Dipolar filtered 1H-13C heteronuclear correlation spectroscopy for resonance assignment of proteins

Resonance assignment is necessary for the comprehensive structure determination of insoluble proteins by solid-state NMR spectroscopy. While various 2D and 3D correlation techniques involving ¹³C and ¹⁵N spins have been developed for this purpose, ¹H chemical shift has not been exploited sufficiently. We demonstrate the combination of the regular ¹H-¹³C heteronuclear correlation (HETCOR) experiment and a dipolar filtered HETCOR technique to obtain better resolved ¹H chemical shift spectra. The dipolar filtered experiment, MELODI-HETCOR, simplifies the ¹H spectra by suppressing the directly bonded C-H correlation peaks and retaining only the medium- and long-range cross peaks. We apply this MELODI-HETCOR technique to several amino acids and proteins with various isotopic labeling patterns. The enhanced ¹H chemical shift resolution allows the assignment of overlapping H and H resonances in Ser, identifies the ¹H chemical shift differences between neutral and cationic imidazole rings of His, and permits the assignment of residues with side chain nitrogen atoms in ubiquitin. The potential utility of this dipolar filtered HETCOR technique to resonance assignment of extensively labeled proteins is discussed.     

Structure refinement of flexible proteins using dipolar couplings: Application to the protein p8MTCP1

The present study deals with the relevance of using mobility-averaged dipolar couplings for the structure refinement of flexible proteins. The 68-residue protein p8^MTCP1 has been chosen as model for this study. Its solution state consists mainly of three -helices. The two N-terminal helices are strapped in a well-determined -hairpin, whereas, due to an intrinsic mobility, the position of the third helix is less well defined in the NMR structure. To further characterize the degrees of freedom of this helix, we have measured the dipolar coupling constants in the backbone of p8^MTCP1 in a bicellar medium. We show here that including D _HN ^dip dipolar couplings in the structure calculation protocol improves the structure of the -hairpin but not the positioning of the third helix. This is due to the motional averaging of the dipolar couplings measured in the last helix. Performing two calculations with different force constants for the dipolar restraints highlights the inconstancy of these mobility-averaged dipolar couplings. Alternatively, prior to any structure calculations, comparing the values of the dipolar couplings measured in helix III to values back-calculated from an ideal helix demonstrates that they are atypical for a helix. This can be partly attributed to mobility effects since the inclusion of the ¹⁵N relaxation derived order parameter allows for a better fit.     

Optimized set of two-dimensional experiments for fast sequential assignment,secondary structure determination,and backbone fold validation of 13C/15N-labelled proteins

NMR experiments are presented which allow backbone resonance assignment, secondary structure identification, and in favorable cases also molecular fold topology determination from a series of two-dimensional ¹H-¹⁵N HSQC-like spectra. The ¹H-¹⁵N correlation peaks are frequency shifted by an amount ± _X along the ¹⁵N dimension, where _X is the C, C, or H frequency of the same or the preceding residue. Because of the low dimensionality (2D) of the experiments, high-resolution spectra are obtained in a short overall experimental time. The whole series of seven experiments can be performed in typically less than one day. This approach significantly reduces experimental time when compared to the standard 3D-based methods. The here presented methodology is thus especially appealing in the context of high-throughput NMR studies of protein structure, dynamics or molecular interfaces.     

1H and 15N NMR resonance assignments and solution secondary structure of oxidized Desulfovibrio desulfuricans flavodoxin

Summary Sequence-specific ¹H and ¹⁵N resonance assignments have been made for 137 of the 146 nonprolyl residues in oxidized Desulfovibrio desulfuricans [Essex 6] flavodoxin. Assignments were obtained by a concerted analysis of the heteronuclear three-dimensional ¹H-¹⁵N NOESY-HMQC and TOCSY-HMQC data sets, recorded on uniformly ¹⁵N-enriched protein at 300 K. Numerous side-chain resonances have been partially or fully assigned. Residues with overlapping ¹H^N chemical shifts were resolved by a three-dimensional ¹H-¹⁵N HMQC-NOESY-HMQC spectrum. Medium-and long-range NOEs, ³J_NH coupling constants, and ¹H^N exchange data indicate a secondary structure consisting of five parallel -strands and four -helices with a topology similar to that of Desulfovibrio vulgaris [Hidenborough] flavodoxin. Prolines at positions 106 and 134, which are not conserved in D. vulgaris flavodoxin, contort the two C-terminal -helices.Abbreviations CSI chemical shift index - DQF-COSY double-quantum-filtered correlation spectroscopy - DIPSI decoupling in the presence of scalar interactions - FMN flavin mononucleotide - GARP globally optimized alternating phase rectangular pulse - HMQC heteronuclear multiple-quantum coherence - HSQC heteronuclear single-quantum coherence - NOE nuclear Overhauser effect - NOESY nuclear Overhauser enhancement spectroscopy - TOCSY total correlation spectroscopy - TPPI time-proportional phase increments - TSP 3-(trimethylsilyl)propionic-2,2,3,3-d ₄ acid, sodium salt     

Three-dimensional experiment for solid-state NMR of aligned protein samples in high field magnets

A pulse sequence that yields three-dimensional ¹H chemical shift / ¹H-¹⁵N heteronuclear dipolar coupling / ¹⁵N chemical shift solid-state NMR spectra is demonstrated on a uniformly ¹⁵N labeled membrane protein in magnetically aligned phospholipid bilayers. Based on SAMPI4, the pulse sequence yields high resolution in all three dimensions at a ¹H resonance frequency of 900 MHz with the relatively low rf field strength (33 kHz) available for a lossy aqueous sample with a commercial spectrometer and probe. The ¹H chemical shift frequency dimension is shown to select among amide resonances, which will be useful in studies of larger polytopic membrane proteins where the resonances overlap in two-dimensional spectra. Moreover, the ¹H chemical shift, which can be measured from these spectra, provides an additional orientationally dependent frequency as input for structure calculations. Both Alexander A. Nevzorov and Sang Ho Park contributed equally to this work.     

Towards high-resolution solid-state NMR on large uniformly 15N- and [13C,15N]-labeled membrane proteins in oriented lipid bilayers

Based on exact numerical simulations, taking into account isotropic and conformation-dependent anisotropic nuclear spin interactions, we systematically analyse the prospects for high-resolution solid-state NMR on large isotope-labeled membrane proteins macroscopically oriented in phospholipid bilayers. Using the known X-ray structures of rhodopsin and porin as models for large membrane proteins with typical -helical and -barrel structural motifs, the analysis considers all possible one- to six-dimensional spectra comprised of frequency dimensions with evolution under any combination of amide ¹H, amide ¹⁵N, and carbonyl ¹³C chemical shifts as well as ¹H-¹⁵N dipole-dipole couplings. Under consideration of typical nuclear spin interaction and experimental line-shape parameters, the analysis provides new insight into the resolution capability and orientation-dependent transfer efficiency of existing experiments as well as guidelines as to improved experimental approaches for the study of large uniformly ¹⁵N- and [¹³C,¹⁵N]-labeled membrane proteins. On basis of these results and numerical optimizations of coherence-transfer efficiencies, we propose several new high-resolution experiments for sequential protein backbone assignment and structure determination.     

Backbone dynamics of bacteriorhodopsin as studied by <Superscript>13</Superscript>C solid-state NMR spectroscopy

The surface dynamics of bacteriorhodopsin was examined by measurements of site-specific ¹³C–¹H dipolar couplings in [3-¹³C]Ala-labeled bacteriorhodopsin. Motions of slow or intermediate frequency (correlation time <50 µs) scale down ¹³C–¹H dipolar couplings according to the motional amplitude. The two-dimensional dipolar and chemical shift (DIPSHIFT) correlation technique was utilized to obtain the dipolar coupling strength for each resolved peak in the ¹³C MAS solid-state NMR spectrum, providing the molecular order parameter of the respective site. In addition to the rotation of the Ala methyl group, which scales the dipolar coupling to 1/3 of the rigid limit value, fluctuations of the C–C vector result in additional motional averaging. Typical order parameters measured for mobile sites in bacteriorhodopsin are between 0.25 and 0.29. These can be assigned to Ala103 of the C–D loop and Ala235 at the C-terminal -helix protruded from the membrane surface, and Ala196 of the F–G loop, as well as to Ala228 and Ala233 of the C-terminal -helix and Ala51 from the transmembrane -helix. Such order parameters departing significantly from the value of 0.33 for rotating methyl groups are obviously direct evidence for the presence of fluctuation motions of the Ala C–C vectors of intact preparations of fully hydrated, wild-type bacteriorhodopsin at ambient temperature. The order parameter for Ala160 from the expectantly more flexible E–F loop, however, is unavailable under highest-field NMR conditions, probably because increased chemical shift anisotropy together with intrinsic fluctuation motions result in an unresolved ¹³C NMR signal.     

The effect of noncollinearity of 15N-1H dipolar and 15N CSA tensors and rotational anisotropy on 15N relaxation, CSA/dipolar cross correlation, and TROSY

Current approaches to 15N relaxation in proteins assume that the 15N-1H dipolar and 15N CSA tensors are collinear. We show theoretically that, when there is significant anisotropy of molecular rotation, different orientations of the two tensors, experimentally observed in proteins, nucleic acids, and small peptides, will result in differences in site- specific correlation functions and spectral densities. The standard treatments of the rates of longitudinal and transverse relaxation of amide 15N nuclei, of the 15N CSA/15N-1H dipolar cross correlation, and of the TROSY experiment are extended to account for the effect of noncollinearity of the 15N-1H dipolar and 15N CSA (chemical shift anisotropy) tensors. This effect, proportional to the degree of anisotropy of the overall motion, (D/D–1), is sensitive to the relative orientation of the two tensors and to the orientation of the peptide plane with respect to the diffusion coordinate frame. The effect is negligible at small degrees of anisotropy, but is predicted to become significant for D/D1.5, and at high magnetic fields. The effect of noncollinearity of 15N CSA and 15N-1H dipolar interaction is sensitive to both gross (hydrodynamic) properties and atomic-level details of protein structure. Incorporation of this effect into relaxation data analysis is likely to improve both precision and accuracy of the derived characteristics of protein dynamics, especially at high magnetic fields and for molecules with a high degree of anisotropy of the overall motion. The effect will also make TROSY efficiency dependent on local orientation in moderately anisotropic systems.     

Direct measurement of the 15N CSA/dipolar relaxation interference from coupled HSQC spectra

Here we propose a method for the measurement of the ¹⁵N CSA/dipolar relaxation interference based on direct comparison of the ¹⁵N doublet components observed in a ¹H-coupled ¹H-¹⁵N HSQC-type spectrum. This allows the determination of the cross-correlation rates with no need for correction factors associated with other methods. The signal overlap problem of coupled HSQC spectra is addressed here by using the IPAP scheme (Ottiger et al., 1998). The approach is applied to the B3 domain of protein G to show that the method provides accurate measurements of the ¹⁵N CSA/dipolar cross-correlation rates.     

Assignment of amide proton signals by combined evaluation of HN,NN and HNCA MAS-NMR correlation spectra

In this paper, we present a strategy for the ¹H^N resonance assignment in solid-state magic-angle spinning (MAS) NMR, using the -spectrin SH3 domain as an example. A novel 3D triple resonance experiment is presented that yields intraresidue H^N-N-C correlations, which was essential for the proton assignment. For the observable residues, 52 out of the 54 amide proton resonances were assigned from 2D (¹H-¹⁵N) and 3D (¹H-¹⁵N-¹³C) heteronuclear correlation spectra. It is demonstrated that proton-driven spin diffusion (PDSD) experiments recorded with long mixing times (4 s) are helpful for confirming the assignment of the protein backbone ¹⁵N resonances and as an aid in the amide proton assignment.     

A set of HNCO-based experiments for measurement of residual dipolar couplings in 15N, 13C, (2H)-labeled proteins

Several HNCO-based three-dimensional experiments are described for the measurement of ¹³C(i–1)-¹³C(i–1), ¹⁵N(i)-¹³C(i–1), ¹⁵N(i)-¹³C(i), ¹⁵N(i)-¹³C(i–1), ¹H^N(i)-¹³C(i), ¹H^N(i)-¹³C(i–1), and ¹³C(i–1)-¹³C(i–1) scalar and dipolar couplings in ¹⁵N, ¹³C, (²H)-labelled protein samples. These pulse sequences produce spin-state edited spectra superficially resembling an HNCO correlation spectrum, allowing accurate and simple measurement of couplings without introducing additional spectral crowding. Scalar and dipolar couplings are measured with good sensitivity from relatively large proteins, as demonstrated with three proteins: cardiac Troponin C, calerythrin and ubiquitin. Measurement of several dipolar couplings between spin-1/2 nuclei using spin-state selective 3D HNCO spectra provides a wealth of structural information.     

Analysis of the amide <Superscript>15</Superscript>N chemical shift tensor of the C<Subscript>α</Subscript> tetrasubstituted constituent of membrane-active peptaibols,the α-aminoisobutyric acid residue,compared to those of di- and tri-substituted proteinogenic amino acid residues

In protein NMR spectroscopy the chemical shift provides important information for the assignment of residues and a first structural evaluation of dihedral angles. Furthermore, angular restraints are obtained from oriented samples by solution and solid-state NMR spectroscopic approaches. Whereas the anisotropy of chemical shifts, quadrupolar couplings and dipolar interactions have been used to determine the structure, dynamics and topology of oriented membrane polypeptides using solid-state NMR spectroscopy similar concepts have been introduced to solution NMR through the measurements of residual dipolar couplings. The analysis of ¹⁵N chemical shift spectra depends on the accuracy of the chemical shift tensors. When investigating alamethicin and other peptaibols, i.e. polypeptides rich in α-aminoisobutyric acid (Aib), the ¹⁵N chemical shift tensor of this C_α-tetrasubstituted amino acid exhibits pronounced differences when compared to glycine, alanine and other proteinogenic residues. Here we present an experimental investigation on the ¹⁵N amide Aib tensor of N-acetyl-Aib-OH and for the Aib residues within peptaibols. Furthermore, a statistical analysis of the tensors published for di- (glycine) and tri-substituted residues has been performed, where for the first time the published data sets are compiled using a common reference. The size of the isotropic chemical shift and main tensor elements follows the order di- < tri- < tetra-substituted amino acids. A ¹⁵N chemical shift-¹H-¹⁵N dipolar coupling correlation NMR spectrum of alamethicin is used to evaluate the consequences of variations in the main tensor elements for the structural analysis of this membrane peptide.     

1H-15N Spin–spin couplings in alumichrome

We report the determination of two- and three-bond ¹H-¹⁵N spin–spin couplings in the nmr spectra of a polypeptide. The ¹H- and ¹⁵N-nmr spectra of 99.2% ¹⁵N-enriched alumichrome have been studied at 360 MHz and 10.1 MHz, repectively. While some ²J and ³J coupling are of the order of 5 Hz, most splitting resulting from the heteronuclear interaction are ?2 Hz, which introduces strigent requirements of spectral resolution. In the ¹H spectra these requirements were met by digital deconvolution with a sine bell routine combined with positive exponential filtering. Although the ¹⁵N spectra clearly exhibit features of fine structure, mainly because of the intrinsic higher nmir sensitivity of protons, observation of ¹H-¹⁵N spin–spin couplings was found to be more practical in the ¹H than in the ¹⁵N spectra. We find that the alumichrome data do not satisfy a simple cyclic relationship linking the heteronuclear couplings to the crystallographic ψ dihedral angles. It is suggested that a formal treatment of the ψ-related interresidue ¹H-¹⁵N coupling might have to take into account a more complex dependence of the intervening ³J on the overall local electronic structure, which is dependent on ?,ψ, and ω simultaneoulsy. In contrast, our analysis indicates that χ¹ can be readily determined from the measurement of the corresponding heteronuclear ³J coupling in the ¹H^β or in the amide ¹⁵N resonances. Karplus relationships are proposed that relate this heteronuclear ³J to the corresponding dihedral angle θ and which, on average, yield      

Order Parameters of a Transmembrane Helix in a Fluid Bilayer: Case Study of a WALP Peptide

A new solid-state NMR-based strategy is established for the precise and efficient analysis of orientation and dynamics of transmembrane peptides in fluid bilayers. For this purpose, several dynamically averaged anisotropic constraints, including ¹³C and ¹⁵N chemical shift anisotropies and ¹³C-¹⁵N dipolar couplings, were determined from two different triple-isotope-labeled WALP23 peptides (²H, ¹³C, and ¹⁵N) and combined with previously published quadrupolar splittings of the same peptide. Chemical shift anisotropy tensor orientations were determined with quantum chemistry. The complete set of experimental constraints was analyzed using a generalized, four-parameter dynamic model of the peptide motion, including tilt and rotation angle and two associated order parameters. A tilt angle of 21° was determined for WALP23 in dimyristoylphosphatidylcholine, which is much larger than the tilt angle of 5.5° previously determined from ²H NMR experiments. This approach provided a realistic value for the tilt angle of WALP23 peptide in the presence of hydrophobic mismatch, and can be applied to any transmembrane helical peptide. The influence of the experimental data set on the solution space is discussed, as are potential sources of error.     

3D 13C-15N-heteronuclear two-spin coherence spectroscopy for polypeptide backbone assignments in 13C-15N-double-labeled proteins

Summary The pulse sequence of a new constant-time 3D triple-resonance experiment, ct-HA[CAN]HN, is presented. This experiment delineates exclusively scalar connectivities and uses ¹³C–¹⁵N heteronuclear two-spin coherence to overlay the chemical shift evolution periods of the ¹³C and ¹⁵N nuclei, thereby providing the four resonance frequencies of the -proton, the -carbon, the amide nitrogen, and the amide proton of a given amino acid residue in three dimensions. This experiment promises to be a valid alternative to 4D experiments, providing the same information on intraresidue polypeptide backbone connectivities in ¹³C-¹⁵N-double-labeled proteins.Abbreviations 3D, 4D three-dimensional, four-dimensional - TPPI time-proportional phase incrementation - ct constant-time - rf radiofrequency - NOE nuclear Overhauser enhancement - NOESY two-dimensional nuclear Overhauser enhancement spectroscopy - glutaredoxin(C14S) mutant E. coli glutaredoxin with the cysteine at position 14 replaced by serine     

Addressing the overlap problem in the quantitative analysis of two dimensional NMR spectra: Application to <Superscript>15</Superscript>N relaxation measurements

A quantitative analysis of 2D ¹H-¹⁵N spectra is often complicated by resonance overlap. Here a simple method is presented for resolving overlapped correlations by recording 2D projection planes from HNCO data sets. Applications are presented involving the measurement of ¹⁵N T₁ relaxation rates in a high molecular weight protein, malate synthase G, and in a system that exchanges between folded and unfolded states, the drkN SH3 domain. By supplementing relaxation data recorded in the conventional way as a series of 2D ¹H-¹⁵N data sets with a series of a pair of projection planes the number of dynamics probes is increased significantly for both systems studied.     

Structure and alignment of the membrane-associated peptaibols ampullosporin A and alamethicin by oriented 15N and 31P solid-state NMR spectroscopy

Ampullosporin A and alamethicin are two members of the peptaibol family of antimicrobial peptides. These compounds are produced by fungi and are characterized by a high content of hydrophobic amino acids, and in particular the α-tetrasubstituted amino acid residue α-aminoisobutyric acid. Here ampullosporin A and alamethicin were uniformly labeled with ¹⁵N, purified and reconstituted into oriented phophatidylcholine lipid bilayers and investigated by proton-decoupled ¹⁵N and ³¹P solid-state NMR spectroscopy. Whereas alamethicin (20 amino acid residues) adopts transmembrane alignments in 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) or 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) membranes the much shorter ampullosporin A (15 residues) exhibits comparable configurations only in thin membranes. In contrast the latter compound is oriented parallel to the membrane surface in 1,2-dimyristoleoyl-sn-glycero-3-phosphocholine and POPC bilayers indicating that hydrophobic mismatch has a decisive effect on the membrane topology of these peptides. Two-dimensional ¹⁵N chemical shift - ¹H-¹⁵N dipolar coupling solid-state NMR correlation spectroscopy suggests that in their transmembrane configuration both peptides adopt mixed α-/3₁₀-helical structures which can be explained by the restraints imposed by the membranes and the bulky α-aminoisobutyric acid residues. The ¹⁵N solid-state NMR spectra also provide detailed information on the helical tilt angles. The results are discussed with regard to the antimicrobial activities of the peptides.     

Direct measurement of 1H-1H dipolar couplings in proteins: A complement to traditional NOE measurements

An intensity-based constant-time COSY (CT-COSY) method is described for measuring ¹H-¹H residual dipolar couplings of proteins in weakly aligned media. For small proteins, the overall sensitivity of this experiment is comparable to the NOESY experiment. In cases where the ¹H-¹H distances are defined by secondary structure, such as ¹H-¹H^N and ¹H^N-¹H^N sequential distances in -helices and -sheets, these measurements provide useful orientational constraints for protein structure determination. This experiment can also be used to provide distance information similar to that obtained from NOE connectivities once the angular dependence is removed. Because the measurements are direct and non-coherent processes, such as spin diffusion, do not enter, the measurements can be more reliable. The 1/r ³ distance dependence of directly observed dipolar couplings, as compared with the 1/r ⁶ distance dependence of NOEs, also can provide longer range distance information at favorable angles. A simple 3D, ¹⁵N resolved version of the pulse sequence extends the method to provide the improved resolution required for application to larger biomolecules.     

Helix conformations in 7TM membrane proteins determined using oriented-sample solid-state NMR with multiple residue-specific 15N labeling

Oriented solid-state NMR in combination with multiple-residue-specific ¹⁵N labeling and extensive numerical spectral analysis is proposed to determine helix conformations of large membrane proteins in native membranes. The method is demonstrated on uniaxially oriented samples of ¹⁵N-methionine, -valine, and -glycine-labeled bacteriorhopsin in native purple membranes. Experimental two-dimensional ¹H-¹⁵N dipole-dipole coupling versus ¹⁵N chemical shift spectra for all samples are analyzed numerically to establish combined constraints on the orientation of the seven transmembrane helices relative to the membrane bilayer normal. Since the method does not depend on specific resonance assignments and proves robust toward nonidealities in the sample alignment, it may be generally feasible for the study of conformational arrangement and function-induced conformation changes of large integral membrane proteins.     

3D Triple-resonance NMR techniques for the sequential assignment of NH and 15N resonances in 15N- and 13C-labelled proteins

Summary Two new 3D ¹H-¹⁵N-¹³C triple-resonance experiments are presented which provide sequential cross peaks between the amide proton of one residue and the amide nitrogen of the preceding and succeeding residues or the amide proton of one residue and the amide proton of the preceding and succeeding residues, respectively. These experiments, which we term 3D-HN(CA)NNH and 3D-H(NCA)NNH, utilize an optimized magnetization transfer via the ²J_NC coupling to establish the sequential assignment of backbone NH and ¹⁵N resonances. In contrast to NH-NH connectivities observable in homonuclear NOESY spectra, the assignments from the 3D-H(NCA)NNH experiment are conformation independent to a first-order approximation. Thus the assignments obtained from these experiments can be used as either confirmation of assignments obtained from a conventional homonuclear approach or as an initial step in the analysis of backbone resonances according to Ikura et al. (1990) [Biochemistry, 29, 4659–4667]. Both techniques were applied to uniformly ¹⁵N- and ¹³C-labelled ribonuclease T1.