Interpretation of the IR spectrum and structure of cellulose nitrate

Based on our experimental data on the polarized IR spectra of the oriented fiber of cellulose nitrate (CN), the IR spectra of¹⁵N CN, and its structural data published earlier, we have revised the interpretation of the IR spectrum of CN and give a more specific interpretation. We established a relationship between the form of vibration bands of the nitrate groups and their position and conformation state in the glucopyranose cycle of CN. The relative intensities of the valence vibration bands of the CH₂ groups are explained by the Fermi resonance with a complex tone of valence vibrations of the nitrate groups. In view of the strong dichroism of some low-frequency bands in the IR spectrum of CN, we offer assignments of these bands to vibrations of the chain skeleton and suggest the rationale for the high orientation of CN macromolecules both in the ordered and disordered regions. Such an orientation is assumed to be inherited by CN from the starting cellulose.Kazan Chemical Engineering Institute. Translated fromZhurnal Strukturnoi Khimii, Vol. 34, No. 4, pp. 59–66, July–August, 1993.Translated by L. Smolina     

Crystal structure, thermal analysis and IR spectrometric investigation of L-tyrosine hydrazide sulfate

Chemical preparation, X-ray single crystal, thermal analysis and IR spectrometric investigation of (C₉H₁₅N₃O₂)SO₄ denoted LTHS are described. The LTHS crystallizes in the monoclinic system with P2₁ space group. Its unit cell dimensions are a=5.5386(1) Å, b=8.0467(4) Å, c=14.0780(6) Å, β=93.339(3)° with V=626.36(4) Å³ and Z=2. The structure has been solved using direct method and refined to a reliability R factor of 0.0212. The LTHS structure is built up from organic chains parallel to the b axis, linked via N---H…O hydrogen bonds and interconnected by inorganic groups so as to build a three-dimensional arrangement.     

Crystal structure and vibrational spectrum of copper mercury ortho-thiophosphate CuHgPS4

The compound CuHgPS₄ crystallizes in the orthorhombic system, space group Pna2₁ (No. 33), Z = 4, with lattice parameters a = 12.660(3), b = 7.3498(7), c = 6.0943(4) Å, and δ_calc = 4.96 g/cm³. The title compound is stable in air and moisture and behaves as a semiconductor. The crystal structure consists of discrete tetrahedral PS₄^3- anions joined together by Cu⁺ and Hg²⁺ cations. The arrangement of the sulfur atoms is approximately hexagonal close-packed in which P, Cu, and Hg occupy tetrahedral sites. The PS₄, HgS₄, and CuS₄ tetrahedra are slightly distorted with mean distances d(P-S) = 2.055, d(Hg-S) = 2.524, and d(Cu S) = 2.320 Å, and 8% of the Hg atoms were found to be disordered, occupying interstitial tetrahedral sites. The title compound is isotypic to AgZnPS₄ and can be considered to be a defect structure of Enargite (Cu₃AsS₄), which is a substitution derivative of the Wurtzite (ZnS) structure. The CuHgPS₄ vibrational spectrum has been recorded. The internal modes experimentally observed are in accord with the factor group prediction. A tentative assignment of the vibrational frequencies is proposed.     

Finding the 3D structure of a molecule in its IR spectrum

 The labile iron(II) and iron(III) species are complexed directly in the sample solution with 1,10 phenanthroline and ferron (8-hydroxy-7-iodoquinoline-5-sulfonic acid), respectively. The complexes thus formed are mutually adsorbed and separated by solid phase extraction. The direct determination of iron(III) and iron(II) species with flame atomic absorption spectrometry (FAAS) follows the elution of the iron(III)-ferron complex adsorbed by an anion-exchange and an iron(II)-phenanthroline complex adsorbed by a non-polar RP-18 phase. In the case of indirect determination, the iron(II)-phenanthroline complex that passes through the anion-exchange phase, is measured, and the content of iron(III) is calculated by the difference of the iron(II) and the total iron content. A direct determination with this method has been applied to the iron species analysis in wine samples and the results are compared with those obtained for the determination with adsorptive stripping voltammetry (ASV) as reference method. Received: 17 August 1995/Revised: 12 February 1996/Accepted: 14 February 1996     

Synthesis,thermal analysis,IR spectrum,and crystal structure of rubidium hexanitratothorate

Rubidium hexanitratothorate was synthesized, and its crystal structure was determined by X-ray diffraction analysis: space group P2₁/n; a = 8.347(1) Å, b = 6.890(1) Å, c = 13.069(1) Å, β = 91.88(1)°, Z = 2; 1812 independent reflections, R = 0.0165.     

Synthesis and structure of tetraphenylantimony hydrogen phthalate

Tetraphenylantimony hydrogen phthalate, Ph4SbOC(O)C6H4000H-o, was prepared by the reaction of pentaphenylantimony with phthalic acid. According to the data of X-ray structural analysis, the resulting compound is a trigonal-bipyramidal complex of antimony with three phenyl groups in equatorial positions; the fourth phenyl group and the carboxyl fragment are in axial positions. The CSbO angle is 177.5(1)° the Sb-C(Ph)_eq and Sb-C(Ph)ax distances are 2.099(4)-2.177(4) A and 2.129(4) A, respectively. The H atom of the free carboxyl group and the carbonyl O atom of another carboxylate group form an intramolecular hydrogen bond.DeceasedTranslated fromIzvestiya Akademii Nauk. Seriya Khimicheskaya, No. 8, pp. 2082–2085, August, 1996.     

Crystal structure and IR spectrum of 1-O-α- -glucopyranosyl- -mannitol–ethanol (2/1)

1-O-α- -Glucopyranosyl- -mannitol–ethanol (2/1), (C₁₂H₂₄O₁₁)₂–C₂H₅OH, crystallizes in the monoclinic space group P2₁ with unit cell dimensions a=11.4230(8) Å, b=9.525(4) Å, c=15.854(2) Å, β=102.751(7)° and V=1682.4(7) ų, Z=2, D_x=1.45 Mg m⁻³, λ (Mo-K_α)=0.71069 Å, μ=0.128 mm⁻¹, F(000)=788 and T=293(2) K. The structure was solved by direct methods and refined by least-squares calculations on F² to R₁=0.0371[I>2σ(I)], and 0.0930 (all data, 3542 independent reflections, R_int=0.021). There are two molecules of glucopyranosylmannitol (GPM) and one ethanol molecule in the asymmetric unit, and the glucopyranosyl ring adopts a chair conformation in both GPM molecules. Bond lengths and angles accord well with the mean values of related structures. The conformation along the mannitol side chain for one of the GPM molecules was the same as for the known polymorphs of -mannitol, while the conformation of the other molecule was different, indicating different conformational arrangements in the terminal carbon atoms of the mannitol side chains of the two GPM molecules. The structure in 1-O-α- -glucopyranosyl- -mannitol–ethanol (2/1) is held together by a very complex hydrogen bonding system, which consists of an infinte chain propagating along the b-axis and a discontinuous chain, which binds the ethanol molecule to the structure. The FTIR spectra for anhydrous GPM, GPM dihydrate and GPM–ethanol (2/1) were recorded. Both IR and X-ray results indicate the extensive hydrogen bonding in crystalline state.     

Synthesis and properties of poly(dipropargyl sulfoxide)

The preparation and cyclopolymerization of dipropargyl sulfoxide were studied. The polymerization of dipropargyl sulfoxide was carried out by various transition metal catalysts. WCl₆–EtAlCl₂, MoCl₅, and PdCl₂ catalyst systems were very effective. The resulting poly(dipropargyl sulfoxide) structures were characterized by NMR (¹H and ¹³C), IR, and elemental analysis to have conjugated polyene units. Poly(dipropargyl sulfoxide) prepared by PdCl₂ was mostly soluble in organic solvents such as DMF and DMSO. Thermal and oxidative properties of poly(dipropargyl sulfoxide) were also studied. The electrical conductivity of iodine-doped poly(dipropargyl sulfoxide) was 5.2 × 10^?2 Ω^?1 cm^?1. Comparisons of poly(dipropargyl sulfoxide) properties with other similar polymers from dipropargyl sulfur derivatives such as dipropargyl sulfide and dipropargyl sulfone were also carried out. © 1993 John Wiley & Sons, Inc.     

IR spectrum and structure of protonated ethanol dimer: implications for the mobility of excess protons in solution

This Communication reports IR spectra and density functional calculations for the isolated protonated ethanol dimer and its N2-microsolvated complexes, (EtOH)2H+-(N2)n (n = 0-2) to investigate the degree of delocalization of the excess proton in this fundamental building block of an alcohol proton wire. The first spectroscopic characterization of isolated and microsolvated (EtOH)2H+ suggests that the excess proton is (nearly) equally shared between both EtOH units under symmetric solvation conditions (Zundel-type ion, n = 0 and 2), whereas it is largely localized on a single EtOH molecule for asymmetric solvation (Eigen-type ion, n = 1).     

UV Absorption spectra of solutions of dipropargyl ethers

Conclusions The dipropargyl ethers of 4,4-dihydroxydiphenylpropane, methylphosphinic acid, diphenoxysilane, hexafluoro-2,2-bis-(hydroxyphenyl)propane, terephthalic, isophthalic acids, orcinol, resorcinol, 1,4-dihydroxyanthraquinone, maleic and succinic acids, dipropargylbenzal, dipropargylacetal, and dipropargylformal were identified by means of their UV spectra.Translated from Izvestiya Akademii Nauk SSSR, Seriya Khimicheskaya, No. 7, pp. 1349–1352, July, 1964     

Crystal structure,phase transitions,and IR spectroscopic investigations of a new sulfate templated by diethylene triammonium

A novel organic sulfate (C₄H₁₆N₃)SO₄?HSO₄ has been prepared and characterized by single-crystal X-ray diffraction, infrared spectroscopy, thermogravimetric analysis and differential scanning calorimetry (DSC). The structure consists of linked HSO₄^? and SO₄^2? anions assembled into clusters. Organic triple-protonated diethylene triammonium cations are interconnected to these clusters via N–H?O hydrogen bonds to create the three dimensional arrangement. The Hirshfeld surface and associated fingerprint plots of the compound were presented to explore the nature of intermolecular interactions and their relative contributions to building the solid-state architecture. TG-DTA and DSC studies showed the presence of two phase transitions. Infrared spectrum is reported and discussed on the basis of group theoretical analysis and on Density Functional Theory calculations.     

The Ni2+O2 reaction: the IR spectrum and structure of Ni2O2. A combined IR matrix isolation and theoretical study

The formation of Ni2O2 can be observed from the condensation of effusive beams of Ni and O2 in neon or argon matrices. Observation of 58Ni(2)16O2, 58Ni60Ni16O2, 60Ni2(16)O2, Ni(2)18O2 and Ni(2)16O18O isotopic data for five fundamental transitions enable a discussion of structural parameters for matrix-isolated Ni2O2 in its cyclic ground state. Analysis of the nickel isotopic effects on the 58,60Ni2(16)O18O fundamentals suggest an elongated rhombic structure with a Ni-O bond force constant (240+/-10 N m-1) and NiONi bond angles around 79 degrees. The latter points to a Ni-Ni internuclear distance shorter than the O-O one. Low-lying singlet, triplet and quintet states have been studied using density functional theory with an unrestricted wave function and broken symmetry formalism. The high spin states and closed shell singlet states have been also investigated at the CCSD(T) level. The Ni2O2 ground state is calculated to be an antiferromagnetic singlet state with all the hybrid functionals. The first order properties (energies, geometry) calculated with a hybrid functional are very similar when different exchange-correlation functionals with different exact exchange fractions are used and the calculated ground state geometry (NiONi bond angle near 80 degrees, NiO bond distance around 179.5 pm) is in good agreement with the experimental estimate. Nevertheless, a correct reproduction of the experimental vibrational properties is found only when a hybrid functional containing an exact exchange fraction in the 0.4-0.5 range is used. The orbital and topological bonding analyses of Ni2O2 reveal that the relatively short Ni-Ni internuclear distance within the molecule should not be interpreted as a remaining metal-metal bonding interaction, but clearly indicate that the bonding driving force is due to the formation of four strong and highly polarized Ni-O bonds. Even in such an early stage of metal oxidation, the Ni-Ni interaction has virtually disappeared.     

Crystal structure and magnetic structure of TbOOH

The monoclinic modification of terbium oxide hydroxide, TbOOH, was prepared using hydrothermal technique. The crystal structure was investigated by three-dimensional single-crystal X-ray analysis and was refined to a conventional R-value of 8.1%. The space group is $\text{P2}{}_1\text{m}$, No. 11, with a = 6.04 Å, b = 3.69 Å, c = 4.33 Å, and β = 109.0°. The terbium atom is seven coordinated with oxygen atoms, and the structure is not hydrogen bonded.The compound is antiferromagnetic with a Néel temperature of 10°K. Neutron diffraction powder patterns were measured at 300°K and 4.2°K. The magnetic super lattice reflections were indexed on the basis of a monoclinic unit cell with the dimensions a_M = 2a, b_M = b, c_M = c, and β_M = β, where a, b, c, and β are the dimensions of the chemical unit cell. The structure contains two independent magnetic atoms. A nonclinear antiferromagnetic arrangement of the spins describes the magnetic structure. The spin at one atom has an angle of 43° with the ac plane and the projection of the spin on the ac plane has an angle of 59° with the a axis. The spin on the other atom has an angle of ?43° with the ac plane, the projection having the same angle of 59° with the a axis.     

High-resolution IR spectrum of fluoroform: a close resonance

A very close triple resonance is observed in the Q-branch region of the C-H stretching fundamental transition in CF₃H. The vibrational perturbations are analysed in terms of the rotational structure and of the vibrational zero-order spectrum of totally symmetric states. The relationship to time-dependent intramolecular processes is discussed.