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B型和Z型聚(dG-dC)·聚(dG-dC)中的内部运动:1H NMR弛豫研究

Internal motions in B- and Z-form poly(dG-dC).poly(dG-dC): 1H NMR relaxation studies.

作者信息

Mirau P A, Behling R W, Kearns D R

出版信息

Biochemistry. 1985 Oct 22;24(22):6200-11. doi: 10.1021/bi00343a026.

Abstract

Proton NMR relaxation measurements are used to compare the molecular dynamics of 60 base pair duplexes of B- and Z-form poly(dG-dC).poly(dG-dC). The relaxation rates of the exchangeable guanine imino protons (Gim) in H2O and in 90% D2O show that below 20 degrees C spin-lattice relaxation is exclusively from proton-proton magnetic dipolar interactions while proton-nitrogen interactions contribute about 30% to the spin-spin relaxation. The observation that the spin-lattice relaxation is nonexponential and that the initial spin-lattice relaxation rate of the Gim, G-H8 and C-H6 protons depends on the selectivity of the exciting pulse shows that spin-diffusion dominates the spin-lattice relaxation. The relaxation rates of the Gim, C-H5, and C-H6 in B- and Z-form poly(dG-dC).poly(dG-dC) cannot be explained by assuming the DNA behaves as a rigid rod. The data can be fit by assuming large-amplitude out of plane motions (+/- 30-40 degrees, tau = 1-100 ns) and fast, large-amplitude local torsional motions (+/- 25-90 degrees, tau = 0.1-1.5 ns) in addition to collective torsional motions. The results for the B and Z forms show that the rapid internal motions are similar and large in both conformations although backbone motions are slightly slower, or of lower amplitude, in Z DNA. At high temperatures (greater than 60 degrees C), imino proton exchange with solvent dominates the spin-lattice relaxation of B-form poly(dG-dC).poly(dG-dC), but in the Z form no exchange contribution (less than 2 s-1) is observed at temperatures as high as 85 degrees C. Conformational fluctuations that expose the imino protons to the solvent are strikingly different in the B and Z forms. The results obtained here are compared with those previously reported for poly(dA-dT).poly(dA-dT).

摘要

利用质子核磁共振弛豫测量来比较B型和Z型聚(dG-dC)·聚(dG-dC)60个碱基对双链体的分子动力学。在H₂O和90%D₂O中可交换鸟嘌呤亚氨基质子(Gim)的弛豫速率表明,在20℃以下,自旋晶格弛豫完全来自质子-质子磁偶极相互作用,而质子-氮相互作用对自旋-自旋弛豫的贡献约为30%。Gim、G-H8和C-H6质子的自旋晶格弛豫是非指数性的,且其初始自旋晶格弛豫速率取决于激发脉冲的选择性,这一观察结果表明自旋扩散主导自旋晶格弛豫。B型和Z型聚(dG-dC)·聚(dG-dC)中Gim、C-H5和C-H6的弛豫速率不能通过假设DNA表现为刚性棒来解释。除了集体扭转运动外,通过假设大幅度的平面外运动(±30-40°,τ = 1-100 ns)和快速、大幅度的局部扭转运动(±25-90°,τ = 0.1-1.5 ns),数据可以得到拟合。B型和Z型的结果表明,尽管Z-DNA中的主链运动稍慢或幅度较小,但两种构象中的快速内部运动相似且幅度较大。在高温(高于60℃)下,亚氨基质子与溶剂的交换主导了B型聚(dG-dC)·聚(dG-dC)的自旋晶格弛豫,但在Z型中,在高达85℃的温度下未观察到交换贡献(小于2 s⁻¹)。使亚氨基质子暴露于溶剂的构象波动在B型和Z型中显著不同。将此处获得的结果与先前报道的聚(dA-dT)·聚(dA-dT)的结果进行比较。

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