Kojima C, Ono A, Kainosho M, James T L
Department of Pharmaceutical Chemistry, University of California, San Francisco, California, 94143-0446, USA.
J Magn Reson. 1998 Dec;135(2):310-33. doi: 10.1006/jmre.1998.1584.
Dynamics in a DNA decamer duplex, d(CATTTGCATC). d(GATGCAAATG), were investigated via a detailed 13C NMR relaxation study. Every 2'-deoxyadenosine and 2'-deoxyguanidine was chemically enriched with 15% 13C and 98% 15N isotopes. Six nuclear relaxation parameters [R(13Cz), R(1Hz), R(2(1)Hz13Cz), R(13Cx), R(2(1)Hz13Cx) and steady-state 13C¿1H¿ NOE] were measured at 600 MHz and three were measured at 500 MHz (1H frequency) for the CH spin systems of sugar 1', 3', and 4' as well as base 8 and 2 positions. A dependence of relaxation parameter values on chemical position was clearly observed; however, no sequence-specific variation was readily evident within our experimental error of approximately 5-10%, except for 3' and 5' termini. It was demonstrated that the random 15% 13C enrichment effectively suppressed both scalar and dipolar contributions of the neighboring carbons and protons on the relaxation parameters. To analyze dynamics via all observed relaxation parameters, full spectral density mapping (1992, J. W. Peng and G. Wagner, J. Magn. Reson. 98, 308) and the "model-free" approach (1982, Lipari and Szabo, J. Am. Chem. Soc. 104, 4546) were applied complementarily. A linear correlation between three spectral density values, J(omegaC), J(omegaH - omegaC), and J(omegaH + omegaC) was observed in plots containing all measured values, but not for the other spectral density terms including J(0). These linear correlations reflect the effect of overall motion and similar internal motions for each CH vector in the decamer. The correlations yielded two correlation times, 3-4 ns and 10-200 ps. One value, 3-4 ns, corresponds to the value of 3.3 ns obtained for the overall isotropic tumbling correlation time determined from analysis of 13C T1/T2 ratios. The possibility of overall anisotropic tumbling was examined, but statistical analysis showed no advantage over the assumption of simple isotropic tumbling. Lack of correlations entailing J(0) implies that a relatively slow chemical exchange contributes to yielding of effective Jeff(0) values. Based on spectral density mapping and the T1/T2 ratio analysis, three basic assumptions were initially employed (and subsequently justified) for the model-free calculation: isotropic overall tumbling, one internal motion, and the presence of chemical exchange terms. Except for terminal residues, the order parameter S2 and the corresponding fast internal motion correlation time were determined to be about 0.8 +/- 0.1 and 20 +/- 20 ps, respectively, for the various CH vectors. Only a few differences were observed between or within sugars and bases. The internal motion is very fast (ps-ns time scale) and its amplitude restricted; e.g., assuming a simple wobble-in-a-cone model, the internal motion is restricted to an angular amplitude of +/-22. 5 degrees for each of the 1', 3', 4', 2, and 8 positions in the purine nucleotides in the entire duplex.
通过详细的(^{13}C)核磁共振弛豫研究,对DNA十聚体双链体d(CATTTGCATC).d(GATGCAAATG)的动力学进行了研究。每个2'-脱氧腺苷和2'-脱氧鸟苷都用15%的(^{13}C)和98%的(^{15}N)同位素进行了化学富集。在600 MHz下测量了六个核弛豫参数([R(^{13}Cz), R(^{1}Hz), R(2(1)Hz^{13}Cz), R(^{13}Cx), R(2(1)Hz^{13}Cx))和稳态(^{13}C-^{1}H) NOE],并在500 MHz((^{1}H)频率)下测量了糖的1'、3'和4'以及碱基8和2位置的CH自旋系统的三个参数。弛豫参数值对化学位置的依赖性清晰可见;然而,除了3'和5'末端外,在我们约5-10%的实验误差范围内,没有明显的序列特异性变化。结果表明,随机15%的(^{13}C)富集有效地抑制了相邻碳和质子对弛豫参数的标量和偶极贡献。为了通过所有观察到的弛豫参数分析动力学,互补地应用了全谱密度映射(1992年,J.W.彭和G.瓦格纳,《磁共振杂志》98,308)和“无模型”方法(1982年,利帕里和萨博,《美国化学会志》104,4546)。在包含所有测量值的图中观察到三个谱密度值(J(\omega C))、(J(\omega H - \omega C))和(J(\omega H + \omega C))之间存在线性相关性,但对于包括(J(0))在内的其他谱密度项则没有。这些线性相关性反映了十聚体中每个CH向量的整体运动和相似内部运动的影响。相关性产生了两个相关时间,3-4 ns和10-200 ps。一个值3-4 ns对应于通过分析(^{13}C) (T_1/T_2)比值确定的整体各向同性翻滚相关时间的3.3 ns值。研究了整体各向异性翻滚的可能性,但统计分析表明,与简单各向同性翻滚的假设相比没有优势。缺乏与(J(0))相关的相关性意味着相对缓慢的化学交换有助于产生有效的(J_{eff}(0))值。基于谱密度映射和(T_1/T_2)比值分析,最初为无模型计算采用了三个基本假设(随后得到了验证):各向同性整体翻滚、一种内部运动以及化学交换项的存在。除了末端残基外,对于各种CH向量,序参数(S^2)和相应的快速内部运动相关时间分别确定为约0.8±0.1和20±20 ps。在糖和碱基之间或内部仅观察到一些差异。内部运动非常快(皮秒-纳秒时间尺度)且其幅度受限;例如,假设一个简单的圆锥内摆动模型,对于整个双链体中嘌呤核苷酸的1'、3'、4'、2和8位置中的每一个,内部运动被限制在±22.5度的角幅度内。