Refined atomic model of the four-layer aggregate of the tobacco mosaic virus coat protein at 2.4-A resolution.

Previous x-ray studies (2.8-A resolution) on crystals of tobacco mosaic virus coat protein grown from solutions containing high salt have characterized the structure of the protein aggregate as a dimer of a bilayered cylindrical disk formed by 34 chemically identical subunits. We have determined the crystal structure of the disk aggregate at 2.4-A resolution using x-ray diffraction from crystals maintained at cryogenic temperatures. Two regions of interest have been extensively refined. First, residues of the low-radius loop region, which were not modeled previously, have been traced completely in our electron density maps. Similar to the structure observed in the virus, the right radial helix in each protomer ends around residue 87, after which the protein chain forms an extended chain that extends to the left radial helix. The left radial helix appears as a long alpha-helix with high temperature factors for the main-chain atoms in the inner portion. The side-chain atoms in this region (residues 90-110) are not visible in the electron density maps and are assumed to be disordered. Second, interactions between subunits in the symmetry-related central A pair have been determined. No direct protein-protein interactions are observed in the major overlap region between these subunits; all interactions are mediated by two layers of ordered solvent molecules. The current structure emphasizes the importance of water in biological macromolecular assemblies.     

Control of crystal forms of apoferritin by site-directed mutagenesis

Surface charges of protein molecules are not only important to biological functions but also crucial to the molecular assembly responsible for crystallization. Appropriate alteration in the surface charge distribution of a protein molecule induces new molecular alignment in the proper direction in the crystal and, hence, controls the crystal form. Apoferritin molecules are known to crystallize in two- and three-dimensional forms in the presence of cadmium ions, which bridge neighboring protein molecules. Here we report a controlled transformation of the apoferritin 2-D crystal by site-directed mutagenesis. In mutant apoferritin, two amino acid residues binding a cadmium-ion through their negative charge, were replaced by one type of nonionic amino acid residues. The amino acid residues, Asp-84 and Gln-86 in the sequence of recombinant (i.e., wild-type) horse L -apoferritin, were replaced by Ser. The wild-type apoferritin yielded a hexagonal lattice 2-D crystal in the presence of cadmium ions. In contrast, the mutant apoferritin yielded two types of oblique crystals independent of the presence of cadmium ions. Image reconstruction of electron micrographs of the mutant crystals made clear that the mutant apoferritin molecules oriented themselves with the 2-fold symmetry axis perpendicular to the crystal plane in both crystals, while the wild-type apoferritin molecules oriented themselves with the 3-fold symmetry axis perpendicular to the crystal plane. The changes of crystal forms and molecular orientation in the 2-D crystals were well explained by a change of the electrostatic interactions induced by the mutagenesis. © 1995 Wiley-Liss, Inc.     

Significant role of electrostatic interactions for stabilization of protein assemblies

Contribution of electrostatic interactions to stability of BPTI orthorhombic, pig-insulin cubic crystals, and horse L ferritin crystals was evaluated with numerical calculation of Poisson-Boltzmann equation based on a dielectric model. The stability of a ferritin molecule (24-mer) composed of 24 subunits was also evaluated. It was found that the surface charge-charge interactions at separation distances (< 5 Å) were insensitive to variations in the ionic strength, and thus stabilized assembled states of the proteins (i.e., crystalline state and oligomeric state). It was also revealed that the charge density and the packing of the protein crystals were largely responsible for the ionic strength dependence of the crystal stability. The stability of the 5PTI crystalline state with a high charge density drastically increased as the concentration of the solvent ions increased. In contrast, that of the insulin crystal with a low charge density and large solvent region was insensitive to changes in the ionic concentration. The electrostatic interaction between ferritin 24-mers was attributed to two salt bridges mediated by Cd ion. For the stability of the ferritin 24-mer, which is evolutionally designed, the electrostatic stabilization between the subunits was attributed to polar bonds such as buried salt bridges or hydrogen bonds, which occasionally yielded more than 5 kcal/mol and were numerous and very strong compared with the bonds between molecules in the 5PTI and 9INS crystals.By analyzing the atomic charge-charge interactions in detail, it was found that charge pairs separated by less than 3 Å, such as hydrogen bonds, dominantly stabilize the assembled states, and that pairs 3 to 5 Å apart were also important. The stability of the assembled states evaluated by the total EET was determined by the fine balance between the two competing contributions arising from the stabilizing atoms and the destabilizing atoms.Changes of the ASA and hydration free energy were also evaluated in accordance with the process of the subunit assembly. The change of hydration free energy, which was very large (i.e., ~+ 100 kcal/mol/subunit) and unfavorable for the assembly, was proportional to the electrostatic hydration energy (i.e., Born energy change in the hydration process). Hydrophobic groups were likely to appear more frequently than hydrophilic groups at the interfaces.This study offers a method which can improve the stability of protein crystals by introducing polar or charged residues that are properly designed to form specific hydrogen bonds or salt bridges between neighboring protein molecules. This method is also applicable to crystallography, because it improves refinement of protein structures in crystals by taking the inter-protein interactions into account.     

The structure of NADH:ubiquinone oxidoreductase from beef-heart mitochondria. Crystals containing an octameric arrangement of iron-sulphur protein fragments

We have investigated the structure of two-dimensional crystals from preparations of NADH:ubiquinone oxidoreductase from beef-heart mitochondria. The crystal structure of these crystals was previously determined to be equivalent with two native enzyme molecules per unit cell, i.e. a p2 symmetry [Boekema, E. J., Van Heel, M. G. & Van Bruggen, E. F. J. (1984) Biochim. Biophys. Acta 787, 19-26]. However, the optical diffraction patterns of the crystals displayed a clear fourfold symmetry. A Fourier analysis carried out on the calculated diffraction pattern proved unambiguously that the crystal symmetry was p42(1)2. Following crystallographic rules the unit cell therefore contained eight identical molecules. As a consequence, only a subcomplex of the enzyme rather than the intact enzyme formed the crystal. Electron microscopy of isolated, single molecules of the iron-sulphur protein, a dissociation product of complex I, revealed the presence of square complexes with sides of approximately 15 nm. Since these complexes were indistinguishable from the building blocks (unit cells) of the two-dimensional crystals, the crystals could be composed of Fe-S protein fragments only. The nature of the fragments in the unit cell was probed by immuno-labelling with monovalent antibodies (Fab's), raised against the 75-kDa subunit from the Fe-S protein, followed by image analysis. We found at least four binding sites for the anti-(75-kDa subunit) Fab per unit cell, indicating the presence of at least four copies of the antigen. In order to account for these observations we postulate the hypothesis that the two-dimensional crystals obtained from complex I are composed of iron-sulphur protein molecules in an octameric arrangement.     

Three-dimensional structure of ubiquinol: Cytochrome C reductase from Neurospora mitochondria determined by electron microscopy of membrane crystals

Membrane crystals have been prepared from mitochondrial ubiquinol: cytochrome c reductase by mixing the enzyme-Triton complex with phospholipid-Triton micelles and subsequently removing the Triton. The electron micrographs of the negatively stained crystals diffract to 2·5 nm, with unit cell dimensions of 13·7 nm by 17·4 nm. The enzyme is arranged in a two-sided plane group P22₁2₁, i.e. alternate molecules span the bilayer in an up and down manner. By combining tilted views of the membrane crystals, a low-resolution three-dimensional structure of the enzyme has been calculated. The structure shows that the enzyme is a dimer, the monomers being related by a 2-fold axis running perpendicular to the membrane. The monomeric units of the enzyme are elongated, extending approximately 15 nm across the membrane. The protein is unequally distributed with about 30% of the total mass located in the bilayer, 50% in a section which extends 7 nm from one side of the bilayer and 20% in a section which extends 3 nm from the opposite side of the bilayer. The two monomeric units are in contact only in the membraneous section. This structure is compared with a model of the enzyme which is derived from biochemical properties of the isolated subunits.     

Effect of various humidity on local dynamic structure of lysozyme in a spin-labeled tetragonal crystal

The dynamics of the side groups of amino acid residues and local conformational changes in the lysozyme molecule upon dehydration and rehydration of lysozyme crystals were studied by the methods of spin label, X-ray diffraction, and molecular dynamics. The His15 residue of lysozyme from chicken egg white was modified by spin label, and spin-labeled tetragonal crystals of the protein were grown. The spatial structure of the covalently bound spin label and its immediate surroundings in the lysozyme tetragonal crystal was determined. The conformation of a fragment of the lysozyme molecule with the spin label on His15, optimized by the method of molecular dynamics, closely agreed with X-ray data. It was found by the X-ray diffraction analysis that a decrease in relative humidity to 40% is accompanied by both a decrease in the unit cell volume by 27% and a change in the diffraction field of roentgenograms from 0.23 to 0.60 HM. The dehydration of spin-labeled lysozyme crystals leads to an anomalous widening of EPR peaks without changes in their position. The dehydration in the humidity range studied has a two-stage character. The decrease in humidity to 75% is accompanied by a sharp change in the parameters measured, and on further decrease in humidity to 40% they change insignificantly. The first stage is caused by the removal of the greater part of molecules of bulk water, and the second stage is due to the removal of the remaining bulk water and possible changes in the dynamics of weakly bound water molecules and their position. The simulation of experimental EPR spectra showed that the anomalous broadening of the spectrum upon dehydration is related to an increase in the dispersion of spin label orientations induced by changes in the network of hydrogen bonds generated by water molecules in the vicinity of the spin label and a possible turn (by no more than 5 degrees) of the entire protein molecule. After rehydration, the physical state of the lysozyme crystal did not return to the starting point.     

SDSL-ESR-based protein structure characterization

As proteins are key molecules in living cells, knowledge about their structure can provide important insights and applications in science, biotechnology, and medicine. However, many protein structures are still a big challenge for existing high-resolution structure-determination methods, as can be seen in the number of protein structures published in the Protein Data Bank. This is especially the case for less-ordered, more hydrophobic and more flexible protein systems. The lack of efficient methods for structure determination calls for urgent development of a new class of biophysical techniques. This work attempts to address this problem with a novel combination of site-directed spin labelling electron spin resonance spectroscopy (SDSL-ESR) and protein structure modelling, which is coupled by restriction of the conformational spaces of the amino acid side chains. Comparison of the application to four different protein systems enables us to generalize the new method and to establish a general procedure for determination of protein structure.     

Two-dimensional crystals of apoferritin

A simple 2D crystallization method using unfolded protein film as a supporting film of crystals was described, which allows modification of protein surfaces by injecting chemical reagents into the subphase after the crystal formation. As an example, glutaraldehyde was used to cross-link adjacent proteins and then stabilize protein crystals. The second layer of other proteins can also be formed on the apoferritin array using cross-linkers.The array of apoferritin is not only beneficial for electron crystallography but also for practical applications. For example, apoferritin produces a mineral core with a size which can be adjusted by the size to the cavity (i.e. 6 nm). Fabrication of such a small size of well defined fine particles is currently not easy using physical or chemical procedures. Using apoferritin, however, it is easy to produce uniform fine particles. If the core is designed to add interesting properties such as magnetism it is possible to make the highest class of magnetic film with ferritin 2D crystals.Basic researches toward practical applications of 2D protein crystal is now under way in various fields. The well defined size and function of protein molecules will benefit to many applications. The function and crystalline order can be designed by site-directed mutagenesis with the development of protein engineering.     

Rational design of crystal contact‐free space in protein crystals for analyzing spatial distribution of motions within protein molecules

Contacts with neighboring molecules in protein crystals inevitably restrict the internal motions of intrinsically flexible proteins. The resultant clear electron densities permit model building, as crystallographic snapshot structures. Although these still images are informative, they could provide biased pictures of the protein motions. If the mobile parts are located at a site lacking direct contacts in rationally designed crystals, then the amplitude of the movements can be experimentally analyzed. We propose a fusion protein method, to create crystal contact‐free space (CCFS) in protein crystals and to place the mobile parts in the CCFS. Conventional model building fails when large amplitude motions exist. In this study, the mobile parts appear as smeared electron densities in the CCFS, by suitable processing of the X‐ray diffraction data. We applied the CCFS method to a highly mobile presequence peptide bound to the mitochondrial import receptor, Tom20, and a catalytically relevant flexible segment in the oligosaccharyltransferase, AglB. These two examples demonstrated the general applicability of the CCFS method to the analysis of the spatial distribution of motions within protein molecules.     

Desulfovibrio desulfuricans G20 tetraheme cytochrome structure at 1.5 Angstrom and cytochrome interaction with metal complexes

The structure of the type I tetraheme cytochrome c(3) from Desulfovibrio desulfuricans G20 was determined to 1.5 Angstrom by X-ray crystallography. In addition to the oxidized form, the structure of the molybdate-bound form of the protein was determined from oxidized crystals soaked in sodium molybdate. Only small structural shifts were obtained with metal binding, consistent with the remarkable structural stability of this protein. In vitro experiments with pure cytochrome showed that molybdate could oxidize the reduced cytochrome, although not as rapidly as U(VI) present as uranyl acetate. Alterations in the overall conformation and thermostability of the metal-oxidized protein were investigated by circular dichroism studies. Again, only small changes in protein structure were documented. The location of the molybdate ion near heme IV in the crystal structure suggested heme IV as the site of electron exit from the reduced cytochrome and implicated Lys14 and Lys56 in binding. Analysis of structurally conserved water molecules in type I cytochrome c(3) crystal structures identified interactions predicted to be important for protein stability and possibly for intramolecular electron transfer among heme molecules.     

The structure of 2Zn pig insulin crystals at 1.5 A resolution

The paper describes the arrangement of the atoms within rhombohedral crystals of 2Zn pig insulin as seen in electron density maps calculated from X-ray data extending to 1.5 A (1 A = 10(-10) m = 10(-1) nm) at room temperature and refined to R = 0.153. The unit cell contains 2 zinc ions, 6 insulin molecules and about 3 x 283 water molecules. The atoms in the protein molecules appear well defined, 7 of the 102 side chains in the asymmetric unit have been assigned alternative disordered positions. The electron density over the water molecules has been interpreted in terms of 349 sites, 217 weighted 1.0, 126 weighted 0.5, 5 at 0.33 and 1 at 0.25 giving ca. 282 molecules. The positions and contacts of all the residues belonging to the two A and B chains of the asymmetric unit are shown first and then details of their arrangement in the two insulin molecules, 1 and 2, which are different. The formation from these molecules of a compact dimer and the further aggregation of three dimers to form a hexamer around two zinc ions, follows. It appears that in the packing of the hexamers in the crystal there are conflicting influences; too-close contacts between histidine B5 residues in neighbouring hexamers are probably responsible for movements of atoms at the beginning of the A chain of one of the two molecules of the dimer that initiate movements in other parts, particularly near the end of the B chain. At every stage of the building of the protein structure, residues to chains of definite conformation, molecules, dimers, hexamers and crystals, we can trace the effect of the packing of like groups to like, aliphatic groups together, aromatic groups together, hydrogen-bonded structures, positive and negative ions. Between the protein molecules, the water is distributed in cavities and channels that are continuous throughout the crystals. More than half the water molecules appear directly hydrogen bonded to protein atoms. These are generally in contact with other water molecules in chains and rings of increasing disorder, corresponding with their movement through the crystals. Within the established crystal structure we survey next the distribution of hydrogen bonds within the protein molecules and between water and protein and water and water; all but eight of the active atoms in the protein form at least one hydrogen bond.(ABSTRACT TRUNCATED AT 400 WORDS)     

The detection of substructures within proteoglycan molecules. Electron-microscopic immuno-localization with the use of Protein A-gold.

Proteoglycan monomers from pig laryngeal cartilage were examined by electron microscopy with benzyldimethylalkylammonium chloride as the spreading agent. The proteoglycans appeared as extended molecules with a beaded structure, representing the chondroitin sulphate chains collapsed around the protein core. Often a fine filamentous tail was present at one end. Substructures within proteoglycan molecules were localized by incubation with specific antibodies followed by Protein A-gold (diameter 4 nm). After the use of an anti-(binding region) serum the Protein A-gold (typically one to three particles) bound at the extreme end of the filamentous region. A small proportion of the labelled molecules (10-15%) showed the presence of gold particles at both ends. A monoclonal antibody specific for a keratan sulphate epitope (MZ15) localized a keratan sulphate-rich region at one end of the proteoglycan, but gold particles were not observed along the extended part of the protein core. This distribution was not changed by prior chondroitin AC lyase digestion of the proteoglycan. Localization with a different monoclonal antibody to keratan sulphate (5-D-4) caused a change in the spreading behaviour of a proportion (approx. 20%) of the proteoglycan monomers that lost their beaded structure and appeared with the chondroitin sulphate chains projecting from the protein core. In these molecules the Protein A-gold localized antibody (5-D-4) along the length of the protein core whereas in those molecules with a beaded appearance it labelled only at one end. Labelling with either of the monoclonal antibodies was specific, as it was inhibited by exogenously added keratan sulphate. The differential localization achieved may reflect structural differences within the proteoglycan population involving keratan sulphate and the protein core to which it is attached. The results showed that by this technique substructures within proteoglycan molecules can be identified by Protein A-gold labelling after the use of specific monoclonal or polyclonal antibodies.     

Structure of light-harvesting chlorophyll a/b protein complex from plant photosynthetic membranes at 7 A resolution in projection

The structure of thin three-dimensional crystals of the light-harvesting chlorophyll a/b protein complex, an integral membrane protein from the photosynthetic membrane of chloroplasts, has been determined at 7 A (1 A = 0.1 nm) resolution in projection. The structure analysis was carried out by image processing of low-dose electron micrographs, and electron diffraction of thin three-dimensional crystals preserved in tannin. The three-dimensional crystals appeared to be stacks of two-dimensional crystals having p321 symmetry. Results of the image analysis indicated that the crystals were disordered, due to random translational displacement of stacked layers. This was established by a translation search routine that used the low-resolution projection of a single layer as a reference. The reference map was derived from the symmetrized average of two images that showed features consistent with the projected structure of negatively stained two-dimensional crystals. The phase shift resulting from the displacement of each layer was corrected. Phase shifts were then refined by minimizing the phase residual, bringing all layers to the same phase origin. Refined phases from different images were in agreement and reliable to 7 A resolution. A projection map was generated from the averaged phases and electron diffraction amplitudes. The map showed that the complex was a trimer composed of three protein monomers related by 3-fold symmetry. The projected density within the protein monomer suggested membrane-spanning alpha-helices roughly perpendicular to the crystal plane. The density in the centre and on the periphery of the trimeric complex was lower than that of the protein, indicating that this region contained low-density matter, such as lipids and antenna chlorophylls.     

Preliminary crystal structure studies of a ternary electron transfer complex between a quinoprotein, a blue copper protein, and a c-type cytochrome.

A ternary electron transfer protein complex has been crystallized and a preliminary structure investigation has been carried out. The complex is composed of a quinoprotein, methylamine dehydrogenase (MADH), a blue copper protein, amicyanin, and a c-type cytochrome (c551i). All three proteins were isolated from Paracoccus denitrificans. The crystals of the complex are orthorhombic, space group C222(1) with cell dimensions a = 148.81 A, b = 68.85 A, and c = 187.18 A. Two types of isomorphous crystals were prepared: one using native amicyanin and the other copper-free apo-amicyanin. The diffraction data were collected at 2.75 A resolution from the former and at 2.4 A resolution from the latter. The location of the MADH portion was determined by molecular replacement. The copper site of the amicyanin molecule was located in an isomorphous difference Fourier while the iron site of the cytochrome was found in an anomalous difference Fourier. The MADH from P. denitrificans (PD-MADH) is an H2L2 hetero-tetramer with the H subunit containing 373 residues and the L subunit 131 residues, the latter containing a novel redox cofactor, tryptophan tryptophylquinone (TTQ). The amicyanin of P. denitrificans contains 105 residues and the cytochrome c551i contains 155 residues. The ternary complex consists of one MADH tetramer with two molecules of amicyanin and two of c551i, forming a hetero-octamer; the octamer is located on a crystallographic diad. The relative positions of the three redox centers--i.e., the TTQ of MADH, the copper of amicyanin, and the heme group of c55li--are presented.     

Structure of bacteriorhodopsin at 1.55 A resolution.

Th?e atomic structure of the light-driven ion pump bacteriorhodopsin and the surrounding lipid matrix was determined by X-ray diffraction of crystals grown in cubic lipid phase. In the extracellular region, an extensive three-dimensional hydrogen-bonded network of protein residues and seven water molecules leads from the buried retinal Schiff base and the proton acceptor Asp85 to the membrane surface. Near Lys216 where the retinal binds, transmembrane helix G contains a pi-bulge that causes a non-proline? kink. The bulge is stabilized by hydrogen-bonding of the main-chain carbonyl groups of Ala215 and Lys216 with two buried water molecules located between the Schiff base and the proton donor Asp96 in the cytoplasmic region. The results indicate extensive involvement of bound water molecules in both the structure and the function of this seven-helical membrane protein. A bilayer of 18 tightly bound lipid chains forms an annulus around the protein in the crystal. Contacts between the trimers in the membrane plane are mediated almost exclusively by lipids.     

Preliminary crystallographic data and quaternary structural implications of the central subunit of the multi-subunit complex transcarboxylase

The hexameric central subunit (Mr = 360,000) of the multi-subunit complex transcarboxylase has been crystallized by bulk dialysis against 250 mM-sodium acetate (pH 5.5). The crystals are cubic, a = 193.1 A, space group P4(1)32 or enantiomorph. The number of molecules per unit cell is four and was deduced from the density of the crystals (1.10 g cm-3) and the mother liquor (1.01 g cm-3) and the specific volume of the protein calculated from molecular dimensions obtained from electron microscopy studies. Four molecules per cell requires the central subunits to lie on 3-fold axes, which are perpendicular to 2-fold rotation axes, so that the molecules satisfy 32 symmetry giving one subunit as the asymmetric unit. Of the four possible models that have been considered for the quaternary structure of transcarboxylase, only that with antiparallel subunits, two sets of isologous binding sites and D3 symmetry is in agreement with the symmetry requirements of the cubic crystals.     

The formation of intracellular crystals in midgut glands of Limnoria lignorum

Certain morphological features of intracellular crystal formation within the midgut glands of Limnoria lignorum (Rathke) have been studied with the electron microscope and cytochemical methods. A correlation has been established between Golgi membranes and formation of the crystals. The Prussian blue reaction reveals quantities of iron localized in the intracellular crystals and in small granular structures seen in the apical region of the cells. These granules can be identified as accumulations of Golgi membranes, with which iron-containing particles are associated. When these membrane configurations are studied with the electron microscope, they can be classified and arranged in an assumed sequence which is thought to represent successive stages in the development of crystals. As the membrane systems become progressively specialized, increasing accumulations of dense granular material appear within their interstices. This material is rich in iron and probably represents the component responsible for the positive Prussian blue reaction. This material also appears to be a precursor substance for iron-containing protein molecules which are synthesized and arranged to make up the crystals. These iron-containing molecules are first deposited in orderly array as double rows of dense particles on certain internal membranes of the specialized Golgi complexes. The membranes later disappear and the particles form definitive crystals by rearrangement into a hexagonal close-packed pattern.     

Atomic models by cryo-EM and site-directed spin labeling: application to the N-terminal region of Hsp16.5

We report an approach for determining the structure of macromolecular assemblies by the combined application of cryo-electron microscopy (cryo-EM) and site-directed spin labeling electron paramagnetic resonance spectroscopy (EPR). This approach is illustrated for Hsp16.5, a small heat shock protein that prevents the aggregation of nonnative proteins. The structure of Hsp16.5 has been previously studied by both cryo-EM and X-ray crystallography. The crystal structure revealed a roughly spherical protein shell with dodecameric symmetry; however, residues 1-32 were found to be disordered. The cryo-EM reconstruction at 13 A resolution appeared similar to the crystal structure but with additional internal density corresponding to the N-terminal regions of the 24 subunits. In this study, a systematic application of site-directed spin labeling and EPR spectroscopy was carried out. By combining the EPR constraints from spin label accessibilities and proximities with the cryo-EM density, we obtained an atomic model for a portion of the Hsp16.5 N-terminal region in the context of the oligomeric complex.     

Locating a Lipid at the Portal to the Lipoxygenase Active Site

Lipoxygenase enzymes initiate diverse signaling pathways by specifically directing oxygen to different carbons of arachidonate and other polyunsaturated acyl chains, but structural origins of this specificity have remained unclear. We therefore determined the nature of the lipoxygenase interaction with the polar-end of a paramagnetic lipid by electron paramagnetic resonance spectroscopy. Distances between selected grid points on soybean seed lipoxygenase-1 (SBL1) and a lysolecithin spin-labeled on choline were measured by pulsed (electron) dipolar spectroscopy. The protein grid was designed by structure-based modeling so that five natural side chains were replaced with spin labels. Pairwise distances in 10 doubly spin-labeled mutants were examined by pulsed dipolar spectroscopy, and a fit to the model was optimized. Finally, experimental distances between the lysolecithin spin and each single spin site on SBL1 were also obtained. With these 15 distances, distance geometry localized the polar-end and the spin of the lysolecithin to the region between the two domains in the SBL1 structure, nearest to E236, K260, Q264, and Q544. Mutation of a nearby residue, E256A, relieved the high pH requirement for enzyme activity of SBL1 and allowed lipid binding at pH 7.2. This general approach could be used to locate other flexible molecules in macromolecular complexes.     

Structure of rhodopsin and the metarhodopsin I photointermediate

The structure of the visual pigment rhodopsin in the dark state was first investigated by electron microscopy (EM). More recently, rhodopsin has been crystallised in two different space groups--a tetragonal P4(1) crystal form and a trigonal P3(1) packing arrangement. The structures of the pigment, determined by X-ray crystallography from these two crystal forms, show many similarities, but also significant differences. These differences are most extensive in the G-protein-binding region of the cytoplasmic surface, where the location of the loop between helices 5 and 6 is highly variable. A combination of EM and spin labelling suggests that this loop adopts the native conformation in the P3(1) crystal form. The X-ray structures also show the location of structural water molecules that are important for colour tuning, stabilisation of the ground state and receptor activation, and act as a template for modelling other G-protein-coupled receptors. A major current focus of structural work on rhodopsin is investigation of the activated state of the receptor. After careful spectroscopic characterisation of light activation in two-dimensional crystals, a map of the metarhodopsin I intermediate was obtained by EM from two-dimensional crystals. In addition, NMR studies are providing information about the structure of activated states of rhodopsin. In the future, structural information will show how rhodopsin becomes activated and how it couples to downstream signalling pathways.