Low angle x-ray diffraction studies of HeLa metaphase chromosomes: effects of histone phosphorylation and chromosome isolation procedure

To test whether gross changes in chromatin structure occur during the cell cycle, we compared HeLa mitotic metaphase chromosomes and interphase nuclei by low angle x-ray diffraction. Interphase nuclei and metaphase chromosomes differ only in the 30-40-nm packing reflection, but not in the higher angle part of the x-ray diffraction pattern. Our interpretation of these results is that the transition to metaphase affects only the packing of chromatin fibers and not, to the resolution of our method, the internal structure of nucleosomes or the pattern of nucleosome packing within chromatin fibers. In particular, phosphorylation of histones H1 and H3 at mitosis does not affect chromatin fiber structure, since the same x-ray results are obtained whether or not histone dephosphorylation is prevented by isolating metaphase chromosomes in the presence of 5,5'-dithiobis(2- nitrobenzoate) or low concentrations of p-chloromercuriphenylsulfonate (ClHgPhSO3). We also compared metaphase chromosomes isolated by several different published procedures, and found that the isolation procedure can significantly affect the x-ray diffraction pattern. High concentrations of ClHgPhSO3 can also profoundly affect the pattern.     

Nucleosomes in metaphase chromosomes.

Previous studies of the structure of metaphase chromosomes have relied heavily on electron micrography and have revealed the existence of a 10-nm unit fiber that is thought to generate the native 23-30-nm fiber by higher order folding. The structural relationship of these metaphase fibers to the interphase fiber remains obscure. Recent studies on the digestion of interphase chromatin have revealed the existence of a regularly repeating subunit of DNA and histone, the nucleosome that generates the appearance of 10-nm beads connected by a short fiber of DNA seen on electron micrographs. It was therefore of interest to probe the structure of the metaphase chromosome for the presence of nucleosomal subunits. To this end metaphase chromosomes were prepared from colchicine-arrested cultures of mouse L-cells and were subjected to digestion with stayphylococcal nuclease. Comparison of the early and limit digestion products of metaphase chromosomes with those obtained from interphase nuclei indicates that although significant morphologic changes occur within the chromatin fiber during mitosis, the basic subunit structure of the chromatin fiber is retained by the mitotic chromosome.     

Nucleosome packing in interphase chromatin.

Higher-order chromatin fibers (200--300 A in diameter) are reproducibly released from nuclei after lysis in the absence of formalin and/or detergent. Electron microscope analysis of these fibers shows that they are composed of a continuous array of closely apposed nucleosomes which display several distinct packing patterns. Analysis of the organization of nucleosomes within these arrays and their distribution along long stretches of chromatin suggest that the basic 100-A chromatin fiber is not packed into discrete superbeads and is not folded into a uniform solenoid within the native 250-A fiber. Furthermore, because similar higher-order fibers have been visualized in metaphase chromosomes, the existence of this fiber class appears to be independent of the degree of in vivo chromatin condensation.     

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 m 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.     

Higher order structure in metaphase chromosomes

The morphology of metaphase chromosome-derived chromatin fibers released from cells by non-ionic detergent cell lysis in the presence of divalent cations has been studied by electron microscopy. In these preparations the euchromatic arms appear as a series of loops, 200–300 Å in diameter, which are composed of closely-apposed nucleosome arrays. The higher order fiber in chromosomes derived from detergent-lysed cells appears to be less stable than chromatin fibers obtained by mechanical cell lysis. The fiber breaks down into a series of non-uniform nucleosome aggregates (superbeads) and finally to chromatin in a beads-on-a-string morphology upon incubation at 31° for 20 min. These observations allow us to suggest a relationship between uniform thick fibers, superbead-containing fibers, and beads-on-a-string chromatin within metaphase chromosomes.     

Stabilization of chromonema--one of the highest compactization levels--by visible light in the presence of ethidium bromide

This paper deals with the ultrastructure and behavior of interphase chromatin and metaphase chromosomes of L-197 culture cells under experimental conditions, which help to reveal the chromonemal level of chromosomal structure after the treatment of living cells with 0.1% Triton X-100 and 3 mM CaCl2. In these conditions, the chromonemata can be seen as dense chromatin fibers with thickness about 100 nm. Such chromosomes, whose chromonemal substructure after the treatment with hypotonic solution (10 mM Tris-HCl), look like loose chromosomal bodies composed of elementary 30 nm DNP fibrils. On the other hand, if chromosomes, in which chromonemal levels were revealed by 3 mM CaCl2, were treated with etidium bromide and then illuminated by light with length wave about 460 nm, no chromosomal decondensation in hypotonic conditions is observed. Chromonemata in chromosomes stabilized by light retain their density and dimensions. It is very important that chromonemata in stabilizated chromatin of metaphase chromosome keep specific connections between themselves and also general trend in their composition inside the chromosome. Thus, we have found conditions for observation of chromonemal elements in metaphase chromosome, providing the possibility for future three-dimensional investigation of chromonema packing in mitotic chromosomes.     

Assembly of chromatin fibers into metaphase chromosomes analyzed by transmission electron microscopy and scanning electron microscopy.

The higher-order assembly of the approximately 30 nm chromatin fibers into the characteristic morphology of HeLa mitotic chromosomes was investigated by electron microscopy. Transmission electron microscopy (TEM) of serial sections was applied to view the distribution of the DNA-histone-nonhistone fibers through the chromatid arms. Scanning electron microscopy (SEM) provided a complementary technique allowing the surface arrangement of the fibers to be observed. The approach with both procedures was to swell the chromosomes slightly, without extracting proteins, so that the densely-packed chromatin fibers were separated. The degree of expansion of the chromosomes was controlled by adjusting the concentration of divalent cations (Mg2+). With TEM, individual fibers could be resolved by decreasing the Mg2+ concentration to 1.0-1.5 mM. The predominant mode of fiber organization was seen to be radial for both longitudinal and transverse sections. Using SEM, surface protuberances with an average diameter of 69 nm became visible after the Mg2+ concentration was reduced to 1.5 mM. The knobby surface appearance was a variable feature, because the average diameter decreased when the divalent cation concentration was further reduced. The surface projections appear to represent the peripheral tips of radial chromatin loops. These TEM and SEM observations support a "radial loop" model for the organization of the chromatin fibers in metaphase chromosomes.     

Linker histones: conformational changes and the role in the structural organization of chromatin

Histones, linker histones of the H1 family, their postsyntetic modifications, DNA-histone H1 interaction are reviewed. A question of protein change in spermatogenesis at the formation of inactive nucleus with high degree of DNA density is considered. Special attention was paid to sperm-specific histones of the H1 family of sperm cells. Their role in organization of high-order chromatin structure of sperm cells is discussed. Also, results of different studies on the structural organization of chromatin (nucleosomes, 30-nm fibers, chromatin loops and metaphase chromosomes) are discussed.     

Self-assembly of thin plates from micrococcal nuclease-digested chromatin of metaphase chromosomes

The three-dimensional organization of the enormously long DNA molecules packaged within metaphase chromosomes has been one of the most elusive problems in structural biology. Chromosomal DNA is associated with histones and different structural models consider that the resulting long chromatin fibers are folded forming loops or more irregular three-dimensional networks. Here, we report that fragments of chromatin fibers obtained from human metaphase chromosomes digested with micrococcal nuclease associate spontaneously forming multilaminar platelike structures. These self-assembled structures are identical to the thin plates found previously in partially denatured chromosomes. Under metaphase ionic conditions, the fragments that are initially folded forming the typical 30-nm chromatin fibers are untwisted and incorporated into growing plates. Large plates can be self-assembled from very short chromatin fragments, indicating that metaphase chromatin has a high tendency to generate plates even when there are many discontinuities in the DNA chain. Self-assembly at 37°C favors the formation of thick plates having many layers. All these results demonstrate conclusively that metaphase chromatin has the intrinsic capacity to self-organize as a multilayered planar structure. A chromosome structure consistent of many stacked layers of planar chromatin avoids random entanglement of DNA, and gives compactness and a high physical consistency to chromatids.     

Cell cycle-specific changes in the ultrastructural organization of prematurely condensed chromosomes

Prematurely condensed chromosomes (PCC) of HeLa cells synchronized in different phases of the cell cycle were analyzed by high-resolution scanning electron microscopy. The purpose of this study was to examine changes in the arrangement of the basic 30-nm chromatin fiber within interphase chromosomes associated with progression through the cell cycle. These studies revealed that highly condensed metaphase chromosomes and early G1-PCC consisted of tightly packed looping fibers. Early to mid G1-PCC were more extended and exhibited gyres suggestive of a despiralized chromonema. Further attenuation of PCC during progression through G1 was associated with a gradual transition from packed looping fibers to single extended longitudinal fibers. This process occurs prior to the initiation of DNA synthesis which appears to be localized within single longitudinal fibers. Following replication of a chromosome segment, extended longitudinal fibers were rapidly reorganized into packed looping fiber clusters concomitant with the formation of a multifibered chromosome axis. This results in the characteristic “pulverized” appearance of S-PCC when viewed by light microscopy. Subsequently, adjacent looping fiber domains coalesce, resulting in the uniformly packed, looping fiber arrangement observed in G2-PCC. Spiralization of the chromonema during the G2-mitotic transition results in the formation of highly compact metaphase chromosomes.     

Spermiogenesis and chromatin condensation in the common tree shrew, <Emphasis Type="Italic">Tupaia glis</Emphasis>

We have investigated the cellular characteristics, especially chromatin condensation and the basic nuclear protein profile, during spermiogenesis in the common tree shrew, Tupaia glis. Spermatids could be classified into Golgi phase, cap phase, acrosome phase, and maturation phase. During the Golgi phase, chromatin was composed of 10-nm and 30-nm fibers with few 50-nm to 60-nm knobby fibers. The latter were then transformed into 70-nm knobby fibers during the cap phase. In the acrosome phase, all fibers were packed into the highest-order knobby fibers, each about 80–100 nm in width. These chromatin fibers became tightly packed in the maturation phase. In a mature spermatozoon, the discoid-shaped head was occupied by the acrosome and completely condensed chromatin. H3, the core histone, was detected by immunostaining in all nuclei of germ cell stages, except in spermatid steps 15–16 and spermatozoa. Protamine, the basic nuclear protein causing the tight packing of sperm chromatin, was detected by immunofluorescence in the nuclei of spermatids at steps 12–16 and spermatozoa. Cross-immunoreactivity of T. glis H3 and protamine to those of primates suggests the evolutionary resemblance of these nuclear basic proteins in primate germ cells. This work was supported by the Thailand Research Fund (Senior Research Fellowship to Prof. Prasert Sobhon).     

High concentration of DNA in condensed chromatin.

The lengths of the DNA molecules of eukaryotic genomes are much greater than the dimensions of the metaphase chromosomes in which they are contained during mitosis. From this observation it has been generally assumed that the linear packing ratio of DNA is an adequate measure of the degree of DNA compaction. This review summarizes the evidence suggesting that the local concentration of DNA is more appropriate than the linear packing ratio for the study of chromatin condensation. The DNA concentrations corresponding to most of the models proposed for the 30-40 nm chromatin fiber are not high enough for the construction of metaphase chromosomes. The interdigitated solenoid model has a higher density because of the stacking of nucleosomes in secondary helices and, after further folding into chromatids, it yields a final concentration of DNA that approaches the experimental value found for condensed chromosomes. Since recent results have shown that metaphase chromosomes contain high concentrations of the chromatin packing ions Mg2+ and Ca2+, it is discussed that dynamic rather than rigid models are required to explain the condensation of the extended fibers observed in the absence of these cations. Finally, considering the different lines of evidence demonstrating the stacking of nucleosomes in different chromatin complexes, it is suggested that the face-to-face interactions between nucleosomes may be the driving force for the formation of higher order structures with a high local concentration of DNA.     

Neutron diffraction of chromatin in interphase nuclei and metaphase chromosomes

We have used neutron diffraction to study chromatin structure in interphase nuclei and metaphase chromosomes as a function of decreasing ion concentration. Aliquots of a suspension of rat liver nuclei prepared in a polyamine-free buffer were washed in buffers of 1/3, 1/6 and 1/12 if the original concentration of monovalent and divalent cations (40 mM KCl; 20 mM NaCl; 1.2 mM MgCl2). After the first dilution step (1/1 to 1/3), only small changes occurred in the diffraction pattern. They can be interpreted by a loosening of the original structure, i.e. by the formation of isolated buffer-filled spaces with an overall size of the order of 35-45 nm. Drastic changes in the diffraction pattern were observed, however, when the nuclei were washed in the more diluted buffers (1/6 and 1/12). The profiles of the distances distribution functions indicate the formation of supranucleosomal particles with an overall diameter of 40-50 nm. The compact chromatin structure disassembled directly into these fundamental structural units. Structural transformations in the Chinese hamster ovary metaphase chromosomes were induced by diminishing the Ca2+ ion concentration of the buffer from originally 3.0 mM to 0.3 mM and/or by increasing the pH value of the buffer from originally 7.0 up to 8.0. The neutron diffraction patterns remained essentially unchanged during these treatments, i.e. the decondensation of the chromosomes as observed in the light microscope is not accompanied by disassembly at the ultrastructural level between 2 nm and 150 nm.     

Physical constraints in the condensation of eukaryotic chromosomes. Local concentration of DNA versus linear packing ratio in higher order chromatin structures

The local concentration of DNA in metaphase chromosomes of different organisms has been determined in several laboratories. The average of these measurements is 0.17 g/mL. In the first level of chromosome condensation, DNA is wrapped around histones forming nucleosomes. This organization limits the DNA concentration in nucleosomes to 0. 3-0.4 g/mL. Furthermore, in the structural models suggested in different laboratories for the 30-40 nm chromatin fiber, the estimated DNA concentration is significantly reduced; it ranges from 0.04 to 0.27 g/mL. The DNA concentration is further reduced when the fiber is folded into the successive higher order structures suggested in different models for metaphase chromosomes; the estimated minimum decrease of DNA concentration represents an additional 40%. These observations suggest that most of the models proposed for the 30-40 nm chromatin fiber are not dense enough for the construction of metaphase chromosomes. In contrast, it is well-known that the linear packing ratio increases dramatically in each level of DNA folding in chromosomes. Thus, the consideration of the linear packing ratio is not enough for the study of chromatin condensation; the constraint resulting from the actual DNA concentration in metaphase chromosomes must be considered for the construction of models for condensed chromatin.     

Structure of chromatin and chromosomes in preparations of interphase nucleus derivatives, prepared by removal of the nucleuar envelopes. II. Structure of chromatin and associations of chromosomes in stretched amembranous nuclei and mitotic figures]

Preparations of surface stretched amembranous nuclei and mitotic figures were used for revealing the high order nuclear and chromosomal structures. The preparations were obtained by dropping amembraneous nuclei and mitotic figures suspension in methanol-glacial acetic acid mixture (3:1) on wetted superclean slides. Amembraneous nuclei and mitotic figures were isolated from intact murine and human cells (lines L1210, SK-UT-1B, PHA-stimulated lymphocytes) by means of their 1-5 min prefixational capillary pipetting with freshly prepared 0.018-0.06% Triton X-100 solution in the conditional cultural medium. Stretched amembraneous nuclei and mitotic figures had no features of induced chromatin dispersion and compaction. Stretched interphase amembraneous nuclei showed spatially separated individual structures (thin chromatin fibres, nucleoli, intranuclear bodies), polymorphous pattern of perinucleolar chromatin aggregation and episodically expressed beaded thick chromatin fibres and a chromocenter. The chromomeric pattern of the spread chromosomes of mitotic figures was quite similar but hardly identical with that of G-banding. The stretched prometaphase mitotic figures in all tested cell types always contained loose "residual" nucleoli looking like typical prophase nucleoli as concerns their shape and number per cell (mitotic figure). The majority of chromosomes of stretched mitotic figures and of prophase amembraneous nuclei were attached to the nucleolar material. All tested cell lines showed almost the same variation in number of nucleolus-attached chromosomes, per both prophase amembraneous nucleus and prometaphase mitotic figure. Some chromosomes of stretched mitotic figures were colocated with "residual" nucleoli and looked shortened and strongly condensed. Other chromosomes, locally associated with "residual" nucleoli, were straight and oriented radially to these. Mutual chromosomal arrangements in mitotic cells on smears and in stretched mitotic figures were analogous. Equatorial plates from PBS-washed SK-UT-1B cells displayed a better stretching capacity than those from untreated cells. In the former case metaphase chromosomes were seen more uniformly stretched and well identified after GTG-banding procedure. The number of interchromosomal (mainly telomere-telomeric and telomere-centromeric) connections per stretched mitotic figure (or per stretched prophase amembraneous nucleus) was minimum in late prometaphase, maximum in prophase and early prometaphase, and intermediate in metaphase. The obtained data are discussed in terms of topology and longitudinal heterogeneity of mitotic chromosomes.     

Proteome analysis of human metaphase chromosomes

DNA is packaged as chromatin in the interphase nucleus. During mitosis, chromatin fibers are highly condensed to form metaphase chromosomes, which ensure equal segregation of replicated chromosomal DNA into the daughter cells. Despite >1 century of research on metaphase chromosomes, information regarding the higher order structure of metaphase chromosomes is limited, and it is still not clear which proteins are involved in further folding of the chromatin fiber into metaphase chromosomes. To obtain a global view of the chromosomal proteins, we performed proteome analyses on three types of isolated human metaphase chromosomes. We first show the results from comparative proteome analyses of two types of isolated human metaphase chromosomes that have been frequently used in biochemical and morphological analyses. 209 proteins were quantitatively identified and classified into six groups on the basis of their known interphase localization. Furthermore, a list of 107 proteins was obtained from the proteome analyses of highly purified metaphase chromosomes, the majority of which are essential for chromosome structure and function. Based on the information obtained on these proteins and on their localizations during mitosis as assessed by immunostaining, we present a four-layer model of metaphase chromosomes. According to this model, the chromosomal proteins have been newly classified into each of four groups: chromosome coating proteins, chromosome peripheral proteins, chromosome structural proteins, and chromosome fibrous proteins. This analysis represents the first compositional view of human metaphase chromosomes and provides a protein framework for future research on this topic.     

Structure of metaphase chromosomes: a role for effects of macromolecular crowding

In metaphase chromosomes, chromatin is compacted to a concentration of several hundred mg/ml by mechanisms which remain elusive. Effects mediated by the ionic environment are considered most frequently because mono- and di-valent cations cause polynucleosome chains to form compact ~30-nm diameter fibres in vitro, but this conformation is not detected in chromosomes in situ. A further unconsidered factor is predicted to influence the compaction of chromosomes, namely the forces which arise from crowding by macromolecules in the surrounding cytoplasm whose measured concentration is 100-200 mg/ml. To mimic these conditions, chromosomes were released from mitotic CHO cells in solutions containing an inert volume-occupying macromolecule (8 kDa polyethylene glycol, 10.5 kDa dextran, or 70 kDa Ficoll) in 100 μM K-Hepes buffer, with contaminating cations at only low micromolar concentrations. Optical and electron microscopy showed that these chromosomes conserved their characteristic structure and compaction, and their volume varied inversely with the concentration of a crowding macromolecule. They showed a canonical nucleosomal structure and contained the characteristic proteins topoisomerase IIα and the condensin subunit SMC2. These observations, together with evidence that the cytoplasm is crowded in vivo, suggest that macromolecular crowding effects should be considered a significant and perhaps major factor in compacting chromosomes. This model may explain why ~30-nm fibres characteristic of cation-mediated compaction are not seen in chromosomes in situ. Considering that crowding by cytoplasmic macromolecules maintains the compaction of bacterial chromosomes and has been proposed to form the liquid crystalline chromosomes of dinoflagellates, a crowded environment may be an essential characteristic of all genomes.     

Biochemical and cytological studies of bleomycin actions on chromatin and chromosomes

Interaction of bleomycin with nuclei isolated from a variety of mammalian cells resulted in the release of nucleosomes. When isolated mononucleosomes (core plus linker) were re-treated with bleomycin, no further degradation of DNA occurred. The results suggest that the bleomycin cleavage sites in chromatin are present only in the linker region and that there are probably only one or two cleavage sites per linker. The repeat lengths of nucleosomal DNA released by bleomycin from nuclei of different species are different; this variability is considered to reflect the length of the linker. Incorporation of BrdU into DNA did not alter the bleomycin action on nucleosomes. When mitotic cells were held at metaphase for a prolonged period, bleomycin caused a gradual disintegration of chromosomes, although the bleomycin cleavage sites in metaphase chromosomes were found to be the same as those in interphase nuclei.