Temperature coefficients of amide proton NMR resonance frequencies in trifluoroethanol: A monitor of intramolecular hydrogen bonds in helical peptides?

Summary 2D ¹H NMR spectroscopy of two -helical peptides which differ in their amphipathicity has been used to investigate the relationships between amide-proton chemical shifts, amide-proton exchange rates, temperature, and trifluoroethanol (TFE) concentration. In 50% TFE, in which the peptides are maximally helical, the amide-proton chemical shift and temperature coefficient patterns are very similar to each other in each peptide. Temperature coefficients from –10 to –6 ppb/K, usually indicative of the lack of intramolecular hydrogen bonds, were observed even for hydrophobic amino acids in the center of the -helices. However, slow hydrogen isotope exchange for residues from 4 to 16 in both 18-mer helices indicates intact intramolecular hydrogen bonds over most of the length of these peptides. Based on these anomalous observations, we suggest that the pattern of amide-proton shifts in -helices in H₂O/TFE solvents is dominated by bifurcated intermolecular hydrogen-bond formation between the backbone carbonyl groups and TFE. The amide-proton chemical shift changes with increasing temperature may be interpreted by a disruption of intermolecular hydrogen bonds between carbonyl groups and the TFE in TFE/water rather than by the length of intramolecular hydrogen bonds in -helices. Supplementary Material is available upon request, comprising seven pages with listings of experimental details and the NMR shift data for the two peptides.     

Hydrogen bond formation in regioselectively functionalized 3-mono-O-methyl cellulose

The hydrogen bond systems of cellulose and its derivatives are one of the most important factors regarding their physical- and chemical properties such as solubility, crystallinity, gel formation, and resistance to enzymatic degradation. In this paper, it was attempted to clarify the intra- and intermolecular hydrogen bond formation in regioselectively functionalized 3-mono-O-methyl cellulose (3MC). First, the 3MC was synthesized and the cast film thereof was characterized in comparison to 2,3-di-O-methyl cellulose, 6-mono-O-methyl cellulose, and 2,3,6-tri-O-methyl cellulose by means of wide angle X-ray diffraction (WAXD) and (13)C cross polarization/magic angle spinning NMR spectroscopy. Second, the hydrogen bonds in the 3MC film were analyzed by means of FTIR spectroscopy in combination with a curve fitting method. After deconvolution, the resulting two main bands (Fig. 3) indicated that instead of intramolecular hydrogen bonds between position OH-3 and O-5 another intramolecular hydrogen bond between OH-2 and OH-6 may exist. The large deconvoluted band at 3340cm(-1) referred to strong interchain hydrogen bonds involving the hydroxyl groups at C-6. The crystallinity of 54% calculated from the WAXD supports also the dependency of the usually observed crystallization in cellulose of the hydroxyl groups at C-6 to engage in interchain hydrogen bonding.     

Use of 13C chemical shift surfaces in the study of carbohydrate conformation. Application to cyclomaltooligosaccharides (cyclodextrins) in the solid state and in solution

The anomeric carbon chemical shifts of free cyclomaltohexaose, -heptaose, -octaose, -decaose, and -tetradecaose (alpha-, beta-, gamma-, epsilon-, and eta-cyclodextrin, respectively), and of alpha-cyclodextrin inclusion complexes, both in the solid state and in solution, were computed using ab initio 13C chemical shift surfaces for the D-Glcp-alpha-(1-->4)-D-Glcp linkage as a function of the glycosidic bond dihedral angles. Chemical shift calculations in the solid state used angle pairs measured from cyclodextrin X-ray structures as input. For estimations in the liquid state two different approaches were employed to account for dynamic averaging. In one, the computed solid-state anomeric carbon chemical shifts for each cyclodextrin D-Glcp monomer were simply averaged to obtain an estimate of the 13C shifts in solution. In the other, chemical shifts for the anomeric carbons were determined by averaging back-calculated 13C shift trajectories derived from a series of 5 ns molecular dynamic simulations for the oligosaccharides with explicit representation of water. Good agreement between calculated and experimental 13C shifts was found in all cases. Furthermore, our results show that the ab initio 13C chemical shift surfaces are sufficiently sensitive to reproduce the small variations observed for the anomeric 13C shifts of the different cyclodextrin D-Glcp units in the solid state with excellent accuracy. The use of chemical shift surfaces as tools in conformational studies of oligosaccharides is discussed.     

Solid-state structure of N-o-, N-m-, and N-p-nitrophenyl-2,3,4-tri-O-acetyl-β-D-xylopyranosylamines

Comprehensive structural analyses were performed for N-o-, N-m-, and N-p-nitrophenyl-2,3,4-tri-O-acetyl-β-D-xylopyranosylamines. Single-crystal X-ray diffraction data were collected and revealed that one compound under investigation undergoes temperature-dependent polymorph transitions (crystal structures of three polymorphs were obtained). The number of molecules in the independent part of the crystal unit cells was in agreement with the number of resonances in solid-state (13)C NMR spectra. Therefore, the compounds exist as single polymorphs at room temperature, as confirmed by powder X-ray diffraction measurements. Significant differences in (13)C chemical shifts between solution and solid-state NMR for selected carbon atoms confirmed the existence of intra- and/or intermolecular interactions.     

Crystal structure and solid-state 13C NMR analysis of N-o-, N-m- and N-p-nitrophenyl-2,3,4,6-tetra-O-acetyl-beta-D-glucopyranosylamines, and their N-acetyl derivatives

The X-ray diffraction analysis of N-o-nitrophenyl-2,3,4,6-tetra-O-acetyl-β-d-glucopyranosylamine (1), N-m-nitrophenyl-2,3,4,6-tetra-O-acetyl-β-d-glucopyranosylamines, N-p-nitrophenyl-2,3,4,6-tetra-O-acetyl-β-d-glucopyranosylamines, and their N-acetyl derivatives was performed. The sugar moieties always adopt ⁴C₁ conformations, however, due to crystal packing forces they are always slightly distorted. It was found that except N-acetyl, N-m-nitrophenyl-2,3,4,6-tetra-O-acetyl-β-d-glucopyranosylamine (5), none of the glucopyranosylamines studied in this paper form strong hydrogen bonds in the crystal lattice. Additionally, (5) crystallizes with a molecule of water, which occupies a special crystallographic position (on the twofold axis) and links two sugar molecules by hydrogen bonds. The CP MAS NMR spectra confirmed the presence of the intermolecular hydrogen bond involving the molecule of water in (5). Moreover, it was proved that in (1) an intramolecular hydrogen bond is formed between the glycosidic linkage and the nitro group.     

Single-crystal and powder X-ray diffraction and solid-state C NMR of p-nitrophenyl glycopyranosides, the derivatives of d-galactose, d-glucose, and d-mannose

The X-ray diffraction patterns, ¹³C CP MAS NMR spectra, and powder X-ray diffraction analyses were obtained for selected p-nitrophenyl glycosides: α- and β-d-galactopyranosides (1 and 2), α- and β-d-glucopyranosides (3 and 4), and α- and β-d-mannopyranosides (5 and 6). In X-ray diffraction analysis of 1 and 2, characteristic shortening and lengthening of selected bonds were observed in the molecules of 1 due to anomeric effect, and in the crystal lattice of 1 and 2, hydrogen bonds of complex network were detected. In the crystal asymmetric unit of 1 there were two independent molecules, whereas in 2 there was one molecule. For 1 and 3–6 the number of resonances in solid-state ¹³C NMR spectra exceeded the number of the carbon atoms in the molecules, while for 2 there were distinct singlet resonances in its solid-state NMR spectrum. Furthermore, the powder X-ray diffraction (PXRD) performed for 1–3 and 5 revealed that 1, 3, and 5 existed as single polymorphs proving that the doublets observed in appropriate solid-state NMR spectra were connected with two non-equivalent molecules in the crystal asymmetric unit. On the other hand 2 existed as a mixture of two polymorphs, one of them was almost in agreement with the calculated pattern obtained from XRD (the difference in volumes of the unit cells), and the subsequent unknown polymorph existed in small amounts and therefore it was not observed in solid-state NMR measurements.     

A Structural and Thermodynamic Analysis of Novatrone and Flavin Mononucleotide Heteroassociation in Aqueous Solution by <Superscript>1</Superscript>H NMR Spectroscopy

A heteroassociation of the antitumor antibiotic novatrone (NOV) and flavin mononucleotide (FMN) in aqueous solution was studied by one- and two-dimentional ¹H NMR spectroscopy (500 MHz) to elucidate the molecular mechanism of the possible combined action of the antibiotic and the vitamin. The equilibrium reaction constants, the induced proton chemical shifts, and the thermodynamic parameters (ΔH and Δ_S) of the NOV and FMN heteroassociation were determined from the concentration and temperature dependences of proton chemical shifts of the aromatic molecules. The most favorable structure of the 1 : 1 NOV-FMN complex was determined by both the method of molecular mechanics (X-PLOR software) and the induced proton chemical shifts of the molecules. An analysis of the results suggests that the NOV-FMN intermolecular complexes are mainly stabilized by stacking interactions of their aromatic chromophores. An additional stabilization is possible due to intermolecular hydrogen bonds. It was concluded that the aromatic molecules of vitamins, in particular, FMN, can form energetically favorable heterocomplexes with aromatic antitumor antibiotics in aqueous solutions, which could result in a modulation of their medical and biological action.     

Crystal structure of a zwitterionic detergent: n-octyl-2-hydroxyethylsulfoxide

The crystal structure of n-octyl-2-hydroxyethylsulfoxide (1) (space group P2(1)/c, a = 16.516(7), b = 9.053(4), c = 8.222(4) A, beta = 97.58 degrees) was determined by X-ray diffraction methods to 0.94 A resolution and refined to R = 0.050 (Rw = 0.052). In the crystal lattice the molecules are not arranged tail-to-tail, as usually observed with amphiphilic compounds, but head-to-tail and aligned in the a-axis direction. They form layers in the b, c plane which are interdigitated such that adjacent molecules in one layer are in antiparallel orientation. The packing is stabilized by intermolecular hydrogen bonds O-H--O-S. No solvent molecules were detectable.     

Solid-state structure of N-o-, N-m-, and N-p-nitrophenyl-2,3,4-tri-O-acetyl-β-d-xylopyranosylamines

Comprehensive structural analyses were performed for N-o-, N-m-, and N-p-nitrophenyl-2,3,4-tri-O-acetyl-β-d-xylopyranosylamines. Single-crystal X-ray diffraction data were collected and revealed that one compound under investigation undergoes temperature-dependent polymorph transitions (crystal structures of three polymorphs were obtained). The number of molecules in the independent part of the crystal unit cells was in agreement with the number of resonances in solid-state ¹³C NMR spectra. Therefore, the compounds exist as single polymorphs at room temperature, as confirmed by powder X-ray diffraction measurements. Significant differences in ¹³C chemical shifts between solution and solid-state NMR for selected carbon atoms confirmed the existence of intra- and/or intermolecular interactions.     

1H NMR spectra of branched-chain cyclomaltohexaoses (alpha-cyclodextrins)

The 1H NMR spectra of seven branched alpha-cyclodextrins (alpha-CDs) were observed and analyzed in detail. They were compared with spectra of alpha-CD and amylose. Although these branched alpha-CDs consist only of alpha-D-glucose with the same alpha-(1-->4) O-glucosyl binding, aside from one exception, differences in chemical shifts of corresponding signals were significantly large. Especially, differences in the chemical shift in anomeric protons were considerably large. Subtle differences in glucosyl binding directly influences chemical shifts of these protons because anomeric protons are located adjacent to the glucosyl binding sites.     

Contribution of intra- and intermolecular hydrogen bonds to the conformational stability of human lysozyme(,).

In globular proteins, there are intermolecular hydrogen bonds between protein and water molecules, and between water molecules, which are bound with the proteins, in addition to intramolecular hydrogen bonds. To estimate the contribution of these hydrogen bonds to the conformational stability of a protein, the thermodynamic parameters for denaturation and the crystal structures of five Thr to Val and five Thr to Ala mutant human lysozymes were determined. The denaturation Gibbs energy (DeltaG) of Thr to Val and Thr to Ala mutant proteins was changed from 4.0 to -5.6 kJ/mol and from 1.6 to -6.3 kJ/mol, respectively, compared with that of the wild-type protein. The contribution of hydrogen bonds to the stability (DeltaDeltaG(HB)) of the Thr and other mutant human lysozymes previously reported was extracted from the observed stability changes (DeltaDeltaG) with correction for changes in hydrophobicity and side chain conformational entropy between the wild-type and mutant structures. The estimation of the DeltaDeltaG(HB) values of all mutant proteins after removal of hydrogen bonds, including protein-water hydrogen bonds, indicates a favorable contribution of the intra- and intermolecular hydrogen bonds to the protein stability. The net contribution of an intramolecular hydrogen bond (DeltaG(HB[pp])), an intermolecular one between protein and ordered water molecules (DeltaG(HB[pw])), and an intermolecular one between ordered water molecules (DeltaG(HB[ww])) could be estimated to be 8. 5, 5.2, and 5.0 kJ/mol, respectively, for a 3 A long hydrogen bond. This result shows the different contributions to protein stability of intra- and intermolecular hydrogen bonds. The entropic cost due to the introduction of a water molecule (DeltaG(H)()2(O)) could be also estimated to be about 8 kJ/mol.     

Solid-state CP/MAS C-NMR analysis of cellulose and tri-O-substituted cellulose ethers

Highly crystalline tri-O-substituted cellulose ethers having ethyl, n-propyl, n-butyl, allyl, and methallyl substituents were prepared from low-molecular weight cellulose (DP = 15). Influences of conformational and packing effects on solid-state ¹³C-NMR spectra were studied by using X-ray diffraction and solid- and solution-state ¹³C-NMR analyses of the cellulose derivatives. Unit-cell sizes tentatively obtained from X-ray diffraction patterns of the cellulose derivatives indicated that conformations and packing states of cellulose chains and alkyl chains of substituents were different between the derivatives. Solid- and solution-state ¹³C-NMR spectra of cellulose allomorphs, and effects of hydrogen bonds present in celluloses I, II, and III on chemical shifts of their solid-state ¹³C-NMR spectra were proposed.     

Comparative (1)H NMR and molecular modeling study of hydroxy protons of beta-D-Galp-(1-->4)-beta-D-GlcpNAc-(1-->2)-alpha-D-Manp-(1-->O)(CH(2))(7)CH(3) analogues in aqueous solution

The (1)H chemical shifts, coupling constants, temperature coefficients, exchange rates, and inter-residual ROEs have been measured, in aqueous solution, for the hydroxy and amine/amide proton resonances of a set of beta-D-Galp-(1-->4)-beta-D-GlcpNAc-(1-->2)-alpha-D-Manp-(1-->O)(CH(2))(7)CH(3) analogues. From the structural data, a few significant structural features could be ascertained, such as a preferential anti-conformation for the amide protons of the N-acetyl and N-propionyl groups. The introduction of systematic modifications at Gal 2-C and Gal 6-C resulted in alterations of the Gal 4-OH, Gal 3-OH, and GlcNAc 3-OH areas, since variations in chemical shifts and temperature coefficient were observed. In order to verify the possibility of hydrogen bonds, molecular dynamics simulations in the gas phase and explicit solvent were performed and correlated with the experimental data. A network of hydrogen bonds to solvent molecules was observed, but no strong intramolecular hydrogen bonding was observed.     

Molecular recognition in noncovalent antitumor agent-DNA complexes: NMR studies of the base and sequence dependent recognition of the DNA minor groove by netropsin

We have investigated intermolecular interactions and conformational features of the netropsin complexes with d(G1-G2-A3-A4-T5-T6-C7-C8) duplex (AATT 8-mer) and the d(G1-G2-T3-A4-T5-A6-C7-C8) duplex (TATA 8-mer) by one and two-dimensional NMR studies in solution. We have assigned the amide, pyrrole and methylene protons of netropsin and the base and sugar H1' protons of the nucleic acid from an analysis of the nuclear Overhauser effect (NOESY) and correlated (COSY) spectra of the complex at 25 degrees C. The directionality of the observed distance-dependent NOEs demonstrates that the 8-mer helices remain right-handed and that the arrangement of concave and convex face protons of netropsin are retained in the complexes. The observed changes in NOE patterns and chemical shift changes on complex formation suggest small conformational changes in the nucleic acid at the AATT and TATA antibiotic binding sites and possibly the flanking G.C base pairs. We observe intermolecular NOEs between all three amide and both pyrrole protons on the concave face of the antibiotic and the minor groove adenosine H2 proton of the two central A4.T5 base pairs of the AATT 8-mer and TATA 8-mer duplexes. The concave face pyrrole protons of the antibiotic also exhibit NOEs to the sugar H1' protons of residues 5 and 6 in the AATT and TATA 8-mer complexes. We also detect intermolecular NOEs between the guanidino and propioamidino methylene protons at either end of netropsin and the adenosine H2 proton of the two flanking A3.T6 base pairs in the AATT 8-mer and T3.A6 base pairs in the TATA 8-mer duplexes. These studies establish a set of nine contacts between the concave face of the antibiotic and the minor groove AATT segment and TATA segment of the 8-mer duplexes in solution. The observed magnitude of the NOEs require that there be no intervening water molecules sandwiched between the concave face of the antibiotic and the minor groove of the DNA so that release of the minor groove spine of hydration is a prerequisite for netropsin complex formation. The observed differences in the netropsin amide proton chemical shifts in the AATT 8-mer and TATA 8-mer complexes suggest differences in the strength and/or type of intermolecular hydrogen bonds at the AATT and TATA binding sites.(ABSTRACT TRUNCATED AT 400 WORDS)     

Temperature coefficients of peptides dissolved in hexafluoroisopropanol monitor distortions of helices

Summary Temperature coefficients are widely used as an indication of solvent accessibility to amide protons. Low temperature coefficients are related to low accessibility and are often interpreted as evidence for intramolecular hydrogen bonding. Conformational shifts, i.e. the difference between chemical shifts of a particular residue in a structured and in a random-coil conformation, provide information on secondary structure. In particular, negative CH^α conformational shifts are often used to delineate the extent of helical stretches. NH conformational shifts show large oscillations within a helix that have been interpreted as the result of helix distortions affecting hydrogen bond lengths. In the ocurse of the study of differnet peptides that adopt a helical structure in the presence of the structure-inducing solvent hexafluoroisopropanol (HFIP), we have found a strong correlation between temperature coefficients and amide conformational shifts. However, contrary to the initial expectations, lower temperature coefficients were associated to amide protons involved in longer, and presumably weaker, hydrogen bonds. The correlation can be explained, however, assuming that, in helical peptides dissolved in HFIP, temperature affects the chemical shift of amide protons mainly by changing the average length of intramolecular hydrogen bonds and changes in solvent accessibility play only a secondary role under these experimental conditions. The pattern of temperature coefficients in helical peptides can therefore be used to identify short or long hydragen bonds causing bending of the helix axis.     

Temperature coefficients of peptides dissolved in hexafluoroisopropanol monitor distortions of helices

Temperature coefficients are widely used as an indication of solvent accessibility to amide protons. Low temperature coefficients are related to low accessibility and are often interpreted as evidence for intramolecular hydrogen bonding. Conformational shifts, i.e. the difference between chemical shifts of a particular residue in a structured and in a random-coil conformation, provide information on secondary structure. In particular, negative CH conformational shifts are often used to delineate the extent of helical stretches. NH conformational shifts show large oscillations within a helix that have been interpreted as the result of helix distortions affecting hydrogen bond lengths. In the course of the study of different peptides that adopt a helical structure in the presence of the structure-inducing solvent hexafluoroisopropanol (HFIP), we have found a strong correlation between temperature coefficients and amide conformational shifts. However, contrary to the initial expectations, lower temperature coefficients were associated to amide protons involved in longer, and presumably weaker, hydrogen bonds. The correlation can be explained, however, assuming that, in helical peptides dissolved in HFIP, temperature affects the chemical shift of amide protons mainly by changing the average length of intramolecular hydrogen bonds and changes in solvent accessibility play only a secondary role under these experimental conditions. The pattern of temperature coefficients in helical peptides can therefore be used to identify short or long hydrogen bonds causing bending of the helix axis.     

C, N CP MAS and high resolution multinuclear NMR study of methyl

Triphenyl(6-thiopurinyl)tin has been prepared and its structure reinvestigated by X-ray diffraction. In the structure, a new coordination mode was observed that was different from those reported previously from investigations by infrared and Mössbauer spectroscopy. In the molecule, 6-thiopurine coordinated to tin by the S and N(1) atoms. The discrete molecules were connected to form a zigzag 1D network through intermolecular H?N hydrogen bonds. The tin environment is pentacoordinated with cis-trigonal bipyramidal geometry.     

An exact coordination mode of 6-thiopurine with an organotin(IV): preparation and crystal structure of triphenyl(6-thiopurinyl)tin(IV)

Triphenyl(6-thiopurinyl)tin has been prepared and its structure reinvestigated by X-ray diffraction. In the structure, a new coordination mode was observed that was different from those reported previously from investigations by infrared and Mössbauer spectroscopy. In the molecule, 6-thiopurine coordinated to tin by the S and N(1) atoms. The discrete molecules were connected to form a zigzag 1D network through intermolecular H?N hydrogen bonds. The tin environment is pentacoordinated with cis-trigonal bipyramidal geometry.     

Synthesis, X-ray crystallographic structures of thio substituted N-acetyl N'-methylamide alanine and evaluation of sp sulfur parameters of the CFF91 force field.

Acetyl thioalanine N-methyl (Ac-Alat-NHMe) and thioacetyl alanine N-methyl (Act-Ala-NHMe) were synthesized, crystallized and their X-ray diffraction structures determined for the first time. Both molecules adopted beta-sheet conformations and showed similar hydrogen bonding patterns with one molecular surface forming two oxo hydrogen bonds and the other forming two thio hydrogen bonds. The crystal structure data for the two thioamides provided a validation of the thioamide parameters for the newly derived CFF91 force field because the observed crystal (phi, psi) angles were situated in the global minimum regions of the theoretical (phi, psi) map predicted using the parameters. In addition, the parameters were further validated because conformational energy minimization of the crystal structure produced low deviations in unit cell dimensions, bond lengths, bond angles and torsional angles, and a 120-ps molecular dynamics simulation also gave a low deviation for the most probable N-H...S=C bond distance.     

Nuclear-magnetic-resonance study of aggregations and conformations of melanostatin and related peptides.

The 1H and 13C nuclear magnetic resonance spectra of melanostatin (Pro-Leu-Gly-NH2) and related peptides (Pro-Leu-Gly, Z-Pro-Leu-Gly, Z-Pro-Leu-Gly-NH2 and Z-Pro-Leu-Gly-OCH3, where Z = benzyloxycarbonyl) were analysed in a variety of solvents. At physiological pH, the melanostatin molecule is N-protonated in aqueous solution. The concentration dependences of the chemical shifts of amide-proton and carbonyl-carbon resonances and of proton spin-lattice relaxation times were observed in relation to molecular aggregations. In dimethylsulfoxide solution, aggregations were observed for N-protonated melanostatin and Pro-Leu-Gly prepared with HCl and for the Na salt of Z-Pro-Leu-Gly but not for N-protonated melanostatin prepared with HClO4 or HNO3, unprotonated melanostatin, Z-Pro-Leu-Gly-NH2, or Z-Pro-Leu-Gly-OCH3. The leucine NH and glycine CO groups of N-protonated melanostatin are involved in the intermolecular hydrogen bonds of aggregates. The leucine NH group of N-protonated Pro-Leu-Gly also forms the intermolecular hydrogen bond. The solvent and temperature dependences of the chemical shifts of amide-proton and carbonyl-carbon resonances were measured to determine intramolecular hydrogen bonding. In dimethylsulfoxide solution, N-protonated melanostatin molecules in part take the beta-turn structure and the trans carboxamide NH proton and carbonyl oxygen of the proline residue form an intramolecular hydrogen bond.