A double coil chromatin sub-unit model

A model is proposed for the structure of DNA in chromatin sub-units. Each sub-unit is proposed to contain two turns of an inner coil, with a pitch of about 40and an external diameter of 70 . Around the inner coil is wound, in opposite handedness, a slightly larger amount of DNA at a diameter of about 150 . The total contour length consistent with the electron micrographs and X-ray scattering is 600–700 , or about 200 base pairs. It is suggested that the inner coil is protein rich and contains all of the histones except H1, which is associated with the outer coil. The double-coil model is consistent with previous biochemical and biophysical studies of chromatin. The existence of 200 and 100 base pair digestion fragments and a 6 to 1 DNA compaction are readily explained.This model is based upon the electron microscopic observation of replicas of frozen chromatin and X-ray and neutron scattering. Structural details of 25are preserved and visualized by the freeze fracture electron microscopy techniques employed.     

A model for chromatin structure.

A model for chromatin structure is presented. (a) Each of four histone species, H2A (IIbl or f2a2), H2B (IIb2 or f2b), H3 (III or f3) and H4 (IV or f2al) can form a parallel dimer. (b) These dimers can form two tetramers, (H2A)2(H2b)2 and (H3)2(H4)2. (C) These two tetramers bind a segment of DNA and condense it into a "C" segments. (d) The adjacent segments, termed extended or "E" segments, are bound by histone H1 (I or fl) for the major fraction of chromatin; the other "E" regions can be either bound by non-histone proteins or free of protein binding. (e) The binding of histones causes a structural distortion of the DNA which, depending upon the external conditions, may generate the formation of either an open structure with a heterogeneous and non-uniform supercoil or a compact structure with a string of beads. The model is supported by experimental data on histone-histone interaction, histone-DNA interaction and histone subunit-DNA interaction.     

A model chromatin assembly system. Factors affecting nucleosome spacing

Poly[d(A-T)].poly[d(A-T)], when reconstituted with chicken erythrocyte core histones and subsequently incubated with sufficient histone H5 in a solution containing polyglutamic acid, forms structures resembling chromatin. H5 induces nucleosome alignment in about two hours at physiological ionic strength and 37 degrees C. The nucleosome spacing and apparent linker heterogeneity in the assembled nucleoprotein are very similar to those in chicken erythrocyte chromatin. Also, condensed chromatin-like fibers on the polynucleotide can be visualized. The binding of one mole of H5 per mole of core octamer is necessary to generate the physiological nucleosome spacing, which remains constant with the addition of more H5. The nucleosome repeat length is not a function of the core histone to poly[d(A-T)] ratio for values lower than the physiological ratio. With increasing ratios, in excess of the physiological value, nucleosome spacing first becomes non-uniform, and then takes on the close packing limit of approximately 165 base-pairs. In addition to eliminating possible base sequence effects on nucleosome positioning, poly[d(A-T)] allows nucleosomes to slide more readily than does DNA, thereby facilitating alignment. Evidence is presented that polyglutamic acid facilitates the nucleosome spacing activity of histone H5, primarily by keeping the nucleoprotein soluble. This model system should be useful for understanding how different repeat lengths arise in chromatin.     

A model for particulate structure in chromatin

A model is proposed for the structure of nuclease-resistant chromatin particles. The model is novel in that it proposes that the DNA in such a particle is wound about a protein core, made up of the hydrophobic regions of histone molecules.     

Beta-sheet coil transitions in a simple polypeptide model.

A simplified model of a polypeptide chain is used to study the dynamics of the beta-sheet-coil transition. Each amino acid residue is treated as a single quasiparticle in an effective potential that approximates the potential of mean force in solution. The model is used to study the equilibrium and dynamic aspects of the sheet-coil transition. Systems studied include ones with both strands free to move (two-strand sheet), and ones with either strand fixed in position (multistrand sheet). The equilibrium properties examined include sheet-coil equilibrium constants and their dependence on chain position. Dynamic properties are investigated by a stochastic simulation of the Brownian motion of the chain in its solvent surroundings. Time histories of the dihedral angles and residue-residue cross-strand distances are used to study the behavior of the sheet structure. Auto- and cross-correlation functions are calculated from the time histories with relaxation times of tens to hundreds of picoseconds. Sheet-coil rate constants of tens of ns-1 were found for the fixed strand cases.     

The double helix coiled coil structure of murein lipoprotein from Escherichia coli.

A rod-like structure is proposed for the murein lipoprotein of Escherichia coli, built of two parallel unbroken α-helices arranged in a coiled coil of the same type as in the muscle protein tropomyosin. The amino acid sequence has the required regular pattern of hydrophobic amino acids at intervals of three and four residues and the secondary structure predicted from the sequence is 80% helical. A space-filling model confirms that the coiled coil model is stereochemically reasonable, and energy calculations for a series of coils with different radii suggest that the best structure is one with the helix axes 8.25 Å apart. Energyrefined atomic co-ordinates have been calculated which show that the hydrophobic side-chains form a series of close-packed unstrained contacts between the two helices along the entire length of the sequence. On the basis of this study the hexagonal membrane pore model and the segmented helix model proposed by others seem unlikely. The coiled coil has a strongly hydrophilic outer surface, suggesting that the protein has a watery environment within the E. coli cell envelope and is not strictly a membrane protein. Probably only the fatty acid portion of the lipoprotein penetrates into the lipid region of the outer membrane, so that the protein may act as a tie or a spacer between the lipid and the murein wall.     

A model for chromatin opening: stimulation of topoisomerase II and restriction enzyme cleavage of chromatin by distamycin.

Histone H1 preferentially and cooperatively binds scaffold-associated regions (SARs) in vitro via specific interactions with the numerous short A + T-rich tracts (A-tracts) contained in these sequences. Selective titration of A-tracts by the oligopeptide distamycin abolishes this interaction and results in a redistribution of H1. Similarly, treatment of intact cells and isolated nuclei with distamycin specifically enhances cleavage of internucleosomal linkers of SARs by topoisomerase II and restriction enzymes. The increased accessibility of these linkers is thought to result from the unfolding (or opening) of the chromatin fiber and to be due to a reduced occupancy by histone H1. Chromatin extraction and H1 assembly experiments support this view. We discuss a model whereby open, H1-depleted chromatin regions may be generated by titration of A-tracts by putative distamycin analogues; this local opening may spread to adjacent regions assuming highly cooperative H1-H1 interactions in chromatin.     

Signaling network model of chromatin

We suggest that common principles underlie both cellular signaling networks and chromatin. To exemplify similarities, we focus on signaling complexes that form at membrane receptors and on nucleosomes. Multiple signal-transducing modifications on side chain residues of receptor tyrosine kinases (RTKs) and histone proteins are used to create docking sites that facilitate proximal relations of enzymes and their substrates. We argue that multiple histone modifications, like RTK modifications, promote switch-like behavior and ensure robustness of the signal, and we compare this interpretation with the histone code hypothesis. This view provides insight into chromatin function and epigenetic inheritance.     

A polymer model for large-scale chromatin organization in lower eukaryotes

A quantitative model of large-scale chromatin organization was applied to nuclei of fission yeast Schizosaccharomyces pombe (meiotic prophase and G2 phase), budding yeast Saccharomyces cerevisiae (young and senescent cells), Drosophila (embryonic cycles 10 and 14, and polytene tissues) and Caenorhabditis elegans (G1 phase). The model is based on the coil-like behavior of chromosomal fibers and the tight packing of discrete chromatin domains in a nucleus. Intrachromosomal domains are formed by chromatin anchoring to nuclear structures (e.g., the nuclear envelope). The observed sizes for confinement of chromatin diffusional motion are similar to the estimated sizes of corresponding domains. The model correctly predicts chromosome configurations (linear, Rabl, loop) and chromosome associations (homologous pairing, centromere and telomere clusters) on the basis of the geometrical constraints imposed by nuclear size and shape. Agreement between the model predictions and literature observations supports the notion that the average linear density of the 30-nm chromatin fiber is approximately 4 nucleosomes per 10 nm contour length.     

A model for chromatin based upon two symmetrically paired half-nucleosomes

We propose that the basic unit of chromatin is constructed of two isologously paired heterotypic protein tetramers each containing one molecule of H2A, H2B, H3, and H4 histone. These proteins form a core that holds 140 base pairs (bp) of DNA in a single left-handed, non-interwound DNA supercoil approximately 95 bp in circumference, creating A nucleosome particle (DNA and protein) organized about a dyad axis of symmetry. Such a nucleosome can open up into its separate half-nucleosomes to allow genetic readout without requiring histone displacement     

Protein dissociation from DNA in model systems and chromatin.

Salt induced dissociation of protamine, poly(L-lysine) and poly(L-arginine) from DNA was measured by relative light scattering at theta = 90 degrees and/or centrifugation. Dissociation of histones from DNA was studied using relative light scattering and intrinsic tyrosine fluorescence. Protamine was dissociated from DNA at 0.15 M MgCl2 (ionic strength mu = 0.45) or 0.53 M NaCl (mu = 0.53) based on light scattering data and at approximately 0.2 M MgCl2 (mu = 0.6) or 0.6 M NaCl based on centrifugation data. NaCl induced dissociation of poly(Lys) or poly(Arg) from natural DNAs measured by light scattering did not depend on the guanine plus cytosine content. To dissociate poly(Arg) from DNA higher ionic strength using NaCl, MgCl2, or CaCl2, similar ionic strength using NaClo4, and lower ionic strength using Na2SO4 was needed then to dissociated poly(Lys). Both the decrease in light scattering and the enhancement of tyrosine fluorescence of chromatin occurred between 0.5 and 1.5 M NaCl when histones were dissociated.     

Helix–coil transition in heterogeneous chains. II. DNA model

Melting curves are calculated for infinitely long DNA-like random copolymers composed of AT and GC pairs of nucleotides. The entropy of random coil rings formed on melting is explicitly included through use of the Jacobson-Stockmayer ring-weighting factors. Transition curves are calculated for values of the cooperativity parameter σ in the range 10^?2 ? σ ? 10^?4. Ninety percent of the melting occurs in ca. 0.2°C for σ ? 10^?3 regardless of the mole fraction of GC. We conclude that observed breadths of thermal denaturation curves for native DNAs result from a superposition of essentially all-or-none melting of various regions of the molecule. It is argued that refined approximations to the ring-weighting factors are probably not important when compared with the effects produced by long-range base sequence correlations which are known to occur in native DNA.     

A triple helix model for the structure of chromatin fiber

A model of chromatin fiber structure is presented in which a repeating unit of a trinucleosome forms a 3-dimensional zigzag. Twisting and compression of the zigzag result in a triple helix structure. The model is built mainly on the flow linear dichroism data showing that nucleosomal disc faces are tilted relative to the fiber axis, the orientation of nucleosomes does not change upon folding and unfolding of chromatin, and the orientation of nucleosomes is maintained by the globular domain of histone H1.     

A model for the structure of chromatin in mammalian sperm

DNA in mammalian, and most vertebrate sperm, is packaged by protamines into a highly condensed, biochemically inert form of chromatin. A model is proposed for the structure of this DNA-protamine complex which describes the site and mode of protamine binding to DNA and postulates, for the first time, specific inter- and intraprotamine interactions essential for the organization of this highly specialized chromatin. In this model, the central polyarginine segment of protamine binds in the minor groove of DNA, crosslinking and neutralizing the phosphodiester backbone of DNA while the COOH- and NH2-terminal ends of protamine participate in the formation of inter- and intraprotamine hydrogen, hydrophobic, and disulfide bonds. Each protamine segment is of sufficient length to fill one turn of DNA, and adjacent protamines are locked in place around DNA by multiple disulfide bridges. Such an arrangement generates a neutral, insoluble chromatin complex, uses all protamine sulfhydryl groups for cross linking, conserves volume, and effectively renders the chromatin invulnerable to most external influences.     

Roles of chromatin remodellers in DNA double strand break repair

Now that we have a good understanding of the DNA double strand break (DSB) repair mechanisms and DSB-induced damage signalling, attention is focusing on the changes to the chromatin environment needed for efficient DSB repair. Mutations in chromatin remodelling complexes have been identified in cancers, making it important to evaluate how they impact upon genomic stability. Our current understanding of the DSB repair pathways suggests that each one has distinct requirements for chromatin remodelling. Moreover, restricting the extent of chromatin modifications could be a significant factor regulating the decision of pathway usage. In this review, we evaluate the distinct DSB repair pathways for their potential need for chromatin remodelling and review the roles of ATP-driven chromatin remodellers in the pathways.