Thermal denaturation of nucleohistones--effects of formaldehyde reaction

Thermal denaturation of native or partially dehistonized nucleohistones shows two melting bands at 66 and 81° in 2.5 × 10^?4 M EDTA, pH 8.0. These correspond to the melting of DNA segments bound by the less basic and the more basic half-molecules of histones, respectively. These two melting bands combine into a broad melting band from around 70 to 85° when these nucleohistones are pre-treated with formaldehyde. A formaldehyde reaction which fixes histones on DNA by covalent bonds account for the effect. Formaldehyde fixation also increases the melting temperature of some free DNA segments from around 42 to around 55°. This is interpreted as a result of closed or rigid boundaries between free DNA and formaldehyde-reacted histone-bound DNA segments. MgCl₂ dissociates histones from DNA more effectively and leaves longer free DNA segments than does NaCl. Thermal denaturation of a formaldehyde-reacted nucleoprotein thus provides an effective tool for comparing the relative size of free DNA regions on nucleoproteins. The effect of reversible binding of ligands on helix-coil transition of DNA is descussed and found not adequate for thermal denaturation of nucleohistones.     

Urea perturbation and the reversibility of nucleohistone conformation

Urea effect on conformation and thermal stabilities in nucleohistone and NaCl-treated partially dehistonized nucleohistones has been studied by circular dichroism (CD) and thermal denaturation. Urea imposes a CD change at 278mm of DNA base pairs in native and NaCl-treated nucleohistones which can be decomposed into two parts: a decrease in Δε₂₇₈ for histone-free base pairs and an increase for histone-bound base pairs. The reduction by urea of Δε₂₂₀ of bound histones is approximately proportional to the increase of Δε₂₇₈ of histone-bound base pairs. Urea also lowers the melting temperatures of base pairs both free and bound by histones. The presence of urea indeed destroys the secondary structure of bound histones, causing changes in the conformation and thermal stabilities of histone-bound base pairs in nucleohistone. Such a urea perturbation on nucleohistone conformation is reversible.     

Studies on interaction between histone V (f2c) and deoxyribonucleic acids.

Histone V (2fc) from chick erythroctes was used in the study of its interaction with DNA from various sources. Complexes between this histone and DNA were formed using the procedure of continuous NaCl gradient dialysis in urea. Two physical methods, namely thermal denaturation and circular dichroism (CD), were used as analytical tools. Thermal denaturation of nucleohistone V with chick or calf thymus DNA shows three melting bands: band I at 45-50 degrees corresponds to free base pairs; band II at 75-79 degrees, and band III at 90-93 degrees correspond to histone-bound base pairs. In histone-bound regions, there are 1.5 amino acid residues/nucleotide in nucleohistone V. In contrast, a value between 2.9 and 3.3 was determined for nucleohistone I (fl) (H. J. Li (1973), Biopolymers 12, 287). Similar melting properties have been observed for histone V complexed with bacterial DNA from Micrococcus luteus. Histone V binding to DNA induces a slight transition from a B-type CD spectrum to a C-type spectrum. Trypsin treatment of nucleohistone V reduces melting band III much more effectively than band II. Such a treatment also restores DNA to B conformation in the free state. Reduction of the melting bands of nucleohistone V by polylysine binding follows the order of I greater than II greater than III, accompanied by the increase of a new band at 100 degrees. When two bacterial DNAs of varied A + T (adenine + thymine) content simultaneously compete for the binding of histone V, the more (A " T)-rich DNA is selectively favored. Under experimental conditions described here, Clostridium perfringens DNA with 69% A + T is bound by histone V in preference to chicken DNA with 56% A + T although the latter has natural sequences for histone V binding.     

Circular dichrotic probes for aspects of chromatin structure: aromatic polycationic ionen probes

Two ionens (II and X) formed complexes with DNA and chromatin with extrinsic CD bands and reduced intrinsic bands. The salt and urea sensitive, AT-specific probe (II) gave Δε > 100 L-(residue II)^?1-cm^?1 with DNA and Δε=0–14 with chromatin; II reduced the intrinsic bands from Δε≈0.7 to Δε≈0.5. Ionen X gave Δε₃₄₅=30 with DNA, and Δε₃₄₅=15–20 with chromatin. X reduced the intrinsic band to ?1.6. X show less base specificity. Extrinsic Δε_λ of X increased linearly to r (residue/phosphate) = 0.5 for DNA and only 0.3 in chromatin. DNA in chromatin may have ～10% of the II and 50–60% of the X binding sites and those in an altered conformation.     

Ultraviolet radiation response to the physical properties of the reconstituted nucleohistone

The effect of UV irradiation on the reconstituted nucleohistone have been studied with reference to its (nucleohistone) changes in physical properties, after irradiation at different UV doses. The rate of fall of specific viscosity ratio of the reconstituted nucleohistone as a function of UV dose decreased gradually with the increasing histone to DNA weight ratio (r). This effect, was not observed when the histones remained dissociated from DNA, in high ionic strength (1.5 M NaCl). Histone-DNA complex (r=0.97) irradiated up to a dose of 3.6×10⁴ J/m² had a stable melting temperature unlike free DNA where UV irradiation lowered the melting temperature and the heterogeneous melting profiles were observed. Rate of formaldehyde reaction, with DNA recovered from the irradiated complex, was slower than that with native DNA treated at the same dose. All this suggested that the effect of UV in the DNA of the nucleohistone was less, compared to that in free DNA.     

Helix-coil transition in nucleoprotein: renaturation of polylysine-DNA and polylysine-nucleohistone complexes

Thermal denaturation and renaturation of directly mixed and reconstituted polylysine–DNA, directly mixed polylysine–nucleohistone complexes, and NaCl-treated nucleohistones in 2.5 × 10^?4 M EDTA, pH 8.0 have been studied. At the same input ratio of polylysine to DNA, the percent of renaturation of free base pairs in a directly mixed polylysine–DNA complex is higher than that in a reconstituted complex. For a directly mixed complex, the renaturation of free base pairs is proportional to the fraction of DNA bound by polylysine or inversely proportional to the sizes of free DNA loops. A of large amount of renaturation of free base pairs has also been observed for 0.6 M and 1.6 M NaCl-treated nucleohistones. The binding of polylysine to nucleohistone enhances the renaturation of histone-bound base pairs. The percent of renaturation of polylysine–bound base pairs is high and is approximately independent of the extent of binding on DNA by polylysine. This is true in polylysine–DNA complexes prepared either by reconstitution or by directly mixing. It also applies for polylysine–nucleohistone complexes. The model where polylysine-bound base pairs collapse at T_m′ with two complementary strands still bound by polylysine is favored over the model where polylysine is dissociated from DNA during melting. The low renaturation of histone-bound base pairs in nucleo-histone indicates that either histones do not hold two complementary strands of DNA tightly or that histones are fully or partially dissociated from DNA when the nucleo-histone is fully denatured.     

Thermodynamic Study of Interactions of Distamycin A with Chromatin in Rat Liver Nuclei in the Presence of Polyamines

We studied the thermodynamics of melting of isolated rat liver nuclei with different degrees of chromatin condensation determined by the concentration of polyamines (PA) and the solution ionic strength, as well as the effect of the antibiotic distamycin A (DM) on melting. Differential scanning calorimetry (DSC) profiles of nuclear preparations contained three peaks that reflected melting of three main chromatin domains. The number of peaks did not depend on the degree of condensation; however, nuclei with more condensed chromatin had a higher total enthalpy. DM stabilized peaks II and III corresponding to the melting of relaxed and topologically strained DNA, respectively, but destabilized peak I corresponding to the melting of nucleosome core histones. At the saturating concentration (DM/DNA molar ratio = 0.1), DM increased T_m of peaks II and III by ~5°C and decreased T_m of peak I by ~2.5°C. Based on the dependence of ΔH on DM concentration, we established that at low DM/DNA ratio (?0.03), when DM interacted predominantly with AT-rich DNA regions, the enthalpy of peak II decreased in parallel with the increase in the enthalpy of peak III, which indicated that DM induces structural transitions in the nuclear chromatin associated with the increase in torsional stress in DNA. An increase in free energy under saturation conditions was equal to the change in the free energy of DM interaction with DNA. However, the increase in the enthalpy of melting of the nuclei in the presence of DM was much greater than the enthalpy of titration of nuclei with DM. This indicates a significant increase in the strength of interaction between the two DNA strands apparently due, among other things, to changes in the torsional stress of DNA in the nuclei. Titration of the nuclei with increasing PA concentrations resulted in the decrease in the number of DM-binding sites and the non-monotonous dependence of the enthalpy and entropy contribution to the binding free energy on the PA content. We suggested that the observed differences in the thermodynamic parameters were due to the different width of the minor groove in the nuclear chromatin DNA, which depends on PA concentration.     

Studies on poly(L-lysine50, L-tyrosine50)-DNA interaction

Interaction between poly(Lys⁵⁰, Tyr⁵⁰) and DNA has been studied by absorption, circular dichroism (CD), and fluorescence spectroscopy and thermal denaturation in 0.001M Tris, pH 6.8. The binding of this copolypeptide to DNA results in an absorbance enhancement and fluorescence quenching on tyrosine. There is also an increase in the tyrosine CD at 230 nm. The CD of DNA above 250 nm is slightly shifted to the longer wavelength which is qualitatively similar to, but quantitatively much smaller than, that induced by polylysine binding. At physiological pH the poly(Lys⁵⁰, Tyr⁵⁰)–DNA complex is soluble until there is one lysine and one tyrosine per nucleotide in the complex. The same ratio of amino acid residues to nucleotide has also been observed in copolypeptide-bound regions of the complex. The addition of more poly(Lys⁵⁰, Tyr⁵⁰) to DNA yields a constant melting temperature, T_m′, for bound base pairs at 90°C which is close to that of polylysine-bound DNA under the same condition. The melting temperature, T_m, of free base pairs at about 60°C on the other hand, is increased by 10°C as more copolypeptide is bound to DNA. As the temperature is raised, both absorption and CD spectra of the complexes with high coverage are changed, suggesting structural alteration, perhaps deprotonation, on bound tyrosine. The results in this report also suggest that intercalation of tyrosine in DNA is unlikely to be the mode of binding.     

Spectroscopic and calorimetric studies on the DNA recognition of pyrrolo[2,1-c][1,4]benzodiazepine hybrids

DNA binding of two hybrid ligands composed of an alkylating pyrrolo[2,1-c][1,4]benzodiazepine (PBD) moiety tethered to either a naphthalimide or a phenyl benzimidazole chromophore was studied by DNA melting experiments, UV and fluorescence titrations, CD spectroscopy and isothermal titration calorimetry (ITC). Binding of both hybrids results in a remarkable thermal stabilization with an increase of DNA melting temperatures by up to 40 °C for duplexes that allow for a covalent attachment of the PBD moiety to guanine bases in their minor groove. CD spectroscopic measurements suggest that the naphthalimide moiety of the drug interacts through intercalation. In contrast, the PBD-benzimidazole hybrid binds in the DNA minor groove with a preference for (A,T)₄G sequences. Whereas the binding of both ligands is enthalpy-driven and associated with a negative entropy, the benzimidazole hybrid exhibits a less favourable binding enthalpy that is counterbalanced by a more favourable entropic term when compared to the naphthalimide hybrid.     

Interaction between poly(L-lysine48, L-histidine52) and DNA.

Poly(Lys⁴⁸, His⁵²), a random copolypeptide of L -lysine (48%) and L -histidine (52%), was used as a model protein for investigating the effects of protonation on the imidazole group of histidines on protein binding to DNA. The complexes formed between poly(Lys⁴⁸, His⁵²) and DNA were examined using absorbance, circular dichroism (CD), and thermal denaturation. Although increasing pH reduces the charges on histidine side chains in the model protein, the protein still binds the DNA with approximately one positive charge per negative charge in protein-bound regions. Nevertheless, CD and melting properties of poly(Lys⁴⁸, His⁵²)-DNA complexes still depend upon the solution pH which determines the protonation state of imidazole group of histidine side chains. At pH 7.0, the complexes show two characteristic melting bands with a t_m (46–51°C) for free base pairs and a t′_m (94°C) for protein-bound base pairs. The t′_m of the complexes is reduced to 90°C at pH 9.2, although at this pH there is still one lysine per phosphate in protein-bound regions. Presumably, the presence of deprotonated histidine residues destabilizes the native structure of protein-bound DNA. The binding of this model protein to DNA causes a red shift of the crossover point and both a red shift and a reduction of the positive CD band of DNA near 275 nm. This phenomenon is similar to that caused by polylysine binding. These effects, however, are greatly diminished when histidine side chains in the model protein are deprotonated. The structure of already formed poly(Lys⁴⁸, His⁵²)·DNA complexes can be perturbed by changing the solution pH. However, the results suggest a readjustment of the complex to accommodate charge interactions rather than a full dissociation of the complex followed by reassociation between the model protein and DNA.     

Studies on the thermal denaturation of nucleohistones

The thermal denaturation profiles of nucleohistone from calf thymus, sea urchin sperm and sea cucumber male gonad, are studied and compared under a variety of conditions. These include melting in the presence of either one of the following agents: urea, methanol, divalent cations or excess histones. The influence of ionic strength, pH, formaldehyde treatment and partial denaturation is also studied. Particular attention is given to the factors which influence the bimodal appearance of the profiles. The melting curves of the three materials used are qualitatively similar under all conditions, although they show quantitative differences. The histone:DNA ratio appears to be the most important parameter to define the denaturation properties of a given nucleohistone preparation. It is shown that redistribution of histones may determine the melting profile, since during denaturation histones can migrate from locally denatured regions towards those regions which contain native DNA. It is also shown that there are regions of phosphate negative charges of DNA not protected by histone. These regions can be protected against denaturation either by additional histones or by certain divalent cations. The results are interpreted in terms of the various models possible for the distribution of histones on DNA in native nucleohistone. Their biological significance is also discussed.     

The satellite bands of the DNA of Drosophila virilis

Purified DNA has been prepared from Drosophila virilis using a modification of the method derived for bacteria (Marmur, 1961). Some physical properties have been examined, a new hidden satellite discovered, and a difference found in the satellite banding pattern of different tissues. — In addition to the three satellite bands lighter than the main band previously reported (Gall et al., 1970), a new satellite heavier than the main band has been detected after thermal denaturation of the DNA (which substantially shifts the buoyant density of the main band but not that of the satellites indicating that all are fast-annealing). The satellite pattern of DNA extracted from heads alone differed from that of the entire animals: the amount of satellite I was decreased and II increased; III was unaffected; IV was increased relative to the amount in the main band. The total content of satellite material in the heads (assumed to be entirely diploid) was 42%, the highest amount reported for any organism. — Thermal transitions were determined for the DNA from adults and larvae. After preparative CsCl density gradient fractionation of adult DNA, two sets of bimodal thermal curves were obtained (in SSC) with agreement between the initial position in the preparative gradient, the thermal transitions, and the G+C content from density except for satellite III for which the T_m gave a more accurate G+C amount. DNA from satellites I and II together generated a T_m of 81.2° which was similar to a calculated T_m of 81.9° making the naive assumption that the thermal components of the two satellites would interact in a simple additive fashion. A T_m of 71.9° was ascribed to satellite III which indicates that it is not the equivalent of the poly (A-T) band found at the same density in D. melanogaster (Fansler et al., 1970). The calculated overall base composition from the density equivalents (using the value for satellite III from thermal data) gave an expected G+C content of 36.6%. The measured value was 36.0%. The possible significance of the differential satellite pattern has been discussed.     

Carboxyl-terminal peptides from histone H1 variants: DNA binding characteristics and solution conformation

The carboxyl-terminal domains of the histone H1 proteins bind to DNA and are important in condensation of DNA. Little is known about the details of the interactions between H1 histones and DNA, and in particular, there is little known about differences among variant H1 histones in their interactions with DNA. Questions concerning H1 histone-DNA affinity and H1 conformation were investigated using peptide fragments from the carboxyl terminal domains of four nonallelic histone H1 variant proteins (mouse H1-1, H1-4 and H1^°, and rat H1T). Three of the four peptides showed a slight preference for binding to a GC-rich region of a 214-base-pair DNA fragment, rather than to an AT-rich region. The fourth peptide, H1t, appeared to bind preferentially to the AT-rich region of the 214-base-pair fragment. The results show that these small peptides bind preferentially to a subset of DNA sequences; such sequence preference might be exhibited by the intact H1 histones themselves. CD spectra of the peptides, which are from regions of the proteins that are not compactly folded, showed that the α-helical content of the peptides was minimal if the peptides were in 10 mM phosphate buffer, but increased if the peptides were in 1 M NaClO₄ and 50% trifluoroethanol, conditions that are postulated to approximate certain aspects of binding to DNA. H1-4 peptide, which was predicted to be 70% α-helix, but was not α-helical in 10 mM phosphate buffer, appeared from difference CD spectra to be more α-helical when it was bound to DNA. The regions of the proteins from which these peptides are derived, which are extended in solution, may fold, forming α-helices, upon binding to DNA. © 1996 John Wiley & Sons, Inc.     

Distribution of histone F1 on calf thymus nucleohistone DNA.

A method of large-scale preparation of the histone F1-DNA complex by removing all other proteins from calf thymus nucleohistone was established. This involved gel filtration of nucleohistone through a column containing a band of sodium dodecyl sulfate. The F1-DNA complex obtained had the original amount of F1 and no other. The F1-DNA complex exhibited distinct two-step melting on thermal denaturation. The first step was apparently attributable to naked DNA regions and the second step, about 30 deg. C higher than the first step, to the regions covered with F1. Buoyant density experiments with the complex after fixation with formalin revealed that F1 was distributed fairly evenly over DNA fragments of an average molecular weight of about 4 × 10⁶. Electron microscopic examination of the complex after various degrees of denaturation with formalin indicated that the longest stretch of unbound DNA was about 0·3 μm.     

Thermal Stability Investigation and the Kinetic Study of Folnak<Superscript>®</Superscript> Degradation Process Under Nonisothermal Conditions

The nonisothermal degradation process of Folnak^® drug samples was investigated by simultaneous thermogravimetric and differential thermal analysis in the temperature range from an ambient one up to 810°C. It was established that the degradation proceeds through the five degradation stages (designated as I, II, III, IV, and V), which include: the dehydration (I), the melting process of excipients (II), as well as the decomposition of folic acid (III), corn starch (IV), and saccharose (V), respectively. It was established that the presented excipients show a different behavior from that of the pure materials. During degradation, all excipients increase their thermal stability, and some kind of solid–solid and/or solid–gas interaction occurs. The kinetic parameters and reaction mechanism for the folic acid decomposition were established using different calculation procedures. It was concluded that the folic acid decomposition mechanism cannot be explained by the simple reaction order (ROn) model (n?=?1) but with the complex reaction mechanism which includes the higher reaction orders (RO, n?>?1), with average value of <n?>?=?1.91. The isothermal predictions of the third (III) degradation stage of Folnak^® sample, at four different temperatures (T _iso?=?180°C, 200°C, 220°C, and 260°C), were established. It was concluded that the shapes of the isothermal conversion curves at lower temperatures (180–200°C) were similar, whereas became more complex with further temperature increase due to the pterin and p-amino benzoic acid decomposition behavior, which brings the additional complexity in the overall folic acid decomposition process.     

Temperature dependence of CD spectra of DNA from various sources

The CD spectra of DNA from various sources (T2; T4; C_d; Escherichia coli; calf thymus; Streptomyces chrysomalis) were investigated. A new band Δ_ε210 in the CD spectra of glucosylated DNA of the T even phages was found. The temperature dependence of the CD spectra of DNA was obtained over a wide range of temperatures, including those of the helix–coil transition. The band Δ_ε275 for all DNAs does not appreciably change in the range of the helix–coil transition. The monotonic increase of this band before melting, and its decrease after melting is observed with an increase in temperature. The amplitude of the CD band Δ_ε245 for all the DNAs studied and Δ_ε210 (glucosylated DNA) parallels the change of E₂₆₀ absorbance.     

Extrinsic cotton effect and helix-coil transition in a DNA-polycation complex

A strong, positive, extrinsic CD band ([θ]_242.5 = ～2 × 10^?3 deg cm²/dmole) has been observed for a α-bromo-poly[methylene-1,4-phenylenecarbonyloxyethylene(dimethylamino) bromide] (I). The extrinsic Cotton effect is attributed to the ordered arrangement of the aromatic chromophores along the DNA helix. The extrinsic band had a linear dependence on the amount of polycation I added from r ≤ 0.3 to r = ～0.5, but decreased thereafter. Addition of the polycation decreased the positive CD band of DNA at 275 nm. The transformation of B → C form in the presence of salts or other polycations caused similar changes. The decrease in [θ]₂₇₅ was reversed at higher concentrations of the polycation (r > 0.4). Thermal denaturation studies indicated both stabilization of the helix conformation (Δt_m = 21°C) and a high degree of cooperativity in the melting of DNA-polycation complex as compared to native calf thymus DNA. Using the linear relationship between r (polycation residue/DNA phosphate) and F (fraction of bound base pairs), a value of 0.6 was derived for β (number of monomer residues of polycation/nucleotide). Both electrostatic and hydrophobic effects probably influence the stability of the DNA-polycation complex, since the strength of the 242.5 nm CD band is a function of both salt and urea concentrations.     

133 Designed DNA crystals with a triple-helix veneer

DNA has been used as a tool for the self-assembly of nano-sized objects and arrays in two and three-dimensions. Triplex-forming oligonucleotides (TFOs) can be exploited to recognize and introduce functionality at precise duplex regions within these DNA nanostructures (Rusling et al., 2012). Here we have examined the feasibility of using TFOs to bind to specific locations within a 3-turn DNA tensegrity triangle motif. The tensegrity triangle is a rigid DNA motif with three-fold rotational symmetry, consisting of three helices directed along three linearly independent directions (Liu et al., 2004). The triangles form a three-dimensional crystalline lattice stabilized via sticky-end cohesion (Zheng et al., 2009). The TFO 5′-TTCTTTCTTCTCT was used to target the tensegrity motif containing an appropriately embedded oligopurine–oligopyrimidine binding site. Formation of DNA triplex in the motif was characterized by an electrophoretic mobility shift assay (EMSA), UV melting studies and FRET analysis. Non-denaturing gel analysis of annealed DNA motifs showed a band with slower mobility only in the presence of TFO and only when the DNA motif contained the triplex binding site. Experiments were undertaken at pH 5.0, since the formation of a triplex with cytidine-containing TFOs requires slightly acidic conditions (pH<?6.0). TFOs with modified C-analogs and T-analogs having a higher pK _a worked at a more neutral pH, also evidenced by EMSA. UV melting studies revealed that the melting point of the 3-turn triangle was 64?°C and the TFO binding increased the melting point to 80?°C. FRET analysis was done by labeling the triangle with fluorescein and the TFO with a cyanine dye (Cy5). The FRET melting curve revealed that a signal was observed only when the TFO was bound to the DNA motif and the results were consistent with UV melting studies. These results indicate that a TFO can be specifically targeted to the tensegrity triangle motif.     

Binding of ligands to a one-dimensional heterogeneous lattice. II. Intercalation of tilorone with DNA and polynucleotides

The interaction of tilorone with DNA and five synthetic polydeoxyribonucleotides [(I): poly[d(A-T)]·poly[d(A-T)]; (II): poly[d(A-C)]·poly[d(G-T)]; (III): poly[d(G-C)]·poly[d(G-C)]; (IV): poly(dG)·poly(dC); and (V): poly(dA)·poly(dT)] has been investigated. Binding isotherms for the homopolymers were obtained by microdialysis equilibria using ¹⁴C-labeled tilorone and interpreted with different models: exclusion effect, associated or not associated with cooperativity, or variable exclusion. Affinity appears to be related more to local structure than to base composition and decreases in the following order: (I) > (II) > (III) > (IV) > (V). Intercalation in circular DNA was demonstrated by electrophoresis migration and electron microscopy, which yielded an average unwinding angle of 7° per bound dye. The behavior observed in CD and UV spectroscopy shows a sequence similar to the affinities. Tilorone seems to be less intercalated in (IV) and not at all in (V). The experimental binding isotherm of tilorone to DNA was well fitted on the basis of a model where DNA acts as a heterogeneous lattice built with the six different possible couples of adjacent base pairs, each potential site behaving as if it were in the corresponding homopolymer. The results are discussed in terms of specificity of alternating Pyr-Pur sequences and related to theoretical calculations on intercalation energies of DNA.