Projection structure of channelrhodopsin-2 at 6 Å resolution by electron crystallography

Channelrhodopsin-2 (ChR2) is the prototype of a new class of light-gated ion channels that is finding widespread applications in optogenetics and biomedical research. We present a  6-Å projection map of ChR2, obtained by cryo-electron microscopy of two-dimensional crystals grown from pure, heterologously expressed protein. The map shows that ChR2 is the same dimer with non-crystallographic 2-fold symmetry in three different membrane crystals. This is consistent with biochemical analysis, which shows a stable dimer in detergent solution. Comparison to the projection map to bacteriorhodopsin indicates a similar structure of seven transmembrane alpha helices. Based on the projection map and sequence alignments, we built a homology model of ChR2 that potentially accounts for light-induced channel gating. Although a monomeric channel is not ruled out, comparison to other membrane channels and transporters suggests that the ChR2 channel is located at the dimer interface on the 2-fold axis, lined by transmembrane helices 3 and 4.     

The outer pore of the glutamate receptor channel has 2-fold rotational symmetry

The ligand binding domain of glutamate receptors (GluRs) has 2-fold rotational symmetry. The structure including the symmetry of the GluR ion channel remains undefined. Here we used substituted cysteines in the pore-lining M3 segment of the AMPAR GluR-A subunit and various cysteine-reactive agents to study the structure of the channel during gating. We find that cysteines substituted at A+6, located in the highly conserved SYTANLAAF motif, are grouped in pairs consistent with a 2-fold symmetry in the extracellular part of the pore. To account for this symmetry and crosslinking, we propose that the M3 segments in two neighboring GluR subunits are kinked within SYTANLAAF in opposite directions relative to the central axis of the pore. Our results extend the 2-fold rotational symmetry from the ligand binding domain to at minimum the extracellular part of the channel and suggest a model of gating movements in GluR pore-forming domains.     

Structure of glycolate oxidase from spinach at a resolution of 5.5 Å

The crystal structure of glycolate oxidase from spinach has been determined to 5.5 Å resolution, using two isomorphous heavy-atom derivatives and their anomalous contributions. In the electron density map the boundaries of the octameric molecules are clearly seen. The subunit molecular weight is 37,000. Two protomers are in very close contact around one of the crystallographic 2-fold axes. Four such dimers are in contact around the 4-fold axis, so that the glycolate oxidase molecules are arranged as octamers with 422 symmetry in the crystal lattice. The roughly spherical octameric molecules have a diameter of approximately 100 Å. These octamers are arranged in a network, such that large solvent channels, approximately 60Å in diameter, pass right through the crystal lattice.The secondary structure of two-thirds of the subunit density has been interpreted in terms of eight consecutive β strand-α-helix units forming a cylinder very similar to the structure of triose phosphate isomerase. This interpretation is based on the very characteristic arrangement of the eight helices which form such a cylinder. The binding site of a substrate analogue, thioglycolate, has been localized in a deep cleft of the subunit at one end of the βα-barrel close to its axis.     

Emerging models of glutamate receptor ion channel structure and function

Excitatory synaptic transmission in the brain is mediated by ligand-gated ion channels (iGluRs) activated by glutamate. Distinct from other neurotransmitter receptors, the extracellular domains of iGluRs are loosely packed assemblies with two clearly distinct layers, each of which has both local and global 2-fold axes of symmetry. By contrast, the iGluR transmembrane segments have 4-fold symmetry and share a conserved pore loop architecture found in tetrameric voltage-gated ion channels. The striking layered architecture of iGluRs revealed by the 3.6?? resolution structure of an AMPA receptor homotetramer likely arose from gene fusion events that occurred early in evolution. Although this modular design has greatly facilitated biophysical and structural studies on individual iGluR domains, and suggested conserved mechanisms for iGluR gating, recent work is beginning to reveal unanticipated diversity in the structure, allosteric regulation, and assembly of iGluR subtypes.     

Crystal structure of soybean proglycinin A1aB1b homotrimer

Soybean glycinin is a member of the 11 S globulin family. The crystal structure of proglycinin was determined by X-ray crystallography at 2.8 A resolution with an R-factor of 0.199 and a free R-factor of 0.250. A trimer molecule was found in an asymmetric unit of crystals. The trimer model contains three A1aB1b subunits and comprises 1128 amino acid residues and 34 water molecules. The constituent protomers of the homo-trimeric protein are arranged around a 3-fold symmetry axis with dimensions of 95 Ax95 Ax40 A. The protomer model is composed of five fragments which correspond roughly to conserved regions based on the sequence alignment of various 11 S globulins. The core of the protomer consists of two jelly-roll beta-barrels and two extended helix domains. This structure of proglycinin is similar to those of canavalin and phaseolin belonging to the 7 S globulin family, strongly supporting the hypothesis that both 7 S and 11 S globulins are derived from a common ancestor. The inter and intra-chain disulfide bonds conserved in the 11 S globulin family are clearly observed. It is found that the face with the inter-chain disulfide bond (IE face) contains more hydrophobic residues than that with the intra-chain disulfide bond. This suggests that a mature hexamer is formed by the interaction between the IE faces after processing.     

The shape of L-arabinose isomerase from Escherichia coli.

L-Arabinose isomerase, EC 5.3.1.4, catalyzes the conversion of L-arabinose to L-ribulose, the first step in the catabolism of L-arabinose by Escherichia coli B/r. Patrick and Lee (1969) J. Biol. Chem. 244, 4277--4283) demonstrated that native L-arabinose isomerase is composed of six identical subunits of approximately Mr = 60,000. In this paper we describe an electron microscopy study of the arrangement of the six identical subunits. The isomerase is seen in two distinctly different orientations. The first has three subunits visible, with a 3-fold axis of symmetry, corresponding to a face-on view of two stacked, eclipsed trimers. The second orientation is rectangular in shape with 2-fold symmetry; suggesting a side-on view of the stacked trimers. The six identical subunits are thus arranged with D3 symmetry as in a trigonal prism. Measurements were made on the maximum profile of the three 2-fold axes of symmetry of the face-on orientations, and of both the long and short dimensions of the side-on orientation. The best estimate for the maximum profile of the 2-fold axes of symmetry of the face-on view is 106 +/- 8 A, using glutamine synthetase as an internal size standard. Measurements from micrographs of the isomerase alone, using an external magnification calibration, give the following results: for the maximum profile of the three 2-fold axes of symmetry of the face-on view, 132 +/- 7 A; for the long axis of the side-on view, 136 +/- 10 A; and for the short axis, 105 +/- 6 A. These measurements are consisting with the interpretation of the profiles as representing two different orientations of the L-arabinose isomerase.     

Bundles of amphipathic transmembrane alpha-helices as a structural motif for ion-conducting channel proteins: studies on sodium channels and acetylcholine receptors

Channel proteins are transmembrane symmetric (or pseudosymmetric) oligomers organized around a central ionic pore. We present here a molecular model of the pore forming structures of two channel proteins with different primary structures and oligomeric size: the voltage-sensitive sodium channel and the nicotinic cholinergic receptor. We report low-energy arrangements of alpha-helical bundles calculated by semiempiricial potential energy functions and optimization routines and further refined using molecular dynamics. The ion-conducting pore is considered to be a symmetric or pseudosymmetric homooligomer of 3-5 amphipathic alpha-helices arranged such that the polar residues line a central hydrophilic pathway and the apolar residues face the hydrophobic bilayer interior. The channel lining exposes either charged (Asp, Glu, Arg, Lys) or polar-neutral (Ser, Thr) residues. A bundle of four parallel helices constrained to C4 symmetry, the helix axis aligned with the symmetry axis, and the helices constrained to idealized dihedral angles, produces a structure with a pore of the size inferred for the sodium channel protein (area approximately 16 A2). Similarly, a pentameric array optimized with constraints to maintain C5 symmetry and backbone torsions characteristic of alpha-helices adopts a structure that appears well suited to form the lining of the nicotinic cholinergic receptor (pore area approximately 46 A2). Thus, bundles of amphipathic alpha-helices satisfy the structural, energetic, and dynamic requirements to be the molecular structural motif underlying the function of ionic channels.     

Low resolution crystal structure of muconolactone isomerase. A decamer with a 5-fold symmetry axis

Muconolactone isomerase from Pseudomonas putida crystallizes from sodium sulfate solution in space group P2(1) (a = 65.84 A, b = 105.70 A, c = 77.20 A, beta = 90.5 degrees) with ten 11,000 Mr subunits per asymmetric unit. The 7 A resolution crystal structure was solved by single isomorphous replacement followed by 10-fold symmetry averaging. The decameric enzyme has an uncommon non-crystallographic 5-fold symmetry axis and a large cavity in its center.     

Molecular design of PhoE porin and its functional consequences

The three-dimensional structure of PhoE porin from Escherichia coli, negatively stained with uranyl acetate, has been determined by electron crystallographic techniques to a resolution of about 18 A. The structure shows that PhoE porin consists of trimeric stain-filled channels as the basic unit. The trimeric channels converge as they transverse the membrane but they do not merge. Our three-dimensional structure of PhoE porin indicates that there is a short, narrower segment of channel, which extends beyond the visible strain-filled portion of the channel. The map of glucose-embedded PhoE porin in projection normal to the membrane has also been determined to a resolution of 6.5 A. The projected map shows trimeric ring-like structures, which are presumably cylindrical domains of beta-sheet. At the 3-fold symmetry axis of the trimer, there is a low density region, which is suggested to be a site of lipopolysaccharide that is required for channel and bacteriophage receptor activities. The structural model of the PhoE monomer consists of a flattened cylinder with a large water-filled vestibule about 35 A long with an elliptically shaped opening that is 27 A along the major axis and 18 A along the minor axis. The vestibule has a narrower extension about 10 A long with an average diameter of about 10 A. The vestibule wall is formed by beta-sheet, which may have a large fraction of the beta-strands oriented normal to membrane. Our structural model provides a clue as to how the surface charges on the outer membrane may regulate the permeation of ionic solutes through the channel.     

P2X(1) receptor subunit contribution to gating revealed by a dominant negative PKC mutant

The family of ATP-gated P2X receptor channels have a conserved protein kinase C site in the N-terminal intracellular domain. This site was disrupted in human P2X(1) receptors by the mutation T18A. T18A mutants were expressed at normal levels in Xenopus oocytes; however, the peak current amplitude was reduced by >99% and showed approximately 10 fold faster desensitisation in response to ATP than wild type (WT) receptors showed. P2X receptor subunits form functional trimeric channels. Co-expression of T18A and WT receptors (90:10 ratio) produced heteromeric T18A/WT channels with the rapid T18A time-course and an approximately 90-fold increase in peak current amplitude compared to T18A. Similarly, T18A dominated the desensitisation phenotype of heteromeric channels composed of T18A and slowly desensitising K68A mutants. These results suggest that phosphorylation of P2X(1) receptors has a dramatic effect on the time-course of the response and may provide a mechanism for regulating channel function.     

Regulators of cell volume: The structural and functional properties of anion channels of the LRRC8 family

Members of the LRRC8 family participate in the response of vertebrate cells to osmotic changes in their environment. These proteins form heteromeric assemblies composed of the obligatory subunit LRRC8A and at least one of the other four homologs, which together function as anion-selective channels with distinct properties that are activated upon cell-swelling. The hexameric complexes share a conserved architecture consisting of a membrane-inserted pore domain with an ion permeation path located at the axis of symmetry and cytoplasmic leucine-rich repeat domains that regulate the open probability of the channel. In this review, we summarize the current understanding of structure–function relationships of these unusual ion channels whose mechanisms are, despite their large physiological importance, still poorly understood.     

Structure of satellite tobacco necrosis virus after crystallographic refinement at 2.5 Å resolution

The structure of the protein subunit of satellite tobacco necrosis virus has been solved at 3.7 Å resolution. We have now crystallographically refined the original model and extended the resolution to 2.5 Å in order to get a model accurate enough to explain the details of the subunit interactions. The refinement was done with a novel method utilizing the icosahedral symmetry of the virus particle.The final model shows a complicated network of interactions, involving salt linkages, hydrogen bonds and hydrophobic contacts. In addition, we have located three different metal ion sites in the protein shell, linking the protein subunits together. These sites are probably occupied by calcium ions. One site is found in a general position near the icosahedral 3-fold axis of the virus. The ligands form an octahedral arrangement, with two main chain carbonyl oxygens (O-61 and O-64), one carboxylate oxygen (OD1 from Asp194) of the same subunit and a second carboxylate oxygen (OE1 of Glu25) from a 3-fold related subunit. Two water molecules complete the octahedral arrangement. A second site is on the icosahedral 3-fold axis and is liganded by the carboxylate oxygens of the 3-fold related Asp55 residues. The third metal ion site is found on the 5-fold axis, liganded by the five carbonyl oxygens of Thr138 and two water molecules.We are unable to locate the first 11 N-terminal amino acid residues, which point into the virus interior. No interpretable density for RNA has been found, indicating that the nucleic acid of the virus does not have a unique orientation in the crystal.     

Structure of a diubiquitin conjugate and a model for interaction with ubiquitin conjugating enzyme (E2).

Covalent ligation of multiubiquitin chains targets eukaryotic proteins for degradation. In such multiubiquitin chains, successive ubiquitins are linked by an isopeptide bond involving the side chain of Lys48 and the carboxyl group of Gly76. The crystal structure of a diubiquitin conjugate has been determined and refined at 2.3-A resolution. The molecule has internal approximate 2-fold symmetry with multiple hydrophobic and hydrophilic contacts along the 2-fold axis. The structure of the diubiquitin conjugate suggests determinants for recognition of multiubiquitin chains. A model for the interaction of diubiquitin and a ubiquitin conjugating enzyme (E2) is proposed.     

Flexible architecture of IP3R1 by Cryo-EM

Inositol 1,4,5-trisphosphate receptors (IP3Rs) play a fundamental role in generating Ca2+ signals that trigger many cellular processes in virtually all eukaryotic cells. Thus far, the three-dimensional (3D) structure of these channels has remained extremely controversial. Here, we report a subnanometer resolution electron cryomicroscopy (cryo-EM) structure of a fully functional type 1 IP3R from cerebellum in the closed state. The transmembrane region reveals a twisted bundle of four α helices, one from each subunit, that form a funnel shaped structure around the 4-fold symmetry axis, strikingly similar to the ion-conduction pore of K+ channels. The lumenal face of IP3R1 has prominent densities that surround the pore entrance and similar to the highly structured turrets of Kir channels. 3D statistical analysis of the cryo-EM density map identifies high variance in the cytoplasmic region. This structural variation could be attributed to genuine structural flexibility of IP3R1.     

Three-dimensional structure of P-glycoprotein: the transmembrane regions adopt an asymmetric configuration in the nucleotide-bound state

Multidrug resistance of cancer cells and pathogens is a serious clinical problem. A major factor contributing to drug resistance in cancer is the over-expression of P-glycoprotein, a plasma membrane ATP-binding cassette (ABC) drug efflux pump. Three-dimensional structural data with a resolution limit of approximately 8 A have been obtained from two-dimensional crystals of P-glycoprotein trapped in the nucleotide-bound state. Each of the two transmembrane domains of P-glycoprotein consists of six long alpha-helical segments. Five of the alpha-helices from each transmembrane domain are related by a pseudo-2-fold symmetry, whereas the sixth breaks the symmetry. The two alpha-helices positioned closest to the (pseudo-) symmetry axis at the center of the molecule appear to be kinked. A large loop of density at the extracellular surface of the transporter is likely to correspond to the glycosylated first extracellular loop, whereas two globular densities at the cytoplasmic side correspond to the hydrophilic, nucleotide-binding domains. This is the first three-dimensional structure for an intact eukaryotic ABC transporter. Comparison with the structures of two prokaryotic ABC transporters suggests significant differences in the packing of the transmembrane alpha-helices within this protein family.     

Cystic fibrosis transmembrane conductance regulator. Physical basis for lyotropic anion selectivity patterns

The selectivity of Ca2+ over Na+ is approximately 3.3-fold larger in cGMP-gated channels of cone photoreceptors than in those of rods when measured under saturating cGMP concentrations, where the probability of channel opening is 85-90%. Under physiological conditions, however, the probability of opening of the cGMP-gated channels ranges from its largest value in darkness of 1-5% to essentially zero under continuous, bright illumination. We investigated the ion selectivity of cGMP-gated channels as a function of cyclic nucleotide concentration in membrane patches detached from the outer segments of rod and cone photoreceptors and have found that ion selectivity is linked to gating. We determined ion selectivity relative to Na+ (PX/PNa) from the value of reversal potentials measured under ion concentration gradients. The selectivity for Ca2+ over Na+ increases continuously as the probability of channel opening rises. The dependence of PCa/PNa on cGMP concentration, in both rods and cones, is well described by the same Hill function that describes the cGMP dependence of current amplitude. At the cytoplasmic cGMP concentrations expected in dark-adapted intact photoreceptors, PCa/PNa in cone channels is approximately 7.4-fold greater than that in rods. The linkage between selectivity and gating is specific for divalent cations. The selectivity of Ca2+ and Sr2+ changes with cGMP concentration, but the selectivity of inorganic monovalent cations, Cs+ and NH4+, and organic cations, methylammonium+ and dimethylammonium+, is invariant with cGMP. Cyclic nucleotide-gated channels in rod photoreceptors are heteromeric assemblies of alpha and beta subunits. The maximal PCa/PNa of channels formed from alpha subunits of bovine rod channels is less than that of heteromeric channels formed from alpha and beta subunits. In addition, Ca2+ is a more effective blocker of channels formed by alpha subunits than of channels formed by alpha and beta subunits. The cGMP-dependent shift in divalent cation selectivity is a property of alphabeta channels and not of channels formed from alpha subunits alone.     

The projection structure of EmrE, a proton-linked multidrug transporter from Escherichia coli, at 7 A resolution

EmrE belongs to a family of eubacterial multidrug transporters that confer resistance to a wide variety of toxins by coupling the influx of protons to toxin extrusion. EmrE was purified and crystallized in two dimensions by reconstitution with dimyristoylphosphatidylcholine into lipid bilayers. Images of frozen hydrated crystals were collected by cryo-electron microscopy and a projection structure of EmrE was calculated to 7 A resolution. The projection map shows an asymmetric EmrE dimer with overall dimensions approximately 31 x 40 A, comprising an arc of highly tilted helices separating two helices nearly perpendicular to the membrane from another two helices, one tilted and the other nearly perpendicular. There is no obvious 2-fold symmetry axis perpendicular to the membrane within the dimer, suggesting that the monomers may have different structures in the functional unit.     

The cell envelope of Thermoproteus tenax: three-dimensional structure of the surface layer and its role in shape maintenance

The sulphur-dependent archaebacterium Thermoproteus tenax has a cylindrical cell shape variable in length, but constant in diameter. Its whole surface is covered by a regular protein layer (S-layer). The lattice has p6 symmetry and a lattice constant of 32.8 nm. The three-dimensional reconstruction from a tilt series of isolated and negatively stained S-layer shows a complex mass distribution of the protein: a prominent, pillar-shaped protrusion is located at the 6-fold crystallographic axis with radiating arms connecting neighbouring hexamers in the vicinity of the 3-fold axis. The base vectors of the S-layer lattice have a preferred orientation with respect to the longitudinal axis of the cell. The layer can be seen as a helical structure consisting of a right-handed, two-stranded helix, with the individual chains running parallel. Supposing that new S-layer protein is inserted at lattice faults (wedge disclinations) near the poles, growing of the layer would then proceed by moving a disclination at the end of the helix. The constant shape of the cell, as well as the particular structure of the layer, strongly suggest that this S-layer has a shape-maintaining function.     

Circulation of the plasma membrane in Dictyostelium

We have developed a fluorimetric assay with the use of the dye FM1-43 to determine the rate at which Dictyostelium amoebae endocytose their surface membrane. Our results show that they do so about once each 4-10 min. A clathrin null mutant takes its surface up only approximately 30% more slowly, showing that this membrane uptake cannot be caused by clathrin-coated vesicles. Surprisingly, Ax2 and its parent, NC4, which differ in their rates of fluid-phase internalization by approximately 60-fold, take up their surfaces at the same rates. These results show that, in axenic cells, the uptake of fluid and of surface area are separate processes. The large activity of this new endocytic cycle in both Ax2 and NC4 amoebae appears capable of delivering sufficient new surface area to advance the cells' fronts during migration.     

Surface crystallisation of the plasma membrane H+-ATPase on a carbon support film for electron crystallography

Large two-dimensional crystals of H+-ATPase, a 100 kDa integral membrane protein, were grown directly onto the carbon surface of an electron microscope grid. This procedure prevented the fragmentation that is normally observed upon transfer of the crystals from the air-water interface to a continuous carbon support film. Crystals grown by this method measure approximately 5 microm across and have a thickness of approximately 240 A. They are of better quality than the monolayers previously obtained at the air-water interface, yielding structure factors to at least 8 A in-plane resolution by electron image processing. Unlike most other two-dimensional crystals of membrane proteins they do not contain a lipid bilayer, but consist of detergent-protein micelles of H+-ATPase hexamers tightly packed on a trigonal lattice. The crystals belong to the two-sided plane group p321 (a=b=165 A), containing two layers of hexamers related by an in-plane axis of 2-fold symmetry. The protein is in contact with the carbon surface through its large, hydrophilic 70 kDa cytoplasmic portion, yet due to the presence of detergent in the crystallizing buffer, the hydrophobicity of the carbon surface does not appear to affect crystal formation. Surface crystallisation may be a useful method for other proteins which form fragile two-dimensional crystals, in particular if conditions for obtaining three-dimensional crystals are known, but their quality or stability is insufficient for X-ray structure determination.