Chromonema and chromomere: Structural units of mitotic and interphase chromosomes

Helical chromonema coiling is conserved in eukaryotes

Efficient chromatin condensation is required to transport chromosomes during mitosis and meiosis, forming daughter cells. While it is well accepted that these processes follow fundamental rules, there has been a controversial debate for more than 140 years on whether the higher-order chromatin organization in chromosomes is evolutionarily conserved. Here, we summarize historical and recent investigations based on classical and modern methods. In particular, classical light microscopy observations based on living, fixed, and treated chromosomes covering a wide range of plant and animal species, and even in single-cell eukaryotes suggest that the chromatids of large chromosomes are formed by a coiled chromatin thread, named the chromonema. More recently, these findings were confirmed by electron and super-resolution microscopy, oligo-FISH, molecular interaction data, and polymer simulation. Altogether, we describe common and divergent features of coiled chromonemata in different species. We hypothesize that chromonema coiling in large chromosomes is a fundamental feature established early during the evolution of eukaryotes to handle increasing genome sizes.

Fiber-Like Organization as a Basic Principle for Euchromatin Higher-Order Structure

A detailed understanding of the principles of the structural organization of genetic material is of great importance for elucidating the mechanisms of differential regulation of genes in development. Modern ideas about the spatial organization of the genome are based on a microscopic analysis of chromatin structure and molecular data on DNA–DNA contact analysis using Chromatin conformation capture (3C) technology, ranging from the “polymer melt” model to a hierarchical folding concept. Heterogeneity of chromatin structure depending on its functional state and cell cycle progression brings another layer of complexity to the interpretation of structural data and requires selective labeling of various transcriptional states under nondestructive conditions. Here, we use a modified approach for replication timing-based metabolic labeling of transcriptionally active chromatin for ultrastructural analysis. The method allows pre-embedding labeling of optimally structurally preserved chromatin, thus making it compatible with various 3D-TEM techniques including electron tomography. By using variable pulse duration, we demonstrate that euchromatic genomic regions adopt a fiber-like higher-order structure of about 200 nm in diameter (chromonema), thus providing support for a hierarchical folding model of chromatin organization as well as the idea of transcription and replication occurring on a highly structured chromatin template.

Visualization of chromosome condensation in plants with large chromosomes

BACKGROUND

Most data concerning chromosome organization have been acquired from studies of a small number of model organisms, the majority of which are mammals. In plants with large genomes, the chromosomes are significantly larger than the animal chromosomes that have been studied to date, and it is possible that chromosome condensation in such plants was modified during evolution. Here, we analyzed chromosome condensation and decondensation processes in order to find structural mechanisms that allowed for an increase in chromosome size.

RESULTS

We found that anaphase and telophase chromosomes of plants with large chromosomes (average 2C DNA content exceeded 0.8 pg per chromosome) contained chromatin-free cavities in their axial regions in contrast to well-characterized animal chromosomes, which have high chromatin density in the axial regions. Similar to animal chromosomes, two intermediates of chromatin folding were visible inside condensing (during prophase) and decondensing (during telophase) chromosomes of Nigella damascena: approximately 150 nm chromonemata and approximately 300 nm fibers. The spatial folding of the latter fibers occurs in a fundamentally different way than in animal chromosomes, which leads to the formation of chromosomes with axial chromatin-free cavities.

CONCLUSION

Different compaction topology, but not the number of compaction levels, allowed for the evolution of increased chromosome size in plants.

Chromatin fibers: from classical descriptions to modern interpretation

The first description of intrachromosomal fibers was made by Baranetzky in 1880. Since that time, a plethora of fibrillar substructures have been described inside the mitotic chromosomes, and published data indicate that chromosomes may be formed as a result of the hierarchical folding of chromatin fibers. In this review, we examine the evolution and the current state of research on the morphological organization of mitotic chromosomes.

Systematic chromosomal analysis of cultured mouse neural stem cell lines

The potential use of neural stem cells (NSCs) in basic research, drug testing, and for the development of therapeutic strategies is dependent on their large scale in vitro amplification which, however, introduces considerable risks of genetic instability and transformation. NSCs have been derived from different sources, but the occurrence of chromosomal instability has been monitored only to a limited extent in relationship to the source of derivation, growth procedure, long-term culture, and genetic manipulation. Here we have systematically investigated the effect of these parameters on the chromosomal stability of pure populations of mouse NSCs obtained after neuralization from embryonic stem cells (ESCs) or directly from fetal or adult mouse brain. We found that the procedure of NSCs establishment is not accompanied by genetic instability and chromosomal aberration. On the contrary, we observed that a composite karyotype appears in NSCs above extensive passaging. This phenomenon is more evident in ESC- and adult sub-ventricular zone-derived NSCs and further deteriorates after genetic engineering of the cells. Fetal-derived NSCs showed the greatest euploidy state with negligible clonal structural aberrations, but persistent clonal numerical abnormalities. It was previously published that long-term passaged ESC- and adult sub-ventricular zone-derived NSCs did not show any defects in the cells' proliferative and differentiative capacity nor induced in vivo tumour formation, although we here report on the chromosomal abnormalities of these cells. Although chromosomal aberrations are known to occur less frequently in human cells, studies performed on murine stem cells provide an important complement to understand the biological events occurring in human lines.

Linking topology of tethered polymer rings with applications to chromosome segregation and estimation of the knotting length

The Gauss linking number (Ca) of two flexible polymer rings which are tethered to one another is investigated. For ideal random walks, mean linking-squared varies with the square root of polymer length while for self-avoiding walks, linking-squared increases logarithmically with polymer length. The free-energy cost of linking of polymer rings is therefore strongly dependent on degree of self-avoidance, i.e., on intersegment excluded volume. Scaling arguments and numerical data are used to determine the free-energy cost of fixed linking number in both the fluctuation and large-Ca regimes; for ideal random walks, for |Ca|>N;{1/4} , the free energy of catenation is found to grow proportional, variant|Ca/N;{1/4}|;{4/3} . When excluded volume interactions between segments are present, the free energy rapidly approaches a linear dependence on Gauss linking (dF/dCa approximately 3.7k_{B}T) , suggestive of a novel "catenation condensation" effect. These results are used to show that condensation of long entangled polymers along their length, so as to increase excluded volume while decreasing number of statistical segments, can drive disentanglement if a mechanism is present to permit topology change. For chromosomal DNA molecules, lengthwise condensation is therefore an effective means to bias topoisomerases to eliminate catenations between replicated chromatids. The results for mean-square catenation are also used to provide a simple approximate estimate for the "knotting length," or number of segments required to have a knot along a single circular polymer, explaining why the knotting length ranges from approximately 300 for an ideal random walk to 10;{6} for a self-avoiding walk.

Micromechanical studies of mitotic chromosomes

Mitotic chromosomes respond elastically to forces in the nanonewton range, a property important to transduction of stresses used as mechanical regulatory signals during cell division. In addition to being important biologically, chromosome elasticity can be used as a tool for investigating the folding of chromatin. This paper reviews experiments studying stretching and bending stiffness of mitotic chromosomes, plus experiments where changes in chromosome elasticity resulting from chemical and enzyme treatments were used to analyse connectivity of chromatin inside chromosomes. Experiments with nucleases indicate that non-DNA elements constraining mitotic chromatin must be isolated from one another, leading to the conclusion that mitotic chromosomes have a chromatin 'network' or 'gel' organization, with stretches of chromatin strung between 'crosslinking' points. The as-yet unresolved questions of the identities of the putative chromatin crosslinkers and their organization inside mitotic chromosomes are discussed.

Structural-functional model of the mitotic chromosome

In the present review the structural role of noncoding DNA, mechanisms of differential staining of mitotic chromosomes, and structural organization of different levels of DNA compactization are discussed. A structural-functional model of the mitotic chromosome is proposed based on the principle of discreteness of structural levels of DNA compactization.

Visualization of early chromosome condensation: a hierarchical folding, axial glue model of chromosome structure

Current models of mitotic chromosome structure are based largely on the examination of maximally condensed metaphase chromosomes. Here, we test these models by correlating the distribution of two scaffold components with the appearance of prophase chromosome folding intermediates. We confirm an axial distribution of topoisomerase IIα and the condensin subunit, structural maintenance of chromosomes 2 (SMC2), in unextracted metaphase chromosomes, with SMC2 localizing to a 150–200-nm-diameter central core. In contrast to predictions of radial loop/scaffold models, this axial distribution does not appear until late prophase, after formation of uniformly condensed middle prophase chromosomes. Instead, SMC2 associates throughout early and middle prophase chromatids, frequently forming foci over the chromosome exterior. Early prophase condensation occurs through folding of large-scale chromatin fibers into condensed masses. These resolve into linear, 200–300-nm-diameter middle prophase chromatids that double in diameter by late prophase. We propose a unified model of chromosome structure in which hierarchical levels of chromatin folding are stabilized late in mitosis by an axial “glue.”

Macromolecular and ultrastructural organization of the mitotic chromosome scaffold

Using electron microscopy (EM), we have examined three structural domains of the mitotic chromosome scaffold of mouse erythroleukemia (MEL) Friend cells with different morphologic organization: centromeric, intermediate, and telomeric. The intermediate, most extensive, domain exhibited a specific fibrogranular structure representing tightly packed granular bodies with diameters between 20 and 60 nm. The chromosome scaffold contained three main components: proteins (81%), RNA (12%), and DNA (7%). The residual DNA extracted from the scaffold represented short fragments, 300 bp on average, belonging to the class of tandemly arranged repetitive DNA. In situ hybridization experiments confirmed its typical centromeric location. Scaffold RNA represented three fractions: a major RNA fraction with an electrophoretic mobility corresponding to that of 5S RNA and two minor fractions with electrophoretic mobilities somewhat lower than that of 18S RNA. Scaffold RNA was localized mainly in the centromeric region. We show that the newly synthesized protein component of the chromosome scaffolds migrates slowly to the chromosomes, reaching a maximum specific radioactivity 12 h from the onset of the chase period.

A chromomeric model for nuclear and chromosome structure

The basic structural elements of chromatin and chromosomes are reviewed. Then a model involving only three architectural motifs, nucleosomes, chromatin loops and transcription factories/chromomeres, is presented. Loops are tied through transcription factors and RNA polymerases to factories during interphase and to the remnants of those factories, chromomeres, during mitosis. On entry into mitosis, increased adhesiveness between nucleosomes and between factories drives a ‘sticky-end’ aggregation to the most compact and stable structure, a cylinder of nucleosomes around an axial chromomeric core.

Stably DNA-bound chromosomal proteins

DNA accomplishes its biological function in a complex with nuclear proteins. A minor protein fraction has been found in chromatin which could not be dissociated from DNA by reagents abolishing non-covalent type of interactions. The controversy surrounding the nature of the protein moiety and the nature of the bond linking the two components on the one hand, and the fact pointing to its evolutionary conservatism and metabolic stability on the other, make it necessary to critically evaluate the data in view of the possible biological function for such proteins.

A fractal model of chromosomes and chromosomal DNA replication

With the aim of clarifying topological problems involved in the process of chromosomal DNA replication, a fractal model of chromosomes was built based on the assumption that a part of a chromosome, e.g. a radial loop, is similar in shape to a whole chromosome and each radial loop represents structures in the lower-order organization (an assumption of self-similarity). Several other assumptions used include (i) one continuous DNA fiber makes a whole chromosome (a unineme hypothesis), (ii) in situ DNA exists in the form of a double duplex or a tetraplex which is made of two duplex DNAs, although a duplex DNA may appear transiently in S-phase (multi-strandedness hypothesis) and (iii) torsional stress on a DNA fiber causes the fiber to supercoil and thus stabilizes chromosome structure (torque-based stabilization). This model allowed to calculate of a fractal dimension of a representative metaphase chromosome (e.g. d = 2.34), to predict the mode of replication of double duplex and to furnish a topological basis for the decondensation unit hypothesis. It must also be admitted that all the arguments in this report except for the possible existence of split telomeres hold true without assuming a tetraplex organization of chromosomes. Implications of this model was discussed and the importance of the fractal dimension as a measure of chromatin condensation stressed.

Large-scale chromatin structural domains within mitotic and interphase chromosomes in vivo and in vitro

Higher-order chromatin structural domains approximately 130 nm in width are observed as prominent components of both Drosophila melanogaster and human mitotic chromosomes using buffer conditions which preserve chromosome morphology as determined by light microscopic comparison with chromosomes within living cells. Spatially discrete chromatin structural domains of similar size also exist as prominent components within interphase nuclei prepared under equivalent conditions. Examination of chromosomes during the anaphase-telophase transition suggests that chromosomes decondense largely through the progressive straightening or uncoiling of these large-scale chromatin domains. A quantitative analysis of the size distribution of these higher-order domains in telophase nuclei indicated a mean width of 126 +/- 36 nm. Three-dimensional views using stereopairs of chromosomes and interphase nuclei from 0.5 micron thick sections suggest that these large-scale chromatin domains consist of 30 nm fibers packed by tight folding into larger, linear, fiber-like elements. Reduction in vitro of either polyamine or divalent cation concentrations within two different buffer systems results in a loss of these large-scale domains, with no higher-order chromatin organization evident above the 20-30 nm fiber. Under these conditions the DNA distribution within mitotic chromosomes and interphase nuclei appears significantly diffuse relative to the appearance by light microscopy within living cells, or, by electron microscopy, within cells fixed directly without permeabilization in buffer. These results suggest that these large-scale chromatin structural domains are fundamental elements of chromosome architecture in vivo.

Differential decondensation of mitotic chromosomes during hypotonic treatment of living cells as a possible cause of G-banding: an ultrastructural study

The chromosomal ultrastructure of Chinese hamster cells treated with 0.075 M KCl - a solution ordinarily used for making preparations of spread chromosomes - was studied. The hypotonic treatment was shown to result in differential decondensation of chromosomes which consists in the uneven distribution of deoxyribonucleoprotein (DNP) fibrils along chromatids. Fixation of cells with methanol acetic acid causes an abrupt restructuring of chromosomes. However, the DNP preserves its uneven distribution along chromatids. As seen on ultra-thin sections of marker nucleolus organizer chromosomes, the densely packed regions may correspond to G-bands detected in the selfsame chromosomes by standard methods of differential staining. The results suggest that the capacity of chromosomes for differential staining is based on the different resistance of G- and R-bands to the decondensing action of hypotonic solutions on living cells.

Ultrastructure of somatic and meiotic nucleoids

In this review emphasis is placed on the contribution of transmission electron microscopy to the analysis of spread chromosomes and nucleoids. Support is advanced for the DNA loop and rosette organization of meiotic and metaphase chromosomes and nucleoids. Extensive discussion is given to the biochemical treatments used for producing nucleoids and the effect of divalent cations and chelating agents on chromatin compactization (supercoiling). Detailed studies on nucleoids from hepatocytes are presented, with emphasis on the significance of DNA attachment to the internal nuclear matrix and to the nuclear lamina. It is firmly predicted that from the increasing knowledge of the structural organization of eukaryotic chromatin and the genome, a greater understanding of the functional roles of the various intranuclear structures will ultimately follow.

Two mechanisms of chromatin compaction

2 types of chromatin compaction were studied by cytochemical and ultrastructural approach. The 1st type was induced by cultivating transformed cells with dimethylsulfoxide. It caused cell transition into a more differentiated state coupled with the appearance of multiple small chromatin condensates. The 2nd type was induced by nonionic detergent Triton X-100 and/or saline penetration inside the nuclei. It was found to be connected with hypercompaction of chromocenters with their integral areas left unincreased. Both types of chromatin compaction differ in their capacity to induce toluidine blue polymerization on DNA substrate and in stability of DNA towards an early step of acid hydrolysis. The relation of the 2 mechanisms of chromatin compaction to different ways of DNA folding is discussed.

Packing of the 30 nm chromatin fiber in the human metaphase chromosome

The human genetic material is packed hierarchically within the metaphase chromosome: the DNA molecule together with histone proteins form 11 nm diameter nucleosomes, which are then ordered into the 30 nm thick chromatin fiber. Little is known about the packing of this fiber within the chromosome. We have developed a tracking algorithm with which we followed its path within a three-dimensional reconstruction of a human chromosome computed from a series of electron micrographic projections. Fiber segments were seen to form loops of 100-350 nm diameter. Our observations indicate that these loops--which themselves show no preferred orientation--are organised into regions of roughly 200 nm axial extent.

Three-dimensional reconstruction of a human metaphase chromosome from electron micrographs

A complete human metaphase chromosome has been reconstructed from a series of electron microscopical projections obtained by tilting the specimen stage at 3 degree intervals from -60 to +60 degrees. The reconstructed structure is about 3.0 microns long, 1.6 micron wide, and 0.8 micron thick. The mass distribution was fairly homogeneous within the chromatids and neither a hollow nor a dense core was observed. The distribution and course of fibers observed are most consistent with a looping model of chromosome structure.

High-order structure of metaphase chromosomes: evidence for a multiple coiling model

When chromosome preparations made by the conventional air-drying method were processed with the OSO4/TCH technique and examined by scanning electron microscopy (SEM), spiral structures in chromatids, which have been frequently observed to be present by light microscopy, were found to be composed of 30 nm fibres. In some portions these fibres appeared to be arranged in coils to form thicker fibres. When chromosome preparations were processed for SEM without air drying, chromosomes appeared to consist of fairly homogeneous thick fibrous structures measuring about 200 nm in diameter. In relatively condensed chromosomes, these 200 nm fibres appeared to be arranged perpendicular to the long axis of the chromatid. These findings suggest that chromatid spiral structures represent a regularly loosened state of the compactly spiralized 200 nm fibres which in turn consist of spiralized 30 nm fibres.

A novel magnesium-dependent structural transition of chicken erythrocyte chromatin in situ

Lowering magnesium concentration below the value of 1 mM leads to a structural transition of chicken erythrocyte chromatin in situ, which results in a change in its fragmentation by pancreatic DNAase (DNAase I) from double-nucleosome to 100-basepairs mode. At 0.75 mM MgCl2, the pattern of chromatin fragmentation by DNAase I is similar to that generated by DNAase II, and it is further changed at lower concentrations of magnesium. This transition is, at least partly, reversible, and is, presumably, related to packing of the 25-30 nm chromatin fiber into higher-order structures.