Sedimentation Coefficient S20 Research Articles

Self-association of the glycopeptide antibiotic teicoplanin A2 in aqueous solution studied by molecular hydrodynamics

The natural glycopeptide antibiotic teicoplanin is used for the treatment of serious Gram-positive related bacterial infections and can be administered intravenously, intramuscularly, topically (ocular infections), or orally. It has also been considered for targeting viral infection by SARS-CoV-2. The hydrodynamic properties of teicoplanin A2 (M1 = 1880 g/mol) were examined in phosphate chloride buffer (pH 6.8, I = 0.10 M) using sedimentation velocity and sedimentation equilibrium in the analytical ultracentrifuge together with capillary (rolling ball) viscometry. In the concentration range, 0–10 mg/mL teicoplanin A2 was found to self-associate plateauing > 1 mg/mL to give a molar mass of (35,400 ± 1000) g/mol corresponding to ~ (19 ± 1) mers, with a sedimentation coefficient s20, w = ~ 4.65 S. The intrinsic viscosity [eta] was found to be (3.2 ± 0.1) mL/g: both this, the value for s20,w and the hydrodynamic radius from dynamic light scattering are consistent with a globular macromolecular assembly, with a swelling ratio through dynamic hydration processes of ~ 2.

The solution structure of the human IgG2 subclass is distinct from those for human IgG1 and IgG4 providing an explanation for their discrete functions

Human IgG2 antibody displays distinct therapeutically-useful properties compared with the IgG1, IgG3, and IgG4 antibody subclasses. IgG2 is the second most abundant IgG subclass, being able to bind human FcγRII/FcγRIII but not to FcγRI or complement C1q. Structural information on IgG2 is limited by the absence of a full-length crystal structure for this. To this end, we determined the solution structure of human myeloma IgG2 by atomistic X-ray and neutron-scattering modeling. Analytical ultracentrifugation disclosed that IgG2 is monomeric with a sedimentation coefficient (s20, w0) of 7.2 S. IgG2 dimer formation was ≤5% and independent of the buffer conditions. Small-angle X-ray scattering in a range of NaCl concentrations and in light and heavy water revealed that the X-ray radius of gyration (Rg ) is 5.2-5.4 nm, after allowing for radiation damage at higher concentrations, and that the neutron Rg value of 5.0 nm remained unchanged in all conditions. The X-ray and neutron distance distribution curves (P(r)) revealed two peaks, M1 and M2, that were unchanged in different buffers. The creation of >123,000 physically-realistic atomistic models by Monte Carlo simulations for joint X-ray and neutron-scattering curve fits, constrained by the requirement of correct disulfide bridges in the hinge, resulted in the determination of symmetric Y-shaped IgG2 structures. These molecular structures were distinct from those for asymmetric IgG1 and asymmetric and symmetric IgG4 and were attributable to the four hinge disulfides. Our IgG2 structures rationalize the existence of the human IgG1, IgG2, and IgG4 subclasses and explain the receptor-binding functions of IgG2.

Oligomeric state of αB-crystallin under crowded conditions

Small heat shock proteins (sHsps) are molecular chaperones preventing protein aggregation. Dynamics of quaternary structure plays an important role in the chaperone-like activity of sHsps. However, an interrelation between the oligomeric state and chaperone-like activity of sHsps remains insufficiently characterized. Most of the accumulated data were obtained in dilute protein solutions, leaving the question of the oligomeric state of sHsps in crowded intracellular media largely unanswered. Here, we analyzed the effect of crowding on the oligomeric state of αB-crystallin (αB-Cr) using analytical ultracentrifugation. Marked increase in the sedimentation coefficient of αB-Cr was observed in the presence of polyethylene glycol (PEG), polyvinylpyrrolidone (PVP) and trimethylamine N-oxide (TMAO) at 48 °C. An especially pronounced effect was detected for the PEG and TMAO mixture, where the sedimentation coefficient (s20,w) of αB-Cr increased from 10.7 S in dilute solution up to 40.7 S in the presence of crowding agents. In the PEG + TMAO mixture, addition of model protein substrate (muscle glycogen phosphorylase b) induced dissociation of large αB-Cr oligomers and formation of complexes with smaller sedimentation coefficients, supporting the idea that, under crowding conditions, protein substrates can promote dissociation of large αB-Cr oligomers.

Modeling the Early Stages of Aggregation in Disordered Elastin-Like Proteins

Elastin-like proteins (ELPs) are known to aggregate reversibly above a defined transition temperature. Because aggregation occurs reversibly, ELPs can be a useful system to study the early stages of this process in proteins. Previous studies suggested that, as temperature increases, ELPs experience an increased propensity for type II β-turns. However, how the ELPs behave during the aggregation itself is still elusive. Here, we investigate a hypothesis: aggregation is initiated at the β-turn positions. To test this hypothesis, we designed an ELP construct (ELP40, 16 kDa) suitable for NMR measurements. We observe that this construct does indeed exhibit increase β-turn propensity at higher temperature. Based on this observation, a series of structural ensembles were generated incorporating differing amounts of β-turn bias, from 1% to 50% throughout the chain. To mimic the early stages of aggregation, two monomers were paired, assuming preferential interaction at β-turn regions. This approach was justified by the observation that buried hydrophobic turns are frequently observed to interact in the PDB. Following dimerization, the ensemble-averaged hydrodynamic properties were calculated for each degree of β-turn bias, and results were compared with analytical ultracentrifugation (AUC) experiments on ELPs in at various temperatures. We find that the temperature dependence of the sedimentation coefficient (s20,W) can be reproduced by increasing the β-turn content in the structural ensemble. This analysis allows us to estimate the secondary structure and weak associations under experimental conditions. Moreover, our models can be used to generate structural hypotheses for the early stages of IDP self-association. In addition, because disordered proteins frequently exhibit weak biases in secondary structure propensity, these structurally-biased ensemble calculations may be a promising method for modeling IDPs generally.

Characterization of Factor VIII Immune Complexes By Analytical Ultracentrifugation

Inhibitory polyclonal IgG antibodies (inhibitors) to factor VIII (fVIII) represent the most significant complication in patients with congenital hemophilia A. FVIII also is the most frequently targeted coagulation factor in autoimmunity. Antibodies recognizing epitopes in the fVIII A2 and C2 domains are present in most inhibitor patients. In the current study, we characterized the hydrodynamic properties of fVIII immune complexes formed by murine anti-human anti-A2 and anti-C2 fVIII monoclonal antibodies (MAbs) 4A4 and 3D12. 4A4 is representative of the most frequently identified group of anti-A2 MAbs identified in the murine hemophilia A immune response to human fVIII. 3D12 is a classical anti-C2 MAb that inhibits the binding of fVIII to von Willebrand factor (VWF) and phospholipid membranes. Velocity sedimentation of immune complexes formed by varying ratios of 4A4 and 3D12 with a high-expression fVIII construct designated ET3 was conducted at 55,000g and 20 °C by measuring protein absorbance at 280 nm in a Beckman XL-I analytical ultracentrifuge. Sedimentation coefficient (s20,w) distributions of fVIII, MAbs and immune complexes were determined using SEDFIT. The sedimentation coefficients of fVIII in the absence of MAbs and of the MAbs in the absence of fVIII were 7.7 S and 6.4 S, respectively. Under conditions of excess MAb (equimolar 4A4 and 3D12 each in five-fold molar excess over fVIII), a 10.3 S immune complex was observed, representing singly-ligated MAbs (Figure, red trace). Under conditions of excess fVIII (fVIII in four-fold molar excess over equimolar 4A4 and 3D12), 11.9 S doubly-ligated MAb complexes were observed (Figure, green trace). A mixture containing equimolar fVIII and 4A4/3D12 MAb binding sites produced a dominant 14.0 S species and a minor 18.8 S species, indicative of cross-linked 3D12-fVIII-4A4 immune complexes (Figure, blue trace). Indefinite association or immunoprecipitation was not observed. These results demonstrate that a biclonal, bivalent anti-fVIII antibody population can form higher-order immune complexes. These complexes may be a driving factor in the immune response to fVIII by promoting B cell activation and/or antigen presentation. Additionally, these results indicate that analytical ultracentrifugation is a useful tool to characterize fVIII immune complexes. [Display omitted] DisclosuresNo relevant conflicts of interest to declare.

Domain structure of human complement C4b extends with increasing NaCl concentration: implications for its regulatory mechanism.

During the activation of complement C4 to C4b, the exposure of its thioester domain (TED) is crucial for the attachment of C4b to activator surfaces. In the C4b crystal structure, TED forms an Arg104-Glu1032 salt bridge to tether its neighbouring macroglobulin (MG1) domain. Here, we examined the C4b domain structure to test whether this salt bridge affects its conformation. Dual polarisation interferometry of C4b immobilised at a sensor surface showed that the maximum thickness of C4b increased by 0.46 nm with an increase in NaCl concentration from 50 to 175 mM NaCl. Analytical ultracentrifugation showed that the sedimentation coefficient s20,w of monomeric C4b of 8.41 S in 50 mM NaCl buffer decreased to 7.98 S in 137 mM NaCl buffer, indicating that C4b became more extended. Small angle X-ray scattering reported similar RG values of 4.89-4.90 nm for C4b in 137-250 mM NaCl. Atomistic scattering modelling of the C4b conformation showed that TED and the MG1 domain were separated by 4.7 nm in 137-250 mM NaCl and this is greater than that of 4.0 nm in the C4b crystal structure. Our data reveal that in low NaCl concentrations, both at surfaces and in solution, C4b forms compact TED-MG1 structures. In solution, physiologically relevant NaCl concentrations lead to the separation of the TED and MG1 domain, making C4b less capable of binding to its complement regulators. These conformational changes are similar to those seen previously for complement C3b, confirming the importance of this salt bridge for regulating both C4b and C3b.

The effects of monovalent metal ions on the conformation of human telomere DNA using analytical ultracentrifugation.

A human telomere DNA segment (HT-DNA) can fold into a G-quadruplex in the presence of some monovalent cations. These cations can interact with the phosphate groups of the DNA segment and/or with the O6 oxygen atom of guanines, which are called non-specific interactions and specific interactions, respectively. However, until now how these two interactions affect the structure of HT-DNA has not been well understood. In this study, a combination of analytical ultracentrifugation (AUC) and circular dichroism (CD) was used to explore the effects of these two interactions on the structure of a 22-mer single-stranded DNA with a sequence of 5'-AGGG(TTAGGG)3-3'. The results showed that the standard sedimentation coefficient (s20,w) of HT-DNA starts to increase when the concentration of potassium ions (CK(+)) is higher than 10.0 µM due to the formation of a G-quadruplex through specific interactions. Whereas, for a control DNA, a higher CK(+) value of 1.0 mM was needed for increasing s20,w due to non-specific interactions. Moreover, potassium ions could promote the formation of the G-quadruplex much more easily than lithium, sodium and cesium ions, presumably due to its appropriate size in the dehydrated state and easier dehydration. The molar mass of DNA at different cation concentrations was nearly a constant and close to the theoretical value of the molar mass of monomeric HT-DNA, indicating that what we observed is the structural change of individual DNA chains.

The Solution Structures of Two Human IgG1 Antibodies Show Conformational Stability and Accommodate Their C1q and FcγR Ligands

The human IgG1 antibody subclass shows distinct properties compared with the IgG2, IgG3, and IgG4 subclasses and is the most exploited subclass in therapeutic antibodies. It is the most abundant subclass, has a half-life as long as that of IgG2 and IgG4, binds the FcγR receptor, and activates complement. There is limited structural information on full-length human IgG1 because of the challenges of crystallization. To rectify this, we have studied the solution structures of two human IgG1 6a and 19a monoclonal antibodies in different buffers at different temperatures. Analytical ultracentrifugation showed that both antibodies were predominantly monomeric, with sedimentation coefficients s20,w (0) of 6.3-6.4 S. Only a minor dimer peak was observed, and the amount was not dependent on buffer conditions. Solution scattering showed that the x-ray radius of gyration Rg increased with salt concentration, whereas the neutron Rg values remained unchanged with temperature. The x-ray and neutron distance distribution curves P(r) revealed two peaks, M1 and M2, whose positions were unchanged in different buffers to indicate conformational stability. Constrained atomistic scattering modeling revealed predominantly asymmetric solution structures for both antibodies with extended hinge structures. Both structures were similar to the only known crystal structure of full-length human IgG1. The Fab conformations in both structures were suitably positioned to permit the Fc region to bind readily to its FcγR and C1q ligands without steric clashes, unlike human IgG4. Our molecular models for human IgG1 explain its immune activities, and we discuss its stability and function for therapeutic applications.

The Fab Conformations in the Solution Structure of Human Immunoglobulin G4 (IgG4) Restrict Access to Its Fc Region: IMPLICATIONS FOR FUNCTIONAL ACTIVITY

Human IgG4 antibody shows therapeutically useful properties compared with the IgG1, IgG2, and IgG3 subclasses. Thus IgG4 does not activate complement and shows conformational variability. These properties are attributable to its hinge region, which is the shortest of the four IgG subclasses. Using high throughput scattering methods, we studied the solution structure of wild-type IgG4(Ser(222)) and a hinge mutant IgG4(Pro(222)) in different buffers and temperatures where the proline substitution suppresses the formation of half-antibody. Analytical ultracentrifugation showed that both IgG4 forms were principally monomeric with sedimentation coefficients s20,w(0) of 6.6-6.8 S. A monomer-dimer equilibrium was observed in heavy water buffer at low temperature. Scattering showed that the x-ray radius of gyration Rg was unchanged with concentration in 50-250 mm NaCl buffers, whereas the neutron Rg values showed a concentration-dependent increase as the temperature decreased in heavy water buffers. The distance distribution curves (P(r)) revealed two peaks, M1 and M2, that shifted below 2 mg/ml to indicate concentration-dependent IgG4 structures in addition to IgG4 dimer formation at high concentration in heavy water. Constrained x-ray and neutron scattering modeling revealed asymmetric solution structures for IgG4(Ser(222)) with extended hinge structures. The IgG4(Pro(222)) structure was similar. Both IgG4 structures showed that their Fab regions were positioned close enough to the Fc region to restrict C1q binding. Our new molecular models for IgG4 explain its inability to activate complement and clarify aspects of its stability and function for therapeutic applications.

The Solution Structure of Heparan Sulfate Differs from That of Heparin: IMPLICATIONS FOR FUNCTION

The highly sulfated polysaccharides heparin and heparan sulfate (HS) play key roles in the regulation of physiological and pathophysiological processes. Despite its importance, no molecular structures of free HS have been reported up to now. By combining analytical ultracentrifugation, small angle x-ray scattering, and constrained scattering modeling recently used for heparin, we have analyzed the solution structures for eight purified HS fragments dp6-dp24 corresponding to the predominantly unsulfated GlcA-GlcNAc domains of heparan sulfate. Unlike heparin, the sedimentation coefficient s20,w of HS dp6-dp24 showed a small rotor speed dependence, where similar s20,w values of 0.82-1.26 S (absorbance optics) and 1.05-1.34 S (interference optics) were determined. The corresponding x-ray scattering measurements of HS dp6-dp24 gave radii of gyration RG values from 1.03 to 2.82 nm, cross-sectional radii of gyration RXS values from 0.31 to 0.65 nm, and maximum lengths L from 3.0 to 10.0 nm. These data showed that HS has a longer and more bent structure than heparin. Constrained scattering modeling starting from 5,000 to 12,000 conformationally randomized HS structures gave best fit dp6-dp24 molecular structures that were longer and more bent than their equivalents in heparin. Alternative fits were obtained for HS dp18 and dp24, indicating their higher bending and flexibility. We conclude that HS displays bent conformations that are significantly distinct from that for heparin. The difference is attributed to the different predominant monosaccharide sequence and reduced sulfation of HS, indicating that HS may interact differently with proteins compared with heparin.

Scaling laws between the hydrodynamic parameters and molecular weight of linear poly(2-ethyl-2-oxazoline)

Poly(2-ethyl-2-oxazoline) (PEtOx), as an alternative polymer to poly(ethylene glycol), has potential applications in biomedical fields. The hydrodynamic parameters, such as the hydrodynamic radius and sedimentation coefficient, are important to understand its dynamics and properties, including its effect on the interactions between proteins and cells. In this study, we have investigated the hydrodynamic properties and thermodynamic parameters of a series of narrowly distributed PEtOx polymers with molecular weights ranging from 1.3 × 103 to 3.1 × 105 g mol−1, and the scaling laws between them by the use of a combination of analytical ultracentrifugation and laser light scattering. It is found that the sedimentation coefficient (s20,w) and hydrodynamic radius (Rh,0) at infinite dilution scale with molecular weight (Mw) as s20,w = Ks × Mαw = 0.0071 (S) × M0.462±0.019w and Rh,0 = KRh × Mβw = 0.0179 (nm) × M0.539±0.012w, respectively.

Characterization and Solution Structure of Mouse Myristoylated Methionine Sulfoxide Reductase A

Methionine sulfoxide reductase A is an essential enzyme in the antioxidant system which scavenges reactive oxygen species through cyclic oxidation and reduction of methionine and methionine sulfoxide. The cytosolic form of the enzyme is myristoylated, but it is not known to translocate to membranes, and the function of myristoylation is not established. We compared the biochemical and biophysical properties of myristoylated and nonmyristoylated mouse methionine sulfoxide reductase A. These were almost identical for both forms of the enzyme, except that the myristoylated form reduced methionine sulfoxide in protein much faster than the nonmyristoylated form. We determined the solution structure of the myristoylated protein and found that the myristoyl group lies in a relatively surface exposed "myristoyl nest." We propose that this structure functions to enhance protein-protein interaction.

C-reactive Protein Exists in an NaCl Concentration-dependent Pentamer-Decamer Equilibrium in Physiological Buffer

C-reactive protein (CRP) is an acute phase protein of the pentraxin family that binds ligands in a Ca(2+)-dependent manner, and activates complement. Knowledge of its oligomeric state in solution and at surfaces is essential for functional studies. Analytical ultracentrifugation showed that CRP in 2 mM Ca(2+) exhibits a rapid pentamer-decamer equilibrium. The proportion of decamer decreased with an increase in NaCl concentration. The sedimentation coefficients s(20,w)(0) of pentameric and decameric CRP were 6.4 S and in excess of 7.6 S, respectively. In the absence of Ca(2+), CRP partially dissociates into its protomers and the NaCl concentration dependence of the pentamer-decamer equilibrium is much reduced. By x-ray scattering, the radius of gyration R(G) values ranged from 3.7 nm for the pentamer to above 4.0 nm for the decamer. An averaged K(D) value of 21 microM in solution (140 mM NaCl, 2 mM Ca(2+)) was determined by x-ray scattering and modeling based on crystal structures for the pentamer and decamer. Surface plasmon resonance showed that CRP self-associates on a surface with immobilized CRP with a similar K(D) value of 23 microM (140 mM NaCl, 2 mM Ca(2+)), whereas CRP aggregates in low salt. It is concluded that CRP is reproducibly observed in a pentamer-decamer equilibrium in physiologically relevant concentrations both in solution and on surfaces. Both 2 mM Ca(2+) and 140 mM NaCl are essential for the integrity of CRP in functional studies and understanding the role of CRP in the acute phase response.

The Nonplanar Secretory IgA2 and Near Planar Secretory IgA1 Solution Structures Rationalize Their Different Mucosal Immune Responses

Secretory IgA (SIgA) is the most prevalent human antibody and is central to mucosal immunity. It exists as two subclasses, SIgA1 and SIgA2, where SIgA2 has a shorter hinge joining the Fab and Fc regions. Both forms of SIgA are predominantly dimeric and contain an additional protein called the secretory component (SC) that is attached during the secretory process and is believed to protect SIgA in harsh mucosal conditions. Here we locate the five SC domains relative to dimeric IgA2 within SIgA2 using constrained scattering modeling. The x-ray and sedimentation parameters showed that SIgA2 has an extended solution structure. The constrained modeling of SIgA2 was initiated using two IgA2 monomers that were positioned according to our best fit solution structure for dimeric IgA1. SC was best located along the convex edge of the Fc-Fc region. The best fit models showed that SIgA2 is significantly nonplanar in its structure, in distinction to our previous near planar SIgA1 structure. Both the shorter IgA2 hinges and the presence of SC appear to displace the four Fab regions out of the Fc plane in SIgA2. This may explain the noncovalent binding of SC in some SIgA2 molecules. This nonplanar structure is predicted to result in specific immune properties for SIgA2 and SIgA1. It may explain differences observed between the SIgA1 and SIgA2 subclasses in terms of their interactions with antigens, susceptibility to proteases, effects on receptors, and distribution in different tissues. The different structures account for the prevalence of both forms in mucosal secretions.

A Comprehensive Model for Packing and Hydration for Amyloid Fibrils of β2-Microglobulin

Volume can provide informative structural descriptions of macromolecules such as proteins in solution because a final volumetric outcome accompanies the exquisite equipoise of packing effects between residues, and residues and waters inside and outside proteins. Here we performed systematic investigations on the volumetric nature of the amyloidogenic conformations of beta2-microglobulin (beta2-m) and its amyloidogenic core peptide, K3, using a high precision densitometer. The transition from the acid-denatured beta2-m to the mature amyloid fibrils was accompanied by a positive change in the partial specific volume, which was larger than that observed for the transition from the acid-denatured beta2-m to the native structure. The data imply that the mature amyloid fibrils are more voluminous than the native structure because of a sparse packing density of side chains. In contrast, the formation of the mature amyloid-like fibrils of the K3 from the random coil was followed by a considerable decrease in the partial specific volume, suggesting a highly compact core structure. Interestingly, the immature amyloid-like fibrils of beta2-m exhibited a volume intermediate between those of the mature fibrils of beta2-m and K3, because of the core structure at their center and the relatively noncompact region around the core with much hydration. These volumetric differences would result from the nature of main-chain-dominated fibrillogenesis. We suggest comprehensive models for these three types of fibrils illustrating packing and hydrational states.

Structure and Evolution of a Novel Dimeric Enzyme from a Clinically Important Bacterial Pathogen

Dihydrodipicolinate synthase (DHDPS) catalyzes the first committed step of the lysine biosynthetic pathway. The tetrameric structure of DHDPS is thought to be essential for enzymatic activity, as isolated dimeric mutants of Escherichia coli DHDPS possess less than 2.5% that of the activity of the wild-type tetramer. It has recently been proposed that the dimeric form lacks activity due to increased dynamics. Tetramerization, by buttressing two dimers together, reduces dynamics in the dimeric unit and explains why all active bacterial DHDPS enzymes to date have been shown to be homo-tetrameric. However, in this study we demonstrate for the first time that DHDPS from methicillin-resistant Staphylococcus aureus (MRSA) exists in a monomer-dimer equilibrium in solution. Fluorescence-detected analytical ultracentrifugation was employed to show that the dimerization dissociation constant of MRSA-DHDPS is 33 nm in the absence of substrates and 29 nm in the presence of (S)-aspartate semialdehyde (ASA), but is 20-fold tighter in the presence of the substrate pyruvate (1.6 nm). The MRSA-DHDPS dimer exhibits a ping-pong kinetic mechanism (k(cat)=70+/-2 s(-1), K(m)(Pyruvate)=0.11+/-0.01 mm, and K(m)(ASA)=0.22+/-0.02 mm) and shows ASA substrate inhibition with a K(si)(ASA) of 2.7+/-0.9 mm. We also demonstrate that unlike the E. coli tetramer, the MRSA-DHDPS dimer is insensitive to lysine inhibition. The near atomic resolution (1.45 A) crystal structure confirms the dimeric quaternary structure and reveals that the dimerization interface of the MRSA enzyme is more extensive in buried surface area and noncovalent contacts than the equivalent interface in tetrameric DHDPS enzymes from other bacterial species. These data provide a detailed mechanistic insight into DHDPS catalysis and the evolution of quaternary structure of this important bacterial enzyme.

Structural and Functional Characterization of Recombinant Matrilin-3 A-domain and Implications for Human Genetic Bone Diseases

Mutations in matrilin-3 result in multiple epiphyseal dysplasia, which is characterized by delayed and irregular bone growth and early onset osteoarthritis. The majority of disease-causing mutations are located within the beta-sheet of the single A-domain of matrilin-3, suggesting that they disrupt the structure and/or function of this important domain. Indeed, the expression of mutant matrilin-3 results in its intracellular retention within the rough endoplasmic reticulum of cells, where it elicits an unfolded protein response. To understand the folding characteristics of the matrilin-3 A-domain we determined its structure using CD, analytical ultracentrifugation, and dual polarization interferometry. This study defined novel structural features of the matrilin-3 A-domain and identified a conformational change induced by the presence or the absence of Zn(2+). In the presence of Zn(2+) the A-domain adopts a more stable "tighter" conformation. However, after the removal of Zn(2+) a potential structural rearrangement of the metal ion-dependent adhesion site motif occurs, which leads to a more "relaxed" conformation. Finally, to characterize the interactions of the matrilin-3 A-domain we performed binding studies on a BIAcore using type II and IX collagen and cartilage oligomeric matrix protein. We were able to demonstrate that it binds to type II and IX collagen and cartilage oligomeric matrix protein in a Zn(2+)-dependent manner. Furthermore, we have also determined that the matrilin-3 A-domain appears to bind exclusively to the COL3 domain of type IX collagen and that this binding is abolished in the presence of a disease causing mutation in type IX collagen.

An Archaeal Peptidase Assembles into Two Different Quaternary Structures

Cellular proteolysis involves large oligomeric peptidases that play key roles in the regulation of many cellular processes. The cobalt-activated peptidase TET1 from the hyperthermophilic Archaea Pyrococcus horikoshii (PhTET1) was found to assemble as a 12-subunit tetrahedron and as a 24-subunit octahedral particle. Both quaternary structures were solved by combining x-ray crystallography and cryoelectron microscopy data. The internal organization of the PhTET1 particles reveals highly self-compartmentalized systems made of networks of access channels extended by vast catalytic chambers. The two edifices display aminopeptidase activity, and their organizations indicate substrate navigation mechanisms different from those described in other large peptidase complexes. Compared with the tetrahedron, the octahedron forms a more expanded hollow structure, representing a new type of giant peptidase complex. PhTET1 assembles into two different quaternary structures because of quasi-equivalent contacts that previously have only been identified in viral capsids.

The Ectodomain of the Viral Receptor YueB Forms a Fiber That Triggers Ejection of Bacteriophage SPP1 DNA

The irreversible binding of bacteriophages to their receptor(s) in the host cell surface triggers release of the naked genome from the virion followed by transit of viral DNA to the host cell cytoplasm. We have purified, for the first time, a receptor from a Gram-positive bacterium that is active to trigger viral DNA ejection in vitro. This extracellular region ("ectodomain") of the Bacillus subtilis protein YueB (YueB780) was a 7 S elongated dimer forming a 36.5-nm-long fiber. YueB780 bound to the tail tip of bacteriophage SPP1. Although a stable receptor-phage interaction occurred between 0 and 37 degrees C, complete blocking of phage DNA release or partial ejection events were observed at temperatures below 15 degrees C. We also showed that the receptor was exposed to the B. subtilis surface. YueB differed structurally from phage receptors from Gram-negative bacteria. Its properties revealed a fiber spanning the full length of the 30-nm-thick peptidoglycan layer. The fiber is predicted to be anchored in the cell membrane through transmembrane segments. These features, highly suitable for a virus receptor in Gram-positive bacteria, are very likely shared by a large number of phage receptors.

Solution Structure of the Complex between CR2 SCR 1-2 and C3d of Human Complement: An X-ray Scattering and Sedimentation Modelling Study

Complement receptor type 2 (CR2, CD21) forms a tight complex with C3d, a fragment of C3, the major complement component. Previous crystal structures of the C3d-CR2 SCR 1-2 complex and free CR2 SCR 1-2 showed that the two SCR domains of CR2 form contact with each other in a closed V-shaped structure. SCR 1 and SCR 2 are connected by an unusually long eight-residue linker peptide. Medium-resolution solution structures for CR2 SCR 1-2, C3d, and their complex were determined by X-ray scattering and analytical ultracentrifugation. CR2 SCR 1-2 is monomeric. For CR2 SCR 1-2, its radius of gyration R(G) of 2.12(+/-0.05) nm, its maximum length of 10nm and its sedimentation coefficient s20,w(o) of 1.40(+/-0.03) S do not agree with those calculated from the crystal structures, and instead suggest an open structure. Computer modelling of the CR2 SCR1-2 solution structure was based on the structural randomisation of the eight-residue linker peptide joining SCR 1 and SCR 2 to give 9950 trial models. Comparisons with the X-ray scattering curve indicated that the most favoured arrangements for the two SCR domains corresponded to an open V-shaped structure with no contacts between the SCR domains. For C3d, X-ray scattering and sedimentation velocity experiments showed that it exists as a monomer-dimer equilibrium with a dissociation constant of 40 microM. The X-ray scattering curve for monomeric C3d gave an R(G) value of 1.95 nm, and this together with its s20,w(o) value of 3.17 S gave good agreement with the monomeric C3d crystal structure. Modelling of the C3d dimer gave good agreements with its scattering and ultracentrifugation parameters. For the complex, scattering and ultracentrifugation experiments showed that there was no dimerisation, indicating that the C3d dimerisation site was located close to the CR2 SCR 1-2 binding site. The R(G) value of 2.44(+/-0.1) nm, its length of 9 nm and its s20,w(o) value of 3.45(+/-0.01) S showed that its structure was not much more elongated than that of C3d. Calculations with 9950 models of CR2 SCR 1-2 bound to C3d through SCR 2 showed that SCR 1 formed an open V-shaped structure with SCR 2 and was capable of interacting with the surface of C3d. We conclude that the open V-shaped structures formed by CR2 SCR 1-2, both when free and when bound to C3d, are optimal for the formation of a tight two-domain interaction with its ligand C3d.