Despite the key role of the linker histone H1 in chromatin structure and dynamics, its location and interactions with nucleosomal DNA have not been elucidated. In this work we have used a combination of electron cryomicroscopy, hydroxyl radical footprinting, and nanoscale modeling to analyze the structure of precisely positioned mono-, di-, and trinucleosomes containing physiologically assembled full-length histone H1 or truncated mutants of this protein.Single-base resolution •OH footprinting shows that the globular domain of histone H1 (GH1) interacts with the DNA minor groove located at the center of the nucleosome and contacts a 10-bp region of DNA localized symmetrically with respect to the nucleosomal dyad. In addition, GH1 interacts with and organizes about one helical turn of DNA in each linker region of the nucleosome. We also find that a seven amino acid residue region (121-127) in the COOH terminus of histone H1 was required for the formation of the stem structure of the linker DNA. A molecular model on the basis of these data and coarse-grain DNA mechanics provides novel insights on how the different domains of H1 interact with the nucleosome and predicts a specific H1-mediated stem structure within linker DNA.nucleosome structure | chromatin higher order structure T he nucleosome is the fundamental repeating unit of chromatin in the nucleus of eukaryotic cells. The composition and the basic organization of the nucleosome is well established, and the structure of the nucleosomal core particle (NCP) has been described with nearly atomic precision by X-ray diffraction (1). However, similar information for the structure of a complete nucleosome, i.e., the NCP with associated linker DNA segments and a linker histone, is still lacking. Electron microscopy and electron cryomicroscopy (ECM) imaging have provided a relatively low-resolution picture of the complete nucleosome, both native (2) and reconstituted (3). However, important features of the structure remain obscure.Linker histones are typically ∼200 aa in length with a rather short nonstructured N terminus, followed by a ∼70-80 aa structured ("globular") domain, and a ∼100 aa long apparently unstructured C terminal domain, highly enriched in lysines. The globular domain of the linker histone appears to be internally located in the 30-nm chromatin fiber (4, 5), but its exact position within the nucleosome remains a subject of debate (for review, see ref. 6). A second question not yet resolved concerns the interactions and location of the linker histone C terminus. These issues have their origin in difficulties related to the preparation of well-defined nucleosomal samples. Indeed, direct binding of linker histone to nucleosomes in vitro is inefficient and complicated by the formation of large aggregates because of the nonspecific association of linker histones with DNA (7, 8).The situation can be considerably improved by using chaperones for linker histone deposition in vitro, a mechanism that is likely used in vivo (9). It was recently shown that NAP...

Fluorescence in-situ hybridization (FISH) and chromosome conformation capture (3C) are two powerful techniques for investigating the three-dimensional organization of the genome in interphase nuclei. The use of these techniques provides complementary information on average spatial distances (FISH) and contact probabilities (3C) for specific genomic sites. To infer the structure of the chromatin fiber or to distinguish functional interactions from random colocalization, it is useful to compare experimental data to predictions from statistical fiber models. The current estimates of the fiber stiffness derived from FISH and 3C differ by a factor of 5. They are based on the wormlike chain model and a heuristic modification of the Shimada-Yamakawa theory of looping for unkinkable, unconstrained, zero-diameter filaments. Here, we provide an extended theoretical and computational framework to explain the currently available experimental data for various species on the basis of a unique, minimal model of decondensing chromosomes: a kinkable, topologically constraint, semiflexible polymer with the (FISH) Kuhn length of l(K) = 300 nm, 10 kinks per Mbp, and a contact distance of 45 nm. In particular: 1), we reconsider looping of finite-diameter filaments on the basis of an analytical approximation (novel, to our knowledge) of the wormlike chain radial density and show that unphysically large contact radii would be required to explain the 3C data based on the FISH estimate of the fiber stiffness; 2), we demonstrate that the observed interaction frequencies at short genomic lengths can be explained by the presence of a low concentration of curvature defects (kinks); and 3), we show that the most recent experimental 3C data for human chromosomes are in quantitative agreement with interaction frequencies extracted from our simulations of topologically confined model chromosomes.