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[(dppc)(Cl)Cu(μ-Cl)2Cu(Cl)(dppc)] | 476630-09-8

中文名称
——
中文别名
——
英文名称
[(dppc)(Cl)Cu(μ-Cl)2Cu(Cl)(dppc)]
英文别名
[(diisopropylpyridine-2,6-dicarboxylate)(Cl)Cu(μ-Cl)2Cu(Cl)(diisopropylpyridine-2,6-dicarboxylate)]
[(dppc)(Cl)Cu(μ-Cl)2Cu(Cl)(dppc)]化学式
CAS
476630-09-8
化学式
C26H34Cl4Cu2N2O8
mdl
——
分子量
771.469
InChiKey
GVKFATAZEKIMFV-UHFFFAOYSA-J
BEILSTEIN
——
EINECS
——
  • 物化性质
  • 计算性质
  • ADMET
  • 安全信息
  • SDS
  • 制备方法与用途
  • 上下游信息
  • 反应信息
  • 文献信息
  • 表征谱图
  • 同类化合物
  • 相关功能分类
  • 相关结构分类

计算性质

  • 辛醇/水分配系数(LogP):
    None
  • 重原子数:
    None
  • 可旋转键数:
    None
  • 环数:
    None
  • sp3杂化的碳原子比例:
    None
  • 拓扑面积:
    None
  • 氢给体数:
    None
  • 氢受体数:
    None

反应信息

  • 作为产物:
    描述:
    copper dichloride 、 diisopropyl pyridine-2,6-dicarboxylate四氢呋喃异丙醇 为溶剂, 以76%的产率得到[(dppc)(Cl)Cu(μ-Cl)2Cu(Cl)(dppc)]
    参考文献:
    名称:
    Structural, Electronic, and Magnetic Consequences of O-Carbonyl vs O-Alkoxy Ester Coordination in New Dicopper Complexes Containing the Cu2(μ-Cl)2 Core
    摘要:
    The complexes [Cu-2(mu-Cl)(2)(Cl)(2)(L)(2)] (L = dialkylpyridine-2,6-dicarboxylate; R = Et, L = depc, 1; R = i-Pr, L = dppc, 2) have been prepared and their magnetic properties studied. The crystal structures of complexes 1 and 2 have been solved. Compound 1 belongs to the P1 space group with Z = 2, a = 8.3020(10) Angstrom, b = 9.2050(10) Angstrom, c = 10.065(2) Angstrom, a = 99.040(10)degrees, beta = 100.810(10)degrees, and gamma = 106.502(10)degrees whereas 2 belongs to the C2/c space group with Z = 8, a = 11.6360(10) Angstrom, b = 25.906(3) Angstrom, c = 11.76579(10) Angstrom, and beta = 107.900(10)degrees. The different alkyl ester substitutes produce substantial structural and electronic differences. The Cu2Cl2 core geometry is planar for 1 whereas it adopts a butterfly shape in the case of 2. Furthermore, in 2 the dppc ligand coordinates only by the carbonyl oxygen atoms whereas in 1 the depc ligand coordinates through carbonyl and alkoxy oxygen atoms. Magnetic susceptibility data show a ferromagnetic coupling between the two Cu(II) centers in both cases (J = 39.9(6) cm(-1) for 1, and J = 51.3(5) cm(-1) for 2) with very weak antiferromagnetic interactions (J' = -0.59 cm(-1) and -0.57 cm(-1) for 1 and 2, respectively). Theoretical calculations at the extended Huckel level have also been carried out to further understand the electronic nature of complexes 1 and 2.
    DOI:
    10.1021/ic025568i
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