Conformation of DNA in chromatin reconstituted from poly [d(A-T)] and the core histones.

Present results provide direct evidence of the nature of a conformational change in DNA when nucleosomes are formed from core histones and poly [d(A-T)]. First, we have found some features which have characteristic aspects of the A like conformation of DNA. Thus, an increased contribution due to a sugar conformation close to C3'-endo puckering is detected in the Raman spectra. In addition, the circular dichroism (C.D.) spectra of reconstituted chromatin with poly [d(A-T)] exhibits an increases intensity at about 262 nm. A second feature acquired by poly [d(A-T)] in nucleosome formation from core histones is related to the presence of a negative band at about 280 nm in the C.D.spectra. The nature of this change is correlated with a DNA conformation characterized by a decreased number of base pairs per turn (28,29). This indicates that these two features of reconstituted nucleosomes reflect the presence of two types of DNA conformations, which overall form is of the B type (22,36).     

A comparison of the circular dichroism spectra of synthetic DNA sequences of the homopurine . homopyrimidine and mixed purine- pyrimidine types.

We have obtained the ultraviolet circular dichroism spectra of two repeating trinucleotide DNAs, poly [d(A-G-G).d(C-C-T)] and poly[d(A-A-G).d(C-T-T)], that have all purines on one strand and all pyrimidines on the other. These spectra, together with spectra of other synthetic polymers, can be combined to give 3 first-neighbor calculations of the spectrum of poly[d(A).d(T)] and 2 first-neighbor calculations of the spectrum of poly [d(G).d(C)]. The results show (1) that first-neighbor calculations utilizing only spectra of homopurine.homopyrimidine DNA sequences are no more accurate than are similar calculations that involve spectra of mixed purine-pyrimidine sequences, demonstrating that double-stranded homopurine.homopyrimidine sequences do not obviously belong to a special class of secondary conformations, and (2) that the wavelength region above 250 nm in the CD spectra of synthetic DNAs is least predictable from first-neighbor equations, probably because this region is especially sensitive to sequence-dependent conformational differences.     

Specificity of the binding of fd gene 5 protein to polydeoxyribonucleotides

The long-wavelength circular dichroism (CD) changes induced by binding of fd gene 5 protein to the alternating DNA sequences poly[d(A-C)] and poly[d(C-T)] were similar to those induced by the protein complexed with the homopolymers poly[d(A)], poly[d(C)], and poly[d(T)]. The fd gene 5 protein showed different binding affinities for the various polymers. The affinity for the alternating sequences was not compositionally weighted with respect to the affinities for the homopolymers, indicating that both base composition and base sequence of the template are important for the binding of fd gene 5 protein.     

Specificity of the Binding of fd Gene 5 Protein to Polydeoxyribonucleotides

Abstract

The long-wavelength circular dichroism (CD) changes induced by binding of fd gene 5 protein to the alternating DNA sequences poly[d(A-C)] and poly [d(C-T)] were similar to those induced by the protein complexed with the homopolymers poly[d(A)], poly[d(C)], and poly[d(T)]. The fd gene 5 protein showed different binding affinities for the various polymers. The affinity for the alternating sequences was not compositionally weighted with respect to the affinities for the homopolymers, indicating that both base composition and base sequence of the template are important for the binding of fd gene 5 protein.     

Base tilt of poly[d(A)]-poly[d(T)] and poly[d(AT)]-poly[d(AT)] in solution determined by linear dichroism

We have measured the CD, isotropic absorption, and LD of poly[d(A)]–poly[d(T)] and poly[d(AT)]–poly[d(AT)] in the vacuum-uv spectral region. The reduced dichroism (LD divided by isotropic absorption) varied as a function of wavelength and was independent of shear gradient. Thus, the bases are not perpendicular to the helix axis in solution. Since the directions of the transition dipoles are known, the orientations of the bases in the polymers can be calculated from the reduced dichroism spectra. The results show that the base normals are tilted at angles greater than 25°, with respect to the helix axis, and thymine is tilted more than adenine for both polymers. The tilt axes of adenine and thymine are not parallel, indicating a large propeller twist. Space-filling models of poly[d(A)]–poly[d(T)] and poly[(AT)]–poly[d(AT)] are built based on our results, and the conformations of the two (A + T) polymers in solution are discussed.     

A model chromatin assembly system. Factors affecting nucleosome spacing

Poly[d(A-T)].poly[d(A-T)], when reconstituted with chicken erythrocyte core histones and subsequently incubated with sufficient histone H5 in a solution containing polyglutamic acid, forms structures resembling chromatin. H5 induces nucleosome alignment in about two hours at physiological ionic strength and 37 degrees C. The nucleosome spacing and apparent linker heterogeneity in the assembled nucleoprotein are very similar to those in chicken erythrocyte chromatin. Also, condensed chromatin-like fibers on the polynucleotide can be visualized. The binding of one mole of H5 per mole of core octamer is necessary to generate the physiological nucleosome spacing, which remains constant with the addition of more H5. The nucleosome repeat length is not a function of the core histone to poly[d(A-T)] ratio for values lower than the physiological ratio. With increasing ratios, in excess of the physiological value, nucleosome spacing first becomes non-uniform, and then takes on the close packing limit of approximately 165 base-pairs. In addition to eliminating possible base sequence effects on nucleosome positioning, poly[d(A-T)] allows nucleosomes to slide more readily than does DNA, thereby facilitating alignment. Evidence is presented that polyglutamic acid facilitates the nucleosome spacing activity of histone H5, primarily by keeping the nucleoprotein soluble. This model system should be useful for understanding how different repeat lengths arise in chromatin.     

Assembly and characterization of nucleosomal cores on B- vs. Z-form DNA

The ability of right- vs. left-handed alternating purine/pyrimidine copolymers to support the formation of nucleosomes has been examined by using a trout testis assembly factor. The protein, which is thermostable, has a molecular weight of 29000 and will assemble nucleosomes onto both SV40 and calf thymus DNA. This assembly factor has been used to assemble nucleosomes onto the B and Z conformations of poly[d(Gm5C)] and the B conformation of poly[d(GC)]. The isolated B-form particles, which sediment at approximately 11 S in a sucrose density gradient, contain DNA of 140-200 bases in length and the four core histones. The isolated Z-form particles, which also sediment at approximately 11 S, contain the four core histones and DNA of 170-250 bases in length. Physical analysis of the particles by absorbance and circular dichroic spectroscopy indicates that the DNA remains in the original conformation throughout the isolation procedure. Further, the particles reconstituted onto left-handed DNA compete effectively for an anti-Z DNA antibody, while the corresponding right-handed particles do not. Analytical sedimentation velocity determinations indicate that the B-form poly[d(Gm5C)] and poly[d(GC)] particles sediment at 11.2 and 11.1 S, respectively. In contrast, the poly[d(Gm5C)] Z-form particles have an S20,w of 10.6 S. The differences in the sedimentation velocity and the density of the cores, and in the lengths of DNA associated with the particles, suggest that the conformation of the DNA affects the manner in which it associates with the histone octamer.     

A reexamination of the reported B----Z DNA transition in nucleosomes reconstituted with poly(dG-m5dC).poly(dG-m5dC)

Polynucleosomes with poly(dG-m5dC).poly(dG-m5dC) have been reconstituted, and well-defined nucleosome core particles from these have been prepared. Upon addition of MgCl2 to the levels used to induce the B to Z transition in this highly methylated DNA, significant changes in the circular dichroism spectrum are observed in solutions of these particles. However, such core particles also exhibit a noticeable instability when compared to chicken erythrocyte core particles under the same conditions. The change in circular dichroism can be entirely accounted for on the assumption that only free nucleotide, released by core particle dissociation, undergoes the B----Z transition. Therefore, no evidence has been found for "Z nucleosomes" in these solutions. In fact, the histone-DNA interaction in the nucelosome seems to partially inhibit the B to Z transition of the DNA. The analysis of our results is consistent with a model in which all of the DNA that remains bound to the histone octamer retains the B form.     

The analysis of circular dichroism spectra of natural DNAs using spectral components from synthetic DNAs

We have tested 21 different basis sets of synthetic DNA circular dichroism spectra and have slected one for use in spectral analyses of natural DNAs. This “standard” set consists of spectra of eight polymers: poly[d(A-A-T)·d(A-T-T)], poly[d(A-G-G)·d(C-C-T)], poly[d(A-T)·d(A-T)], poly[d(G-C)·d(G-C)], poly[d(A-G)·d(C-T)], poly[d(A-C)·d(G-T)], poly[d(A-T-C)·d(G-A-T)], and poly[d(A-G-C)·d(G-C-T)]. This basis set, applied according to the first-neighbor polymer procedure of Gray and Tinoco, allows a more uniformly accurate spectral analysis of six natural complex DNAs and eight (A+T)-rich satellite DNAs for base composition and first-neighbor frequencies than was previously possible. We find that spectra of poly[d(A)·d(T)] and/or poly[d(A-C-T-)·d(A-G-T)] are not generally required for good analysis results but we show in this and the following paper that these spectra are needed for the most accurate analyses of some satellite DNAs.     

Nucleosome reconstitution of core-length poly(dG).poly(dC) and poly(rG-dC).poly(rG-dC)

The double-stranded polypurine.polypyrimidines poly(dG).poly(dC) and poly[d(A-G)].poly[d(T-C)] and the mixed ribose-deoxyribose polynucleotide poly(rG-dC).poly(rG-dC) have been successfully reconstituted into nucleosomes. The radioactively labeled particles comigrate in gel electrophoresis and sucrose density gradient experiments with authentic nucleosomes derived from chicken erythrocyte chromatin. These results show that nucleosomes are able to accommodate a wider variety of polynucleotides than was previously believed.     

Nonhistone nuclear high mobility group proteins 14 and 17 stabilize nucleosome core particles

Nucleosome core particles form well defined complexes with the nuclear nonhistone proteins HMG 14 or 17. The binding of HMG 14 or 17 to nucleosomes results in greater stability of the nucleosomal DNA as shown by circular dichroism and thermal denaturation. Under appropriate conditions the binding is cooperative, and cooperativity is ionic strength dependent. The specificity and cooperative transitions of high mobility group (HMG) binding are preserved in 1 M urea. Specificity is lost in 4 M urea. Thermal denaturation and circular dichroism show a dramatic reversal of the effects of urea on nucleosomes when HMG 14 or 17 is bound, indicating stabilization of the nucleosome by HMG proteins. Complexes formed between reconstructed nucleosomes containing purified inner histones plus poly(dA-dT) and HMG 14 or 17 demonstrate that the HMG binding site requires only DNA and histones. Electron microscopy reveals no major structural alterations in the nucleosome upon binding of HMG 14 or 17. Cross-linking the nucleosome extensively with formaldehyde under cooperative HMG binding conditions does not prevent the ionic strength-dependent shift to noncooperative binding. This suggests mechanisms other than internal nucleosome conformational changes may be involved in cooperative HMG binding.     

Circular dichroism evidence for G·U and G·T base pairing in poly[r(G-U)] and poly[d(G-T)]

We have measured the circular dichroism (CD) and absorption properties of poly[r(G-U)] and poly [d(G-T)] over a wide range of Na⁺ concentrations and temperatures. We find evidence for self-complexed forms of these polymers at lower temperatures and/or higher Na⁺ concentrations than generally needed for double-strand formation in other DNA and RNA polymers. These self-complexes could be composed of double-stranded regions with weak G·U or G·T base pairs.     

Poly(dA).poly(dT) rich sequences are not sufficient to exclude nucleosome formation in a constitutive yeast promoter.

It was suggested that poly(dA).poly(dT) rich sequences in yeast Saccharomyces cerevisiae act as elements of constitutive promoters by exclusion of nucleosomes (Struhl, K. (1985). Proc. Natl. Acad. Sci. USA 82, 8419-8423). We have mapped the chromatin structure of the pet56-his3-ded1 region in minichromosomes and show that the poly(dA).poly(dT) sequences are located in nuclease sensitive regions. DNA fragments from the nuclease sensitive promoter region of DED1 were used for nucleosome reconstitution in vitro. We show that all sequences can form nucleosome cores and that the poly(dA).poly(dT) sequence can be incorporated in nucleosome cores. The results suggest that the nuclease sensitivity found in vivo is not established by poly(dA).poly(dT) mediated exclusion of nucleosomes.     

The vacuum UV CD bands of repeating DNA sequences are dependent on sequence and conformation

CD spectra were obtained for eight synthetic double-stranded DNA polymers down to at least 175 nm in the vacuum uv. Three sets of sequence isomers were studied: (a) poly[d(A-C).d(G-T)] and poly[d(A-G).d(C-T)], (b) poly[d(A-C-C).d(G-G-T)] and poly[d(A-C-G).d(C-G-T)], and (c) poly[d(A).d(T)], poly[d(A-T).d(A-T)], poly[d(A-A-T).d(A-T-T)], and poly[d(A-A-T-T).d(A-A-T-T)]. There were significant differences in the CD spectra at short wavelengths among each set of sequence isomers. The (G.C)-containing sequences had the largest vacuum uv bands, which were positive and in the wavelength range of 180-191 nm. There were no large negative bands at longer wavelengths, consistent with the polymers all being in right-handed conformations. Among the set of sequences containing only A.T base pairs, poly[d(A).d(T)] had the largest vacuum uv CD band, which was at 190 nm. This CD band was not present in the spectra of the other (A.T)-rich polymers and was absent from two first-neighbor estimations of the poly[d(A).d(T)] spectrum obtained from the other three sequences. We concluded that the sequence dependence of the vacuum uv spectra of the (A.T)-rich polymers was due in part to the fact that poly[d(A).d(T)] exists in a noncanonical B conformation.     

Vacuum UV CD spectra of homopolymer duplexes and triplexes containing A.T or A.U base pairs.

Vacuum UV circular dichroism (CD) spectra were measured down to 174 nm for five homopolymers, five duplexes, and four triplexes containing adenine, uracil, and thymine. Near 190 nm, the CD bands of poly[d(A)] and poly[r(A)] were larger than the CD bands of the polypyrimidines, poly[d(T)], poly[d(U)], and poly[r(U)]. Little change was observed in the 190 nm region upon formation of the duplexes (poly[d(A).d(T)], poly[d(A).d(U)], poly[r(A).d(T)], poly[r(A).d(U)], and poly[r(A).r(U)]) or upon formation of two of the triplexes (poly[d(T).d(A).d(T)] and poly[d(U).d(A).d(U)]). This showed that the purine strand had the same or a similar structure in these duplexes and triplexes as when free in solution. Both A.U and A.T base pairing induced positive bands at 177 and 202 nm. For three triplexes containing poly[d(A)], the formation of a triplex from a duplex and a free pyrimidine strand induced a negative band centered between 210 and 215 nm. The induction of a band between 210 and 215 nm indicated that these triplexes had aspects of the A conformation.     

Elsamicin A can convert the Z-form of poly[d(G-C)] and poly[(G-m5C)] back to B-form DNA.

The interaction of poly[(G-C)] and poly[d(G-m5C)] with the antitumor antibiotic elsamicin A, which binds to alternating guanine + cytosine tracts in DNA, has been studied under the B and Z conformations. Both the rate and the extent of the B-to-Z transition are diminished by the antibiotic, as inferred by spectroscopic methods under ionic conditions that otherwise favor the left-handed conformation of the polynucleotides. Moreover, elsamicin converts the Z-form DNA back to the B-form. The circular dichroism data indicate that elsamicin binds to poly[d(G-C)] and poly[d(G-m5C)] to form a right-handed bound elsamicin region(s). The transition can be followed by changes of the molar ellipticity at 250 nm, thus providing a convenient wavelength to monitor the Z-to-B conformational change of the polymers as elsamicin is added. The elsamicin A effect might be explained by a model in which the antibiotic binds preferently to a B-form DNA, playing a role as an allosteric effector on the equilibrium between the B and Z conformations, thus favoring the right-handed one.     

Nucleosome core particles of calf thymus, Tetrahymena, and the reconstituted hybrid. Their structure reflects the nature of the histone octamer

The circular dichroism spectra and the thermal denaturation profiles of the nucleosome core particles isolated by micrococcal nuclease digestion from nuclei of calf thymus and the protozoan Tetrahymena pyriformis were compared with those of the homogeneous and hybrid core particles reconstituted from calf core DNA and either calf or Tetrahymena histone octamer. The core DNA was obtained from the calf core particle, and both the histone octamers were reconstituted from the acid-extracted four core histones of calf thymus or Tetrahymena, whose amino acid sequences show the largest differences hitherto known. The reconstituted homogeneous core particle was identical in both the physical properties with the isolated calf core particle, showing that the correct reconstitution was achieved. The circular dichroism spectra of the calf and Tetrahymena core particles and the hybrid core particle showed no essential differences, indicating that the three core particles have the same overall structure. The derivative thermal-denaturation profiles, however, clearly differed; the calf core particle showed two melting transitions at 60 degrees C and 72 degrees C, while the Tetrahymena and hybrid core particles showed the same three transitions at 48-50 degrees C, 60-61 degrees C, and 72 degrees C. Thus, the thermal denaturation properties of nucleosome core particles do not reflect the nature of DNA, but rather that of the histone octamer bound to the DNA. We conclude that the Tetrahymena histones are more weakly bound to the DNA than the calf thymus histones in the same overall structure of nucleosomes.     

CD of six different conformational rearrangements of poly[d(A-G).d(C-T)] induced by low pH.

On the basis of circular dichroism (CD) data, we have now identified six different conformational states (other than the duplex) of poly[d(A-G).d(C-T)] at pH values between 8 and 2.5 (at 0.01M Na+; 20 degrees C). Three of these structural rearrangements were observed as the pH was lowered from 8 to 2.5, and three additional rearrangements were observed as the pH was raised from 2.5 back to neutral pH. The major components of the six conformational states were defined using appropriate combinations of the CD spectra of the duplex, triplex, and denatured forms of this polymer, as well as the CD spectra of the individual single strands and their respective acid-induced self-complexes. Our results show that the acid-induced rearrangements of poly[d(A-G).d(C-T)] include not only the poly[d(C+-T).d(A-G).d(C-T)] triplex, but also include the poly[d(C-T)] loop-out structure and a self-complexed form of the poly[d(A-G)] strand that is pH-dependent.     

Vacuum UV circular dichroism is diagnostic for the left-handed Z form of poly [d(A-C).d(G-T)] and other polydeoxynucleotides.

Circular dichroism spectra are extended into the vacuum UV to about 178 nm for four polydeoxynucleotides of various sequences capable of assuming the left-handed Z form. It is found that each of these polymers, including those with brominated bases and those with the four different bases, have a characteristic negative feature at short wavelengths when in the Z form. In contrast, the B form only has a positive band between 180 and 200 nm. Furthermore, a blue shift of the short wavelength crossover is diagnostic of the B- to Z-form transition for all polymers studied so far. These results confirm that poly[d(A-C).d(G-T)] can assume the Z form in solution at low concentration.     

Intercalative and nonintercalative binding of large cationic porphyrin ligands to polynucleotides

The interactions of two positional isomers and one analogue of meso-tetra (4-N-methylpyridyl) porphine, with the synthetic polynucleotides poly[d(A-T)] . poly[d(A-T)] and poly[d(G-C)] . poly[d(G-C)] have been investigated by circular dichroism. All four porphyrins were found to bind to the polynucleotides as shown by the induction of circular dichroism in their Soret bands. Furthermore, the sign of the induced ellipticity reflects selective occupation of binding sites by the porphyrin ligands. The conformational lability of poly[d(A-T)] X poly[d(A-T)] was found to be appreciable as micromolar amounts of meso-substituted 4-N-methylpyridyl, 3-N-methylpyridyl, and p-N-trimethylanilinium porphines induced a CD spectrum similar but not identical to that of DNA in the Z-form, i.e. a negative band at 280 nm and a positive band at 259 nm. The effect of porphyrin binding to poly[d(G-C)] X poly[d(G-C)] was less pronounced and dissimilar to that seen in the AT polymer.