The relative orientation of the fibronectin 6F11F2 module pair: A 15N NMR relaxation study

The structure of a pair of modules (⁶F1¹F2), that forms part of the collagen-binding region of fibronectin, is refined using heteronuclear relaxation data. A structure of the pair was previously derived from ¹H-¹H NOE and ³ J _HHN data [Bocquier et al. (1999) Structure, 7, 1451–1460] and a weak module–module interface, comprising Leu19 and Leu28, in ⁶F1, and Tyr68 in ²F1, was identified. In this study, the definition of the average relative orientation of the two modules is improved using the dependence of ¹⁵N relaxation on rotational diffusion anisotropy. This structure refinement is based on the selection of a subset of structures from sets calculated with NOE and ³ J _HHN data alone, using the quality of the fits to the relaxation data as the selection criterion. This simple approach is compared to a refinement strategy where ¹⁵N relaxation data are included in the force field as additional restraints [Tjandra et al. (1997) Nat. Struct. Biol., 4, 443–449].     

Backbone dynamics of a bacterially expressed peptide from the receptor binding domain of Pseudomonas aeruginosa pilin strain PAK from heteronuclear 1H-15N NMR spectroscopy

The backbone dynamics of a ¹⁵N-labeled recombinant PAK pilin peptide spanning residues 128–144 in the C-terminal receptor binding domain of Pseudomonas aeruginosa pilin protein strain PAK (Lys¹²⁸-Cys-Thr-Ser-Asp-Gln-Asp-Glu-Gln-Phe-Ile-Pro-Lys-Gly-Cys-Ser-Lys¹⁴⁴) were probed by measurements of ¹⁵N NMR relaxation. This PAK(128–144) sequence is a target for the design of a synthetic peptide vaccine effective against multiple strains of P. aeruginosa infection. The ¹⁵N longitudinal (T₁) and transverse (T₂) relaxation rates and the steady-state heteronuclear {¹H}-¹⁵N NOE were measured at three fields (7.04, 11.74 and 14.1 Tesla), five temperatures (5, 10, 15, 20, and 25°C ) and at pH 4.5 and 7.2. Relaxation data was analyzed using both the `model-free' formalism [Lipari, G. and Szabo, A. (1982) J. Am. Chem. Soc., 104, 4546–4559 and 4559–4570] and the reduced spectral density mapping approach [Farrow, N.A., Szabo, A., Torchia, D.A. and Kay, L.E. (1995) J. Biomol. NMR, 6, 153–162]. The relaxation data, spectral densities and order parameters suggest that the type I and type II -turns spanning residues Asp¹³⁴-Glu-Gln-Phe¹³⁷ and Pro¹³⁹-Lys-Gly-Cys¹⁴², respectively, are the most ordered and structured regions of the peptide. The biological implications of these results will be discussed in relation to the role that backbone motions play in PAK pilin peptide immunogenicity, and within the framework of developing a pilin peptide vaccine capable of conferring broad immunity across P. aeruginosa strains.     

Enhancement of the steady-state magnetization in TROSY experiments

Under the condition that the longitudinal relaxation time of spin I is shorter than the longitudinal relaxation time of spin S the steady-state magnetization in [S,I]-TROSY-type experiments can be enhanced by intermediate storage of a part of the steady-state magnetization of spin I on spin S with a pulse sequence element during the relaxation delay. It is demonstrated with samples ranging in size from the 1 kDa cyclosporin to the 110 kDa ¹⁵N,²H-labeled dihydroneopterin Aldolase that intermediate storage of steady-state magnetization in a [¹⁵N,¹H]-TROSY experiment yields a signal gain of 10–25%. The method proposed here for intermediate storage of steady-state magnetization can be implemented in any [¹⁵N,¹H]-TROSY-type experiments.     

The use of TROSY for detection and suppression of conformational exchange NMR line broadening in biological macromolecules

The interference between conformational exchange-induced time-dependent variations of chemical shifts in a pair of scalar coupled ¹H and ¹⁵N spins is used to construct novel TROSY-type NMR experiments to suppress NMR signal loss in [¹⁵N,¹H]-correlation spectra of a 14-mer DNA duplex free in solution and complexed with the Antp homeodomain. An analysis of double- and zero-quantum relaxation rates of base ¹H–¹⁵N moieties showed that for certain residues the contribution of conformational exchange-induced transverse relaxation might represent a dominant relaxation mechanism, which, in turn, can be effectively suppressed by TROSY. The use of the new TROSY method for exchange-induced transverse relaxation optimization is illustrated with two new experiments, 2D ^h1 J _HN,^h2 J _NN-quantitative [¹⁵N,¹H]-TROSY to measure ^h1 J _HN and ^h2 J _NN scalar coupling constants across hydrogen bonds in nucleic acids, and 2D (^h2 J _NN+^h1 J _NH)-correlation-[¹⁵N,¹H]-TROSY to correlate ¹H^N chemical shifts of bases with the chemical shifts of the tertiary ¹⁵N spins across hydrogen bonds using the sum of the trans-hydrogen bond coupling constants in nucleic acids.     

Backbone dynamics of ribonuclease T1 and its complex with 2′GMP studied by two-dimensional heteronuclear NMR spectroscopy

Summary The backbone dynamics of free ribonuclease T1 and its complex with the competitive inhibitor 2GMP have been studied by ¹⁵N longitudinal and transverse relaxation experiments, combined with {¹H, ¹⁵H} NOE measurements. The intensity decay of individual amide cross peaks in a series of (¹H, ¹⁵N)-HSQC spectra with appropriate relaxation periods (Kay, L.E. et al. (1989) Biochemistry, 28, 8972–8979; Kay, L.E. et al. (1992) J. Magn. Reson., 97, 359–375) was fitted to a single exponential by using a simplex algorithm in order to obtain ¹⁵N T₁ and T₂ relaxation times. These experimentally obtained values were analysed in terms of the model-free approach introduced by Lipari and Szabo (Lipari, G. and Szabo, A. (1982) J. Am. Chem. Soc., 104, 4546–4559; 4559–4570). The microdyramical parameters accessible by this approach clearly indicate a correlation between the structural flexibility and the tertiary structure of ribonuclease T1, as well as restricted mobility of certain regions of the protein backbone upon binding of the inhibitor. The results obtained by NMR are compared to X-ray crystallographic data and to observations made in molecular dynamics simulations.     

CPMG sequences with enhanced sensitivity to chemical exchange

Improved relaxation-compensated Carr–Purcell–Meiboom-Gill pulse sequences are reported for studying chemical exchange of backbone ¹⁵N nuclei. In contrast to the original methods [J. P. Loria, M. Rance, and A. G. Palmer, J. Am. Chem. Soc. 121, 2331–2332 (1999)], phenomenological relaxation rate constants obtained using the new sequences do not contain contributions from ¹H-¹H dipole-dipole interactions. Consequently, detection and quantification of chemical exchange processes are facilitated because the relaxation rate constant in the limit of fast pulsing can be obtained independently from conventional ¹⁵N spin relaxation measurements. The advantages of the experiments are demonstrated using basic pancreatic trypsin inhibitor.     

Doubly sensitivity-enhanced 3D TOCSY-HSQC

Summary Recently, strategies for double sensitivity enhancement in heteronuclear three-dimensional NMR experiments were introduced (Krishnamurthy, V.V. (1995) J. Magn. Reson., B106, 170–177; Sattler et al. (1995) J. Biomol. NMR, 6, 11–22; Sattler et al. (1995) J. Magn. Reson., B108, 235–242). Since a sensitivity enhancement of a factor 2^1/2 can be achieved for each indirect dimension, nD spectra can theoretically be enhanced up to a factor of 2^((n-1)/2). We propose and analyze a doubly enhanced three-dimensional TOCSY-HSQC sequence. The application of the doubly enhanced three-dimensional {¹⁵N, ¹H} TOCSY-HSQC sequence is shown for uniformly ¹³C-/¹⁵N- and ¹⁵N-labeled samples of the relatively large Azotobacter vinelandii flavodoxin II (179 amino acids). The main factors that contribute to the final signal-to-noise enhancement have been systematically investigated. The sensitivity enhancement obtained for the doubly enhanced TOCSY-HSQC pulse sequence as compared to the standard (unenhanced) version is close to the theoretically expected factor of two.     

Assignments of1H−15N magnetic resonances and identification of secondary structure elements of the λ-cro repressor

Summary The assignments of¹H–¹⁵N magnetic resonances of the -cro repressor are presented. Individual¹⁵N-amino acids were incorporated into the protein, or it was uniformly labeled with¹⁵N. For the¹³C–¹⁵N double-labeling experiments,¹³C-amino acids were incorporated into the uniformly¹⁵N-labeled protein. All the amide¹H–¹⁵N resonances could be assigned with such specific labeling, and sequential connectivities obtained by two-dimensional (2D)¹H–¹⁵N reverse correlation spectroscopies and three-dimensional (3D)¹H/¹⁵N NOESY-HMQC spectroscopy. Conventional 2D¹H–¹H correlation spectroscopies were applied to the assignment of the side-chain protons. Some of the¹H resonance assignments are inconsistent with those previously reported [Weber, P.L., Wemmer, D.E. and Reid, B.R. (1985)Biochemistry,24, 4553–4562]. The sequential NOE connectivities and H-D exchange rates indicate several elements of the secondary structure, including -helices consisting of residues 8–15, 19–25 and 28–37, and three extended strands consisting of residues 4–7, 39–45 and 49–55. Based on several long-range NOEs, the three extended strands could be combined to form an antiparallel -sheet. The amide proton resonances of the C-terminal residues except Ala⁶⁶ (residues 60–65) were hardly observed at neutral pH, indicating that the arm is flexible. The identified secondary structure elements in solution show good agreement with those in the crystal structure of the cro protein [Anderson, W.F., Ohlendorf, D.H., Takeda, Y. and Matthews, B.W. (1981)Nature,290, 754–758].     

The auto-orientation in high magnetic fields of oxidized cytochrome b562 as source of constraints for solution structure determination

¹⁵N-¹H ¹J couplings were measured at 500 MHz and 800 MHz for ¹⁵N enriched oxidized cytochrome b ₅₆₂ from E. coli. The magnetic field dependence of 70 ¹J values, which could be measured without signal overlap, shows that there is a molecular magnetic anisotropy which provides partial molecular orientation in the magnetic field and, consequently, residual dipolar couplings (rdc). The rdc were used as further constraints to improve the existing structure [Arnesano et al. (1999) Biochemistry, 38, 8657–8670] with a protocol which uses the rhombic anisotropy [Banci et al. (1998) J. Am. Chem. Soc., 120, 12903–12909]. The overall large molecular magnetic anisotropy has been found to be determined by both the low spin iron (III) and the four helix bundle structure magnetic susceptibility anisotropy contributions.     

Synthetic analogues of the histidine–chlorophyll complex: a NMR study to mimic structural features of the photosynthetic reaction center and the light-harvesting complex

Mg(II)–porphyrin–ligand and (bacterio)chlorophyl–ligand coordination interactions have been studied by solution and solid-state MAS NMR spectroscopy. ¹H, ¹³C and ¹⁵N coordination shifts due to ring currents, electronic perturbations and structural effects are resolved for imidazole (Im) and 1-methylimidazole (1-MeIm) coordinated axially to Mg(II)-OEP and (B)Chl a. As a consequence of a single axial coordination of Im or 1-MeIm to the Mg(II) ion, 0.9–5.2 ppm ¹H, 0.2–5.5 ppm ¹³C and 2.1–27.2 ppm ¹⁵N coordination shifts were measured for selectively labeled [1,3-¹⁵N]-Im, [1,3-¹⁵N,2-¹³C]-Im and [1,3-¹⁵N,1,2-¹³C]-1-MeIm. The coordination shifts depend on the distance of the nuclei to the porphyrin plane and the perturbation of the electronic structure. The signal intensities in the ¹H NMR spectrum reveal a five-coordinated complex, and the isotropic chemical shift analysis shows a close analogy with the electronic structure of the BChl a–histidine in natural light harvesting 2 complexes. The line broadening of the ligand responses support the complementary IR data and provide evidence for a dynamic coordination bond in the complex.Abbreviations (B)Chl a (bacterio)chlorophyll a - HMBC heteronuclear multiple bond correlation - Im imidazole - LH light-harvesting - 1-MeIm 1-methylimidazole - Mg(II)-Por Mg(II)-porphyrin macrocycle - OEP 2,3,7,8,12,13,17,18-octaethylporphyrin     

[15N,1H]/[13C,1H]-TROSY for simultaneous detection of backbone 15N–1H, aromatic 13C–1H and side-chain 15N–1H2 correlations in large proteins

This paper describes a [¹⁵N,¹H]/[¹³C,¹H]-TROSY experiment for the simultaneous acquisition of the heteronuclear chemical shift correlations of backbone amide ¹⁵N–¹H groups, side chain ¹⁵N–¹H₂ groups and aromatic ¹³C–¹H groups in otherwise highly deuterated proteins. The ¹⁵N–¹H and ¹³C–¹H correlations are extracted from two subspectra of the same data set, thus preventing possible spectral overlap of aromatic and amide protons in the ¹H dimension. The side-chain ¹⁵N–¹H₂ groups, which are suppressed in conventional [¹⁵N,¹H)-TROSY, are observed with high sensitivity in the ¹⁵N–¹H subspectrum. [¹⁵N,¹H]/[¹³C,¹H]-TROSY was used as the heteronuclear correlation block in a 3D [¹H,¹H]-NOESY-[¹⁵N,¹H]/[¹³C,¹H]-TROSY experiment with the membrane protein OmpA reconstituted in detergent micelles of molecular weight 80000 Da, which enabled the detection of numerous NOEs between backbone amide protons and both aromatic protons and side chain ¹⁵N–¹H₂ groups.     

A TROSY CPMG sequence for characterizing chemical exchange in large proteins

A new NMR spin relaxation experiment is described for measuring chemical exchange time constants from approximately 0.5 ms to 5 ms in ¹⁵N-labeled macromolecules. The pulse sequence is based on the Carr–Purcell–Meiboom–Gill technique [Carr and Purcell (1954) Phys. Rev., 94, 630–638; Meiboom and Gill (1958) Rev. Sci. Instrum., 29, 688–691; Loria et al. (1999) J. Am. Chem. Soc., 121, 2331–2332], but implements TROSY selection [Pervushin et al. (1997) Proc. Natl. Acad. Sci. USA, 94, 12366–12371] to permit measurement of exchange linebroadening contributions to the narrower component of the ¹H-¹⁵N scalar-coupled doublet. This modification extends the size limitation imposed on relaxation measurements due to the fast decay of transverse magnetization in larger macromolecules. The new TROSY-CPMG experiment is demonstrated on a [U-98% ¹⁵ N] labeled sample of basic pancreatic trypsin inhibitor and a [U-83% ²H, U-98% ¹⁵ N] labeled sample of triosephosphate isomerase, a 54 kDa homodimeric protein.     

Extending the range of amide proton relaxation dispersion experiments in proteins using a constant-time relaxation-compensated CPMG approach

Relaxation compensated constant-time Carr–Purcell–Meiboom–Gill relaxation dispersion experiments for amide protons are presented that detect s-ms time-scale dynamics of protein backbone amide sites. Because of their ten-fold larger magnetogyric ratio, much shorter 180° pulses can be applied to ¹H than to ¹⁵N spins; therefore, off-resonance effects are reduced and a wider range of effective rf fields can often be used in the case of ¹H experiments. Applications to [¹H-¹⁵N]-ubiquitin and [¹H-¹⁵N]-perdeuterated HIV-1 protease are discussed. In the case of ubiquitin, we present a pulse sequence that reduces artifacts that arise from homonuclear ³J(H_N-H) coupling. In the case of the protease, we show that relaxation dispersion of both ¹H and ¹⁵N spins provides a more comprehensive picture of slow backbone dynamics than does the relaxation dispersion of either spin alone. We also compare the relative merits of ¹H versus ¹⁵N transverse relaxation measurements and note the benefits of using a perdeuterated protein to measure the relaxation dispersion of both spin types.     

Pressure effect on the dynamics of an isolated α-helix studied by 15N-1H NMR relaxation

Dynamics and structure of (1–36)bacteriorhodopsin solubilized in chloroform/methanol mixture (1:1) were investigated by ¹H-¹⁵N NMR spectroscopy under a hydrostatic pressure of 2000 bar. It was shown that the peptide retains its spatial structure at high pressure. ¹⁵N transverse and longitudinal relaxation times, ¹⁵N{¹H} nuclear Overhauser effects, chemical shifts and the translation diffusion rate of the peptide at 2000 bar were compared with the respective data at ambient pressure [Orekhov et al. (1999) J. Biomol. NMR, 14, 345–356]. The model free analysis of the relaxation data for the helical 9–31 fragment revealed that the high pressure decreases the overall rotation and translation diffusion, as well as apparent order parameters of fast picosecond internal motions (S² _f) but has no effect on internal nanosecond motions (S² _s and _s) of the peptide. The decrease of translation and overall rotation diffusion was attributed to the increase in solvent viscosity and the decrease of apparent order parameters S² _f to a compression of hydrogen bonds. It is suggested that this compression causes an elongation of H-N bonds and a decrease of absolute values of chemical shift anisotropy (CSA). In particular, the observed decrease of S² _f at 2000 bar can be explained by 0.001 nm increase of N-H bond lengths and 10 ppm decrease of ¹⁵N CSA values.     

High-level 2H/13C/15N labeling of proteins for NMR studies

Summary The protein human carbonic anhydrase II (HCA II) has been isotopically labeled with ²H, ¹³C and ¹⁵N for high-resolution NMR assignment studies and pulse sequence development. To increase the sensitivity of several key ¹H/¹³C/¹⁵N triple-resonance correlation experiments, ²H has been incorporated into HCA II in order to decrease the rates of ¹³C and ¹H_N T₂ relaxation. NMR quantities of protein with essentially complete aliphatic ²H incorporation have been obtained by growth of E. coli in defined media containing D₂O, [1,2-¹³C₂, 99%] sodium acetate, and [¹⁵N, 99%] ammonium chloride. Complete aliphatic deuterium enrichment is optimal for ¹³C and ¹⁵N backbone NMR assignment studies, since the ¹³C and ¹H_N T₂ relaxation times and, therefore, sensitivity are maximized. In addition, complete aliphatic deuteration increases both resolution and sensitivity by eliminating the differential ²H isotopic shift observed for partially deuterated CH_nD_m moieties.     

Aliphatic 1H and 13C resonance assignments for the 26-10 antibody VL domain derived from heteronuclear multidimensional NMR spectroscopy

Summary Extensive ¹H and ¹³C assignments have been obtained for the aliphatic resonances of a uniformly ¹³C-and ¹⁵N-labeled recombinant V_L domain from the anti-digoxin antibody 26-10. Four-dimensional triple resonance NMR data acquired with the HNCAHA and HN(CO)CAHA pulse sequences [Kay et al. (1992) J. Magn. Reson., 98, 443–450] afforded assignments for the backbone H^N, N, H and C resonances. These data confirm and extend H^N, N and H assignments derived previously from three-dimensional ¹H-¹⁵N NMR studies of uniformly ¹⁵N-labeled V_L domain [Constantine et al. (1992), Biochemistry, 31, 5033–5043]. The identified H and C resonances provided a starting point for assigning the side-chain aliphatic ¹H and ¹³C resonances using three-dimensional HCCH-COSY and HCCH-TOCSY experiments [Clore et al. (1990), Biochemistry, 29, 8172–8184]. The C and C chemical shifts are correlated with the V_L domain secondary structure. The extensive set of side-chain assignments obtained will allow a detailed comparison to be made between the solution structure of the isolated V_L domain and the X-ray structure of the V_L domain within the 26–10 Fab.     

Manifestation of intramolecular motions on pico- and nanosecond time scales in 1H−15N NMR relaxation: Analysis of dynamic models of one- and two-helical subunits of bacterioopsin

Summary The influence of the internal dynamics of two polypeptides comprising transmembrane -helix A or two -helices A and B of bacterioopsin on experimentally accessible ¹⁵N NMR relaxation rates was investigated by molecular dynamics (MD) simulations, combined with more simple mechanic considerations. Model-free order parameters and correlation times of internal motions [Lipari, G. and Szabo, A. (1982) J. Am. Chem. Soc., 104, 4546–4559] were calculated for these models. It was found that both peptides exhibit two types of internal motions of the amide bonds, on the pico- and nanosecond time scales, affecting ¹⁵N NMR relaxation. The fast fluctuations are local and correspond to the librational motions of the individual N–H vectors in an effective potential of atoms of the surrounding matrix. In contrast, the motions on the nanosecond time scale imply concerted collective vibrations of a large number of atoms and could be represented as bending oscillation of -helices, strongly overdamped by the ambient solvent. A few other molecular mechanisms of slow internal motion were found, such as local distortions of the -helices (e.g., -aneurysm), delocalized distortions of the -helical backbone, as well as oscillations of the tilt angle between the axes of the -helices A and B. The results are compared with ¹⁵N NMR relaxation data measured for the (1–36)bacterioopsin and (1–71)bacterioopsin polypeptides in chloroform-methanol (1:1) and in SDS micelles [Orekhov, V.Yu., Pervushin, K.V. and Arseniev, A.S. (1994) Eur. J. Biochem., 219, 887–896].Abbreviations C2 baeterioopsin-(7–63)-peptide - sA bacterioopsin-(7–32)-peptide - CPMG Carr-Purcell-Meiboom-Gill - MD molecular dynamics - rmsd root-mean-square deviation     

Suppression of anti-TROSY lines in a sensitivity enhanced gradient selection TROSY scheme

A simple modification of the TROSY pulse transfer scheme, suggested by Yang and Kay [J. Biomol. NMR 13 (1999) 3–10], is proposed which results in the suppression of unwanted anti-TROSY lines without any extra loss in sensitivity. The higher sensitivity of this TROSY transfer scheme therefore becomes available for 2D [¹⁵N, ¹H] TROSY correlation and 3D/4D ¹⁵N separated NOESY type experiments where complete suppression of the broad anti-TROSY lines is essential.     

Dynamic aspects of extracellular loop region as a proton release pathway of bacteriorhodopsin studied by relaxation time measurements by solid state NMR

Local dynamics of interhelical loops in bacteriorhodopsin (bR), the extracellular BC, DE and FG, and cytoplasmic AB and CD loops, and helix B were determined on the basis of a variety of relaxation parameters for the resolved ¹³C and ¹⁵N signals of [1-¹³C]Tyr-, [¹⁵N]Pro- and [1-¹³C]Val-, [¹⁵N]Pro-labeled bR. Rotational echo double resonance (REDOR) filter experiments were used to assign [1-¹³C]Val-, [¹⁵N]Pro signals to the specific residues in bR. The previous assignments of [1-¹³C]Val-labeled peaks, 172.9 or 171.1 ppm, to Val69 were revised: the assignment of peak, 172.1 ppm, to Val69 was made in view of the additional information of conformation-dependent ¹⁵N chemical shifts of Pro bonded to Val in the presence of ¹³C-¹⁵N correlation, although no assignment of peak is feasible for ¹³C nuclei not bonded to Pro. ¹³C or ¹⁵N spin-lattice relaxation times (T₁), spin-spin relaxation times under the condition of CP-MAS (T₂), and cross relaxation times (T_CH and T_NH) for ¹³C and ¹⁵N nuclei and carbon or nitrogen-resolved, ¹H spin-lattice relaxation times in the rotating flame (¹H T_1ρ) for the assigned signals were measured in [1-¹³C]Val-, [¹⁵N]Pro-bR. It turned out that V69-P70 in the BC loop in the extracellular side has a rigid β-sheet in spite of longer loop and possesses large amplitude motions as revealed from ¹³C and ¹⁵N conformation-dependent chemical shifts and T₁, T₂, ¹H T_1ρ and cross relaxation times. In addition, breakage of the β-sheet structure in the BC loop was seen in bacterio-opsin (bO) in the absence of retinal.     

Clean SEA-HSQC: a method to map solvent exposed amides in large non-deuterated proteins with gradient-enhanced HSQC

The recent introduction of the SEA-TROSY experiment (Pellecchia et al. (2001) J. Am. Chem. Soc., 123, 4633–4634) can alleviate the problem of resonance overlap in ¹⁵N/²H labeled proteins. This method selectively observes solvent exposed amide protons with a SEA element. However, SEA-TROSY spectra may be contaminated with exchange-relayed NOE contributions from fast exchanging hydroxyl or amine protons and longitudinal relaxation contributions. Furthermore, for non-deuterated proteins or protein-ligand complexes, SEA-TROSY spectra may contain NOE contributions from aliphatic protons. In this communication, a modified version of the SEA element, a Clean SEA element, is introduced to eliminate these artifacts.