Environment-dependent long-range structural distortion in a temperature-sensitive point mutant

Extensive environment-dependent rearrangement of the helix-turn-helix DNA recognition region and adjacent L-tryptophan binding pocket is reported in the crystal structure of dimeric E. coli trp aporepressor with point mutation Leu75Phe. In one of two subunits, the eight residues immediately C-terminal to the mutation are shifted forward in helical register by three positions, and the five following residues form an extrahelical loop accommodating the register shift. In contrast, the second subunit has wildtype-like conformation, as do both subunits in an isomorphous wildtype control structure. Treated together as an ensemble pair, the distorted and wildtype-like conformations of the mutant apoprotein agree more fully than either conformation alone with previously reported NOE measurements, and account more completely for its diverse biochemical and biophysical properties. The register-shifted segment Ile79-Ala80-Thr81-Ile82-Thr83 is helical in both conformations despite low helical propensity, suggesting an important structural role for the steric constraints imposed by β-branched residues in helical conformation.     

Temperature‐induced partially unfolded state of hUBF HMG Box‐5: Conformational and dynamic investigations of the Box‐5 thermal intermediate ensemble

Human upstream binding factor (hUBF) HMG Box‐5 is a highly conserved protein domain, containing 84 amino acids and belonging to the family of the nonspecific DNA‐binding HMG boxes. Its native structure adopts a twisted L shape, which consists of three α‐helices and two hydrophobic cores: the major wing and the minor wing. In this article, we report a reversible three‐state thermal unfolding equilibrium of hUBF HMG Box‐5, which is investigated by differential scanning calorimetry (DSC), circular dichroism spectroscopy, fluorescence spectroscopy, and NMR spectroscopy. DSC data show that Box‐5 unfolds reversibly in two separate stages. Spectroscopic analyses suggest that different structural elements exhibit noncooperative transitions during the unfolding process and that the major form of the Box‐5 thermal intermediate ensemble at 55°C shows partially unfolded characteristics. Compared with previous thermal stability studies of other boxes, it appears that Box‐5 possesses a more stable major wing and two well separated subdomains. NMR chemical shift index and sequential ¹H^N_i‐¹H^N_i+1 NOE analyses indicate that helices 1 and 2 are native‐like in the thermal intermediate ensemble, while helix 3 is partially unfolded. Detailed NMR relaxation dynamics are compared between the native state and the intermediate ensemble. Our results implicate a fluid helix‐turn‐helix folding model of Box‐5, where helices 1 and 2 potentially form the helix 1‐turn‐helix 2 motif in the intermediate, while helix 3 is consolidated only as two hydrophobic cores form to stabilize the native structure. Proteins 2009. © 2009 Wiley‐Liss, Inc.     

Exploring the dynamic information content of a protein NMR structure: Comparison of a molecular dynamics simulation with the NMR and X‐ray structures of Escherichia coli ribonuclease HI

The multiconformer nature of solution nuclear magnetic resonance (NMR) structures of proteins results from the effects of intramolecular dynamics, spin diffusion and an uneven distribution of structural restraints throughout the molecule. A delineation of the former from the latter two contributions is attempted in this work for an ensemble of 15 NMR structures of the protein Escherichia coli ribonuclease HI (RNase HI). Exploration of the dynamic information content of the NMR ensemble is carried out through correlation with data from two crystal structures and a 1.7‐ns molecular dynamics (MD) trajectory of RNase HI in explicit solvent. Assessment of the consistency of the crystal and mean MD structures with nuclear Overhauser effect (NOE) data showed that the NMR ensemble is overall more compatible with the high‐resolution (1.48 Å) crystal structure than with either the lower‐resolution (2.05 Å) crystal structure or the MD simulation. Furthermore, the NMR ensemble is found to span more conformational space than the MD simulation for both the backbone and the sidechains of RNase HI. Nonetheless, the backbone conformational variability of both the NMR ensemble and the simulation is especially consistent with NMR relaxation measurements of two loop regions that are putative sites of substrate recognition. Plausible side‐chain dynamic information is extracted from the NMR ensemble on the basis of (i) rotamericity and syn‐pentane character of variable torsion angles, (ii) comparison of the magnitude of atomic mean‐square fluctuations (msf) with those deduced from crystallographic thermal factors, and (iii) comparison of torsion angle conformational behavior in the NMR ensemble and the simulation. Several heterogeneous torsion angles, while adopting non‐rotameric/syn‐pentane conformations in the NMR ensemble, exist in a unique conformation in the simulation and display low X‐ray thermal factors. These torsions are identified as sites whose variability is likely to be an artifact of the NMR structure determination procedure. A number of other torsions show a close correspondence between the conformations sampled in the NMR and MD ensembles, as well as significant correlations among crystallographic thermal factors and atomic msf calculated from the NMR ensemble and the simulation. These results indicate that a significant amount of dynamic information is contained in the NMR ensemble. The relevance of the present findings for the biological function of RNase HI, protein recognition studies, and previous investigations of the motional content of protein NMR structures are discussed. Proteins 1999;36:87–110. © 1999 Wiley‐Liss, Inc.     

Conformation of the Ras-binding domain of Raf studied by molecular dynamics and free energy simulations

Recognition of Ras by its downstream target Raf is mediated by a Ras-recognition region in the Ras-binding domain (RBD) of Raf. Residues 78–89 in this region occupy two different conformations in the ensemble of NMR solution structures of the RBD: a fully α-helical one, and one where 87–90 form a type IV β-turn. Molecular dynamics simulations of the RBD in solution were performed to explore the stability of these and other possible conformations of both the wild-type RBD and the R89K mutant, which does not bind Ras. The simulations sample a fully helical conformation for residues 78–89 similar to the NMR helical structures, a conformation where 85–89 form a 3₁₀-helical turn, and a conformation where 87–90 form a type I |iB-turn, whose free energies are all within 0.3 kcal/mol of each other. NOE patterns and H^α chemical shifts from the simulations are in reasonable agreement with experiment. The NMR turn structure is calculated to be 3 kcal/mol higher than the three above conformations. In a simulation with the same implicit solvent model used in the NMR structure generation, the turn conformation relaxes into the fully helical conformation, illustrating possible structural artifacts introduced by the implicit solvent model. With the Raf R89K mutant, simulations sample a fully helical and a turn conformation, the turn being 0.9 kcal/mol more stable. Thus, the mutation affects the population of RBD conformations, and this is expected to affect Ras binding. For example, if the fully helical conformation of residues 78–89 is required for binding, its free energy increase in R89K will increase the binding free energy by about 0.6 kcal/mol. Proteins 31:186–200, 1998. © 1998 Wiley-Liss, Inc.     

Conformational preferences of a short Aib/Ala‐based water‐soluble peptide as a function of temperature

The amino acid Aib predisposes a peptide to be helical with context‐dependent preference for either 3₁₀‐ or α‐ or a mixed helical conformation. Short peptides also show an inherent tendency to be unfolded. To characterize helical and unfolded states adopted by water‐soluble Aib‐containing peptides, the conformational preference of Ac‐Ala‐Aib‐Ala‐Lys‐Ala‐Aib‐Lys‐Ala‐Lys‐Ala‐Aib‐Tyr‐NH₂ was determined by CD, NMR and MD simulations as a function of temperature. Temperature‐dependent CD data indicated the contribution of two major components, each an admixture of helical and extended/polyproline II structures. Both right‐ and left‐handed helical conformations were detected from deconvolution of CD data and ¹³C NMR experiments. The presence of a helical backbone, more pronounced at the N‐terminal, and a temperature‐induced shift in α‐helix/3₁₀‐helix equilibrium, more pronounced at the C‐terminal, emerged from NMR data. Starting from polyproline II, the N‐terminal of the peptide folded into a helical backbone in MD simulations within 5 ns at 60°C. Longer simulations showed a mixed‐helical backbone to be stable over the entire peptide at 5°C while at 60°C the mixed‐helix was either stable at the N‐terminus or occurred in short stretches through out the peptide, along with a significant population of polyproline II. Our results point towards conformational heterogeneity of water‐soluble Aib‐based peptide helices and the associated subtleties. The problem of analyzing CD and NMR data of both left‐ and right‐handed helices are discussed, especially the validity of the ellipticity ratio [θ]₂₂₂/[θ]₂₀₇, as a reporter of α‐/3₁₀‐ population ratio, in right‐ and left‐handed helical mixtures. Proteins 2009. © 2008 Wiley‐Liss, Inc.     

Exploring the free energy landscape of a model β‐hairpin peptide and its isoform

Secondary structural transitions from α‐helix to β‐sheet conformations are observed in several misfolding diseases including Alzheimer's and Parkinson's. Determining factors contributing favorably to the formation of each of these secondary structures is therefore essential to better understand these disease states. β‐hairpin peptides form basic components of anti‐parallel β‐sheets and are suitable model systems for characterizing the fundamental forces stabilizing β‐sheets in fibrillar structures. In this study, we explore the free energy landscape of the model β‐hairpin peptide GB1 and its E2 isoform that preferentially adopts α‐helical conformations at ambient conditions. Umbrella sampling simulations using all‐atom models and explicit solvent are performed over a large range of end‐to‐end distances. Our results show the strong preference of GB1 and the E2 isoform for β‐hairpin and α‐helical conformations, respectively, consistent with previous studies. We show that the unfolded states of GB1 are largely populated by misfolded β‐hairpin structures which differ from each other in the position of the β‐turn. We discuss the energetic factors contributing favorably to the formation of α‐helix and β‐hairpin conformations in these peptides and highlight the energetic role of hydrogen bonds and non‐bonded interactions. Proteins 2014; 82:2394–2402. © 2014 Wiley Periodicals, Inc.     

Sequence-specific NMR assignments of the trp repressor from Escherichia coli using three-dimensional 15N/1H heteronuclear techniques.

Sequence-specific 15N and 1H assignments for the trp holorepressor from Escherichia coli are reported. The trp repressor consists of two identical 107-residue subunits which are highly helical in the crystal state [Schevitz, R., Otwinowski, Z., Joachimiak, A., Lawson, C. L. & Sigler, P. B. (1985) Nature 317, 782-786]. The high helical content and the relatively large size of the protein (Mr = 25,000) make it difficult to assign even the main-chain resonances by conventional homonuclear two-dimensional NMR methods. However, we have now assigned the main-chain resonances of 94% of the residues by using three-dimensional 15N/1H heteronuclear experiments on a sample of protein uniformly labelled with 15N. The additional resolution obtained by spreading out the signals into three dimensions proved indispensable in making these assignments. In particular, we have been able to resolve signals from residues in the N-terminal region of the A helix for the first time in solution. The observed NOE results confirm that the repressor is highly helical in solution, and contains no extended chain conformations.     

Flexibility of the DNA-binding domains of trp repressor

An orthorhombic crystal form of trp repressor (aporepressor plus L-tryptophan ligand) was solved by molecular replacement, refined to 1.65 A resolution, and compared to the structure of the repressor in trigonal crystals. Even though these two crystal forms of repressor were grown under identical conditions, the refined structures have distinctly different conformations of the DNA-binding domains. Unlike the repressor/aporepressor structural transition, the conformational shift is not caused by the binding or loss of the L-tryptophan ligand. We conclude that while L-tryptophan binding is essential for forming a specific complex with trp operator DNA, the corepressor ligand does not lock the repressor into a single conformation that is complementary to the operator. This flexibility may be required by the various binding modes proposed for trp repressor in its search for and adherence to its three different operator sites.     

Molecular dynamics simulations of a highly charged peptide from an SH3 domain: possible sequence-function relationship

A seven-residue peptide that is highly conserved in SH3 domains despite being far from the active site has been shown by NMR to be stable in solution. This peptide, biologically important because it is a likely folding nucleus for SH3 domains, provides a challenging subject for molecular dynamics because it is highly charged. We present stable, 10-ns simulations of both the native-like diverging turn structure and a helical model. Free energies of these two conformations, estimated through MM-PBSA analysis using several force fields, suggest a comparable free energy (DeltaDeltaG < or =6 kcal/mol) for native and helix conformations. NOE intensities calculated from the native trajectory reproduce experimental data quite well, suggesting that the conformations sampled by the trajectory reasonably represent those observed in the NMR experiment. The molecular dynamics results, as well as sequence analysis of a diverse 690-member family of SH3 domain proteins, suggest that the presence of two elements is essential for formation of the diverging turn structure: a pair of residues with low helical propensity in the turn region and, as previously recognized, two hydrophobic residues to close the end of the diverging turn. Thus, these two sequence features may form the structural basis for the function of this peptide as a folding nucleus in this family of proteins.     

Structural characterization of a neurotoxic threonine‐rich peptide corresponding to the human prion protein α2‐helical 180–195 segment,and comparison with full‐length α2‐helix‐derived peptides

The 173–195 segment corresponding to the helix 2 of the globular PrP domain is a good candidate to be one of the several ‘spots’ of intrinsic structural flexibility, which might induce local destabilization and concur to protein transformation, leading to aggregation‐prone conformations. Here, we report CD and NMR studies on the α2‐helix‐derived peptide of maximal length (hPrP[180–195]) that is able to exhibit a regular structure different from the prevalently random arrangement of other α2‐helix‐derived peptides. This peptide, which has previously been shown to be affected by buffer composition via the ion charge density dependence typical of Hofmeister effects, corresponds to the C‐terminal sequence of the PrP^C full‐length α2‐helix and includes the highly conserved threonine‐rich 188–195 segment. At neutral pH, its conformation is dominated by β‐type contributions, which only very strong environmental modifications are able to modify. On TFE addition, an increase of α‐helical content can be observed, but a fully helical conformation is only obtained in neat TFE. However, linking of the 173–179 segment, as occurring in wild‐type and mutant peptides corresponding to the full‐length α2‐helix, perturbs these intrinsic structural propensities in a manner that depends on whether the environment is water or TFE. Overall, these results confirm that the 180–195 parental region in hPrP^C makes a strong contribution to the chameleon conformational behavior of the segment corresponding to the full‐length α2‐helix, and could play a role in determining structural rearrangements of the entire globular domain. Copyright © 2008 European Peptide Society and John Wiley & Sons, Ltd.     

The solution structures of Escherichia coli trp repressor and trp aporepressor at an intermediate resolution

We have determined the solution structures and examined the dynamics of the Escherichia coli trp repressor (a 25-kDa dimer), with and without the co-repressor L-tryptophan, from NMR data. This is the largest protein structure thus far determined by NMR. To obtain a set of data sufficient for a structure determination it was essential to resort to isotopic spectral editing. Line broadening observed in this molecular mass range precludes for the most part the measurement of coupling constants and stereospecific assignments, with the inevitable result that the attainable resolution of the final structure will be somewhat lower than the resolution reported for smaller proteins and peptides. Nevertheless the general topology of the protein can be deduced from the subsets of NOEs defining the secondary and tertiary structure, providing a basis for further refinement using the full set of NOEs and energy minimization. We report here (a) an intermediate resolution structure that can be deduced from NMR data, covalent, angular and van-der-Waals constraints only, without resort to detailed energy calculations, and (b) the limits of uncertainty within which this structure is valid. An examination of these structures combined with backbone amide exchange data shows that even at this resolution three important conclusions can be drawn: (a) the protein structure changes upon binding tryptophan; (b) the putative DNA binding region is much more flexible than the core of the molecule, with backbone amide proton exchange rates 1000 times faster than in the core; (c) the binding of tryptophan stabilizes the repressor molecule, which is reflected in both the appearance of additional NOEs, and in the slowing of backbone proton exchange rates by factors of 3-10. Sequence-specific 1H-NMR assignments and the secondary structure of the holopressor (L-tryptophan-bound form) have been reported previously [C. H. Arrowsmith, R. Pachter, R. B. Altman, S. B. Iyer & O. Jardetzky (1990) Biochemistry 29, 6332-6341]. Those for the trp aporepressor (L-tryptophan-free form), made using the same methods and conditions as described in the cited paper, are reported here. The secondary structure of the aporepressor was calculated from sequential and medium-range NOEs and is the same as reported for the holorepressor except that helix E is shorter. The tertiary solution structures for both forms of the repressor were calculated from long-range NOE data.(ABSTRACT TRUNCATED AT 400 WORDS)     

Identification of initiation sites for T4 lysozyme folding using CD and NMR spectroscopy of peptide fragments

Using CD and 2D (1)H NMR spectroscopy, we have identified potential initiation sites for the folding of T4 lysozyme by examining the conformational preferences of peptide fragments corresponding to regions of secondary structure. CD spectropolarimetry showed most peptides were unstructured in water, but adopted partial helical conformations in TFE and SDS solution. This was also consistent with the (1)H NMR data which showed that the peptides were predominantly disordered in water, although in some cases, nascent or small populations of partially folded conformations could be detected. NOE patterns, coupling constants, and deviations from random coil Halpha chemical shift values complemented the CD data and confirmed that many of the peptides were helical in TFE and SDS micelles. In particular, the peptide corresponding to helix E in the native enzyme formed a well-defined helix in both TFE and SDS, indicating that helix E potentially forms an initiation site for T4 lysozyme folding. The data for the other peptides indicated that helices D, F, G, and H are dependent on tertiary interactions for their folding and/or stability. Overall, the results from this study, and those of our earlier studies, are in agreement with modeling and HD-deuterium exchange experiments, and support an hierarchical model of folding for T4 lysozyme.     

Bihelix: Towards de novo structure prediction of an ensemble of G‐protein coupled receptor conformations

G‐Protein Coupled Receptors (GPCRs) play a critical role in cellular signal transduction pathways and are prominent therapeutic targets. Recently there has been major progress in obtaining experimental structures for a few GPCRs. Each GPCR, however, exhibits multiple conformations that play a role in their function and we have been developing methods aimed at predicting structures for all these conformations. Analysis of available structures shows that these conformations differ in relative helix tilts and rotations. The essential issue is, determining how to orient each of the seven helices about its axis since this determines how it interacts with the other six helices. Considering all possible helix rotations to ensure that no important packings are overlooked, and using rotation angle increments of 30° about the helical axis would still lead to 12⁷ or 35 million possible conformations each with optimal residue positions. We show in this paper how to accomplish this. The fundamental idea is to optimize the interactions between each pair of contacting helices while ignoring the other 5 and then to estimate the energies of all 35 million combinations using these pair‐wise interactions. This BiHelix approach dramatically reduces the effort to examine the complete set of conformations and correctly identifies the crystal packing for the experimental structures plus other near‐native packings we believe may play an important role in activation. This approach also enables a detailed structural analysis of functionally distinct conformations using helix‐helix interaction energy landscapes and should be useful for other helical transmembrane proteins as well. Proteins 2012. © 2011 Wiley Periodicals, Inc.     

Insight into a Random Coil Conformation and an Isolated Helix: Structural and Dynamical Characterisation of the C-Helix Peptide from Hen Lysozyme

A 17 residue peptide corresponding to the C-helix of hen lysozyme (residues 86 to 102) has been investigated in detail to assess the factors that determine its conformation in both aqueous and trifluoroethanol (TFE) solutions. A thorough characterisation of the peptide by CD and NMR techniques under both conditions has been performed including the determination of complete NMR proton sequential assignments, and measurement of NOE effects,³J_HNαcoupling constants, temperature coefficients and residue-specific hydrogen-exchange rates. In water, the peptide adopts a largely unstructured conformation and NMR data, particularly coupling constants and chemical shift deviations, have been shown to agree closely with predictions from a model for a random coil based on the φ,ψ distributions in a protein database. This indicates that under these conditions the intrinsic conformational preferences of the individual amino acid residues are the dominating factors that determine the population of conformers adopted. With increasing concentrations of TFE a cooperative transition to an extensively helical conformation occurs and the resultant changes in CαH chemical shifts have been shown to correlate with the changes in φ,ψ populations. Using NOE and coupling constant data for this state, an ensemble of structures has been calculated and provides a model for a helix in the absence of tertiary interactions. In this model fluctuations, which increase in amplitude towards the termini, occur about the average helical φ,ψ angles and are responsible for increasing the values of³J_HNαcoupling constants above those anticipated for a static helix. The residue-specific rates of hydrogen exchange for the peptide in 50% TFE-d₃are consistent with such a model, the maximum protection from exchange being observed for residues in the centre of the helix.     

Conformation of membrane‐bound proteins revealed by vacuum‐ultraviolet circular‐dichroism and linear‐dichroism spectroscopy

Knowledge of the conformations of a water‐soluble protein bound to a membrane is important for understanding the membrane‐interaction mechanisms and the membrane‐mediated functions of the protein. In this study we applied vacuum‐ultraviolet circular‐dichroism (VUVCD) and linear‐dichroism (LD) spectroscopy to analyze the conformations of α‐lactalbumin (LA), thioredoxin (Trx), and β‐lactoglobulin (LG) bound to phosphatidylglycerol liposomes. The VUVCD analysis coupled with a neural‐network analysis showed that these three proteins have characteristic helix‐rich conformations involving several helical segments, of which two amphiphilic or hydrophobic segments take part in interactions with the liposome. The LD analysis predicted the average orientations of these helix segments on the liposome: two amphiphilic helices parallel to the liposome surface for LA, two hydrophobic helices perpendicular to the liposome surface for Trx, and a hydrophobic helix perpendicular to and an amphiphilic helix parallel to the liposome surface for LG. This sequence‐level information about the secondary structures and orientations was used to formulate interaction models of the three proteins at the membrane surface. This study demonstrates the validity of a combination of VUVCD and LD spectroscopy in conformational analyses of membrane‐binding proteins, which are difficult targets for X‐ray crystallography and nuclear magnetic resonance spectroscopy. Proteins 2016; 84:349–359. © 2016 Wiley Periodicals, Inc.     

Systematic evaluation of CS‐Rosetta for membrane protein structure prediction with sparse NOE restraints

We critically test and validate the CS‐Rosetta methodology for de novo structure prediction of ‐helical membrane proteins (MPs) from NMR data, such as chemical shifts and NOE distance restraints. By systematically reducing the number and types of NOE restraints, we focus on determining the regime in which MP structures can be reliably predicted and pinpoint the boundaries of the approach. Five MPs of known structure were used as test systems, phototaxis sensory rhodopsin II (pSRII), a subdomain of pSRII, disulfide binding protein B (DsbB), microsomal prostaglandin E2 synthase‐1 (mPGES‐1), and translocator protein (TSPO). For pSRII and DsbB, where NMR and X‐ray structures are available, resolution‐adapted structural recombination (RASREC) CS‐Rosetta yields structures that are as close to the X‐ray structure as the published NMR structures if all available NMR data are used to guide structure prediction. For mPGES‐1 and Bacillus cereus TSPO, where only X‐ray crystal structures are available, highly accurate structures are obtained using simulated NMR data. One main advantage of RASREC CS‐Rosetta is its robustness with respect to even a drastic reduction of the number of NOEs. Close‐to‐native structures were obtained with one randomly picked long‐range NOEs for every 14, 31, 38, and 8 residues for full‐length pSRII, the pSRII subdomain, TSPO, and DsbB, respectively, in addition to using chemical shifts. For mPGES‐1, atomically accurate structures could be predicted even from chemical shifts alone. Our results show that atomic level accuracy for helical membrane proteins is achievable with CS‐Rosetta using very sparse NOE restraint sets to guide structure prediction. Proteins 2017; 85:812–826. © 2016 Wiley Periodicals, Inc.     

Folding of immunogenic peptide fragments of proteins in water solution. II. The nascent helix

1H nuclear magnetic resonance experiments indicate formation of secondary structures in water solutions of a synthetic immunogenic peptide of sequence EVVPHKKMHKDFLEKIGGL corresponding to the C-helix (residues 69 to 87) of myohemerythrin. The conformational ensemble consists of a set of turn-like structures, distributed over the C-terminal half of the peptide and rapidly interconverting by way of unfolded states. These structures, termed nascent helix, are stabilized into helical structure with long-range order in water/trifluorethanol mixtures. Circular dichroism measurements confirm the presence of 50% helix in water/trifluoroethanol but show no evidence of helicity in water solutions of the peptide. It is apparent that no one member of the transient set of helical conformations which constitutes the nascent helix is sufficiently long to be detectable by circular dichroism experiments. No preferred conformations could be detected by nuclear magnetic resonance in the N-terminal half of the peptide, either in water or water/trifluoroethanol mixtures. This region of the peptide is stabilized in helix by long-range interactions in the folded protein. The possible role of nascent secondary structure in induction of antipeptide antibodies and in initiation of protein folding is discussed.     

Monomeric structure of the cardioprotective chemokine SDF‐1/CXCL12

The chemokine stromal cell‐derived factor‐1 (SDF‐1/CXCL12) directs leukocyte migration, stem cell homing, and cancer metastasis through activation of CXCR4, which is also a coreceptor for T‐tropic HIV‐1. Recently, SDF‐1 was shown to play a protective role after myocardial infarction, and the protein is a candidate for development of new anti‐ischemic compounds. SDF‐1 is monomeric at nanomolar concentrations but binding partners promote self‐association at higher concentrations to form a typical CXC chemokine homodimer. Two NMR structures have been reported for the SDF‐1 monomer, but only one matches the conformation observed in a series of dimeric crystal structures. In the other model, the C‐terminal helix is tilted at an angle incompatible with SDF‐1 dimerization. Using a rat heart explant model for ischemia/reperfusion injury, we found that dimeric SDF‐1 exerts no cardioprotective effect, suggesting that the active species is monomeric. To resolve the discrepancy between existing models, we solved the NMR structure of the SDF‐1 monomer in different solution conditions. Irrespective of pH and buffer composition, the C‐terminal helix remains tilted at an angle with no evidence for the perpendicular arrangement. Furthermore, we find that phospholipid bicelles promote dimerization that necessarily shifts the helix to the perpendicular orientation, yielding dipolar couplings that are incompatible with the NOE distance constraints. We conclude that interactions with the alignment medium biased the previous structure, masking flexibility in the helix position that may be essential for the distinct functional properties of the SDF‐1 monomer.     

Interaction of the Escherichia coli trp aporepressor with its ligand, L-tryptophan

We have examined the interaction of the Escherichia coli trp aporepressor with its ligand, L-tryptophan, using both equilibrium dialysis and flow dialysis methods. Results obtained by the two procedures were equivalent and indicate that the trp aporepressor binds L-tryptophan with an equilibrium dissociation constant (Kd) of 40 microM at 25 degrees C under standard binding assay conditions (10 mM potassium phosphate, pH 7.4, 0.2 M potassium chloride, 0.1 mM EDTA, 5% glycerol). Molecular sizing of the purified trp aporepressor shows that in the absence of ligand the regulatory protein exists as a dimeric species with greater than 99% purity and an apparent molecular weight of 30,000. Under the storage and assay conditions used, the dimer appears quite stable, and essentially no monomer or higher multimeric species are detected. Analysis of binding data by Scatchard and direct linear plot methods shows two identical and independent ligand-binding sites/native trp aporepressor dimer. When examined as a function of temperature, L-tryptophan binding by trp aporepressor varied over 7-fold (Kd = 28 microM at 6.5 degrees C to Kd = 217 microM at 40 degrees C). At the optimal growth temperature for E. coli (37 degrees C), the dissociation constant was 160 microM for the ligand, L-tryptophan. From the relationship between temperature and L-tryptophan binding by trp aporepressor, the apparent enthalpy change delta H = -10.6 +/- 0.6 kcal mol-1 and the apparent entropy change delta S = -17 +/- 2 cal degree-1 mol-1 were determined.     

Location of an alpha-helix in fragment 96-133 from bovine somatotropin by 1H NMR spectroscopy

By use of two-dimensional NMR techniques most of the proton resonances (greater than 90%) are assigned for the tryptic digest fragment 96-133 of bovine somatotropin in 30% 2,2,2-trifluoroethanol-d3/70% H2O. Qualitative analysis of the nuclear Overhauser enhancement (NOE) data indicates that a region of alpha-helix spans residues 106-128, while the N- and C-terminal regions assume nonregular structures. Amide-exchange rates and comparison of two-dimensional NOE spectra indicate that the most stable piece of helix spans residues 120-125 and that this piece of helix is stable in water at 25 degrees C. Evidence is given to support the fact that intermolecular association of the helical segments stabilizes the helix.