Higher-order structure of chromatin and chromosomes

The linear array of nucleosomes that comprises the primary structure of chromatin is folded and condensed to varying degrees in nuclei and chromosomes forming 'higher order structures'. We discuss the recent findings from novel experimental approaches that have yielded significant new information on the different hierarchical levels of chromatin folding and their functional significance.     

Fundamental features of chromatin structure

Which mechanisms regulate nuclear plasticity? Part of the answer to that question lies in understanding how genes are expressed and regulated in the context of chromatin structure. It is now clear that the genes are regulated in discrete and controlled stages, from packaging into chromatin to their localization within the nucleus. Whereas the genetic information provides the framework for the manufacture of all proteins necessary to create a living cell, chromatin structure controls how, where, and when the genetic information should be used. In this minireview, I summarize the main characteristics of chromatin structure and highlight some of the modifications usually associated with the regulation of gene expression.     

Cell cycle variations in chromatin structure detected by DNase I

We have recently developed a reproducible method for the use of DNase I as a sensitive probe of chromatin structure (Prentice, D A & Gurley, L R, Biochim biophys acta 740 (1983) 134) [12] and have used this probe to investigate chromatin structure during the interphase of the cell cycle. Chinese hamster cells (line CHO) were synchronized by: (1) mitotic detachment, to obtain M-phase cells; (2) isoleucine deprivation, to obtain G1-phase cells; and (3) sequential use of isoleucine deprivation followed by release into the presence of hydroxyurea, to obtain cells blocked at the start of S phase. The cells were released from the various blocking schemes and nuclei were isolated and digested with DNase I at various times. The digestion kinetics were monitored to detect possible changes in chromatin condensation through the cell cycle. The chromatin was much more accessible to DNase I in G1 phase than in S or G2 phase, with only small variations in structure detected in late G1 and very early S phase. From early S phase up to mitosis, the chromatin became increasingly condensed and inaccessible to DNase I action. These results support the concept of a chromatin condensation cycle during interphase as well as during mitosis.     

Orientation of interphase chromosomes as detected by Giemsa C-bands

The orientation of Giemsa C-bands has been studied in mitotic and interphase cells of Allium cepa, A. sativum and of Aloe vera. The C-bands in these three species are located at the telomeres, secondary constriction region of the nucleolar chromosomes and the centromeric regions, respectively. Observations in A. cepa and Aloe indicate clearly that the interphase chromosomes are non-random in their orientation and possibly maintain their telophase configuration through the attachment of telomeres and perhaps of kinetochores with the nuclear membrane. Electron micrographs of onion cells also reveal that certain heterochromatic segments are associated with the nuclear membrane. — The nucleolar interstitial C-bands in A. sativum remain free in the nucleoplasm and may come close to each other due to heterochromatic attraction. Such a heterochromatic attraction is also evident between telomeric regions and between centromeres. However, a two by two attachment could not be noticed. A diagrammatic representation of the orientation of interphase chromosomes has been presented.The major part of this work was presented at the First International Congress on Cell Biology, Boston, Sept. 5–10, 1976 (Platform Session 36, J. Cell Biol. 70, 418a (1976)     

Overall DNA methylation and chromatin structure of normal and abnormal X chromosomes

DNA methylation patterns were studied at the chromosome level in normal and abnormal X chromosomes using an anti-5-methylcytosine antibody. In man, except for the late-replicating X of female cells, the labeled chromosome structures correspond to R- and T-bands and heterochromatin. Depending on the cell type, the species, and cell culture conditions, the late-replicating X in female cells appears to be more or less undermethylated. Under normal conditions, the only structures that remain methylated on the X chromosomes correspond to pseudoautosomal regions, which harbor active genes. Thus, active genes are usually hypomethylated but are located in methylated chromatin. Structural rearrangements of the X chromosome, such as t(X;X)(pter;pter), induce a Turner syndrome-like phenotype that is inconsistent with the resulting triple-X constitution. This suggests a position effect controlling gene inactivation. The derivative chromosomes are always late replicating, and their duplicated short arms, which harbor pseudoautosomal regions, replicate later than the normal late-replicating X chromosomes. The compaction or condensation of this segment is unusual, with a halo of chromatin surrounding a hypocondensed chromosome core. The chromosome core is hypomethylated, but the surrounding chromatin is slightly labeled. Thus, unusual DNA methylation and chromatin condensation are associated with the observed position effect. This strengthens the hypothesis that DNA methylation at the chromosome level is associated with both chromatin structure and gene expression.     

Conservation of interphase chromatin nonhistone antigens as components of metaphase chromosomes

The degree of conservation of HeLa interphase chromatin nonhistone antigens among the nonhistones of isolated metaphase chromosomes was determined with immunological procedures. Proteins were separated on SDS-polyacrylamide gels and electrophoretically transferred to diazophenylthioether (DPT)-paper, which was then overlaid with antiserum to chromatin from interphase nuclei. The bound antibodies were detected with 125I-labeled protein A. Alternatively, polyacrylamide gels were directly overlaid with antiserum and with 125I-protein A. Densitometry of autoradiograms and stained gels revealed the degree of conservation of nonhistone antigenic determinants from interphase to metaphase to be over 90% for chromatin.     

Dense chromatin plates in metaphase chromosomes

In a previous work we observed multilayered plate-like structures surrounding partially denatured HeLa chromosomes at metaphase ionic conditions. This unexpected finding has led us to carry out an extensive investigation of these structures. Our results show that plates can also be found in metaphase chromosomes from chicken lymphocytes. We have used atomic force microscopy (AFM) to image and investigate the mechanical properties of plates in aqueous solution. Plates are thin (~6.5 nm each layer) but compact and resistant to penetration by the AFM tip: their Young’s modulus is ~0.2 GPa and the stress required for surface penetration is ~0.03 GPa in the presence of Mg²⁺ (5–20 mM). Low-ionic strength conditions produce emanation of chromatin fibers from the edges of uncrosslinked plates. These observations and AFM results obtained applying high forces indicate that the chromatin filament is tightly tethered inside the plates. Images of metal-shadowed plates and cryo-electron microscopy images of frozen-hydrated plates suggest that nucleosomes are tilted with respect to the plate surface to allow an interdigitation between the successive layers and a thickness reduction compatible with the observed plate height. The similarities between denatured plates from chicken chromosomes and aggregates of purified chromatin from chicken erythrocytes suggest that chromatin has intrinsic structural properties leading to plate formation. Scanning electron micrographs and images obtained with the 200-kV transmission microscope show that plates are the dominant component of compact chromatids. We propose that metaphase chromosomes are formed by many stacked plates perpendicular to the chromatid axis.     

Higher order structure of chromatin: evidence from photochemically detected linear dichroism

We have used photochemically detected linear dichroism to measure the separate average angular orientations of nucleosomes and linker DNA in 30-nm chromatin fibers of varying linker size (20-80 base pairs). Our results indicate that the average tilt angles vary with linker size, but not in a monotonic manner, suggesting that the constancy of geometry of the 30-nm fiber is maintained by compensatory changes of nucleosomal tilt which accommodate packing of variable lengths of linker DNA. We discuss the compatibility of our results with the various classes of models that have been proposed for the 30-nm fiber, including the continuous solenoid model and models built from the basic unit of the zig-zag ribbon. Many models can be eliminated, and all have to be modified to fit our results for chromatins with very long linkers.     

Micromechanics of chromatin and chromosomes.

The enzymes that transcribe, recombine, package, and duplicate the eukaryotic genome all are highly processive and capable of generating large forces. Understanding chromosome function therefore will require analysis of mechanics as well as biochemistry. Here we review development of new biophysical-biochemical techniques for studying the mechanical properties of isolated chromatin fibers and chromosomes. We also discuss microscopy-based experiments on cells that visualize chromosome structure and dynamics. Experiments on chromatin tell us about its flexibility and fluctuation, as well as quantifying the forces generated during chromatin assembly. Experiments on whole chromosomes provide insight into the higher-order organization of chromatin; for example, recent experiments have shown that the mitotic chromosome is held together by isolated chromatin-chromatin links and not a large, mechanically contiguous non-DNA "scaffold".     

Restriction endonuclease resistant chromatin in human chromosomes

Summary The recent addition of restriction endonucleases in obtaining selective bands in the human genome has added a new dimension to molecular genetics. However, a considerable discrepancy exists in banding patterns produced by AluI in chromosomes 19 and 20, by MboI in chromosomes 4, 5, 8, 21 and 22 and by RsaI in chromosomes 12, 21 and 22. The principal causes of these differences are highlighted.     

Visualizing chromatin and chromosomes in living cells

The dynamic organization of eukaryotic genomes in cell nuclei recently came into the focus of research interest. The kinetics of genome dynamics can be addressed only by approaches involving live cell microscopy. Different methods are available to visualize chromatin, specific chromatin fractions, or individual chromosome territories within nuclei of living mammalian cells. Appropriate labeling procedures as well as cell chamber systems and important controls for live cell microscopy are described.     

Evidence for tertiary structure in natural single stranded RNAs in solution.

Binding isotherms (20 degrees C) of ethidium bromide to a number of tRNA species at various ionic strengths indicate that i) the number ni of intercalation sites is high 7 to 11 per molecule, in the low salt form III, but small, 2 to 1, at high Mg2+ or Na+ when form I predominates. ii) modification of tRNA at strategic positions for 3D folding prevents full expression of intercalation restriction iii) maximal restriction is obtained at salt concentrations higher than needed for full conversion to form I. It is inferred that restriction, which is not observed with bihelical RNA (or DNA), requires the native tRNA 3D structure but also some physical coupling between the region of 3D folding and bihelical arms. Ribosomal RNAs, some viral RNAs, mRNA from sheep mammary gland as well as the random copolymers Poly UG, Poly AUG, Poly AUCG all exhibit intercalation restriction. Hence 3D folding of the polyribonucleotide chains appears to be a feature common to single-stranded RNAs when free in solution under physiological conditions.     

Structural features of 3C6/C7 interband chromatin organization in Drosophila melanogaster polytene chromosomes

Mechanisms of chromatin decompaction in interbands of Drosophila polytene chromosomes have been studied. Using the example of interband 3C6/C7 of the X chromosome, we investigated the ability of different DNA segments to form an interband in a new genetic environment. We applied site-specific FLP recombination between two transposons with FRT-sites that allows introducing the DNA fragments from the interband 3C6/C7 into pICon(dv) transposon located in cytologically well-characterized 84F region of chromosome 3 followed by electron microscopic analysis of changes in the region caused by insertion of the DNA fragments into the transposon. It was shown that the insertion of a 276-bp DNA fragment from the 3C6/C7 region into the pICon(dv) transposon leads to the formation of a new interband between two thin bands represented by the transposon material. This DNA fragment is the known minimal sequence that is necessary and sufficient for interband generation. In addition, the sequence containing three copies repeated in tandem of 0.9 kb DNA from the interband 3C6/C7, including the 276-bp fragment, were integrated in the transposon. The presence of introduced DNA fragments did not change the morphology of the resulting interband. It was shown that the sites of DNase I hypersensitivity were saved in transposon sequences introduced into a new genetic environment. The data obtained allow analysis to be started of specific factors (proteins, DNA motifs, etc.) that determine the formation of decompacted chromatin in a certain interband region and chromomeric organization of interphase chromosomes in Drosophila as a whole.     

Differential silver staining of chromatin in metaphase chromosomes

The silver techniques used to demonstrate nucleolar organizer regions and cores in chromosomes can also differentially stain chromatin within chromosomes. Direct silver staining of mouse and human chromosomes resulted in preferential staining of centromeric regions and non-nucleolar secondary constrictions, both of which are composed of constitutive heterochromatin. After C-banding, these regions were no longer silver-stainable, suggesting that the biochemical constituents (presumably non-histone proteins) which contain the reaction sites for silver are extracted during the banding treatment. Light and electron microscopy of chromosomes G-banded with trypsin and then silver-stained revealed heavier deposits of silver over the condensed aggregates of chromatin within the band regions than over the more dispersed interband chromatin. At the ultrastructural level, chromatin fibres were covered with silver grains, indicating that there are many reaction sites for this metal along the fibres. These results suggest that the degree of silver staining in any region of the chromosome may be contingent upon the concentration of chromatin in that region. This finding may have important implications concerning the nature of the silver-stained core-like structure in chromosomes. If a preferential dispersion of chromatin fibres occurs at the periphery of the chromosome during slide preparation, leaving the central region of each chromatid relatively undispersed, this difference in the concentration of chromatin may account for the differential silver staining of these regions and the consequent appearance of a core-like structure.