A general enhancement scheme in heteronuclear multidimensional NMR employing pulsed field gradients

Summary General pulse sequence elements that achieve sensitivity-enhanced coherence transfer from a heteronucleus to protons of arbitrary multiplicity are introduced. The building blocks are derived from the sensitivity-enhancement scheme introduced by Cavanagh et al. ((1991) J. Magn. Reson., 91, 429–436), which was used in conjunction with gradient coherence selection by Kay et al. ((1992) J. Am. Chem. Soc., 114, 10663–10665), as well as from a multiple-pulse sequence effecting a heteronuclear planar coupling Hamiltonian. The building blocks are incorporated into heteronuclear correlation experiments, in conjunction with coherence selection by the formation of a heteronuclear gradient echo. This allows for efficient water suppression without the need for water presaturation. The methods are demonstrated in HSQC-type experiments on a sample of a decapeptide in H₂O. The novel pulse sequence elements can be incorporated into multidimensional experiments.     

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.     

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.     

Two- and three-dimensional 31P-driven NMR procedures for complete assignment of backbone resonances in oligodeoxyribonucleotides

Summary We describe a strategy for sequential assignment of ³¹P and deoxyribose ¹H NMR resonances in oligodeoxyribonucleotides. The approach is based on ³¹P–¹H J-cross-polarization (hetero TOCSY) experiments, recently demonstrated for the assignment of resonances in RNA [Kellogg, G.W. (1992) J. Magn. Reson., 98, 176; Kellogg, G.W. et al. (1992) J. Am. Chem. Soc., 114, 2727]. Two-dimensional hetero TOCSY and hetero TOCSY-NOESY experiments are used to connect proton spin systems from adjacent nucleotides in the dodecamer d(CGCGAATTCGCG)₂ entirely on the basis of through-bond scalar connectivities. All phosphorus resonances of the dodecamer are assigned by this method, and many deoxyribose ¹H resonances can be assigned as well. A new three-dimensional hetero TOCSY-NOESY experiment is used for backbone proton 4, 5 and 5 resonance assignments, completing assignments begun on this molecule in 1983 [Hare, D.R. et al. (1983) J. Mol. Biol., 171, 319]. Numerical simulations of the time dependence of coherence transfer aid in the interpretation of hetero TOCSY spectra of oligonucleotides and address the dependence of hetero TOCSY and related spectra on structural features of nucleic acids. The possibility of a generalized backbone-driven ¹H and ³¹P resonance-assignment strategy for oligonucleotides is discussed.To whom correspondence should be addressed.     

Mapping of the spectral density function of a Cα−Hα bond vector from NMR relaxation rates of a 13C-labelled α-carbon in motilin

Summary The peptide hormone motilin was synthesised with a ¹³C-enriched -carbon in the leucine at position 10. In aqueous solution, six different relaxation rates were measured for the ¹³C–H fragment as a function of temperature and with and without the addition of 30% (v/v) of the cosolvent d ₂-1,1,1,3,3,3-hexafluoro-2-propanol (HFP). The relaxation rates were analysed employing the spectral density mapping technique introduced by Peng and Wagner [(1992) J. Magn. Reson., 98, 308–322] and using the model-free approach by Lipari and Szabo [(1982) J. Am. Chem. Soc., 104, 4546–4570]. The fit to various models of dynamics was also considered. Different procedures to evaluate the overall rotational correlation time were compared. A single exponential time correlation function was found to give a good fit to the measured spectral densities only for motilin in 30% (v/v) HFP at low temperatures, whereas at high temperatures in this solvent, and in D₂O at all temperatures, none of the considered models gave an acceptable fit. A new empirical spectral density function was tested and found to accurately fit the experimental spectral density mapping points. The application of spectral density mapping based on NMR relaxation data for specific ¹³C–¹H vector is shown to be a highly useful method to study biomolecular dynamics. Advantages are high sensitivity, high precision and uniform sampling of the spectral density function over the frequency range.Abbreviations CD circular dichroism - NOE nuclear Overhauser enhancement - NOESY two-dimensional NOE spectroscopy - INEPT insensitive nuclei enhanced by polarisation transfer - DANTE delays alternating with nutations for tailored excitation - WALTZ-16 wideband, alternating phase, low-power technique for zero residual splitting - FID Free induction decay - ppm parts per million - TSPA 3-trimethylsilyl-(3,3,2,2-d)-propionic acid - HFP d ₂-1,1,1,3,3,3-hexafluoro-2-propanol - CPMG Carr-Purcell-Meiboom-Gill - TFD time-resolved fluorescence depolarisation - CSA chemical shift anisotropy Partly presented at the symposium Dynamics and Function of Biomolecules, Szeged, Hungary, July 31–August 2, 1993.     

A new 3D HN(CA)HA experiment for obtaining fingerprint HN-Hα cross peaks in15N- and13C-labeled proteins

Summary A new 3D¹H–¹⁵N–¹³C triple resonance experiment is presented that provides in-phase absorptive cross peaks between amide protons and -protons of the same and the sequentially preceding residue. The experiment yields similar connectivities as those described previously by Montelione and Wagner (1990a) [J. Magn. Reson.,87, 183–188] and Kay et al. (1991) [J. Magn. Reson.,91, 84–92]. However, the pulse sequence was designed to minimize the time that transverse coherence of the¹³C nucleus is present, since this nucleus has the shortest transverse relaxation time of all the nuclei involved in these experiments. This is achieved by using a coherence transfer pathway from¹H^N to¹⁵N,¹³C,¹H and back to the¹H^N. In the sequence described, transverse¹³C coherence is present only for a length of ca. I¹J(C-H). This reduces loss of signal due to transverse relaxation. We tested the technique on uniformly¹⁵N- and¹³C-enriched T4 lysozyme.     

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.     

Accurate measurement of <Superscript>15</Superscript>N–<Superscript>13</Superscript>C residual dipolar couplings in nucleic acids

New 3D HCN quantitative J (QJ) pulse schemes are presented for the precise and accurate measurement of one-bond ¹⁵N_1/9–¹³C₁, ¹⁵N_1/9–¹³C_6/8, and ¹⁵N_1/9–¹³C_2/4 residual dipolar couplings (RDCs) in weakly aligned nucleic acids. The methods employ ¹H–¹³C multiple quantum (MQ) coherence or TROSY-type pulse sequences for optimal resolution and sensitivity. RDCs are obtained from the intensity ratio of H₁–C₁–N_1/9 (MQ-HCN-QJ) or H_6/8–C_6/8–N_1/9 (TROSY-HCN-QJ) correlations in two interleaved 3D NMR spectra, with dephasing intervals of zero (reference spectrum) and 1/(2J_NC) (attenuated spectrum). The different types of ¹⁵N–¹³C couplings can be obtained by using either the 3D MQ-HCN-QJ or TROSY-HCN-QJ pulse scheme, with the appropriate setting of the duration of the constant-time ¹⁵N evolution period and the offset of two frequency-selective ¹³C pulses. The methods are demonstrated for a uniformly ¹³C, ¹⁵N-enriched 24-nucleotide stem-loop RNA sequence, helix-35, aligned in the magnetic field using phage Pf1. For measurements of RDCs systematic errors are found to be negligible, and experiments performed on a 1.5 mM helix-35 sample result in an estimated precision of ca. 0.07 Hz for ¹D_NC, indicating the utility of the measured RDCs in structure validation and refinement. Indeed, for a complete set of ¹⁵N_1/9–¹³C₁, ¹⁵N_1/9–¹³C_6/8, and ¹⁵N_1/9–¹³C_2/4 dipolar couplings obtained for the stem nucleotides, the measured RDCs are in excellent agreement with those predicted for an NMR structure of helix-35, refined using independently measured observables, including ¹³C–¹H, ¹³C–¹³C and ¹H–¹H dipolar couplings.Supplementary material to this paper is available in electronic form at http://dx.doi.org/10.1007/s10858-005-0646-2.     

Off-resonance R1rho relaxation outside of the fast exchange limit: an experimental study of a cavity mutant of T4 lysozyme

An ¹⁵N off-resonance R ₁ spin relaxation study of an L99A point mutant of T4 lysozyme is presented. Previous CPMG-based relaxation dispersion studies of exchange in this protein have established that the molecule interconverts between a populated ground state and an excited state (3.4%) with an exchange rate constant of 1450 s^–1 at 25°C. It is shown that for the majority of residues in this protein the offset dependence of the R ₁ relaxation rates cannot be well fit using models which are only valid in the fast exchange regime. In contrast, a recently derived expression by Trott and Palmer (J. Magn. Reson., 154, 157–160, 2002) which is valid over a wider window of exchange than other relations, is shown to fit the data well. Values of (signed) chemical shift differences between exchanging sites have been extracted and are in reasonable agreement with shift differences measured using CPMG methods. A set of simulations is presented which help establish the exchange regimes that are best suited to analysis by off-resonance R ₁ techniques.     

Phase labeling of C−H and C−C spin-system topologies: Application in PFG-HACANH and PFG-HACA(CO)NH triple-resonance experiments for determining backbone resonance assignments in proteins

Summary Triple-resonance experiments can be designed to provide useful information on spin-system topologies. In this paper we demonstrate optimized proton and carbon versions of PFG-CT-HACANH and PFG-CT-HACA(CO)NH straight-through triple-resonance experiments that allow rapid and almost complete assignments of backbone H, ¹³C, ¹⁵N and H^N resonances in small proteins. This work provides a practical guide to using these experiments for determining resonance assignments in proteins, and for identifying both intraresidue and sequential connections involving glycine residues. Two types of delay tunings within these pulse sequences provide phase discrimination of backbone Gly C and H resonances: (i) C–H phase discrimination by tuning of the refocusing period _{a_f}; (ii) C–C phase discrimination by tuning of the ¹³C constant-time evolution period 2T_c. For small proteins, C–C phase tuning provides better S/N ratios in PFG-CT-HACANH experiments while C–H phase tuning provides better S/N ratios in PFG-CT-HACA(CO)NH. These same principles can also be applied to triple-resonance experiments utilizing ¹³C-¹³C COSY and TOCSY transfer from peripheral side-chain atoms with detection of backbone amide protons for classification of side-chain spin-system topologies. Such data are valuable in algorithms for automated analysis of resonance assignments in proteins.     

Solution structure of a synthetic peptide corresponding to a receptor binding region of FSH (hFSH-beta 33-53).

The receptor binding surface of human follicle-stimulating hormone (hFSH) is mimicked by synthetic peptides corresponding to the hFSH- chain amino acid sequences 33–53 [Santa-Coloma, T. A., Dattatreyamurty, D., and Reichert, L. E., Jr. (1990),Biochemistry 29, 1194–1200], 81–95 [Santa-Coloma, T. A., and Reichert, L. E., Jr. (1990),J. Biol. Chem. 265, 5037–5042], and the combined sequence (33–53)–(81–95) [Santa-Coloma, T. A., Crabb, J. W., and Reichert, L. E., Jr. (1991),Mol. Cell. Endocrinol. 78, 197–204]. These peptides have been shown to inhibit binding of hFSH to its receptor. Circular dichroism (CD) and nuclear magnetic resonance (NMR) spectroscopy were used to determine the structure of the first peptide in this series, the 21 amino acid peptide hFSH--(33–53), H₂N-YTRDLVYKDPARPKIQKTCTF-COOH. Analysis of CD data indicated the presence of approximately equal amounts of antiparallel -pleated sheet, turns including a -turn, other structures, and a small amount ofa-helix. The major characteristics of the structure were found to be relatively stable at acidicpH and the predominant effect of increased solvent polarity was a small increase ina-helical content. One- and two-dimensional NMR techniques were used to obtain full proton and carbon signal assignments in aqueous solution atpH 3.1. Analysis of NMR results confirmed the presence of the structural features revealed by CD analysis and provided a detailed picture of the secondary structural elements and global folding pattern in hFSH--(33–53). These features included an antiparallel -sheet (residues 38–51 and 46–48), turns within residues 41–46, and 50–52 (a -turn) and a small N-terminal helical region comprised of amino acids 34–36. One of the turns is facilitated by prolines 42 and 45. Proline-45 was constrained to thetrans conformation, whereas proline-42 favored thetrans conformer (70%) over thecis (30%). Two resonances were observed for the single alanine residue (A-43) sequentially proximal to P-42, but the rest of the structure was minimally affected by the isomerization at proline-42. The major population of molecules, containingtrans-42 andtrans-45 prolines, presented 120 NOEs. Distance geometry calculations with 140 distance constraints and energy minimization refinements were used to derive a moderately well-defined model of the peptide's structure. The hFSH--(33–53) structure has a highly polar surface composed of six cationic amino acid (arginie-35, lysine-40, arginine-44, lysine-46, glutamine-48, and lysine-49) and two anionic residues (aspartate-36 and aspartic acid-41). A hydrophobic region in the structure is composed of residues in the antiparallel -sheet and -turn which fold to produce a distorted hairpin. The structure of this domain, together with the protruding and positively charged region in the vicinity of residues 42–45, may mimic the surface of hFSH that binds to the receptor.Abreviations used: hFSH, human follicle-stimulating hormone; PB, 25 mM Na₂KPO₄, 25 mM KH₂PO₄, and 5 mM Mg Cl₂; CD, circular dichroism spectrapolarimetry; NMR, nuclear magnetic resonance spectrometry; COSY, homonuclear correlated spectroscopy; NOESY, 2D nuclear Overhauser effect spectroscopy; HOHAHA, homonuclear Hartman-Han coherence transfer; HMQCHY, reverse-detected heteronuclear multiple shift correlation, one bond; HMBC, reverse-detected heteronuclear multiple bond correlation; S/N, signal to noise ratio; TFE, trifluoroethanol.Dr. Santa-Coloma is on leave of absence from the National Research Council of Argentina (CONICET).     

Preferred conformations and dynamics of five core structures of mucin typeO-glycans determined by NMR spectroscopy and force field calculations

Glycosyltransferases acting onO-glycans have been shown to exhibit distinct specificity for the carbohydrate and the peptide moiety of their substrates. As an approach to study the 3-dimensional interactions between enzymes andO-glycan substrates, we determined the preferred conformations of five oligosaccharide-core structures of mucin type glycoproteins by NMR spectroscopy and by static and dynamic force field calculations. Seven oligosaccharides, representing five basic core structures, were investigated: Gal(1–3)GalNAcBzl (1, core 1), GlcNAc(1–6)[Gal(1–3)]GalNAcBzl (2, core 2), GlcNAc(1–3)GalNacBzl (3, core 3), GlcNAc(1–6)[GlcNAc(1–3)]GalNAcBzl (4, core 4), GlcNAc(1–6)GalNAcBzl (5, core 6), the elongated core 2, Gal(1–4)GlcNAc(1–6)[Gal(1–3)]GalNAcpNp (6) and GalNAc-Bzl (7). The dynamic behaviour of the molecules was studied by Metropolis Monte Carlo (MMC) simulations. Experimental coupling constants, chemical shift changes, and NOEs were compared with results from static energy minimizations and dynamic MMC simulations and show a good agreement. MMC simulations show that the (1–6) linkage is much more flexible than the (1–3) or the (1–4) linkages. The preferred conformations of the disaccharides (1) and (3) show only slight differences due to the additionalN-acetyl group in (3). The conformational equilibrium of (1–3) glycosidic bonds of1 and3 was not affected by attaching a (1–6) linked GlcNAc unit to the GalNAc residue in2 and4. However, experimental and theoretical data show that the (1–6) linkages of the trisaccharides2 and4, which carry an additional (1–3) linked glycosyl residue, change their preferred conformations when compared with (5). The 6-branch also shows significant interactions with the benzyl aglycon altering the preferred conformation of the hydroxymethyl group of the GalNAc to a higher proportion of the gt conformer. The (1–6) linkage of2, 4, and6 can have two different families of conformations of which the lower energy state is populated only to about 20% of the time whereas the other state with a relative enthalpy of 4 kcal mol^–1 is populated to 80%. This fact demonstrates that the two conformational states have different entropy contents. Entropy is implicitly included in MMC simulations but cannot be derived from energy minimizations.Abbreviations Bzl benzyl - COSY correlation spectroscopy - Gal d-galactose - GalNAc N-acetyl-d-galactosamine - GalNAc-ol N-acetylgalactosaminitol - GlcNAc N-acetyl-d-glucosamine - HOHAHA homonuclear Hartmann-Hahn-spectroscopy - MMC metropolis Monte Carlo - NOE nuclear Overhauser enhancement - pNp p-nitrophenyl - ROESY rotating frame Overhauser enhancement spectroscopy - TOCSY totally correlated spectroscopy     

An NMR investigation of putative interresidue H-bonding in methyl α-cellobioside in solution

Methyl α-cellobioside (methyl β-d-glucopyranosyl-(1→4)-α-d-glucopyranoside) was labeled with ¹³C at C4′ for use in NMR studies in DMSO-d₆ solvent to attempt the detection of a trans-H-bond J-coupling (^3hJ_CCOH) between C4′ and OH3. Analysis of the OH3 signal at 600 MHz revealed only the presence of two homonuclear J-couplings: ³J_H3,OH3 and a smaller, longer range J_HH. No evidence for ^3hJ_C4′,OH3 was found. The longer range J_HH was traced to ⁴J_H4,OH3 based on 2D ¹H–¹H COSY data and inspection of the H2 and H4 signal lineshapes. A limited set of DFT calculations was performed on a methyl cellobioside mimic to evaluate the structural dependencies of ⁴J_H2,O3H and ⁴J_H4,O3H on the H3–C3–O3–H torsion angle. Computed couplings range from about −0.7 to about +1.1 Hz, with maximal values observed when the C–H and O–H bonds are roughly diaxial.     

A spin-state-selective experiment for measuring heteronuclear one-bond and homonuclear two-bond couplings from an HSQC-type spectrum

Recently, a set of selective 1D experiments with spin-state-selective excitation for CH spin systems was introduced by Parella and Belloc (J. Magn. Reson., 148, 78–87 (2001)). We have expanded and generalized this concept further, and demonstrated that a very simple experiment utilizing spin-state-selective filtering can be used for simultaneous measurement of heteronuclear ¹ J _NH (or ¹ J _CH) and geminal ² J _HH couplings from two-dimensional ¹⁵N-¹H (or ¹³C-¹H) correlation spectrum. The experiment has very high sensitivity owing to the preservation of equivalent coherence transfer pathways analogous to the sensitivity and gradient enhanced HSQC experiment. However, overall length of the pulse sequence is 1/(2J) shorter than the gradient selected SE-HSQC experiment. Furthermore, the spin-state-selection can be utilized between NH and NH₂ (or CH and CH₂) moieties by changing the phase of only one pulse. The pulse scheme will be useful for the measurement of scalar and residual dipolar couplings in wide variety of samples, due to its high sensitivity and artifact suppression efficiency. The method is tested on NH₂ and CH₂ moieties in ¹⁵N- and ¹⁵N/¹³C–labeled ubiquitin samples.     

The three-dimensional structure of acyl-coenzyme A binding protein from bovine liver: Structural refinement using heteronuclear multidimensional NMR spectroscopy

Summary The 3D structure of bovine recombinant acyl-coenzyme A binding protein has been determined using multidimensional heteronuclear magnetic resonance spectroscopy in a study that combines investigations of ¹⁵N-labeled and unlabeled protein. The present structure determination is a refinement of the structure previously determined (Andersen, K.V. and Poulsen, F.M. (1992) J. Mol. Biol., 226, 1131–1141). It is based on 1096 distance restraints and 124 dihedral angle restraints of which 69 are for -angles and 8 for chiral centers and 47 for prochiral centers. The new experimental input for the structure determination has provided an increase of 263 distance restraints, 5 -angle restraints, and 32 -angle restraints in 2 chiral centers, and 31 prochiral centers restraining an additional 23 ¹, 8 ², and 1 ³ angles. The increase of 300 distance and dihedral angle restraints representing an additional 30% of input parameters for the structure determination has been shown to be in agreement with the first structure. A set of 29 structures has been calculated and each of the structures has been compared to a mean structure to give an atomic root mean square deviation of 0.44±0.12 (1 is 0.1 nm) for the backbone atoms C, C, and N in the four -helices A1, residues 4–15, A2, residues 21–36, A3, residues 51–62 and A4, residues 65–84. The loop-region of residues Gly⁴⁵-Lys⁵⁰ could not be defined by the restraints obtained by NMR.The program PRONTO has been used for the spectrum analysis, assignment of the individual nuclear Overhauser effects, the integration of the cross peaks, and the measurement of the coupling constants. The programs DIANA, X-PLOR and INSIGHT have been used in the structure calculations and evaluations.     

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     

Transverse relaxation optimised spin-state selective NMR experiments for measurement of residual dipolar couplings

Three transverse relaxation optimised NMR experiments (TROSY) for the measurement of scalar and dipolar couplings suitable for proteins dissolved in aqueous iso- and anisotropic solutions are described. The triple-spin-state-selective experiments yield couplings between ¹H^N-¹³C, ¹⁵N-¹³C, ¹H^N-¹³C _i–1, ¹⁵N-¹³C _i–1, ¹H^N-¹³C_i–1, ¹⁵N-¹³C_i–1, and ¹³C_i–1-¹³C _i–1 without introducing nonessential spectral crowding compared with an ordinary two-dimensional ¹⁵N-¹H correlation spectrum and without requiring explicit knowledge of carbon assignments. This set of /-J-TROSY experiments is most useful for perdeuterated proteins in studies of structure–activity relationships by NMR to observe, in addition to epitopes for ligands, also conformational changes induced by binding of ligands.     

Modelling continuous culture of Rhodospirillum rubrum in photobioreactor under light limited conditions

Rhodospirillum rubrum was grown continuously and photoheterotrophically under light limitation using a cylindrical photobioreactor in which the steady state biomass concentration was varied between 0.4 to 4 kg m^–3 at a constant radiant incident flux of 100 W m^–2. Kinetic and stoichiometric models for the growth are proposed. The biomass productivities, acetate consumption rate and the CO₂ production rate can be quantitatively predicted to a high level of accuracy by the proposed model calculations. Nomenclature: C _X, biomass concentration (kg m^–3) D, dilution rate (h^–1) Ea, mean mass absorption coefficient (m² kg^–1) I , total available radiant light energy (W m^–2) K, half saturation constant for light (W m^–2) R _W, boundary radius defining the working illuminated volume (m) r _X, local biomass volumetric rate (kg m^–3 h^–1) <r _X>, mean volumetric growth rate (kg m^–3 h^–1) V _W, illuminated working volume in the PBR (m^–3). Greek letters: , working illuminated fraction (–) _M, maximum quantum yield (–) bar, mean energetic yield (kg J^–1).     

A 4D HCC(CO)NNH experiment for the correlation of aliphatic side-chain and backbone resonances in 13C/15N-labelled proteins

Summary We recently proposed a novel four-dimensional (4D) NMR strategy for the assignment of backbone nuclei in spectra of ¹³C/¹⁵N-labelled proteins (Boucher et al. (1992) J. Am. Chem. Soc., 114, 2262–2264 and J. Biomol. NMR, 2, 631–637). In this paper we extend this approach with a new constant time 4D HCC(CO)NNH experiment that also correlates the chemical shifts of the aliphatic sidechain (¹H and ¹³C) and backbone (¹H, ¹³C and ¹⁵N) nuclei. It separates the sidechain resonances, which may heavily overlap in spectra of proteins with large numbers of similar residues, according to the backbone nitrogen and amide proton chemical shifts. When used in conjunction with a 4D HCANNH or HNCAHA experiment it allows, in principle, complete assignment of aliphatic sidechain and backbone resonances with just two 4D NMR experiments.