Ashby M T, Alguindigue S S, Schwane J D, Daniel T A
Department of Chemistry and Biochemistry, The University of Oklahoma, 620 Parrington Oval, Rm. 208, Norman, Oklahoma 73019, USA.
Inorg Chem. 2001 Dec 17;40(26):6643-50. doi: 10.1021/ic0105720.
Thioether complexes with the formula Delta/Lambda-chloro(thioether)bis(2,2'-bipyridine)metal(II) (M = Ru, Os; thioether = dimethyl sulfide (3a(+)), diethyl sulfide (3b(+)), and tetrahydrothiophene (3c(+))) have been synthesized. The rates of inversion at the sulfur atom of the thioether ligands have been measured by spin-inversion transfer and line-shape NMR methods. In every case, the ruthenium derivative exhibits a faster inversion frequency at a given temperature than the corresponding osmium derivative. In contrast, similar complexes with the formula chloro(delta/lambda-1,1'-biisoquinoline)(2,2':6',2"-terpyridine)metal(II), 4(M=Ru,Os)(+), undergo atropisomerization of the misdirected 1,1'-biisoquinoline (1,1'-biiq) ligand with rates that are faster for osmium than ruthenium. As a result of the lanthanide contraction effect and the similar metric parameters associated with the structures of second-row and third-row transition metal derivatives, steric factors associated with the isomerizations are presumably similar for the Ru and Os derivatives of these compounds. Since third-row transition metal complexes tend to have larger bond dissociation enthalpies (BDE) than their second-row congeners, we conclude the difference in reactivities of 3(M=Ru)(+) versus 3(M=Os)(+) and 4(M=Ru)(+) versus 4(M=Os)(+) are attributed to electronic effects. For 3, the S3p lone pair of the thioether, the principal sigma donor orbital, is orthogonal to the metal sigma acceptor orbital in the transition state of inversion at sulfur and the S 3s orbital is an ineffective sigma donor. Thus, a regular relationship between the kinetic and thermodynamic stabilities of 3(M=Ru)(+) and 3(M=Os)(+) is observed for the directed <==> [misdirected] <==> directed (DMD) isomerization (the more thermodynamically stable bond is less reactive). In contrast, atropisomerization of 4(+) involves redirecting (strengthening) the M-N bonds of the misdirected 1,1'-biiq ligand in the transition state. Therefore, an inverse relationship between the kinetic and thermodynamic stabilities of 4(M=Ru)(+) and 4(M=Os)(+) is observed for the misdirected <==> [directed] <==> misdirected (MDM) isomerization (the more thermodynamically stable bond is more reactive). The rates obtained for 4(+) are consistent with the rates of atropisomerization of Delta/Lambda-(delta/lambda-1,1'-biisoquinoline)bis(2,2'-bipyridine)metal(II), 1(M=Ru,Os)(2+), and (eta(6)-benzene) Delta/Lambda-(delta/lambda-1,1'-biisoquinoline)halometal(II), 2(M=Ru,Os;halo=Cl,I)(+), that we reported previously. We term the relative rates of reaction of second-row versus third-row transition metal derivatives kinetic element effects (KEE = k(second)/k(third)). While the KEE appears to be generally useful when comparing reactions of isostructural species (e.g. the relative rates of 1(M=Ru)(2+), 1(M=Os)(2+), and 1(M=Ir)(3+)), different temperature dependencies of reactions prevent the comparison of related reactions between species that have different structures (e.g., the 1,1'-biiq atropisomerization reactions of 1(M=Ru,Os)(2+) versus 2(M=Ru,Os;halo=Cl,I)(+) versus 4(M=Ru,Os)(+)). This problem is overcome by comparing entropies of activation and kinetic enthalpy effects (KHE = DeltaH(third)/DeltaH(second)). For a given class of 1,1'-biiq complexes, we observe a structure/reactivity relationship between DeltaH and the torsional twist of the 1,1'-biiq ligands that are measured in the solid state.
已合成通式为Δ/Λ - 氯(硫醚)双(2,2'-联吡啶)金属(II)(M = Ru,Os;硫醚 = 二甲基硫醚(3a(+))、二乙基硫醚(3b(+))和四氢噻吩(3c(+)))的硫醚配合物。通过自旋反转转移和线形核磁共振方法测量了硫醚配体硫原子处的反转速率。在每种情况下,钌衍生物在给定温度下的反转频率都比相应的锇衍生物快。相比之下,通式为氯(Δ/Λ - 1,1'-联异喹啉)(2,2':6',2"-三联吡啶)金属(II),4(M = Ru,Os)(+)的类似配合物,会发生方向错误的1,1'-联异喹啉(1,1'-biiq)配体的阻转异构化,其速率对于锇比钌更快。由于镧系收缩效应以及与第二排和第三排过渡金属衍生物结构相关的类似度量参数,这些化合物的钌和锇衍生物的异构化相关空间因素可能相似。由于第三排过渡金属配合物的键解离焓(BDE)往往比它们第二排的同系物更大,我们得出3(M = Ru)(+)与3(M = Os)(+)以及4(M = Ru)(+)与4(M = Os)(+)反应活性差异归因于电子效应。对于3,硫醚的S3p孤对电子,即主要的σ供体轨道,在硫原子反转的过渡态中与金属σ受体轨道正交,且S 3s轨道是无效的σ供体。因此,对于定向⇌[方向错误的]⇌定向(DMD)异构化,观察到3(M = Ru)(+)和3(M = Os)(+)的动力学稳定性和热力学稳定性之间存在常规关系(热力学上更稳定的键反应性更低)。相比之下,4(+)的阻转异构化涉及在过渡态中重新定向(加强)方向错误的1,1'-biiq配体的M - N键。因此,对于方向错误的⇌[定向的]⇌方向错误的(MDM)异构化,观察到4(M = Ru)(+)和4(M = Os)(+)的动力学稳定性和热力学稳定性之间存在相反关系(热力学上更稳定的键反应性更高)。4(+)得到的速率与我们之前报道的Δ/Λ - (Δ/Λ - 1,1'-联异喹啉)双(2,2'-联吡啶)金属(II), 1(M = Ru,Os)(2+)以及(η⁶ - 苯)Δ/Λ - (Δ/Λ - 1,1'-联异喹啉)卤金属(II), 2(M = Ru,Os;卤 = Cl,I)(+)的阻转异构化速率一致。我们将第二排与第三排过渡金属衍生物反应的相对速率称为动力学元素效应(KEE = k(第二)/k(第三))。虽然在比较同结构物种的反应时(例如1(M = Ru)(2+)、1(M = Os)(2+)和1(M = Ir)(3+)的相对速率)KEE似乎普遍有用,但反应的不同温度依赖性阻止了对具有不同结构的物种之间相关反应的比较(例如1(M = Ru,Os)(2+)与2(M = Ru,Os;卤 = Cl,I)(+)与4(M = Ru,Os)(+)的1,1'-biiq阻转异构化反应)。通过比较活化熵和动力学焓效应(KHE = ΔH(第三)/ΔH(第二))克服了这个问题。对于给定类别的1,1'-biiq配合物,我们观察到在固态中测量的ΔH与1,1'-biiq配体的扭转扭曲之间存在结构/反应性关系。