Reinterpretation of Linear Dichroism of Chromatin Supports a Perpendicular Linker Orientation in the Folded State

Abstract

We present a reinterpretation of linear dichroism data for the salt induced condensation of chromatin. A conflict between electric and flow linear dichroism data for identical chromatin samples, studied at varying degrees of Mg²⁺ induced folding, can be solved if the orientation in electric fields is mainly determined through the polarization of counter ions along the linker parts, whereas the orientation in flow is governed by the hydrodynamical response of the entire chromatin fiber. The orientation of a chromatin fiber in an electric field would then depend on the linker tilt angle so that at an angle larger than 55° the fiber would tend to orient perpendicular to the applied field. The different orientation distributions obtained with the two methods of alignment may in this way provide extra information about the structure and folding of chromatin.     

Structure of hyperacetylated chromatin: light scattering and flow linear dichroism study

Cation-induced folding of 10 nm chromatin filament to 30 nm fiber was studied with hyperacetylated chromatin using light scattering at 90 degrees and flow linear dichroism. Acetylated chromatin folded in a way indistinguishable from that of the control chromatin: both the compactness of chromatin and the orientation of nucleosomes relative to the fiber axis were identical at a given salt concentration.     

Higher order folding of chromatin is induced in different ways by monovalent and by bivalent cations

The condensation of the 10 nm chromatin filament in the 30 nm fiber by monovalent cations, polyamines and bivalent cations was studied with light scattering at 90 degrees and flow linear dichroism methods. It was found that monovalent cation- and polyamine-induced folding was a two-step process: a precondensation, when a rotation of nucleosomes takes place only, and a condensation step without changes in nucleosome orientation. Divalent cations affected the structure of chromatin in one step only -- condensation of the chromatin filament being accompanied by nucleosome reorientation.     

A triple helix model for the structure of chromatin fiber

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

Optical anisotropy of chromatin. Flow linear dichroism and electric dichroism studies

The optical anisotropy of chromatin with different length of the linker DNA isolated from a variety of sources (Frend erythroleukemia cells, calf thymus, hen erythrocytes and sea urchin sperm) has been studied in a large range of mono- and bivalent cations concentrations by the use of flow linear dichroism (LD) and electric dichroism. We have found that all chromatins studied displayed negative LD values in the range of 0.25 mM EDTA - 2 mM NaCl and close positive values in the range of 2-100 mM NaCl. Mg2+ cations, in contrast to Na+ cations, induce optically isotropic chromatin fibers. All chromatin samples exhibit positive form effect amounting to 5-10% of LD amplitude observed at 260 nm. This form effect is determined by the anisotropic scattering of polarized light by single chromatin fibers. The conformational transition at 2 mM NaCl leads to the distortion of chromatin filament structure. The reversibility of this distortion depends on the length of the linker DNA - for chromatins with the linker DNA of 10-30 b.p. it is parially reversible, while for preparations with longer linker DNA it is irreversible. Relatively low electric field does not affect chromatin structure, while higher electric field (more than 7 kV/cm) distorts the structure of chromatin. Presented results explain the contradictory data obtained by electrooptical and hydrooptical methods.     

Higher order structure of chromatin: orientation of nucleosomes within the 30 nm chromatin solenoid is independent of species and spacer length

We have used electric dichroism to study the arrangement of nucleosomes in 30 nm chromatin solenoidal fibers prepared from a variety of sources (CHO cells, HeLa cells, rat liver, chicken erythrocytes, and sea urchin sperm) in which the nucleosome spacer length varies from approximately 10 to approximately 80 bp. Field-free relaxation times are consistent only with structures containing 6 +/- 1 nucleosomes for every 11 nm of solenoidal length. With very few assumptions about the arrangement of the spacer DNA, our dichroism data are consistent with the same orientation of the chromatosomes for every chromatin sample examined. This orientation, which maintains the faces of the radially arranged chromatosomes inclined at an angle between 20 degrees-33 degrees to the solenoid axis, thus appears to be a general structural feature of the higher order chromatin fiber.     

Optical Anisotropy of Chromatin. Flow Linear Dichroism and Electric Dichroism Studies

Abstract

The optical anisotropy of chromatin with different length of the linker DNA isolated from a variety of sources (Frend erythroleukemia cells, calf thymus, hen erythrocytes and sea urchin sperm) has been studied in a large range of mono- and bivalent cations concentraitons by the use of flow linear dichroism (LD) and electric dichroism.

We have found that all chromatins studied displayed negative LD values in the range of 0.25 mM EDTA—2 mM NaCl and close positive values in the range of 2–100 mM NaCl. Mg²⁺ cations, in contrast to Na⁺ cations, induce optically isotropic chromatin fibers. All chromatin samples exhibit positive form effect amounting to 5–10% of LD amplitude observed at 260 nm. This form effect is determined by the anisotropic scattering of polarized light by single chromatin fibers.

The conformational transition at 2 mM NaCl leads to the distortion of chromatin filament structure. The reversibility of this distortion depends on the length of the linker DNA—for chromatins with the linker DNA of 10–30 b.p. it is parially reversible, while for preparations with longer linker DNA it is irreversible.

Relatively low electric field does not affect chromatin structure, while higher electric field (more than 7 kV/cm) distorts the structure of chromatin.

Presented resutls explain the contradictory data obtained by electrooptical and hydrooptical methods.     

Interaction of benz[a]pyrene diol epoxide with chromatin studied by flow linear dichroism

Chromatin isolated from Ehrlich ascites cells was incubated with the tumourigenic compound (+)-7 beta,8 alpha-dihydroxy-9 alpha,10 alpha-epoxy-7,8,9,10- tetrahydrobenz[a]pyrene [(+)-anti-BPDE] at low ionic strength and the modified chromatin was analysed using flow linear dichroism (LD). The results confirm that (+)-anti-BPDE preferentially binds to the DNA in the linker regions, and furthermore show that the long axis of the bound pyrenyl chromophore is oriented parallel or close to parallel to the average orientation of the chromatin fiber axis. The data indicate that the binding geometry of (+)-anti-BPDE in chromatin is similar to that in pure DNA and deoxyguanosine-containing double-helical oligonucleotides.     

Linear dichroism of chromatin fibers

The optical anisotropy of chromatin with different length of the linker DNA isolated from a variety of sources (Friend erythroleukemia cells, calf thymus, hen erythrocytes and sea urchin sperm) has been studied in a large range of mono- and bivalent cations by the use of flow linear dichroism and electric dichroism. We have found that all chromatins studied displayed negative LD values in the range of 0.25 mM EDTA--2 mM NaCl and close positive values in the range of 2-100 mM NaCl. Mg2+ cations, in contrast to Na+ cations, induce optically isotropic chromatin fibers. All chromatin samples exhibit positive form effect amounting to 5-10% of LD amplitude observed at 260 nm. This form effect is determined by the anisotropic scattering of polarized light by single chromatin fibers. The conformational transition at 2 mM NaCl leads to the distortion of chromatin filament structure. The reversibility of this distortion depends on the length of the linker DNA--for chromatins with linker DNA 10-30 b.p. it is partially reversible, while for preparations with longer linker DNA it is irreversible. Relatively low electric fields do not have an effect on chromatin structure, while higher electric fields (more than 7 kV/cm) distort the structure of chromatin.     

Structural transitions of chromatin at low salt concentrations: a flow linear dichroism study

We have studied the structure of nuclease-solubilized chromatin from Ehrlich ascites cells by flow linear dichroism (LD) using the anisotropic absorption of the DNA bases and of two intercalated dyes, ethidium bromide and methylene blue. It is confirmed that intercalation occurs preferentially in the linker part of the chromatin fiber, at binding ratios (dye/base) below 0.020. Using this information, we determined the orientation of the linker in relation to the average DNA organization in chromatin. The LD measurements indicate that the conformation of chromatin is considerably changed in the ionic strength interval 0.1-10 mM NaCl: with increasing salt concentration, the LD of the intrinsic DNA base absorption changes signs, from negative to positive, at approximately 2.5 mM NaCl. The LD of the intercalated dyes also changes signs, however, at a somewhat higher salt concentration. The results are analyzed in terms of possible allowed combinations of tilt angles of nucleosomes and pitch or tilt angles of linker DNA sections relative to the fiber axis, at different salt concentrations in the interval 0.1-10 mM NaCl. Two models for the salt-induced structural change of chromatin are discussed.     

Electric dichroism of chromatin

The linear dichroism of sheared calf thymus chromatin, oriented in solution by a pulsed electric field, has been measured. The limiting value of this dichroism is considerably less negative than that of calf thymus DNA, but does not approach the positive values predicted if chromatin were uniformly supercoiled in the manner suggested by X-ray studies. The decay of the dichroism of chromatin, after termination of the electric pulse, is similar to that of DNA, indicating that chromatin retains a high degree of chain flexibility. These data, as well as previous flow dichroism studies (Ohba, 1966; Smart &; Bonner, 1971), suggest that chromatin is not predominantly supercoiled in solutions of low ionic strength. Evidence for a structurally heterogeneous model for chromatin is discussed.     

The superstructure of chromatin and its condensation mechanism

Electric dichroism and X-ray scattering measurements on solutions of uncondensed and condensed chicken erythrocyte chromatin were interpreted on the basis of model calculations. Information about the state of uncondensed fibers in the conditions of electric dichroism measurements was obtained from scattering patterns recorded as a function of pH, in the presence of spermine and at very low monovalent cation concentrations. Electric dichroism measurements on a complex of uncondensed chromatin with methylene blue were made to determine the contribution of the linker and of the nucleosomes to the total dichroism.A new approach to calculate the dichroism from realistic structural models, which also yields other structural parameters (radius of gyration, radius of gyration of the cross-section, mass per unit length) was used. Only a restricted range of structures is simultaneously compatible with all experimental results. Further, it is shown that previous interpretations of dichroism measurements on chromatin were in contradiction with X-ray scattering data and failed to take into account the distribution of orientation of the nucleosomes in the fibers. When this is done, it is found that the linker DNA in chicken erythrocyte and sea urchin chromatin must run nearly perpendicularly to the fibre axis. Taken together with the dependence of the fibre diameter on the linker length, these results provede the strongest evidence hitherto available for a model in which the linker crosses the central part of the fibre.     

Polarized fluorescence in an electric field: comparison with other electrooptical effects for rodlike fragments of DNA and the problem of the saturation of the induced moment in polyelectrolytes

Electrical birefringence, electrical dichroism and polarisation of fluorescence in an electric field experiments have been performed at high fields on sonicated fragments of DNA labelled with Acridine Orange. The latter electrooptical effect gives access to the field dependence of the fourth moment of the orientation function while the two former give access to the field dependence of the second moment. The origin of the large departure from an E2 dependence at rather low degrees of orientation is extensively discussed. Following a suggestion of Shirai on the calculation of orientational averages for a saturated induced moment, we can show that this model rationalizes the existence of a linear E dependence of the orientation factor at intermediate fields and explains very well our experimental results. When applied to previous dichroic data at higher fields it shows that the low value of the dichroism at saturation introduced to fit with other models, in contradiction with the absence of base tilting in the B form of DNA, is not required for a quantitative fit with this new orientation mechanism. The transition from an E2 dependence at low fields to an E dependence at intermediate fields gives an estimate of the field required for the saturation of the ionic polarisation E approximately 6 kV/cm.     

Electrooptical analysis of alpha-chymotrypsin at physiological salt concentration

The electric dichroism of alpha-chymotrypsin has been measured in a buffer containing 0.1 M Na(+), 10 mM Mg(2+) and 25 mM Tris-cacodylate pH 7.2. The reduced dichroism as a function of the electric field strength can be represented by the orientation function for permanent dipoles and is not consistent with the orientation function for induced dipoles. After correction for the internal directing field, the dipole moment is 1.1 x 10(-27) Cm (+/- 10%), corresponding to 340 D, at 20 degrees C. The assignment of the permanent dipole moment is confirmed by the shape of the dichroism rise curves, which require two exponentials with amplitudes of opposite sign for fitting. The dichroism decay time constants measured in the range of temperatures between 2 and 30 degrees C indicate a temperature induced change of the structure, which is equivalent to an increase of the hydrodynamic radius from r = 26.6 A at 2 degrees C to 28.5 A at 30 degrees C. Our results demonstrate that electrooptical investigations of proteins with a high time resolution can be extended to physiological salt concentrations without serious problems by use of appropriate instruments.     

Electric dichroism and bending amplitudes of DNA fragments according to a simple orientation function for weakly bent rods

The linear dichroism is calculated for DNA fragments in their thermal bending equilibrium. These calculations are given for relatively short fragments, where bent molecules can be described by an arc model. Using the measured value of 350 A for the persistence length, the limit dichroism (corresponding to complete alignment) decreases due to thermal bending, e.g., for a fragment with 100 base pairs to 80% of the value expected for straight molecules. Thermal bending should lead to a strong continuous decrease of the dichroism with increasing chain length, which is not observed, however, in electric dichroism experiments due to electric stretching. The influence of the electric field on the bending equilibrium is described by a contribution to the bending energy, which is calculated from the movement of charge equivalents against the potential gradient upon bending. The charge equivalents, which are assigned to the helix ends, are derived from the dipole moments causing the stationary degree of orientation. By this procedure the energy term inducing DNA stretching is given for induced, permanent, and saturating induced dipole models without introduction of any additional parameter. The stationary dichroism at a given electric field strength is then calculated according to an arc model by integration over all angles of orientation of helix axes or chords with respect to the field vector, and at each of these angles the contribution to the dichroism is calculated by integration over all helices with different degrees of bending. Orientation functions obtained by this procedure are fitted to dichroism data measured for various restriction fragments. Optimal fits are found for an induced dipole model with saturation of the polarizability. The difference between orientation functions with and without electric stretching is used to evaluate dichroism bending amplitudes. Both chain length and field strength dependence of bending amplitudes are consistent with experimental amplitudes derived from the dichroism decay in low salt buffers containing multivalent ions like Mg2+, spermine, or [CoNH3)6]3+. Bending amplitudes can be used to evaluate the persistence length from electrooptical data obtained for a single DNA restriction fragment. Bending and stretching effects are considerable already at relatively low chain length, and thus should not be neglected in any quantitative evaluation of experimental data.     

Electric properties and structure of DNA-restriction fragments from measurements of the electric dichroism

The electric dichroism of 17 homogeneous DNA fragments, ranging in size from 43 to 4362 base-pairs, has been analyzed in high electric fields. The orientation of the small fragments can be described in terms of an induced dipole moment, whereas the large fragments are oriented according to a constant dipole mechanism. In the intermediate size range, DNA orients according to an induced dipole mechanism at low field strengths and according to a constant dipole mechanism at high field strengths. From these observations we propose an orientation mechanism with a saturating induced dipole. The induced dipole observed at low field strengths is saturated at a field strength Eo within a transition range Em to give a constant dipole moment at high field strengths. These parameters together with the polarizability and the limit reduced dichroism are evaluated by a least-squares analysis of the experimental data. Eo and Em are found to decrease with increasing chain length from Eo approximately 40 kV/cm (Em approximately 14 kV/cm) at 65 base-pairs to 10 kV/cm (6 kV/cm) at 194 base-pairs. The polarizability is found to increase with the square of the chain length, whereas the saturated dipole increases with chain length N at low N and goes to a limit value at high N. The temperature dependence of the orientation parameters is found to be very small. The values obtained for the limit dichroism are between -1.0 and -1.3 for chain lengths between 60 and 1000 base-pairs, whereas values around -1.4 are observed at chain lengths greater than 1000 base-pairs. These data indicate that electric fields extend the contour of DNA strands at high chain lengths from a weakly bent to a more linear form. The variations of the limit dichroism observed for short fragments suggest sequence-dependent differences in the secondary structure of the helix. The experimental results are compared with numerical calculations based on simple polyelectrolyte models. For short fragments the magnitude of several electrochemical parameters can be adequately explained by a polarization of the ion cloud around the DNA molecules. However, these polyelectrolyte models do not adequately describe the observed chain length dependence of the orientation phenomena.     

Electric and flow linear dichroism of unfolded and condensed chromatin: a comparative study at low and intermediate ionic strength

Identical samples containing polynucleosomal chains of chicken erythrocyte (CE) and Ehrlich ascites tumour (EA) chromatin were studied under various ionic conditions with regard to electric linear dichroism (ELD) and flow linear dichroism (FLD). Both orientation techniques consistently confirmed that, in the limit of very low ionic strength and in the absence of multivalent cations, the reduced linear dichroism of chromatin is negative in the DNA-base absorption band, as expected for an extended zig-zag polynucleosomal conformation. With increasing electrolyte content, both ELD and FLD decreased drastically in amplitude, but in contrast to the ELD which remains negative in an intermediate range of low ionic strength (0.1-0.5 mM Mg2+) the FLD changes sign and becomes positive. The ELD and FLD amplitudes decrease with higher Mg2+ concentrations and FLD even vanishes in the region of 0.2-0.4 mM; both signals are positive above 0.4-0.5 mM Mg2+. The origin of the dissimilarities between ELD and FLD observations is still not fully understood. Several possibilities are considered: ELD signals are more influenced than FLD by the presence of short chromatin chains, nucleosomes and small pieces of naked DNA, while FLD is more susceptible to the presence of large, easily orientable, scattering aggregates. Different preferred orientation directions of the chromatin fibre with respect to electric and hydrodynamic fields may also be involved. Finally, FLD and ELD probably "see" different features of the chromatin structure.     

The role of histone H1 and non-structured domains of core histones in maintaining the orientation of nucleosomes within the chromatin fiber

Calf thymus chromatin was digested with trypsin and the structural alterations which occurred were followed by flow linear dichroism. After a sharp initial increase, the amplitude of the positive signal gradually decreased followed by a change of the sign of the dichroism and further increase of the negative signal up to a plateau. These changes of the dichroism were compared to the respective changes in the histone pattern. It was shown that the positive dichroism of chromatin did not depend on the condensation state of chromatin, and that the orientation of the nucleosomes along the chromatin fiber was maintained by the globular domain of H1 and the non-structured parts of core histones.     

Electric and Flow Linear Dichroism of Unfolded and Condensed Chromatin: A Comparative Study at Low and Intermediate Ionic Strength

Abstract

Identical samples containing polynucleosomal chains of chicken erythrocyte (CE) and Ehrlich ascites tumour (EA) chromatin were studied under various ionic conditions with regard to electric linear dichroism (ELD) and flow linear dichroism (FLD). Both orientation techniques consistently confirmed that, in the limit of very low ionic strength and in the absence of multivalent cations, the reduced linear dichroism of chromatin is negative in the DNA-base absorption band, as expected for an extended zig-zag polynucleosomal conformation. With increasing electrolyte content, both ELD and FLD decreased drastically in amplitude, but in contrast to the ELD which remains negative in an intermediate range of low ionic strength (0.1–0.5 mM Mg²⁺) the FLD changes sign and becomes positive. The ELD and FLD amplitudes decrease with higher Mg²⁺ concentrations and FLD even vanishes in the region of 0.2–0.4 mM; both signals are positive above 0.4–0.5 mM Mg²⁺.

The origin of the dissimilarities between ELD and FLD observations is still not fully understood. Several possibilities are considered: ELD signals are more influenced than FLD by the presence of short chromatin chains, nucleosomes and small pieces of naked DNA, while FLD is more susceptible to the presence of large, easily orientable, scattering aggregates. Different preferred orientation directions of the chromatin fibre with respect to electric and hydrodynamic fields may also be involved. Finally, FLD and ELD probably “see” different features of the chromatin structure.     

An all-atom model of the chromatin fiber containing linker histones reveals a versatile structure tuned by the nucleosomal repeat length

In the nucleus of eukaryotic cells, histone proteins organize the linear genome into a functional and hierarchical architecture. In this paper, we use the crystal structures of the nucleosome core particle, B-DNA and the globular domain of H5 linker histone to build the first all-atom model of compact chromatin fibers. In this 3D jigsaw puzzle, DNA bending is achieved by solving an inverse kinematics problem. Our model is based on recent electron microscopy measurements of reconstituted fiber dimensions. Strikingly, we find that the chromatin fiber containing linker histones is a polymorphic structure. We show that different fiber conformations are obtained by tuning the linker histone orientation at the nucleosomes entry/exit according to the nucleosomal repeat length. We propose that the observed in vivo quantization of nucleosomal repeat length could reflect nature's ability to use the DNA molecule's helical geometry in order to give chromatin versatile topological and mechanical properties.