Marion C, Bezot P, Hesse-Bezot C, Roux B, Bernengo J C
Eur J Biochem. 1981 Nov;120(1):169-76. doi: 10.1111/j.1432-1033.1981.tb05685.x.
Quasielastic laser light scattering measurements have been made on chromatin oligomers to obtain information on the transition in their electrooptical properties, previously observed for the hexameric structures [Marion, C. and Roux, B. (1978) Nucleic Acids Res. 5, 4431-4449]. Translational diffusion coefficients were determined for mononucleosomes to octanucleosomes containing histone H1 over a range of ionic strength. At high ionic strength, oligomers show a linear dependence of the logarithm of diffusion coefficient upon the logarithm of number of nucleosomes. At low ionic strength a change occurs between hexamer and heptamer. Our results agree well with the recent sedimentation data of Osipova et al. [Eur. J. Biochem. (1980) 113, 183-188] and of Butler and Thomas [J. Mol. Biol. (1980) 140, 505-529] showing a change in stability with hexamer. Various models for the arrangements of nucleosomes in the superstructure of chromatin are discussed. All calculations clearly indicate a conformational change with the hexanucleosome and the results suggest that, at low ionic strength, the chromatin adopts a loosely helical structure of 28-nm diameter and 22-nm pitch. These results are also consistent with a discontinuity every sixth nucleosome, corresponding to a turn of the helix. This discontinuity may explain the recent electric dichroism data of Lee et al. [Biochemistry (1981) 20, 1438-1445]. The hexanucleosome structure which we have previously suggested, with the faces of nucleosomes arranged radially to the helical axis has been recently confirmed by Mc Ghee et al. [Cell (1980) 22, 87-96]. With an increase of ionic strength, the helix becomes more regular and compact with a slightly reduced outer diameter and a decreased pitch, the dimensions resembling those proposed for solenoid models.
已对染色质寡聚体进行了准弹性激光光散射测量,以获取有关其电光性质转变的信息,这种转变先前在六聚体结构中已观察到[马里昂,C. 和鲁克斯,B.(1978年)《核酸研究》5,4431 - 4449]。在一系列离子强度范围内,测定了包含组蛋白H1的单核小体至八聚核小体的平动扩散系数。在高离子强度下,寡聚体的扩散系数对数与核小体数量对数呈线性关系。在低离子强度下,六聚体和七聚体之间会发生变化。我们的结果与奥西波娃等人[《欧洲生物化学杂志》(1980年)113,183 - 188]以及巴特勒和托马斯[《分子生物学杂志》(1980年)140,505 - 529]最近的沉降数据吻合良好,这些数据表明六聚体的稳定性发生了变化。讨论了染色质超结构中核小体排列的各种模型。所有计算都清楚地表明六聚核小体存在构象变化,结果表明,在低离子强度下,染色质采用直径28纳米、螺距22纳米的松散螺旋结构。这些结果也与每隔六个核小体出现一次的不连续性一致,这对应于螺旋的一圈。这种不连续性可能解释了李等人[《生物化学》(1981年)20,1438 - 1445]最近的电二色性数据。我们先前提出的六聚核小体结构,即核小体的面沿螺旋轴呈放射状排列,最近已被麦吉等人[《细胞》(1980年)22,87 - 96]证实。随着离子强度的增加,螺旋变得更加规则和紧凑,外径略有减小,螺距减小,其尺寸类似于螺线管模型所提出的尺寸。