Interaction of chromatin with NaCl and MgCl2: Solubility and binding studies,transition to and characterization of the higher-order structure

Chicken erythrocyte chromatin containing histones H1 and H5 was carefully separated into a number of well-characterized fractions. A distinction could be made between chromatin insoluble in NaCl above about 80 mm, and chromatin soluble at all NaCl concentrations. Both chromatin forms were indistinguishable electrophoretically and both underwent the transition from the low salt “10 nm” coil to the “30 nm” higher-order structure solenoid by either raising the MgCl₂ concentration to about 0.3 mm or the NaCl concentration to about 75 mm. The transitions were examined in detail by elastic light-scattering procedures. It could be shown that the 10 nm form is a flexible coil. For the 30 nm solenoid, the assumption of a rigid cylindrical structure was in good agreement with 5.7 nucleosomes per helical turn. However, disagreement of calculated frictional parameters with values derived from quasielastic light-scattering and sedimentation introduced the possibility that the higher-order structure, under these conditions, is more extended, flexible, or perhaps a mixture of structures. Values for density and refractive index increments of chromatin are also given.To understand the interaction of chromatin with NaCl and with MgCl₂, a number of experiments were undertaken to study solubility, precipitation, conformational transitions and binding of ions over a wide range of experimental conditions, including chromatin concentration.     

The fine structure of euchromatin and centromeric heterochromatin in Tenebrio molitor chromosomes

The fine structure of constitutive heterochromatin and euchromatin was compared in electron microscope whole-mount preparations of Tenebrio molitor (Insecta, Coleoptera) spermatocyte nuclei. Tenebrio molitor pachytene chromosomes display extended segments of centromeric heterochromatin and thus are especially suitable for this purpose. When nuclei were incubated in solutions containing different concentrations of NaCl or of MgCl₂, two levels of chromatin fine structures were observed in the euchromatic segments: nucleosome fibers (0.1 mM–20 mM NaCl) and supranucleosomal fibers with 28 nm in diameter (40 mM–100 mM NaCl, 0.2 mM–1.0 mM MgCl₂). The fine structure in the heterochromatic segments was the same as that in the euchromatic segments in all NaCl concentrations and in MgCl₂ concentrations up to 0.4 mM. In higher MgCl₂ concentrations the heterochromatin remained more compact than the euchromatin and consisted of 37-nm-thick fibers in 0.6 mM MgCl₂ and of 65-nm-thick fibers in 1.0 mM MgCl₂. After the 37-nm and the 65-nm fibers had been dispersed in Mg²⁺-free solutions they could be recondensed by incubation in 0.6 mM and 1.0 mM MgCl₂, respectively. It is concluded that a Mg²⁺-sensitive component of the heterochromatin is responsible for the folding of the nucleosome chain to heterochromatin-specific supranucleosomal structures.     

Aggregation of mono- and dinucleosomes into chromatin-like fibers

Three classes of chicken erythrocyte chromatin particles differing in their content of lysine-rich histones and/or spacer DNA have been studied in order to determine their ability to aggregate into complexes resembling those observed in native chromatin. The complexes have been obtained in the presence of MgCl₂ and NaCl and studied by electron microscopy. Mononucleosomes, containing spacer DNA and histones H1 and H5, give rise to thick (about 70 nm) ellipsoidal particles in the presence of 0.5 mM MgCl₂. These particles are disrupted by the addition of small amounts of NaCl (5–20 mM). On the other hand in 0.5 mM MgCl₂ dinucleosomes give rise to regular fibrous complexes of about 40 nm in diameter which are very similar to native chromatin fibers. These complexes are much more stable when NaCl is added. We conclude that for the stability of nucleosomal aggregates, similar to native chromatin fibers, a continuity of DNA structure is not required, but the presence of divalent cations, spacer DNA and lysine-rich histones is essential.     

Comparison of the structure of ribosomal 5S RNA from E. coli and from rat liver using X-ray scattering and dynamic light scattering

The structures of eukaryotic ribosomal 5S RNA from rat liver and of prokaryotic 5S RNA from E. coli (A-conformer) have been investigated by scattering methods. For both molecules, a molar mass of 44,500±4,000 was determined from small angle X-ray scattering as well as from dynamic light scattering. The shape parameters of the two rRNAs, volume V _c, surface O _c, radius of gyration R _s, maximum dimension of the molecule L, thickness D, and cross section radius of gyration R _sq, agree within the experimental error limits. The mean values are V _c=57±3 nm³, O _c=165±10 nm², R _s=3.37±0.05 nm, L=10.8±0.7 nm, D=1.57±0.07 nm, R _sa=0.92±0.01 nm.Identical structures for the E. coli 5S rRNA and the rat liver 5S rRNA at a resolution of 1 nm can be deduced from this agreement and from the comparison of experimental X-ray scattering curves and of experimental electron distance distribution function. The flat shape model derived for prokaryotic and eukaryotic 5S rRNA shows a compact region and two protruding arms. Double helical stems are eleven-fold helices with a mean base pair distance of 0.28 nm. Combining the shape information obtained from X-ray scattering with the information about the frictional behaviour of the molecules, deduced from the diffusion coefficients D _20,w ⁰ =(5.9±0.2)·10^-7 cm²s^-1 and (6.2±0.2)·10^-7 cm²s^-1 for rat liver 5S rRNA and E. coli 5S rRNA, respectively, a solvation shell of about 0.3 nm thickness around both molecules is determined. This structural similarity and the consensus secondary structure pattern derived from comparative sequence analyses suggest that all 5S rRNAs may indeed have conserved essentially the same type of folding of their polynucleotide strands during evolution, despite having very different sequences.     

Synchrotron X-ray scattering study of chromatin condensation induced by monovalent salt: analysis of the small-angle scattering data

Small-angle X-ray scattering experiments were carried out on rat thymus chromatin in "native" and "H1-depleted" states at various NaCl concentrations using synchrotron radiation. From the analysis of cross-sectional Guinier plots, the radius of gyration of the cross section (Rc) and the mass per unit length (Mc) of native chromatin were evaluated. In the absence of NaCl, the cross section of chromatin filament has a radius of gyration of 3.44 nm, suggesting the structure corresponding to the "10 nm" filament. With increasing NaCl concentration, the Rc value increases steeply to 6.74 nm at 5 mM NaCl and then gradually to 8.82 nm at 50 mM NaCl, whereas the Mc value, which is determined relative to that of tobacco mosaic virus (TMV), increases steadily from 1.58 nucleosomes per 10 nm in the absence of NaCl to 7.66 nucleosomes per 10 nm at 50 mM NaCl. However, since calibration with TMV tends to overestimate the Mc value, the actual Mc values may be less than those values. Above about 40 mM NaCl, aggregation of chromatin is suggested. Similar analysis of H1-depleted chromatin confirmed that H1-depleted chromatin takes a more disordered structure than native chromatin at low ionic strength and does not undergo a definite structure change upon further addition of NaCl.     

X-ray scattering of antibodies: the monomeric 8S subunit of human IgM

8S monomeric subunit of a human immunoglobulin M was investigated by small-angle X-ray scattering. The following molecular parameters were determined: radius of gyration 5.9 nm, maximum length 21 nm, hydrated volume 410 nm³ and two radii of gyration of the cross-section: 2.6 and 1.8 nm. A model equivalent in scattering was found and compared with the model for a human IgG also based on small-angle X-ray scattering data. The Cμ2 domain of the IgM obviously has a very loose structure, and the Fab angle of the 8S IgM (90°) is smaller than that of the IgG (134°).     

Studies on the structure of isolated chromatin in three different solvents.

Properties of calf thymus chromatin, prepared by mild procedures, have been studied in various solvents. In 0.2 mM EDTA s-values ranged from 20 to 30 S and intrinsic viscosities from 5 to 24 dl/g. Dialysis against 0.15 M NaCl or 0.2 mM MgCl2 changed these values to 80 to 100 S and 0.2 to 5 dl/g, respectively, indicating an essentially more compact structure. In 0.2 mM EDTA X-ray scattering yielded a cross section diameter of 9 nm, which is associated with the tertiary structure of chromatin fiber (M/L = 21200 Dalton/nm). By dialysis against 0.15 M NaCl or 0.2 mM MgCl2 part of the material spontaneously formed quarterny structures (cross section diameters 25-29 nm). The rest of the material with cross section diameters less than 9 nm is supposed to be more strongly sheared tertiary structure which seems to be unable to form quarterny structure due to artificial conformational changes.     

Interpretation of the X-ray scattering profiles of chromatin at various NaCl concentrations by a simple chain model.

In order to interpret the change in the X-ray scattering profiles from rat thymus chromatin, extensive model calculation was carried out. Chromatin is modelled as a string of subunits (nucleosomes) in which disorder is introduced into the positions of adjacent subunits. Disposition parameters characterizing the arrangement of subunits were estimated for various states of chromatin, so that the main feature of the scattering profiles is described. The result indicated that the structure of chromatin changes, as the NaCl concentration increases, from the extended "beads-on-a string" structure to the condensed helical structure. The latter has an outer diameter of about 26 nm with 3-4 nucleosomes per turn. In the intermediate state, it has a loose helical structure. The estimation of disorder suggested that the arrangement of subunits is appreciably disordered even in the condensed helical filament at 50 mM NaCl. Our model for chromatin condensation seems to support models of the "crossed linker" type.     

Cholinergic ligand-induced affinity changes in Torpedo californica acetylcholine receptor

Measurement of small-angle X-ray scattering from a sample of hyaluronic acid of high molecular weight in 0.05 m HNO₃ gave persistence length plots which agreed in form with theory and led to apparent persistence lengths of from 4 to 6 nm. Similar measurements in 0.2 m NaCl gave plots which deviated somewhat in form from theoretical expectation, but which could be interpreted to give a persistence length of 4 nm in this solvent. Data for intrinsic viscosity [η] as a function of molecular weight were in reasonable agreement with the Yamakawa-Fujii treatment of [η] for the worm-like chain model for a persistence length of about 4 nm in both 0.5 m NaCl and 0.1 m HCl, perhaps slightly higher in the latter. The values of persistence length estimated from [η] depend somewhat on the choice of chain parameters and the method of correction of experimental data to unperturbed solvent conditions. Experimental data for the sedimentation coefficient, while less definitive, were consistent within experimental uncertainty with the same parameters of the worm-like chain model. These calculated results are in substantial agreement with the values derived from small-angle X-ray scattering. A fraction of hyaluronic acid of low molecular weight in 0.05 m HNO₃ gave an estimated molecular weight of 2.7 × 10⁴ and a radius of gyration of 8 nm, in reasonable agreement with expected values based on the worm-like chain model for a persistence length of about 4 nm.     

Small angle X-ray scattering of intact and lysing cell nuclei

X-ray scattering at very low angles has been applied to the study of chromatin structure in intact and lying nuclei. From maxima and minima in the very low angle range, higher order or very large structures could be deduced, the existence of which has not been found in isolated chromatin; up to now, such structures could be demonstrated only be electron-micrographs of whole nuclei. A strong maximum at 0.12 nm^?1 or a shoulder at 0.08 nm^?1 is interpreted as a hollow or solid cylinder with diameter ～ 70 nm; however, another possible explanation, a side by side packing of 30 nm solenoids^1–4 with a distance of 52 nm, cannot be excluded. A shoulder at 0.033 nm^?1 leads to the conclusion that an even larger structure exist in interphase nuclei. A slight minimum at 0.2 nm^?1 is in the range where mildly isolated chromatin has its first order minimum. This accounts for a coil diameter ～ 30 nm. While in intact nuclei these characteristics of the scattering curve have only a low intensity (except the maximum at 0.12 nm^?1 lysing nuclei exhibit much more pronounced maxima.     

Quaternary structure of immunoglobulin m: A model based on small-angle X-ray scattering data

This paper presents some data on a human Waldenström immunoglobulin M.IgM_GAL based on small-angle X-ray scattering data. the IgM_GAL had molecular weight 970 000, volume 1760 nm³, radius of gyration 12 nm and maximum diameter 37 nm. The conclusions from various model calculations are discussed. A flat, star-shaped model is compatible both with X-ray scattering data and electron micrographs.     

Solution structure of human plasma fibronectin as a function of NaCl concentration determined by small-angle X-ray scattering

The structure of human plasma fibronectin in 50 mM Tris-HCl buffer, pH 7.4, containing varying concentrations of NaCl, has been investigated using the small-angle X-ray method.Below 0.3 M NaCl the overall structure of the molecule is disc-shaped; at 0 M NaCl the axial ratio of the disc is about 1:7 and between 0.1 M to 0.3 M it is slightly more asymmetric, with an axial ratio of 1:10.At about 0.3 M NaCl there is a reversible transition to a more open structure, and, from 0.3 M up to 1.1 M NaCl the small-angle X-ray data can be explained by models consisting of ensembles of flexible, non-overlapping, bead-chains generated by a Monte Carlo procedure. Within this concentration range there is a gradual increase in the stiffness of the chains, as well as a decrease in bead radius, which indicates that the molecule becomes more open when the NaCl concentration is increased.The transition to a more open structure is also demonstrated by the average radius of gyration which increases gradually from 8.26 nm at 0 M NaCl to 8.75 nm at physiological or near-physiological conditions, and up to 16.2 nm at 1.1 M NaCl.Abbreviations hpFN human plasma fibronectin - SAXS smallangle X-ray scattering - Tris tris (hydroxymethyl) aminomethane - DTT dithiothreitol - BA benzamidine hydrochloride - PMSF phenylmethylsulfonyl fluoride     

Effect of the cations sodium,potassium and calcium on the interaction of hyaluronate chains: a light scattering and viscometric study

Light scattering and viscometric studies have been carried out on two preparations, A and B, of rooster comb hyaluronate. Sedimentation rate studies have also been performed with A. Light scattering measurements in 0.2 m KCl for preparation A gave a molecular weight of 3.3 × 10⁶ and for B, 1.0 × 10⁶. In (0.1–0.3) M NaCl similar measurements gave a particle weight for A of (4.4–6.4 × 10⁶ and for B (1.7–2.8 × 10⁶. In 0.066 m CaCl₂ molecular weight values of 9.5 × 10⁶ for A and 1.7 × 10⁶ for B were obtained. Thus in the presence of Na⁺ and Ca²⁺ ions aggregates of chains persisted into dilute solution. Measurements by light scattering on A and B in 4 m guanidinium chloride gave values in the same range as those obtained in 0.2 m KCl. Sedimentation rate studies on A gave values of 10.3 Svedbergs in 0.2 m KCl and 12.2 Svedbergs in 0.2 m NaCl and 0.066m CaCl₂. The shear dependence of the viscosity was studied using a conicylindrical viscometer at shear rates between 0.5 and 20 s^?1. Preparation A in 0.2 m KCl and NaCl yielded values for (ν_sp/cc→0 of 5000 and 7100 ml g^?1 respectively in keeping with the tendency to aggregate. The behaviour for preparation B was similar. In 0.066 m CaCl₂ there was a marked dependence of viscosity on shear speed below 10 s^?1 for all concentrations and the value of (ν_sp/c)→0 at 0 s^?1 for preparation A was 7700 ml g^?1 while at a shear rate of 8 s^?1 (ν_sp/c)c→0 ? 5000 ml g ^?1. Similar effects were found for preparation B and the data suggest associations of chains disruptable by weak shear forces. The increase in viscosity with concentration in the presence of 0.066 m CaCl₂ was much less than in the presence of KCl or NaCl, suggesting that the Ca²⁺ had a marked effect on the ”rigidity’ of the molecules in solution. A viscometric titration experiment with Ca^2? showed that a level of 0.02 m CaCl₂ in 0.2 m NaCl was sufficient to produce the change in viscosity presented above and that significant perturbations of the viscosity were present at 0.005?0.01 m CaCl₂.     

X-ray small angle scattering study of chromatin as a function of fiber length

This work investigates the structure of native calf thymus chromatin as a function of fiber length and isolation procedures by using X-ray small angle scattering technique. Two methods of chromatin isolation have been compared in order to better understand the differences reported by various authors in terms of chromatin high order structure. In addition to these experimental results the effects of shearing have also been studied. In order to explain the differences among these chromatin preparations we built several models of chromatin fibers (represented as a chain of spherical subunits) assuming increasing level of condensation at increasing salt concentrations. For all these fiber models the corresponding theoretical X-ray scattering curves have been calculated and these results have been used to explain the influence of fiber length on the scattering profiles of chromatin. The comparison between experimental and theoretical curves confirms that the high molecular weight chromatin-DNA prepared by hypotonic swelling of nuclei (without enzymatic digestion) displays a partially folded structure even at low ionic strength, whereas the low molecular weight chromatin-DNA prepared by a brief nuclease digestion appears very weakly folded at the same ionic conditions.     

Benzamide-inhibitable alterations in spectral properties of chromatin accompany DNA repair in UVC-exposed L5178Y cells

Summary We examined the response of chromatin to increasing NaCl and MgCl₂ concentrations in UVC-irradiated L5178Y (LY) R and S cells, using the spectral index method (Dixon and Burkholder 1985). We have found an alteration in chromatin properties 1 h after UVC-irradiation of repair proficient LY-S cells, but no change in repair deficient LY-R cells. The change was shown as lowered spectral index, indicating that at given Na⁺ and Mg⁺⁺ concentrations (1 or 200 mM NaCl, 0 or 0.5 mM MgCl₂) chromatin from UVC-irradiated LY-S cells was more compact than that from unirradiated ones. Benzamide treatment reversed the effect of UVC-irradiation in LY-S cells and did not change the response pattern of chromatin from LY-R cells or unirradiated LY-S cells.     

Dependence of laser light scattering of DNA on NaCl concentration

We show that the persistence length a of DNA, derived from total intensity laser light scattering of linear Col E₁ DNA and corrected for excluded-volume effects, varies from about 68 nm in 0.005M NaCl to about 40 nm in 0.2M NaCl, leveling off to a constant value (about 27 nm) at high NaCl (1–4M) concentration. These observations do not agree with current views on the effect of electrostatic charge and ionic conditions on DNA dimensions. The apparent diffusion constant D_app, determined from laser light scattering autocorrelation as a function of scattering vector q, at NaCl concentrations 0.005–4M, correctly yields the translational diffusion coefficient D_t at low values of q and scales with molecular dimensions rather than segment length at high values of q; thus, D_app/D_t yields a universal curve when plotted against q²R, where R_g is the radius of the gyration. The sedimentation coefficients s at 0.1 and 0.2M NaCl concentration closely agree with the well-tested empirical relations, and a combination of s, D_t, and the appropriate density increments yield correct molar masses over the whole salt concentration range. Approximate constancy of D_tR_g indicates limited draining in translational flow. We present some observations and thoughts on the regimes in which a dependence of the correlation decay times on q³ rather than q² applies. We conclude that quasielastic laser light scattering discloses little information about dynamics of internal motion of DNA chains.     

Effects of Mg(2+) on activation of the (Na(+) + K(+)-dependent ATPase by Na(+1).

The effects of MgCl₂ on Na activation of three different enzymatic reactions catalyzed by a rat brain (Na + K)-dependent ATPase (adenosine 5′-triphosphatase) were studied. For the Na⁺-dependent ATPase reaction measured with 6 μm ATP, the K_0.5 for Na increased from 0.4 to 1.7 mm as the MgCl₂ concentration was raised from 50 to 2000 μm; the half-maximal effect occurred at a free Mg²⁺ concentration near 0.8 mm. By contrast, with 3 mm ATP and 3 mm MgCl₂ the K_0.5 for Na was again 0.4 mm, but further addition of 2 mm MgCl₂ then had little effect on the K_0.5 for Na. For the Na-dependent phosphorylation of the enzyme, measured with 6 μm ATP, the K_0.5 for Na increased similarly, from 0.2 to 0.8 mM, as the MgCl₂ concentration was raised from 50 to 2000 μm, but for the (Na + K)-dependent ATPase reaction the K_0.5 for Na was 13 mm and increased by only one-third as the MgCl₂ concentration was raised. The K_0.5 for K was also little affected by changes in MgCl₂ concentration. Finally, with 3 mm ATP and 3 mm MgCl₂ the K_0.5 for Na in the (Na + K)-dependent ATPase reaction decreased to 5 mm. These observations are considered in terms of an enzyme having high-affinity and low-affinity substrate sites, with occupancy of the low-affinity sites modifying Na activation differently, depending both on the specific reaction catalyzed and on whether occupancy is by free Mg²⁺ or by Mg-ATP.     

Superhelical DNA studied by solution scattering and computer models

We present here recent results on the structure of superhelical DNA and its changes with salt concentration between 0.01 and 1.5 M NaCl. Scattering curves of two different superhelical DNAs were determined by static light scattering. The measured radii of gyration do not change significantly with salt concentration. Small-angle neutron scattering, together with calculations from a Monte Carlo model, allows to determine the superhelix diameter. Measured and simulated scattering curves agreed almost quantitatively. Experimentally we find that the diameter decreases from 16.0±0.9 nm at 10 mM to 9.0±0.7 nm at 100 mM NaCl. The superhelix diameter from the simulated conformations decreased from 18.0±1.5 nm at 10 mM to 9.4±1.5 nm at 100 mM NaCl. At higher salt concentrations up to 1.5 M NaCl, the diameter stays constant at 9 nm.This revised version was published online in October 2005 with corrections to the Cover Date.     

Conformation of heparin studied with macromolecular hydrodynamic methods and X-ray scattering

The hydrodynamic characteristics of heparin fractions in a 0.2 M NaCl solution have been determined. Experimental values varied over the following ranges: the sedimentation coefficient (at 20.0 °C), 1.3<s₀×10¹³<3.2 s; the Gralen coefficient (sedimentation concentration-dependence parameter), 10<k_s<70 cm³ g^–1; the translational diffusion coefficient, 3.9<D₀×10⁷<15.4 cm² s^–1; the intrinsic viscosity, 7.9<[]<40 cm³ g^–1. Combination of s₀ with D₀ using the Svedberg equation yielded molecular weights in the range 3.9<M×10^–3<37 g mol^–1. The value of the mass per unit length of the heparin molecule, M_L, was determined using the theory of hydrodynamic properties of a weakly bending rod, giving M_L=570±50 g nm^–1 mol^–1. The equilibrium rigidity, Kuhn segment length (A=9±2 nm) and hydrodynamic diameter (d=0.9±0.1 nm) of heparin were evaluated on the basis of the worm-like coil theory without the excluded volume effect, using the combination of hydrodynamic data obtained from fractions of different sizes. Small-angle X-ray scattering for three heparin fractions allowed an estimate for the cross-sectional radius of gyration as 0.43 nm; from the evolution with the macromolecule contour length of the radius of gyration, a value for the Kuhn segment length of 9±1 nm was obtained. A good correlation is thus observed for the conformational parameters of heparin from hydrodynamic and X-ray scattering data. These values describe heparin as a semi-rigid polymer, with an equilibrium rigidity that is essentially determined by a structural component, the electrostatic contribution being negligible in 0.2 M NaCl.Presented at the conference for Advances in Analytical Ultracentrifugation and Hydrodynamics, 8–11 June 2002, Grenoble, France     

Experimental Visualization of Chromoneme as a Higher Level of Chromatin Compactization in the Mitotic Chromosome

We succeeded to visualize the chromoneme or a filamentous chromatin structure, with the mean thickness 0.1–0.2 μm, as a higher level of chromatin compactization in animal and plant cells at different stages of chromosome condensation at mitotic prophase and during chromatid decondensation at telophase. Under the natural conditions, chromoneme elements are not detected in the most condensed chromatin of metaphase chromosomes on ultrathin sections. We studied the ultrastructure and behavior of the chromatin of mitotic chromosomes in situ in cultured mouse L-197 cells under the conditions selectively demonstrating the chromoneme structure of the mitotic chromosomes in the presence of Ca²⁺. Loosely packaged dense chromatin bands, ca. 100 nm in diameter, chromonemes, were detected in chromosome arms in a solution containing 3 mM CaCl₂. When transferred in a hypotonic solution containing 10 mM tris-HCl, these chromosomes swelled, lost the chromoneme level of structure, and rapidly transformed in loose aggregates of elementary DNP fibrils, 30 nm in diameter. After this decondensation in the low ionic strength solution, the chromoneme structure of mitotic chromosomes was restored when they were transferred in a Ca₂₊ containing solution. The morphological characteristics of the chromoneme and pattern of its packaging in the chromosome were preserved. However, when the mitotic cells with chromosomes, in which the chromoneme structure was visualized with the help of 3 mM CaCl₂, were treated with a photosensitizer, ethidium bromide, and illuminate with a light with the wavelength 460 nm, chromatic decondensation under the hypotonic solution was not observed. The chromoneme elements in a stabilized chromatin of the mitotic chromosome preserved specific interconnection and the general pattern of their packaging in the chromatid was also preserved. The chromoneme elements in the chromosomes stabilized by light preserved their density and diameter even in a 0.6 M NaCl solution, which normally leads to chromoneme destruction. An even more rigid treatment of the stabilized chromosomes with a 2 M NaCl solution, which normally fully decondenses the chromosomes, made it possible to detect a 3D reticular skeleton devoid of any axial structures. __________ Translated from Ontogenez, Vol. 36, No. 5, 2005, pp. 323–332. Original Russian Text Copyright ? 2005 by Burakov, Tvorogova, Chentsov.