Orbital-overlap control of the reactivity of a bicyclic 1-hydroxy-1,4-biradical.
Orbital-overlap control of the reactivity of a bicyclic 1-hydroxy-1,4-biradical.
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DOI:
10.1002/anie.200500983
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发表时间:
2005-08
影响因子:
--
通讯作者:
C. Yang;W. Xia;J. Scheffer;M. Botoshansky;M. Kaftory
中科院分区:
文献类型:
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作者:
C. Yang;W. Xia;J. Scheffer;M. Botoshansky;M. Kaftory
1, 4-Biradicals are among the most ubiquitous reactive intermediates in organic chemistry, and are formed or implicated in a variety of reactions including [2+ 2] photocycloaddition,[1] the Paterno–Büchi reaction (oxetane formation),[2] the Norrish–Yang type II reaction,[3] and the elimination of nitrogen from cyclic azo compounds.[4] Once formed, 1, 4-biradicals suffer two main fates: closure to form compounds containing a four-membered ring, and cleavage of the central bond to produce a pair of double-bond-containing fragments.[5] Based on organic intuition backed by semiempirical calculations,[6] and supported by a wide variety of product studies,[1–4] the generally accepted qualitative picture of biradical reactivity is that cleavage is favored when the conformation allows the radical-containing orbitals at positions 1 and 4 to overlap with the sigma bond between positions2 and 3. Increasing amounts of cyclization are observed as this overlap diminishes, provided that the radical termini are within reasonable bonding distance of one another. However, quantitative experimental tests of this hypothesis are rare, in part as a result of the difficulty of establishing structure–reactivity relationships for conformationally mobile systems in fluid media. In the case of triplet 1, 4-biradicals, the picture is complicated by the likelihood that biradical behavior reflects the geometry in which the singlet biradical is formed by intersystem crossing (isc) from the triplet, which may differ significantly from the geometry of the conformationally equilibrated species.[7] For these reasons, we have elected to work with compounds in the crystalline state, where molecular conformation is fixed and determinable by X-ray crystallography, and where the singlet biradical formed by isc has the same geometry as its triplet precursor. We have shown that 1-hydroxy-1, 4-biradicals can be generated conveniently in the solid state by the Norrish–Yang typeII reaction, and that because hydrogen-atom transfer occurs with very little movement of the associated heavy atoms, the structure and conformation of the biradicals can be inferred directly from the X-ray crystal structures of their ground-state precursors.[8] Herein, we compare and contrast the behavior of 1-hydroxy-1, 4-biradicals of general structures 1 and 2. These biradicals are interesting because, unlike the majority of biradicals studied previously, they have only one significant degree of conformational freedom, namely, rotation about the C1ÀC2 bond. Among the questions we wished to answer about these biradicals were: 1) how does the orientation of the p orbital at the C1 position affect the ratio of cyclization to cleavage; and 2) can we correlate the orientation of the porbital at C1 with preferential cleavage of either the C2ÀC3 or C2ÀC3’bond? As described below, satisfactory answers to these questions were obtained by generating biradicals 1 and 2 in the crystalline state and correlating their behavior in this medium with their conformations as determined by X-ray crystallography. We are not the first to study biradicals of types 1 and 2. The solution-phase behavior of biradical 2 (Ar= Ph) was reported in 1972 by Padwa and Eisenberg and shown to consist of 66% cleavage and 30% cyclization.[9] Similarly, Alexander and Uliana showed in 1976 that, in solution, biradical 1 (Ar= Ph) bearing a phenyl substituent at the C2 position undergoes 100% cyclization.[10] In both cases, the biradicals were formed by a Norrish–Yang typeII photoreaction of the corresponding ketone. In the present work, we chose to investigate ketones in which the aryl group bears a carboxylic acid substituent in the para position, that is, ketones of general structures 3 and …