Unfolding individual nucleosomes by stretching single chromatin fibers with optical tweezers.

Single chromatin fibers were assembled directly in the flow cell of an optical tweezers setup. A single lambda phage DNA molecule, suspended between two polystyrene beads, was exposed to a Xenopus laevis egg extract, leading to chromatin assembly with concomitant apparent shortening of the DNA molecule. Assembly was force-dependent and could not take place at forces exceeding 10 pN. The assembled single chromatin fiber was subjected to stretching by controlled movement of one of the beads with the force generated in the molecule continuously monitored with the second bead trapped in the optical trap. The force displayed discrete, sudden drops upon fiber stretching, reflecting discrete opening events in fiber structure. These opening events were quantized at increments in fiber length of approximately 65 nm and are attributed to unwrapping of the DNA from around individual histone octamers. Repeated stretching and relaxing of the fiber in the absence of egg extract showed that the loss of histone octamers was irreversible. The forces measured for individual nucleosome disruptions are in the range of 20-40 pN, comparable to forces reported for RNA- and DNA-polymerases.     

ACF catalyses chromatosome movements in chromatin fibres

Nucleosome-remodelling factors containing the ATPase ISWI, such as ACF, render DNA in chromatin accessible by promoting the sliding of histone octamers. Although the ATP-dependent repositioning of mononucleosomes is readily observable in vitro, it is unclear to which extent nucleosomes can be moved in physiological chromatin, where neighbouring nucleosomes, linker histones and the folding of the nucleosomal array restrict mobility. We assembled arrays consisting of 12 nucleosomes or 12 chromatosomes (nucleosomes plus linker histone) from defined components and subjected them to remodelling by ACF or the ATPase CHD1. Both factors increased the access to DNA in nucleosome arrays. ACF, but not CHD1, catalysed profound movements of nucleosomes throughout the array, suggesting different remodelling mechanisms. Linker histones inhibited remodelling by CHD1. Surprisingly, ACF catalysed significant repositioning of entire chromatosomes in chromatin containing saturating levels of linker histone H1. H1 inhibited the ATP-dependent generation of DNA accessibility by only about 50%. This first demonstration of catalysed chromatosome movements suggests that the bulk of interphase euchromatin may be rendered dynamic by dedicated nucleosome-remodelling factors.     

DNA-loop formation on nucleosomes shown by in situ scanning force microscopy of supercoiled DNA

The flexibility of the chromatin structure, necessary for the processing of the genomic DNA, is controlled by a number of factors where flexibility and mobility of the nucleosomes is essential. Here, the influence of DNA supercoiling on the structure of single nucleosomes is investigated. Circular supercoiled plasmid DNA sub-saturated with histones was visualized by scanning force microscopy (SFM) in aqueous solution. SFM-imaging compared with topological analysis indicates instability of nucleosomes when the salt concentration is raised from 10 mM to 100 mM NaCl. Nucleosomes were observed after the deposition to the used scanning surface, i.e. mica coated with polylysine. On the images, the nucleosomes appear with a high probability in end-loops near the apices of the superhelices. In 100 mM NaCl but not in 10 mM NaCl, a significant number of complexes present the nucleosomes on superhelical crossings mainly located adjacent to an end-loop. The morphology of these structures and statistical analysis suggest that DNA loops were formed on the histone octamers, where the loop size distribution shows a pronounced peak at 50 nm. Recently, the formation and diffusion of loops on octamers has been discussed as a mechanism of translocations of nucleosomes along DNA. The presented data likely confirm the occurrence of loops, which may be stabilized by supercoiling. Analysis of the structure of regular nucleosomes not located on crossings indicates that reducing the salt concentration leads to more conformations, where DNA is partially unwrapped from the distal ends of the octamer.     

The RSC chromatin remodelling ATPase translocates DNA with high force and small step size

ATP-dependent chromatin remodelling complexes use the energy of ATP hydrolysis to reposition and reconfigure nucleosomes. Despite their diverse functions, all remodellers share highly conserved ATPase domains, many shown to translocate DNA. Understanding remodelling requires biophysical knowledge of the DNA translocation process: how the ATPase moves DNA and generates force, and how translocation and force generation are coupled on nucleosomes. Here, we characterize the real-time activity of a minimal RSC translocase 'motor' on bare DNA, using high-resolution optical tweezers and a 'tethered' translocase system. We observe on dsDNA a processivity of ～35 bp, a speed of ～25 bp/s, and a step size of 2.0 (±0.4, s.e.m.) bp. Surprisingly, the motor is capable of moving against high force, up to 30 pN, making it one of the most force-resistant motors known. We also provide evidence for DNA 'buckling' at initiation. These observations reveal the ATPase as a powerful DNA translocating motor capable of disrupting DNA-histone interactions by mechanical force.     

Histone H1 compacts DNA under force and during chromatin assembly

Histone H1 binds to linker DNA between nucleosomes, but the dynamics and biological ramifications of this interaction remain poorly understood. We performed single-molecule experiments using magnetic tweezers to determine the effects of H1 on naked DNA in buffer or during chromatin assembly in Xenopus egg extracts. In buffer, nanomolar concentrations of H1 induce bending and looping of naked DNA at stretching forces below 0.6 pN, effects that can be reversed with 2.7-pN force or in 200 mM monovalent salt concentrations. Consecutive tens-of-nanometer bending events suggest that H1 binds to naked DNA in buffer at high stoichiometries. In egg extracts, single DNA molecules assemble into nucleosomes and undergo rapid compaction. Histone H1 at endogenous physiological concentrations increases the DNA compaction rate during chromatin assembly under 2-pN force and decreases it during disassembly under 5-pN force. In egg cytoplasm, histone H1 protects sperm nuclei undergoing genome-wide decondensation and chromatin assembly from becoming abnormally stretched or fragmented due to astral microtubule pulling forces. These results reveal functional ramifications of H1 binding to DNA at the single-molecule level and suggest an important physiological role for H1 in compacting DNA under force and during chromatin assembly.     

Atomic force microscopy sees nucleosome positioning and histone H1-induced compaction in reconstituted chromatin.

We addressed the question of how nuclear histones and DNA interact and form a nucleosome structure by applying atomic force microscopy to an in vitro reconstituted chromatin system. The molecular images obtained by atomic force microscopy demonstrated that oligonucleosomes reconstituted with purified core histones and DNA yielded a 'beads on a string' structure with each nucleosome trapping 158 +/- 27 bp DNA. When dinucleosomes were assembled on a DNA fragment containing two tandem repeats of the positioning sequence of the Xenopus 5S RNA gene, two nucleosomes were located around each positioning sequence. The spacing of the nucleosomes fluctuated in the absence of salt and the nucleosomes were stabilized around the range of the positioning signals in the presence of 50 mM NaCl. An addition of histone H1 to the system resulted in a tight compaction of the dinucleosomal structure.     

Quantitative analysis of single-molecule force spectroscopy on folded chromatin fibers

Single-molecule techniques allow for picoNewton manipulation and nanometer accuracy measurements of single chromatin fibers. However, the complexity of the data, the heterogeneity of the composition of individual fibers and the relatively large fluctuations in extension of the fibers complicate a structural interpretation of such force-extension curves. Here we introduce a statistical mechanics model that quantitatively describes the extension of individual fibers in response to force on a per nucleosome basis. Four nucleosome conformations can be distinguished when pulling a chromatin fiber apart. A novel, transient conformation is introduced that coexists with single wrapped nucleosomes between 3 and 7 pN. Comparison of force-extension curves between single nucleosomes and chromatin fibers shows that embedding nucleosomes in a fiber stabilizes the nucleosome by 10 k_BT. Chromatin fibers with 20- and 50-bp linker DNA follow a different unfolding pathway. These results have implications for accessibility of DNA in fully folded and partially unwrapped chromatin fibers and are vital for understanding force unfolding experiments on nucleosome arrays.     

Chromatin Remodelers Act Globally, Sequence Positions Nucleosomes Locally

The precise placement of nucleosomes has large regulatory effects on gene expression. Recent work suggests that nucleosome placement is regulated in part by the affinity of the underlying DNA sequence for the histone octamer. Nucleosome locations are also regulated by several different ATP-dependent chromatin remodeling enzymes. This raises the question of whether DNA sequence influences the activity of chromatin remodeling enzymes. DNA sequence could most simply regulate nucleosome remodeling through its effect on nucleosome stability. In such a model, unstable nucleosomes would be remodeled faster than stable nucleosomes. It is also possible that certain DNA elements could regulate remodeling by inhibiting the interaction of nucleosomes with the remodeling enzyme. A third possibility is that DNA sequence could regulate the outcome of remodeling by influencing how reaction intermediates collapse into a particular set of stable nucleosomal positions. Here we dissect the contribution from these potential mechanisms to the activities of yeast RSC and human ACF, which are representative members of two major classes of remodeling complexes. We find that varying the histone-DNA affinity over 3 orders of magnitude has negligible effects on the rates of nucleosome remodeling and ATP hydrolysis by these two enzymes. This suggests that the rate-limiting step for nucleosome remodeling may not involve the disruption of histone-DNA contacts. We further find that a specific curved DNA element previously hypothesized to inhibit ACF activity does not inhibit substrate binding or remodeling by ACF. The element, however, does influence the distribution of nucleosome positions generated by ACF. Our data support a model in which remodeling enzymes move nucleosomes to new locations by a general sequence-independent mechanism. However, consequent to the rate-limiting remodeling step, the local DNA sequence promotes a collapse of remodeling intermediates into highly resolved positions that are dictated by thermodynamic differences between adjacent positions.     

Salt-dependent compaction of di- and trinucleosomes studied by small-angle neutron scattering

Using small-angle neutron scattering (SANS), we have measured the salt-dependent static structure factor of di- and trinucleosomes from chicken erythrocytes and from COS-7 cells. We also determined the sedimentation coefficients of these dinucleosomes and dinucleosomes reconstituted on a 416-bp DNA containing two nucleosome positioning sequences of the 5S rDNA of Lytechinus variegatus at low and high salt concentrations. The internucleosomal distance d was calculated by simulation as well as Fourier back-transformation of the SANS curves and by hydrodynamic simulation of sedimentation coefficients. Nucleosome dimers from chicken erythrocyte chromatin show a decrease in d from approximately 220 A at 5 mM NaCl to 150 A at 100 mM NaCl. For dinucleosomes from COS-7 chromatin, d decreases from 180 A at 5 mM to 140 A at 100 mM NaCl concentration. Our measurements on trinucleosomes are compatible with a compaction through two different mechanisms, depending on the salt concentration. Between 0 and 20 mM NaCl, the internucleosomal distance between adjacent nucleosomes remains constant, whereas the angle of the DNA strands entering and leaving the central nucleosome decreases. Above 20 mM NaCl, the adjacent nucleosomes approach each other, similar to the compaction of dinucleosomes. The internucleosomal distance of 140-150 A at 100 mM NaCl is in agreement with distances measured by scanning force microscopy and electron microscopy on long chromatin filaments.     

Multistep chromatin assembly on supercoiled plasmid DNA by nucleosome assembly protein-1 and ATP-utilizing chromatin assembly and remodeling factor

We examine in vitro nucleosome assembly by nucleosome assembly protein-1 (NAP-1) and ATP-utilizing chromatin assembly and remodeling factor (ACF). In contrast to previous studies that used relaxed, circular plasmids as templates, we have found that negatively supercoiled templates reveal the distinct roles of NAP-1 and ACF in histone deposition and the formation of an ordered nucleosomal array. NAP-1 can efficiently deposit histones onto supercoiled plasmids. Furthermore, NAP-1 exhibits a greater affinity for histones H2A-H2B than does naked DNA, but in the presence of H3-H4, H2A-H2B are transferred from NAP-1 to the plasmid templates. These observations underscore the importance of a high affinity between H2A-H2B and NAP-1 for ordered transfer of core histones onto DNA. In addition, recombinant ACF composed of imitation switch and Acf1 can extend closely packed nucleosomes, which suggests that recombinant ACF can mobilize nucleosomes. In the assembly reaction with a supercoiled template, ACF need not be added simultaneously with NAP-1. Regularly spaced nucleosomes are generated even when recombinant ACF is added after core histones are transferred completely onto the DNA. Atomic force microscopy, however, suggests that NAP-1 alone fails to accomplish the formation of fine nucleosomal core particles, which are only formed in the presence of ACF. These results suggest a model for the ordered deposition of histones and the arrangement of nucleosomes during chromatin assembly in vivo.     

Involvement of histone H1 in the organization of the nucleosome and of the salt-dependent superstructures of chromatin

We describe the results of a systematic study, using electron microscopy, of the effects of ionic strength on the morphology of chromatin and of H1-depleted chromatin. With increasing ionic strength, chromatin folds up progressively from a filament of nucleosomes at approximately 1 mM monovalent salt through some intermediate higher- order helical structures (Thoma, F., and T. Koller, 1977, Cell 12:101- 107) with a fairly constant pitch but increasing numbers of nucleosomes per turn, until finally at 60 mM (or else in approximately 0.3 mM Mg++) a thick fiber of 250 A diameter is formed, corresponding to a structurally well-organized but not perfectly regular superhelix or solenoid of pitch approximately 110 A as described by Finch and Klug (1976, Proc. Natl. Acad. Sci. U.S.A. 73:1897-1901). The numbers of nucleosomes per turn of the helical structures agree well with those which can be calculated from the light-scattering data of Campbell et al. (1978, Nucleic Acids Res. 5:1571-1580). H1-depleted chromatin also condenses with increasing ionic strength but not so densely as chromatin and not into a definite structure with a well-defined fiber direction. At very low ionic strengths, nucleosomes are present in chromatin but not in H1-depleted chromatin which has the form of an unravelled filament. At somewhat higher ionic strengths (greater than 5 mM triethanolamine chloride), nucleosomes are visible in both types of specimen but the fine details are different. In chromatin containing H1, the DNA enters and leaves the nucleosome on the same side but in chromatin depleted of H1 the entrance and exit points are much more random and more or less on opposite sides of the nucleosome. We conclude that H1 stabilizes the nucleosome and is located in the region of the exit and entry points of the DNA. This result is correlated with biochemical and x-ray crystallographic results on the internal structure of the nucleosome core to give a picture of a nucleosome in which H1 is bound to the unique region on a complete two-turn, 166 base pair particle (Fig. 15). In the formation of higher-order structures, these regions on neighboring nucleosomes come closer together so that an H1 polymer may be formed in the center of the superhelical structures.     

Linker histone H1 per se can induce three-dimensional folding of chromatin fiber

Higher-order architectures of chromosomes play important roles in the regulation of genome functions. To understand the molecular mechanism of genome packing, an in vitro chromatin reconstitution method and a single-molecule imaging technique (atomic force microscopy) were combined. In 50 mM NaCl, well-stretched beads-on-a-string chromatin fiber was observed. However, in 100 mM NaCl, salt-induced interaction between nucleosomes caused partial aggregation. Addition of histone H1 promoted a further folding of the fiber into thicker fibers 20-30 nm in width. Micrococcal nuclease digestion of these thicker fibers produced an approximately 170 bp fragment of nucleosomal DNA, which was approximately 20 bp longer than in the absence of histone H1 ( approximately 150 bp), indicating that H1 is correctly placed at the linker region. The width of the fiber depended on the ionic strength. Widths of 20 nm in 50 mM NaCl became 30 nm as the ionic strength was changed to 100 mM. On the basis of these results, a flexible model of chromatin fiber formation was proposed, where the mode of the fiber compaction changes depending both on salt environment and linker histone H1. The biological significance of this property of the chromatin architecture will be apparent in the closed segments ( approximately 100 kb) between SAR/MAR regions.