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1.
Ab initio GAUSSIAN 80 calculations with two different basis sets (STO-3G and 4–31 G*) were performed on hydrogen bonded cresol isomers for comparison with experimental data from free jet fluorescence excitation spectroscopy. Form-cresol, the calculated barriers for hindered internal rotation of the OH-group and the CH3-group are in good agreement with experiment. The calculations show the trans-linear configuration ofp-cresol·B-clusters (B = H2O, CH3OH) to be more stable than the all-planar configuration. This agrees with CI calculations and microwave spectroscopic investigations of the water dimer. Calculations of both the intermolecular stretch and bend frequencies ofp-cresol·B-clusters show little dependence on the all-planar or trans-linear configuration but a strong dependence on the choice of the basis set. With the minimal basis set STO-3G, the vibrational energies are generally too high. The agreement between the calculated vibrational frequencies from the 4–31 G* basis set and the experimental values is fair.  相似文献   

2.
Ab initio SCF calculations with minimal STO-3G and extended 44-31G basis sets have been performed on the simple alkyl chlorides, HCl to t-BuCl, and their protonated analogs. MINDO/3 calculations are also reported for these species and a variety of cyclic and bicyclic chlorides. The much closer agreement with experiment for STO-3G proton affinities than for 44-31G values is in sharp contrast to the results for first-row bases. An excellent correlation is found between both the STO-3G and MINDO/3 proton affinities and the charge on the CIH fragment in RCIH+. For the acyclic chlorides, correlations of PA's with the polar substituent constant, σ*, and IP's are also reasonable. In addition, the calculated carbonium ion-HCl interaction energy for t-BuClH+ indicates that protonated tertiary chlorides are no more than marginally stable in the gas phase.  相似文献   

3.
Vibrational frequency calculations at the 6–31G*, 6–31G and STO-3G levels in addition to an STO-3G basis set with only a 1s orbital on lithium reveal that both bridged and linear dilithioacetylenes are minima on the potential energy surface.  相似文献   

4.
The conformational behaviour of the six isomers of thiobispyridine has been investigated using ab initio STO-3G*//rigid-roto, STO-3G*//STO-3G* and 6–31G**//STO-3G* molecular orbital models. The analysis reveals both the importance of optimising critical structure parameters and the basis set dependence of calculated rotational barrier heights. The most reliable model (6–31G**//STO-3G*) clearly indicates that the minimum energy conformers are not planar and that energy barriers between 30–100 kJ mol?1 restrict inter-conversion to planar structures, thereby preventing conjugation between the p-electrons of the sulfur atom and the π system of both pyridine rings. From the calculated barrier heights, two mechanisms can be employed to explain conformer interconversion about the C? S bond: a disrotatory one-ring flip or a conrotatory two-ring flip mechanism. Where comparisons can be made (eg. 2,2′-thiobispyridine), dipole moment calculations are shown to be in good agreement with experiment. Finally, of the six isomers, appropriately substituted 2,2′, 2,3′- and 2,4′-thiobispyridines are most prone to a Smiles rearrangment.  相似文献   

5.
The internal rotation in peroxyformic acid was investigated using the ab initio SCF MO LCAO method with the STO-3G and 4-31G basis-sets and with experimental and optimum values of the geometrical parameters. Both basis sets yield a rather flat double-minimum potential for the COOH torsion, the trans planar form being lightly preferred in comparison with the cis one. The effects on the internal rotation of the geometry relaxation, of the intramolecular hydrogen bond and of the methyl group of peroxyacetic acid are also discussed.  相似文献   

6.
The lowest excited states of the diimide molecule have been calculated by three different SCF-type methods, the performances of which are analyzed in regard to the prediction of geometries and energies. The calculations have been performed with two basis sets (STO-3G and 4-31G) both supplemented with more diffuse functions on the N atoms. Lowest energy pathways for thetrans-cis interconversion in the various states are presented for the three calculation methods and for the two basis sets.  相似文献   

7.
The electrostatic potential-derived charges for the catecholamine neurotransmitter dopamine were calculated at the STO-3G and 6-31G* basis sets for six different molecular conformations. The degree of variance of the charges with changing conformations was examined. The 6-31G* basis set produced charges that were more sensitive to changes in conformation than those derived from the STO-3G electrostatic potentials. The implication of the charge variations in molecular mechanics calculations was also investigated. The molecular mechanics results in the gas phase exhibited a variance depending upon the charge set used. The force field calculations varied much less when aqueous solvation was included in the calculations through a continuum model. © 1993 John Wiley & Sons, Inc.  相似文献   

8.
The conformational energies of 1-amino-2-propanol, 2-amino-1-propanol and 1,2-diaminopropane are studied using ab initio molecular orbital theory employing minimal (STO-3G) and extended (4-31G) basis sets. Calculations at both levels of theory generally favor conformations stabilized by internal H-bonding for all molecules considered. Results are first presented for conformations employing assumed geometries. Since the conformational energy differences as found by the initial set of calculations are in some cases rather small it then becomes necessary to introduce geometry optimizations into the study at the minimal STO-3G level. In addition, to get a better estimate of the energy differences of the various conformations 4-31G calculations are performed on the STO-3G optimized structures. These latter results indicate the following, (a) For 1-amino-2-propanol only one conformation that is stabilized by intramolecular H-bonding is low in energy; this has the methyl and amino groups anti. The other H-bonded conformer, where the methyl and amino groups are gauche, is predicted to be ca. 1.2 kcal mol?1 less stable. Similar findings for this molecule have recently been provided by micro-wave spectroscopy. (b) For 2-amino-1-propanol the two H-bonded conformers are only separated by about 0.5 kcal mol?1, with the anti conformer being more stable. Micro-wave spectroscopy again supports these calculations. (c) For 1,2-diaminopropane the gauche conformer is predicted to be of rather high energy (ca. 2.5 kcal mol?1) compared to the corresponding anti H-bonded conformer. The value of 2.5 kcal mol?1should be taken as an upper limit, since the geometry optimization of the gauche conformer of 1,2-diaminopropane is incomplete compared to the optimization carried out for the anti conformer.  相似文献   

9.
Ab initio calculations were performed on 2-hydroxy-1,3-oxathiolane: and the two products of its breakdown: Complete geometry optimizations were performed at minimal (STO-3G) and split-valence (3-21G) basis set levels. In addition, a single point calculation was performed at 6-31G* level withd orbitals added on sulfur only. The conformation of the oxathiolane intermediate and its stability relative to the breakdown products was investigated. The STO-3G basis set gave an envelope form while 3-21G gave the twist form of the five-membered ring as the most stable. For all three basis sets the ester product was more stable than thioester.  相似文献   

10.
Quantum mechanical calculations of the geometric, energetic, electronic, and vibrational features of a transition structure for gas-phase water–formaldehyde addition (FW1?) are described, and a new transition-structure search algorithm is presented. Basis-set-dependent effects are assessed by comparisons of computed properties obtained from self-consistent field (SCF) molecular orbital (MO) calculations with STO-3G, 4-31G, and 6-31G** basis sets in the absence of electron correlation. The results obtained suggest that STO-3G-level calculations may be sufficiently reliable for the prediction of the transition structure of FW1? and for the transition structures of related carbonyl addition reactions. Moreover, the calculated activation energy for formation of FW1? from water and formaldehyde (?44 kcal mol?1) is very similar in all three basis sets. However, the energy of formaldehyde hydration predicted by STO-3G (? ?45 kcal mol?1) is about three times larger than that predicted by the other two basis sets, with the activation energy for dihydroxymethane dehydration also being too large in STO-3G. Calculated force constants in all three basis sets are generally too large, leading to vibrational frequencies that are also too large. However, uniformly scaled force constants (in internal coordinates) give much better agreement with experimental frequencies, scaled 4-31G force constants being slightly superior to scaled STO-3G force constants.  相似文献   

11.
Employing the STO-3G and 4–31 G basis sets within the unrestricted Hartree-Fock method the equilibrium structure of the CCl3 radical was calculated. The calculations predict the radical to be non-planar with both basis sets used. Using the UHF optimized geometries the SWXα calculations have been performed to calculate energy levels, ionization potentials and electron affinities of CCl3.  相似文献   

12.
The geometries of molecules H_3AXAH_3(X=O,S,Se and A=C,Si)have been optimizedusing STO-3G ab initio calculations and gradient method and the results are in good agreement withreported experimental values.From the STO-3G optimized geometries,we have also calculated theelectronic structures of these molecules using 4-31G and 6-31G basis sets to obtain the MO energies.atomic net charges and dipole moments.The ionization potentials calculated by 6-31G basis set are ingood agreement with experimental values.  相似文献   

13.
用量子化学从头算方法(STO-3G基组)对(C5H5)2Ti(CO)2进行几何优化,得到平衡几何构型,并在此基础上采用STO-3-21G基组对(C5H5)2Ti(CO)2进行单点计算,计算结果表明:(C5H5)2Ti(CO)2的HOMO具有Ti→CO反馈π键性质,理论计算结果与实验相符。  相似文献   

14.
MO STO-3G ab initio calculations have been carried out for the antiparallel dipole and the head-to-tail dipole model of acetonitrile dimers. The optimized interaction enthalpy is about half of the lowest experimental estimate. The calculated interaction distance for the antiparallel dipole model is very close to the sum of intermolecular radii of N and C; the distance for the head-to-tail model is about 20% higher than the sum of N and H intermolecular radii. The discussion of the interaction in terms of the supermolecule MO's suggests for both models a bonding of mainly electrostatic character. The shortcomings of the STO-3G basis set in dealing with this problem are compared with those reported in the literature. The influence of the basis set on the calculated electron distribution in acetonitrile monomer was examined as a preliminary part of the present study, and is also reported in the paper.  相似文献   

15.
The results of ab initio STO-3G and STO-4G calculations are reported on tTt- and tCt-1,3,5-hexatriene, including a STO-3G partial geometry optimization of all C/C bond lengths in both isomers. Results are also reported from a partial INDO geometry optimization on.the tTt-isomer, and complete optimizations on both isomers using empirical consistent force Meld programs. Significant discrepancies are found to exist between these calculated structures and those based on the electron diffraction analysis of Traetteberg. In addition, further results of a CNDO/S spectral analysis are presented and compared with experiment.  相似文献   

16.
Ab initio calculations with an STO-3G basis and geometry optimization have been performed on n-propyl cyanide and isocyanide in four rotational conformations, trans, cis, and gauche, with, in the latter case, two different dihedral angles, 90° and 120° from the trans position, being employed. The trans and gauche 120° isomers are predicted to be the most stable for both the cyanide and isocyanide, and the cyanide—isocyanide energy difference is calculated to be approximately 22 kcal mole?1 for each rotational isomer. The results of a population analysis are employed to discuss the electronic structures of the cyanide, isocyanide, and the isomerization process.  相似文献   

17.
Harmonic force constants, in-plane vibrational frequencies, and in-plane vibrational modes of cytosine were calculated by an ab initio Hartree—Fock SCF MO method. The force contants were calculated by the use of an energy gardient method with the STO-3G basis set, and then they were corrected into “4-31G force constants” by the scaling factors given by us previously for the case of uracil. The corrected set of force constants can produce a calculated vibrational spectra of cytosine and cytosine-1,amino-d3, that can be well corrected with the observed Raman and infrared spectra of these compounds, with little ambiguity. Thus, the assignments of all the in-plane vibrations are now practically established. The calculated vibrational modes, in addition, can account for the recently published resonance Raman effects of cytosine residue.  相似文献   

18.
Possible refinements of semiempirical methods include the use of larger basis sets and of correlated wave functions. These possibilities are investigated in semiempirical NDDO SCF calculations with the STO-3G and 4-31G basis sets, and in correlated calculations at the STO-3G level. The present approach is characterized by the analytical evaluation of all one-center terms and two-electron integrals, and the semiempirical adjustment of the remaining one-electron integrals and the nuclear repulsions. The NDDO SCF results tend to reproduce the correspondingab initio results more closely than experimental data, even if they are parametrized with respect to experiment. The explicit inclusion of electron correlation at the STO-3G level improves the calculated results only slightly.  相似文献   

19.
Summary A comparison of semi-empirical (MNDO) and ab initio (GAUSSIAN) calculations for disiloxane and related molecules is given. The STO-3G* basis set well reproduced the observed geometries of disiloxane (*), DZP, TZVP) gave much poorer agreement with the observed geometries.Comparison of the STO-3G* and the STO-3G basis sets demonstrates the necessity of including d-orbitals on the silicon. However, the semi-empirical MNDO program gave, despite the absence of d-orbitals, a better approximation to the molecular geometry than the complex ab initio basis sets.Force field parameters have been calculated for kSiOSi, kOSiO, 0.089 and 0.73 mdyneÅ/rad2, and the SiOSiO torsion which has a V1 potential of –0.68 kcal/mol. In addition, the HSiOH torsion is shown to have a three-fold potential of 0.78 kcal/mol. These are profoundly different from the analogous carbon-oxygen force constants, demonstrating that C-O parameters cannot be transferred to the corresponding Si-O systems.  相似文献   

20.
Ab initio molecular orbital calculations using the STO-6G and STO6-21G basis sets have been performed for the cluster series Li n + , Li n , and Li n (wheren=2–7). Thirty-two optimized structures are discussed and reported, many of which (especially for the anionic structures) have not yet been considered. The calculations suggest that for all three species the optimum geometries are planar. Of the two levels of theories that were investigated, STO-6G//STO-6G and STO6-21G//STO-6G, the latter hybrid theory was found to be less reliable. In particular, for the anionic structures these calculations should provide a platform from which more sophisticated, i.e., configuration interaction, geometry optimization can be performed.  相似文献   

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