Westerlund Fredrik, Nordell Pär, Blechinger Julia, Santos Teresa M, Nordén Bengt, Lincoln Per
Department of Chemical and Biological Engineering, Chalmers University of Technology, SE-41296 Gothenburg, Sweden.
J Phys Chem B. 2008 May 29;112(21):6688-94. doi: 10.1021/jp711116z. Epub 2008 May 2.
We recently reported that ruthenium complexes, with general structure mu-bidppz(bipy)4Ru2 (B) or mu-bidppz(phen)4Ru2 (P) (bidppz=11,11'-bi(dipyrido[3,2- a:2',3'-c]phenazinyl)), show extreme kinetic selectivity for long AT tracts over mixed-sequence calf thymus DNA (ct-DNA), a selectivity that also varies markedly with the size (between B and P) and sense of chirality of the complex. Earlier studies, exploiting the great increase in luminescence intensity when the compound intercalates, have yielded complex kinetics indicating the presence of both first- and second-order processes. Even with a homogeneous DNA sequence, such as poly(dAdT)2, the luminescence kinetics generally requires more than a single exponential for a satisfactory fit. We here reveal that at least part of the complexity is a result of the extreme sensitivity of the effective quantum yield of the complexes, so that the luminescence trajectories also reflect subtle variations in the environment and binding geometry that the complex is sampling on its path to its final binding site. By monitoring the rearrangement process using circular dichroism (CD), we show that threading of both enantiomers of B and P into poly(dAdT)2 is effectively a monoexponential process, as expected if the compounds are not affecting each other during the intercalation process. Thus, the complex luminescence trajectories may be explained by slow relaxations in the binding geometry (DNA conformation) and associated changes in the environment of the entering complexes. To further disentangle the intriguing features of the threading intercalation kinetics, and how they may depend on the flexibility and size of the ruthenium complexes, we have also designed and studied two new ruthenium complexes, mu-dtpf(phen)4Ru2 (F) (dtpf=4,5,9,12,16,17,21,25-octaaza-23 H-ditriphenyleno[2,3-b:2,3-h]fluorene), in which the bridging ligand is made totally rigid, and mu-bidppz([12]aneS4) 2Ru2 (S), which has less bulky, nonaromatic ancillary ligands. The threading of F into poly(dAdT)2, also found to be a monoexponential process, is about 3 times slower than for P, indicating that the flexibility of the bridging ligand is an important factor for the intercalation rate. Surprisingly, in contrast to all other compounds, S requires two exponentials to fit its binding kinetics as monitored by CD. Also surprisingly, in view of the smaller steric bulk, even the fastest phase is roughly 2 times slower for S than for B and P. Thus, not only the size of the ancillary ligand but also other properties that can influence the energy landscape of the threading path are rate-determining factors. With mixed-sequence ct-DNA, threading of B and that of P are both multiphasic processes when monitored with CD as well as with luminescence. The rate constants for threading into ct-DNA show much larger variations between complexes than for poly(dAdT)2, confirming earlier results based on luminescence data.
我们最近报道,具有通式μ-bidppz(bipy)₄Ru₂(B)或μ-bidppz(phen)₄Ru₂(P)(bidppz = 11,11'-联(二吡啶并[3,2-a:2',3'-c]吩嗪基))的钌配合物,对长AT序列比对混合序列的小牛胸腺DNA(ct-DNA)表现出极高的动力学选择性,这种选择性也随配合物的大小(B和P之间)以及手性方向而显著变化。早期研究利用化合物插入时发光强度的大幅增加,得到了复杂的动力学结果,表明存在一级和二级过程。即使对于均匀的DNA序列,如聚(dAdT)₂,发光动力学通常也需要不止一个指数函数才能得到满意的拟合。我们在此揭示,至少部分复杂性是由于配合物有效量子产率的极高敏感性,因此发光轨迹也反映了配合物在其到达最终结合位点的过程中所采样的环境和结合几何结构的细微变化。通过使用圆二色性(CD)监测重排过程,我们表明B和P的两种对映体插入聚(dAdT)₂实际上是单指数过程,这与化合物在插入过程中不相互影响的预期一致。因此,复杂的发光轨迹可以通过结合几何结构(DNA构象)中的缓慢弛豫以及进入配合物环境中的相关变化来解释。为了进一步解开穿线插入动力学的有趣特征,以及它们如何可能取决于钌配合物的柔韧性和大小,我们还设计并研究了两种新的钌配合物,μ-dtpf(phen)₄Ru₂(F)(dtpf = 4,5,9,12,16,17,21,25-八氮杂-23H-二三亚苯并[2,3-b:2,3-h]芴),其中桥连配体完全刚性,以及μ-bidppz([12]aneS₄)₂Ru₂(S),其具有体积较小的非芳香辅助配体。F插入聚(dAdT)₂也被发现是单指数过程,比P慢约3倍,表明桥连配体的柔韧性是插入速率的重要因素。令人惊讶的是,与所有其他化合物相比,S需要两个指数函数来拟合其通过CD监测的结合动力学。同样令人惊讶的是,鉴于较小的空间体积,即使是最快的相,S也比B和P慢约2倍。因此,不仅辅助配体的大小,而且其他可以影响穿线路径能量景观的性质都是速率决定因素。对于混合序列的ct-DNA,用CD以及发光监测时,B和P的穿线都是多相过程。插入ct-DNA的速率常数在配合物之间的变化比聚(dAdT)₂大得多,证实了基于发光数据的早期结果。