Role of nonhistone chromosomal proteins in determining circular dichroism spectra of chromatin.

Complexing of histone proteins, from WI-38 cells with pure DNA from WI-38 cells, causes a marked decrease in the amplitude of the positive ellipticity band and a red shift in circular dichroism spectra in the 250–300 nm region. Total nonhistone chromosomal proteins from WI-38 cells (without histones) cause an analogous effect, but of significantly reduced magnitude. However, the two effects are not additive, because, when DNA is complexed with both histones and nonhistones, the amplitude of the positive ellipticity band has an intermediate value, between the histone-DNA complex and the nonhistone-DNA complex. Removal of certain nonhistone proteins from chromatin of WI-38 cells, by extraction with 0.25–0.35 m NaCl, causes a decrease in the positive circular dichroism band in the 250–300 nm region. Removal of histones and other nonhistone proteins from chromatin by extraction with 0.75 and 1.5 m NaCl causes a strong increase in positive ellipticity. This suggests the existence of modest but definite effects of nonhistone proteins in determining DNA conformation in native chromatin. Taken as a whole, nonhistone chromosomal proteins have a weaker but analogous effect to that of histones, while the nonhistone proteins extractable with 0.25–0.35 m NaCl have an opposite effect.     

Nucleic acid vibrational circular dichroism, absorption, and linear dichroism spectra. I. A DeVoe theory approach.

Infrared (IR) vibrational circular dichroism (VCD), absorption, and linear dichroism (LD) spectra of four homopolyribonucleotides, poly(rA), poly(rG), poly(rC), and poly(rU), have been calculated, in the 1750-1550 cm-1 spectral region, using the DeVoe polarizability theory. A newly derived algorithm, which approximates the Hilbert transform of imaginaries to reals, was used in the calculations to obtain real parts of oscillator polarizabilities associated with each normal mode. The calculated spectra of the polynucleotides were compared with previously measured solution spectra. The good agreement between calculated and measured polynucleotide spectra indicates, for the first time, that the DeVoe theory is a useful means of calculating the VCD and IR absorption spectra of polynucleotides. For the first time, calculated DeVoe theory VCD and IR absorption spectra of oriented polynucleotides are presented. The calculated VCD spectra for the oriented polynucleotides are used to predict the spectra for such measurements made in the future. The calculated IR spectra for the oriented polynucleotides are useful in interpreting the linear dichroism of the polynucleotides.     

Comparative study of nucleosome particles in chromatin from normal and tumor cells. I. Structural parameters

The composition and structure of nucleosomic fragments isolated from the ascitic hepatoma 22A cells, liver and from cells of C3HA mice in norm and after partial hepatectomy were investigated. Via electrophoresis in 1.5% agarose gel with the emplogment of reperic restrictive DNA fragments and with the help of mathematical processing, the value of the nucleosomic DNA repeat in ascitic hepatoma 22A was calculated to be 187 b.p., and in regenerating liver--196 b.p. The absence of the H1 degree subfraction in chromatin of ascitic hepatoma 22A cells was found. Lower electrophoretic mobility in 5% polyacrylamid gel of nucleosomic chromatin fragments of ascitic hepatoma 22A as compared with their counterparts from healthy mice liver was established. The method of circular dichroism allowed to reveal differences in the RNA and protein structural state in nucleosomes of normal and tumour cells. The structure of nucleosomes of regenerating mice liver of the C3HA strain did not differ from that of normal liver of the same mice.     

Circular dichroism and magnetic circular dichroism spectra of chlorophylls in nematic liquid crystals. I. Electric and weak magnetic field effects on the dichroism spectra

Dichroism spectra of chlorophyll a, chlorophyll b and bacteriochlorophyll a in various nematic liquid crystals are reported. The initial orientation of chlorophylls in such a sample is determined by the interaction of the aggregate formed from the pigment and the liquid crystal molecules with the electrode surface on the cell windows. Reorientation is carried out by either an electric or magnetic field. The analysis of the circular dichroism spectra obtained from these samples on the basis of the Mueller matrix shows that the intensity is predominantly related to the texture of the sample. Chlorophyll molecules can be aggregated with liquid crystals in two ways: (1) through the chlorin magnesium atom, which results in the liquid crystal chain being almost perpendicular to the porphyrin ring, or (2) attached parallel to the line connecting the first and third pyrrole rings of the chlorin, the chlorin now lying in the plane of the liquid crystal chains. By comparing the dichroism spectra of various chlorophylls in the same liquid crystal we can draw conclusions concerning the preferred type of aggregation, not only with liquid crystals, but also with biological molecules. These liquid crystal systems are models of the orientation effects found for chlorophyll in lamellae. The model studied in this work is much simpler than the lamellar system but it does exhibit several common properties with the latter. Both systems are anisotropic and show much more intense dichroism signals, often of opposite sign, compared with those observed for photosynthetic pigments in isotropic solutions. Dichroism signals of organism fragments are much more complex than those of our model, which can either be related to the occurrence in the organism of several types of pigments or, for a given type of pigment, could be the result of exciton splitting. On the basis of our model it is shown that small changes in the anisotropy of the pigment in the surroundings have a strong influence on the sign and amplitude of the observed circular dichroism signal. Such effects may be responsible for the structure of the dichroism spectra observed for biological samples. Such structures can be partially related to the superposition of the dichroism signal from various ‘domains’ of chromophore which are different in both pigment arrangement and in the anisotropy of the surroundings of the pigment molecules themselves.     

Determination of protein secondary structure from circular dichroism spectra. III. Protein-derived base spectra of circular dichroism for antiparallel and parallel beta-structures

Protein-derived basic CD spectra for alpha-helix, antiparallel and parallel beta-structures, beta-bends and irregular form of proteins have been determined from the experimental CD spectra of six (myoglobin, lysozyme, ribonuclease A, papain, lactate dehydrogenase, subtilisin BPN') or seven (glyceraldehyde-3-phosphate dehydrogenase added) reference proteins and the analysis of the X-ray data. The secondary structures of thirteen proteins (seven reference and six additional ones) have been analysed using the basic CD spectra thus obtained. The data obtained have been compared with the results of the X-ray data analysis. It is shown that the accuracy of determination of the beta-structure and beta-bends contents using our basic CD spectra is about 2-3 times better than using the basic spectra reported by Chang et al. (Analyt. Biochem. 91, 13-31, 1978).     

Circular dichroism and magnetic circular dichroism spectra of chlorophylls a and b in nematic liquid crystals. II. Magnetic circular dichroism spectra

Absorption and magnetic circular dichroism (MCD) spectra are reported for chlorophyll (Chl) a and Chl b dissolved in nematic liquid crystal solvents. The spectra were measured with the dye molecules oriented uniaxially along the direction of. the magnetic field and measuring light beam. It is significant that under such conditions the MCD spectra recorded in the wavelength region of the Q and Soret bands of the chlorophyll are essentially unchanged with respect to rotation of the sample cell around this axis, even though there is almost complete orientation of the chlorophyll molecules by the liquid crystals. The MCD spectra of Chl a and b in the nematic liquid crystal solvents used in this study are surprisingly similar to the spectra obtained under isotropic conditions. These results illustrate an important technique with which to examine the optical spectra of dyes oriented in liquid crystal matrices in which the anisotropic effects can be reduced the negligible proportions by the application of a strong magnetic field parallel to the direction of the measuring light beam. The first deconvolution calculations are reported that describe the deconvolution of pairs of absorption and MCD spectra, in the Q and B band regions, for both Chl a and b. The spectral analysis to obtain quantitative estimates of transition energies was accomplished by carrying out detailed deconvolution calculations in which the both the absorption and MCD spectral envelopes were fitted with the same number of components; each pair of components had the same hand centres and bandwidth values. This procedure resulted in an assignment of each of the main transitions in the absorption spectra of both Chl a and b. Chl a is clearly monomeric, with Qy, Qx, By and Bx located at 671, 582, 439 and 431 nm, respectively. Analysis of the spectral data for Chl b located Qy, By and Bx, at 662, 476 and 464 nm, respectively.     

Deconvolution of the circular dichroism spectra of proteins: the circular dichroism spectra of the antiparallel beta-sheet in proteins.

A recently developed algorithm, called Convex Constraint Analysis (CCA), was successfully applied to determine the circular dichroism (CD) spectra of the pure beta-pleated sheet in globular proteins. On the basis of X-ray diffraction determined secondary structures, the original data set used (Perczel, A., Hollosi, M., Tusnady, G. Fasman, G.D. Convex constraint analysis: A natural deconvolution of circular dichroism curves of proteins, Prot. Eng., 4:669-679, 1991), was improved by the addition of proteins with high beta-pleated sheet content. The analysis yielded CD curves of the pure components of the main secondary structural elements (alpha-helix, antiparallel beta-pleated sheet, beta-turns, and unordered conformation), as well as a curve attributed to the "aromatic contribution" in the wavelength range of 195-240 nm. Upon deconvolution the curves obtained were assigned to various secondary structures. The calculated weights (percentages determining the contributions of each pure component curve in the measured CD spectra of a given protein) were correlated with the X-ray diffraction determined percentages in an assignment procedure and were evaluated. The Pearson product correlation coefficients (R) are significant for all five components. The new pure component curves, which were obtained through deconvolution of the protein CD spectra alone, are promising candidates for determining the percentages of the secondary structural components in globular proteins without the necessity of adopting an X-ray database. The CD spectrum of the CheY protein was interesting because it has the characteristic shape associated with the alpha-helical structure, but upon analysis yielded a considerable amount of beta-sheet in agreement with the X-ray structure.     

Chirality of aromatic bis-imides from their circular dichroism spectra

It is demonstrated that chirality of molecules composed of 1,2,4, 5-benzenetetracarboxydiimide (pyromellitic diimide) or 1,4,5, 8-naphthalenetetracarboxydiimide units is reflected by their exciton Cotton effects. The analysis is based on the calculated (ZINDO/S) excited states of the model diimide chromophores 1a and 2a. Rotation of the diimide chromophores around the C-N bond in diimides 3-5 is evaluated from the dynamic (1)H NMR data. A comparison of chiroptical properties of bis-diimides 3-5 with the CD spectra of bis-imides 6-8 is also presented. Copyright 2000 Wiley-Liss, Inc.     

Spectroscopy and structure of bacteriochlorophyll dimers. I. Structural consequences of nonconservative circular dichroism spectra.

The origin of the nonconservative nature of the circular dichroism (CD) spectrum of bacteriochlorophyll dimers is investigated. It is shown that coupling between the Qy and Qx transitions can, under rather restricting circumstances, lead to an asymmetrical CD spectrum: only for a limited set of relative orientations of the monomers within the dimer is the spectrum found to be asymmetrical. The relation between intensity and asymmetry of the CD spectrum is elucidated. The results are applied to the B820 subunit of the LH1 antenna system and subsequently to the antenna system LH1 itself. Differences in the geometry of the BChls in LH1 versus the LH2 structure are discussed.     

Computer-aided analysis of infrared, circular dichroism and absorption spectra

Marquardt and Powell optimization methods without constraintson the optimized spectral parameters were employed for decompositionof complex i.r., c.d. and absorption spectra into componentbands. The procedure resolved experimental spectra into eightcomponent bands and it can be easily adjusted for a larger setof component bands. The CPU time required for achievement ofsatisfactory convergence of parameters for eight component bandsis rather large even when using mainframe computers and thereforedivision of spectra into a few non-overlapped parts is advisable.The program also can be used for calculation of absorption,c.d. and difference spectra from formatted raw spectral data. Received on January 13, 1986; accepted on April 7, 1986     

Variability of light-induced circular dichroism spectra of photosystem I complexes of cyanobacteria

Circular dichroism (CD) spectra of photosystem I (PSI) complexes of the cyanobacteria Thermosynechococcus elongatus, Arthrospira platensis and Synechocystis sp. PCC 6803 were studied. CD spectra of dark-adapted PSI trimers and monomers, measured at 77 K, show common bands at 669–670(+), 673(+), 680(−), 683–685(−), 696–697(−), 702(−) and 711(−) nm. The intensities of these bands are species specific. In addition, bands at 683–685(−) and 673(+) nm differ in intensity for trimeric and monomeric PSI complexes. CD difference spectra (P700⁺–P700) of PSI complexes at 283 K exhibit conservative bands at 701(−) and 691(+) nm due to changes in resonance interaction of chlorophylls in the reaction center upon oxidation of P700. Additional bands are observed at 671(−), 678(+), 685(−), 693(−) nm and in the region 720–725 nm those intensities correlate with intensities of analogous bands of antenna chlorophylls in dark-adapted CD spectra. It is suggested that the variability of CD difference spectra of PSI complexes is determined by changes in resonance interaction of reaction center chlorophylls with closely located antenna chlorophylls.     

Effect of formaldehyde on the circular dichroism of chicken erythrocyte chromatin.

Formaldehyde (HCHO) fixation of chicken erythrocyte chromatin produces a marked decrease in its positive circular dichroism (CD), above 260 nm, and the appearance of s small negative ellipticity around 295 nm. The ultraviolet spectrum of chromatin is unaffected, nor does HCHO produce any changes in the uv or CD spectra of chicken erythrocyte DNA. The extent of the circular dichroism transition from the native chromatin to the suppressed spectrum is dependent on the concentration of HCHO and salt concentration. The kinetics of the reactions are complex, implicating at least two reactive species. Studies of the reaction of HCHO with chromatin in ethylene glycol and CD measurements of aqueous chromatin solution with added glutaraldehyde preclude simple dehydration and general cross-linking effects as causes of the CD changes observed. The results are interpreted as indicating a conformational change of the DNA in chromatin caused by histone-DNA or histone-histone cross-linking.     

Vibrational circular dichroism spectra of unblocked proline oligomers.

Vibrational Circular Dichroism (VCD) spectra of unblocked L-proline oligopeptides, (Pro)n n = 3 to 7, dissolved in D2O are reported. For these oligomers, the VCD spectra can be attributed to a conformational dominance of the trans amide conformation with subunits interrelated by a left-handed twist, particularly for the longer oligomers. As a function of oligomer length, formation of this conformation starts at n = 3; and by n = 5 a spectrum closely resembling that of the poly-L-proline II helix in shape and magnitude is seen. The VCD data are compared with previous (Pro)n results using IR, CD, Raman and NMR spectroscopies, and reasons for the variations in interpretation are discussed.     

Nucleic acid vibrational circular dichroism, absorption, and linear dichroism spectra. II. A DeVoe theory approach.

The DeVoe polarizability theory is used to calculate vibrational circular dichroism (VCD) and infrared (IR) absorption spectra of four polyribonucleotides: poly(rA) x poly(rU), poly(rU) x poly(rA) x poly(rU), poly(rG) x poly(rC), and poly(rC+) x poly(rI) x poly(rC). This is the first report on the use of the DeVoe theory to calculate VCD, oriented VCD, IR absorption, and IR linear dichroism (LD) spectra of double- and triple-stranded polyribonucleotides. Results are reported for DeVoe theory calculations--within the base-stretching 1750-1550 cm(-1) spectral region--on several proposed multistranded polyribonucleotide geometries. The calculated spectra obtained from these proposed geometries are compared with previously reported measured and calculated VCD and IR spectral results. Base-base hydrogen-bonding effects on the frequencies and magnitudes of the base carbonyl stretching modes are explicitly considered. The good agreements found between calculated and measured spectra are proposed to be further evidence of the usefulness of the DeVoe theory in drawing three-dimensional structural conclusions from measured polyribonucleotide VCD and IR spectra.     

Absolute configuration of an axially chiral sulfonate determined from its optical rotatory dispersion,electronic circular dichroism,and vibrational circular dichroism spectra

The absolute configuration (AC) of an axially chiral sulfonate (aCSO), 3,5‐dimethyl‐2‐(naphthalen‐1‐yl)‐6‐(naphthalen‐1‐yl)benzenesulfonate (labeled as aCSO5), was investigated using optical rotatory dispersion (ORD), electronic circular dichroism (ECD), and vibrational circular dichroism (VCD) spectroscopies. All three methods led to the same conclusion and the AC of aCSO5 is reliably determined to be (−)‐(aR , aR ), or conversely (+)‐(aS , aS ).     

Determination of the secondary structure of proteins from circular dichroism spectra. IV. Contribution of aromatic amino acid residues into circular dichroism spectra of proteins in the peptide region

A new method for determination of the secondary protein structure from the CD spectra taking into account the contribution of aromatic amino acid residues is proposed. New proteins reference CD spectra for five secondary structures (alpha-helices, antiparallel and parallel beta-structures, beta-bends and irregular form) without contribution of aromatic residues are obtained. By means of this new method the secondary structure of sixteen different proteins was analysed. There is a good correlation of these results with the X-ray data.     

Structure of centromere chromatin: from nucleosome to chromosomal architecture

The centromere is essential for the segregation of chromosomes, as it serves as attachment site for microtubules to mediate chromosome segregation during mitosis and meiosis. In most organisms, the centromere is restricted to one chromosomal region that appears as primary constriction on the condensed chromosome and is partitioned into two chromatin domains: The centromere core is characterized by the centromere-specific histone H3 variant CENP-A (also called cenH3) and is required for specifying the centromere and for building the kinetochore complex during mitosis. This core region is generally flanked by pericentric heterochromatin, characterized by nucleosomes containing H3 methylated on lysine 9 (H3K9me) that are bound by heterochromatin proteins. During mitosis, these two domains together form a three-dimensional structure that exposes CENP-A-containing chromatin to the surface for interaction with the kinetochore and microtubules. At the same time, this structure supports the tension generated during the segregation of sister chromatids to opposite poles. In this review, we discuss recent insight into the characteristics of the centromere, from the specialized chromatin structures at the centromere core and the pericentromere to the three-dimensional organization of these regions that make up the functional centromere.