Crystal structures of two Bordetella pertussis periplasmic receptors contribute to defining a novel pyroglutamic acid binding DctP subfamily

Gram-negative bacteria have developed several different transport systems for solute uptake. One of these, the tripartite ATP independent periplasmic transport system (TRAP-T), makes use of an extracytoplasmic solute receptor (ESR) which captures specific solutes with high affinity and transfers them to their partner permease complex located in the bacterial inner membrane. We hereby report the structures of DctP6 and DctP7, two such ESRs from Bordetella pertussis. These two proteins display a high degree of sequence and structural similarity and possess the "Venus flytrap" fold characteristic of ESRs, comprising two globular alpha/beta domains hinged together to form a ligand binding cleft. DctP6 and DctP7 both show a closed conformation due to the presence of one pyroglutamic acid molecule bound by highly conserved residues in their respective ligand binding sites. BLAST analyses have revealed that the DctP6 and DctP7 residues involved in ligand binding are strictly present in a number of predicted TRAP-T ESRs from other bacteria. In most cases, the genes encoding these TRAP-T systems are located in the vicinity of a gene coding for a pyroglutamic acid metabolising enzyme. Both the high degree of conservation of these ligand binding residues and the genomic context of these TRAP-T-coding operons in a number of bacterial species, suggest that DctP6 and DctP7 constitute the prototypes of a novel TRAP-T DctP subfamily involved in pyroglutamic acid transport.     

Perturbation of the equilibrium between open and closed conformations of the periplasmic C4-dicarboxylate binding protein from Rhodobacter capsulatus.

A kinetic and thermodynamic analysis has been carried out on the conformational transitions of the periplasmic C4-dicarboxylate binding protein (DctP) from the photosynthetic bacterium Rhodobacter capsulatus. This protein is distinct from other periplasmic binding proteins characterized to date in that the transition between the putative closed-unliganded (BP1) and open-unliganded (BP2) conformations is slow compared to the rate of ligand binding [Walmsley, A. R., Shaw, J. G., & Kelly, D. J. (1992) J. Biol. Chem. 276, 8064-8072]. Using stopped-flow fluorescence techniques, we have probed the conformational dynamics of the closed to open transition of DctP in the absence and presence of ligand. Both the forward rate constant for the BP1 to BP2 interconversion (k1) and the fumarate dissociation rate constant (k-3) were found to increase in a biphasic manner between pH 5 and pH 11. The data were fitted to a two-pKa function which gave pKa values of 10.3 and 5.4 for the BP1 to BP2 interconversion and 8.9 and 4.5 for the closed-liganded (BP3L) to open-liganded (BP2L) transition. An increase in ionic strength at constant pH resulted in a hyperbolic increase in both k1 and k-3 to maximal rates that were similar in each case to the values obtained in pH variation experiments. Measurement of the temperature dependencies of k1 and k-3 also gave similar activation energies. Gibbs free energy, enthalpy, and entropy changes were determined for the open to closed transitions of DctP in both the presence and absence of ligand.(ABSTRACT TRUNCATED AT 250 WORDS)     

Selected-fit versus induced-fit protein binding: kinetic differences and mutational analysis

The binding of a ligand molecule to a protein is often accompanied by conformational changes of the protein. A central question is whether the ligand induces the conformational change (induced-fit), or rather selects and stabilizes a complementary conformation from a pre-existing equilibrium of ground and excited states of the protein (selected-fit). We consider here the binding kinetics in a simple four-state model of ligand-protein binding. In this model, the protein has two conformations, which can both bind the ligand. The first conformation is the ground state of the protein when the ligand is off, and the second conformation is the ground state when the ligand is bound. The induced-fit mechanism corresponds to ligand binding in the unbound ground state, and the selected-fit mechanism to ligand binding in the excited state. We find a simple, characteristic difference between the on- and off-rates in the two mechanisms if the conformational relaxation into the ground states is fast. In the case of selected-fit binding, the on-rate depends on the conformational equilibrium constant, whereas the off-rate is independent. In the case of induced-fit binding, in contrast, the off-rate depends on the conformational equilibrium, while the on-rate is independent. Whether a protein binds a ligand via selected-fit or induced-fit thus may be revealed by mutations far from the protein's binding pocket, or other "perturbations" that only affect the conformational equilibrium. In the case of selected-fit, such mutations will only change the on-rate, and in the case of induced-fit, only the off-rate.     

Unactivated PKR exists in an open conformation capable of binding nucleotides

The dsRNA-activated protein kinase, PKR, plays a pivotal role in the cellular antiviral response. PKR contains an N-terminal dsRNA binding domain (dsRBD) and a C-terminal kinase domain. An autoinhibition model has been proposed in which latent PKR exists in a closed conformation where the substrate binding cleft of the kinase is blocked by the dsRBD. Binding to dsRNA activates the enzyme by inducing an open conformation and enhancing dimerization. We have tested this model by characterizing the affinity and kinetics of binding of a nucleotide substrate to PKR. The fluorescent nucleotide mant-AMPPNP binds to unactivated PKR with a Kd of approximately 30 microM, and the affinity is not strongly affected by autophosphorylation or binding to dsRNA. We observe biphasic binding kinetics in which the fast phase depends on ligand concentration but the slow phase is ligand-independent. The kinetic data fit to a two-step model of ligand binding followed by a slow conformation change. The kinetics are also not strongly affected by phosphorylation state or dsRNA binding. Thus, the equilibrium and kinetic data indicate that the substrate accessibility of the kinase is not modulated by PKR activation state as predicted by the autoinhibition model. In atomic force microscopy images, monomers of the latent protein are resolved with three separate regions linked by flexible, bridgelike structures. The resolution of the individual domains in the images supports a model in which unactivated PKR exists in an open conformation where the kinase domain is accessible and capable of binding substrate.     

X-ray crystallographic studies of streptavidin mutants binding to biotin

On the basis of high resolution crystallographic studies of streptavidin and its biotin complex, three principal binding motifs have been identified that contribute to the tight binding. A flexible binding loop can undergo a conformational change from an open to a closed form when biotin is bound. Additional studies described here of unbound wild-type streptavidin have provided structural views of the open conformation. Several tryptophan residues packing around the bound biotin constitute the second binding motif, one dominated by hydrophobic interactions. Mutation of these residues to alanine or phenylalanine have variable effects on the thermodynamics and kinetics of binding, but they generate only small changes in the molecular structure. Hydrogen bonding interactions also contribute significantly to the binding energetics of biotin, and the D128A mutation which breaks a hydrogen bond between the protein and a ureido NH group results in a significant structural alteration that could mimic an intermediate on the dissociation pathway. In this review, we summarize the structural aspects of biotin recognition that have been gained from crystallographic analyses of wild-type and site-directed streptavidin mutants.     

Characterizing the energetic states of the GluR2 ligand binding domain core-dimer

Tetrameric ligand binding domains of the family of ionotropic glutamate receptors assemble as dimers-of-dimers. Crystallographic studies of several glutamate receptor subtype isolated core-dimers suggest a single stable dimeric conformation. A binding domain dimer has not been captured in other conformations without the aid of biochemical methods to disrupt a critical dimer interface. Molecular dynamics simulations and continuum electrostatics calculations reveal that the active glutamate bound form of the ligand-binding domain found in typical crystal structures is the preferred energetic state of the isolated core-dimer in the presence of agonist glutamate. A desensitized conformational state is a higher energy ligand-bound state of the core-dimer. The resting apo conformational state is comparatively the least energetically favored conformation and does not contain a single state but a set of energetically equivalent conformational core-dimer states. We hypothesize the energetic balance of an open versus closed transmembrane region must be included to characterize the absolute energetic states of the full receptor, which in the presence of the ligand is believed to be a desensitized state.     

How maltose influences structural changes to bind to maltose‐binding protein: Results from umbrella sampling simulation

A well‐studied periplasmic‐binding protein involved in the abstraction of maltose is maltose‐binding protein (MBP), which undergoes a ligand‐induced conformational transition from an open (ligand‐free) to a closed (ligand‐bound) state. Umbrella sampling simulations have been us to estimate the free energy of binding of maltose to MBP and to trace the potential of mean force of the unbinding event using the center‐of‐mass distance between the protein and ligand as the reaction coordinate. The free energy thus obtained compares nicely with the experimentally measured value justifying our theoretical basis. Measurement of the domain angle (N‐terminal‐domain – hinge – C‐terminal‐domain) along the unbinding pathway established the existence of three different states. Starting from a closed state, the protein shifts to an open conformation during the initial unbinding event of the ligand then resides in a semi‐open conformation and later resides predominantly in an open‐state. These transitions along the ligand unbinding pathway have been captured in greater depth using principal component analysis. It is proposed that in mixed‐model, both conformational selection and an induced‐fit mechanism combine to the ligand recognition process in MBP. Proteins 2013. © 2012 Wiley Periodicals, Inc.     

Insights into binding of fatty acids by fatty acid binding proteins

Members of the phylogenetically related intracellular lipid binding protein (iLBP) are characterized by a highly conserved tertiary structure, but reveal distinct binding preferences with regard to ligand structure and conformation, when binding is assessed by the Lipidex method (removal of unbound ligand by hydrophobic polymer) or by isothermal titration calorimetry, a true equilibrium method. Subfamily proteins bind retinoids, subfamily II proteins bind bulky ligands, examples are intestinal bile acid binding protein (I-BABP) and liver fatty acid binding protein (L-FABP) which binds 2 ligand molecules, preferably monounsaturated and n-3 fatty acids. Subfamily III intestinal fatty acid binding protein (I-FABP) binds fatty acid in a bent conformation. The fatty acid bound by subfamily IV FABPs has a U-shaped conformation; here heart (H-) FABP preferably binds n-6, brain (B-) FABP n-3 fatty acids. The ADIFAB-method is a fluorescent test for fatty acid in equilibrium with iLBP and reveals some correlation of binding affinity to fatty acid solubility in the aqueous phase; these data are often at variance with those obtained by the other methods. Thus, in this review published binding data are critically discussed, taking into account on the one hand binding increments calculated for fatty acid double bonds on the basis of the solubility hypothesis, on the other hand the interpretation of calorimetric data on the basis of crystallographic and solution structures of iLBPs.     

The E. coli replication factor DnaC protein exists in two conformations with different nucleotide binding capabilities. I. Determination of the binding mechanism using ATP and ADP fluorescent analogues

The kinetic mechanism of binding of ATP and ADP fluorescent analogues to the E. coli replicative factor DnaC protein has been studied using the fluorescence stopped-flow technique. The experiments have been performed under pseudo-first-order conditions with respect to the nucleotide cofactor or the DnaC concentration. Three relaxation processes are observed at a large excess of the nucleotide, while only two relaxation processes are detected in the excess of the protein. Such behavior of the kinetic system is a diagnostic indication of the presence of the protein conformational equilibrium prior to the ligand binding. The obtained data indicate that the minimum mechanism that describes the observed kinetics includes the conformational transition of the DnaC protein, prior to nucleotide binding, followed by the two-step, sequential association of the cofactor to only one of the protein conformations, as defined by In the examined solution conditions, the conformation of the DnaC protein is shifted toward the state (DnaC)(2) that binds the nucleotide. The lack of any cofactor binding to the (DnaC)(1) state points to the existence of a stringent locking mechanism of the nucleotide binding-site in the protein. Binding of ATP and ADP analogues obeys the same mechanism, with similar rate constants, indicating that ATP and ADP analogues bind to the same protein conformation. The (C)(1) intermediate dominates the distribution of the DnaC protein population in the presence of cofactors. The formation of (C)(1) is accompanied by a low nucleotide fluorescence increase, indicating a hydrophilic environment around the ribose of bound cofactors. Transition to (C)(2) places the ribose region in a highly hydrophobic environment with relative molar fluorescence intensity approximately 8-fold higher than that of the free cofactor. The significance of these results for the functioning of the DnaC protein is discussed.     

Stopped flow kinetics of carbamylcholine binding to membrane bound acetylcholine receptor

Conformational changes upon binding of carbamylcholine to acetylcholine receptor-enriched membrane fragments have been observed by stopped-flow methods using the fluorescent probe ethidium bromide. A model consistent with both equilibrium and kinetic experiments is proposed in which the receptor binds two molecules of carbamylcholine with high affinity in a non-cooperative manner followed by binding of a third and possibly a fourth molecule with increasingly lower affinity. The receptor ligand precomplexes isomerize to different non-interconvertible complexes depending on the number of ligands bound. This kinetic model fits the data for carbamylcholine interactions with receptor prepared initially either in a low or high affinity form for ligands.     

Structural studies of the streptavidin binding loop.

The streptavidin-biotin complex provides the basis for many important biotechnological applications and is an interesting model system for studying high-affinity protein-ligand interactions. We report here crystallographic studies elucidating the conformation of the flexible binding loop of streptavidin (residues 45 to 52) in the unbound and bound forms. The crystal structures of unbound streptavidin have been determined in two monoclinic crystal forms. The binding loop generally adopts an open conformation in the unbound species. In one subunit of one crystal form, the flexible loop adopts the closed conformation and an analysis of packing interactions suggests that protein-protein contacts stabilize the closed loop conformation. In the other crystal form all loops adopt an open conformation. Co-crystallization of streptavidin and biotin resulted in two additional, different crystal forms, with ligand bound in all four binding sites of the first crystal form and biotin bound in only two subunits in a second. The major change associated with binding of biotin is the closure of the surface loop incorporating residues 45 to 52. Residues 49 to 52 display a 3(10) helical conformation in unbound subunits of our structures as opposed to the disordered loops observed in other structure determinations of streptavidin. In addition, the open conformation is stabilized by a beta-sheet hydrogen bond between residues 45 and 52, which cannot occur in the closed conformation. The 3(10) helix is observed in nearly all unbound subunits of both the co-crystallized and ligand-free structures. An analysis of the temperature factors of the binding loop regions suggests that the mobility of the closed loops in the complexed structures is lower than in the open loops of the ligand-free structures. The two biotin bound subunits in the tetramer found in the MONO-b1 crystal form are those that contribute Trp 120 across their respective binding pockets, suggesting a structural link between these binding sites in the tetramer. However, there are no obvious signatures of binding site communication observed upon ligand binding, such as quaternary structure changes or shifts in the region of Trp 120. These studies demonstrate that while crystallographic packing interactions can stabilize both the open and closed forms of the flexible loop, in their absence the loop is open in the unbound state and closed in the presence of biotin. If present in solution, the helical structure in the open loop conformation could moderate the entropic penalty associated with biotin binding by contributing an order-to-disorder component to the loop closure.     

Ligand Induced Conformational Changes of the Human Serotonin Transporter Revealed by Molecular Dynamics Simulations

The competitive inhibitor cocaine and the non-competitive inhibitor ibogaine induce different conformational states of the human serotonin transporter. It has been shown from accessibility experiments that cocaine mainly induces an outward-facing conformation, while the non-competitive inhibitor ibogaine, and its active metabolite noribogaine, have been proposed to induce an inward-facing conformation of the human serotonin transporter similar to what has been observed for the endogenous substrate, serotonin. The ligand induced conformational changes within the human serotonin transporter caused by these three different types of ligands, substrate, non-competitive and competitive inhibitors, are studied from multiple atomistic molecular dynamics simulations initiated from a homology model of the human serotonin transporter. The results reveal that diverse conformations of the human serotonin transporter are captured from the molecular dynamics simulations depending on the type of the ligand bound. The inward-facing conformation of the human serotonin transporter is reached with noribogaine bound, and this state resembles a previously identified inward-facing conformation of the human serotonin transporter obtained from molecular dynamics simulation with bound substrate, but also a recently published inward-facing conformation of a bacterial homolog, the leucine transporter from Aquifex Aoelicus. The differences observed in ligand induced behavior are found to originate from different interaction patterns between the ligands and the protein. Such atomic-level understanding of how an inhibitor can dictate the conformational response of a transporter by ligand binding may be of great importance for future drug design.     

A role for both conformational selection and induced fit in ligand binding by the LAO protein

Molecular recognition is determined by the structure and dynamics of both a protein and its ligand, but it is difficult to directly assess the role of each of these players. In this study, we use Markov State Models (MSMs) built from atomistic simulations to elucidate the mechanism by which the Lysine-, Arginine-, Ornithine-binding (LAO) protein binds to its ligand. We show that our model can predict the bound state, binding free energy, and association rate with reasonable accuracy and then use the model to dissect the binding mechanism. In the past, this binding event has often been assumed to occur via an induced fit mechanism because the protein's binding site is completely closed in the bound state, making it impossible for the ligand to enter the binding site after the protein has adopted the closed conformation. More complex mechanisms have also been hypothesized, but these have remained controversial. Here, we are able to directly observe roles for both the conformational selection and induced fit mechanisms in LAO binding. First, the LAO protein tends to form a partially closed encounter complex via conformational selection (that is, the apo protein can sample this state), though the induced fit mechanism can also play a role here. Then, interactions with the ligand can induce a transition to the bound state. Based on these results, we propose that MSMs built from atomistic simulations may be a powerful way of dissecting ligand-binding mechanisms and may eventually facilitate a deeper understanding of allostery as well as the prediction of new protein-ligand interactions, an important step in drug discovery.     

Alternative binding modes of proline-rich peptides binding to the GYF domain

Recognition of proline-rich sequences plays an important role for the assembly of multiprotein complexes during the course of eukaryotic signal transduction and is mediated by a set of protein folds that share characteristic features. The GYF (glycine-tyrosine-phenylalanine) domain is known as a member of the superfamily of recognition domains for proline-rich sequences. Recent studies on the complexation of the CD2BP2-GYF domain with CD2 peptides showed that the peptide adopts an extended conformation and forms a polyproline type-II helix involving residues Pro4-Pro7 [Freund et al. (2002) EMBO J. 21, 5985-5995]. R/K/GxxPPGxR/K is the key signature for the peptides that bind to the GYF domain [Kofler et al. (2004) J. Biol. Chem. 279, 28292-28297]. In our combined theoretical and experimental study, we show that the peptides adopt a polyproline II helical conformation in the unbound form as well as in the complex. From molecular dynamics simulations, we identify a novel binding mode for the G8W mutant and the wild-type peptide (shifted by one proline in register). In contrast, the conformation of the peptide mutant H9M remains close to the experimentally derived wild-type GYF-peptide complex. Possible functional implications of this altered conformation of the bound ligand are discussed in the light of our experimental and theoretical results.     

Enhanced recA protein binding to Z DNA represents a kinetic perturbation of a general duplex DNA binding pathway

recA protein binding to duplex DNA is enhanced when a B form DNA substrate is replaced with a left-handed Z form helix. This represents a kinetic rather than an equilibrium effect. Binding to Z DNA is much faster than binding to B DNA. In other respects, binding to the two DNA forms is quite similar. recA protein binds to B or Z DNA with a stoichiometry of 1 monomer/4 base pairs. The final protein filament exhibits a right-handed helical structure when either B or Z form DNAs are bound. There are only two evident differences: the kcat for ATP hydrolysis is reduced 3-4-fold when Z DNA is bound, and recA binding at equilibrium is less stable on Z DNA than on B DNA. At steady state, the binding favors B DNA in competition experiments. The results indicate that Z DNA binding by recA protein follows the same pathway as for recA binding to B DNA, but that the nucleation step is faster on the Z form helix.     

Interactions between micellar ligand systems and acceptors: Forms of binding curves

A previously formulated expression describing the competitive binding to an acceptor of two states of a ligand, monomeric and polymeric, coexisting in equilibrium is examined in terms of the different forms of Scatchard plots which may arise in cases of exclusive and of preferential binding of the ligand states. It is shown by differentiation of the binding equation written in Scatchard format, and by numerical examples, that exclusive binding of the monomeric form of ligand leads to Scatchard plots that are either sigmoidal or convex to the abscissa, whereas exclusive binding of the polymeric form results in plots concave to the abscissa and exhibiting a maximum. Particular attention is given to Scatchard plots which possess two critical points, a situation which is shown to be possible when the polymeric form of ligand binds preferentially (but not exclusively) to the acceptor. The two-state ligand concept is especially pertinent to solutes capable of globular micelle formation and several examples are cited of binding studies which have been conducted with such micellar systems. Of these, the chlorpromazine-brain tubulin system is given detailed consideration in order to illustrate the use of the present theory in describing the binding results which exhibit two critical points when plotted in Scatchard format.     

Conformational consequences of coupling bullous pemphigoid antigenic peptides to glutathione-S-transferase and their diagnostic significance.

Recombinant epitopic peptides BP1 and BP2 representing the Bullous pemphigoid autoantigens of BP230 and BP180 bound to the fusion partner glutathione-S-transferase (pGEX-4T-2, Pharmacia) have been previously shown to increase the efficacy of diagnosis of the disease. Using glutathione-S-transferase-bound monomer peptides, the sensitivity of the immunological reaction exceeded that of the free synthetic epitopes and was further increased with the number of epitopic blocks in the multimer fusion products. This has been explained by the avidity effect of the fusion partner dimer formation and the high ligand affinity due to the tandem repetitions of epitopic sequences. However, a beneficial conformation of the bound epitopic peptides might also contribute to the above phenomenon. Circular dichroism (CD) and Fourier transform infrared (FTIR) absorption spectroscopic studies revealed the importance of glutathione-S-transferase to induce and stabilize ordered secondary structures of the epitopic peptides. The free monomer and multimer peptides in aqueous buffer were present as a mixture of unordered and beta-sheet conformation, while binding them to the fusion partner the proportion of ordered secondary structures increased in parallel with the number of antigenic epitopes. The most prominent changes in the conformational state of the monomers in the fusion form were the increase of alpha-helical and beta-sheet and the decrease of unordered conformation, while in the case of oligomeric peptides the adoption of a helical conformation was accompanied by the decrease of beta-sheet structure. An outstanding alpha-helix content (46%) was detected in the case of the trimeric BP1 in its recombinant fusion form.     

Kinetics of drug-DNA interaction. Dependence of the binding mechanism on structure of the ligand

Kinetic and equilibrium studies of the binding of several phenanthridines and acridines to DNA have been performed to investigate the physical processes underlying the direct ligand transfer mechanism of drug-DNA interaction· Substitution of the 6-phenyl ring of dimidium with a p-carboxyl residue, or complete removal of either the 6-substituent or the 3-amino group, does not prevent the phenanthridine chromophore from transferring directly between binding sites. Loss of the aromatic ring increases association rate constants three- to ninefold and enhances dissociation rates by factors of up to 12; the rates of direct transfer and dissociation from site 1 are the most perturbed. The presence of a phenyl ring stabilizes the site 1 complex and lowers the binding constant to site 2. Introduction of the p-carboxyl group does not affect the equilibrium distribution of bound forms but produces equivalent increases (2·5-fold) in forward and reverse rate constants for binding to site 1 and for the direct transfer step. The 3-amino group greatly stabilizes the site 1 complex. Its removal accelerates all kinetic processes except for the reverse transfer step; the transfer rate is enhanced 25-fold and binding to site 2 is increased 12-fold. The dissociation rate from site 1 rises by a factor of 45 and that from site 2 by a factor of 5·8.10-Methyl-9-aminoacridine binds via the direct transfer pathway with rate and equilibrium constants similar to those of the 3-desamino derivative of ethidium. This compound provides the first fully characterized example of an acridine that utilizes bimolecular transfer. By contrast, rivanol (6,9-diamino-2-ethoxyacridine) interacts with DNA via a two-step sequential mechanism analogous to that seen with proflavine, yet its intrinsic association constant is three times higher. This results from tighter ‘external’ attachment to the helix, together with a decrease in equilibrium constant for the insertion step, which is markedly slower than that of proflavine. There appears to be a simple relation between the apparent enthalpy of binding and the number of extracyclic amino substituents on the intercalating chromophore.We propose that the two bound forms that participate in direct ligand transfer represent molecules intercalated via one or other of the grooves of DNA, and that the transfer pathway corresponds to exchange of drug between the wide groove of one helix and the narrow groove of another. The ability to form strongly bound complexes at the surface of the helix appears to play a major role in determining the mechanism of ligand binding.     

Solution NMR study of the monomeric form of p13suc1 protein sheds light on the hinge region determining the affinity for a phosphorylated substrate.

Cyclin-dependent kinase subunit (CKS) proteins bind to cyclin-dependent kinases and target various proteins to phosphorylation and proteolysis during cell division. Crystal structures showed that CKS can exist both in a closed monomeric conformation when bound to the kinase and in an inactive C-terminal beta-strand-exchanged conformation. With the exception of the hinge loop, however, both crystal structures are identical, and no new protein interface is formed in the dimer. Protein engineering studies have pinpointed the crucial role of the proline 90 residue of the p13(suc1) CKS protein from Schizosaccharomyces pombe in the monomer-dimer equilibrium and have led to the concept of a loaded molecular spring of the beta-hinge motif. Mutation of this hinge proline into an alanine stabilizes the protein and prevents the occurrence of swapping. However, other mutations further away from the hinge as well as ligand binding can equally shift the equilibrium between monomer and dimer. To address the question of differential affinity through relief of the strain, here we compare the ligand binding of the monomeric form of wild-type S. pombe p13(suc1) and its hinge mutant P90A in solution by NMR spectroscopy. We indeed observed a 5-fold difference in affinity with the wild-type protein being the most strongly binding. Our structural study further indicates that both wild-type and the P90A mutant proteins adopt in solution the closed conformation but display different dynamic properties in the C-terminal beta-sheet involved in domain swapping and protein interactions.     

High resolution structure of an alternate form of the ferric ion binding protein from Haemophilus influenzae

The periplasmic iron binding protein of pathogenic Gram-negative bacteria performs an essential role in iron acquisition from transferrin and other iron sources. Structural analysis of this protein from Haemophilus influenzae identified four amino acids that ligand the bound iron: His(9), Glu(57), Tyr(195), and Tyr(196). A phosphate provides an additional ligand, and the presence of a water molecule is required to complete the octahedral geometry for stable iron binding. We report the 1.14-A resolution crystal structure of the iron-loaded form of the H. influenzae periplasmic ferric ion binding protein (FbpA) mutant H9Q. This protein was produced in the periplasm of Escherichia coli and, after purification and conversion to the apo form, was iron-loaded. H9Q is able to bind ferric iron in an open conformation. A surprising finding in the present high resolution structure is the presence of EDTA located at the previously determined anion ternary binding site, where phosphate is located in the wild type holo and apo structures. EDTA contributes four of the six coordinating ligands for iron, with two Tyr residues, 195 and 196, completing the coordination. This is the first example of a metal binding protein with a bound metal.EDTA complex. The results suggest that FbpA may have the ability to bind and transport iron bound to biological chelators, in addition to bare ferric iron.