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ClpPs are a conserved family of serine proteases that collaborate with ATP-dependent translocases to degrade protein substrates. Drugs targeting these enzymes have attracted interest for the treatment of cancer and bacterial infections due to their critical role in mitochondrial and bacterial proteostasis, respectively. As such, there is significant interest in understanding structure-function relationships in this protein family. ClpPs are known to crystallize in extended, compact, and compressed forms; however, it is unclear what conditions favor the formation of each form and whether they are populated by wild-type enzymes in solution. Here, we use cryo-EM and solution NMR spectroscopy to demonstrate that a pH-dependent conformational switch controls an equilibrium between the active extended and inactive compressed forms of ClpP from the Gram-negative pathogen Neisseria meningitidis . Our findings provide insight into how ClpPs exploit their rugged energy landscapes to enable key conformational changes that regulate their function.

The 300-kDa ClpP1P2 protease from Mycobacterium tuberculosis collaborates with the AAA+ (ATPases associated with a variety of cellular activities) unfoldases, ClpC1 and ClpX, to degrade substrate proteins. Unlike in other bacteria, all of the components of the Clp system are essential for growth and virulence of mycobacteria, and their inhibitors show promise as antibiotics. MtClpP1P2 is unique in that it contains a pair of distinct ClpP1 and ClpP2 rings and also requires the presence of activator peptides, such as benzoyl-leucyl-leucine (Bz-LL), for function. Understanding the structural basis for this requirement has been elusive but is critical for the rational design and improvement of antituberculosis (anti-TB) therapeutics that target the Clp system. Here, we present a combined biophysical and biochemical study to explore the structure-dynamics-function relationship in MtClpP1P2. Electron cryomicroscopy (cryo-EM) structures of apo and acyldepsipeptide-bound MtClpP1P2 explain their lack of activity by showing loss of a key β-sheet in a sequence known as the handle region that is critical for the proper formation of the catalytic triad. Methyl transverse relaxation-optimized spectroscopy (TROSY)-based NMR, cryo-EM, and biochemical assays show that, on binding Bz-LL or covalent inhibitors, MtClpP1P2 undergoes a conformational change from an inactive compact state to an active extended structure that can be explained by a modified Monod-Wyman-Changeux model. Our study establishes a critical role for the handle region as an on/off switch for function and shows extensive allosteric interactions involving both intra- and interring communication that regulate MtClpP1P2 activity and that can potentially be exploited by small molecules to target M. tuberculosis ., Competing Interests: The authors declare no competing interest.

Protein homeostasis is critically important for cell viability. Key to this process is the refolding of misfolded or aggregated proteins by molecular chaperones or, alternatively, their degradation by proteases. In most prokaryotes and in chloroplasts and mitochondria, protein degradation is performed by the caseinolytic protease ClpP, a tetradecamer barrel-like proteolytic complex. Dysregulating ClpP function has shown promise in fighting antibiotic resistance and as a potential therapy for acute myeloid leukemia. Here we use methyl-transverse relaxation-optimized spectroscopy (TROSY)-based NMR, cryo-EM, biochemical assays, and molecular dynamics simulations to characterize the structural dynamics of ClpP from Staphylococcus aureus (SaClpP) in wild-type and mutant forms in an effort to discover conformational hotspots that regulate its function. Wild-type SaClpP was found exclusively in the active extended form, with the N-terminal domains of its component protomers in predominantly β-hairpin conformations that are less well-defined than other regions of the protein. A hydrophobic site was identified that, upon mutation, leads to unfolding of the N-terminal domains, loss of SaClpP activity, and formation of a previously unobserved split-ring conformation with a pair of 20-Å-wide pores in the side of the complex. The extended form of the structure and partial activity can be restored via binding of ADEP small-molecule activators. The observed structural plasticity of the N-terminal gates is shown to be a conserved feature through studies of Escherichia coli and Neisseria meningitidis ClpP, suggesting a potential avenue for the development of molecules to allosterically modulate the function of ClpP., Competing Interests: The authors declare no conflict of interest.

The histidine kinase, CheA, couples environmental stimuli to changes in bacterial swimming behavior, converting a sensory signal to a chemical signal in the cytosol via autophosphorylation. The kinase activity is regulated in the platform of chemotaxis signaling complexes formed by CheW, chemoreceptors, and the regulatory domain of CheA. Our previous computational and mutational studies have revealed that two interdomain linkers play important roles in CheA's enzymatic activity. Of the two linkers, one that connects the dimerization and ATP binding domains is essential for both basal autophosphorylation and activation of the kinase. However, the mechanistic role of this linker remains unclear, given that it is far from the autophosphorylation reaction center (the ATP binding site). Here we investigate how this interdomain linker is coupled to CheA's enzymatic activity. Using modern nuclear magnetic resonance (NMR) techniques, we find that by interacting with the catalytic domain, the interdomain linker initiates long-range structural and dynamic changes directed toward the catalytic center of the autophosphorylation reaction. Subsequent biochemical assays define the functional relevance of these NMR-based observations. These findings extend our understanding of the chemotaxis signal transduction pathway.

NMR spectroscopy and computer simulations were used to examine changes in chemical shifts and in dynamics of the ribonuclease barnase that result upon binding to its natural inhibitor barstar. Although the spatial structures of free and bound barnase are very similar, binding results in changes of the dynamics of both fast side-chains, as revealed by (2)H relaxation measurements, and NMR chemical shifts in an extended beta-sheet that is located far from the binding interface. Both side-chain dynamics and chemical shifts are sensitive to variations in the ensemble populations of the inter-converting molecular states, which can escape direct structural observation. Molecular dynamics simulations of free barnase and barnase in complex with barstar, as well as a normal mode analysis of barnase using a Gaussian network model, reveal relatively rigid domains that are separated by the extended beta-sheet mentioned above. The observed changes in NMR parameters upon ligation can thus be rationalized in terms of changes in inter-domain dynamics and in populations of exchanging states, without measurable structural changes. This provides an alternative model for the propagation of a molecular response to ligand binding across a protein that is based exclusively on changes in dynamics.

(15)N spin relaxation data have provided a wealth of information on protein dynamics in solution. Standard R(1), R(1)(rho), and NOE experiments aimed at (15)N[(1)H] amide moieties are complemented in this work by HA(CACO)N-type experiments allowing the measurement of nitrogen R(1) and R(1)(rho) rates at deuterated (15)N[(2)D] sites. Difference rates obtained using this approach, R(1)((15)N[(1)H]) - R(1)((15)N[(2)D]) and R(2)((15)N[(1)H]) - R(2)((15)N[(2)D]), depend exclusively on dipolar interactions and are insensitive to (15)N CSA and R(ex) relaxation mechanisms. The methodology has been tested on a sample of peptostreptococcal protein L (63 residues) prepared in 50% H(2)O-50% D(2)O solvent. The results from the new and conventional experiments are found to be consistent, with respect to both local backbone dynamics and overall protein tumbling. Combining several data sets permits evaluation of the spectral density J(omega(D) + omega(N)) for each amide site. This spectral density samples a uniquely low frequency (26 MHz at a 500 MHz field) and, therefore, is expected to be highly useful for characterizing nanosecond time scale local motions. The spectral density mapping demonstrates that, in the case of protein L, J(omega(D) + omega(N)) values are compatible with the Lipari-Szabo interpretation of backbone dynamics based on the conventional (15)N relaxation data.

Simple pulse schemes are presented for the measurement of methyl (13)C and (1)H CSA values from (1)H-(13)C dipole/(13)C CSA and (1)H-(13)C dipole/(1)H CSA cross-correlated relaxation. The methodology is applied to protein L and malate synthase G. Average (13)C CSA values are considerably smaller for Ile than Leu/Val (17 vs 25 ppm) and are in good agreement with previous solid state NMR studies of powders of amino acids and dipeptides and in reasonable agreement with quantum-chemical DFT calculations of methyl carbon CSA values in peptide fragments. Small averaged (1)H CSA values on the order of 1 ppm are measured, consistent with a solid state NMR determination of the methyl group (1)H CSA in dimethylmalonic acid.

Rotating-frame relaxation rates, R(1)(rho), are often measured in NMR studies of protein dynamics. We show here that large systematic errors can be introduced into measured values of heteronuclear R(1)(rho) rates using schemes which are usually employed to suppress cross-correlation between dipole-dipole and CSA relaxation mechanisms. For example, in a scalar-coupled two-spin X-H spin system the use of (1)H WALTZ16 decoupling or (1)H pulses applied at regularly spaced intervals leads to a significant overestimation of heteronuclear R(1)(rho) values. The problem is studied experimentally and theoretically for (15)N-(1)H and (13)C-(1)H spin pairs, and simple schemes are described which eliminate the artifacts. The approaches suggested are essential replacements of existing methodology if accurate dynamics parameters are to be extracted from spin-lock relaxation data sets.

In the previous paper in this issue we have demonstrated that it is possible to measure the five different relaxation rates of a deuteron in (13)CH(2)D methyl groups of (13)C-labeled, fractionally deuterated proteins. The extensive set of data acquired in these experiments provides an opportunity to investigate side-chain dynamics in proteins at a level of detail that heretofore was not possible. The data, acquired on the B1 domain of peptostreptococcal protein L, include 16 (9) relaxation measurements at 4 (2) different magnetic field strengths, 25 degrees C (5 degrees C). These data are shown to be self-consistent and are analyzed using a spectral density mapping procedure which allows extraction of values of the spectral density function at a number of frequencies with no assumptions about the underlying dynamics. Dynamics data from 31 of 35 methyls in the protein for which data could be obtained were well-fitted using the two-parameter Lipari-Szabo model (Lipari, G.; Szabo, A. J. Am. Chem. Soc. 1982, 104, 4546). The data from the remaining 4 methyls can be fitted using a three-parameter version of the Lipari-Szabo model that takes into account, in a simple manner, additional nanosecond time-scale local dynamics. This interpretation is supported by analysis of a molecular dynamics trajectory where spectral density profiles calculated for side-chain methyl sites reflect the influence of slower (nanosecond) time-scale motions involving jumps between rotameric wells. A discussion of the minimum number of relaxation measurements that are necessary to extract the full complement of dynamics information is presented along with an interpretation of the extracted dynamics parameters.

New pulse sequences are presented for the measurement of the relaxation of deuterium double quantum, quadrupolar order, and transverse antiphase magnetization in (13)CH(2)D methyl groups of (15)N-, (13)C-labeled, fractionally deuterated proteins. Together with previously developed experiments for measuring deuterium longitudinal and transverse decay rates [Muhandiram, D. R.; Yamazaki, T.; Sykes, B. D.; Kay, L. E. J. Am. Chem. Soc. 1995, 117, 11536], these schemes allow measurement of the five unique decay constants of a single deuteron, providing an unprecedented opportunity to investigate side-chain dynamics in proteins. All five deuterium relaxation rates have been measured for deuterons in the methyl groups of the B1 immunoglobulin binding domain of peptostreptococcal protein L and the N-terminal SH3 domain from the protein drk. Since values of the spectral density function at only three different frequencies contribute to the five relaxation rates, the self-consistency of the relaxation data is readily established. Very good agreement is obtained between calculated parameters describing the amplitudes and time scales of motion when different subsets of the relaxation data are employed.

One bond methyl 1H-13C and 13Cmethyl-13C scalar and residual dipolar couplings have been measured at sites in an 15N, 13C, approximately 50% 2H labeled sample of the B1 immunoglobulin binding domain of peptostreptococcal protein L to investigate changes in the structure of methyl groups in response to deuterium substitution. Both one bond methyl 1H-13C and 13Cmethyl-13C scalar coupling constants have been found to decrease slightly with increasing deuterium content. Previous studies have shown that 1H-13C couplings in methyl groups are exquisitely sensitive to electronic structure, with decreases in coupling values as a function of deuteration consistent with a slight lengthening of the remaining H-C bonds. Changes in the HmethylCmethylC angle are found to be small, with average differences on the order of 0.3+/-0.1 degrees and 0.4+/-0.2 degrees between CH3, CH2D and CH3, CHD2 isotopomers, respectively. Knowledge of methyl geometry is a prerequisite for the extraction of accurate dynamics parameters from spin relaxation studies involving these groups.

Experiments are presented for the measurement of one-bond carbon-proton dipolar coupling values at CH and CH2 ositions in 13C-labeled, approximately 50% fractionally deuterated proteins. 13Cbeta-1Hbeta dipolar couplings have been measured for 38 of 49 possible residues in the 63-amino-acid B1 domain of peptostreptococcal protein L in two aligning media and interpreted in the context of side-chain chi1 torsion angle dynamics. The beta protons for 18 of the 25 beta-methylene-containing amino acids for which dipolar data are available can be unambiguously stereoassigned, and for those residues which are best fit to a single rotamer model the chi(1) angles obtained deviate from crystal structure values by only 5.2 degrees (rmsd). The results for 11 other residues are significantly better fit by a model that assumes jumps between the three canonical (chi1 approximately -60 degrees, 60 degrees, 180 degrees ) rotamers. Relative populations of the rotamers are determined to within +/-6% uncertainty on average and correlate with dihedral angles observed for the three molecules in the crystal asymmetric unit. Entropic penalties for quenching chi1 jumps are considered for six mobile residues thought to be involved in binding to human immunoglobulins. This study demonstrates that dipolar couplings may be used to characterize both the conformation of static residues and side-chain motion with high precision.

Solution NMR studies on the physiologically relevant ligand-free and maltotriose-bound states of maltodextrin-binding protein (MBP) are presented. Together with existing data on MBP in complex with beta-cyclodextrin (non-physiological, inactive ligand), these new results provide valuable information on changes in local structure, dynamics and global fold that occur upon ligand binding to this two-domain protein. By measuring a large number of different one-bond residual dipolar couplings, the domain conformations, critical for biological function, were investigated for all three states of MBP. Structural models of the solution conformation of MBP in a number of different forms were generated from the experimental dipolar coupling data and X-ray crystal structures using a quasi-rigid-body domain orientation algorithm implemented in the structure calculation program CNS. Excellent agreement between relative domain orientations in ligand-free and maltotriose-bound solution conformations and the corresponding crystal structures is observed. These results are in contrast to those obtained for the MBP/beta-cyclodextrin complex where the solution state is found to be approximately 10 degrees more closed than the crystalline state. The present study highlights the utility of residual dipolar couplings for orienting protein domains or macromolecules with respect to each other., (Copyright 2001 Academic Press.)

The global fold of maltose-binding protein in complex with the substrate beta-cyclodextrin was determined by solution NMR methods. The two-domain protein is comprised of a single polypeptide chain of 370 residues, with a molecular mass of 42 kDa. Distance information in the form of H(N)-H(N), H(N)-CH(3) and CH(3)-CH(3) NOEs was recorded on (15)N, (2)H and (15)N, (13)C, (2)H-labeled proteins with methyl protonation in Val, Leu, and Ile (C(delta1) only) residues. Distances to methyl protons, critical for the structure determination, comprised 77 % of the long-range restraints. Initial structures were calculated on the basis of 1943 NOEs, 48 hydrogen bond and 555 dihedral angle restraints. A global pair-wise backbone rmsd of 5.5 A was obtained for these initial structures with rmsd values for the N and C domains of 2.4 and 3.8 A, respectively. Direct refinement against one-bond (1)H(N)-(15)N, (13)C(alpha)-(13)CO, (15)N-(13)CO, two-bond (1)H(N)-(13)CO and three-bond (1)H(N)-(13)C(alpha) dipolar couplings resulted in structures with large numbers of dipolar restraint violations. As an alternative to direct refinement against measured dipolar couplings we have developed an approach where discrete orientations are calculated for each peptide plane on the basis of the dipolar couplings described above. The orientation which best matches that in initial NMR structures calculated from NOE and dihedral angle restraints exclusively is used to refine further the structures using a new module written for CNS. Modeling studies from four different proteins with diverse structural motifs establishes the utility of the methodology. When applied to experimental data recorded on MBP the precision of the family of structures generated improves from 5.5 to 2.2 A, while the rmsd with respect to the X-ray structure (1dmb) is reduced from 5.1 to 3.3 A., (Copyright 2000 Academic Press.)

Protein function is often regulated by conformational changes that occur in response to ligand binding or covalent modification such as phosphorylation. In many multidomain proteins these conformational changes involve reorientation of domains within the protein. Although X-ray crystallography can be used to determine the relative orientation of domains, the crystal-state conformation can reflect the effect of crystal packing forces and therefore may differ from the physiologically relevant form existing in solution. Here we demonstrate that the solution-state conformation of a multidomain protein can be obtained from its X-ray structure using an extensive set of dipolar couplings measured by triple-resonance multidimensional NMR spectroscopy in weakly aligning solvent. The solution-state conformation of the 370-residue maltodextrin-binding protein (MBP) loaded with beta-cyclodextrin has been determined on the basis of one-bond (15)N-H(N), (15)N-(13)C', (13)C(alpha)-(13)C', two-bond (13)C'-H(N), and three-bond (13)C(alpha)-H(N) dipolar couplings measured for 280, 262, 276, 262, and 276 residues, respectively. This conformation was generated by applying hinge rotations to various X-ray structures of MBP seeking to minimize the difference between the experimentally measured and calculated dipolar couplings. Consistent structures have been derived in this manner starting from four different crystal forms of MBP. The analysis has revealed substantial differences between the resulting solution-state conformation and its crystal-state counterpart (Protein Data Bank accession code 1DMB) with the solution structure characterized by an 11(+/-1) degrees domain closure. We have demonstrated that the precision achieved in these analyses is most likely limited by small uncertainties in the intradomain structure of the protein (ca 5 degrees uncertainty in orientation of internuclear vectors within domains). In addition, potential effects of interdomain motion have been considered using a number of different models and it was found that the structures derived on the basis of dipolar couplings accurately represent the effective average conformation of the protein., (Copyright 2000 Academic Press.)

Deuterium decoupled, triple resonance NMR spectroscopy was used to analyze complexes of 2H, 15N, 13C labelled intact and (des2-7) trp repressor (delta 2-7 trpR) from E. coli bound in tandem to an idealized 22 basepair trp operator DNA fragment and the corepressor 5-methyltryptophan. The DNA sequence used here binds two trpR dimers in tandem resulting in chemically nonequivalent environments for the two subunits of each dimer. Sequence- and subunit-specific NMR resonance assignments were made for backbone 1HN, 15N, 13c alpha positions in both forms of the protein and for 13 C beta in the intact repressor. The differences in backbone chemical shifts between the two subunits within each dimer of delta 2-7 trpR reflect dimer-dimer contacts involving the helix-turn-helix domains and N-terminal residues consistent with a previously determined crystal structure [Lawson and Carey (1993) Nature, 366, 178-182]. Comparison of the backbone chemical shifts of DNA-bound delta 2-7 trpR with those of DNA-bound intact trpR reveals significant changes for those residues involved in N-terminal-mediated interactions observed in the crystal structure. In addition, our solution NMR data contain three sets of resonances for residues 2-12 in intact trpR suggesting that the N-terminus has multiple conformations in the tandem complex. Analysis of C alpha chemical shifts using a chemical shift index (CSI) modified for deuterium isotope effects has allowed a comparison of the secondary structure of intact and delta 2-7 tprR. Overall these data demonstrate that NMR backbone chemical shift data can be readily used to study specific structural details of large protein complexes.

The Escherichia coli histidine autokinase CheA plays an important role in coupling signals received from membrane-bound receptors to changes in the swimming behavior of the cells in order to respond appropriately to environmental signals. Here we describe the structure of the 14 kDa fragment of the chemotaxis kinase CheA, residues 124--257, which binds to the downstream targets of phosphorylation, the response regulators CheY and CheB. This protein fragment contains the CheY-binding domain flanked on each side by regions that correspond to domain linkers in the intact protein. The structure of the domain was determined from 1429 restraints derived from heteronuclear multidimensional NMR experiments. Hybrid distance geometry--dynamical simulated annealing methods were used to calculate a family of structures that satisfy the experimental distance restraints and torsion angle restraints. The root mean square deviation of the 69 ordered residues in the domain is 0.52 A for the backbone heavy atoms and 0.99 A for all heavy atoms. The residues that have been implicated as important for CheY binding form a face consisting of several partially buried hydrophobic residues, framed by charged residues. The dynamic properties of this protein fragment were measured and analyzed using both isotropic and anisotropic models of molecular motion. The linker regions are very flexible and disordered, as evidenced by the very dynamics properties as compared to the CheY-binding domain. The CheY-binding domain of CheA is structurally similar to the histidine-containing phosphocarrier, HPr, which is a protein involved in the phosphoenolpyruvate:sugar phosphotransferase (PTS) pathway. This structural similarity suggests a possible evolutionary relationship of the PTS and chemotaxis pathways.

CheA is the histidine autokinase in the Escherichia coli chemotaxis signal transduction pathway responsible for coupling of signals received by transmembrane receptors to the response regulators CheY and CheB. Here NMR spectroscopy is used to study a 14 kDa fragment of CheA, residues 124-257, that binds the response regulator CheY. Backbone atom resonance assignments were obtained by analysis of 3D HNCACB, 3D CBCA(CO)NH, and HNCO spectra, whereas side-chain assignments were obtained primarily by analysis of 3D H(CCO)NH, 3D C(CO)NH, 3D HCCH-TOCSY, and 3D 1H, 15N TOCSY-HSMQC spectra. NOE cross peak patterns and intensities as well as torsion angle restraints were used to determine the secondary structure, and a low-resolution structure was calculated by hybrid distance-geometry simulated annealing methods. The CheA124-257 fragment consists of four antiparallel beta strands and two helices, arranged in an "open-faced beta-sandwich" motif, as well as two unstructured ends that correspond to domain linkers in the full-length protein. The 15N-1H correlation spectrum of 15N-labeled CheA124-257 bound to unlabeled CheY shows specific localized changes that may correspond to a CheY-binding face on CheA.

A pulsed field gradient three-dimensional isotope-filtered 13C HMQC-NOESY experiment has been developed to characterize intermolecular contacts in a 37 kDa macromolecular ternary complex consisting of uniformly 13C labeled trp-repressor, its natural abundance co-repressor, L-tryptophan, and natural abundance operator DNA. The pulse scheme makes use of pulsed field gradients for the removal of artifacts and dephasing of unwanted magnetization during isotope filtering, and employs a strategy to minimize the time that magnetization resides in the transverse plane. The experiment provides solely intermolecular NOE contacts between protons of the labeled protein and protons of the unlabeled species, and has proven to be especially useful in eliminating ambiguities between intra- and intermolecular NOEs in the isotope-edited 3D 13C HMQC-NOESY spectrum of the complex.

Multidimensional heteronuclear NMR spectroscopy has been used to determine almost complete backbone and side-chain 1H, 15N, and 13C resonance assignments of calcium loaded Myxococcus xanthus protein S (173 residues). Of the range of constant-time triple resonance experiments recorded, HNCACB and CBCA(CO)NH, which correlate C alpha and C beta with backbone amide resonances of the same and the succeeding residue respectively, proved particularly useful in resolving assignment ambiguities created by the 4-fold internal homology of the protein S amino acid sequence. Extensive side-chain 1H and 13C assignments have been obtained by analysis of HCCH-TOCSY and 15N-edited TOCSY-HMQC spectra. A combination of NOE, backbone amide proton exchange, 3JNH alpha coupling constant, and chemical shift data has been used to show that each of the protein S repeat units consists of four beta-strands in a Greek key arrangement. Two of the Greek keys contain a regular alpha-helix between the third and fourth strands, resulting in an unusual and possibly unique variation on this common folding motif. Despite similarity between two nine-residue stretches in the first and third domains of protein S and one of the Ca(2+)-binding sequences in bovine brain calmodulin [Inouye, S., Franceschini, T., & Inouye, M. (1983) Proc. Natl. Acad. Sci. U.S.A. 80, 6829-6833], the protein S topology in these regions is incompatible with an EF-hand calmodulin-type Ca(2+)-binding site.

The solution conformation of uniformly labeled 15N human thioredoxin has been studied by two-dimensional heteronuclear 15N-1H nuclear magnetic resonance spectroscopy. Assignments of the 15N resonances of the protein are obtained in a sequential manner using heteronuclear multiple quantum coherence (HMQC), relayed HMQC-correlated (COSY), and relayed HMQC-nuclear Overhauser (NOESY) spectroscopy. Values of the 3JHN alpha splittings for 87 of the 105 residues of thioredoxin are extracted from a variant of the HMQC-COSY experiment, known as HMQC-J, and analyzed to give accurate 3JHN alpha coupling constants. In addition, long-range C alpha H(i)-15N(i + 1) scaler connectivities are identified by heteronuclear multiple bond correlation (HMBC) spectroscopy. The presence of these three-bond scaler connectivities in predominantly alpha-helical regions correlates well with the secondary structure determined previously from a qualitative analysis of homonuclear nuclear Overhauser data [Forman-Kay, J. D., Clore, G. M., Driscoll, P.C., Wingfield, P. T., Richards, F. M., & Gronenborn, A. M. (1989) Biochemistry 28, 7088-7097], suggesting that this technique may provide additional information for secondary structure determination a priori. The accuracy with which 3JHN alpha coupling constants can be obtained from the HMQC-J experiment permits a more precise delineation of the beginnings and ends of secondary structural elements of human thioredoxin and of irregularities in these elements.