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可溶解 AgCl 的互贯配位笼中的抗衡离子动力学。

Counterion dynamics in an interpenetrated coordination cage capable of dissolving AgCl.

机构信息

Institute for Inorganic Chemistry, Georg-August University Göttingen, Tammannstrasse 4, 37077 Göttingen, Germany.

出版信息

Chemistry. 2013 Feb 4;19(6):2114-21. doi: 10.1002/chem.201203086. Epub 2012 Dec 19.

DOI:10.1002/chem.201203086
PMID:23255121
Abstract

In solution, the eight BF(4)(-) counterions of a positively charged D(4)-symmetric interpenetrated Pd(4)ligand(8) double cage (1) are localized in distinct positions. At low temperatures, one BF(4)(-) ion is encapsulated inside the central pocket of the supramolecular structure, two BF(4)(-) ions are bound inside the equivalent outer pockets, and the remaining five BF(4)(-) ions are located outside the cage structure (expressed by the formula [3 BF(4)@1]BF(4)). On warming, the two BF(4)(-) ions in the outer pockets are found to exchange with the exterior ions in solution whereas the central BF(4)(-) ion stays locked inside the central cavity (here written as [BF(4)@1]BF(4)). The exchange kinetics were determined by exchange spectroscopy (EXSY) NMR experiments and line-shape fitting in different solvents. The tremendously high affinity of this double cage for the binding of two chloride ions inside the outer pockets allows for complete exchange of two BF(4)(-) ions by the addition of solid AgCl to give [2 Cl+BF(4)@1]BF(4). The uptake of the two chloride ions is allosteric and is thus accompanied by a structural rearrangement (compression along the Pd(4) axis) of the double cage structure. An analysis by using 900 MHz NOESY NMR spectroscopy shows that this compression of about 3.3% is associated with a helical twist of 8°, which together resemble a screw motion. As a consequence of squeezing each of the outer two pockets by 53%, the volume of the central pocket is increased by 43%, which results in an increase of 36% in the (19)F spin-lattice relaxation time (T(1)) of the central BF(4)(-) ion. The packing coefficients (PC) for the ions in the outer pockets (103% for BF(4)(-) and 96% for Cl(-)) were calculated.

摘要

在溶液中,带正电荷的 D(4)-对称互穿 Pd(4)配体(8) 双笼 (1) 的 8 个 BF(4)(-)抗衡离子被定位在不同的位置。在低温下,一个 BF(4)(-)离子被包裹在超分子结构的中央口袋内,两个 BF(4)(-)离子被结合在等效的外口袋内,其余五个 BF(4)(-)离子位于笼状结构之外(用公式 [3 BF(4)@1]BF(4) 表示)。升温时,发现外口袋中的两个 BF(4)(-)离子与溶液中的外部离子发生交换,而中央的 BF(4)(-)离子则被锁定在中央腔室中(这里表示为 [BF(4)@1]BF(4))。通过交换光谱 (EXSY) NMR 实验和不同溶剂中的线宽拟合确定了交换动力学。这种双笼对两个氯离子在外部口袋中结合的极高亲和力允许通过添加固体 AgCl 完全交换两个 BF(4)(-)离子,得到 [2 Cl+BF(4)@1]BF(4)。两个氯离子的摄取是变构的,因此伴随着双笼结构的结构重排(沿 Pd(4)轴压缩)。使用 900 MHz NOESY NMR 光谱进行的分析表明,这种压缩约为 3.3%,与 8°的螺旋扭曲有关,这两者共同类似于螺旋运动。由于将每个外部两个口袋压缩 53%,中央口袋的体积增加了 43%,这导致中央 BF(4)(-)离子的 (19)F 自旋晶格弛豫时间 (T(1)) 增加了 36%。计算了外口袋中离子的堆积系数 (PC)(BF(4)(-)为 103%,Cl(-)为 96%)。

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