Étude de l'interaction de la thiamine diphosphate avec l'ion magnésium

The action of magnesium ion on the exchange rate of the proton in C₂ of thiamine and thiamine diphosphate is studied at different values of pD. Above pD 5 the ion Mg²⁺ increases this exchange rate. The phenomenon is markedly enhanced for TDP rather than thiamine and increases with pD. Below pD 5 magnesium decreases the exchange rate. This decrease is greater for TDP than for thiamine. The maximum effect is reached at a magnesium concentration of 0.5/1 for thiamine and of 1/1 for TDP.T₁ measurements are made for different pH values with and without magnesium ion. Results seem to prove that an increase in pD values from 3.9 to 5.9 leads to an accentuation of the molecules «folded form. Nevertheless for a given pD value the TDP-Mg complex seems to have a more «folded form than TDP.     

Conformation and dynamic structure of poly(inosinic acid) in neutral aqueous solution by 1H-, 2H-, 13C-, and 31P-NMR spectroscopy

The conformation and dynamic structure of single-stranded poly(inosinic acid), poly(I), in aqueous solution at neutral pH have been investigated by nmr of four nuclei at different frequencies: ¹H (90 and 250 MHz), ²H (13.8 MHz), ¹³C (75.4 MHz), and ³¹P (36.4 and 111.6 MHz). Measurements of the proton-proton coupling constants and of the ¹H and ¹³C chemical shifts versus temperature show that the ribose is flexible and that base-base stacking is not very significant for concentrations varying from 0.04 to 0.10M in the monomer unit. On the other hand, the proton T₁ ratios between the sugar protons, T₁ (H₁′)/T₁ (H₃′), indicate a predominance of the anti orientation of the base around the glycosidic bond. The local motions of the ribose and the base were studied at different temperatures by measurements of nuclear Overhauser enhancement (NOE) of protonated carbons, the ratio of the proton relaxation times measured at two frequencies (90 and 250 MHz), and the deuterium quadrupolar transverse relaxation time T₂. For a given temperature between 22 and 62°C, the ¹³C-{¹H} NOE value is practically the same for seven protonated carbons (C₂, C₈, C_1′, C_2′, C_3′, C_4′, C_5′). This is also true for the T₁ ratio of the corresponding protons. Thus, the motion of the ribose–base unit can be considered as isotropic and characterized by a single correlation time, τ_c, for all protons and carbons. The τ_c values determined from either the ¹³C-{¹H} NOE or proton T₁ ratios, T₁(90 MHz)/T₁(250 MHz), and/or deuterium transverse relaxation time T₂ agree well. The molecular motion of the sugar-phosphate backbone (O-P-O) and the chemical-shift anisotropy (CSA) were deduced from T₁ (³¹P) and ³¹P-{¹H} NOE measurements at two frequencies. The CSA contribution to the phosphorus relaxation is about 12% at 36.4 MHz and 72% at 111.6 MHz, corresponding to a value of 118 ppm for the CSA (σ = σ∥ ? σ?). Activation energies of 2–6 kcal/mol for the motion of the ribose–base unit and the sugarphosphate backbone were evaluated from the proton and phosphorus relaxation data.     

Water proton magnetic resonance studies of normal and sickle erythrocytes Temperature and volume dependence

The temperature and cell volume dependence of the NMR water proton linewidth, spin-lattice, and spin-spin relaxation times have been studied for normal and sickle erythrocytes as well as hemoglobin A and hemoglobin S solutions. Upon deoxygenation, the spin-spin relaxation time (T₂) decreases by a factor of 2 for sickle cells and hemoglobin S solutions but remains relatively constant for normal cells and hemoglobin A solutions. The spin-lattice relaxation time (T₁) shows no significant change upon dexygenation for normal or sickle packed red cells. Studies of the change in the NMR linewidth, T₁ and T₂ as the cell hydration is changed indicate that these parameters only slightly by a 10–20% cell dehydration. This result suggests that the reported 10% cell dehydration observed with sickling is not important in the altered NMR properties. Low temperature studies of the linewidth and T₁ for oxy and deoxy hemoglobin A and hemoglobin S solutions suggest that the “bound” water possesses similar properties for all four species. The low temperature linewidth ranges from about 250 Hz at ?15°C to 500 Hz at ?36°C and analysis of the NMR curves yield hydration values near 0.4 g water/g hemoglobin for all four species. The low temperature T₁ data go through a minimum at ?35°C for measurements at 44.4 MHz and ?50°C for measurements at 17.1 MHz and are similar for oxy and deoxy hemoglobin A and hemoglobin S. These similarities in the low temperature NMR data for oxy and deoxy hemoglobin A and hemoglobin S suggest a hydrophobically driven sickling mechanism. The room temperature and low temperature relaxation time data for normal and sickle cells are interpreted in terms of a three-state model for intracellular water. In the context of this model the relaxation time data imply that type III, or irratationally bound water, is altered during the sickling process.     

Molecular mobilities of soluble components in the aqueous phase of chromaffin granules

NMR relaxation times have been used to characterize molecular motion and intermolecular complexes in the aqueous phase of bovine chromaffin granules. Partially relaxed ¹³C and proton spectra have been obtained at 3 and 25°C. T₁ measurements of five protonated carbons on epinephrine (C₂, C₅, C₆ CHOH and NCH₃) give a correlation time of 0.15 (10^?9) s at 25°C for the catechol ring and methine carbon, while the effective correlation time for the NCH₃ group is somewhat shorter due to its internal degree of rotational freedom. Resonances of protonated carbons on the soluble protein chromogranin give very similar corerlation times: 0.20 (10^?9) s for the peptide α-carbon and 0.2 (10^?9) s for the methylene sidechain carbons of glutamic acid. The correlation time (τ_R) of ATP was not measured direrctly using ¹³C T₁ data due to the weakness of its spectrum, but its reorinetation appears to be substantially slower than that of epinephrine or chromogranin. This conclusion is based on three observations: (1) the qualitative temperature dependence of T₁ for H₂ and H₈ on the adenine ring places τ_R for ATP to the right of the T₁ minimum, or τ_R ? 1.0 (10^?9) s; (2) ¹³C resonances of ATP have anomalously low amplitudes compared with epinphrine resonances, a fact that is readily explained only if ATP undergoes substantially slower reorientation; and (3) a comparision of the T₁ data on H₈ on chromaffin granules and in a dilute aqueous solution, where ρ_R for ATP cam be measured directly, indicates that τ_R ～ 1.0 (10^?9 s at 25°C in the granules. The relaxation data are consistent with the concept of a storage complex based on electrostatic interaction between a polyion (chromogranin) and its counterious (ATP and epinephrine), in which ATP cross-links cationic sidechains of the protein.     

13C NMR studies on bilayers formed from synthetic di-10-methyl-stearoyl phosphatidylcholine enriched with 13C in the N-methyl carbons

¹³C NMR relaxation measurements have been carried out on phospholipid bilayer systems formed from synthetic di-10-methyl-stearoyl phosphatidylcholine with 92% enrichment in one of the N-methyl carbons. Studies on single-walled vesicles prepared by sonication from this lipid, and on large multi-lamellar liposomes show that although T₁ values are nearly the same, T₂¹ values are markedly different. It is proposed that equivalent segmental motions in the two systems give rise to similar T₁ values. The T₂¹ values, on the other hand, are consistent with the view that the single-walled vesicles have a more disordered molecular organization than do the multi-lamellar bilayers.     

The effect of altered lipid composition on the transport of various amino acids in Candida albicans.

Candida albicans cells grown on alkanes of different chain lengths (C₁₃, C₁₄, C₁₅, C₁₆, C₁₇, and C₁₈) exhibited a low growth rate and gradual increase in the total lipid content with the increase in the length of alkanes. There was a significant change in the phospholipids and sterols content of various alkane-grown cells compared to glucose-grown cells. In glucose-grown cells, the transport of various amino acids, e.g., proline, glutamic acid, lysine, glycine, phenylalanine, serine, methionine, and leucine was found to be energy dependent and against a concentration gradient. In alkane-grown cells, the transport of lysine, proline, serine, and methionine was reduced, however, there was no effect on the uptake of glycine, glutamic acid, phenylalanine, and leucine. The results were interpreted as different carrier(s) responsible for amino acid uptake responsed differently to the change of lipid environment.     

Nuclear magnetic resonance of E. coli ribosomes and viruses.

¹H Nuclear Magnetic Resonance spectra of a number of viruses and E. Coli ribosomes revealed that experimental values of the linewidth (πT₂)^?1 (< 320 Hz) and T₁ (< 1 sec) of the observable nuclei are too small to be accounted for by the system's molecular weight. The nuclei therefore must be internally mobile. From ¹³C Nuclear Magnetic Resonance spectra of 12% ¹³C enriched E. Coli ribosomes, it follows that 30% of the 5000 $\text{CH}{}_2\text{CH}{}_3$ groups, 10–20% of the 225 Phe residues, 20% of the δ-Arg and β-Lys carbons, ～ 100 nucleotides and a number of C_α carbons are internally mobile. It is demonstrated that ¹³C Nuclear Magnetic Resonance can fruitfully be applied to intact ribosomes.     

NMR study of the structure of short-chain peptides in solution.

The electron-mediated spin–spin coupling constant J between the amide NH and the α-CH protons in the dipeptide fragment C^α? CO(NH? C^αH)R? C′ONH? C^α is dependent on the dihedral angle of rotation (Φ) around the N? C bond. Measurement of J in a series of zwitterionic dipeptides H₃N⁺? CHR₁? CONH? CHR₂? CO₂^? (which is conformationally similar to the dipeptide fragment) in TFA solution shows that J is independent of R₁, but dependent on the steric bulk of R₂. The data are interpreted in terms of a model that assumes that what we measure is an average value of J? a thermal average over all the possible rotamers. The groups R₁ and R₂ are, in most cases, sterically kept apart by the trans and planar amide bonds, and hence the independence of J of R₁. This model is consistent with the theoretical calculations done on the dipeptide fragment. The effect of the structural characteristics of the side chains (e.g., the effect of lengthening and branching the side chains) on the J values in dipeptides is discussed in the light of the existing results of theoretical calculations. Study of 〈J〉 values in tripeptides (C₆H₅CH₂OCONH? CHR₁? CONH? CHR₂? CO₂CH₃, essentially three linked peptide units) shows that electrostatic interaction between the two amide bonds modifies the potential energy surface and the 〈J〉 value of a dipeptide subunit in the tripeptides. Also in some cases, direct steric interaction between the two side chains in the two adjacent dipeptide subunits in the tripeptide affects the potential energy surfaces of the individual dipeptide subunits and hence the 〈J〉 values. The influence of the structural characteristics of the side chains of individual amino acids on structure formation at or beyond the dipeptide level is discussed at various points. The J(NH? ^αCH) values of CH₃CONH? CHR? CONH₂ and CH₃CONH? CHR? CO₂CH₃ with the same R are quite different for R = valine, leucine, phenylalanine, methionine, but equal for R = glycine. This, coupled with the fact that one of the carboxamide NH resonances has a chemical shift different from its counterpart in simple amides like CH₃CONH₂ and the other carboxamide NH has the same chemical shift as its counterpart in CH₃CONH₂, suggest the presence of a hydrogen bond in dipeptide CH₃CONH? CHR? CONH₂ with carboxamide NH as the donor. Theoretical evidence for two seven-membered hydrogen-bonded rings with the carboxamide NH as donor and the acetyl oxygen as acceptor is summarized. Our data cannot suggest the number of such hydrogen-bonded rings, nor can they conclude the relative proportion of these rings in a particular dipeptide. A discussion of the difficulty of interpretation is presented and the data are discussed under certain simplifying assumptions.     

Azaadamantyl nitroxide spin label: complexation with β-cyclodextrin and electron spin relaxation

Abstract

An iodoacetamide azaadamantyl spin label was studied in fluid solution and in 9:1 trehalose:sucrose glass. In 9:1 toluene:CH₂Cl₂ solution at 293 K, the isotropic nitrogen hyperfine coupling is 19.2?G, T₁ is 0.37 µs and T₂ is 0.30–0.35 µs. Between about 80 and 150 K 1/T_m in 9:1 trehalose:sucrose is approximately independent of temperature demonstrating that the absence of methyl groups decreases 1/T_m relative to that which is observed in spin labels with methyl groups on the alpha carbons. Spin lattice relaxation rates between about 80 and 293 K in 9:1 trehalose:sucrose are similar to those observed for other nitroxide spin labels, consistent with the expectation that relaxation is dominated by Raman and local mode processes. Although complexation of the azaadamantyl spin label with β-cyclodextrin slows tumbling in aqueous solution by about a factor of 10, it has little impact on 1/T₁ or 1/T_m in 9:1 trehalose:sucrose between 80 and 293 K.     

1H NMRD studies of solutions of paramagnetic metal ions in ethyleneglycol

Solvent¹H T^?1₁ values at magnetic fields between 2.3 × 10^?4 and 1.2 T were measured for ethyleneglycol solutions of manganese(II), cobalt(II), nickel(II), copper(II), and gadolinium(III) salts in the temperature range ?10–+40 °C. The T^?1₁ profiles were interpreted on the ground of the available theories according to whether the electronic relaxation times or the rotational times are the correlation times for the interaction. The comparison among systems experiencing different correlation times and electronic structures (metal ions in water, ethyleneglycol, and in proteins) allowed us to test the general theoretical approach regarding nuclear relaxation times in paramagnetic systems. Such theoretical approaches allow researchers to extract structural parameters and information on the correlation times and dynamic processes operative in the various investigated systems.     

Intrinsic proton relaxation parameters of hydrated polyglycine from two‐dimensional time domain NMR

Proton two‐dimensional time domain nmr involving T₁, T_1ρ, T_1D, and T₂ measurements was applied to hydrated polyglycine powders. The results were analyzed for magnetization exchange and found to be consistent with a general three‐site (glycine–water–glycine) exchange model. The intrinsic glycine and water proton relaxation parameters as well as the three exchange rates were obtained. Estimates of correlation times for water molecule motion at hydration sites are presented. © 1999 John Wiley & Sons, Inc. Biopoly 50: 630–640, 1999     

Cyclic peptides. XVIII. 13C spin-lattice relaxation times of (X-pro-Y)2 cyclic hexapeptides

¹³C spin-lattice relaxation times (T₁'s) of four cyclic hexapeptides of sequence, (X-L -Pro-Y)₂, are reported. The T₁'s of the protonated carbons, which undergo dipolar relaxation, are interpreted qualitatively in terms of the overall tumbling motion of the molecule and in terms of internal motion. It is found that three of the cyclic hexapeptides, those which adopt all-trans β-conformers, tumble isotropically and appear to lack internal motion in the peptide backbone. The method of Torchia and Lyerla was applied to these compounds in order to compare the mobility of the proline rings. The results show that the sequence and particular type of β-turn present affect the internal motion of the Pro ring. Data on a fourth cyclic hexapeptide, which occurs in a conformation with two-cis X-Pro bonds, suggests that internal motion of the backbone contributes an additional frequency component to the motion of the Y residue α-carbons. A consideration of the mobility of the proline rings in the conformer with two-cis peptide bonds revealed that they are significantly more rigid in the two-cis structure than in the all-trans.     

Cross-correlation suppressed T1 and NOE experiments for protein side-chain 13CH2 groups

Relaxation measurements of side-chain ¹³CH₂-groups of uniformly ¹³C labeled human ubiquitin were performed at 600 MHz and 800 MHz magnetic field strength at 30°C. Dipole-dipole cross-correlated relaxation effects in T₁ experiments were suppressed by the combination of radio-frequency pulses and pulsed field gradients during the relaxation delay leading to monoexponential relaxation decays that allow a more accurate extraction of the ¹³C T₁ relaxation times. Heteronuclear ¹H-¹³C NOEs obtained by using different proton saturation schemes indicate that the influence of cross-correlation is small. The experimental T₁ and NOE data were interpreted in a model-free way in terms of a generalized order parameter and an internal correlation time.     

Determination of 13Cα relaxation times in uniformly 13C/15N-enriched proteins

Summary Relaxation times of ¹³C carbons of uniformly ¹³C/¹⁵N-enriched probes have been investigated. The relaxation behaviour was analyzed in terms of a multispin system. Pulse sequences for the determination of T₁, T₂ and the heteronuclear NOE of ¹³C in uniformly ¹³C/¹⁵N-enriched ribonuclease T1 are presented. The experiments performed in order to obtain T₁ and the heteronuclear NOE were similar to those of the corresponding ¹⁵N experiments published previously. The determination of T₂ for the C-carbon in a completely labeled protein is more complicated, since the magnetization transfer during the T₂ evolution period owing to the scalar coupling of C–C must be suppressed. Various different pulse sequences for the T₂ evolution period were simulated in order to optimize the bandwidth for which reliable T₂ relaxation times can be obtained. A proof for the quality of these pulse sequences is given by fitting the intensity decay of individual ¹H–¹³C cross peaks, in a series of (¹H, ¹³C)-ct-HSQC spectra with a modified CPMG sequence as well as a T_1p sequence for the transverse relaxation time, to a single exponential using a simplex algorithm.     

Effects of molecular association on structure and dynamics of a collagenous peptide

Peptide GVKGDKGNPGWPGAPY from the triple-helix domain of type IV collagen aggregates in solution at a critical aggregation concentration of 18 mM. This molecular self association process is investigated by ¹H- and ¹³C-nmr spectroscopy. As a function of increasing peptide concentration, selective ¹H resonances are cooperatively chemically shifted by up to 0.04 ppm to apparently saturable values at high concentration. Pulsed field gradient nmr was used to derive translation diffusion constants that, as the peptide concentration is increased, also cooperatively and monotonically decrease to an apparent limiting value. An average number of 6 monomer units per aggregate have been estimated from diffusion constant and ¹³C relaxation data. Comparative ¹H nuclear Overhauser effect spectroscopy (NOESY) spectra accumulated at high and low peptide concentrations suggest that average internuclear distances are decreased as a result of peptide association. ¹³C-nmr multiplet spin-lattice relaxation and ¹³C- {¹H} NOE effects on ¹³C-enriched glycine methylene positions in the peptide demonstrate that overall molecular tumbling and backbone internal motions are attenuated in the aggregate state. Lowering the solution pD from pD 6 to pD 2 disrupts the aggregate state, suggesting a role for electrostatic interactions in the association process. Based on thermodynamic considerations, hydrophobic interactions also probably act to stabilize the aggregate state. These data are discussed in terms of an nmr/NOE constrained computer-modeled structure of the peptide. © 1993 John Wiley & Sons, Inc.     

Structural versatility of peptides from Cα, α-disubstituted glycines: Crystal-state conformational analysis of homopeptides from Cα-methyl,Cα-benzylglycine [(αMe)Phe]n

The molecular and crystal structures of one derivative and three homopeptides (from the di-to the tetrapeptide level) of the chiral, C^{α, α}-disubstituted glycine C^α-methyl, C^α-benzylglycine [(αMe)Phe], have been determined by x-ray diffraction. The derivative is mClAc-D -(αMe)Phe-OH, and the peptides are pBrBz-[D -(αMe)Phe]₂-NHMe, pBrBz-[D -(αMe)Phe]₃-OH hemihydrate, and pBrBz-[D -(αMe)Phe]₄-OtBu sesquihydrate. All (αMe)Phe residues prefer ?,ψ torsion angles in the helical region of the conformational map. The dipeptide methylamide and the tripeptide carboxylic acid adopt a β-turn conformation with a 1 ← 4 C?O…?H? N intramolecular H bond. The structure of the tripeptide carboxylic acid is further stabilized by a 1 ← 4 C?O…?H? O intramolecular H bond, forming an “oxy-analogue” of a β-turn. The tetrapeptide ester is folded in a regular (incipient) 3₁₀-helix. In general, the relationship between (αMe)Phe chirality and helix screw sense is opposite to that exhibited by protein amino acids. A comparison is made with the conclusions extracted from published work on homopeptides from other C^α-methylated α-amino acids. © 1993 John Wiley & Sons, Inc.     

Nuclear magnetic resonance investigation of lysine–oligopeptides and a complex with d(pA)3pGpC(pT)3

We report proton magnetic resonance studies of a series of lysine oligopeptides in H₂O solution. At pH 5 the protonated ε-amino groups are seen as broad resonances; the peptide NH proton resonances are split by spin–spin coupling with the C^α-H proton, and appear at positions which depend on position in the chain and on chain length. Assignments were made by the europium shift method, and we observed the expected effect of catalysis by the terminal —NH₃⁺ of exchange of the adjacent peptide NH. Coupling constants and the temperature coefficient of chemical shift values were consistent with a non-hydrogen-bonded structure for the oligolysines. The rate and mechanism of NH hydrogen exchange were investigated by line-broadening measurements of the peptide protons as a function of pH. Exchange was found to be OH^? catalyzed, with large differences in the rate depending on position in the chain. Preliminary studies of the complex between double-helical d(pA)₃pGpC(pT)₃ and tetra(L -lysine) were performed using ¹H- and ³¹P-nmr techniques. Pmr spectra of the complex at pH values ranging from 3.98 to 8.15 showed very complicated patterns. Downfield shifts and reduction in exchange rates were observed for several tetra(L -lysine) protons. ³¹P-nmr spectra of the complex reveal an upfield shift of 1 ppm for 3′-5′ phosphate diester resonances on complexation. ³¹P T₁ relaxation times change little on complex formation at low temperature but are altered at higher temperature.     

CPMG relaxation dispersion NMR experiments measuring glycine 1Hα and 13Cα chemical shifts in the ‘invisible’ excited states of proteins

Carr-Purcell-Meiboom-Gill (CPMG) relaxation dispersion NMR experiments are extremely powerful for characterizing millisecond time-scale conformational exchange processes in biomolecules. A large number of such CPMG experiments have now emerged for measuring protein backbone chemical shifts of sparsely populated (>0.5%), excited state conformers that cannot be directly detected in NMR spectra and that are invisible to most other biophysical methods as well. A notable deficiency is, however, the absence of CPMG experiments for measurement of ¹H^α and ¹³C^α chemical shifts of glycine residues in the excited state that reflects the fact that in this case the ¹H^α, ¹³C^α spins form a three-spin system that is more complex than the AX ¹H^α–¹³C^α spin systems in the other amino acids. Here pulse sequences for recording ¹H^α and ¹³C^α CPMG relaxation dispersion profiles derived from glycine residues are presented that provide information from which ¹H^α, ¹³C^α chemical shifts can be obtained. The utility of these experiments is demonstrated by an application to a mutant of T4 lysozyme that undergoes a millisecond time-scale exchange process facilitating the binding of hydrophobic ligands to an internal cavity in the protein.     

Molecular mobility of polypeptides containing proline as determined by 13C magnetic resonance

The molecular conformations and dynamics of poly(L -prolyl), poly(hydroxyl-L -prolyl), poly(L -prolyl-glycyl), poly(hydroxyl-L -prolyl), and poly(glycyl-glycyl-L -prolyl-glycyl), in aqueous solution, have been studied using ¹³C pulse Fourier transform nmr spectroscopy. From a measurement of the intensities of major and minor resonances in the spectra of the copolypeptides, it was determined that 15–20% of the glycyl-prolyl and glycyl-hydroxyprolyl peptide bonds are cis. Effective rotational correlation times (τ_eff), obtained from measurements of spin-lattice relaxation times (T₁) of individual backbone and side-chain carbons, demonstrated that backbone reorientation is approximately isotropic for the five polypeptides and is characterized by correlation times of ca. 0.3–0.6 nanoseconds as a result of rapid segmental motion. In a given polypeptide glycyl and pyrrolidine residues were found to have the same backbone correlation times, but backbone carbon τ_eff values did decrease as the glycyl content of the peptides increased. A semi-quantitative analysis of C^β, C^γ, and C^δ correlation times suggests that rapid ring motion in both prolyl and hydroxyprolyl involves primarily C^γ and C^β, with the prolyl ring being more mobile than the hydroxyprolyl ring.