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Two monoclinic crystal forms (P2(1),C2) of chicken erythrocyte nucleosomes have been under study in this laboratory. The x-ray structure of the P2(1) crystal form has been solved to 15 A resolution. The B-DNA superhelix has a relatively uniform curvature, with only several local distortions observed in the superhelix. The individual histone domains have been localized and specific contacts between each histone and the DNA can be observed. Histone contacts to the inner surface of the DNA superhelix occur predominantly at the minor groove sites. Most of the histone core is contained within the inner surface of the superhelical DNA, except for part of H2A which extends between the DNA gyres near the terminus of the DNA. No part of H2A blocks the DNA terminus or would prevent a smooth exit of the DNA into the linker region. A similar extension of a portion of histone H4 between the DNA gyres occurs close to the dyad axis. Both unique nucleosomes in the P2(1) asymmetric unit demonstrate good dyad symmetry and are similar to each other throughout the histone core and DNA regions.

Several investigators have recognized the importance of non-periodic DNA sequence information in determining the translational position of precisely positioned nucleosomes. The purpose of this study is to determine the extent of such information, in addition to the character of periodic information present. This is accomplished by examining the half-nucleosome DNA sequences of a considerable number of precisely positioned nucleosomes, and determining the probability of occurrence of each dinucleotide type as a function of position from the nucleosome center to the terminus (positions 0 to 72). By the nature of this procedure, no assumptions of periodicity are made. The results show the importance of several DNA sequence periodicities including 6-7, 10, and 21 base pairs, in addition to significant nonperiodic information. The results demonstrate that each dinucleotide type is unique in terms of its positional preference in precisely positioned nucleosomes (for example AA not equal to TT). The probabilities of occurrence for the dinucleotide types can be used to predict the translational positions of a number of observed nucleosomes.

The x-ray crystallographic structure of the nucleosome core particle has been determined using 8 A resolution diffraction data. The particle has a mean diameter of 106 A and a maximum thickness of 65 A in the superhelical axis direction. The longest chord through the histone core measures 85 A and is in a non-axial direction. The 1.87 turn superhelix consists of B-DNA with about 78 base pairs or 7.6 helical repeats per superhelical turn. The mean DNA helical repeat contains 10.2 +/- 0.05 base pairs and spans 35 A, slightly more than standard B-DNA. The superhelix varies several Angstroms in radius and pitch, and has three distinct domains of curvature (with radii of curvature of 60, 45 and 51 A). These regions are separated by localized sharper bends +/- 10 and +/- 40 base pairs from the center of the particle, resulting in an overall radius of curvature about 43 A. Compression of superhelical DNA grooves on the inner surface and expansion on the outer surface can be seen throughout the DNA electron density. This density has been fit with a double helical ribbon model providing groove width estimates of 12 +/- 1 A inside vs. 19 +/- 1 A outside for the major groove, and 8 +/- 1 A inside vs. 13 +/- 1 A outside for the minor groove. The histone core is primarily contained within the bounds defined by the superhelical DNA, contacting the DNA where the phosphate backbone faces in toward the core. Possible extensions of density between the gyres have been located, but these are below the significance level of the electron density map. In cross-section, a tripartite organization of the histone octamer is apparent, with the tetramer occupying the central region and the dimers at the extremes. Several extensions of histone density are present which form contacts between nucleosomes in the crystal, perhaps representing flexible or "tail" histone regions. The radius of gyration of the histone portion of the electron density is calculated to be 30.4 A (in reasonable agreement with solution scattering values), and the histone core volume in the map is 93% of its theoretical volume.