Pi7, an orphan peptide from the scorpion Pandinus imperator: a 1H-NMR analysis using a nano-NMR Probe

The three-dimensional solution structure of a novel peptide, Pi7, purified from the venom of the scorpion Pandinus imperator, and for which no specific receptor has been found yet, was determined by two-dimensional homonuclear proton NMR methods from a nanomole amount of compound using a nano-nmr probe. Pandinus imperator peptide 7 does not block voltage-dependent K(+)-channels and does not displace labeled noxiustoxin from rat brain synaptosomal membranes. The toxin has 38 amino acid residues and, similarly to Pi1, is stabilized by four disulfide bridges (Cys6-Cys27, Cys12-Cys32, Cys16-Cys34, and Cys22-Cys37). In addition, the lysine at position 26 crucial for potassium-channel blocking is replaced in Pi7 by an arginine. Tyrosine 34, equivalent to Tyr36 of ChTX is present, but the N-terminal positions 1 and 2 are occupied by two acidic residues Asp and Glu, respectively. The dihedral angles and distance restraints obtained from measured NMR parameters were used in structural calculations in order to determine the conformation of the peptide. The disulfide-bridge topology was established using distance restraints allowing ambiguous partners between S atoms combined with NMR-derived structural information. The structure is organized around a short alpha-helix spanning residues Thr9 to Thr20/Gly21 and a beta-sheet. These two elements of secondary structure are stabilized by two disulfide bridges, Cys12-Cys32 and Cys16-Cys34. The antiparallel beta-sheet is composed of two strands extending from Asn22 to Cys34 with a tight turn at Ile28-Asn29 in contact with the N-terminal fragment Ile4 to Cys6.     

NMR structure of the Euplotes raikovi pheromone Er-23 and identification of its five disulfide bonds.

The NMR solution structure of the 51 residue pheromone Er-23 from the ciliated protozoan Euplotes raikovi (Er) was calculated with the torsion angle dynamics program DYANA from 582 nuclear Overhauser enhancement (NOE) upper limit distance constraints, 46 dihedral angle constraints and 30 disulfide bond constraints. The disulfide bridges had not been assigned by chemical methods, and initially were assigned tentatively on the basis of inspection of the positioning of the Cys sulfhydryl groups in a bundle of 20 conformers that was calculated without disulfide bond constraints. The assignment of disulfide bridges was then validated by structure calculations that assessed the compatibility of plausible alternative Cys-Cys disulfide combinations with the input of NOE upper distance constraints and dihedral angle constraints. For a group of 20 conformers used to characterize the solution structure, the average pairwise root-mean-square distances from the mean coordinates calculated for the backbone heavy atoms N, C(alpha) and C' of resideus 1-51 is 0.38 A. The molecular architecture consists of a three-dimensional arrangement of five helices comprised of residues 2-8, 14-17, 26-29, 34-36 and 38-47, with five disulfide bridges in the positions 3-24, 6-16, 13-47, 27-40, and 35-51, which has so far not been represented in the Protein Data Bank. Er-23 is unique among presently known Er-pheromones with respect to size, sequence, the number of disulfide bonds and the three-dimensional structure, thus providing a new structural basis for rationalizing the physiological functions of this protein family.     

BTK-2, a new inhibitor of the Kv1.1 potassium channel purified from Indian scorpion Buthus tamulus

A novel inhibitor of voltage-gated potassium channel was isolated and purified to homogeneity from the venom of the red scorpion Buthus tamulus. The primary sequence of this toxin, named BTK-2, as determined by peptide sequencing shows that it has 32 amino acid residues with six conserved cysteines. The molecular weight of the toxin was found to be 3452 Da. It was found to block the human potassium channel hKv1.1 (IC(50)=4.6 microM). BTK-2 shows 40-70% sequence similarity to the family of the short-chain toxins that specifically block potassium channels. Multiple sequence alignment helps to categorize the toxin in the ninth subfamily of the K+ channel blockers. The modeled structure of BTK-2 shows an alpha/beta scaffold similar to those of the other short scorpion toxins. Comparative analysis of the structure with those of the other toxins helps to identify the possible structure-function relationship that leads to the difference in the specificity of BTK-2 from that of the other scorpion toxins. The toxin can also be used to study the assembly of the hKv1.1 channel.     

Determination of the spatial structure of insectotoxin 15A from Buthus erpeus by (1)H-NMR spectroscopy data]

The solution structure of insectotoxin 15A (35 residues) from scorpion Buthus eupeus was determined on the basis of 386 interproton distance restraints 12 hydrogen-bonding restraints and 113 dihedral angle restraints derived from 1H NMR experiments. A group of 20 structures was calculated with the distance geometry program DIANA followed by the restrained energy minimization with the program CHARMM. The atomic RMS distribution about the mean coordinate position is 0.64 +/- 0.11 A for the backbone atoms and 1.35 +/- 0.20 A for all atoms. The structure contains an alpha-helix (residues 10-20) and a three-stranded antiparallel beta-sheet (residues 2-5, 24-28 and 29-33). A pairing of the eight cysteine residues of insectotoxin 15A was established basing on NMR data. Three disulfide bridges (residues 2-19, 16-31 and 20-33) connect the alpha-helix with the beta-sheet, and the fourth one (5-26) joins beta-strands together. The spatial fold of secondary structure elements (the alpha-helix and the beta-sheet) of the insectotoxin 15A is very similar to those of the other short and long scorpion toxins in spite of a low (about 20%) sequence homology.     

Determination of three-dimensional solution structure of waglerin I,a toxin from Trimeresurus wagleri,using 2D-NMR and molecular dynamics simulation

The solution conformation of a synthetic snake venom toxin waglerin I, has been determined by using proton nuclear magnetic resonance spectroscopy. By y a combination of various two-dimensional NMR techniques, the ¹H-NMR spectrum of waglerin I was completely assigned. A set of 247 interproton distance restraints was derived from nuclear Overhauser enhancement (NOE) measurements. These NOE constraints, in addition to the 2 dihedral angle restraints (from coupling constant measurements) and 7 ω torsion angle restraints for prolines, formed the basis of three-dimensional structure determined by molecular dynamics techniques. The 19 structures that were obtained satisfy the experimental restraints, and display small deviation from idealized covalent geometry. Analysis of converged structures indicates that the toxin has no special secondary structure. In the solution structure of waglerin I, the central ring region is well defined but the N- and C-termini possesses more disorder.     

Solution structure of neuronal bungarotoxin determined by two-dimensional NMR spectroscopy: sequence-specific assignments, secondary structure, and dimer formation

The solution structure of neuronal bungarotoxin (nBgt) has been studied by using two-dimensional 1H NMR spectroscopy. Sequence-specific assignments for over 95% of the backbone resonances and 85% of the side-chain resonances have been made by using a series of two-dimensional spectra at four temperatures. From these assignments over 75% of the NOESY spectrum has been assigned, which has in turn provided 582 distance constraints. Twenty-seven coupling constants (NH-alpha CH) were determined from the COSY spectra, which have provided dihedral angle constraints. In addition, hydrogen exchange experiments have suggested the probable position of hydrogen bonds. The NOE constraints, dihedral angle constraints, and the rates of amide proton exchange suggest that a triple-stranded antiparallel beta sheet is the major component of secondary structure, which includes 25% of the amino acid residues. A number of NOE peaks were observed that were inconsistent with the antiparallel beta-sheet structure. Because we have confirmed by sedimentation equilibrium that nBgt exists as a dimer, we have reinterpreted these NOE constraints as intermolecular interactions. These constraints suggest that the dimer consists of a six-stranded antiparallel beta sheet (three from each monomer), with residues 55-59 forming the dimer interface.     

The Three-Dimensional NMR Solution Structure of α-Cobratoxin at pH 7.5 and Conformational Differences With the NMR Solution Structure at pH 3.2

Abstract The 3D solution structure of α-cobratoxin, a neurotoxin purified from the Naja naja siamensis snake venom, has been determined by Nuclear Magnetic Resonance spectroscopy, in conjunction with distance geometry and restrained molecular dynamics, at pH 7.5. A total of 490 distance restraints were obtained from NOE intensities and 25 φ dihedral angle restraints deduced from J- coupling data. The generated structures are well defined with root mean square deviations from a geometrical mean structure of 0.107 ± 0.036 nm for the backbone atoms and 0.128 ±0.073 nm for the side-chain atoms (considering residues 1 to 66 minus 26 to 35). A comparison between the generated structures at pH 7.5 and the mean NMR solution structure at pH 3.2 revealed that the 3D structure of α-cobratoxin is more compact at neutral pH. This major difference is mainly due to the pH-dependant conformational variations of three residues His(18), Thr(44) and Thr(59).     

Backbone structure of a small helical integral membrane protein: A unique structural characterization

The structural characterization of small integral membrane proteins pose a significant challenge for structural biology because of the multitude of molecular interactions between the protein and its heterogeneous environment. Here, the three‐dimensional backbone structure of Rv1761c from Mycobacterium tuberculosis has been characterized using solution NMR spectroscopy and dodecylphosphocholine (DPC) micelles as a membrane mimetic environment. This 127 residue single transmembrane helix protein has a significant (10 kDa) C‐terminal extramembranous domain. Five hundred and ninety distance, backbone dihedral, and orientational restraints were employed resulting in a 1.16 Å rmsd backbone structure with a transmembrane domain defined at 0.40 Å. The structure determination approach utilized residual dipolar coupling orientation data from partially aligned samples, long‐range paramagnetic relaxation enhancement derived distances, and dihedral restraints from chemical shift indices to determine the global fold. This structural model of Rv1761c displays some influences by the membrane mimetic illustrating that the structure of these membrane proteins is dictated by a combination of the amino acid sequence and the protein's environment. These results demonstrate both the efficacy of the structural approach and the necessity to consider the biophysical properties of membrane mimetics when interpreting structural data of integral membrane proteins and, in particular, small integral membrane proteins.     

Exploring structural features of the interaction between the scorpion toxinCnErg1 and ERG K+ channels

The gamma-KTx-type scorpion toxins specific for K+ channels were found to interact with ERG channels on the turret region, while alpha-KTx3.2 Agitoxin-2 binds to the pore region of the Shaker K+ channel, and alpha-KTx5.3 BmP05 binds to the intermediate region of the small-conductance calcium-activated K-channel (SK(Ca)). In order to explore the critical residues for gamma-KTx binding, we determined the NMR structure of native gamma-KTx1.1 (CnErg1), a 42 amino acid residues scorpion toxin isolated from the venom of the Mexican scorpion Centruro?des noxius Hoffmann, and we used computational evolutionary trace (ET) analysis to predict possible structural and functional features of interacting surfaces. The 1H-NMR three-dimensional solution structure of native ergtoxin (CnErg1) was solved using a total of 452 distance constraints, 13 3J(NH-Halpha) and 10 hydrogen bonds. The structure is characterized by 2 segments of alpha-helices and a triple-stranded antiparallel beta-sheet stabilized by 4 disulfide bridges. The ET and structural analysis provided indication of the presence of two important amino acid residue clusters, one hydrophobic and the other hydrophilic, that should be involved in the surface contact between the toxin and the channel. Some features of the proposed interacting surface are discussed.     

The high-precision solution structure of Yersinia modulating protein YmoA provides insight into interaction with H-NS

The high-resolution solution structure of Yersinia modulating protein YmoA is presented. The protein is all helical with the first three of four helices forming the central core. Structures calculated with only NOE and dihedral restraints exhibit a backbone root-mean-square deviation (rmsd) of 0.77 A. Upon refinement against Halpha-Calpha, HN-N, and Calpha-C' J-modulated residual dipolar couplings, the backbone rmsd improves to 0.22 A. YmoA has a high amino acid sequence identity to and a similar overall fold to Escherichia coli hemolysin expression modulating protein Hha; however, structural differences do occur. YmoA is also found to be structurally similar to the histone-like nucleoid structuring protein H-NS, indicating that YmoA may intercalate into higher-order H-NS suprastructuring by substituting for an H-NS dimer.     

Three-dimensional structure of the neurotoxin ATX Ia from Anemonia sulcata in aqueous solution determined by nuclear magnetic resonance spectroscopy

With the aid of 1H nuclear magnetic resonance (NMR) spectroscopy, the three-dimensional structure in aqueous solution was determined for ATX Ia, which is a 46 residue polypeptide neurotoxin of the sea anemone Anemonia sulcata. The input for the structure calculations consisted of 263 distance constraints from nuclear Overhauser effects (NOE) and 76 vicinal coupling constants. For the structure calculation several new or ammended programs were used in a revised strategy consisting of five successive computational steps. First, the program HABAS was used for a complete search of all backbone and chi 1 conformations that are compatible with the intraresidual and sequential NMR constraints. Second, using the program DISMAN, we extended this approach to pentapeptides by extensive sampling of all conformations that are consistent with the local and medium-range NMR constraints. Both steps resulted in the definition of additional dihedral angle constraints and in stereospecific assignments for a number of beta-methylene groups. In the next two steps DISMAN was used to obtain a group of eight conformers that contain no significant residual violations of the NMR constraints or van der Waals contacts. Finally, these structures were subjected to restrained energy refinement with a modified version of the molecular mechanics module of AMBER, which in addition to the energy force field includes potentials for the NOE distance constraints and the dihedral angle constraints. The average of the pairwise minimal RMS distances between the resulting refined conformers calculated for the well defined molecular core, which contains the backbone atoms of 35 residues and 20 interior side chains, is 1.5 +/- 0.3 A. This core is formed by a four-stranded beta-sheet connected by two well-defined loops, and there is an additional flexible loop consisting of the eleven residues 8-18. The core of the protein is stabilized by three disulfide bridges, which are surrounded by hydrophobic residues and shielded on one side by hydrophilic residues.     

Localized solution structure refinement of an F45W variant of ubiquitin using stochastic boundary molecular dynamics and NMR distance restraints.

The local structure within an 8-A radius around residue 45 of a recombinant F45W variant of human ubiquitin has been determined using 67 interproton distance restraints measured by two-dimensional proton NMR. Proton chemical shift evidence indicates that structural perturbations due to the F45W mutation are minimal and limited to the immediate vicinity of the site of mutation. Simulated annealing implemented with stochastic boundary molecular dynamics was applied to refine the structure of Trp 45 and 10 neighboring residues. The stochastic boundary method allowed the entire protein to be reassembled from the refined coordinates and the outlying unrefined coordinates with little distortion at the boundary. Refinement began with four low-energy indole ring orientations of F45W-substituted wild-type (WT) ubiquitin crystal coordinates. Distance restraints were derived from mostly long-range NOE cross peaks with 51 restraints involving the Trp 45 indole ring. Tandem refinements of 64 structures were done using either (1) upper and lower bounds derived from qualitative inspection of NOE crosspeak intensities or (2) quantitative analysis of cross-peak heights using the program MARDIGRAS. Though similar to those based on qualitative restraint, structures obtained using quantitative NOE analysis were superior in terms of precision and accuracy as measured by back-calculated sixth-root R factors. The six-membered portion of the indole ring is nearly coincident with the phenyl ring of the WT and the indole NH is exposed to solvent. Accommodation of the larger ring is accompanied by small perturbations in the backbone and a 120 degrees rotation of the chi 2 dihedral angle of Leu 50.     

Nuclear magnetic resonance solution structure of the alpha-neurotoxin from the black mamba (Dendroaspis polylepis polylepis).

The three-dimensional structure in solution of the alpha-neurotoxin from the black mamba (Dendroaspis polylepis polylepis) has been determined by nuclear magnetic resonance spectroscopy. A high quality structure for this 60-residue protein was obtained from 656 NOE distance constraints and 143 dihedral angle constraints, using the distance geometry program DIANA for the structure calculation and AMBER for restrained energy minimization. For a group of 20 conformers used to represent the solution structure, the average root-mean-square deviation value calculated for the polypeptide backbone heavy atoms relative to the mean structure was 0.45 A. The protein consists of a core region from which three finger-like loops extend outwards. It includes a short, two-stranded antiparallel beta-sheet of residues 1-5 and 13-17, a three-stranded antiparallel beta-sheet involving residues 23-31, 34-42 and 51-55, and four disulfide bridges in the core region. There is also extensive non-regular hydrogen bonding between the carboxy-terminal tail of the polypeptide chain and the rest of the core region. Comparison with the crystal structure of erabutoxin-b indicates that the structure of alpha-neurotoxin is quite similar to other neurotoxin structures, but that local structural differences are seen in regions thought to be important for binding of neurotoxins to the acetylcholine receptor. For two regions of the alpha-neurotoxin structure there is evidence for an equilibrium between multiple conformations, which might be related to conformational rearrangements upon binding to the receptor. Overall, the alpha-neurotoxin presents itself as a protein with a stable core and flexible surface areas that interact with the acetylcholine receptor in such a way that high affinity binding is achieved by conformational rearrangements of the deformable regions of the neurotoxin structure.     

Solution structure of an M-1 conotoxin with a novel disulfide linkage

The M-superfamily of conotoxins has a typical Cys framework (-CC-C-C-CC-), and is one of the eight major superfamilies found in the venom of the cone snail. Depending on the number of residues located in the last Cys loop (between Cys4 and Cys5), the M-superfamily family can be divided into four branches, namely M-1, -2, -3 and -4. Recently, two M-1 branch conotoxins (mr3e and tx3a) have been reported to possess a new disulfide bond arrangement between Cys1 and Cys5, Cys2 and Cys4, and Cys3 and Cys6, which is different from those seen in the M-2 and M-4 branches. Here we report the 3D structure of mr3e determined by 2D (1)H NMR in aqueous solution. Twenty converged structures of this peptide were obtained on the basis of 190 distance constraints obtained from NOE connectivities, as well as six varphi dihedral angle, three hydrogen bond, and three disulfide bond constraints. The rmsd values about the averaged coordinates of the backbone atoms were 0.43 +/- 0.19 A. Although mr3e has the same Cys arrangement as M-2 and M-4 conotoxins, it adopts a distinctive backbone conformation with the overall molecule resembling a 'flying bird'. Thus, different disulfide linkages may be employed by conotoxins with the same Cys framework to result in a more diversified backbone scaffold.     

A refined model for the solution structure of oxidized putidaredoxin

A refined model for the solution structure of oxidized putidaredoxin (Pdxo), a Cys4Fe2S2 ferredoxin, has been determined. A previous structure (Pochapsky et al. (1994) Biochemistry 33, 6424-6432; PDB entry ) was calculated using the results of homonuclear two-dimensional NMR experiments. New data has made it possible to calculate a refinement of the original Pdxo solution structure. First, essentially complete assignments for diamagnetic 15N and 13C resonances of Pdxo have been made using multidimensional NMR methods, and 15N- and 13C-resolved NOESY experiments have permitted the identification of many new NOE restraints for structural calculations. Stereospecific assignments for leucine and valine CH3 resonances were made using biosynthetically directed fractional 13C labeling, improving the precision of NOE restraints involving these residues. Backbone dihedral angle restraints have been obtained using a combination of two-dimensional J-modulated 15N,1H HSQC and 3D (HN)CO(CO)NH experiments. Second, the solution structure of a diamagnetic form of Pdx, that of the C85S variant of gallium putidaredoxin, in which a nonligand Cys is replaced by Ser, has been determined (Pochapsky et al. (1998) J. Biomol. NMR 12, 407-415), providing information concerning structural features not observable in the native ferredoxin due to paramagnetism. Third, a crystal structure of a closely related ferredoxin, bovine adrenodoxin, has been published (Müller et al. (1998) Structure 6, 269-280). This structure has been used to model the metal binding site structure in Pdx. A family of fourteen structures is presented that exhibits an rmsd of 0.51 A for backbone heavy atoms and 0.83 A for all heavy atoms. Exclusion of the modeled metal binding loop region reduces overall the rmsd to 0.30 A for backbone atoms and 0.71 A for all heavy atoms.     

Strategy for supplementing structure calculations using limited data with hydrophobic distance restraints

Introductory biochemistry texts often note that the fold of a protein is completely defined when the dihedral angles phi and psi are known for each amino acid. This assertion was examined with torsion angle dynamics and simulated annealing (TAD/SA) calculations of protein G using only dihedral angle restraints. When all dihedral angles were restrained to within 1 degrees of the values of the X-ray structure, the TAD/SA structures gave a backbone root mean square deviation to the target of 4 A. Factors that contributed to divergence from the correct solution include deviations of peptide bonds from planarity, internal conflicts resulting from the nonuniform energies of different phi, psi combinations, and relaxation to extended conformations in the absence of long-range constraints. Simulations including hydrogen-bond restraints showed that even a few long-range contacts constrain the fold better than a complete set of accurate dihedral restraints. A procedure is described for TAD/SA calculations using hydrogen-bond restraints, idealized dihedral restraints for residues in regular secondary structures, and "hydrophobic distance restraints" derived from the positions of hydrophobic residues in the amino acid sequence. The hydrogen-bond restraints are treated as inviolable, whereas violated hydrophobic restraints are removed following reduction of restraint upper bounds from 2 to 1 times the predicted radius of gyration. The strategy was tested with simulated restraints from X-ray structures of proteins from different fold classes and NMR data for cold shock protein A that included only backbone chemical shifts and hydrogen bonds obtained from a long-range HNCO experiment.     

Conotoxin TVIIA, a novel peptide from the venom of Conus tulipa 2. Three-dimensional solution structure.

The three-dimensional solution structure of conotoxin TVIIA, a 30-residue polypeptide from the venom of the piscivorous cone snail Conus tulipa, has been determined using 2D 1H NMR spectroscopy. TVIIA contains six cysteine residues which form a 'four-loop' structural framework common to many peptides from Conus venoms including the omega-, delta-, kappa-, and muO-conotoxins. However, TVIIA does not belong to these well-characterized pharmacological classes of conotoxins, but displays high sequence identity with conotoxin GS, a muscle sodium channel blocker from Conus geographus. Structure calculations were based on 562 interproton distance restraints inferred from NOE data, together with 18 backbone and nine side-chain torsion angle restraints derived from spin-spin coupling constants. The final family of 20 structures had mean pairwise rms differences over residues 2-27 of 0.18+/-0.05 A for the backbone atoms and 1.39+/-0.33 A for all heavy atoms. The structure consists of a triple-stranded, antiparallel beta sheet with +2x, -1 topology (residues 7-9, 16-20 and 23-27) and several beta turns. The core of the molecule is formed by three disulfide bonds which form a cystine knot motif common to many toxic and inhibitory polypeptides. The global fold, molecular shape and distribution of amino-acid sidechains in TVIIA is similar to that previously reported for conotoxin GS, and comparison with other four-loop conotoxin structures provides further indication that TVIIA and GS represent a new and distinct subgroup of this structural family. The structure of TVIIA determined in this study provides the basis for determining a structure-activity relationship for these molecules and their interaction with target receptors.     

Combined use of homo- and heteronuclear coupling constants as restraints in molecular dynamics simulations.

A penalty function for scalar coupling constants has been applied in molecular dynamics simulations as an experimental constraint. The function is based on the difference between the coupling constant calculated from the dihedral angle and the experimentally measured coupling constant. The method is illustrated on a model cyclic pentapeptide for which 3JHN-H alpha and 3JHN-C beta, both about the phi backbone dihedral angle, have been measured. The function is efficient in producing structures consistent with the scalar couplings, but removed from the conformation observed in solution. This arises from the lack of J restraints for the psi dihedral angle. Simulations with both nuclear Overhauser effect (NOE) and J-coupling restraints illustrates small but significant differences from simulations using only NOEs.     

Secondary structure and dynamics of an intrinsically unstructured linker domain

The transient secondary structure and dynamics of an intrinsically unstructured linker domain from the 70 kDa subunit of human replication protein A was investigated using solution state NMR. Stable secondary structure, inferred from large secondary chemical shifts, was observed for a segment of the intrinsically unstructured linker domain when it is attached to an N-terminal protein interaction domain. Results from NMR relaxation experiments showed the rotational diffusion for this segment of the intrinsically unstructured linker domain to be correlated with the N-terminal protein interaction domain. When the N-terminal domain is removed, the stable secondary structure is lost and faster rotational diffusion is observed. The large secondary chemical shifts were used to calculate phi and psi dihedral angles and these dihedral angles were used to build a backbone structural model. Restrained molecular dynamics were performed on this new structure using the chemical shift based dihedral angles and a single NOE distance as restraints. In the resulting family of structures a large, solvent exposed loop was observed for the segment of the intrinsically unstructured linker domain that had large secondary chemical shifts.     

NMR solution structure and receptor peptide binding of the CC chemokine eotaxin-2

The human CC chemokine eotaxin-2 is a specific agonist for the chemokine receptor CCR3 and may play a role in the recruitment of eosinophils in allergic diseases and parasitic infections. We report the solution structure of eotaxin-2 determined using heteronuclear and triple resonance NMR methods. A family of 20 structures was calculated by hybrid distance geometry-simulated annealing from 854 NOE distance restraints, 48 dihedral angle restraints, and 12 hydrogen bond restraints. The structure of eotaxin-2 (73 amino acid residues) consists of a helical turn (residues 17-20) followed by a 3-stranded antiparallel beta-sheet (residues 22-26, 37-41, and 44-49) and an alpha-helix (residues 54-66). The N-loop (residues 9-16) is packed against both the sheet and the helix with the two conserved disulfide bonds tethering the N-terminal/N-loop region to the beta-sheet. The average backbone and heavy atom rmsd values of the 20 structures (residues 7-66) are 0.52 and 1.13 A, respectively. A linear peptide corresponding to the N-terminal region of CCR3 binds to eotaxin-2, inducing concentration-dependent chemical shift changes or line broadening of many residues. The distribution of these residues suggests that the peptide binds into an extended groove located at the interface between the N-loop and the beta2-beta3 hairpin. The receptor peptide may also interact with the N-terminus of the chemokine and part of the alpha-helix. Comparison of the eotaxin-2 structure with those of related chemokines indicates several structural features that may contribute to receptor specificity.