Jurg P. Rosenbusch

Structural basis for sugar translocation through maltoporin channels at 3.1 A resolution

Trimeric maltoporin (LamB protein) facilitates the diffusion of maltodextrins across the outer membrane of Gram-negative bacteria. The crystal structure of maltoporin from Escherichia coli, determined to a resolution of 3.1 angstroms, reveals an 18-stranded, antiparallel beta-barrel that forms the framework of the channel. Three inwardly folded loops contribute to a constriction about halfway through the channel. Six contingent aromatic residues line the channel and form a path from the vestibule to the periplasmic outlet. Soaking of a crystal with maltotriose revealed binding of the sugar to this hydrophobic track across the constriction, which suggests that maltose and linear oligosaccharides may be translocated across the membrane by guided diffusion along this path.

Transmembrane Signaling across the Ligand-Gated FhuA Receptor: Crystal Structures of Free and Ferrichrome-Bound States Reveal Allosteric Changes

FhuA protein facilitates ligand-gated transport of ferrichrome-bound iron across Escherichia coli outer membranes. X-ray analysis at 2.7 A resolution reveals two distinct conformations in the presence and absence of ferrichrome. The monomeric protein consists of a hollow, 22-stranded, antiparallel beta barrel (residues 160-714), which is obstructed by a plug (residues 19-159). The binding site of ferrichrome, an aromatic pocket near the cell surface, undergoes minor changes upon association with the ligand. These are propagated and amplified across the plug, eventually resulting in substantially different protein conformations at the periplasmic face. Our findings reveal the mechanism of signal transmission and suggest how the energy-transducing TonB complex senses ligand binding.

Protein, lipid and water organization in bacteriorhodopsin crystals: a molecular view of the purple membrane at 1.9 A resolution.

BACKGROUND Bacteriorhodopsin (bR) from Halobacterium salinarum is a proton pump that converts the energy of light into a proton gradient that drives ATP synthesis. The protein comprises seven transmembrane helices and in vivo is organized into purple patches, in which bR and lipids form a crystalline two-dimensional array. Upon absorption of a photon, retinal, which is covalently bound to Lys216 via a Schiff base, is isomerized to a 13-cis,15-anti configuration. This initiates a sequence of events - the photocycle - during which a proton is transferred from the Schiff base to Asp85, followed by proton release into the extracellular medium and reprotonation from the cytoplasmic side. RESULTS The structure of bR in the ground state was solved to 1.9 A resolution from non-twinned crystals grown in a lipidic cubic phase. The structure reveals eight well-ordered water molecules in the extracellular half of the putative proton translocation pathway. The water molecules form a continuous hydrogen-bond network from the Schiff-base nitrogen (Lys216) to Glu194 and Glu204 and includes residues Asp85, Asp212 and Arg82. This network is involved both in proton translocation occurring during the photocycle, as well as in stabilizing the structure of the ground state. Nine lipid phytanyl moieties could be modeled into the electron-density maps. Matrix-assisted laser desorption/ionization mass spectrometry (MALDI-MS) analysis of single crystals demonstrated the presence of four different charged lipid species. CONCLUSIONS The structure of protein, lipid and water molecules in the crystals represents the functional entity of bR in the purple membrane of the bacteria at atomic resolution. Proton translocation from the Schiff base to the extracellular medium is mediated by a hydrogen-bond network that involves charged residues and water molecules.

Structural and Functional Characterization of OmpF Porin Mutants Selected for Larger Pore Size II. FUNCTIONAL CHARACTERIZATION

The effects on the channel characteristics of four single amino acid substitutions in OmpF porin and of a deletion mutant in the constriction loop L3 have been studied. These mutations are all located in the narrow section of the channel of the protein that forms pores across the outer membrane of Escherichia coli. The single channel conductance of the deletion mutant (Δ109-114) is decreased by one third, whereas the point mutations do not exhibit significant deviations from that of the wild-type protein. The mutants exhibit drastic changes in ion selectivities. In the wild-type protein, the critical threshold potential (Vc), above which channels close reversibly, exhibits a strong pH dependence, with a titration point of ∼ pH 7.7, which is abolished in all mutants studied here. Diffusion of six monosaccharides is little affected in the point mutants, while four disaccharides are taken up at highly increased rates by the deletion mutant. The functional results, presented here, are correlated to the x-ray structures of the mutants (Lou, K.-L., Saint, N., Prilipov, A., Rummel, G., Benson, S.A., Rosenbusch, J.P., and Schirmer, T. (1996) J. Biol. Chem. 271, 20669-20675). In most, but not all, cases, the structural changes explain the functional alterations observed.

The structure of OmpF porin in a tetragonal crystal form.

BACKGROUND OmpF porin is a trimeric integral membrane protein responsible for the passive transport of small hydrophilic molecules, such as nutrients and waste products, across the outer membrane of Escherichia coli. Very few membrane proteins have been crystallized in three dimensions, yet this stable protein can be obtained in several crystal forms. Comparison of the structures of the same membrane protein in two different packing environments is of major interest, because it allows us to explore the integrity of the structure outside the natural membrane environment. RESULTS The structure of OmpF porin in a tetragonal crystal form with two trimers per asymmetric unit has been determined at 3.2 A resolution and compared with that obtained previously in a trigonal crystal form. The lattice contacts involve only polar atoms, whereas extensive hydrophobic protein-protein interactions were found in the trigonal lattice. The trimer structure is virtually identical in both. CONCLUSIONS Our comparison reveals that the overall structure of OmpF is not influenced by crystal lattice constraints and, thus, presumably bears close resemblance to the in vivo structure. The tetragonal crystal structure has provided the starting model for the phasing of neutron diffraction data obtained from this crystal form, as described in an accompanying article.

[25] Isolation and crystallization of bacterial porin

Publisher Summary This chapter describes isolation and crystallization of bacterial porin. The unusual aspects of porin crystallization are consistent with the micellar interactions involved in crystal formation. The resulting porin crystals are relatively sensitive to the environment. Care must be taken in handling and mounting crystals for X-ray analysis to avoid significant or abrupt changes in the solvent or detergent environment and uncontrolled variations of temperature. Porin has proven to be rather useful for the optimization of conditions to crystallize membrane proteins as it is very stable over a wide range of conditions. Crystallization experiments (at 20°) are successful also using several other detergents with a moderate to high carboxymethyl cellulose (CMC). Initial problems with reproducibility of porin crystallization revealed that a high degree of purity of this protein is required, and that the removal of tightly bound lipoprotein and glycolipid is critical for success. Although current experience is limited, it seems fair to conclude that with a better understanding of protein–amphiphile interactions, of micellar physical chemistry, and with improvement in crystallization techniques, the outlook for understanding membrane protein structure appears bright.

Crystal structure and functional characterization of OmpK36, the osmoporin of Klebsiella pneumoniae

BACKGROUND Porins are channel-forming membrane proteins that confer solute permeability to the outer membrane of Gram-negative bacteria. In Escherichia coli, major nonspecific porins are matrix porin (OmpF) and osmoporin (OmpC), which show high sequence homology. In response to high osmolarity of the medium, OmpC is expressed at the expense of OmpF porin. Here, we study osmoporin of the pathogenic Klebsiella pneumoniae (OmpK36), which shares 87% sequence identity with E. coliOmpC in an attempt to establish why osmoporin is best suited to function at high osmotic pressure. RESULTS The crystal structure of OmpK36 has been determined to a resolution of 3.2 A by molecular replacement with the model of OmpF. The structure of OmpK36 closely resembles that of the search model. The homotrimeric structure is composed of three hollow 16-stranded antiparallel beta barrels, each delimiting a separate pore. Most insertions and deletions with respect to OmpF are found in the loops that protrude towards the cell exterior. A characteristic ten-residue insertion in loop 4 contributes to the subunit interface. At the pore constriction, the replacement of an alanine by a tyrosine residue does not alter the pore profile of OmpK36 in comparison with OmpF because of the different course of the mainchain. Functionally, as characterized in lipid bilayers and liposomes, OmpK36 resembles OmpC with decreased conductance and increased cation selectivity in comparison with OmpF. CONCLUSIONS The osmoporin structure suggests that not an altered pore size but an increase in charge density is the basis for the distinct physico-chemical properties of this porin that are relevant for its preferential expression at high osmotic strength.

X-ray diffraction analysis of matrix porin, an integral membrane protein from Escherichia coli outer membranes☆

An integral membrane protein forming channels across Escherichia coli outer membranes, porin, has been crystallized using a polyethylene glycol or salt-generated two-phase system. Monodispersity and homogeneity of protein-detergent complexes were found to be prerequisites for reproducible formation of crystals amenable to X-ray structural analysis. By varying pH, detergent and buffer type, large crystals of three different habits can be obtained, two of which are discussed in this paper. The tetragonal form (space group P4(2); unit cell dimensions, a = b = 155 A, c = 172 A) is suitable for X-ray analysis. Low temperature induces a change of the space group to P4(2)22, with a single trimer in the asymmetric unit. This crystal form diffracts to a resolution beyond 2.9 A. The hexagonal crystal form (space group P6(3)22; unit cell dimensions, a = b = 93 A, c = 220 A) is limited in resolution to 4.5 A, but reveals a packing arrangement very similar to that in two-dimensional membrane-like crystalline arrays.

Two-dimensional crystal packing of matrix porin. A channel forming protein in Escherichia coli outer membranes

Two-dimensional crystalline porin sheets were obtained by reconstitution of monodisperse protein trimers and phospholipids (dimyristoylphosphatidylcholine) by detergent dialysis, analogous to the reconstitution method used for functional tests (Schindler & Rosenbusch, 1981). Three different packing arrangements were observed: two were hexagonal (with p3 symmetry and lattice constants of 9.3 nm and 7.9 nm), and one rectangular (a = 7.9 nm, b = 13.9 nm). The different crystals could be correlated to phospholipid-to-protein weight ratios of 0.16 to 0.72. At the higher ratio, large hexagonal lattices predominated. Higher lipid ratios did not reveal other crystal forms. The packing arrangement of the large hexagonal form appears very similar to the hexagonal habit of three-dimensional crystal forms (Garavito et al., 1983). The shape of the stain-penetrated triplet indentations appeared conserved in the crystal forms to a resolution of 2.2 nm. The mass distribution between triplets, however, were significantly different. They are likely to correspond primarily to lipids. Mass determinations of unstained porin by scanning transmission electron microscopy showed that unit cells consisted of single trimers. The mass found (100,000 daltons) is in good agreement with the value obtained by sedimentation equilibrium analysis.

Molecular mechanism for the crystallization of bacteriorhodopsin in lipidic cubic phases.

Crystals of transmembrane proteins may be grown from detergent solutions or in a matrix of membranous lipid bilayers existing in a liquid crystalline state and forming a cubic phase (in cubo). While crystallization in micellar solutions appears analogous to that for soluble proteins, crystallization in lipidic matrices is poorly understood. As this method was shown to be applicable to several membrane proteins, understanding its mechanism will facilitate a rational design of crystallization, minimizing the laborious screening of a large number of parameters. Using polarization microscopy and low‐angle X‐ray diffraction, experimental evidence is provided to support a mechanistic model for the in cubo crystallization of bacteriorhodopsin in a lipid matrix. Membrane proteins are thought to reside in curved lipid bilayers, to diffuse into patches of lower curvature and to incorporate into lattices which associate to form highly ordered three‐dimensional crystals. Critical testing of this model is necessary to generalize it to other membrane proteins.