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Despite more than 20 years of research, the structure of the chromatin fiber and its molecular determinants remain enigmatic. Recent developments in high-resolution microscopic techniques, as well as the application of mathematical modeling to chromatin fiber structure, have allowed the acquisition of some new insights into the structure and its determinants. Here we present some of the newest data on the structure of the chromatin fiber in both its extended and compacted states, and bring together this new knowledge with older data in an attempt to provide a unified view of how chromatin components interact with each other to form its various conformations. The structural transitions that are believed to take place during transcriptional activation and its cessation are also discussed. It becomes obvious that despite some progress in our understanding of the fiber structure and its dynamics, huge gaps continue to exist. Bridging these gaps will require further improvements in already available techniques and the introduction of completely new approaches.

In chromatin, the physiological amount of H1 is one molecule per nucleosome or, roughly, one molecule per 200 bp of DNA. We observed that at such a stoichiometry, H1 selectively binds to supercoiled DNA with magnitude of sigma > or = 0.012 (both negative and positive), leaving relaxed, linear, or nicked DNA molecules unbound. When negative and positive DNA topoisomers of varying superhelicity are simultaneously present in the binding mixture, H1 selectively binds to the molecules with highest superhelicity; less supercoiled forms are gradually involved in binding upon increasing the amount of input protein. We explain this topological preference of H1 as the consequence of an increased probability for more than one H1-DNA contact provided by the supercoiling. The existence of simultaneous contacts of H1 with both intertwined DNA strands in the supercoiled DNA molecules is also inferred by topoisomerase relaxation of H1-DNA complexes that had been prefixed with glutaraldehyde.

We have used magnetic tweezers to study nucleosome assembly on topologically constrained DNA molecules. Assembly was achieved using chicken erythrocyte core histones and histone chaperone protein Nap1 under constant low force. We have observed only partial assembly when the DNA was topologically constrained and much more complete assembly on unconstrained (nicked) DNA tethers. To verify our hypothesis that the lack of full nucleosome assembly on topologically constrained tethers was due to compensatory accumulation of positive supercoiling in the rest of the template, we carried out experiments in which we mechanically relieved the positive supercoiling by rotating the external magnetic field at certain time points of the assembly process. Indeed, such rotation did lead to the same nucleosome saturation level as in the case of nicked tethers. We conclude that levels of positive supercoiling in the range of 0.025–0.051 (most probably in the form of twist) stall the nucleosome assembly process.

Transcription initiation and elongation in the eukaryotic nucleus occur in the context of chromatin. DNA wrapped around the histone core in the nucleosome constitutes a major obstacle to transcription. For transcription to occur, nucleosomes must be removed from the downstream DNA template. Numerous biochemical data indicate that this nucleosome disruption is a temporary event, with nucleosomes quickly reforming in the already transcribed portion of the template. We use a combination of single-molecule approaches (Magnetic Tweezers) and biochemical methods to investigate the mechanics of transcription elongation through nucleosomes. Specifically, we have performed real-time transcription experiments with chromatin templates (208-18 DNA based) and T7 RNA Polymerase. The disassembly of 18 nucleosomes is expected to increase tether length by ∼700 nm (each nucleosome is replaced by naked DNA of ∼146 bp). We observe changes in tether length, the size of which corresponds to diassembly of single nucleosomes. We can say so far that transcription through the nucleosomal array results in disassembly of the nucleosomes. Some additional lengthening occurs as a result of changes in the geometry of the fiber (mutual disposition of nucleosomes, DNA entry-exit angles, etc.)

Little is known about the mechanisms that organize linear arrays of nucleosomes into the three-dimensional structures of extended and condensed chromatin fibers. We have earlier defined, from scanning force microscopy (SFM) and mathematical modeling, a set of simple structural determinants of extended fiber morphology, the critical parameters being the entry-exit angle between consecutive linkers and linker length. Here we study the contributions of the structural domains of the linker histones (LHs) and of the N-terminus of histone H3 to extended fiber morphology by SFM imaging of progressively trypsinized chromatin fibers. We find that cleavage of LH tails is associated with a lengthening of the internucleosomal center-to-center distance, and that the somewhat later cleavage of the N-terminus of histone H3 is associated with a flattening of the fiber. The persistence of the “zigzag” fiber morphology, even at the latest stages of trypsin digestion, can be attributed to the retention of the globular domain of LH in the fiber.