Biomedical subjects
Publications and source records attributed to H J Li.
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The effects of mechanical shearing on chromatin structure were investigated by using thermal denaturation and circular dichroism (CD) spectroscopy. Under ordinary conditions of mechanical shearing used for preparation of soluble chromatin, we observed only minor changes (less than 10%) of chromatin properties with respect to (a) absorption melting curves, (b) CD spectra, (c) CD melting curves and (d) histone transfer from chromatin to exogenous DNA. Such small pertubation of structural properties could be due to the generation of free ends when a large chromatin was cut into smaller fragments and by weakening the binding of histones to DNA near these free ends. In addition to mechanical shearing, sonication was used to shear some samples of chromatin. The effect of sonication on chromatin structure was investigated by the same physical methods used for mechanically sheared chromatin. The results indicate that sonication only slightly changes the chromatin properties with respect to CD spectra, similar to the results obtained by mechanical shearing, but sonication at high settings has a greater effect on the thermal denaturation property of chromatin as contrasted to our results from mechanically sheared chromatin.
Salt induced dissociation of protamine, poly(L-lysine) and poly(L-arginine) from DNA was measured by relative light scattering at theta = 90 degrees and/or centrifugation. Dissociation of histones from DNA was studied using relative light scattering and intrinsic tyrosine fluorescence. Protamine was dissociated from DNA at 0.15 M MgCl2 (ionic strength mu = 0.45) or 0.53 M NaCl (mu = 0.53) based on light scattering data and at approximately 0.2 M MgCl2 (mu = 0.6) or 0.6 M NaCl based on centrifugation data. NaCl induced dissociation of poly(Lys) or poly(Arg) from natural DNAs measured by light scattering did not depend on the guanine plus cytosine content. To dissociate poly(Arg) from DNA higher ionic strength using NaCl, MgCl2, or CaCl2, similar ionic strength using NaClo4, and lower ionic strength using Na2SO4 was needed then to dissociated poly(Lys). Both the decrease in light scattering and the enhancement of tyrosine fluorescence of chromatin occurred between 0.5 and 1.5 M NaCl when histones were dissociated.
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Structural transition in chromatin was measured as a function of counter ions in solution (NaCl or MgCl(2)) and of histones bound on the DNA. The addition of counter ions to aqueous solutions of chromatin, partially dehistonized chromatin, and DNA caused a drastic reduction in viscosity and a significant increase in sedimentation coefficient. Transitions occurred primarily at about 2 x 10(-3) M NaCl and 1 x 10(-5) M MgCl(2) and are interpreted as a change in structure of chromatin induced by tight binding of cations (Na(+) or Mg(++)) to DNA, either free or bound by histones, and is an intrinsic property of DNA rather than of the type of histone bound. At a given ionic condition, removal of histone H1 from chromatin had only a minor effect on the hydrodynamic properties of chromatin while removal of other histones caused a drastic change in these properties. An increase in the sedimentation coefficient of DNA was observed also for protamine. DNA complexes wherein the bound protein contains only unordered coil rather than the alpha-helices found in histones.
Interaction between non-histone protein HMG1 or HMG2 and DNA has been studied by using thermal denaturation and circular dichroism (CD) spectroscopy. We have made the following observations. 1. The binding of each of these two proteins to DNA stabilizes the latter, as shown by an increase in melting temperature of 20 degrees C (from 45 degrees C to about 65 degrees C). 2. There are 6.0 amino acids/nucleotide in HMG1-bound DNA and 5.0 in HMGI-bound DNA which suggests that each HMB1 moleculae would cover about 20 base pairs of DNA and each HMG2 molecule would cover about 25 base pairs. 3. The alpha-helical content of these two non-histone proteins in the complexes, estimated from the CD value at 220 nm, is about one third to one half that of total proteins in calf thymus chromatin. 4. DNA conformation is distorted only slightly by the binding of protein HMG1 or HMG2. 5. Neither the melting nor the CD properties of HMG1-DNA or HMG2-DNA complexes differ substantially whether they are prepared by NaCl-gradient dialysis in urea or by direct mixing of protein and DNA at 0.15 M NaCl, followed by dialysis against the same buffer i.e. 0.25 mM EDTA (pH 8.0).
Histone redistributions between endogenous DNA in calf thymus chromatin and exogenous DNA from Clostridium perfringens (69% A + T) or from Micrococcus luteus (30% A + T) induced by 0.6 M NaCl or by 2% formaldehyde were studied by thermal denaturation. The observed redistribution occurred on histone Hl when the exogenous DNA was (A + T)-richer than the DNA in chromatin, and when the mixture was exposed to 0.6 M NaCl or formaldehyde. When a (G + C)-richer DNA was added as the acceptor for histones, no substantial transfer of histones from chromatin DNA to exogenous DNA was found. Thus the activation energy of histone dissociation from chromatin DNA seems to be substantially lowered by 0.6 M NaCl or formaldehyde such that histones (mostly histone Hl) can be dissociated and bind the (A + T)-richer DNA and form a more stable complex. It is suggested that the formaldehyde effect on histones may be due to the loss of positive charges on lysine and arginin residues (probably more on lysine than on arginine) in histones after their rapid reaction with formaldehyde. Formaldehyde treatment of chromatin also distorts the DNA conformation, as revealed by circular dichroism (CD) studies. This structural effect occurs mainly on those base pairs bound by histones other than Hl, or within the chromatin subunit. Histone redistribution is treated as a thermodynamic phenomenon of histone binding to DNA. The validity of using formaldehyde to study chromatin structure is discussed.
Physical properties of histone-DNA complexes very often depend upon the method of complex formation. In an attempt to make the studies of histone-DNA interactions more relevant to biological systems, results from thermal denaturation of native chromatin were used as references for determining how closely a given histone-DNA complex approaches its native state in chromatin. In the case of arginine-rich histones H3 (III or f3) and H4 (IV or f2a1), four methods were used for making complexes with calf thymus DNA: (A) NaCl gradient dialysis with urea; (B) NaCl gradient dialysis without urea; (C) direct mixing in 2.5 x 10(-4) EDTA, pH 8.0; and (D) direct mixing in 0.01 M sodium phosphate, pH 7.0. It was observed that a complex made by direct mixing in phosphate (method D) is closer to the native than is one made by direct mixing in EDTA (method C) than the one made by gradient dialysis with urea (method A) or without urea (method B). Regardless of the method used for complex formation, no substantial differences were observed between complexes with histone H3 dimer with disulfide bond(s) and a reduced H3 without disulfide bond, implying that perhaps a dimer with or without disulfide bond is a natural fundamental subunit in our experimental conditions. When the method of direct mixing in EDTA is used, the melting properties of the complexes vary only slightly with any one of the following H3 histones: from calf thymus, H3 without disulfide bond, H3 dimer, and H3 oligomer with disulfide bonds, also, from duck erythrocyte, H3 monomer and dimer. The complexes formed between DNA and a mixture of H3 and H4 by method D have melting properties similar to those of native chromatin. Since an equimolar mixture of histone H3 and H4 in 0.01 M phosphate, pH 7.0, was shown to form a tetramer (D'Anna, J.A., and Isenberg, I. (1974), Biochem. Biophys. Res. Commun. 61, 343), our results suggest that, a tetramer of H3 and H4, likely to be (H3)2(H4)2, formed from one H3 dimer and one H4 dimer, can bind DNA in a manner similar to that in native chromatin.
Circular dichroism (CD) was used to investigate the conformations of arginine-rich histones, H3 (III or f3) and H4 (IV or f2a1), and DNA in the complexes prepared by four different methods: (A) NaCl gradient dialysis with urea; (B) NaCl gradient dialysis without urea; (C) direct mixing in 2.5 x 10(-4) M EDTA, pH 8.0; and (D) direct mixing in 0.01 M sodium phosphate, pH 7.0. Using the CD spectrum of native chromatin as a criterion to judge the closeness of a complex to its native state, it was observed that a complex made by direct mixing at low ionic strength (methods C and D) is better than the ones made by NaCl gradient dialysis with or without urea (methods A and B). It is explained as a result of lack of ordered secondary structures in histones due to the presence of urea in method A or due to nonspecific aggregation in NaCl without urea (method B). Compared with all the earlier reports in literature on the CD of histone-DNA complexes, the CD spectra of arginine-rich histone-DNA complexes prepared by methods C and D are closest to that of native chromatin both in shape and in amplitude. These results imply (a) that arginine-rich histones play an important role in maintaining the conformation of chromatin and (b) that the binding of these two histones to DNA prepared by methods C and D are close to that in native chromatin. Noticeable variation in conformation of free and bound histone and histone-bound DNA has also been observed in histone H3 with one or two cysteine residues, and in reduced or oxidized state even when the complexes were prepared and examined in the same condition. CD spectra of arginine-rich histones in 0.01 M phosphates, pH 7.0, indicate the presence of alpha-helix which could be responsible for a favorable binding of the less basic regions of these histones to DNA under this condition as demonstrated by thermal denaturation (Yu, S. .S, Li H. J., and Shih, T. Y. (1976), Bio-chemistry, the preceding paper in this issue). To preserve or generate alpha-helical structures in histones seems to be a critical step in reconstituting good histone-DNA complexes.
Interactions between DNA and model proteins, poly(L-Lys(m)L-Ala(n)), where m + n = 100%, have been investigated using thermal denaturation and circular dichroism (CD). All complexes of DNA with these proteins precipitate in a small range of input ratios, protein to DNA, with the midpoints of all precipitation curves close to a 1:1 ratio of lysine to phosphate. The melting temperature of model protein-bound DNA regions decreases slightly as the alanine content of the model protein is increased, which can be explained as a result of insufficient charge neutralization of phosphates by lysine residues in the model proteins. In the free state, these model proteins possess varying amounts of alpha helix, random coil, or a mixture of these two, depending upon the relative lysine/alanine content. When bound to DNA, the CD of the complex shows a substantial increase in alpha-helical structure for those model proteins with 40-60% alanine, while there is no significant change in alpha-helical structure when the percent alanine is either substantially higher or lower (i.e., 81 or 19% alanine). Only those complexes formed with model proteins having 40-60% alanine undergo a drastic transition from a B-type CD to an A-type in the presence of intermediate ionic strength (0.2 M NaCl, for example). Poly(Lys19Ala81)-DNA complexes show a slight transition toward A-type CD at 0.4 M NaCl or higher. Apparently other factors, in addition to alanine and alpha-helical content, must be responsible for this B leads to A transition. At the other extreme of lysine/alanine ratio, with high lysine content, poly(Lys81Ala19) or polylysine, the presence of NaCl produces a B leads to psi transition. The possible significance of these differences in response to the binding of these model proteins is discussed.
A random copolymer of 58% L-lysine and 42% L-phenylalanine, poly(Lys58Phe42), was used as a model protein for studying the role of phenylalanine residues in protein-DNA interaction. Complexes between this copolypeptide and DNA, made by direct mixing, were studied by absorbance, circular dichroism (CD), fluorescence, and thermal denaturation. Complex formation results in an increase in absorbance, and an enhancement, red-shift, and broadening of phenylalanine fluorescence. The fluorescence enhancement is opposite to the quenching observed when a tyrosine copolypeptide is bound to DNA (R. M. Santella and H.J. Li (1974), Biopolymers 13, 1909). The positive CD band of DNA near 275 nm is reduced and red-shifted by the binding of the phenylalanine copolypeptide to a greater extent than by the tyrosine copolypeptide. Thermal denaturation of the complexes in 2.5 times 10(-4) M EDTA (pH 8.0) shows three characteristic melting bands. For complexes with calf thymus DNA, free base pairs melt at Tm,I (47-49 degrees) and copolypeptide-bound base pairs show two melting bands (Tm,II at 73-75 degrees, and Tm,III at 88 -90 degrees). Similar thermal denaturation results have been observed for complexes with Micrococcus luteus DNA. The fluorecence intensity of the complexes is greatly increased when the temperature is raised to the Tm,II region. In addition to fluorescence measurements, the effects of increasing temperature on absorption and CD spectra of the complexes were also studied. Stacking interaction between the phenylalanine chromophore and DNA bases, either partial or full intercalation, is implicated by the experimental results. Several mechanisms are proposed to describe the reaction between the copolypeptide and DNA, and thermal denaturation of the complex.
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.
The 220-MHz high-resolution proton magnetic resonance (PMR) spectrum of histone IV has been examined as a function of histone concentration, salt concentration, and pD. The hydrophobic C-terminal portion of the histone IV monomer appears to be largely PMR "invisible" indicating that this region of the polypeptide contains rigid secondary structure. Further loss of PMR resonance areas with increased histone IV concentration in neat D2O has been attributed to self-aggregation involving a monomer-dimer equilibrium. An equilibrium between the monomer and large aggregates, on the other hand, appears to dominate at NaCl concentrations above 0.01 M. pD studies reveal an abrupt increase in histone IV aggregation at pD smaller than 0.8 and precipitation of histone IV at pD values in the neighborhood of its isoelectric point, pD similar to 11.
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