Vibrational spectroscopic study of o-, m- and p-hydroxybenzylideneaminoantipyrines

Three structurally similar antipyrine derivatives of o-hydroxybenzylideneaminoantipyrine (o-HBAP), m-hydroxybenzylideneaminoantipyrine (m-HBAP) and p-hydroxybenzylideneaminoantipyrine (p-HBAP) were characterized by FT-IR, FT-Raman experimental techniques and density functional theoretical (DFT) calculations. The comparisons between the calculated and experimental results covering molecular structures, assignments of fundamental vibrational modes and thermodynamic properties were investigated. The optimized molecular geometries agree well with the corresponding experimental values by comparing with the XRD data. The comparisons and assignments of the vibrational frequencies indicate that the experimental spectra also coincide satisfactorily with those of theoretically simulated spectrograms except the hydrogen-bond coupling infrared vibrations, and compounds can be distinguished by the IR and Raman spectra due to the differences of the hydroxyl-substituted positions and molecular packing, and the strong Raman scattering activities of the compounds are tightly relative to the molecular conjugative moieties linked through the Schiff base imines. The thermodynamic functions and their correlations with temperatures were also obtained from the theoretical harmonic frequencies.     

Zur Unterscheidung von o-, m- und p-Phenylendiamin

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Magnetic properties and aromaticity of o-, m-, and p-benzyne

The relative aromaticities of the three singlet benzyne isomers, 1,2-, 1,3-, and 1,4-didehydrobenzenes have been evaluated with a series of aromaticity indicators, including magnetic susceptibility anisotropies and exaltations, nucleus-independent chemical shifts (NICS), and aromatic stabilization energies (all evaluated at the DFT level), as well as valence-bond Pauling resonance energies. Most of the criteria point to the o-benzyne相似文献   

Zur gaschromatographischen Analyse von o-, m- und p-Chloronitrobenzol

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Effect of hydrogen bonding on the polymerization of N-(o-,m-, and p-methoxyphenyl)- and N-(o-,m-, and p-ethoxyphenyl)-methacrylamides

Summary Study of the rates of polymerization of N-(o-, m-, and p-methoxyphenyl)- and N-(o-, m-, and p-ethoxy-phenyl)methacrylamides showed that the ortho isomers of these compounds, in which there is no association between the molecules, polymerize much more rapidly than their meta and para isomers, the molecules of which are associated through hydrogen bonds.     

离子色谱法分析邻,间,对硝基苯酚

建立了一种分析邻，间，对硝基苯酚的离子色谱分析体系，选用亚硝酸钠溶液作为淋洗液，紫外检测波长２５４ｎｍ能很好的分析硝基苯酚异构体，检测限低于１０＾－４ｇ／Ｌ。     

Isomer-specific spectroscopy and conformational isomerization energetics of o-, m-, and p-ethynylstyrenes

The infrared and ultraviolet spectroscopy of o-, m-, and p-ethynylstyrene isomers (oES, mES, and pES) were studied by a combination of methods, including resonance-enhanced two-photon ionization (R2PI), UV-UV hole-burning spectroscopy (UVHB), resonant ion-dip infrared spectroscopy (RIDIRS), and rotationally resolved fluorescence excitation spectroscopy. In addition, the newly developed method of stimulated emission pumping-population transfer spectroscopy (SEP-PTS) was used to determine the energy threshold to conformational isomerization in m-ethynylstyrene. The S(1) <-- S(0) origin transitions of oES and pES occur at 32 369 and 33 407 cm(-1), respectively. In mES, the cis and trans conformations are calculated to be close in energy. In the R2PI spectrum of mES, the two most prominent peaks (32672 and 32926 cm(-1)) were confirmed by UVHB spectroscopy to be S(1) <-- S(0) origins of these two conformers. The red-shifted conformer was identified as the cis structure by least-squares fitting of the rotationally resolved fluorescence excitation spectrum of the origin band. There are also two possible conformations in oES, but transitions due to only one were observed experimentally, as confirmed by UVHB spectroscopy. Density functional theory calculations (B3LYP/6-31+G) predict that the cis-ortho conformer, in which the substituents point toward each other, is about 8 kJ/mol higher in energy than the trans-ortho isomer, and should only be about 5% of the room temperature population of oES. Ground-state infrared spectra in the C-H stretch region (3000-3300 cm(-1)) of each isomer were obtained with RIDIRS. In all three structural isomers, the acetylenic C-H stretch fundamental was split by Fermi resonance. Infrared spectra were also recorded in the excited electronic state, using a UV-IR-UV version of RIDIR spectroscopy. In all three isomers the acetylenic C-H stretch fundamental was unshifted from the ground state, but no Fermi resonance was seen. The first observed and last unobserved transitions in the SEP-PT spectrum were used to place lower and upper bounds on the barrier to cis --> trans isomerization in m-ethynylstyrene of 990-1070 cm(-1). Arguments are given for the lack of a kinetic shift in the measurement. The analogous trans --> cis barrier is in the same range (989-1065 cm(-1)), indicating that the relative energies of the zero-point levels of the two isomers are (E(ZPL)(cis) - E(ZPL)(trans))= -75 to +81 cm(-1). Both the barrier heights and relative energies of the minima are close to those determined by DFT (Becke3LYP/6-31+G) calculations.     

镁铝类水滑石对邻、间、对甲基苯酚的吸附

采用液相非稳态共沉淀法制备了镁铝类水滑石（Mg-Al HTlc）,并研究了邻、间和对甲基苯酚在Mg-Al HTlc上的吸附行为。 结果表明,邻、间和对甲基苯酚在Mg-Al HTlc上的吸附等温方程均符合Freundlich吸附等温式;吸附动力学均符合准二级动力学方程;在实验范围内,Mg-Al HTlc对三者的吸附量为：对甲基苯酚＞邻甲基苯酚＞间甲基苯酚;在pH值5.00~13.00范围内,三者的吸附量均随pH值的增加先增大后减小、随温度升高和电解质（NaCl）浓度的增大而增大。 探讨了吸附机理和苯环上甲基取代基位置对吸附的影响。     

薄层色谱法同时测定邻苯二酚、间苯二酚和对苯二酚异构体

研究了在自制硅胶薄板上邻苯二酚,间苯二酚异构体的薄层色谱特性。展开剂为本：乙醚：冰醋酸＝７：２：１（Ｖ／Ｖ／Ｖ）,Ｒｆ值分别为０．５９,０．５３,０．４８。检测限分别为１．０７×１０＾－４,１．６４×１０＾－４,１．９０×１０＾４ｍｏｌ／Ｌ。其他常见酚不干扰测定。可应用于实际样品的测定,回收率为９６％－１０４％。     

The o-, m-, and p-benzyne radical cations: a theoretical study

On the basis of the CASPT2 (multiconfigurational second-order perturbation theory) geometry optimization calculations, the ground states of the o-C(6)H(4)(+) (C(2v)), m-C(6)H(4)(+) (C(2v)), and p-C(6)H(4)(+) (D(2h)) radical cations were determined to be 1 (2)B(1), 1 (2)A(2), and 1 (2)B(1u), respectively. For o-C(6)H(4)(+) and m-C(6)H(4)(+), the first excited states (1 (2)A(2) and 1 (2)A(1), respectively) lie very close to the respective ground states. The small distance value of 1.419 A between the two dehydrocarbons in the ground-state geometry of m-C(6)H(4)(+) indicates that there is a real chemical bond between the two dehydrocarbons (the distance in the 1 (2)A(1) geometry of m-C(6)H(4)(+) is very long as in the m-C(6)H(4) molecule). The (U)B3LYP isotropic proton hfcc (hyperfine coupling constant) calculation results imply that the ground and first excited states of o-C(6)H(4)(+) will have similar ESR spectrum patterns while the ground and first excited states of m-C(6)H(4)(+) will have completely different ESR spectrum patterns.     

Spin-orbit ab initio investigation of the photolysis of o-, m-, and p-bromotoluene

The photodissociations of o-, m-, and p-bromotoluene were investigated by ab initio and spin-orbit ab initio calculations. The possible photodissociation mechanisms at 266 and 193 nm were clarified by multistate second order multiconfigurational perturbation theory (MS-CASPT2) calculated potential energy curves, vertical excitation energies, and oscillator strengths of low-lying states. The dissociation products with spin-orbit-coupled states of Br(*)((2)P(12)) and Br((2)P(32)) were identified by the MS-CASPT2 method in conjunction with spin-orbit interaction through complete active space state interaction (MS-CASPT2/CASSI-SO) calculations. The effects of methyl rotation and substituent on the photodissociation mechanism were discussed.     

Die quantitative Bestimmung von o-, m- und p-Kresolen nach den Infrarotabsorptionsspektren

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