TROSY-based HNCO pulse sequences for the measurement of 1HN-15N, 15N-13CO, 1HN-13CO, 13CO-13Cα and 1HN-13Cα dipolar couplings in 15N, 13C, 2H-labeled proteins

HNCO-based 3D pulse schemes are presented for measuring ¹HN-¹⁵N,¹⁵N-¹³CO, ¹HN-¹³CO,¹³CO-¹³C and ¹HN-¹³C dipolar couplings in ¹⁵N,¹³C,²-labeled proteins. The experiments are based on recently developed TROSY methodology for improving spectral resolution and sensitivity. Data sets recorded on a complex of Val, Leu, Ile (1 only) methyl protonated ¹⁵N,¹³C,²H-labeled maltose binding protein and -cyclodextrin as well as ¹⁵N,¹³C,²H-labeled human carbonic anhydrase II demonstrate that precise dipolar couplings can be obtained on proteins in the 30–40 kDa molecular weight range. These couplings will serve as powerful restraints for obtaining global folds of highly deuterated proteins.     

Measurement of Scaled Residual Dipolar Couplings in Proteins Using Variable-angle Sample Spinning

NMR spectra of ubiquitin in the presence of bicelles at a concentration of 25% w/v have been recorded under sample spinning conditions for different angles of rotation. For an axis of rotation equal to the magic angle, the (1)H/(15)N HSQC recorded without any (1)H decoupling in the indirect dimension corresponds to the classical spectrum obtained on a protein in an isotropic solution and allows the measurement of scalar J-couplings (1) J (NH). For an angle of rotation smaller than the magic angle, the bicelles orient with their normal perpendicular to the spinning axis, whereas for an angle of rotation greater than the magic angle the bicelles orient with their normal along the spinning axis. This bicelle alignment creates anisotropic conditions that give rise to the observation of residual dipolar couplings in ubiquitin. The magnitude of these dipolar couplings depends directly on the angle that the rotor makes with the main magnetic field. By changing this angle in a controlled manner, residual dipolar couplings can be either scaled up or down thus offering the possibility to study simultaneously a wide range of dipolar couplings in the same sample.     

NMR Structural Studies of Domain 1 of Receptor-associated Protein

The 39 kDa receptor-associated protein (RAP) is an endoplasmic reticulum resident protein that binds tightly to the low-density lipoprotein receptor-related protein (LRP) as well as to other members of the low-density lipoprotein receptor superfamily. The association of RAP with LRP prevents this receptor from interacting with ligands. RAP is a three-domain protein that contains two independent LRP binding sites; one located within domains 1 and 2, and one located within domain 3. As the first step toward defining the structure of the full-length protein and understanding the interaction between RAP and this family of receptors, we have determined the 3D structure of domain 1 using constraints derived from heteronuclear multi-dimensional NMR spectra, including NOEs, dihedral angles, J-couplings and chemical shifts, as well as two sets of non-correlated residual dipolar couplings measured from the protein solutions in anisotropic media of Pf1 and 6% polyacrylamide gel. The backbone C(alpha) rmsd between the current structure and a homo-nuclear NOE-based structure is about 2 A. The large rmsd mainly reflects the significant differences in helical orientation and in the structural details of the long helix (helix 2) between the two structures.     

Using lanthanide ions to align troponin complexes in solution: order of lanthanide occupancy in cardiac troponin C

The potential for using paramagnetic lanthanide ions to partially align troponin C in solution as a tool for the structure determination of bound troponin I peptides has been investigated. A prerequisite for these studies is an understanding of the order of lanthanide ion occupancy in the metal binding sites of the protein. Two-dimensional [(1)H, (15)N] HSQC NMR spectroscopy has been used to examine the binding order of Ce(3+), Tb(3+), and Yb(3+) to both apo- and holo-forms of human cardiac troponin C (cTnC) and of Ce(3+) to holo-chicken skeletal troponin C (sTnC). The disappearance of cross-peak resonances in the HSQC spectrum was used to determine the order of occupation of the binding sites in both cTnC and sTnC by each lanthanide. For the lanthanides tested, the binding order follows that of the net charge of the binding site residues from most to least negative; the N-domain calcium binding sites are the first to be filled followed by the C-domain sites. Given this binding order for lanthanide ions, it was demonstrated that it is possible to create a cTnC species with one lanthanide in the N-domain site and two Ca(2+) ions in the C-domain binding sites. By using the species cTnC.Yb(3+).2 Ca(2+) it was possible to confer partial alignment on a bound human cardiac troponin I (cTnI) peptide. Residual dipolar couplings (RDCs) were measured for the resonances in the bound (15)N-labeled cTnI(129-148) by using two-dimensional [(1)H, (15)N] inphase antiphase (IPAP) NMR spectroscopy.     

Quantitative NMR studies of high molecular weight proteins: application to domain orientation and ligand binding in the 723 residue enzyme malate synthase G

A high-resolution multidimensional NMR study of ligand-binding to Escherichia coli malate synthase G (MSG), a 723-residue monomeric enzyme (81.4 kDa), is presented. MSG catalyzes the condensation of glyoxylate with an acetyl group of acetyl-CoA, producing malate, an intermediate in the citric-acid cycle. We show that despite the size of the protein, important structural and dynamic information about the molecule can be obtained on a per-residue basis. 15N-1HN residual dipolar couplings and carbonyl chemical shift changes upon alignment in Pf1 phage establish that there are no significant domain reorientations in the molecule upon ligand binding, in contrast to what was anticipated on the basis of both the X-ray structure of the glyoxylate-bound form of the enzyme and structural studies of a related set of proteins. The chemical shift changes of 1HN, 15N and 13CO nuclei upon binding of pyruvate, a glyoxylate-mimicking inhibitor, and acetyl-CoA have been mapped onto the three-dimensional structure of the molecule. Binding constants of pyruvate, glyoxylate, and acetyl-CoA (in the presence of pyruvate) have been measured, along with the kinetic parameters for glyoxylate and pyruvate binding. The on-rates of pyruvate and glyoxalate binding, approximately 1.2 x 10(6)M(-1)s(-1) and approximately 2.7 x 10(6)M(-1)s(-1), respectively, are significantly lower than what is anticipated from a simple diffusion-controlled process. Some structural implications of the chemical shift perturbations upon binding and the estimated ligand on-rates are discussed.     

Overcoming the problems associated with poor spectra quality of the protein kinase Byr2 using residual dipolar couplings

For the Ras-binding domain of the protein kinase Byr2, only a limited number of NOE contacts could be initially assigned unambiguously, as the quality of the NOESY spectra was too poor. However, the use of residual (1)H-(15)N dipolar couplings in the beginning of the structure determination process allows to overcome this problem. We used a three-step recipe for this procedure. A previously unknown structure could be calculated reasonably well with only a limited number of unambiguously assigned NOE contacts.     

Refined structure of a flexible heptasaccharide using 1H-13C and 1H-1H NMR residual dipolar couplings in concert with NOE and long range scalar coupling constants

The heptasaccharide isolated from the cell wall polysaccharide of Streptococcus mitis J22 serves as an important model for the dynamics and conformation of complex polysaccharides, illustrating the nature of flexibility with rigid epitopes joined by flexible hinges. One-bond C-H residual dipolar couplings (¹D_CH) and long-range H-H residual dipolar couplings (ⁿD_HH) were measured for the heptasaccharide in a cetylpyridinium chloride/hexanol/brine lamellar liquid crystal medium. A method is proposed to determine the ⁿD_HH in natural abundance based on a ¹³C resolved ¹H TOCSY pulse sequence previously published to determine the homonuclear scalar couplings. Different methods for interpretation of the ¹D_CH and the ⁿD_HH residual dipolar coupling data obtained were compared and combined with the NOE and long-range H,C and C,C scalar couplings available for this heptasaccharide. A flexible model of the heptasaccharide was determined in which two structurally well-defined regions involving four and two sugar residues, respectively are joined by a flexible hinge which involves two 16 glycosidic linkages.     

Structure and orientation of a G protein fragment in the receptor bound state from residual dipolar couplings

Residual dipolar couplings for a ligand that is in fast exchange between a free state and a state where it is bound to a macroscopically ordered membrane protein carry precise information on the structure and orientation of the bound ligand. The couplings originate in the bound state but can be detected on the free ligand using standard high resolution NMR. This approach is used to study an analog of the C-terminal undecapeptide of the alpha-subunit of the heterotrimeric G protein transducin when bound to photo-activated rhodopsin. Rhodopsin is the major constituent of disk-shaped membrane vesicles from rod outer segments of bovine retinas, which align spontaneously in the NMR magnet. Photo-activation of rhodopsin triggers transient binding of the peptide, resulting in measurable dipolar contributions to 1J(NH) and 1J(CH) splittings. These dipolar couplings report on the time-averaged orientation of bond vectors in the bound peptide relative to the magnetic field, i.e. relative to the membrane normal. Approximate distance restraints of the bound conformation were derived from transferred NOEs, as measured from the difference of NOESY spectra recorded prior to and after photo-activation. The N-terminal eight residues of the bound undecapeptide adopt a near-ideal alpha-helical conformation. The helix is terminated by an alpha(L) type C-cap, with Gly9 at the C' position in the center of the reverse turn. The angle between the helix axis and the membrane normal is 40 degrees (+/-4) degrees. Peptide protons that make close contact with the receptor are identified by analysis of the NOESY cross-relaxation pattern and include the hydrophobic C terminus of the peptide.     

Exact solutions for chemical bond orientations from residual dipolar couplings

New methods for determining chemical structures from residual dipolar couplings are presented. The fundamental dipolar coupling equation is converted to an elliptical equation in the principal alignment frame. This elliptical equation is then combined with other angular or dipolar coupling constraints to form simple polynomial equations that define discrete solutions for the unit vector(s). The methods are illustrated with residual dipolar coupling data on ubiquitin taken in a single anisotropic medium. The protein backbone is divided into its rigid groups (namely, its peptide planes and C frames), which may be solved for independently. A simple procedure for recombining these independent solutions results in backbone dihedral angles and that resemble those of the known native structure. Subsequent refinement of these - angles by the ROSETTA program produces a structure of ubiquitin that agrees with the known native structure to 1.1 Å C rmsd.     

Refinement of d(GCGAAGC) hairpin structure using one- and two-bond residual dipolar couplings

The structure of the ¹³C,¹⁵N-labeled d(GCGAAGC) hairpin, as determined by NMR spectroscopy and refined using molecular dynamics with NOE-derived distances, torsion angles, and residual dipolar couplings (RDCs), is presented. Although the studied molecule is of small size, it is demonstrated that the incorporation of diminutive RDCs can significantly improve local structure determination of regions undefined by the conventional restraints. Very good correlation between the experimental and back-calculated small one- and two-bond ¹H-¹³C, ¹H-¹⁵N, ¹³C-¹³C and ¹³C-¹⁵N coupling constants has been attained. The final structures clearly show typical features of the miniloop architecture. The structure is discussed in context of the extraordinary stability of the d(GCGAAGC) hairpin, which originates from a complex interplay between the aromatic base stacking and hydrogen bonding interactions.