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顺磁钌-双咪唑衍生物 [(acac)2Ru(III)(LHn)]m,n/m = 2/+,1/0,0/-。合成、结构、溶液性质及溶液状态下的阴离子受体特征。

Paramagnetic ruthenium-biimidazole derivatives [(acac)2Ru(III)(LHn)]m, n/m = 2/+, 1/0, 0/-. Synthesis, structures, solution properties and anion receptor features in solution state.

机构信息

Department of Chemistry, Indian Institute of Technology Bombay, Powai, Mumbai 400076, India.

出版信息

Dalton Trans. 2010 May 7;39(17):4232-42. doi: 10.1039/b919036h. Epub 2010 Mar 25.

Abstract

The paramagnetic ruthenium-biimidazole complexes [(acac)(2)Ru(III)(LH(-))] (1 = red-brown), (acac)(2)Ru(III)(LH(2)) (2 = pink) and Bu(4)N[(acac)(2)Ru(III)(L(2-))] (3 = greenish yellow) comprising of monodeprotonated, neutral and bideprotonated states of the coordinated biimidazole ligand (LH(n), n = 1, 2, 0), respectively, have been isolated (acac(-) = acetylacetonate). Single-crystal X-ray diffraction of 1 reveals that the asymmetric unit consists of three independent molecules: A-C, where molecule A corresponds to complex 1 and the other two molecules B and C co-exist as a hydrogen bonded dimeric unit perhaps between the cationic 2(+) and anionic 3(-). The packing diagram further reveals that the molecule A in the crystal of 1 also forms a hydrogen bonded dimer with the neighbouring another unit of molecule A. The formation of (acac)(2)Ru(III)(LH(2)) (2) has also been authenticated independently by its single-crystal X-ray structure. The packing diagram of 2 shows multiple hydrogen bonds between the N-H protons of coordinated LH(2) and the counter ClO(4)(-). Paramagnetic complexes show (1)H NMR spectra over a wide range of chemical shift, delta (ppm), +10 to -35 in CDCl(3). One-electron paramagnetic 1-3 (mu/B.M. approximately 1.9) exhibit distinct rhombic-EPR spectra with relatively large g anisotropic factors: 2.136-2.156 and Deltag 0.65-0.77, typical for distorted octahedral ruthenium(III) complexes. The complexes 1-3 are inter-convertible as a function of pH. The pK(a1) and pK(a2) of 6.8 and 11, respectively, for 2 are estimated by monitoring the pH dependent spectral changes. The Ru(III)-Ru(IV) couple near 1.25 V vs. SCE remains almost invariant in 1-3 whereas the corresponding Ru(III)-Ru(II) couple varies appreciably in the range of -0.52 to -0.85 V vs. SCE based on the protonated-deprotonated states of the coordinated biimidazole ligand. Compounds 1-3 exhibit one weak ligand to metal charge transfer (LMCT) transition near 500 nm and intense intraligand transitions in the higher energy UV region. The spectrophotometric titrations of 2 with the TBA (TBA = tetrabutylammonium) salts of a wide variety of anions, F(-), Cl(-), Br(-), I(-), HSO(4)(-), OAc(-), H(2)PO(4)(-) in CH(3)CN reveal that the possible hydrogen bonds between the N-H protons of LH(2) in 2 and Cl(-) or Br(-) or I(-) or HSO(4)(-) or H(2)PO(4)(-) anion are rather weak or negligible. However, in presence of excess H(2)PO(4)(-) anion, the molar ratio of 2 to H(2)PO(4)(-) being 1 : 4, simple liberation of one N-H proton of the coordinated LH(2) in 2 has been taken place which in effect yields 1 and H(3)PO(4). On the contrary, the spectrophotometric titrations of 1 : 1 molar solution of 2 and OAc(-) or F(-) anion suggest the initial formation of hydrogen bonds between the N-H protons of LH(2) in 2 and the anion with the calculated log K value of 5.92 or 4.7, respectively, which eventually leads to the transfer of one of the N-H protons of LH(2) in 2 to the anion, resulting in 1 and HOAc or HF. On addition of excess OAc(-) to the above solution of 1 (molar ratio of OAc(-) to 1, 4 : 1), further hydrogen bonding between the N-H proton of LH(-) in 1 and OAc(-) occurs but without the abstraction of the N-H proton of LH(-). However, excess F(-) anion concentration (molar ratio of anion to 1, 5 : 1) facilitates the removal of the remaining N-H proton of LH(-) in 1 which in turn yields 3 incorporating the bideprotonated form L(2-).

摘要

顺磁的钌-双咪唑配合物[(acac)(2)Ru(III)(LH(-))] (1 = 红棕色)、(acac)(2)Ru(III)(LH(2)) (2 = 粉红色)和 Bu(4)N[(acac)(2)Ru(III)(L(2-))] (3 = 绿黄色),分别包含配位双咪唑配体的单去质子化、中性和双去质子化态(LH(n), n = 1, 2, 0),已被分离出来(acac(-) = 乙酰丙酮根)。1 的单晶 X 射线衍射表明,不对称单元由三个独立的分子组成:A-C,其中分子 A 对应于配合物 1,而另外两个分子 B 和 C 则以可能在阳离子 2(+)和阴离子 3(-)之间的氢键二聚体形式共存。堆积图进一步表明,晶体中的分子 A 也与相邻的另一个分子 A 形成氢键二聚体。(acac)(2)Ru(III)(LH(2)) (2)的形成也通过其单晶 X 射线结构得到了独立的验证。2 的堆积图显示了配位 LH(2)的 N-H 质子与抗衡 ClO(4)(-)之间的多个氢键。顺磁配合物在 CDCl(3)中显示出宽化学位移范围(ppm),从+10 到-35 的(1)H NMR 谱。一电子顺磁体 1-3 (μ/B.M.约 1.9)表现出明显的菱形 EPR 谱,具有相对较大的 g 各向异性因子: 2.136-2.156 和 Deltag 0.65-0.77,这是典型的扭曲八面体钌(III)配合物。配合物 1-3 可以作为 pH 的函数相互转化。通过监测 pH 依赖的光谱变化,2 的 pK(a1)和 pK(a2)分别估计为 6.8 和 11。在 1-3 中,Ru(III)-Ru(IV) 对在 1.25 V 左右与 SCE 几乎不变,而相应的 Ru(III)-Ru(II) 对在-0.52 至-0.85 V 左右与 SCE 之间变化显著,这取决于配位双咪唑配体的质子化-去质子化状态。化合物 1-3 在近 500nm 处表现出一个弱的配体到金属电荷转移(LMCT)跃迁和在高能 UV 区的强烈的内配体跃迁。2 与各种阴离子(TBA = 四丁基铵)盐的 TBA 分光光度滴定实验,如 F(-)、Cl(-)、Br(-)、I(-)、HSO(4)(-)、OAc(-)、H(2)PO(4)(-),表明 2 中 LH(2)的 N-H 质子与 Cl(-)或 Br(-)或 I(-)或 HSO(4)(-)或 H(2)PO(4)(-)阴离子之间的氢键可能较弱或可以忽略不计。然而,在过量 H(2)PO(4)(-)阴离子存在下,2 与 H(2)PO(4)(-)的摩尔比为 1 : 4,2 中配位 LH(2)的一个 N-H 质子已经发生了简单的释放,这实际上生成了 1 和 H(3)PO(4)。相反,2 与 OAc(-)或 F(-)阴离子的 1 : 1 摩尔溶液的分光光度滴定表明,最初在 2 中 LH(2)的 N-H 质子与阴离子之间形成了氢键,其计算的 log K 值分别为 5.92 或 4.7,最终导致 2 中 LH(2)的一个 N-H 质子转移到阴离子上,生成 1 和 HOAc 或 HF。在上述 1 的溶液(阴离子与 1 的摩尔比为 4 : 1)中加入过量的 OAc(-)后,1 中 LH(-)的 N-H 质子与 OAc(-)之间会发生进一步的氢键,但不会发生 LH(-)的 N-H 质子的离解。然而,过量的 F(-)阴离子浓度(阴离子与 1 的摩尔比为 5 : 1)有利于去除 1 中剩余的 LH(-)的 N-H 质子,从而生成了包含双质子化形式 L(2-)的 3。

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