The measurement of relaxation rates of degenerate 1H transitions in methyl groups of proteins using acute angle radiofrequency pulses.

A simple NMR experiment for the measurement of transverse relaxation rates of degenerate 1H spins in 13CH3 methyl groups of deuterated proteins, is described. The experiment relies on the use of acute-angle 1H radio-frequency pulses, whereby a series of methyl 1H R2 decays is acquired with different values of the 1H pulse flip-angle, which modulates the relative contributions of the slow- and fast-relaxing components of 1H magnetization during the relaxation delay. These are subsequently analyzed simultaneously to extract the transverse relaxation rates of both components (RS and RF), along with the rate of cross-relaxation between these components, δ. The dipolar 1H-1H cross-correlated relaxation rate η = (RF - RS)/2 and the cross-relaxation rate δ, extracted from such acute-angle-pulse R2 decay series are compared with those derived from well-established methodology that uses relaxation-violated methyl 1H coherence transfer (so-called 'forbidden' experiments). Good agreement is achieved for the rates η derived from the two techniques, while slightly more accurate values of δ are obtained from analysis of acute-angle-pulse R2 series. Recording of acute-angle-pulse R2 series represents an attractive alternative to existing methodologies for quantifying methyl 1H relaxation and dynamics of the methyl three-fold symmetry axis in selectively [13CH3]-methyl-labeled, deuterated proteins - particularly so for very high-molecular-weight proteins, where the measurements of RF rates or the build-up of methyl 1H magnetization in relaxation-violated coherence transfer experiments, are problematic due to low sensitivity.

Transformation from an easy-plane to an easy-axis antiferromagnetic structure in the mixed rare-earth ferroborates Pr x Y1-x Fe3(BO3)4: magnetic properties and crystal field calculations.

The magnetic structure of the mixed rare-earth system Pr x Y1-x Fe3(BO3)4 (x = 0.75, 0.67, 0.55, 0.45, 0.25) was studied via magnetic and resonance measurements. These data evidence the successive spin reorientation from the easy-axis antiferromagnetic structure formed in PrFe3(BO3)4 to the easy-plane one of YFe3(BO3)4 associated with the weakening of the magnetic anisotropy of the Pr subsystem due to its diamagnetic dilution by nonmagnetic Y. This reorientation occurs through the formation of an inclined magnetic structure, as was confirmed by our previous neutron research in the range of x = 0.67 ÷ 0.45. In the compounds with x = 0.75 and 0.67 whose magnetic structure is close to the easy-axis one, a two-step spin reorientation takes place in the magnetic field H||c. Such a peculiarity is explained by the formation of an interjacent inclined magnetic structure with magnetic moments of Fe ions located closer to the basal plane than in the initial state, with these intermediate states remaining stable in some ranges of the magnetic field. An approach based on a crystal field model for the Pr(3+) ion and the molecular-field approximation is used to describe the magnetic characteristics of the system Pr x Y1-x Fe3(BO3)4. With the parameters of the d-d and f-d exchange interactions, of the magnetic anisotropy of the iron subsystem and of the crystal field parameters of praseodymium thus determined, it is possible to achieve a good agreement between the experimental and calculated temperature and field dependences of the magnetization curves (up to 90 kOe) and magnetic susceptibilities (2-300 K).

Magnetic phase diagram of the olivine-type Mn2GeO4 single crystal estimated from magnetic, resonance and thermodynamic properties.

Mn2GeO4 single crystals with the olivine structure grown by the modified flux method have been investigated. Pronounced magnetic phase transitions at T1 = 47.7 K, T2 = 17 K and T3 = 5.5 K, with T2 being dependent on an applied magnetic field, have been found. Based on the data of magnetic, resonance and temperature measurements, the entire phase diagram of Mn2GeO4 has been built. Mn2GeO4 is shown to be a material with a complex magnetic structure consisting of two magnetic subsystems.

A structural mode-coupling approach to 15N NMR relaxation in proteins.

The two-body Slowly Relaxing Local Structure (SRLS) model was applied to (15)N NMR spin relaxation in proteins and compared with the commonly used original and extended model-free (MF) approaches. In MF, the dynamic modes are assumed to be decoupled, local ordering at the N-H sites is represented by generalized order parameters, and internal motions are described by effective correlation times. SRLS accounts for dynamical coupling between the global diffusion of the protein and the internal motion of the N-H bond vector. The local ordering associated with the coupling potential and the internal N-H diffusion are tensors with orientations that may be tilted relative to the global diffusion and magnetic frames. SRLS generates spectral density functions that differ from the MF formulas. The MF spectral densities can be regarded as limiting cases of the SRLS spectral density. SRLS-based model-fitting and model-selection schemes similar to the currently used MF-based ones were devised, and a correspondence between analogous SRLS and model-free parameters was established. It was found that experimental NMR data are sensitive to the presence of mixed modes. Our results showed that MF can significantly overestimate order parameters and underestimate local motion correlation times in proteins. The extent of these digressions in the derived microdynamic parameters is estimated in the various parameter ranges, and correlated with the time scale separation between local and global motions. The SRLS-based analysis was tested extensively on (15)N relaxation data from several isotropically tumbling proteins. The results of SRLS-based fitting are illustrated with RNase H from E. coli, a protein extensively studied previously with MF.

Ligand-induced structural changes to maltodextrin-binding protein as studied by solution NMR spectroscopy.

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.

Backbone dynamics of escherichia coli adenylate kinase at the extreme stages of the catalytic cycle studied by (15)N NMR relaxation.

Adenylate kinase from Escherichia coli (AKeco), consisting of a single 23.6 kDa polypeptide chain folded into domains CORE, AMPbd, and LID, catalyzes the reaction AMP + ATP --> 2ADP. Domains LID and AMPbd execute large-scale movements during catalysis. Backbone dynamics of ligand-free and AP(5)A-inhibitor-bound AKeco were studied comparatively with (15)N NMR relaxation methods. Overall diffusion with correlation times of 15.05 (11.42) ns and anisotropy D(parallel)/D(perp) = 1.25 (1.10), and fast internal motions with correlation times up to 100 ps (50 ps), were determined for AKeco (AKecoAP(5)A). Fast internal motions affect 93% of the AKeco sites, with pronounced preference for domains AMPbd and LID, and 47% of the AKecoAP(5)A sites, with limited variability along the chain. The mean squared generalized order parameters, , of secondary structure elements and loops are affected by ligand binding differentially and in a domain-specific manner. Nanosecond motions predominate within AMPbd. Prominent exchange contributions, associated in particular with residue G10 of the nucleotide-binding P-loop motif, are interpreted to reflect hydrogen-bond dynamics at the inhibitor-binding site. The hypothesis of energetic counter balancing of substrate binding based on crystallographic data is strongly supported by the solution NMR results. Correlations between backbone dynamics and domain displacement are established.

Probing hydrogen bonds in the antibody-bound HIV-1 gp120 V3 loop by solid state NMR REDOR measurements.

We describe solid state NMR measurements on frozen solutions of the complex of the 24-residue HIV-1 gp120 V3 loop peptide RP135 with the Fab fragment of the anti-gp120 antibody 0.5beta, using rotational echo double resonance (REDOR). In order to probe possible hydrogen bonding between arginine side chains and glycine backbone carbonyls in the region of the conserved Gly-Pro-Gly-Arg (GPGR) motif of the V3 loop, RP135 samples were prepared with 15N labels at the eta nitrogen positions of arginine side chains and 13C labels at glycine carbonyl positions and 13C-detected 13C-15N REDOR measurements were performed on peptide/antibody complexes of these labeled samples. Such hydrogen bonding was previously observed in a crystal structure of the V3 loop peptide/antibody complex RP142/59.1 [Ghiara et al. (1994) Science, 264, 82-85], but is shown by the REDOR measurements to be absent in the RP135/0.5beta complex. These results confirm the antibody-dependent conformational differences in the GPGR motif suggested by previously reported solid state NMR measurements of phi and psi backbone dihedral angles in the RP135/0.53 complex. In addition, we describe REDOR measurements on the helical synthetic peptide MB(i+4)EK in frozen solution that establish our ability to detect 13C-15N dipole-dipole couplings in the distance range appropriate to these hydrogen bonding studies. We also report the results of molecular modeling calculations on the central portion RP135, using a combination of the solid state NMR restraints of Weliky et al. [Nat. Struct. Biol., 6, 141-145, 1999] and the liquid state NMR restraints of Tugarinov et al. (Nat. Struct. Biol., 6, 331-335, 1999]. The dynamics calculations demonstrate the mutual compatibility of the two sets of experimental structural restraints and reduce ambiguities in the solid state NMR restraints that result from symmetry and signal-to-noise considerations.

NMR structure of an anti-gp120 antibody complex with a V3 peptide reveals a surface important for co-receptor binding.

BACKGROUND: The protein 0.5beta is a potent strain-specific human immunodeficiency virus type 1 (HIV-1) neutralizing antibody raised against the entire envelope glycoprotein (gp120) of the HIV-1(IIIB) strain. The epitope recognized by 0.5beta is located within the third hypervariable region (V3) of gp120. Recently, several HIV-1 V3 residues involved in co-receptor utilization and selection were identified. RESULTS: Virtually complete sidechain assignment of the variable fragment (Fv) of 0.5beta in complex with the V3(IIIB) peptide P1053 (RKSIRIQRGPGRAFVTIG, in single-letter amino acid code) was accomplished and the combining site structure of 0.5beta Fv complexed with P1053 was solved using multidimensional nuclear magnetic resonance (NMR). Five of the six complementarity determining regions (CDRs) of the antibody adopt standard canonical conformations, whereas CDR3 of the heavy chain assumes an unexpected fold. The epitope recognized by 0.5beta encompasses 14 of the 18 P1053 residues. The bound peptide assumes a beta-hairpin conformation with a QRGPGR loop located at the very center of the binding pocket. The Fv and peptide surface areas buried upon binding are 601 A and 743 A(2), respectively, in the 0.5beta Fv-P1053 mean structure. The surface of P1053 interacting with the antibody is more extensive and the V3 peptide orientation in the binding site is significantly different compared with those derived from the crystal structures of a V3 peptide of the HIV-1 MN strain (V3(MN)) complexed to three different anti-peptide antibodies. CONCLUSIONS: The surface of P1053 that is in contact with the anti-protein antibody 0.5beta is likely to correspond to a solvent-exposed region in the native gp120 molecule. Some residues of this region of gp120 are involved in co-receptor binding, and in discrimination between different chemokine receptors utilized by the protein. Several highly variable residues in the V3 loop limit the specificity of the 0.5beta antibody, helping the virus to escape from the immune system. The highly conserved GPG sequence might have a role in maintaining the beta-hairpin conformation of the V3 loop despite insertions, deletions and mutations in the flanking regions.

A model of a gp120 V3 peptide in complex with an HIV-neutralizing antibody based on NMR and mutant cycle-derived constraints.

The 0.5beta monoclonal antibody is a very potent strain-specific HIV-neutralizing antibody raised against gp120, the envelope glycoprotein of HIV-1. This antibody recognizes the V3 loop of gp120, which is a major neutralizing determinant of the virus. The antibody-peptide interactions, involving aromatic and negatively charged residues of the antibody 0.5beta, were studied by NMR and double-mutant cycles. A deuterated V3 peptide and a Fab containing deuterated aromatic amino acids were used to assign these interactions to specific V3 residues and to the amino acid type and specific chain of the antibody by NOE difference spectroscopy. Electrostatic interactions between negatively charged residues of the antibody Fv and peptide residues were studied by mutagenesis of both antibody and peptide residues and double-mutant cycles. Several interactions could be assigned unambiguously: F96(L) of the antibody interacts with Pro13 of the peptide, H52(H) interacts with Ile7, Ile9 and Gln10 and D56(H) interacts with Arg11. The interactions of the light-chain tyrosines with Pro13 and Gly14 could be assigned to either Y30a(L) and Y32(L), respectively, or Y32(L) and Y49(L), respectively. Three heavy-chain tyrosines interact with Ile7, Ile20 and Phe17. Several combinations of assignments involving Y32(H), Y53(H), Y96(H) and Y100a(H) may satisfy the NMR and mutagenesis constraints, and therefore at this stage the interactions of the heavy-chain tyrosines were not taken into account. The unambiguous assignments [F96(L), H52(H) and D56(H)] and the two possible assignments of the light-chain tyrosines were used to dock the peptide into the antibody-combining site. The peptide converges to a unique position within the binding site, with the RGPG loop pointing into the center of the groove formed by the antibody complementary determining regions while retaining the beta-hairpin conformation and the type-VI RGPG turn [Tugarinov, V., Zvi, A., Levy, R. & Anglister, J. (1999) Nat. Struct. Biol. 6, 331-335].

Solution Structure of an Antibody-Bound HIV-1(IIIB) V3 Peptide: A Cis Proline Turn Linking Two ß-hairpin Strands.

Abstract The refined solution structure of a peptide representing the full epitope of the HIV-1(IIIB) V3 loop in complex with the anti-gp120 antibody Fv fragment was determined using isotope-filtered and isotope-edited NMR. Both the (15)N-labeled peptide in complex with the unlabeled Fv and the unlabeled peptide complexed with the uniformly (15)N,(13)C-labeled Fv were investigated. The backbone of the bound peptide adopts a well defined ß-hairpin conformation with two twisted anti-parallel ß-strands linked by a type VI tight turn comprising residues RGPG. The central glycine and proline residues of the turn are linked by a cis peptide bond. (15)N{(1)H} NOE measurements demonstrated that the backbone of the bound peptide including the central QRGPGR loop is well ordered in the bound state. The V3 loop peptide solution structure is significantly different from the peptide conformation in the X-ray structures of three anti-peptide antibody/V3(MN) peptide complexes. These differences seem to be dictated by the antibody dependence and HIV strain-specificity of the V3 peptide fold.

A cis proline turn linking two beta-hairpin strands in the solution structure of an antibody-bound HIV-1IIIB V3 peptide.

The refined solution structure of an 18-residue HIV-1IIIB V3 peptide in complex with the Fv fragment of an anti-gp120 antibody reveals an unexpected type VI beta-turn comprising residues RGPG at the center of a beta-hairpin. The central glycine and proline of this turn are linked by a cis peptide bond. The residues of the turn interact extensively with the antibody Fv. 15N[1H] NOE measurements show that the backbone of the peptide, including the central QRGPGR loop, is well ordered in the complex. The solution structure is significantly different from the X-ray structures of HIV-1MN V3 peptides bound to anti-peptide antibodies. These differences could be due to a two-residue (QR) insertion preceding the GPGR sequence in the HIV-1IIIB strain, and the much longer peptide epitope immobilized by the anti-gp120 antibody.

Solution structures of a highly insecticidal recombinant scorpion alpha-toxin and a mutant with increased activity.

The solution structure of a recombinant active alpha-neurotoxin from Leiurus quinquestriatus hebraeus, Lqh(alpha)IT, was determined by proton two-dimensional nuclear magnetic resonance spectroscopy (2D NMR). This toxin is the most insecticidal among scorpion alpha-neurotoxins and, therefore, serves as a model for clarifying the structural basis for their biological activity and selective toxicity. A set of 29 structures was generated without constraint violations exceeding 0.4 A. These structures had root mean square deviations of 0.49 and 1.00 A with respect to the average structure for backbone atoms and all heavy atoms, respectively. Similarly to other scorpion toxins, the structure of Lqh(alpha)IT consists of an alpha-helix, a three-strand antiparallel beta-sheet, three type I tight turns, a five-residue turn, and a hydrophobic patch that includes tyrosine and tryptophan rings in a "herringbone" arrangement. Positive phi angles were found for Ala50 and Asn11, suggesting their proximity to functionally important regions of the molecule. The sample exhibited conformational heterogeneity over a wide range of experimental conditions, and two conformations were observed for the majority of protein residues. The ratio between these conformations was temperature-dependent, and the rate of their interconversions was estimated to be on the order of 1-5 s(-1) at 308 K. The conformation of the polypeptide backbone of Lqh(alpha)IT is very similar to that of the most active antimammalian scorpion alpha-toxin, AaHII, from Androctonus australis Hector (60% amino acid sequence homology). Yet, several important differences were observed at the 5-residue turn comprising residues Lys8-Cys12, the C-terminal segment, and the mutual disposition of these two regions. 2D NMR studies of the R64H mutant, which is 3 times more toxic than the unmodified Lqh(alpha)IT, demonstrated the importance of the spatial orientation of the last residue side chain for toxicity of Lqh(alpha)IT.

[Spectroscopic study of "hole burning" of the initial photoprocesses in photosystem I of mutant strain Chlamydomonas reinhardii 516-3a enriched with P700 reaction centers]. / Issledovanie metodom spektroskopii "vyzhiganiia provalov" pervichnykh fotoprotsessov v fotosisteme 1 mutantnogo shtamma Chlamydomonas reinhardii 516-3a, obogashchennogo reaktsionnymi tsentrami P700.

The effect of "hole burning" in absorption spectrum upon monochromatic illumination at 4.2 degrees K has been investigated on the Chlamydomonas reinhardii mutant strain 516-3a which possesses the chlorophyll a/P700 ratio of about 25. This effect has been earlier discovered for the wild type strain of Chlorella. In the strain 516-3a two types of holes differing in width and in shape have been observed. For their assignment the maximal (saturated) holewidth has been studied as a function of the burning wavelength. It has been shown that for the holes of one type photooxidation of P700 is responsible. The other type of holes is caused by electrochromic transition shift of another component of the reaction centre with the absorption maximum at 693 nm. Using measured holewidths it has been estimated that the lifetime of P700 excited state is not less than 50 ps and that the excited state lifetime of the component responsible for the other type of holes is 8.6 ps. The latter, in assumption that it is limited by energy transfer between two components under consideration, gives a distance of 20 A between them. Possible reasons of disagreement between obtained P700* lifetime and considerably shorter times attributed earlier to the primary electron phototransfer in photosystem I on the basis of picosecond studies are discussed.

["Burning" of troughs in the low-temperature absorption spectra of a strain of Chlamydomonas reinhardii enriched by P700]. / Vyzhiganie provalov v nizkotemperaturnykh spektrakh pogloshcheniia shtamma Chlamydomonas reinhardii, imeiushchego obogashchenie po P700.

Spectral and photochemical parameters were described of the mutant strain of Chlamydomonas reinhardii 516--3a, in which the ratio chlorophyll a/P700 is about 20. Experiments were carried out with this strain for investigating earlier observed for Chlorella effect of burning out of deeps in absorption spectra at 4.2K resulting from irradiation with monochromatic light of the wavelength 698 nm. Arguments are presented in favour of the assumption that phototransformation of P700 is responsible for the formation of deeps. It has been found from the width of the deeps that the lifetime of the excited states of the centres responsible for the formation of deeps is between 16 ps and 65 ps.