-selective conduction. Recent efforts have turned to understanding what this structure tells us about potassium channel structure and function in general and, most importantly, which questions remain unanswered. Successes in solving membrane protein structures are still hard won and slow. High-resolution studies of cytoplasmic channel domains and channel-associated proteins, the most tractable entry points for dissecting large, complex eukaryotic channels, are revealing a modularity of function commonly seen in many other biological systems. Studies of these domains bring into sharp focus issues of channel regulation, how these domains and associated proteins are coupled to the transmembrane domains to influence channel function, and how ion channels are integrated into cellular signaling pathways.     

Short-range molecular rearrangements in ion channels detected by tryptophan quenching of bimane fluorescence

Ion channels are allosteric membrane proteins that open and close an ion-permeable pore in response to various stimuli. This gating process provides the regulation that underlies electrical signaling events such as action potentials, postsynaptic potentials, and sensory receptor potentials. Recently, the molecular structures of a number of ion channels and channel domains have been solved by x-ray crystallography. These structures have highlighted a gap in our understanding of the relationship between a channel's function and its structure. Here we introduce a new technique to fill this gap by simultaneously measuring the channel function with the inside-out patch-clamp technique and the channel structure with fluorescence spectroscopy. The structure and dynamics of short-range interactions in the channel can be measured by the presence of quenching of a covalently attached bimane fluorophore by a nearby tryptophan residue in the channel. This approach was applied to study the gating rearrangements in the bovine rod cyclic nucleotide-gated ion channel CNGA1 where it was found that C481 moves towards A461 during the opening allosteric transition induced by cyclic nucleotide. The approach offers new hope for elucidating the gating rearrangements in channels of known structure.     

Designing Inhibitors of M2 Proton Channel against H1N1 Swine Influenza Virus

Background

M2 proton channel of H1N1 influenza A virus is the target protein of anti-flu drugs amantadine and rimantadine. However, the two once powerful adamantane-based drugs lost their 90% bioactivity because of mutations of virus in recent twenty years. The NMR structure of the M2 channel protein determined by Schnell and Chou (Nature, 2008, 451, 591–595) may help people to solve the drug-resistant problem and develop more powerful new drugs against H1N1 influenza virus.

Methodology

Docking calculation is performed to build the complex structure between receptor M2 proton channel and ligands, including existing drugs amantadine and rimantadine, and two newly designed inhibitors. The computer-aided drug design methods are used to calculate the binding free energies, with the computational biology techniques to analyze the interactions between M2 proton channel and adamantine-based inhibitors.

Conclusions

1) The NMR structure of M2 proton channel provides a reliable structural basis for rational drug design against influenza virus. 2) The channel gating mechanism and the inhibiting mechanism of M2 proton channel, revealed by the NMR structure of M2 proton channel, provides the new ideas for channel inhibitor design. 3) The newly designed adamantane-based inhibitors based on the modeled structure of H1N1-M2 proton channel have two pharmacophore groups, which act like a “barrel hoop”, holding two adjacent helices of the H1N1-M2 tetramer through the two pharmacophore groups outside the channel. 4) The inhibitors with such binding mechanism may overcome the drug resistance problem of influenza A virus to the adamantane-based drugs.     

Surface changes of the mechanosensitive channel MscS upon its activation, inactivation, and closing

MscS is a bacterial mechanosensitive channel that shows voltage dependence. The crystal structure of MscS revealed that the channel is a homoheptamer with a large chamber on the intracellular site. Our previous experiments indicated that the cytoplasmic chamber of the channel is not a rigid structure and changes its conformation upon the channel activation. In this study, we have applied various sized cosolvents that are excluded from protein surfaces. It is well known that such cosolvents induce compaction of proteins and prevent thermal fluctuations. It is also known that they shift channel equilibrium to the state of lower volume. We have found that large cosolvents that cannot enter the channel interior accelerate channel inactivation when applied from the cytoplasmic side, but they slow down inactivation when applied from the extracellular side. We have also found that small cosolvents that can enter the channel cytoplasmic chamber prevent the channel from opening, unlike the large ones. These data support our idea that the channel cytoplasmic chamber shrinks upon inactivation but also give new clues about conformational changes of the channel upon transitions between its functional states.     

Crystal Structure of a Voltage-gated K+ Channel Pore Module in a Closed State in Lipid Membranes

Voltage-gated K⁺ channels underlie the electrical excitability of cells. Each subunit of the functional tetramer consists of the tandem fusion of two modules, an N-terminal voltage-sensor and a C-terminal pore. To investigate how sensor coupling to the pore generates voltage-dependent channel opening, we solved the crystal structure and characterized the function of a voltage-gated K⁺ channel pore in a lipid membrane. The structure of a functional channel in a membrane environment at 3.1 Å resolution establishes an unprecedented connection between channel structure and function. The structure is unique in delineating an ion-occupied ready to conduct selectivity filter, a confined aqueous cavity, and a closed activation gate, embodying a dynamic entity trapped in an unstable closed state.     

Computational studies of proton transport through the M2 channel

The M2 ion channel is an essential component of the influenza A virus. This low-pH gated channel has a high selectivity for protons. Evidence from various experimental data has indicated that the essential structure responsible for the channel is a parallel homo-tetrameric alpha-helix bundle having a left-handed twist with each helix tilted with respect to the membrane normal. A backbone structure has been determined by solid state nuclear magnetic resonance (NMR). Though detailed structures for the side chains are not available yet, evidence has indicated that His37 and Trp41 in the alpha-helix are implicated in the local molecular structure responsible for the selectivity and channel gate. More definitive conformations for the two residues were recently suggested based on the known backbone structure and recently obtained NMR data. While two competitive proton-conductance mechanisms have been proposed, the actual proton-conductance mechanism remains an unsolved problem. Computer simulations of an excess proton in the channel and computational studies of the His37/Trp41 conformations have provided insights into these structural and mechanism issues.     

BKCa通道的结构与功能

BKCa通道将细胞膜电特性与细胞信号系统联系在一起,在细胞功能实现中起着重要作用。该通道广泛且又较高密度地表达于许多物种的多种组织,其分子结构复杂,丰富的超家族成员具有各自不同的表达分布。BKCa通道的分子结构由α亚单位和β亚单位构成,其中α亚单位形成通道的孔道区和活性调节区域,β亚单位修饰通道活性的调节特性。BKCa通道开放几率大、电导率高、调控位点多,并且不同的超家族成员表现出不同的功能特征,如细胞膜电位感受性、细胞内游离钙离子敏感性等。文章概述BKCa通道的分子结构和功能特征。     

Structures of the plasma channels in a Besselian beam

A mechanism for the formation of the structure of an optical discharge in Besselian laser beams is proposed on the basis of analyzing numerous experiments. The discharge structure is determined by the periodicity of the field of a Besselian beam in the radial and longitudinal directions and also depends on the power and duration of the heating pulse. In the initial stage of the plasma channel formation, the configuration of the channel inhomogeneities follows the discharge structure. If the spatial scale of the discharge structure is small, then the developing channel evolves into a homogeneous state. The time required for the structural inhomogeneities of the plasma channel to be smoothed out is estimated as a function of their scale length. __________ Translated from Fizika Plazmy, Vol. 27, No. 9, 2001, pp. 846–858. Original Russian Text Copyright ￠ 2001 by Pyatnitsky.     

Adoption of beta structure by the inactivating "ball" peptide of the Shaker B potassium channel.

The conformation of the inactivating peptide of the Shaker B K+ channel (ShB peptide) and that of a noninactivating mutant (ShBL7E peptide) have been studied. Under all experimental conditions explored, the mutant peptide remains in a predominantly nonordered conformation. On the contrary, the inactivating ShB peptide has a great tendency to adopt a highly stable beta structure, particularly when challenged "in vitro" by anionic phospholipid vesicles. Because the putative peptide binding elements at the inner mouth of the channel comprise a ring of anionic residues and a hydrophobic pocket, we hypothesize that the conformational restrictions imposed on the ShB peptide by its interaction with the anionic lipid vesicles could partly imitate those imposed by the above ion channel elements. Thus, we propose that adoption of beta structure by the inactivating peptide may also occur during channel inactivation. Moreover, the difficulties encountered by the noninactivating ShBL7E peptide mutant to adopt beta structure and the observation that trypsin hydrolysis of the ShB peptide prevent both structure formation and channel inactivation lend further support to the hypothesis that adoption of beta structure by the inactivating peptide in a hydrophobic environment is important in determining channel blockade.     

'Feeling the pressure': structural insights into a gated mechanosensitive channel.

The structure determination of the large-conductance mechanosensitive channel (MscL) from Mycobacterium tuberculosis has revealed the architecture of the first full-length, gated pentameric ion channel. This structure provides insights into the elements participating in the conductance and gating mechanisms of these channels.