Cooperative interaction of histone H1 with DNA.

The cooperative binding of histone H1 with DNA was studied using a fluorescently labelled histone H1. The titration data were analysed in terms of the large ligand model. The stoichiometric number, n = 65 +/- 10 bases/H1, was independent of NaCl concentration (0.02 - 0.35 M). The nucleation and the cooperative binding constants, K' and K, and the cooperativity parameter q were sensitive to salt concentration; K = 3.6 +/- 0.8 X 10(7) M-1 and q = 1.1 +/- 0.4 X 10(3) at 0.2 M NaCl. The dependence of K' on NaCl concentration revealed that 6 Na+ ions were released from DNA upon complex formation. An extrapolation of K' to 1M NaCl yielded a small value, K' = 5 +/- 2 M-1. Thus the binding of H1 is essentially electrostatic, being compatible with its independence of temperature. A calculation of K' based on the counterion release reproduced the salt concentration dependence of K'. Therefore, the binding of H1 is of an electrostatic territorial type. Thus, H1 may move along the DNA chain to a certain extent, when both salt concentration and the degree of saturation are sufficiently low. The condition is so restricted that the sliding would not play an important role in vivo. It was concluded from the DNA concentration independent binding isotherm that H1 can cooperatively bind onto a single DNA molecule. A simple power law dependence of the cooperativity parameter q upon NaCl concentration was found; q oc[NaCl]h with h = 0.72, though the physical basis of this dependence remains unknown.     

Quantitative study of secondary structure of histones H1, H2A, and H4 in solution by infrared spectroscopy.

The secondary structure of histones H1, H2A, and H4 (F1, F2a2, and F2a1) has been quantitatively studied in heavy water (2H2O) solutions in a wide range of histone concentration, p2H, and concentration of sodium chloride using an improved infrared spectroscopy method. Under all conditions there are about 5--10% of alpha helix. Conditions favourable for aggregation induce formation of antiparallel pleated sheet structure to an extent of about 15% in H1 and H2A and about 30% in H4. When the p2H and concentration of NaCl are in the physiological range, there is the same content of this structure in H2A and H4 and none in H1.     

Specific interaction of histone H1 with eukaryotic DNA.

The interaction of calf thymus histone H1 with homologous and heterologous DNA has been studied at different ionic strengths. It has been found that about 0.5 M NaCl histone H1, and its fragments N-H1 (residues 1-72) and C-H1 (residues 73-C terminal), precipitate selectively a small fraction of calf thymus DNA. This selective precipitation is preserved up to very high values (less than 2.0) of the input histone H1/DNA ratio. The percentage of DNA insolubilized by histone H1 under these ionic conditions is dependent upon the molecular weight of the nucleic acid, diminishing from 18% fro a Mw equals 1.0 x 10(7) daltons to 5% for a Mw equals 8.0 x 10(4) daltons. The base composition of the precipitated DNA is similar to that of the bulk DNA. Calf thymus histone H1 also selectively precipitates a fraction of DNA from other eukaryotes (herring, trout), but not from some prokaryotes (E. coli, phage gamma. On the other hand, at 0.5 M NaCl, the whole calf thymus DNA (but not E. coli DNA) presents a limited number of binding sites for histone H1, the saturation ratio histone H1 bound/total DNA being similar to that found in chromatin. A similar behavior is observed from the histone H1 fragments, N-H1 and C-H1, which bind to DNA in complementary saturation ratios. It is suggested that in eukaryotic organisms histone H1 molecules maintain specific interactions with certain DNA sequences. A fraction of such specific complexes could act as nucleation points for the high-order levels of chromatin organization.     

Histone H1--DNA interaction. On the mechanism of DNA strands crosslinking by histone H1.

Crosslinking of DNA fibers by histone H1 or phosphorylated on Ser-37 histone H1, and by the individual fragments of the H1 polypeptide chain was studied by the method of turbidimetry. The dependence of the turbidity of DNA-protein complexes on the ionic strength in solution suggests that the condensation of H1.DNA complexes in vitro is apparently due to both specific histone-DNA interactions with the contribution of hydrogen and/or hydrophobic bonds and the formation of polycationic "bridges" fastening the DNA fibers. The effectiveness of the condensation is postulated to be a function of a proportion between the two mechanisms which in turn can be controlled by slight changes in ionic surroundings. The sharp dependence of shrinkage of H1.DNA complexes on ionic strength at "physiological" salt concentrations could provide a mechanism to regulate density and consequently the total activity of chromatin in the cell nuclei. The phosphorylation of histone H1 on Ser-37 by a specific histone kinase does not noticeably affect the pattern of DNA crosslinking by the H1.     

Salt-dependent co-operative interaction of histone H1 with linear DNA

The nature of the complexes formed between histone H1 and linear double-stranded DNA is dependent on ionic strength and on the H1 : DNA ratio. At an input ratio of less than about 60% (w/w) H1 : DNA, there is a sharp transition from non-co-operative to co-operative binding at a critical salt concentration that depends on the DNA size and is in the range 20 to 50 mM-NaCl. Above this critical ionic strength the H1 binds to only some of the DNA molecules leaving the rest free, as shown by sedimentation analysis. The ionic strength range over which this change in behaviour occurs is also that over which chromatin folding is induced. Above the salt concentration required for co-operative binding of H1 to DNA, but not below it, H1 molecules are in close proximity as shown by the formation of H1 polymers upon chemical cross-linking. The change in binding mode is not driven by the folding of the globular domain of H1, since this is already folded at low salt in the presence of DNA, as indicated by its resistance to tryptic digestion. The H1-DNA complexes at low salt, where H1 is bound distributively to all DNA molecules, contain thickened regions about 6 nm across interspersed with free DNA, as shown by electron microscopy. The complexes formed at higher salt through co-operative interactions are rods of relatively uniform width (11 to 15 nm) whose length is about 1.6 times shorter than that of the input DNA, or are circular if the DNA is long enough. They contain approximately 70% (w/w) H1 : DNA and several DNA molecules. These thick complexes can also be formed at low salt (15 mM-NaCl) when the H1 : DNA input ratio is sufficiently high (approximately 70%).     

Self-assembled pearling structure of long duplex DNA with histone H1.

We report that complexes of giant DNA molecules with histone H1 proteins form a pearl necklace-like structure when the complexes are prepared by natural dilution from a high-salt solution (2 M NaCl) to a low-salt solution (0.2 M and 50 mM NaCl). We performed real-time observations on the conformational changes of individual T4 phage DNA (166 kb) molecules in bulk solution by fluorescence microscopy. To identify H1-binding regions on individual DNA molecules, we also performed immunofluorescence microscopic observations on the DNA-H1 complex spread on a glass surface. It was found that histone H1 binds DNA in a highly co-operative manner and is accompanied by local folding of the DNA. On the basis of the experimental observations and a theoretical simulation, we propose a self-assembling mechanism for the pearling structure.     

Cooperative interaction of the C-terminal domain of histone H1 with DNA

We have studied the interaction of the isolated C-terminal domain of histone H1 with linear DNA using precipitation curves and electron microscopy. The C-terminal domain shows a salt-dependent transition towards cooperative binding, which reaches completion at 60 mM NaCl. At this salt concentration, the C-terminal domain binds to some of the DNA molecules, leaving the rest free. A binding site of 22 base-pairs can be calculated from the stoichiometry of the precipitated fractions. The C-terminal domain condenses the DNA in toroidal particles. The average inner radius of the particles is of the order of 195 A. Consideration of the value of the inner radius of the toroids in the light of counterion condensation theory suggests that in these complexes the isolated C-terminal domain is capable of nearly full electrostatic neutralization of the DNA phosphate charge.     

Phosphorylation of the carboxy-terminal domain of histone H1: effects on secondary structure and DNA condensation

Linker histone H1 plays an important role in chromatin folding. Phosphorylation by cyclin-dependent kinases is the main post-translational modification of histone H1. We studied the effects of phosphorylation on the secondary structure of the DNA-bound H1 carboxy-terminal domain (CTD), which contains most of the phosphorylation sites of the molecule. The effects of phosphorylation on the secondary structure of the DNA-bound CTD were site-specific and depended on the number of phosphate groups. Full phosphorylation significantly increased the proportion of β-structure and decreased that of α-helix. Partial phosphorylation increased the amount of undefined structure and decreased that of α-helix without a significant increase in β-structure. Phosphorylation had a moderate effect on the affinity of the CTD for the DNA, which was proportional to the number of phosphate groups. Partial phosphorylation drastically reduced the aggregation of DNA fragments by the CTD, but full phosphorylation restored to a large extent the aggregation capacity of the unphosphorylated domain. These results support the involvement of H1 hyperphosphorylation in metaphase chromatin condensation and of H1 partial phosphorylation in interphase chromatin relaxation. More generally, our results suggest that the effects of phosphorylation are mediated by specific structural changes and are not simply a consequence of the net charge.     

A study of the structure of human complement component factor H by Fourier transform infrared spectroscopy and secondary structure averaging methods

Fourier transform infrared spectroscopy was used to investigate the secondary structure of human complement component factor H in H2O and 2H2O buffers. The spectra show a broad amide I band which after second-derivative calculations is shown to be composed of three components at 1645, 1663, and 1685 cm-1 in H2O and at 1638, 1661, and 1680 cm-1 in 2H2O. The frequencies of these components are consistent with the existence of an extensive antiparallel beta-strand secondary structure. The exchange properties of the amide protons of factor H as measured in 2H2O buffers are rapid and lead to an estimate of NH proton nonexchange that is comparable with those for small globular proteins. Human factor H is constructed from a linear sequence of 20 short consensus repeats with a mean of 61 residues in each one. To investigate the secondary structure further, secondary structure predictions were carried out on the basis of an alignment scheme for 101 sequences for these repeats as found in human factor H and 12 other proteins. These predictions were averaged in order to improve the reliability of the calculations. Both the Robson and the Chou-Fasman methods indicate significant beta-structural contents. Residues 21-51 in the 61-residue repeat show a clear prediction of four strands of beta-structure and four beta-turns. A structural model based on antiparallel beta-strands in the secondary structure is proposed and discussed.(ABSTRACT TRUNCATED AT 250 WORDS)     

DNA-induced secondary structure of the carboxyl-terminal domain of histone H1

We have studied the secondary structure of the carboxyl-terminal domains of linker histone H1 subtypes H1(0) (C-H1(0)) and H1t (C-H1t), free in solution and bound to DNA, by IR spectroscopy. The carboxyl-terminal domain has little structure in aqueous solution but becomes extensively folded upon interaction with DNA. The secondary structure elements present in the bound carboxyl-terminal domain include the alpha-helix, beta-structure, turns, and open loops. The structure of the bound domain shows a significant dependence on salt concentration. In low salt (10 mm NaCl), there is a residual amount of random coil, 7% in C-H1(0) and 12% in C-H1t. In physiological salt concentrations (140 mm NaCl), the carboxyl termini become fully structured. Under these conditions, C-H1(0) contained 24% alpha-helix, 25% beta-structure, 17% open loops, and 33% turns. The latter component could include a substantial proportion of the 3(10) helix. Despite their low sequence identity (approximately 30%), the representation of the different structural motifs in C-H1t was similar to that in C-H1(0). Examination of the changes in the amide I components in the 20-80 degrees C temperature interval showed that the secondary structure of the DNA-bound C-H1t is for the most part extremely stable. The H1 carboxyl-terminal domain appears to belong to the so-called disordered proteins, undergoing coupled binding and folding.     

Effect of magnesium ions on the structure of DNA thin films: an infrared spectroscopy study

Utilizing Fourier transform infrared spectroscopy we have investigated the vibrational spectrum of thin dsDNA films in order to track the structural changes upon addition of magnesium ions. In the range of low magnesium concentration ([magnesium]/[phosphate] = [Mg]/[P] < 0.5), both the red shift and the intensity of asymmetric PO₂ stretching band decrease, indicating an increase of magnesium-phosphate binding in the backbone region. Vibration characteristics of the A conformation of the dsDNA vanish, whereas those characterizing the B conformation become fully stabilized. In the crossover range with comparable Mg and intrinsic Na DNA ions ([Mg]/[P] ≈ 1) B conformation remains stable; vibrational spectra show moderate intensity changes and a prominent blue shift, indicating a reinforcement of the bonds and binding in both the phosphate and the base regions. The obtained results reflect the modified screening and local charge neutralization of the dsDNA backbone charge, thus consistently demonstrating that the added Mg ions interact with DNA via long-range electrostatic forces. At high Mg contents ([Mg]/[P] > 10), the vibrational spectra broaden and show a striking intensity rise, while the base stacking remains unaffected. We argue that at these extreme conditions, where a charge compensation by vicinal counterions reaches 92–94%, DNA may undergo a structural transition into a more compact form.     

Monitoring of secondary and tertiary structure changes in the gastric H+/K+-ATPase by infrared spectroscopy.

Conformational changes occurring in the catalytic cycle of the H+/K+-ATPase were monitored by Fourier transform infrared spectroscopy (FTIR). Caged compounds were used to release ATP, in the presence of Ca2+, to induce the transition between the E1 and E1-P conformation of the H+/K+-ATPase. In addition to bands associated with the photolysis of the caged compounds, some peaks of the difference infrared spectra were associated with changes in secondary structure and modifications of the ionization in the side chains of amino-acid residues (Glu or Asp). These changes were specific to the reaction between the ligand and the enzyme. We estimated that 39 amino acids changed their secondary structure during the reaction and four amino-acid residues were deprotonated. Similar spectral changes appeared when ADP was released from its precursor. The release of Pi from the same caged molecule did not induce similar changes. Changes in tertiary structure occurring during the binding of adenosine and phosphorylation of the enzyme were demonstrated by recording hydrogen/deuterium exchange kinetics by attenuated total reflectance FTIR spectroscopy (ATR-FTIR). At least 129 amide protons were involved in a tertiary structure change induced by ATP. This suggested that secondary structure change transduced a much larger tertiary structure modification.     

Quantitation of secondary structure in ATR infrared spectroscopy

Polarized attenuated total reflection infrared spectroscopy of aligned membranes provides essential information on the secondary structure content and orientation of the associated membrane proteins. Quantitation of the relative content of different secondary structures, however, requires allowance for geometric relations of the electric field components (E(x), E(y), E(z)) of the evanescent wave, and of the components of the infrared transition moments, in combining absorbances (A() and A( perpendicular)) measured with radiation polarized parallel with and perpendicular to, respectively, the plane of incidence. This has hitherto not been done. The appropriate combination for exact evaluation of relative integrated absorbances is A() + (2E(z)(2)/E(y)(2) - E(x)(2)/E(y)(2))A( perpendicular), where z is the axis of ordering that is normal to the membrane plane, and the x-axis lies in the membrane plane within the plane of incidence. This combination can take values in the range approximately from A() - 0.4A( perpendicular) to A() + 2.7A( perpendicular), depending on experimental conditions and the attenuated total reflection crystal used. With unpolarized radiation, this correction is not possible. Similar considerations apply to the dichroic ratios of multicomponent bands, which are also treated.     

Secondary structure of calf-thymus histone H1 by means of 13C-NMR spectroscopy

¹³C-nmr spectroscopy was used to determine the location of the structured segment of the chain of histone H1 in water and NaCl solutions. The segment found (41–89) is contained in the area proposed by others on the basis of ¹H-nmr studies. The number of basic groups left in the mobile ends of the protein matches the number of bases of internucleosomal DNA.     

Fourier transform infrared evidence for a predominantly alpha-helical structure of the membrane bound channel forming COOH-terminal peptide of colicin E1.

The structure of the membrane bound state of the 178-residue thermolytic COOH-terminal channel forming peptide of colicin E1 was studied by polarized Fourier transform infrared (FTIR) spectroscopy. This fragment was reconstituted into DMPC liposomes at varying peptide/lipid ratios ranging from 1/25-1/500. The amide I band frequency of the protein indicated a dominant alpha-helical secondary structure with limited beta- and random structures. The amide I and II frequencies are at 1,656 and 1,546 cm-1, close to the frequency of the amide I and II bands of rhodopsin, bacteriorhodopsin and other alpha-helical proteins. Polarized FTIR of oriented membranes revealed that the alpha-helices have an average orientation less than the magic angle, 54.6 degrees, relative to the membrane normal. Almost all of the peptide groups in the membrane-bound channel protein undergo rapid hydrogen/deuterium (H/D) exchange. These results are contrasted to the alpha-helical membrane proteins, bacteriorhodopsin, and rhodopsin.     

Electron microscopic study of compactization of individual DNA molecules in films during the interaction with histone H1]

The protein-free method was applied for the investigation of histone H1 DNA complexes formation. The main advantage of this method is the possibility to get intramolecular compact structures at interaction of individual spread molecules of DNA with histone H1. It was shown that in the presence of 0.2-5 micrograms/ml of histone H1 in hypophase there are three types of structures on electronmicroscopic preparations: fibres of non-compacted DNA, compact fibres with twisted strands of duplex DNA and compacted rod-like and circular structures where separate fibres of duplex DNA could not be distinguished. The study of compact structures morphology allows to conclude that they are formed by side-by-side association of DNA fibres, as it takes place in the case of triple rings formation at the compactization of circular DNA due to trivaline binding. At increasing ionic strength there is a tendency for transition from second type structures to the third type structures. The latter can be explained by transition from non-cooperative to cooperative binding of histone H1 to DNA.     

Studies on the interaction of H1 histone with superhelical DNA: characterization of the recognition and binding regions of H1 histones.

The very lysine rich histone, H1, isolated from a variety of sources interacts preferentially with superhelical DNA compared to relaxed DNA duplexes. The nature of this specific interaction has been investigated by studying the ability of various purified fragments of H1 histone from calf thymus to recognize and bind superhelical DNA. The data suggest that the globular region of the H1 histone molecule (amino acid residues 72-106) is involved in the recognition of superhelical DNA. Thus, the H1 histone carboxy-terminal fragment, 72-212, resembles native H1 histone both quantitatively and qualitatively in its ability to discriminate between and bind to superhelical and relaxed DNA while the H1 histone carboxy-terminal fragment, residues 106-212, has lost this specificity, binding superhelical and relaxed DNA equally well. Furthermore, under conditions in which the globular region of the intact H1 histone has been unfolded, the molecule loses its ability to discriminate between superhelical and relaxed DNA, and binds both forms of DNA equally.     

Labelling of histone H5 and its interaction with DNA. 1. Histone H5 labelling with fluorescein isothiocyanate

Histone H5 has been labelled with fluorescein isothiocyanate (FITC) with particular attention to the reaction conditions (pH, reaction time and input FITC/H5 molar ratio) and to the complete elimination of non-covalently bound dye. We preferred to use reaction conditions which yielded non-specific uniform labelling rather than specific alpha-NH2 terminal labelling, in order to obtain higher sensitivity in further studies dealing with the detection of perturbation at the binding sites of H5 on DNA. FITC-labelled H5 was further characterized by absorption and circular dichroism spectroscopy, and the fluorescein probe titrated in the 4-8 pH range. The structural integrity of H5 was found to be preserved after labelling. The positive electrostatic potential of the environment in which the FITC probe is embedded in the arginine/lysine-rich tails of H5 is believed to be responsible for the drop of pK of 1 unit found for H5-FITC as compared to free FITC. For the globular part of H5, the pK of covalently-bound FITC was only slightly lowered; this is a consequence of the much lower content in positively-charged amino-acid side chains in this region.     

Secondary structure of protamine in sperm nuclei: an infrared spectroscopy study

Background  

Protamines are small basic proteins that condense the DNA in mature spermatozoa. Typical protamines are of simple composition and very arginine-rich, usually in the range of 60-80%. Arginine residues are distributed in a number of stretches separated by neutral amino acids. We have used Fourier transform infrared spectroscopy (FTIR) to gain access for the first time to the secondary structure of protamines in sperm nuclei. This technique is particularly well suited to the study of DNA-bound protamine in whole nuclei since it is not affected by turbidity.     

Sequence-specific interaction of Hoechst 33258 with the minor groove of an adenine-tract DNA duplex studied in solution by 1H NMR spectroscopy.

The interaction of Hoechst 33258 with the minor groove of the adenine-tract DNA duplex d(CTTTTGCAAAAG)2 has been studied in both D2O and H2O solutions by 1D and 2D 1H NMR spectroscopy. Thirty-one nuclear Overhauser effects between drug and nucleotide protons within the minor groove of the duplex, together with ring-current induced perturbations to the chemical shifts of basepair and deoxyribose protons, define the position and orientation of the bound dye molecules. Two drug molecules bind cooperatively and in symmetry related orientations at the centre of the 5'-TTTT and 5'-AAAA sequences with the binding interactions spanning only the four A-T basepairs. The positively charged N-methylpiperazine moieties point towards the centre of the duplex while the phenol groups are disposed towards the 3'-ends of the sequence. Resonance averaging is apparent for both the D2/D6 and D3/D5 phenol protons and D2"'/D6"' and D3"'/D5"' of the N-methylpiperazine ring and is consistent with these groups being involved in rapid rotation or ring-flipping motions in the bound state. Interstrand NOEs between adenine H2s and deoxyribose H1' are consistent with a high degree of propeller twisting of the A-T basepairs at the binding site of the aromatic benzimidazole and phenol rings of Hoechst. The data imply that the minor groove is particularly narrow with many contacts between the complementary curved surfaces of the drug and DNA indicating that strong van der Waals interactions, involving the floor and the walls of the minor groove, stabilize the complex. In our model the NH groups of the benzimidazole rings are positioned to make a pair of bifurcated hydrogen bonds with the adenine N3 and thymine O2 on the floor of the minor groove.