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从氙溶液的变温红外光谱、r0 结构参数和吡咯烷的振动分配推断构象稳定性。

Conformational stability from variable-temperature infrared spectra of xenon solutions, r0 structural parameters, and vibrational assignment of pyrrolidine.

机构信息

Department of Chemistry, University of Missouri-Kansas City, Kansas City, Missouri 64110, United States.

出版信息

J Phys Chem A. 2011 Jul 7;115(26):7473-83. doi: 10.1021/jp200692t. Epub 2011 Jun 15.

DOI:10.1021/jp200692t
PMID:21619013
Abstract

The infrared spectra of gaseous and variable-temperature liquid xenon solutions of pyrrolidine have been recorded. The enthalpy difference has been determined to be 109 ± 11 cm(-1) (1.30 ± 0.13 kJ mol(-1)) with the envelope-equatorial conformer more stable than the twist form with 37 ± 3% present at ambient temperature. Ab initio calculations utilizing various basis sets up to MP2(full)/aug-cc-pVTZ have been used to predict the conformational stabilities, energy at the equatorial-axial saddle point, and barriers to planarity. From previously reported microwave rotational constants along with MP2(full)/6-311+G(d,p) predicted structural values, adjusted r(0) parameters have been obtained for both conformers. Heavy atom distances (Å) of equatorial[twist] conformer are as follows: N(1)-C(2) = 1.469(3)[1.476(3)], N(1)-C(3) = 1.469(3)[1.479(3)], C(2)-C(4) = 1.541(3)[1.556(3)], C(3)-C(5) = 1.541(3)[1.544(3)], C(4)-C(5) = 1.556(3)[1.543(3)]; and angles (deg)∠N(1)C(2)C(4) = 102.5(5)[107.6(5)], ∠N(1)C(3)C(5) = 102.5(5)[105.4(5)], ∠C(2)C(4)C(5) = 104.3(5)[104.6(5)], ∠C(3)C(5)C(4) = 104.3(5)[103.7(5)], ∠C(2)N(1)C(3) = 104.1(5)[103.9(5)], τC(2)C(4)C(5)C(3) = 0.0(5)[13.5(5)]. A complete vibrational assignment is proposed for both conformers.

摘要

已记录气态和可变温度液态氙吡咯烷溶液的红外光谱。确定焓差为 109 ± 11 cm(-1)(1.30 ± 0.13 kJ mol(-1)),具有赤道构象的封套比扭曲形式更稳定,在环境温度下存在 37 ± 3%。利用各种基组直至 MP2(full)/aug-cc-pVTZ 的从头算计算被用于预测构象稳定性、赤道-轴向鞍点的能量和平面化的势垒。根据以前报道的微波旋转常数以及 MP2(full)/6-311+G(d,p)预测的结构值,已获得两种构象的调整 r(0)参数。赤道[扭曲]构象的重原子距离(Å)如下:N(1)-C(2) = 1.469(3)[1.476(3)],N(1)-C(3) = 1.469(3)[1.479(3)],C(2)-C(4) = 1.541(3)[1.556(3)],C(3)-C(5) = 1.541(3)[1.544(3)],C(4)-C(5) = 1.556(3)[1.543(3)];以及角度(°)∠N(1)C(2)C(4) = 102.5(5)[107.6(5)],∠N(1)C(3)C(5) = 102.5(5)[105.4(5)],∠C(2)C(4)C(5) = 104.3(5)[104.6(5)],∠C(3)C(5)C(4) = 104.3(5)[103.7(5)],∠C(2)N(1)C(3) = 104.1(5)[103.9(5)],τC(2)C(4)C(5)C(3) = 0.0(5)[13.5(5)]。为两种构象都提出了完整的振动分配。

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