Why are monomeric lithium amides planar?
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Biomedical subjects
Publications and source records attributed to C Giessner-Prettre.
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A DFT analysis of the condensation of monomeric methyllithium and lithium dimethylamide (LMA), as well as their homo and hetero dimers, on formaldehyde and acetaldehyde is reported. A stable complex, exhibiting a directional interaction between a lone pair of the oxygen on the aldehyde and a lithium, is first found. At this stage, the aldehyde carbonyl and the Li-X (X = C or N) bonds lie in the same plane. To proceed, the condensation reaction has to go through a transition state that mainly consists of a rotation of the aldehyde plane, placing it perpendicular to the C-C or C-N forming bond. The reaction then leads, in a strongly exothermic final step, to the addition product that is a lithium alcoholate or alpha-amino alcoholate, associating into an hetero-aggregate with the remaining moiety of the initial dimer. From the relative heights of the activation barriers, it appears that, for the heterodimer MeLi-LMA, the formation of the C-N bond should be kinetically favored over the C-C one, while the lithium ethylate resulting from the C-C binding is the thermodynamic product. A decomposition of the activation energy barriers has been carried out in order to determine the physicochemical forces responsible for the variation of the condensation activation barriers with the structure of the final species formed. The results obtained are discussed in relation with corresponding experimental data.
Extended Huckel theory calculations have been carried out on a model of the oxyhemocyanin active site that includes six imidazoles, the two copper cations, and a dioxygen molecule. The results obtained for the very likely mu-eta 2:eta 2 arrangement of the dioxygen molecule show that the most favorable orientation of O2 is such that the two long Cu-N coordination bonds are perpendicular to the plane formed by the two metal atoms and O2. This arrangement leads to pentacoordinated coppers with a distorted square pyramidal geometry. The molecular electrostatic potential maps of the complexes exhibit a potential well located close to the peroxo anion midbond. The dependence of the energy and of the molecular electrostatic maps on the precise orientation and location of the imidazole rings has been investigated. These results, which show the important role played by the third remote imidazole ligand, are discussed in relation with the first step of tyrosinase-mediated phenol oxidation.
The sum of the magnetic anisotropy and polarization contributions to the magnetic shielding constants of the alpha protons is calculated as a function of the torsion angles about the NC alpha (phi) and C alpha C' (psi) bonds of the dipeptide. The results show that the polarization or electric field effect is several fold larger than the magnetic anisotropy contribution. The calculated variations are large enough to account for the spread of the values measured for these protons in peptides and proteins. The results obtained for polyglycine alpha helices and antiparallel beta sheets are discussed in relation with molecular conformation and environmental effects on the one hand and experimental data on the other.
The binding energy and the geometrical arrangements of the complexes formed by the zinc dication with OH-, one, four, five or six water molecules, SH-, H2S, formic acid, the formate anion, imidazole, its anion and formamide are calculated using the MNDO method. The comparison of the results obtained with those of ab initio computations on the same complexes induced us to propose for Zn++ a set of parameters different from the one determined by Dewar for the neutral metal atom. Using the two MNDO parametrizations, similar calculations are carried out for Zn++ interacting with two molecules of 2-aminoethanethiol and with models of the four ligands which are present at the thermolysin active site, in order to evaluate the possibilities and limitations of this semiempirical method for theoretical studies concerning zinc metalloenzymes. In the last case, the results obtained suggest that, in the crystal state, the water molecule could be deprotonated. This finding is discussed in relation with the mechanism of action of the enzyme which has been proposed.
The aim of this study was to attempt to determine the extent to which the chemical shifts of the nonexchangeable base protons of a DNA helix depend upon the base sequence. We measured the proton NMR spectra of twelve decadeoxynucleotides in order to carry out a "statistical" treatment. In the helices, the chemical shifts were found to be determined within +/- 0.04 ppm, largely by the nearest neighbor residues on the 5'-side, and to a smaller extent by the residue on the 3'-side. The theoretical chemical shift calculations reproduced very well the polymerization shifts measured for H2 protons of adenosines if the electrostatic field effect was taken into account. A fair agreement was also obtained for H8 protons of the adenosine and guanosine residues. However, theory underestimates the polarization effects of the base protons of cytidine. This discrepancy suggests that the conformation of this residue is different in the mononucleotides relative to double helices.
The variation of the nuclear magnetic shielding constant of the different protons and carbons of trans HCO-L-Pro-NH2 with the value of the angle psi is calculated by a non-empirical method for three conformations of the proline ring. The results concerning the CH protons show that the chemical shift of the alpha, beta and gamma endo hydrogens can vary by more than 1 ppm when psi goes from -30 degrees to 180 degrees. The theoretical variation of the chemical shift difference between alpha and gamma or beta and gamma carbons is found to be sensitive to the puckering of the proline ring. For the second of these differences the theoretical results are in agreement with Siemion's relation only for a limited range of molecular conformations. Additional calculations show that the variations of the proton shifts with the value of psi are due to the magnetic anisotropy of the proline carbonyl group and to the polarization of the CH bonds by the multipolar charge distribution carried by this carbonyl. The results are discussed in relation to experiment and the possibility of using 1H and 13C chemical shifts for the determination of the value of the torsion angle about the C alpha C' bond.
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Ab inito computations of the different contributions to chemical shift variations due to intra and interstrand stacking are reported for the GC, CG, AT and TA sequences of a B DNA helix. The results obtained for the non hydrogen atoms of the GC stacks show that the chemical shift variations are mainly due to the polarization contribution, the term which decreases slowly with the intermolecular distance. Because of the weaker polarity of adenine and thymine the geometric and polarization contributions are of closer absolute magnitude for the non hydrogen atoms of the intrastrand stacks but the polarization term is the determining contribution in the corresponding interstrand stacks. For the protons which undergo smaller shifts due to the polarization (or electric field effects) the role of the geometric contribution is more important and is even the leading one for the hydrogens of cytosine and thymine in the case of intrastrand stacking. The charge transfer plus exchange term has a non negligeable value for a limited number of cases corresponding to the shortest intermolecular interatomic distances. These results are discussed in relation with the qualitative differences observed between the proton and carbon spectra of dinucleotides and B-DNA duplexes.
The magnetic shielding constant of the different 13C and 1H nuclei of a deoxyribose are calculated for the C2' endo and C3' endo puckerings of the furanose ring as a function of the conformation about the C4'C5' bond. For the carbons the calculated variations are of several ppm, the C3' endo puckering corresponding in most cases to a larger shielding than the C2' endo one. For the protons the calculated variations of chemical shifts are all smaller than 1.3 ppm, that is of the order of magnitude of the variation of the geometrical shielding produced on these protons by the other units of a DNA double helix, with a change of the overall structure of the helix. The computations carried out on the deoxyribose-3' and 5' phosphates for several conformations of the phosphate group tend to show that the changes of conformation of the charged group of atoms produce chemical shift variations smaller than the two conformational parameters of the deoxyribose itself. The calculations carried out for a ribose do give the general features of the differences between the carbon and proton spectra of deoxynucleosides and nucleosides. The comparison of the measured and calculated phosphorylation shifts tend to show that the counterion contributes significantly, for some nuclei of the deoxyribose, to the shifts measured. The calculated magnitude of this polarization effect on carbon shifts suggests a tentative qualitative interpretation of carbon spectra of the ribose part of DNA double helices.
The magnetic shielding produced by the double helix in a B-DNA and a Z-DNA conformation is calculated for each non exchangeable proton of the oligodeoxynucleotides d(CGm5CG)2 and d(CGm5CGCG)2. The differences between the values obtained for the two helical forms are in good agreement with the variations of chemical shift measured when the salt concentration of the solution is changed from 0.1 M to 2 or 4 M. The analysis of the theoretical chemical shift variations shows that the large upfield shift observed for some of the protons of the cytidine residues is due to the sum of the ring current and local magnetic anisotropy effects of the guanines of the two nearest neighbours residues.
NMR shielding constants are calculated for the base protons of duplexes formed by the dodecamer d(CGTGAATTCGCG) and the decamer d(CCAAGATTGG). A good agreement with experimental data is obtained for B-DNA helices in which the wobble GT and GA pairs are in the plane of the corresponding GC pairs of the parent duplexes formed by d(CGCGAATTCGCG) and d(CCAAGCTTGG), if the glycosyl bonds of T and G or A and G are symmetrical with respect to the dyad axis of the Watson-Crick GC pair. Interaction energy calculations show that this type of geometrical arrangement, which implies a distortion of the ribonphosphate backbone of both strands of the duplexes are more stable than those in which only one strand has its conformation modified by the presence of the wobble pair. For the duplex containing the GA pair, NMR chemical shifts as well as interaction energy computations favour the Watson-Crick hydrogen bonding scheme. The variation of the different contributions (intrastrand, interstrand, pair-pair) to the interaction energy between the bases of the duplexes, with the geometrical arrangement of the wobble pairs, is reported.
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The magnetic shielding constants of the different nuclei of the four nucleic acid bases adenine, uracile, guanine and cytosine are calculated by a non empirical method using a minimal basis set and compared to the available corresponding experimental data. The same calculations carried out for AU and GC pairs give not only the values of the chemical shift variations due to the formation of the pairs but also the relative importance of the three different contributions (geometric, polarization and charge transfer plus exchange) to the total value of delta delta. Their analysis shows the importance of the polarization term. The magnitude of the charge transfer plus exchange term which is obtained for the nuclei belonging to the hydrogen bonding sites indicates that the hydrogen bond length is the major factor in the determination of the magnetic shielding constants of these atoms. On the other hand it appears that the pairing of the bases has a negligible effect on the "geometric" magnetic shielding due to the bases.
The difference between their shielding in a B-DNA duplex and in the single strand having the same conformation has been calculated for all base protons of the dodecamers d-(CGCGAATTCGCG) and d-(CGCGTATACGCG). The calculated chemical shift variations reproduce the qualitative features of the shifts which occur during the pre-melting of the helices. This agreement shows that the pre-melting mechanism consists mainly of a lengthening of the hydrogen bonds between the two strands (in line opening) and that the conformation of the ribophosphate backbone and the orientation of the bases do not undergo major modifications during the first step of the melting.
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Arguments are presented which show that conformations II and III proposed by Lee and Tinoco [Lee, C.H., and Tinoco, I., Jr. (1977), Biochemistry 16, 5403] for ribodinucleoside monophosphates in aqueous solution are untenable. It has been shown that ribodinucleoside monophosphates exist in aqueous solution as an equilibrium blend of the classically recognized right-handed stack (g-g-), loop stack (g+g+), skewed (g+t), and extended arrays. In order to determine the effect of epsilonA base on the conformer distribution in the equilibrium blend, detailed ring-current calculations were performed and the isoshielding curves for epsilonA were derived. Use of these curves vis-a-vis dimerization shift data indicates that introduction of epsilonA perturbs the equilibrium blend which causes an increase in the population of skewed (g+t) arrays.