Theoretical study of the triangular bonding complex formed by carbon tetrabromide, a halide, and a solvent molecule in the gas phase

MP2(full)/aug-cc-pVDZ(-PP) computations predict that new triangular bonding complexes (where X^? is a halide and H–C refers to a protic solvent molecule) consist of one halogen bond and two hydrogen bonds in the gas phase. Carbon tetrabromide acts as the donor in the halogen bond, while it acts as an acceptor in the hydrogen bond. The halide (which commonly acts as an acceptor) can interact with both carbon tetrabromide and solvent molecule (CH₃CN, CH₂Cl₂, CHCl₃) to form a halogen bond and a hydrogen bond, respectively. The strength of the halogen bond obeys the order CBr₄???Cl^? > CBr₄???Br^? > CBr₄???I^?. For the hydrogen bonds formed between various halides and the same solvent molecule, the strength of the hydrogen bond obeys the order C-H???Cl^? > C-H???Br^? > C-H???I^?. For the hydrogen bonds formed between the same halide and various solvent molecules, the interaction strength is proportional to the acidity of the hydrogen in the solvent molecule. The diminutive effect is present between the hydrogen bonds and the halogen bond in chlorine and bromine triangular bonding complexes. Complexes containing iodide ion show weak cooperative effects.

Effect of superalkali substituents on the strengths and properties of hydrogen and halogen bonds

Quantum chemical calculations have been performed for the complexes Li₃OCCX–Y (X?=?Cl, Br, H; Y?=?NH₃, H₂O, H₂S) and Li₃OCN–X′Y′ (X′Y′?=?ClF, BrCl, BrF, HF) to study the role of superalkalis in hydrogen and halogen bonds. The results show that the presence of an Li₃O cluster in a Lewis acid weakens its acidity, while its presence in a Lewis base enhances its basicity. Furthermore, the latter effect is more prominent than the former one, and the presence of an Na₃O cluster causes an even greater effect than Li₃O. The strengths of hydrogen and halogen bonds were analyzed using molecular electrostatic potentials. The contributions of superalkalis to the strength of hydrogen and halogen bonds were elucidated by analyzing differences in electron density.     

Interplay between halogen bonds and hydrogen bonds in OH/SH···HOX···HY (X = Cl, Br; Y = F, Cl, Br) complexes

The character of the cooperativity between the HOX···OH/SH halogen bond (XB) and the Y―H···(H)OX hydrogen bond (HB) in OH/SH···HOX···HY (X = Cl, Br; Y = F, Cl, Br) complexes has been investigated by means of second-order Møller?Plesset perturbation theory (MP2) calculations and “quantum theory of atoms in molecules” (QTAIM) studies. The geometries of the complexes have been determined from the most negative electrostatic potentials (V _S,min) and the most positive electrostatic potentials (V _S,max) on the electron density contours of the individual species. The greater the V _S,max values of HY, the larger the interaction energies of halogen-bonded HOX···OH/SH in the termolecular complexes, indicating that the ability of cooperative effect of hydrogen bond on halogen bond are determined by V _S,max of HY. The interaction energies, binding distances, infrared vibrational frequencies, and electron densities ρ at the BCPs of the hydrogen bonds and halogen bonds prove that there is positive cooperativity between these bonds. The potentiation of hydrogen bonds on halogen bonds is greater than that of halogen bonds on hydrogen bonds. QTAIM studies have shown that the halogen bonds and hydrogen bonds are closed-shell noncovalent interactions, and both have greater electrostatic character in the termolecular species compared with the bimolecular species.

Hydrogen bonds determine the structures of the ternary heterocyclic complexes C₂H₄O···2HF, C₂H₅N···2HF and C₂H₄S···2HF: density functional theory and topological calculations

A theoretical study of structural, electronic, topological and vibrational parameters of the ternary hydrogen-bonded complexes C₂H₄O···2HF, C₂H₅N···2HF and C₂H₄S···2HF is presented here. Different from binary systems with a single proton donor, the tricomplexes have the property of forming multiple hydrogen bonds, which are analyzed from a structural and vibrational point of view, but verified only by means of the quantum theory of atoms in molecules (QTAIM). As traditionally done in the hydrogen bond theory, the charge transfer between proton donors and acceptors was computed using the CHELPG calculations, which also revealed agreement with dipole moment variation and a cooperative effect on the tricomplexes. Furthermore, redshift events on proton donor bonds were satisfactorily identified, although, in this case, an absence of experimental data led to the use of a theoretical argument to interpret these spectroscopic shifts. It was therefore the use of the QTAIM parameters that enabled all intermolecular vibrational modes to be validated. The most stable tricomplex in terms of energy was identified via the strength of the hydrogen bonds, which were modeled as directional and bifurcated.     

Chalcogen- and halogen-bonds involving SX<Subscript>2</Subscript> (X = F,Cl, and Br) with formaldehyde

The capacity of SX₂ (X = F, Cl, and Br) to engage in different kinds of noncovalent bonds was investigated by ab initio calculations. SCl₂ (SBr₂) has two σ-holes upon extension of Cl (Br)?S bonds, and two σ-holes upon extension of S?Cl (Br) bonds. SF₂ contains only two σ-holes upon extension of the F?S bond. Consequently, SCl₂ and SBr₂ form chalcogen and halogen bonds with the electron donor H₂CO while SF₂ forms only a chalcogen bond, i.e., no F···O halogen bond was found in the SF₂:H₂CO complex. The S···O chalcogen bond between SF₂ and H₂CO is the strongest, while the strongest halogen bond is Br···O between SBr₂ and H₂CO. The nature of these two types of noncovalent interaction was probed by a variety of methods, including molecular electrostatic potentials, QTAIM, energy decomposition, and electron density shift maps. Termolecular complexes X₂S···H₂CO···SX′₂ (X = F, Cl, Br, and X′ = Cl, Br) were constructed to study the interplay between chalcogen bonds and halogen bonds. All these complexes contained S···O and Cl (Br)···O bonds, with longer intermolecular distances, smaller values of electron density, and more positive three-body interaction energies, indicating negative cooperativity between the chalcogen bond and the halogen bond. In addition, for all complexes studied, interactions involving chalcogen bonds were more favorable than those involving halogen bonds.

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Graphical Abstract Molecular electrostatic potential and contour map of the Laplacian of the electron density in Cl₂S···H₂CO···SCl₂ complex

     

A theoretical study on the halogen bonding interactions of C6F5I with a series of group 10 metal monohalides

The halogen bonding interactions between C₆F₅I and a series of transition metal monohalides trans-[M(X)(2-C₅NF₄)-(PR₃)₂] (M = Ni, Pd, Pt; X = F, Cl, Br; R = Me, Cy) have been studied with quantum chemical calculations. Optimized geometries of the halogen bonding complexes indicate that angles C₁-I···X are basically linear (178–180°) and angles I···X-M mainly range from 90 to 150°. The strength of these metal-influenced halogen bonds alters with different metal centers, metal-bound halogen atoms and the substitutes on phosphine ligands. Electrostatic potential and natural bond orbital analysis show that both of the electrostatic and orbital interactions make a contribution to the formation of halogen bonds, while the electrostatic term plays a dominant role. AIM analysis suggests that, for trans-[M(F)(2-C₅NF₄)-(PR₃)₂] (M = Ni, Pd, Pt) monomers, the formed halogen bonding complexes are stabilized by local concentration of the charge of intermediate character, while for the metal monomers containing chlorine and bromine, a typical closed-shell interaction exist. These results prove that the structures and geometries of these halogen bonding complexes can be tuned by changing the halogen atoms and metal centers, which may provide useful information for the design and synthesis of new functional materials.

Structures and properties of octaethylporphinato(phenolate)iron(III) complexes with NH?O hydrogen bonds: modulation of Fe-O bond character by the hydrogen bond

Iron(III) porphinate complexes of phenolate that have NH?O hydrogen bonds on the coordinating oxygen, [Fe^III(OEP){O-2,6-(RCONH)₂C₆H₃}] (R = CF₃ (1), CH₃ (3)) and [Fe^III(OEP)(O-2-RCONHC₆H₄)] (R = CF₃ (2), CH₃ (4)) (OEP = 2,3,7,8,12,13,17,18-octaethyl-21H, 23H-porphinato), were synthesized and characterized as models of heme catalase. The presence of NH?O hydrogen bonds was established by their crystal structures and IR shifts of the amide NH band. The crystal structure of 1 shows an extremely elongated Fe-O bond, 1.926(3) Å, compared to 1.887(2) Å in 2 or 1.848(4) Å in [Fe^III(OEP)(OPh)]. The NH?O hydrogen bond decreases an electron donation from oxygen to iron, resulting in a long Fe-O bond and a positive redox potential.     

The molecular properties of heterocyclic and homocyclic hydrogen-bonded complexes evaluated by DFT calculations and AIM densities

This theoretical study presents a comparative analysis of the molecular properties of heterocyclic (C₂H₄O⋯HF and C₂H₅N⋯HF) and homocyclic (C₃H₆⋯HF) hydrogen-bonded complexes. Initially, the equilibrium geometries of these complexes were analyzed in detail at the B3LYP/6–311++G(d,p) level of theory. Subsequently, the interaction energies and polarizabilities were also evaluated, as well as the infrared stretch frequencies and absorption intensities. In addition, by combining intermolecular criteria and charge density concepts, calculations of Bader’s theory of atoms in molecules were used to determine the maxima and minima for electron density in order to measure the strength of the n⋯H and pπ⋯H hydrogen bonds. Finally, the possibility of an F⋯H_α secondary interaction between the fluoride (F) of hydrogen fluoride and the axial hydrogen atoms (H_α) of the C₂H₄O and C₂H₅N heterocyclic rings was explored. Electronic supplementary material  The online version of this article (doi:) contains supplementary material, which is available to authorized users.     

Preparation and characterization of two supramolecular complexes with 5-amino-2,4,6-triiodoisophthalic acid under N-donor auxiliary ligand intervention

Assemblies of 5-amino-2,4,6-triiodoisophthalic acid (H₂ATIBDC) with Cd(II) and Zn(II) in the presence of N-donor auxiliary ligand, 1,4-bis(1,2,4-triazol-1-yl)butane (btb), at ambient conditions yield two new supramolecular complexes, [Cd(ATIBDC)(btb)(H₂O)₂]·3H₂O (1), and [Zn(ATIBDC)(btb)]·2H₂O (2). Generally, these two complexes display 1D ATIBDC²⁻-bridged coordination arrays. Distinct extended 3D network architectures are further constructed with the help of weak secondary interactions especially aromatic stacking, halogen bonding, and hydrogen bonding as supramolecular driving forces. It is worthy to mention that halogen bonds (C-I?π and C-I?N/O) play important roles in the supramolecular assembly. The pentameric cluster (H₂O)₅ in 1 assembles into highly ordered helical infinite chains. Complex 2 exhibits the fascinating single-walled tube-like chain structure. It loses crystallinity rapidly in the air and leads to the formation of [Zn(ATIBDC)(btb)]·H₂O (2A). Thermal stabilities and solid state fluorescent properties of complexes 1 and 2A have been studied.     

The hydrogen bonding of cytosine with guanine: calorimetric and 1H-nmr analysis of the molecular interactions of nucleic acid bases

The enthalpy of hydrogen-bond formation between guanine (G) and cytosine (C) in o-dichlorobenzene and in chloroform at 25°C has been determined by direct calorimetric measurement. We derivatized 2′-deoxyguanosine and 2′-deoxycytidine at the 5′- and 3′-hydroxyls with triisopropylsilyl groups; these groups increase the solubility of the nucleic acid bases in nonaqueous solvents. Such derivatization also prevents the ribose hydroxyls from forming hydrogen bonds. Consequently, hydrogen-bond formation in our system is primarily between the bases, and to a lesser extent, between base and solvent, and can be measured directly with calorimetry. To obtain the data on base-pair formation, we first took into account the contributions from self-association of each base, and where possible, have determined the ΔH of self-association. From isoperibolic titration calorimetry, our measured ΔH of C₂ formation in chloroform is ?1.7 kcal/mol of C. Our measured ΔH of C:G base-pair formation in o-dichlorobenzene is ?6.65 ± 0.32 kcal/mol. Since o-dichlorobenzene does not form hydrogen bonds, the ΔH of C:G base-pair formation in this solvent represents the ΔH of the hydrogen-bonding interaction of C with G in a nonassociating solvent. In contrast, our measured ΔH of C:G base-pair formation in chloroform is ?5.77 ± 0.20 kcal/mol; thus, the absolute value of the enthalpy of hydrogen bonding in the C:G base pair is greater in o-dichlorobenzene than in chloroform. Since chloroform is a solvent known to form hydrogen bonds, the decrease in enthalpic contribution to C:G base pairing in chloroform is due to the formation of hydrogen bonds between the bases and the solvent. The ΔH of hydrogen bonding of G with C reported here differs from previous indirect estimates: Our measurements indicate the ΔH is 50% less in magnitude than the ΔH based on spectroscopic measurements of the extent of interaction. We have also observed that the enthalpy of hydrogen bonding of C with G in chloroform is greater when G is in excess than when C is in excess. This increased heat is due to the formation of C:G_{n > 1} complexes that we have observed using ¹H-nmr. Although C:G₂ structures have previously been observed in triple-stranded polymeric nucleic acids, higher order structures have not been observed between C and G monomers in nonaqueous solvents until now. By using monomers as a model system to investigate hydrogen-bonding interactions in DNA and RNA, we have obtained the following results: A direct measurement of the ΔH of hydrogen bonding in the C:G complex in two nonaqueous solvents, and the first observation of C:G_{n > 1} complexes between monomers. These results reinforce the importance of hydrogen bonding in the stabilization of various nucleic acid secondary and tertiary structures.     

Theoretical investigations on circular and chain-like hydrogen bonded structures found in two crystal forms of α-cyclodextrin hexahydrate: Models for hydration and water clusters

Hydration of macromolecules and the structure of water of crystallization are not understood in detail because in these complex systems. H-atoms cannot be located and the hydrogen bonding schemes are not known. X-ray and neutron diffraction studies on a hydrated oligosaccharide, α-cyclodextrin 6H₂O, ((C₆H₁₀O₅)₆·6H₂O), crystals forms A and B, gave insight into the chain-like and circular arrangement of hydrogen bonds. In the circles, homodromic (unidirectional) and antidromic (counter-running) orientation of five to six hydrogen bounds is observed. PCILO calculations showed that homodromic circles and chains are approx. 8% per hydrogen bond more stable than antidromic circles, that the changes in electronic charges on H and O atoms are greater in homo than in antidromic systems and that the dipole moments are only approx. 3 D in the homodromic circles but 6–8 D in chain-like and antidromic arrangement. These results have been interpreted in terms of cooperative effect. Circular systems are considered as structural elements in hydration shells of macromolecules and in the assembly of ‘flickering’ water clusters.     

Ab Initio Quantum Mechanics Analysis of Imidazole C-H…O Water Hydrogen Bonding and a Molecular Mechanics Forcefield Correction

Abstract

While it is well established that classical hydrogen bonds play an important role in enzyme structure, function and dynamics, the role of weaker, but ‘activated’ C-H donor hydrogen bonds is poorly understood. The most important such case involves histidine which often plays a direct role in enzyme catalysis and possesses the most acidic C-H donor group of the standard amino acids. In the present study, we obtained optimized geometries and hydrogen bond interaction energies for C-H…O hydrogen bonded complexes between methane, ethylene, benzene, acetylene, and imidazole with water at the MP2-FC/6-31++G(2d,2p) and MP2-FC/aug-cc-pVDZ//MP2-FC/6-31++G(2d,2p) levels of theory. A strong linear relationship is obtained between the stability of the various hydrogen bonded complexes and both separation distances for H…0 and C—O. In general, these calculations indicate that C-H…0 interactions can be classified as hydrogen bonding interactions, albeit significantly weaker than the classical hydrogen bonds, but significantly stronger than just van der Waals interactions. For instance, while the electronic energy of stabilization at the MP2-FC/aug-cc-pVDZ//MP2-FC/6-31++G(2d,2p) level of theory of a water C-H…O water hydrogen bond is 4.36 kcal/mol more stable than the methane C-H…O water interaction, the water-water hydrogen bond is only 2.06 kcal/mol more stable than the imidazole C_e?H…O water hydrogen bond. Neglecting this latter hydrogen bonding interaction is obviously unacceptable. We next compare the potential energy surfaces for the imidazole C_e?H…O water and imidazole N_d?H…O hydrogen bonded complexes computed at the MP2/6-31++G(2d,2p) level of theory with the potential energy surface computed using the AMBER molecular mechanics program and forcefields. While the Weiner et al and Cornell et al AMBER forcefields reasonably account for the imidazole N-H…O water interaction, these forcefields do not adequately account for the imidazole C_e?H…O water hydrogen bond. A forcefield modification is offered that results in excellent agreement between the ab initio and molecular mechanics geometry and energy for this C-H…O hydrogen bonded complex.     

A rare supramolecular assembly (stairs) of (cyclic tellurane) 1,3-dihydro-2λ-benzotellurole-2,2-diyldicinnamate [C8H8Te(OCOCHCHC6H5)2] based on intermolecular and intramolecular Te-O secondary bonds and assisted by C-H-O hydrogen bonds

Stairs of cyclic tellurane (1,3-dihydro-2λ⁴-benzotellurole-2,2-diyldicinnamate) [C₈H₈Te(OCOCHCHC₆H₅)₂] 1 assisted by intermolecular Te-O secondary bonds, intramolecular Te-O secondary bonds and C-H-O hydrogen bonds have been obtained. 1 accounts for the rare example, in organotellurium chemistry, containing both intermolecular and intramolecular Te-O secondary bonds acting as crystal structure directors to yield stair type supramolecular association assisted by CH-O hydrogen bonds.     

Differential Stability of the Triple Helix of (Pro-Pro-Gly)10 in H2O and D2O: Thermodynamic and Structural Explanations

Abstract

(Pro-Pro-Gly)₁₀ [(PPG₁₀)], a collagen-like polypeptide, forms a triple-helical, polyproline-II structure in aqueous solution at temperatures somewhat lower than physiological, with a melting temperature of 24.5°C. In this article, we present circular dichroism spectra that demonstrate an increase of the melting temperature with the addition of increasing amounts of D₂O to an H₂O solution of (PPG)₁₀, with the melting temperature reaching 40°C in pure D₂O. A thermodynamic analysis of the data demonstrates that this result is due to an increasing enthalphy of unfolding in D₂O vs. H₂O. To provide a theoretical explanation for this result, we have used a model for hydration of (PPG)₁₀ that we developed previously, in which inter-chain water bridges are formed between sterically crowded waters and peptide bond carbonyls. Energy minimizations were performed upon this model using hydrogen bond parameters for water, and altered hydrogen bond parameters that reproduced the differences in carbonyl oxygen-water oxygen distances found in small-molecule crystal structures containing oxygen-oxygen hydrogen bonds between organic molecules and H₂O or D₂O. It was found that using hydrogen bond parameters that reproduced the distance typical of hydrogen bonds to D₂O resulted in a significant lowering of the potential energy of hydrated (PPG)₁₀. This lowering of the energy involved energetic terms that were only indirectly related to the altered hydrogen bond parameters, and were therefore not artifactual; the intra-(PPG₁₀) energy, plus the water-(PPG₁₀) van der Waals energy (not including hydrogen bond interactions), were lowered enough to qualitatively account for the lower enthalpy of the triple-helical conformation, relative to the unfolded state, in D₂O vs. H₂O. This result indicates that the geometry of the carbonyl-D₂O hydrogen bonds allows formation of good hydrogen bonds without making as much of an energetic sacrifice from other factors as in the case of hydration by H₂O.     

Infrared and raman spectra of metal 1,2,4,5-benzenetetracarboxylates: Evidence for very short,strong hydrogen bonds

Salts of 1,2,4,5-benzenetetracarboxylic acid with copper, aluminum, ammonium, cobalt(II), thallium(I), tin(II), uranyl ion, zinc, manganese, iron(II), nickel, potassium and sodium have been prepared and characterized by their IR spectra. The salts of aluminum, ammonium, thallium(I), tin(II), zinc, iron(II), nickel, potassium and sodium had not been reported before with adequate characterization. Raman spectra of selected compounds also aided structural interpretation. The IR spectra of Na₂C₁₀H₄O₈·2H₂O, Fe(C₁₀H₅O₈)₂·12H₂O, Zn(C₁₀H₅O₈)₂·12H₂O, Ni(C₁₀H₅O₈)₂·12H₂O, (NH₄)₃C₁₀H₃O₈·H₂O and CoC₁₀H₄O₈·6H₂O indicate very short, strong hydrogen bonds in these compounds. The IR and Raman spectra can be used to determine the mode of coordination (if any) of the carboxylate groups of 1,2,4,5- benzenetetracarboxylate to metal ions.     

A systematic evaluation of different hydrogen bonding patterns in unsymmetrical 1,n′-disubstituted ferrocenoyl peptides

The synthesis and spectroscopic characterization of 21 l,l′-disubstituted ferrocenoyl peptides of the general formula [Fe(C₅H₄-CO-Aal-OR) (C₅H₄-CO-Aa2-OR′)] is reported, with Aal and Aa2 being different amino acids. The one-pot synthesis from activated ferrocene-l,l′-dicarboxylic acid and two different amino acid esters gives the unsymmetrical ferrocenoyl peptides in yields between 27% and 42%, which can be easily separated from their symmetrical byproducts by column chromatography. All new compounds are comprehensively characterized by mass spectrometry (El and FAB, including high-resolution EI-MS), ¹H and ¹³C NMR, and UV/Vis spectroscopy. CD spectroscopy in conjunction with ¹H NMR is used to elucidate the solution structures. Using the achiral glycine (Gly) as Aal permits to determine qualitatively the structure-determining influence of the different amino acids Aa2. Helically chiral structures in ferrocene amino acids in this study are stabilized by hydrogen bonds. If one hydrogen bond partner is systematically moved away by the introduction of methylene groups, then indeed the strength of the hydrogen bond decreases as indicated by ¹H NMR chemical shifts of the amide protons and the strength of characteristic CD bands. As proline (Pro) is the only naturally accuring secondary amino acid it cannot contribute any amide proton to intra-strand hydrogen bonding. DFT calculations on the compound [Fe(C₅H₄-CO-Gly-OMe)(C₅H₄-CO-Pro-OMe)] with one achiral and one secondary amino acid were therefore performed to quantify the more subtle influence of the relative orientations of the ferrocene carbonyl groups and the cis-/trans-conformation of both amide bonds. Not unexpectedly, the conformations with both amide bonds in cis orientation are highest in energy. Surprisingly, the calculations suggest the presence of a low-energy conformation with a non-classical hydrogen bond between the proline ester carbonyl oxygen and a glycine H_α atom. However, a second conformation with no apparent intra-strand contacts but optimal positioning of all relevant groups is similar in energy. Although two conformations were observed in solution for this compound, the experimental data did not permit to assign those two conformations.     

A theoretical study on unusual intermolecular T-shaped X–H...π interactions between the singlet state HB=BH and HF, HCl, HCN or H2C2

The unusual T-shaped X–H...π hydrogen bonds are found between the B=B double bond of the singlet state HB=BH and the acid hydrogen of HF, HCl, HCN and H₂C₂ using MP2 and B3LYP methods at 6-311++G(2df,2p) and aug-cc-pVTZ levels. The binding energies follow the order of HB=BH...HF>HB=BH...HCl>HB=BH...HCN>HB=BH...H₂C₂. The hydrogen-bonded interactions in HB=BH...HX are found to be stronger than those in H₂C=CH₂...HX and OCB≡BCO...HX. The analyses of natural bond orbital (NBO) and the electron density shifts reveal that the nature of the T-shaped X–H...π hydrogen-bonded interaction is that much of the lost density from the π-orbital of B=B bond is shifted toward the hydrogen atom of the proton donor, leading to the electron density accumulation and the formation of the hydrogen bond. The atoms in molecules (AIM) theory have also been applied to characterize bond critical points and confirm that the B=B double bond can be a potential proton acceptor. The unusual T-shaped X–H...π hydrogen bonds are found between the B=B double bond of the singlet state HB=BH and the acid hydrogen of HF, HCl, HCN and H₂C₂     

Mechanism of the gas phase reactions of the C5H5Ni and C5H5Co ions with substituted pyridines. A combined experimental and theoretical study

Different products have been observed in the reactions of C₅H₅Co⁺ and C₅H₅Ni⁺ ions with halogen-substituted pyridines (XPy) that have been studied by ion trap mass spectrometry (ITMS) techniques. In particular, an addition product C₅H₅M(XPy)⁺ and a product ion C₅H₄M(Py)⁺ corresponding to a loss of a HX molecule (X = F, Cl, Br) have been detected. The relative yield of these products is determined by the nature of the metal and by the nature and position of the halogen on the pyridine ring. A computational study at the DFT level on model-systems formed by 2-fluoro and 2-bromopyridine reacting either with the C₅H₅Ni⁺ or the C₅H₅Co⁺ ion has been carried out. This study shows the existence of a general mechanistic pattern. The rate-determining step of this mechanism is the migration of the halogen from the pyridine ring to the metal. A final hydrogen abstraction step carried out by the halogen leads to the expulsion of a HX molecule. The existence of avoided crossings between surfaces of different multiplicities (ground and first excited state) allows the system to follow lower energy reaction pathways. The barrier determined for the reactions involving 2-bromopyridine is significantly lower than that found for 2-fluoropyridine. This is mainly due to the poor migrating/leaving character and low polarizability of fluorine compared to that of bromine.     

Synthesis, crystal structures, and fluorescence properties of six complexes with thiophene derivative carboxylic acid ligand

The crystallization of 2,3-dihydro-thieno[3,4-b][1,4] dioxine-5,7-dicarboxylic acid (H₂tddc) with divalent transitional metal (Co, Ni, Zn, Cd) or with tervalent lanthanide metal (Sm) and with mixed ligand 4,4′-bipyridine (4,4′-bipy) or 1,10-phenanthroline (1,10-phen) formed six new complexes: [Co(C₈H₄O₆S) · 3H₂O] (1), [Co(C₈H₄O₆)(1,10-phen)(H₂O)] · H₂O (2), [Ni(C₈H₄O₆S)(4,4′-bipy)(H₂O)] · 3H₂O (3) [Sm(C₈H₄O₆S)(NO₃)(H₂O)₄] · 2H₂O (4), [Zn(C₈H₄O₆S)(H₂O)₃] (5), and [Cd₂(C₈H₄O₆S)₂(4,4′-bipy)₂] (6). The structures of these six crystals have been characterized by single-crystal X-ray diffraction analyses, which revealed that complexes 1, 4, 5 are all one-dimensional chain structures and they self-assemble into three-dimensional super-molecules via the hydrogen bond interactions and π-π stacking interactions, 2 is also a one-dimensional chain structure but still self-assembles into one-dimensional double-chains, the complex 3 has two-dimensional undulating parallelogram grid structure extended along the bc-plane, the crystal of 6 is a 3D threefold interpenetration topology framework with 4⁶6³8 nodes. The photoluminescent properties of the H₂tddc ligand and the six compounds have been measured in the solid state at room temperature. Free ligand has no luminescence, while its complexes 1, 4, and 6 all exhibit intense photoluminescence which implies that these complexes may be excellent candidates for potential photoactive materials.     

Proton and carbon magnetic resonance studies of the synthetic polypentapeptide of elastin.

Proton and ¹³C magnetic resonance studies are reported on the synthetic polypentapeptide of elastin, HCO-(Val₍₁₎-Pro₍₂₎-Gly₍₃₎-Val₍₄₎-Gly₍₅₎)_n-Val-OMe, where n ∼- 18. Temperature and solvent dependence of peptide N$\text{H}$ chemical shift and solvent dependence of peptide carbonyl chemical shift were used to delineate these moieties preliminary to identification of secondary structure.Based on these studies it is proposed, for the organic solvents of dimethyl sulfoxide, methanol, and low-temperature trifluoroethanol, that dynamic hydrogen bonds form in order of decreasing frequency of occurrence between the Val₍₁₎$\text{C}$O and the Val₍₄₎ N$\text{H}$ (a β-turn), between the Gly₍₃₎ N$\text{H}$ and the Gly₍₅₎$\text{C}$O (an 11-atom, hydrogen-bonded ring), and a more limited interaction between the Gly₍₃₎$\text{C}$O and the Gly₍₅₎ N$\text{H}$ (a γ-turn).Arguments are presented that relate the conformational features proposed above to the coacervate, which is a filamentous state.