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A crystallographic and theoretical study of halogen···halogen and halogen···halide synthons.

机译:卤素··卤素和卤素···卤化物合成子的晶体学和理论研究。

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摘要

The physical nature of halogen···halogen and halogen···halide interactions has been investigated using both ab initio calculations and crystallographic studies. Both studies show that halogen···halogen and halogen···halide interactions are electrostatic in nature. An electrostatic model is proposed to explain these interactions. This model is based on two main ideas; (a) the presence of a positive electrostatic cap on the halogen atom (except for fluorine), (b) the electronic charge is anisotropically distributed around the halogen atom. Halogen···halogen contacts in organic molecules can be represented as C-Y1˙˙˙Y2-C [where theta 1= C-Y1˙˙˙Y2, theta2 = Y1˙˙˙Y2-C; Y = Cl, Br, I]. Halogen···halogen interactions are characterized by a Y1···Y 2 separation distance less than the sum of van der Waals radii ( rvdW) of the halogen atoms. According to the electrostatic model, two preferred arrangements are possible; (a) theta1= theta 2 = ca. 150°; (b) theta1 =180° and theta 2 = 90°. The second arrangement is not investigated during our study due to the fact that at this geometry, other interactions interfere with these contacts. A population analysis of the Cambridge Structural Data Base and ab initio calculations confirm the existence of the former geometry. Closely examining this geometry shows that these contacts are influenced by three factors; (a) the type of the halogen atom; (b) hybridization of the ipso carbon; (c) the nature of the other atoms that are bonded to the ipso carbon atom apart from the halogen atom.;Halogen···halide interactions are represented by C-Y···X (X = F-, Cl-, Br -, I-). These interactions are characterized by a Y···X distance less than sum of the rvdW of the halogen atom and the ionic radius of halide anion, as well as a linear C-Y···X angle. This arrangement is expected from the electrostatic model - the halide anion should confront the positive electrostatic potential cap of the halogen. Two types of halogen···halide interactions are studied; (1) simple halogen···halide interactions. Results show that these interactions are influenced by four factors; (i) the type of the halide anion; (ii) the type of the halogen atom; (iii) the hybridization of the ipso carbon; (iv) the nature of the functional groups; (2) C-Y···X-Cu (Y = Cl, Br; X = Cl-, Br-). These interactions are studied in complexes of the type (nCP)2CuX4 (nCP+ = n-chloropyridinium; n = 2, 3, or 4; X = Cl- or Br-) and Cu(nbp)2X2, (nbp = n-bromopyridine; n = 2 and 3). A comparison of the role of these synthons in these and previously published (nBP)2CuX4 structures (nBP = n-bromopyridinium cations; X = Br- or Cl-; n = 2) shows that; (a) the heavier the halogen atom, the stronger these interactions; (b) the lighter the halide anion, the stronger these interactions and; (c) these interactions are stronger in the complexes of the ( nBP)2CuX4 in comparison to Cu(nbp) 2X2. All of these observations fit the electrostatic model. These studies show that halogen···halide interactions are directional in nature. This implies that this synthonic interaction can act as a potential crystal engineering tool in the directed architecture of supramolecular species.
机译:使用从头算和晶体学研究方法研究了卤素··卤素和卤素···卤化物相互作用的物理性质。两项研究均表明,卤素··卤素和卤素···卤化物相互作用本质上是静电的。提出了静电模型来解释这些相互作用。该模型基于两个主要思想; (a)在卤原子(除氟之外)上存在一个正性静电帽,(b)电子电荷各向异性地分布在卤原子周围。有机分子中的卤素··卤素接触可以表示为C-Y1·Y2-C [其中θ1= C-Y1·Y2,θ2= Y1·Y2-C ; Y = Cl,Br,I]。卤素···卤素相互作用的特征在于Y1···Y2的分离距离小于卤素原子的范德华半径(rvdW)之和。根据静电模型,两个优选的布置是可能的;第二个布置是可能的。 (a)theta1 = theta 2 =ca。 150°; (b)theta1 = 180°和theta 2 = 90°。由于在这种几何形状下,其他相互作用会干扰这些接触,因此在我们的研究过程中未研究第二种布置。对剑桥结构数据库的总体分析和从头算的计算证实了前几何的存在。仔细检查这种几何形状,可以发现这些接触受到三个因素的影响。 (a)卤素原子的类型; (b)ipso碳的杂交; (c)除卤素原子外,与ipso碳原子键合的其他原子的性质。卤素···卤化物相互作用用CY··X(X = F-,Cl-,Br-,一世-)。这些相互作用的特征在于Y··X距离小于卤素原子的rvdW与卤化物阴离子的离子半径之和,以及线性C-Y··X角。从静电模型可以预期这种排列方式-卤化物阴离子应面对卤素的正静电势上限。研究了两种类型的卤素·卤化物相互作用: (1)简单的卤素···卤化物相互作用。结果表明,这些相互作用受四个因素的影响。 (i)卤化物阴离子的类型; (ii)卤素原子的类型; (iii)ipso碳的杂交; (iv)职能小组的性质; (2)C-Y···X-Cu(Y = Cl,Br; X = Cl-,Br-)。在(nCP)2CuX4(nCP + = n-氯吡啶鎓; n = 2、3或4; X = Cl-或Br-)和Cu(nbp)2X2(nbp = n-溴吡啶)的配合物中研究了这些相互作用。 ; n = 2和3)。比较这些合成子在这些结构和以前发表的(nBP)2CuX4结构中的作用(nBP = n-溴吡啶鎓阳离子; X = Br-或Cl-; n = 2); (a)卤素原子越重,这些相互作用越强; (b)卤化物阴离子越轻,这些相互作用越强;并且(c)与Cu(nbp)2X2相比,在(nBP)2CuX4的配合物中这些相互作用更强。所有这些观察结果都符合静电模型。这些研究表明卤素···卤化物相互作用本质上是定向的。这意味着这种超音速相互作用可以在超分子物种的定向结构中充当潜在的晶体工程工具。

著录项

  • 作者

    Awwadi, Firas Fandi.;

  • 作者单位

    Washington State University.;

  • 授予单位 Washington State University.;
  • 学科 Chemistry Physical.
  • 学位 Ph.D.
  • 年度 2005
  • 页码 184 p.
  • 总页数 184
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

  • 入库时间 2022-08-17 11:41:37

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