Levy G C, Marchetti P S, Ejchart A, Levy L F, Kumar A, Hilliard P R, Rill R L
N.I.H. Biotechnology Research Resource for Multi-Nuclei NMR and Data Processing, Department of Chemistry, Syracuse University, NY 13210.
J Biomol Struct Dyn. 1983 Dec;1(3):795-808. doi: 10.1080/07391102.1983.10507482.
Phosphorus-31 and especially Carbon-13 NMR measurements have recently become primary input to the understanding of DNA solution dynamics. While the 31P measurements are inherently easier, the quality of 31P dynamics information is suspect and therefore 13C measurements are preferred. In fact, it is necessary to obtain several kinds of 13C data (T1s, NOE's, linewidths, integrated peak intensities) over a wide range of magnetic fields (13C NMR frequencies) in order to identify major features of DNA internal motions. Further information comes from variation of temperature and DNA fragment length and/or concentration. Most of our 13C measurements have been performed at 37.7-90.6 MHz on fully double stranded monomer size (147 base pair) DNA at concentrations in phosphate buffer of approximately less than 10 to approximately greater than 200 mg ml-1; temperatures studied range from 6 to 55 degrees C. Other measurements have been performed on monomer-size single-stranded DNA at 85 and 92 degrees. The large data set we have acquired appears to answer some important questions about the nature and extent of DNA overall and internal motional dynamics. However, the picture remains incomplete and a number of questions arise from these results: 1. Overall motion of the double stranded DNA fragments follows expected hydrodynamic behavior; 2. Restricted but rapid internal motion along the DNA structure is well represented by a spaghetti-like wobbling-in-a-cone model; 3. DNA-DNA Interactions and solvent ordering, present at relatively low DNA concentrations, partially quench the internal motion, consistent with hinge-model structural changes (and the spaghetti model above) but not as compatible with in-plane torsional motion models; 4. The deoxyribose C-2' sites undergo additional motion which is partially uncoupled from the internal wobbling motions: 5. At high DNA concentrations, a phase transition occurs, resulting in ordered structures which drastically affect DNA internal dynamics; 6. DNA interacting with ethidium does not greatly change its conformational mobility; 7. DNA interacting with Hg2+ ions shows less than anticipated change in internal DNA dynamics. The remaining challenge is to interpret our current results in terms of specific conformational processes and to understand why the conformational mobility of double stranded DNA is relatively unhindered by major structural perturbants such as intercalating ethidium and mercury ion.
磷 - 31,尤其是碳 - 13核磁共振测量最近已成为理解DNA溶液动力学的主要输入信息。虽然31P测量本质上更容易,但31P动力学信息的质量令人怀疑,因此13C测量更受青睐。事实上,有必要在很宽的磁场范围(13C NMR频率)内获取几种13C数据(T1值、核Overhauser效应、线宽、积分峰强度),以便识别DNA内部运动的主要特征。进一步的信息来自温度、DNA片段长度和/或浓度的变化。我们大多数的13C测量是在37.7 - 90.6兆赫兹下,对完全双链的单体大小(147个碱基对)的DNA进行的,其在磷酸盐缓冲液中的浓度约小于10毫克/毫升至约大于200毫克/毫升;研究的温度范围是6至55摄氏度。其他测量是在85和92摄氏度下对单体大小的单链DNA进行的。我们获取的大量数据集似乎回答了一些关于DNA整体和内部运动动力学的性质和程度的重要问题。然而,情况仍然不完整,从这些结果中出现了一些问题:1. 双链DNA片段的整体运动遵循预期的流体动力学行为;2. 沿着DNA结构受限但快速的内部运动可以很好地用类似意大利面条在圆锥中摆动的模型来表示;3. 在相对低的DNA浓度下存在的DNA - DNA相互作用和溶剂有序化,部分抑制了内部运动,这与铰链模型的结构变化(以及上述的意大利面条模型)一致,但与平面内扭转运动模型不太兼容;4. 脱氧核糖C - 2'位点经历额外的运动,该运动部分与内部摆动运动解耦;5. 在高DNA浓度下,会发生相变,导致形成有序结构,这极大地影响了DNA内部动力学;6. 与溴化乙锭相互作用的DNA其构象流动性变化不大;7. 与Hg2 +离子相互作用的DNA在内部DNA动力学方面的变化小于预期。剩下的挑战是根据特定的构象过程来解释我们目前的结果,并理解为什么双链DNA的构象流动性相对不受诸如嵌入溴化乙锭和汞离子等主要结构扰动的阻碍。