Structure Of Nucleosome Core Particle Research Articles

Local Alteration of Ionic Strength in a Nucleosome Core Particle and Its Effect on N7-Methyl-2'-deoxyguanosine Depurination.

Positively charged N-terminal histone tails play important roles in maintaining the nucleosome (and chromatin) structure and function. Charge alteration, including those imposed by post-translational modifications, impacts chromatin dynamics, protein binding, and the fate of DNA damage. There is evidence that N-terminal histone tails affect the local ionic environment within a nucleosome core particle (NCP), but this phenomenon is not well understood. Determining the modulation of the local ionic environment within an NCP by histone tails could help uncover the underlying mechanisms of their functions and effects. Utilizing bottom-up syntheses of NCPs containing wild-type or mutated histones and a fluorescent probe that is sensitive to the local ionic environment, we show that interaction with positively charged N-terminal tails increases the local ionic strength near nucleosomal DNA. The effect is diminished by replacing positively charged residues with neutral ones or deleting a tail in its entirety. Replacing the fluorescent probe with the major DNA methylation product, N7-methyl-2'-deoxyguanosine (MdG), revealed changes in the depurination rate constant varying inversely with local ionic strength. These data indicate that the MdG hydrolysis rates depend on and also inform on local ionic strength in an NCP. Overall, histone tail charge contributes to the complexity of the NCP structure and function by modulating the local ionic strength.

Structural basis of nucleosome dynamics modulation by histone variants H2A.B andH2A.Z.2.2.

Nucleosomes are dynamic entities with wide-ranging compositional variations. Human histone variants H2A.B and H2A.Z.2.2 play critical roles in multiple biological processes by forming unstable nucleosomes and open chromatin structures, but how H2A.B and H2A.Z.2.2 confer these dynamic features to nucleosomes remains unclear. Here, we report cryo-EM structures of nucleosome core particles containing human H2A.B (H2A.B-NCP) at atomic resolution, identifying large-scale structural rearrangements in the histone octamer in H2A.B-NCP. H2A.B-NCP compacts approximately 103bp of DNA wrapping around the core histones in approximately 1.2 left-handed superhelical turns, in sharp contrast to canonical nucleosome encompassing approximately 1.7 turns of DNA. Micrococcal nuclease digestion assay reveals that nineteen H2A.B-specific residues, including a ROF ("regulating-octamer-folding") sequence of six consecutive residues, are responsible for loosening of H2A.B-NCPs. Unlike H2A.B-NCP, the H2A.Z.2.2-containing nucleosome (Z.2.2-NCP) adopts a less-extended structure and compacts around 125bp of DNA. Further investigation uncovers a crucial role for the H2A.Z.2.2-specific ROF in both H2A.Z.2.2-NCP opening and SWR1-dependent histone replacement. Taken together, these first high-resolution structure of unstable nucleosomes induced by histone H2A variants elucidate specific functions of H2A.B and H2A.Z.2.2 in enhancing chromatin dynamics.

Structure determination of the nucleosome core particle by selenium SAD phasing.

The eukaryotic genome is compacted inside the nucleus of the cell in the form called chromatin. The fundamental unit of chromatin is the nucleosome, which contains four types of histones (H3, H4, H2A and H2B) and approximately 150 base pairs of DNA wrapped around the histone complex. The structure of the nucleosome is highly conserved across several eukaryotic species, and molecular replacement has been the primary phasing method used to solve nucleosome structures by X-ray crystallography. However, there is currently no simple, widely applicable experimental phasing method for the nucleosome. In the present study, it is demonstrated that selenomethionine-incorporated histones H3, H2A and H2B can be reconstituted into nucleosomes and crystallized for structural determination. Unexpectedly, it was found that the nucleosome can be phased with a relatively small number of Se atoms. The structures of nucleosome core particles containing 12 and 16 Se atoms were solved by SAD phasing at 2.5 and 2.4 Å resolution, respectively. The present study demonstrates a simple method for determining nucleosome structures by experimental phasing, which may be particularly useful for noncanonical structures that cannot be solved by molecular replacement.

Structural Diversity of Nucleosomes Characterized by Native Mass Spectrometry.

Histone tails, which protrude from nucleosome core particles (NCPs), play crucial roles in the regulation of DNA transcription, replication, and repair. In this study, structural diversity of nucleosomes was investigated in detail by analyzing the observed charge states of nucleosomes reconstituted with various lengths of DNA using positive-mode electrospray ionization mass spectrometry (ESI-MS) and molecular dynamics (MD) simulation. Here, we show that canonical NCPs, having 147 bp DNA closely wrapped around a histone octamer, can be classified into three groups by charge state, with the least-charged group being more populated than the highly charged and intermediate groups. Ions with low charge showed small collision cross sections (CCSs), suggesting that the histone tails are generally compact in the gas phase, whereas the minor populations with higher charges appeared to have more loosened structure. Overlapping dinucleosomes, which contain 14 histone proteins closely packed with 250 bp DNA, showed similar characteristics. In contrast, mononucleosomes reconstituted with a histone octamer and longer DNA (≥250 bp), which have DNA regions uninvolved in the core-structure formation, showed only low-charge ions. This was also true for dinucleosomes with free DNA regions. These results suggest that free DNA regions affect the nucleosome structures. To investigate the possible structures of NCP observed in ESI-MS, computational structural calculations in solution and in vacuo were performed. They suggested that conformers with large CCS values have slightly loosened structure with extended tail regions, which might relate to the biological function of histone tails.

Site-Specific Disulfide Crosslinked Nucleosomes with Enhanced Stability

We engineered nucleosome core particles (NCPs) with two site-specific cysteine crosslinks that increase the stability of the particle. The first disulfide was introduced between the two copies of H2A via an H2A-N38C point mutation, effectively crosslinking the two H2A/H2B heterodimers together to stabilize the histone octamer against H2A/H2B dimer dissociation. The second crosslink was engineered between an R40C point mutation on the N-terminal tail of H3 and the NCP DNA ends by the introduction of a convertible nucleotide. This crosslink maintains the nucleosome DNA in a fixed translational setting relative to the histone octamer and prevents dilution-driven dissociation. The X-ray crystal structures of NCPs containing the disulfides in isolation and in combination were determined. Both disulfides stabilize the structure of the NCP without disturbing the overall structure. Nucleosomes containing these modifications will be advantageous for biochemical and structural studies as a consequence of their greater resistance to dissociation during high dilution in purification, elevated salt for crystallization and vitrification for cryogenic electron microscopy.

Development of a “Realistic” Model of the Dynamic Chromatin Fiber using an Integrated Computational Approach

DNA in eukaryotic cells is highly compacted into a hierarchical chromatin structure to fit inside the nucleus. Linker histones play an important role in this packing. Their interaction with the nucleosomes and intervening DNA linkers, in combination with linker length, are believed to affect chromatin folding and long-range interactions. The details of chromatin structure at this level of compaction are still an open question but have profound implications on biological processes, such as gene expression. Two major challenges are that linker histones contain a long intrinsically disordered C-terminal domain (CTD) and determination of high-resolution structures of chromatin has not been possible due to the large size of the system and its dynamic nature.We are taking advantage of the recently published 11-A resolution electron microscopy maps of two chromatin fibers (Song et al., 2014), to construct a complete low-resolution model of chromatin. High-resolution crystal structures of nucleosome core particles are fitted to the electron density maps and the intervening segments of linker DNA are modeled based on a sampling protocol that utilizes new DNA optimization methods. Situs is used to score all models against the density maps. Linker histones are modeled on the densities extracted after accounting for the nucleosomes and linker DNA. The modeled paths of the DNA linkers and the sites of the nucleosomes provide spatial constraints for positioning the globular core and modeling the folding of the disordered CTD of the linker histone. The pathways of the CTD are selected from ensembles of conformations obtained using ab initio structure prediction tools like Rosetta. We are using the model in coarse-grained Monte Carlo simulations of long-range interactions along arrays of precisely positioned nucleosomes in the presence of linker histones.

Nucleosome structure and function.

When fully extended, one copy of the three billion base pair human genome reaches a length of over two meters. Yet, it must be packaged into the nucleus of a cell with an average diameter of less than 10 μm. Within this context, specific segments of the genome must be transcriptionally active or repressed in a coordinated fashion to allow a cell to react to its ever-changing environment. This is akin to arranging 30 miles of thread inside a basketball such that at moment’s notice key segments can be accessed. To establish such compaction while maintaining coordinated accessibility, organisms ranging from yeast to man organize their genomes in a polymeric complex called chromatin. The fundamental unit of the chromatin polymer is the nucleosome, which repeats every 160 to 240 bp across the genome.1 Each nucleosome contains a nucleosome core, composed of an octameric complex of the core histone proteins, which forms a spool to wrap 145 to 147 bp of DNA. The nucleosome core is connected to the adjacent nucleosome core through a segment of linker DNA, which often associates with the linker histone protein (H1 or H5). The nucleosome core with ∼165 bp of DNA together with the linker histone is called the chromatosome.2 The chromatosome and the additional linker DNA constitutes a nucleosome.2 Despite these technical definitions, the nucleosome core particle is often colloquially referred to as the nucleosome. The nucleosome serves three primary functions. First, it brings about the first level of genomic compaction, organizing ∼200 bp of DNA. Second, the nucleosome acts as a signaling hub for chromatin-templated processes by providing a scaffold for the binding of chromatin enzymes and displaying a combinatorial array of post-translational modifications (PTMs). This array of PTMs further regulates the recruitment of chromatin enzymes3 and tunes both nucleosome stability4 and the higher-order compaction of chromatin.5−7 Third, the nucleosome can self-assemble into higher-order chromatin structures, allowing for further compaction of the genome. The first level of higher-order compaction is the 30 nm chromatin fiber for which several models have been created based on experimental data using cryogenic-electron microscopy (cryo-EM) and X-ray crystallography.8 This review focuses on recent advances in our understanding of the structure and function of the nucleosome and is divided into four parts. First, we present a primer covering the fundamentals of the nucleosome core particle structure determined at atomic scale by X-ray crystallography in 1997.9 Next we discuss recent insights into the role of DNA sequence in the structure of nucleosomal DNA based on structure–function studies of nucleosome core particles containing derivatives of the Widom 601 nucleosome positioning sequence.10 We then introduce patterns of nucleosome recognition by chromatin factors using recent crystal structures and NMR and cryo-EM models of peptide and protein macromolecular chromatin factors bound to the nucleosome core particle. Finally, we will compare a recent cryo-EM model for the 30 nm chromatin fiber11 to two previous models based on crystallographic and cryo-EM data.12,13

HMGN1 Protein Regulates Poly(ADP-ribose) Polymerase-1 (PARP-1) Self-PARylation in Mouse Fibroblasts

In mammalian cells, the nucleosome-binding protein HMGN1 (high mobility group N1) affects the structure and function of chromatin and plays a role in repair of damaged DNA. HMGN1 affects the interaction of DNA repair factors with chromatin and their access to damaged DNA; however, not all of the repair factors affected have been identified. Here, we report that HMGN1 affects the self-poly(ADP-ribosyl)ation (i.e., PARylation) of poly(ADP-ribose) polymerase-1 (PARP-1), a multifunctional and abundant nuclear enzyme known to recognize DNA lesions and promote chromatin remodeling, DNA repair, and other nucleic acid transactions. The catalytic activity of PARP-1 is activated by DNA with a strand break, and this results in self-PARylation and PARylation of other chromatin proteins. Using cells obtained from Hmgn1(-/-) and Hmgn1(+/+) littermate mice, we find that in untreated cells, loss of HMGN1 protein reduces PARP-1 self-PARylation. A similar result was obtained after MMS treatment of these cells. In imaging experiments after low energy laser-induced DNA damage, less PARylation at lesion sites was observed in Hmgn1(-/-) than in Hmgn1(+/+) cells. The HMGN1 regulation of PARP-1 activity could be mediated by direct protein-protein interaction as HMGN1 and PARP-1 were found to interact in binding assays. Purified HMGN1 was able to stimulate self-PARylation of purified PARP-1, and in experiments with cell extracts, self-PARylation was greater in Hmgn1(+/+) than in Hmgn1(-/-) extract. The results suggest a regulatory role for HMGN1 in PARP-1 activation.

A Bulky DNA Lesion Derived from a Highly Potent Polycyclic Aromatic Tumorigen Stabilizes Nucleosome Core Particle Structure

The impact of a bulky DNA lesion on the structure and dynamics of a nucleosome core particle (NCP) containing a lesion derived from the unusually potent tumorigen dibenzo[a,l]pyrene that resists nucleotide excision repair (NER) in free DNA was investigated using 65 ns molecular dynamics simulations. Our results reveal that, relative to unmodified NCP, the lesion stabilizes the nucleosome via stacking interactions, improved Watson-Crick base pairing, hydrogen bonding between DNA and histones, and damped dynamics. These findings suggest that such lesions should be as resistant to NER in the nucleosome environment as they are in free DNA.

Reconstitution of Yeast Silent Chromatin: Multiple Contact Sites and O-AADPR Binding Load SIR Complexes onto Nucleosomes In Vitro

At yeast telomeres and silent mating-type loci, chromatin assumes a higher-order structure that represses transcription by means of the histone deacetylase Sir2 and structural proteins Sir3 and Sir4. Here, we present a fully reconstituted system to analyze SIR holocomplex binding to nucleosomal arrays. Purified Sir2-3-4 heterotrimers bind chromatin, cooperatively yielding a stable complex of homogeneous molecular weight. Remarkably, Sir2-3-4 also binds naked DNA, reflecting the strong, albeit nonspecific, DNA-binding activity of Sir4. The binding of Sir3 to nucleosomes is sensitive to histone H4 N-terminal tail removal, while that of Sir2-4 is not. Dot1-mediated methylation of histone H3K79 reduces the binding of both Sir3 and Sir2-3-4. Additionally, a byproduct of Sir2-mediated NAD hydrolysis, O-acetyl-ADP-ribose, increases the efficiency with which Sir3 and Sir2-3-4 bind nucleosomes. Thus, in small cumulative steps, each Sir protein, unmodified histone domains, and contacts with DNA contribute to the stability of the silent chromatin complex.

H2A.Bbd: a quickly evolving hypervariable mammalian histone that destabilizes nucleosomes in an acetylation‐independent way

Molecular evolutionary analyses revealed that histone H2A.Bbd is a highly variable quickly evolving mammalian replacement histone variant, in striking contrast to all other histones. At the nucleotide level, this variability appears to be the result of a larger amount of nonsynonymous variation, which affects to a lesser extent, the structural domain of the protein comprising the histone fold. The resulting amino acid sequence diversity can be predicted to affect the internucleosomal and intranucleosomal histone interactions. Our phylogenetic analysis has allowed us to identify several of the residues involved. The biophysical characterization of nucleosomes reconstituted with recombinant mouse H2A.Bbd and their comparison to similar data obtained with human H2A.Bbd clearly support this notion. Despite the high interspecific amino acid sequence variability, all of the H2A.Bbd variants exert similar structural effects at the nucleosome level, which result in an unfolded highly unstable nucleoprotein complex. Such structure resembles that previously described for the highly dynamically acetylated nucleosomes associated with transcriptionally active regions of the genome. Nevertheless, the structure of nucleosome core particles reconstituted from H2A.Bbd is not affected by the presence of a hyperacetylated histone complement. This suggests that replacement by H2A.Bbd provides an alternative mechanism to unfold chromatin structure, possibly in euchromatic regions, in a way that is not dependent on acetylation.

Protein–Protein Förster Resonance Energy Transfer Analysis of Nucleosome Core Particles Containing H2A and H2A.Z

A protein–protein Förster resonance energy transfer (FRET) system, employing probes at multiple positions, was designed to specifically monitor the dissociation of the H2A–H2B dimer from the nucleosome core particle (NCP). Tryptophan donors and Cys-AEDANS acceptors were chosen because, compared to previous NCP FRET fluorophores, they: (1) are smaller and less hydrophobic, which should minimize perturbations of histone and NCP structure; and (2) have an R0 of 20 Å, which is much less than the dimensions of the NCP (∼50 Å width and ∼100 Å diameter). Equilibrium protein unfolding titrations indicate that the donor and acceptor moieties have minimal effects on the stability of the H2A–H2B dimer and (H3–H4)2 tetramer. NCPs containing the various FRET pairs were reconstituted with the 601 DNA positioning element. Equilibrium NaCl-induced dissociation of the modified NCPs showed that the 601 sequence stabilized the NCP to dimer dissociation relative to weaker positioning sequences. This finding implies a significant role for the H2A–H2B dimers in determining the DNA sequence dependence of NCP stability. The free energy of dissociation determined from reversible and well-defined sigmoidal transitions revealed two distinct phases reflecting the dissociation of individual H2A–H2B dimers, confirming cooperativity as suggested previously; these data allow quantitative description of the cooperativity. The FRET system was then used to study the effects of the histone variant H2A.Z on NCP stability; previous studies have reported both destabilizing and stabilizing effects. H2A.Z FRET NCP dissociation transitions suggest a slight increase in stability but a significant increase in cooperativity of the dimer dissociations. Thus, the utility of this protein–protein FRET system to monitor the effects of histone variants on NCP dynamics has been demonstrated, and the system appears equally well-suited for dissection of the kinetic processes of dimer association and dissociation from the NCP.

Structure of the Histone Chaperone Asf1 Bound to the Histone H3 C-Terminal Helix and Functional Insights

Asf1 is a histone chaperone that favors histone H3/H4 assembly and disassembly. We solved the structure of the conserved domain of human ASF1A in complex with the C-terminal helix of histone H3 using nuclear magnetic resonance spectroscopy. This structure is fully compatible with an association of ASF1 with the heterodimeric form of histones H3/H4. In our model, ASF1 substitutes for the second H3/H4 heterodimer that is normally found in heterotetrameric H3/H4 complexes. This result constitutes an essential step in the fundamental understanding of the mechanisms of nucleosome assembly by histone chaperones. Point mutations that perturb the Asf1/histone interface were designed from the structure. The decreased binding affinity of the Asf1-H3/H4 complex correlates with decreased levels of H3-K56 acetylation and phenotypic defects in vivo.

Crystal structures of histone Sin mutant nucleosomes reveal altered protein-DNA interactions.

Here we describe 11 crystal structures of nucleosome core particles containing individual point mutations in the structured regions of histones H3 and H4. The mutated residues are located at the two protein-DNA interfaces flanking the nucleosomal dyad. Five of the mutations partially restore the in vivo effects of SWI/SNF inactivation in yeast. We find that even nonconservative mutations of these residues (which exhibit a distinct phenotype in vivo) have only moderate effects on global nucleosome structure. Rather, local protein-DNA interactions are disrupted and weakened in a subtle and complex manner. The number of lost protein-DNA interactions correlates directly with an increased propensity of the histone octamer to reposition with respect to the DNA, and with an overall destabilization of the nucleosome. Thus, the disruption of only two to six of the approximately 120 direct histone-DNA interactions within the nucleosome has a pronounced effect on nucleosome mobility and stability. This has implications for our understanding of how these structures are made accessible to the transcription and replication machinery in vivo.

Crystal Structures of Nucleosome Core Particles in Complex with Minor Groove DNA-binding Ligands

We determined the crystal structures of three nucleosome core particles in complex with site-specific DNA-binding ligands, the pyrrole-imidazole polyamides. While the structure of the histone octamer and its interaction with the DNA remain unaffected by ligand binding, nucleosomal DNA undergoes significant structural changes at the ligand-binding sites and in adjacent regions to accommodate the ligands. Our findings suggest that twist diffusion occurs over long distances through tightly bound nucleosomal DNA. This may be relevant to the mechanism of ATP-dependent and spontaneous nucleosome translocation, and to the effect of bound factors on nucleosome dynamics.

Structure of the yeast nucleosome core particle reveals fundamental changes in internucleosome interactions.

Chromatin is composed of nucleosomes, the universally repeating protein-DNA complex in eukaryotic cells. The crystal structure of the nucleosome core particle from Saccharomyces cerevisiae reveals that the structure and function of this fundamental complex is conserved between single-cell organisms and metazoans. Our results show that yeast nucleosomes are likely to be subtly destabilized as compared with nucleosomes from higher eukaryotes, consistent with the idea that much of the yeast genome remains constitutively open during much of its life cycle. Importantly, minor sequence variations lead to dramatic changes in the way in which nucleosomes pack against each other within the crystal lattice. This has important implications for our understanding of the formation of higher order chromatin structure and its modulation by post-translational modifications. Finally, the yeast nucleosome core particle provides a structural context by which to interpret genetic data obtained from yeast. Coordinates have been deposited with the Protein Data Bank under accession number 1ID3.

Helical repeat of DNA in the nucleosome core particle

Although the crystal structure of nucleosome core particle is essentially symmetrical in the vicinity of the dyad, the linker histone binds asymmetrically in this region to select a single high-affinity site from potentially two equivalent sites. To try to resolve this apparent paradox we mapped to base-pair resolution the dyads and rotational settings of nucleosome core particles reassembled on synthetic tandemly repeating 20 bp DNA sequences. In agreement with previous observations, we observed (1) that the helical repeat on each side of the dyad cluster is 10 bp maintaining register with the sequence repeat and (2) that this register changes by 2 bp in the vicinity of the dyad. The additional 2 bp required to effect the change in the rotational settings is accommodated by an adjustment immediately adjacent to the dyad. At the dyad the hydroxyl radical cleavage is asymmetric and we suggest that the inferred structural asymmetry could direct the binding of the linker histone to a single preferred site.

Helical repeat of DNA in the nucleosome core particle

Although the crystal structure of nucleosome core particle is essentially symmetrical in the vicinity of the dyad, the linker histone binds asymmetrically in this region to select a single high-affinity site from potentially two equivalent sites. To try to resolve this apparent paradox we mapped to base-pair resolution the dyads and rotational settings of nucleosome core particles reassembled on synthetic tandemly repeating 20 bp DNA sequences. In agreement with previous observations, we observed (1) that the helical repeat on each side of the dyad cluster is 10 bp maintaining register with the sequence repeat and (2) that this register changes by 2 bp in the vicinity of the dyad. The additional 2 bp required to effect the change in the rotational settings is accommodated by an adjustment immediately adjacent to the dyad. At the dyad the hydroxyl radical cleavage is asymmetric and we suggest that the inferred structural asymmetry could direct the binding of the linker histone to a single preferred site.

The chromo domain protein chd1p from budding yeast is an ATP-dependent chromatin-modifying factor.

CHD proteins are members of the chromo domain family, a class of proteins involved in transcription, DNA degradation and chromatin structure. In higher eukaryotes, there are two distinct subfamilies of CHD proteins: CHD1 and CHD3/4. Analyses carried out in vitro indicate that the CHD3/4 proteins may regulate transcription via alteration of chromatin structure. However, little is known about the role of CHD proteins in vivo, particularly the CHD1 subfamily. To understand better the cellular function of CHD proteins, we initiated a study on the Chd1p protein from budding yeast. Using genomic DNA arrays, we identified genes whose expression is affected by the absence of Chd1p. A synthetic-lethal screen uncovered genetic interactions between SWI/SNF genes and CHD1. Biochemical experiments using Chd1p purified from yeast showed that it reconfigures the structure of nucleosome core particles in a manner distinct from the SWI-SNF complex. Taken together, these results suggest that Chd1p functions as a nucleosome remodeling factor, and that Chd1p may share overlapping roles with the SWI-SNF complex to regulate transcription.

Radiolysis of nucleosome core DNA: a modelling approach

Purpose : To calculate the expected pattern of frank strand breaks (FSB) induced in the DNA of a nucleosome core particle (NCP) by the attack of radiolytic OH •radicals and to compare this with the experimental pattern of FSB induced by the in vitro irradiation of chicken NCP. Materials and methods : The structure of NCP was obtained from the PDB databank. Using molecular modelling, the structure of a linear DNA fragment with the central 60 bp sequence of NCPDNA was determined. The accessibility of the sugar attack sites to OH •radicals at each nucleotide of the linear fragment or of the NCP-DNA was calculated. The probability of reaction of OH •with each sugar reactive site was calculated using a MonteCarlo method-based stochastic model. Results : The accessibility of attack sites in the NCP-DNA and the calculated probabilities of sugar attack are mainly modulated through masking by histones, and only slightly through bending. The periodicity of the calculated FSB probabilities is identical to that of the experimental FSB probabilities in chicken NCP (period 10.4 ±0.1bp). Conclusions : The good agreement between the calculated and experimental results recommends the presented modelling procedure as a tool in predicting the radiosensitivity of DNA in DNA-ligand complexes of known structure.