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A new experiment for the measurement of nJ(C,P) coupling constants along the phosphodiester backbone in RNA and DNA based on a quantitative-J HCP experiment is presented. In addition to coupling constants, in which a carbon atom couples to only one phosphorus atom, both the intraresidual 3J(C4'i,Pi) and the sequential 3J(C4'i,Pi+1) for the C4' resonances that couple to two phosphorus atoms can be obtained. Coupling constants obtained by this new method are compared to values obtained from the P-FIDS experiment. Together with 3J(H,P) coupling constants measured using the P-FIDS experiment, the backbone angles β and ∈ can be determined.

Fractures occurring in human bones produce an acoustic signal, analysis of which permits an evaluation of its source. In the industrial setting acoustic emission analysis (AEA) is used to non-invasively monitor the function of stressed technical systems or parts of systems. During servicing and monitoring of technical systems, acoustic signals emitted by cracks or material deformation are located with the aid of a few acoustic sensors and evaluated for risk-identification purposes. With appropriate technology, therefore, both cortical and trabecular bone can be monitored by acoustic emission analysis. A search is currently ongoing for suitable acoustic technology capable of assessing the extent and location of bone defects and predicting associated risks of fractures occurring. In the present study a system for the measurement and analysis of acoustic emission is described which permits the measurement and analysis of acoustic signals obtained from processed and fresh human and porcine femora. In slightly modified form this system was then used to assess the type and extent of acoustic emission obtained from explanted human femora exposed to cyclical torsional loading until fracture occurred.

Oxidized and reduced hen lysozyme denatured in 8 M urea at low pH have been studied in detail by NMR methods. 15N correlated NOESY and TOCSY experiments have provided near complete sequential assignment for both 1H and 15N resonances. Over 900 NOEs, including 130 (i, i + 2) and 23 (i, i + 3) NOEs, could be identified by analysis of the NOESY spectra of the denatured states, and 3J(HN, Halpha) coupling constants and 15N relaxation rates have been measured. The coupling constant and NOE data were analyzed by comparisons with theoretical predictions from a random coil polypeptide model based on amino acid specific phi,psi distributions extracted from the protein data bank. There is significant agreement between predicted and experimental NMR parameters suggesting that local conformations of the denatured states are largely determined by short-range interactions within the polypeptide chain. This result is supported by the observation that the chemical shift, coupling constant, and NOE data are little affected by whether or not the four disulfide bridge cross-links are formed in the denatured protein. The relaxation data, however, show significant differences between the oxidized and reduced protein. Analysis of the relaxation data in terms of simple dynamics models provides evidence for weak clustering of hydrophobic groups near tryptophan residues and increased barriers to motion in the more compact conformers formed when the polypeptide chain is cross-linked by the disulfide bridges. Using this information, a structural description of these denatured states is given in terms of an ensemble of conformers, which have a complex relationship between their local and global characteristics.

The directed TOCSY pulse sequence element transfers coherence predominantly into "forward-directed" antiphase coherences while simultaneously suppressing in-phase and "backward-directed" antiphase coherences. This novel selection principle, based on the "direction" of the target coherences, provides a new approach for the simplification of crowded spectra. In this article, the theory of directed TOCSY is presented for linear spin systems that are frequently found in carbon-labeled biomolecules.

15N NMR relaxation measurements have been used to study the dynamic behaviour of the main-chain of hen lysozyme in a partially folded state, formed in a 70% (v/v) trifluoroethanol (TFE)/30% water mixture at 37 degrees C and pH 2. This state is characterised by helical secondary structure in the absence of extensive tertiary interactions. The NMR relaxation data were interpreted by mapping of spectral density functions and by derivation of segmental as well as global order parameters. The results imply that the dynamics of lysozyme in TFE can, at least for the great majority of residues, be adequately described by internal motions which are superimposed on all overall isotropic tumbling of the molecule. Although the dynamic behaviour shows substantial variations along the polypeptide chain, it correlates well with the conformational preferences identified in the TFE state by other NMR parameters. Segments of the polypeptide chain which are part of persistent helical structures are highly restricted in their motion (S2 > 0.8 , with effective internal correlation times tau(e) < 200 ps) but are also found to experience conformational exchange on a millisecond timescale. Regions which are stabilised in less persistent helical structure possess greater flexibility (0.6 < S2 < 0.8, 200 ps < tau(e) < 1 ns) and those which lack defined conformational preferences are highly flexible (S2 < 0.6, tau(e) approximately 1 ns). The dynamic behaviour of the main-chain was found to be correlated with other local features of the polypeptide chain, including hydrophobicity and the position of the disulphide bridges. Despite the absence of extensive tertiary interactions, preferential stabilisation of native-like secondary structure by TFE results in a pattern of main-chain dynamics which is similar to that of the native state.

Using a data base of 85 high resolution protein crystal structures the distributions of main chain torsion angles, both in secondary structure and in coil regions where no secondary structure is present, have been analysed. These torsion angle distributions have been used to predict NMR homonuclear and heteronuclear coupling constants for residues in secondary structure using known Karplus relationships. For alpha helices, 3(10) helices and beta strands mean predicted 3JHN alpha coupling constants are 4.8, 5.6 and 8.5 Hz, respectively. These values differ significantly from those expected for the ideal phi angles (3.9, 3.0 and 8.9 Hz; phi = -57 degrees, -49 degrees, -139 degrees for alpha and 3(10) helices and beta strands (antiparallel), respectively) in regular secondary structure, but agree well with available experimental NMR data for nine proteins. The crystallographic data set has also been used to provide a basis for interpreting coupling constants measured for peptides and denatured proteins. Using a model for a random coil, in which all residues adopt distributions of phi, psi angles equivalent to those seen for residues in the coil regions of native folded proteins, predicted 3JHN alpha values for different residue types have been found to range from 5.9 Hz and 6.1 Hz for glycine and alanine, respectively, to 7.7 Hz for valine. A good correlation has been found between the predicted 3JHN alpha coupling constants for this model and experimental values for a set of peptides that other evidence suggest are highly unstructured. For other peptides, however, deviations from the predictions of the model are clear and provide evidence for additional interactions within otherwise disordered states. The values of homonuclear and heteronuclear coupling constants derived from the protein data base listed here therefore provide a basis not only for analysing the secondary structure of native proteins in solution but for assessing and interpreting the extent of structure present in peptides and non-native states of proteins.

Non-native states of proteins are of increasing interest because of their relevance to issues such as protein folding, translocation and stability. A framework for interpreting the wealth of experimental data for non-native states emerging from rapid advances in experimental techniques involves comparison with a "random coll' state, which possesses no structure except that inherent in the local interactions. We review here the concept of a random coil, from its global to its local properties. In particular, we focus on the description of a random coil in terms of statistical distributions in psi, phi space. We show that such a model, in combination with experimental data, provides insight into the structural properties of polypeptide chains and has significance for understanding protein folding and for molecular design.

We introduce the C'-FIDS-(1)H,(15)N-HSQC experiment, a new method for the determination of (3)J(H (infi) (supN) ,C (infi) (sup') ) coupling constants in proteins, yielding information about the torsional angle ϕ. It relies on the (1)H,(15)N-HSQC or HNCO experiment, two of the the most sensitive heteronuclear correlation experiments for isotopically labeled proteins. A set of three (1)H,(15)N-HSQC or HNCO spectra are recorded: a reference experiment in which the carbonyl spins are decoupled during t(1) and t(2), a second experiment in which they are decoupled exclusively during t(1) and a third one in which they are coupled in t(1) as well as t(2). The last experiment yields an E.COSY-type pattern from which the (2)J(H (infi) (supN) ,C (infi-1) (sup') ) and (1)J(N(i),C (infi-1) (sup') ) coupling constants can be extracted. By comparison of the coupled multiplet (obtained from the second experiment) with the decoupled multiplet (obtained from the first experiment) convoluted with the (2)J(H (infi) (supN) ,C (infi-1) (sup') ) coupling, the (3)J(H (infi) (supN) ,C (infi) (sup') ) coupling can be found in a one-parameter fitting procedure. The method is demonstrated for the protein rhodniin, containing 103 amino acids. Systematic errors due to differential relaxation are small for (n)J(H(N),C') couplings in biomacromolecules of the size currently under NMR spectroscopic investigation.

2D and 3D heteronuclear NMR methods have been used to characterize the structure of hen egg-white lysozyme in a partially folded state using uniformly 15N-labeled protein. This state is formed by the denaturation of the protein in 70% trifluoroethanol (TFE)/30% water (v/v) and is characterized by substantial helical secondary structure in the absence of extensive tertiary interactions. 15N-filtered 3D NOESY and TOCSY experiments have allowed the sequential assignment of resonances for all but 2 of the 126 main chain amide nitrogen atoms and of the majority of main and side chain proton resonances. The conformation of the polypeptide chain was characterized by analysis of the pattern of NOEs, H alpha chemical shift perturbations, 3J(HN, H alpha)-coupling constants, and hydrogen exchange protection. These NMR parameters are highly complementary and are consistent with a model for the TFE state in which six regions of the polypeptide chain are substantially ordered in helical conformations. The structure in different regions however, shows different levels of persistency. Five of the helices exhibit significant protection of amide hydrogens against exchange with solvent and are located in regions of the polypeptide which are helical in the native state. By contrast, helical structures of greater flexibility are observed both as extensions to the native-like helices and as a nonnative structure in the region of the molecule which forms the C-terminal part of the beta-sheet in the native state. No specific structural preferences are detected in regions corresponding to the long loop and to the N-terminal part of the beta-sheet of native lysozyme. A combination of local features of the polypeptide chain, including the predicted propensities of residues for helix formation and for their participation in N- and C-terminal helix capping interactions, allows the conformational behavior of the polypeptide chain of hen lysozyme to be rationalized for this partially folded state. The analysis implies that the nonnative structures are a result of interactions which are local to the polypeptide chain. These, and the highly persistent native-like structures, give insight into species which form early during folding.

A three-dimensional 1H, 13C, 31P triple resonance experiment, HCP-CCH-TOCSY, is presented which provides unambiguous through-bond correlation of all 1H ribose protons on the 5' and 3' sides of the intervening phosphorus along the backbone bonding network in 13C-labeled RNA oligonucleotides. The correlation of the complete ribose spin system to the intervening phosphorus is obtained by adding a C,C-TOCSY coherence transfer step to the triple resonance HCP experiment. The C,C-TOCSY transfer step, which utilizes the large and relatively uniform 1J(C,C) coupling constant (approximately 40 Hz for ribose carbons), efficiently correlates the phosphorus-coupled carbons observed in the HCP correlation experiment (i.e., C4' and C5' in the 5' direction and C4' and C3' in the 3' direction) to all other carbons in the ribose spin system. Of the additional correlations observed in the HCP-CCH-TOCSY, that to the relatively well-resolved anomeric H1',C1' resonance pairs provides the greatest gain in terms of facilitating assignment. The gain in spectral resolution afforded by chemical shift labeling with the anomeric resonances should provide a more robust pathway for sequential assignment over the intervening phosphorus in larger RNA oligonucleotides. The HCP-CCH-TOCSY experiment is demonstrated on a uniformly 13C, 15N-labeled 19-nucleotide RNA stem-loop, derived from the antisense RNA I molecule found in the ColE1 plasmid replication control system.

Three experiments are introduced to determine a complete set of coupling constants in RNA oligomers. In the HCCH-E.COSY experiment, the vicinal proton-proton coupling constants can be measured with high accuracy. In the P-FIDS-CT-HSQC experiment, vicinal proton-phosphorus and carbon-phosphorus couplings are measured that depend on the phosphodiester backbone torsion angles beta and epsilon. In the refocussed HMBC experiment, vicinal carbon-proton couplings are measured that depend on the glycosidic torsion angle chi.

A conformational analysis of the valine side chains of ribonuclease T1 (RNase T1) was performed using NMR spectroscopy, in particular homonuclear (1H, 1H and 13C, 13C) and heteronuclear (1H, 15N and 1H, 13C) vicinal spin-spin coupling constants as obtained from E.COSY-type NMR experiments. The coupling constants related to the chi 1 dihedral angle in valine, 3JH alpha H beta, 3JNH beta, 3JC'H beta, 3JH alpha C gamma 1, 3JH alpha C gamma 2, 3JC'C gamma 1, and 3JC'C gamma 2, were evaluated in a quantitative manner. The analysis of 3J data allowed for the stereospecific assignment of the valine methyl resonances. On the basis of various models for motional averaging of coupling constants, a fit of the torsion angles chi 1 to a set of the experimental 3J coupling constants (3JH alpha H beta, 3JNH beta, 3JC'H beta) was carried out. The resulting side-chain conformations were examined with respect to NOE distance informations. Single rotameric states emerged for Val16, Val67, Val79, and Val101, while conformational equilibria between staggered rotamers were found for Val33 and Val78. Using a different model approach, Val52 and Val89 are also likely to exhibit unimodal chi 1 angle distributions. The analysis was found to depend critically on the set of Karplus parameters used. Except for Val52 and Val78, the predominant rotamers obtained from 3J coupling informations agree with the conformation in the crystal structure of ribonuclease T1 (Martinez-Oyanedel et al., 1991).

Sensitive three-dimensional NMR experiments, based on the E.COSY principle, are presented for the measurement of the (3)J(H(N),H(α)) and (3)J(H(N),C') coupling constants in uniformly (13)C- and (15)N-labeled proteins. They employ gradient coherence selection in combination with the sensitivity enhancement method in HSQC-type spectra (Cavanagh et al., 1991; Palmer et al., 1991). In most cases, the two measured coupling constants unambiguously define the ϕ-angle for protein structure determination. The method is applied to uniformly (13)C, (15)N-labeled ribonuclease T(1).

A nucleotide sequence identical with that of the recently identified murine pancreatic ribonuclease (RNAase) was isolated from a murine spleen cDNA library. Active RNAase was expressed and secreted from Escherichia coli lon-htpr- transformed with a plasmid containing the E. coli trp promoter followed by the murine RNAase gene sequence, including the original eukaryotic 26-amino-acid signal sequence. Approx. 1 mg of properly matured RNAase protein/litre was secreted into the medium of a fermentor culture after the promotor was induced by tryptophan starvation. When the signal sequence was deleted from the plasmid, intracellular RNAase activity was very low and there was no significant supernatant RNAase activity. Even higher RNAase yields were obtained with a synthetic gene for bovine pancreatic ribonuclease cloned after the signal sequence of the murine gene. About 2 mg of correctly processed RNAase A/litre was isolated from the growth medium, and a further 8-10 mg of correctly processed RNAase/litre could be isolated from the soluble fraction of the cells. Thus this eukaryotic signal sequence is both recognized by the E. coli transport and processing apparatus and gives efficient secretion, as well as export, of active, mature mammalian RNAases.

130.5 mg of almost pure corpora amylacea was isolated from lyophilized tissue of 35 human brains obtained by autopsy. Staining shaved this material to be homogenous. The greater part of this material is composed of carbohydrates, whereas the protein- and lipid content is small. With regard to composition, one can take for granted that this material is different from amyloid and from the corpora amylacea of the prostatic gland. It may be assumed that corpora amylacea of the brain are caused by the glucose requirement of the brain being reduced, while the supply of glucose for the brain is normal.