Interdomain motion in liver alcohol dehydrogenase. Structural and energetic analysis of the hinge bending mode

A study of the hinge bending mode in the enzyme liver alcohol dehydrogenase is made by use of empirical energy functions. The enzyme is a dimer, with each monomer composed of a coenzyme binding domain and a catalytic domain with a large cleft between the two. Superposition of the apoenzyme and holoenzyme crystal structures is used to determine a rigid rotation axis for closing of the cleft. It is shown that a rigid body transformation of the apoenzyme to the holoenzyme structure corresponds to a 10 degrees rotation of the catalytic domain about this axis. The rotation is not along the least-motion path for closing of the cleft but instead corresponds to the catalytic domain coming closer to the coenzyme binding domain by a sliding motion. Estimation of the energy associated with the interdomain motion of the apoenzyme over a range of 90 degrees (-40 to 50 degrees, where 0 degrees corresponds to the minimized crystal structure) demonstrates that local structural relaxation makes possible large-scale rotations with relatively small energy increments. A variety of structural rearrangements associated with the domain motion are characterized. They involve the hinge region residues that provide the covalent connections between the two domains and certain loop regions that are brought into contact by the rotation. Differences between the energy minimized and the holoenzyme structures point to the existence of alternative conformations for loops and to the importance of the ligands in the structural rearrangements.     

Investigation of Domain Motions in Bacteriophage T4 Lysozyme

Abstract

Hinge-bending in T4 lysozyme has been inferred from single amino acid mutant crystalline allomorphs by Matthews and coworkers. This raises an important question: are the different conformers in the unit cell artifacts of crystal packing forces, or do they represent different solution state structures? The objective of this theoretical study is to determine whether domain motions and hinge-bending could be simulated in T4 lysozyme using molecular dynamics. An analysis of a 400 ps molecular dynamics simulation of the 164 amino acid enzyme T4 lysozyme is presented. Molecular dynamics calculations were computed using the Discover software package (Biosym Technologies). All hydrogen atoms were modeled explicitly with the inclusion of all 152 crystallographic waters at a temperature of 300 K. The native T4 lysozyme molecular dynamics simulation demonstrated hinge-bending in the protein. Relative domain motions between the N-terminal and C-terminal domains were evident. The enzyme hinge bending sites resulted from small changes in backbone atom conformations over several residues rather than rotation about a single bound. Two hinge loci were found in the simulation. One locus comprises residues 8–14 near the C-terminal of the A helix; the other site, residues 77–83 near the C-terminal of the C helix. Comparison of several snapshot structures from the dynamics trajectory clearly illustrates domain motions between the two lysozyme lobes. Time correlated atomic motions in the protein were analyzed using a dynamical cross-correlation map. We found a high degree of correlated atomic motions in each of the domains and, to a lesser extent, anticorrelated motions between the two domains. We also found that the hairpin loop in the N-terminal lobe (residues 19–24) acted as a mobile ‘flap’ and exhibited highly correlated dynamic motions across the cleft of the active site, especially with residue 142.     

E. coli 5'-nucleotidase undergoes a hinge-bending domain rotation resembling a ball-and-socket motion

Structures of nine independent conformers of E. coli 5'-nucleotidase (5'-NT) have been analyzed using four different crystal forms. These data show that the two-domain protein undergoes an unusual 96 degrees hinge-bending domain rotation. Structures of the open and closed forms with substrates and inhibitors reveal that the substrate moves by approximately 25 A with the large domain rotation into the catalytic site. The domain motions derived from a comparison of the nine conformations agree well with motions obtained from a normal mode analysis in that all independent domain rotations are around axes that are roughly located in the plane which includes the domain centers and the hinge. Two residues, Lys355 and Gly356, form the core of the hinge region and undergo a large change of the main-chain torsion angles. The hinge-bending movement observed for 5'-nucleotidase differs markedly from a classical hinge-bending closure motion which involves an opening of the substrate or ligand-binding cleft between two domains. In contrast, the movement observed in 5'-nucleotidase resembles that of a ball-and-socket joint. The smaller C-terminal domain rotates approximately around its center such that the residues at the domain interface move in a sliding motion along the interface. Few direct interdomain contacts and a layer of water molecules between the two domains facilitate the sliding motion.     

Structural study of hinge bending in L-arabinose-binding protein

The L-arabinose-binding protein of Escherichia coli is a periplasmic component of the bacterial L-arabinose transport system. The three-dimensional structure of the molecule has been determined by x-ray diffraction and shown to have two globular domains and a connecting hinge. Theoretical study of the flexibility of the hinge using computer simulation showed that the hinge is quite permissive in that only moderate increases in the internal energy are required for opening the cleft where the L-arabinose-binding site is located. In this study, the structural changes that accompany the hinge bending are analyzed. The results show that bending-induced stresses are accommodated by coupled action of covalent and noncovalent forces within the protein molecule. Strains in internal coordinates (bond lengths, bond angles, and torsional angles) are distributed throughout the hinge region after structural relaxation. The pattern of structural changes within a hinge strand upon bending and relaxation depends in large degree on its geometric relationship with the bending axis (e.g. distance and orientation) and the atomic packing of its immediate environment. The distributed structural changes result in a characteristic zigzag pattern for the directional change at each residue in the hinge strands.     

Structure of a stabilizing disulfide bridge mutant that closes the active-site cleft of T4 lysozyme.

The engineered disulfide bridge between residues 21 and 142 of phage T4 lysozyme spans the active-site cleft and can be used as a switch to control the activity of the enzyme (Matsumura, M. & Matthews, B.W., 1989, Science 243, 792-794). In the oxidized form the disulfide increases the melting temperature of the protein by 11 degrees C at pH 2. The crystal structure of this mutant lysozyme has been determined in both the reduced and oxidized forms. In the reduced form, the crystal structure of the mutant is shown to be extremely similar to that of wild type. In the oxidized form, however, the formation of the disulfide bridge causes the alpha-carbons of Cys 21 and Cys 142, on opposite sides of the active-site cleft, to move toward each other by 2.5 A. In association with this movement, the amino-terminal domain of the protein undergoes a rigid-body rotation of 5.1 degrees relative to the carboxy-terminal domain. This rotation occurs about an axis passing through the junction of the amino-terminal and carboxy-terminal domains and is also close to the axis that best fits the apparent thermal motion of the amino-terminal domain seen previously in crystals of wild-type lysozyme. Even though the engineered Cys 21-Cys 142 disulfide links together the amino-terminal and carboxy-terminal domains of T4 lysozyme, it does not reduce the apparent mobility of the one domain relative to the other. The pronounced "hinge-bending" mobility of the amino-terminal domain that is suggested by the crystallographic thermal parameters of wild-type lysozyme persists in the oxidized (and reduced) mutant structures. In the immediate vicinity of the introduced disulfide bridge the mutant structure is more mobile (or disordered) than wild type, so much so that the exact conformation of Cys 21 remains obscure. As with the previously described disulfide bridge between residues 9 and 164 of T4 lysozyme (Pjura, P.E., Matsumura, M., Wozniak, J.A., & Matthews, B.W., 1990, Biochemistry 29, 2592-2598), the engineered cross-link substantially enhances the stability of the protein without making the folded structure more rigid.     

Model-free methods of analyzing domain motions in proteins from simulation: A comparison of normal mode analysis and molecular dynamics simulation of lysozyme

Model-free methods are introduced to determine quantities pertaining to protein domain motions from normal mode analyses and molecular dynamics simulations. For the normal mode analysis, the methods are based on the assumption that in low frequency modes, domain motions can be well approximated by modes of motion external to the domains. To analyze the molecular dynamics trajectory, a principal component analysis tailored specifically to analyze interdomain motions is applied. A method based on the curl of the atomic displacements is described, which yields a sharp discrimination of domains, and which defines a unique interdomain screw-axis. Hinge axes are defined and classified as twist or closure axes depending on their direction. The methods have been tested on lysozyme. A remarkable correspondence was found between the first normal mode axis and the first principal mode axis, with both axes passing within 3 Å of the alpha-carbon atoms of residues 2, 39, and 56 of human lysozyme, and near the interdomain helix. The axes of the first modes are overwhelmingly closure axes. A lesser degree of correspondence is found for the second modes, but in both cases they are more twist axes than closure axes. Both analyses reveal that the interdomain connections allow only these two degrees of freedom, one more than provided by a pure mechanical hinge. Proteins 27:425–437, 1997. © 1997 Wiley-Liss, Inc.     

Immunoglobulin structure exhibits control over CDR motion

Motions of the IgG structure are evaluated using normal mode analysis of an elastic network model to detect hinges, the dominance of low frequency modes, and the most important internal motions. One question we seek to answer is whether or not IgG hinge motions facilitate antigen binding. We also evaluate the protein crystal and packing effects on the experimental temperature factors and disorder predictions. We find that the effects of the protein environment on the crystallographic temperature factors may be misleading for evaluating specific functional motions of IgG. The extent of motion of the antigen binding domains is computed to show their large spatial sampling. We conclude that the IgG structure is specifically designed to facilitate large excursions of the antigen binding domains. Normal modes are shown as capable of computationally evaluating the hinge motions and the spatial sampling by the structure. The antigen binding loops and the major hinge appear to behave similarly to the rest of the structure when we consider the dominance of the low frequency modes and the extent of internal motion. The full IgG structure has a lower spectral dimension than individual F(ab) domains, pointing to more efficient information transfer through the antibody than through each domain. This supports the claim that the IgG structure is specifically constructed to facilitate antigen binding by coupling motion of the antigen binding loops with the large scale hinge motions.     

Domain motions and the open-to-closed conformational transition of an enzyme: a normal mode analysis of S-adenosyl-L-homocysteine hydrolase

The structure and fluctuations of the enzyme S-adenosyl-L-homocysteine hydrolase (SAHH) are analyzed in an effort to explain its biological function. Besides the previously identified open structure, characteristic of the substrate-free enzyme, we find two distinct structures in enzyme-inhibitor complexes, the closed and closed-twisted conformers. Both closed conformers differ from the open form by a hinge bending motion of two large domains within each subunit, which isolate the inhibitor bound in the active site from the bulk solvent. The closed-twisted form further differs from the closed form by a rigid body twist of the two-subunit dimers. The local structural fluctuations of SAHH are analyzed by performing block normal mode analysis of the tetrameric enzyme in its three forms. For the open form, we find that the four lowest-frequency normal modes, corresponding to the collective motions of the protein with the largest amplitudes, are essentially combinations of the hinge bending deformations of the individual subunits. Thus, the mechanical properties of the open structure of SAHH lead to the presence of structural fluctuations in the direction of the open-to-closed conformational transition. A candidate for such a motion has been observed in previous fluorescence depolarization studies of the enzyme. Both structural and normal mode analyses indicate that residues 180-190 and 350-356 form hinge regions, connecting large domains which tend to move as rigid bodies in response to interactions with substrate, intermediates, and the product of the enzymatic reactions. We propose that these hinge regions play a crucial role in the enzymatic mechanism of SAHH. In contrast to the open form, normal mode calculations for the closed conformations show strong coupling of the hinge bending motions of the individual subunits to each other and to other low-frequency vibrations. Thus, information about structural changes related to reaction progress in one active site may be mechanically transmitted to other subunits of the protein, explaining the cooperativity found in the enzyme kinetics.     

Crystallographic dissection of the thermal motion of protein-sugar complex

The crystal structure of turkey egg lysozyme (TEL) complexed with di-N-acetylchitobiose (NAG2) was refined at 1.19 A resolution by the full-matrix least-squares method with anisotropic temperature factors, and its thermal motion was evaluated by the TLS method. The average ESDs of atomic parameters of nonhydrogen atoms were 0.030 A for coordinates and 0.025 A(2) for anisotropic temperature factors. The active site cleft of TEL binds the alpha-anomer of NAG2 in a nonproductive binding mode with its pyranose rings parallel to a beta-sheet. The TEL structure was compared with the re-refined 1.12 A structure of native TEL. The RMS difference for equivalent Calpha atoms was 0.103 A and a relatively large difference was observed in the region of residues 104-125 rather than in the beta-sheet region where NAG2 was bound. In contrast, the temperature factor of the beta-sheet region was significantly decreased by the NAG2 binding. The TLS model that describes the rigid body motion in translation, libration, and screw motion was adopted for the evaluation of the molecular motion of TEL and NAG2, and the TLS parameters were determined by the least-squares fit to U(ij). The contribution of the external motion of TEL was estimated to be 55.8% of the observed temperature factor for the native structure and 45.9% for the NAG2 complex. The internal motion of TEL represented with atomic thermal ellipsoids was very similar between the native and complex structures except the NAG2 binding region. In the structure of NAG2, the rigid body motion dominates the thermal motion. The center of rotation of NAG2, 4.45A far from the center of gravity, is on the nitrogen atom of the acetylamino group that is hydrogen bonded to the main-chain peptide groups of Asn49 and Ala107. The rigid body motion of NAG2 indicates that the acetylamino group is most strongly bound to the active site, and the recognition of this group is a crucial step of the substrate binding.     

Projection of Monte Carlo and molecular dynamics trajectories onto the normal mode axes: human lysozyme

A method is presented to describe the internal motions of proteins obtained from molecular dynamics or Monte Carlo simulations as motions of normal mode variables. This method calculates normal mode variables by projecting trajectories of these simulations onto the axes of normal modes and expresses the trajectories as a linear combination of normal mode variables. This method is applied to the result of the molecular dynamics and the Monte Carlo simulations of human lysozyme. The motion of the lowest frequency mode extracted from the simulations represents the hinge bending motion very faithfully. Analysis of the obtained motions of the normal mode variables provides an explanation of the anharmonic aspects of protein dynamics as due first to the anharmonicity of the actual potential energy surface near a minimum and second to trans-minimum conformational changes.     

Molecular dynamics of the long neurotoxin LSIII

Long neurotoxins bind tightly and specifically to the nicotinic acetylcholine receptor (AChR) in postsynaptic membranes and are useful for exploring the biology of synapses. In crystallographic studies of long neurotoxins the principal binding loop appears disordered, but the NMR solution structure of the long neurotoxin LSIII revealed significant local order, even though the loop is disordered with respect to the globular core. A possible mechanism for conferring global disorder while preserving local order is rigid-body motion of the loop about a hinge region. Here we report investigations of LSIII dynamics based on (13)C(alpha) magnetic relaxation rates and molecular dynamics simulation. The relaxation rates and MD simulation both confirm the hypothesis of rigid-body motion of the loop and place bounds on the extent and time scale of the motion. The bending motion of the loop is slow compared to the rapid fluctuations of individual dihedral angles, reflecting the collective nature and largely entropic free energy profile for hinge bending. The dynamics of the central binding loop in LSIII illustrates two distinct mechanisms by which molecular dynamics directly impacts biological activity. The relative rigidity of key residues involved in recognition at the tip of the central binding loop lowers the otherwise substantial entropic cost of binding. Large excursions of the loop hinge angle may endow the protein with structural plasticity, allowing it to adapt to conformational changes induced in the receptor.     

Structure of bacteriophage T4 lysozyme refined at 1.7 A resolution

The structure of the lysozyme from bacteriophage T4 has been refined at 1.7 A resolution to a crystallographic residual of 19.3%. The final model has bond lengths and bond angles that differ from "ideal" values by 0.019 A and 2.7 degrees, respectively. The crystals are grown from electron-dense phosphate solutions and the use of an appropriate solvent continuum substantially improved the agreement between the observed and calculated structure factors at low resolution. Apart from changes in the conformations of some side-chains, the refinement confirms the structure of the molecule as initially derived from a 2.4 A resolution electron density map. There are 118 well-ordered solvent molecules that are associated with the T4 lysozyme molecule in the crystal. Four of these are more-or-less buried. There is a clustering of water molecules within the active site cleft but, other than this, the solvent molecules are dispersed around the surface of the molecule and do not aggregate into ice-like structures or pentagonal or hexagonal clusters. The apparent motion of T4 lysozyme in the crystal can be interpreted in terms of significant interdomain motion corresponding to an opening and closing of the active site cleft. For the amino-terminal domain the motion can be described equally well (correlation coefficients approx. 0.87) as quasi-rigid-body motion either about a point or about an axis of rotation. The motion in the crystals of the carboxy-terminal domain is best described as rotation about an axis (correlation coefficient 0.80) although in this case the apparent motion seems to be influenced in part by crystal contacts and may be of questionable relevance to dynamics in solution.     

Toward the mechanism of dynamical couplings and translocation in hepatitis C virus NS3 helicase using elastic network model

Hepatitis C virus NS3 helicase is an enzyme that unwinds double-stranded polynucleotides in an ATP-dependent reaction. It provides a promising target for small molecule therapeutic agents against hepatitis C. Design of such drugs requires a thorough understanding of the dynamical nature of the mechanochemical functioning of the helicase. Despite recent progress, the detailed mechanism of the coupling between ATPase activity and helicase activity remains unclear. Based on an elastic network model (ENM), we apply two computational analysis tools to probe the dynamical mechanism underlying the allosteric coupling between ATP binding and polynucleotide binding in this enzyme. The correlation analysis identifies a network of hot-spot residues that dynamically couple the ATP-binding site and the polynucleotide-binding site. Several of these key residues have been found by mutational experiments as functionally important, while our analysis also reveals previously unexplored hot-spot residues that are potential targets for future mutational studies. The conformational changes between different crystal structures of NS3 helicase are found to be dominated by the lowest frequency mode solved from the ENM. This mode corresponds to a hinge motion of the highly flexible domain 2. This motion simultaneously modulates the opening/closing of the domains 1-2 cleft where ATP binds, and the domains 2-3 cleft where the polynucleotide binds. Additionally, a small twisting motion of domain 1, observed in both mode 1 and the computed ATP binding induced conformational change, fine-tunes the binding affinity of the domains 1-3 interface for the polynucleotide. The combination of these motions facilitates the translocation of a single-stranded polynucleotide in an inchworm-like manner.     

Articulated external fixation of the ankle: minimizing motion resistance by accurate axis alignment

This study describes how an optimal single hinge axis position can be established for the application of articulated external fixation to the ankle joint. By deliberately introducing various amounts of relative mal-alignment between the optimal talocrural joint axis and the actual fixator hinge axis, it was possible to measure the corresponding amounts of additional resistance to joint motion. In a cadaveric study of six ankle specimens, we determined the instant axis of rotation of the talocrural joint from 3-D kinematic data. acquired by an electromagnetic motion tracking system. For each specimen, an optimal fixator hinge position was calculated from these motion data. Compared to the intact natural joint, aligning the fixator along the optimized axis position caused a moderate increase in energy (0.14 J) needed to rotate the ankle through a prescribed plantar/dorsiflexion range. However, malpositioning the hinge by 10 mm caused more than five times that amount of increase in motion resistance. While articulated external fixation with limited internal fixation can establish a favorable environment for the repair of severe injuries such as tibial pilon fractures, the large additional resistance to motion accompanying a malpositioned fixator axis suggests the development of untoward intra-articular forces that could act to disturb fragment alignment.     

Mechanics of channel gating of the nicotinic acetylcholine receptor

The nicotinic acetylcholine receptor (nAChR) is a key molecule involved in the propagation of signals in the central nervous system and peripheral synapses. Although numerous computational and experimental studies have been performed on this receptor, the structural dynamics of the receptor underlying the gating mechanism is still unclear. To address the mechanical fundamentals of nAChR gating, both conventional molecular dynamics (CMD) and steered rotation molecular dynamics (SRMD) simulations have been conducted on the cryo-electron microscopy (cryo-EM) structure of nAChR embedded in a dipalmitoylphosphatidylcholine (DPPC) bilayer and water molecules. A 30-ns CMD simulation revealed a collective motion amongst C-loops, M1, and M2 helices. The inward movement of C-loops accompanying the shrinking of acetylcholine (ACh) binding pockets induced an inward and upward motion of the outer β-sheet composed of β9 and β10 strands, which in turn causes M1 and M2 to undergo anticlockwise motions around the pore axis. Rotational motion of the entire receptor around the pore axis and twisting motions among extracellular (EC), transmembrane (TM), and intracellular MA domains were also detected by the CMD simulation. Moreover, M2 helices undergo a local twisting motion synthesized by their bending vibration and rotation. The hinge of either twisting motion or bending vibration is located at the middle of M2, possibly the gate of the receptor. A complementary twisting-to-open motion throughout the receptor was detected by a normal mode analysis (NMA). To mimic the pulsive action of ACh binding, nonequilibrium MD simulations were performed by using the SRMD method developed in one of our laboratories. The result confirmed all the motions derived from the CMD simulation and NMA. In addition, the SRMD simulation indicated that the channel may undergo an open-close (O ↔ C) motion. The present MD simulations explore the structural dynamics of the receptor under its gating process and provide a new insight into the gating mechanism of nAChR at the atomic level.     

Molecular mechanisms of chaperonin GroEL-GroES function.

The dynamics of the GroEL-GroES complex is investigated with a coarse-grained model. This model is one in which single-residue points are connected to other such points, which are nearby, by identical springs, forming a network of interactions. The nature of the most important (slowest) normal modes reveals a wide variety of motions uniquely dependent upon the central cavity of the structure, including opposed torsional rotation of the two GroEL rings accompanied by the alternating compression and expansion of the GroES cap binding region, bending, shear, opposed radial breathing of the cis and trans rings, and stretching and contraction along the protein assembly's long axis. The intermediate domains of the subunits are bifunctional due to the presence of two hinges, which are alternatively activated or frozen by an ATP-dependent mechanism. ATP binding stabilizes a relatively open conformation (with respect to the central cavity) and hinders the motion of the hinge site connecting the intermediate and equatorial domains, while enhancing the flexibility of the second hinge that sets in motion the apical domains. The relative flexibilities of the hinges are reversed in the nucleotide-free form. Cooperative cross-correlations between subunits provide information about the mechanism of action of the protein. The mechanical motions driven by the different modes provide variable binding surfaces and variable sized cavities in the interior to enable accommodation of a broad range of protein substrates. These modes of motion could be used to manipulate the substrate's conformations.     

Crystal structure combined with genetic analysis of the Thermus thermophilus ribosome recycling factor shows that a flexible hinge may act as a functional switch

Ribosome recycling factor (RRF), in concert with elongation factor EF-G, is required for disassembly of the posttermination complex of the ribosome after release of polypeptides. The crystal structure of Thermus thermophilus RRF was determined at 2.6 A resolution. It is a tRNA-like L-shaped molecule consisting of two domains: a long three-helix bundle (domain 1) and a three-layer beta/alpha/beta sandwich (domain 2). Although the individual domain structures are similar to those of Thermotoga maritima RRF (Selmer et al., Science, 1999, 286:2349-2352), the interdomain angle differs by 33 degrees in two molecules, suggesting that the hinge between two domains is potentially flexible and responsive to different conditions of crystal packing. The hinge connects hydrophobic junctions of domains 1 and 2. The structure-based genetic analysis revealed the strong correlation between the hinge flexibility and the in vivo function of RRF. First, altering the hinge flexibility by making alanine or serine substitutions for large-size residues conserved at the hinge loop and nearby in domain 1 frequently gave rise to gain of function except a Pro residue conserved at the hinge loop. Second, the hinge defect resulting from a too relaxed hinge structure can be compensated for by secondary alterations in domain 1 that seem to increase the hydrophobic contact between domain 1 and the hinge loop. These results show that the hinge flexibility is vital for the function of RRF and that the steric interaction between the hinge loop and domains 1 and 2 restricts the interdomain angle and/or the hinge flexibility. These results indicate that RRF possesses an architectural difference from tRNA regardless of a resemblance to tRNA shape: RRF has a "gooseneck" elbow, whereas the tRNA elbow is rigid, and the direction of flex of RRF and tRNA is at a nearly right angle to each other. Moreover, surface electrostatic potentials of the two RRF proteins are dissimilar and do not mimic the surface potential of tRNA or EF-G. These properties will add a new insight into RRF, suggesting that RRF is more than a simple tRNA mimic.     

Analysis of domain movements in glutamine-binding protein with simple models

In this work, the mechanism of domain movements of glutamine-binding protein (GlnBP), especially the influence of the ligand on GlnBP dynamic behavior is investigated with the aid of a Gaussian network model (GNM) and an anisotropy elastic network model. The results show that the "open-closed" transition mainly appears as the large movement of the small domain, especially the top region including two alpha-helices and two beta-strands. The slowest mode of each three forms of GlnBP--ligand-free open, ligand-bound closed, and ligand-free closed GlnBP--shows that the open-closed motion of the two domains has a common hinge axis centered on Lys-87 and Gln-183. Accompanying the conformational transition, the residues within both large and small domains move in a highly coupled way. The peaks of the fast modes correspond to residues that were thought, in the GNM, to be important for the stability of the protein, and these residues may be involved in the interactions with the membrane-bound components. With the contacts between the large domain and the small domain increasing, the ability of the "open-closed" motion is decreased. All the results agree well with those of molecular dynamics simulations, and it is thought that the open-closed conformation transition is the nature of the topology structure of GlnBP. Also, the influence of the ligand on GlnBP is studied with a modified GNM method. The results obtained show that the ligand does not influence the closed-to-open transition tendency.     

Treponema pallidum TroA is a periplasmic zinc-binding protein with a helical backbone.

The crystal structure of recombinant TroA, a zinc-binding protein component of an ATP-binding cassette transport system in Treponema pallidum, was determined at a resolution of 1.8 A. The organization of the protein is largely similar to other periplasmic ligand-binding proteins (PLBP), in that two independent globular domains interact with each other to create a zinc-binding cleft between them. The structure has one bound zinc pentavalently coordinated to residues from both domains. Unlike previous PLBP structures that have an interdomain hinge composed of beta-strands, the N- and C-domains of TroA are linked by a single long backbone helix. This unique backbone helical conformation was possibly adopted to limit the hinge motion associated with ligand exchange.