Characterization of a bimobile DNA junction

We present here a chemical and enzymatic footprinting analysis of a branched DNA molecule formed from four complementary 50-mer strands. These strands are designed to form a stable junction, in which two steps of branch point migration freedom are possible. Exposure of the junction to Fe(II).EDTA shows protection of 3 or 4 residues in each strand at the branch, while two resolvase enzymes (endonuclease VII from phage T4 and endonuclease I from phage T7), cleave all four strand near the branch. Chemical footprinting of this junction using the reagents MPE.Fe(II) and (OP)2Cu(I) shows that the branch site is hyper-reactive to cutting induced by these probes as it is in an immobile four-arm junction. The effects involve more residues than in the immobile case. In the absence of divalent cations, the structure of the junction alters, sites of enhanced cleavage by MPE.Fe(II) and (OP)2Cu(I) disappear, and purines at the branch become reactive to diethyl pyrocarbonate. Our interpretation of these results is based on the properties of immobile junction analogs and their response to these probes. In the presence of Mg2+, the three migrational isomers coexist, each probably in the form of a 2-fold symmetric structure with two helical arms stacked.     

Thermodynamics of DNA branching.

Branched DNA molecules arise transiently as intermediates in genetic recombination or on extrusion of cruciforms from covalent circular DNA duplexes that contain palindromic sequences. The free energy of these structures relative to normal DNA duplexes is of interest both physically and biologically. Oligonucleotide complexes that can form stable branched structures, DNA junctions, have made it possible to model normally unstable branched states of DNA such as Holliday recombinational intermediates. We present here an evaluation of the free energy of creating four-arm branch points in duplex DNA, using a system of two complementary junctions and four DNA duplexes formed from different combinations of the same set of eight 16-mer strands. The thermodynamics of formation of each branched structure from the matching pair of intact duplexes have been estimated in two experiments. In the first, labeled strands are allowed to partition between duplexes and junctions in a competition assay on polyacrylamide gels. In the second, the heats of forming branched or linear molecules from the component strands have been determined by titration microcalorimetry at several temperatures. Taken together these measurements allow us to determine the standard thermodynamic parameters for the process of creating a branch in an otherwise normal DNA duplex. The free energy for reacting two 16-mer duplexes to yield a four-arm junction in which the branch site is incapable of migrating is + 1.1 (+/- 0.4) kcal mol-1 (at 18 degrees C, 10 mM-Mg2+). Analysis of the distribution of duplex and tetramer products by electrophoresis confirms that the free energy difference between the four duplexes and two junctions is small at this temperature. The associated enthalpy change at 18 degrees C is +27.1 (+/- 1.3) kcal mol-1, while the entropy is +89 (+/- 30) cal K-1 mol-1. The free energy for branching is temperature dependent, with a large unfavorable enthalpy change compensated by a favorable entropy term. Since forming one four-stranded complex from two duplexes should be an entropically unfavorable process, branch formation is likely to be accompanied by significant changes in hydration and ion binding. A significant apparent delta Cp is also observed for the formation of one mole of junction, +0.97 (+/-0.05) kcal deg-1 mol-1.     

Drug binding by branched DNA: selective interaction of tetrapyridyl porphyrins with an immobile junction

The differential binding of a number of water-soluble cationic porphyrins to a branched DNA molecule is reported. Tetrakis(4-N-methylpyridiniumyl)porphine (H2TMpyP-4) interacts near the branch point with an immobile DNA junction formed from four 16-mer strands. Its Cu(II) and Ni(II) derivatives show stronger preferential binding in the neighborhood of the branch point. Axially liganded derivatives, Zn, Co, and Mn, also interact near this branch point, but in a different way. We use the reagents methidiumpropyl-EDTA.Fe(II) [MPE.Fe(II)] and bis(o-phenanthroline)copper(I) [(OP)2Cu(I)] to cleave complexes of DNA duplex controls and the junction with these porphyrins. The resulting cleavage patterns are consistent with previous evidence that the branch point provides a strong site for intercalative binding agents, which is not available in unbranched duplexes of identical sequence. The preferential scission by (OP)2Cu(I) in the presence of Ni and Cu porphyrins near the branch point exceeds that seen for any agents we have studied. This hyperreactivity is not seen in the case of porphyrins with axial ligands, ZnTMpyP-4, CoTMpyP-4, and MnTMpyP-4, although these also interact near the branch point. The Zn derivative tends to protect sites close to the branch point from cutting, while the Co and Mn porphyrins moderately enhance cleavage of sites in this region.     

DNase I cleavage of branched DNA molecules

We report here a potentially useful signature of branched DNA structures. The base 5' to the branch and the five bases flanking the 3' side of the branch site are protected from cleavage by DNase I in both three- and four-arm branched DNA molecules. Our procedure is to measure the cleavage profile for each 5' -labeled strand in a control duplex and compare this with that of the same strand in a branched structure under conditions yielding less than one cut per strand. The resulting cleavage pattern in an immobile four-arm junction is roughly 2-fold symmetric, consistent with the pattern of Fe(II).EDTA-induced cleavage that has been observed previously. In the three-arm junction, the DNase I cleavage pattern is asymmetric, indicating lack of 3-fold symmetry. A variable pattern of protection occurs to the 5' side of the branch in some strands only for both three- and four-arm junctions, extending 2-4 residues 5' to the branch.     

Asymmetric structure of a three-arm DNA junction

We present here experimental evidence that three-arm branched DNA molecules form an asymmetric structure in the presence of Mg2+. Electrophoretic mobility and chemical and enzymatic footprinting experiments on a three-arm branched DNA molecule formed from three 16-mer strands are described. The electrophoretic mobilities of three species of a three-arm junction in which pairs of arms are extended are found to differ in the presence of Mg2+: one combination of elongated arms migrates significantly faster than the other two. This effect is eliminated in the absence of Mg2+, leading us to suggest that the three-arm DNA junction forms an asymmetric structure due to preferential stacking of two of the arms at the junction in the presence of Mg2+. The pattern of self-protection of each 16-mer strand of the core complex exposed to Fe(II).EDTA and DNase I scission is unique, consistent with formation of an asymmetric structure in the presence of Mg2+. We conclude that three-arm junctions resemble four-arm junctions in showing preferential stacking effects at the branch site. Comparison of the scission patterns of linear duplexes and the branched trimer by the reactive probes methidiumpropyl-EDTA.Fe(II) [MPE.Fe(II)] and Cu(I)-[o-phenanthroline]2 [(OP)2CuI] further indicates that the branch point represents a site of enhanced binding for drugs, as it does in the four-arm case. Reaction with diethyl pyrocarbonate (DEPC), a purine-specific probe sensitive to conformation, is enhanced at the branch site, consistent with loosening of base pairing or unpairing at this point.(ABSTRACT TRUNCATED AT 250 WORDS)     

Crystal structure and ligand-binding studies of a screened peptide complexed with streptavidin.

The thermodynamic binding parameters and crystal structure for streptavidin-peptide complexes where the peptide sequences were obtained by random screening methods are reported. The affinities between streptavidin and two heptapeptides were determined by titrating calorimetric methods [Phe-Ser-His-Pro-Gln-Asn-Thr, Ka = 7944 (+/- 224) M-1, delta G degrees = -5.32 (+/- 0.01) kcal/mol, and delta H degrees = -19.34 (+/- 0.48) kcal/mol; His-Asp-His-Pro-Gln-Asn-Leu, Ka = 3542 (+/- 146) M-1, delta G degrees = -4.84 (+/- 0.03) kcal/mol, and delta H degrees = -19.00 (+/- 0.64) kcal/mol]. The crystal structure of streptavidin complexed with one of these peptides has been determined at 2.0-A resolution. The peptide (Phe-Ser-His-Pro-Gln-Asn-Thr) binds in a turn conformation with the histidine, proline, and glutamine side chains oriented inward at the biotin-binding site. A water molecule is immobilized between the histidine and glutamine side chains of the peptide and an aspartic acid side chain of the protein. Although some of the residues that participate in binding biotin also interact with the screened peptide, the peptide adopts an alternate method of utilizing binding determinants in the biotin-binding site of streptavidin.     

Drug binding by branched DNA molecules: analysis by chemical footprinting of intercalation into an immobile junction

Branched DNA structures interact with drugs differently from unbranched control duplexes of similar sequence. A specific interaction between the reagent (methidiumpropyl-EDTA).Fe(II) [MPE.Fe(II)] and a branched DNA molecule formed from 16-mer oligonucleotide strands has been reported [Guo, Q., Seeman, N. C., & Kallenbach, N. R. (1989) Biochemistry 28, 2355-2359]. The structure of the branched molecule is thought to be made up of two double-helical stacking domains with an overall twofold symmetry across the branch site. The MPE-Fe(II) interaction occurs predominantly at or adjacent to the branch site and is eliminated by a second intercalator, propidium iodide. Further studies on the nature and properties of this site are presented here. Comparison of the patterns of scission of linear duplex and branched tetramer by EDTA.Fe(II), MPE.Fe(II), and Cu(I)-(o-phenanthroline)2 [(OP)2Cu(I)] provides a higher resolution picture of the site of enhanced binding. In particular, the sensitive footprinting afforded by (OP)2Cu(I) allows us to localize the major site of preferential interaction with propidium precisely to the branch point itself, with a roughly twofold symmetric pattern of cuts resulting. In detail, the differential pattern with respect to each duplex control is distinct for each arm of the junction. Excess propidium results in apparent reversal of the crossover isomer of the junction, indicating a possible additional avenue for the action of drugs in biological systems--effects on the products of recombination.     

Contribution of the hydrophobic effect to globular protein stability.

The decrease in conformational stability, delta(delta G), has been measured for 72 aliphatic side-chain mutants from four proteins in which a larger side-chain is replaced by a smaller side-chain so that steric effects are minimal. When these delta(delta G) values are corrected to the same accessibility, namely 100% buried, then the following -delta(delta G) values per -CH2- group (in kcal/mol) are obtained: Ile----Val (1.26), Ala (1.26), Gly (1.26); Leu----Ala (1.16), Gly (1.21); Val----Ala (1.23), Gly (1.53). The average of these values is 1.27(+/- 0.07) kcal/mol. The 72 individual values range from 0 to 2.4 kcal/mol with an average value of 1.27(+/- 0.51) (standard deviation) kcal/mol. When the delta Gtr values from n-octanol to water are corrected for the difference in volume between the solutes and the solvents, the average value for the same substitutions is 1.25(+/- 0.05) kcal/mol. This suggests that proteins gain 1.3(+/- 0.5) kcal/mol in stability for each -CH2- group buried in folding, and, furthermore, that the volume corrected delta Gtr values for n-octanol for the amino acid side-chains provide good estimates of the contribution of the hydrophobic effect to globular protein stability.     

Contribution of the intercalated adenosine at the helical junction to the stability of the gag-pro frameshifting pseudoknot from mouse mammary tumor virus

The mouse mammary tumor virus (MMTV) gag-pro frameshifting pseudoknot is an H-type RNA pseudoknot that contains an unpaired adenosine (A14) at the junction of the two helical stems required for efficient frameshifting activity. The thermodynamics of folding of the MMTV vpk pseudoknot have been compared with a structurally homologous mutant RNA containing a G x U to G-C substitution at the helical junction (U13C RNA), and an A14 deletion mutation in that context (U13CdeltaA14 RNA). Dual wavelength optical melting and differential scanning calorimetry reveal that the unpaired adenosine contributes 0.7 (+/-0.2) kcal mol(-1) at low salt and 1.4 (+/-0.2) kcal mol(-1) to the stability (deltaG(0)37) at 1 M NaCl. This stability increment derives from a favorable enthalpy contribution to the stability deltadeltaH = 6.6 (+/-2.1) kcal mol(-1) with deltadeltaG(0)37 comparable to that predicted for the stacking of a dangling 3' unpaired adenosine on a G-C or G x U base pair. Group 1A monovalent ions, NH4+, Mg2+, and Co(NH3)6(3+) ions stabilize the A14 and deltaA14 pseudoknots to largely identical extents, revealing that the observed differences in stability in these molecules do not derive from a differential or specific accumulation of ions in the A14 versus deltaA14 pseudoknots. Knowledge of this free energy contribution may facilitate the prediction of RNA pseudoknot formation from primary nucleotide sequence (Gultyaev et al., 1999, RNA 5:609-617).     

Free energy of the binding of uridylic acid oligomers with double stranded poly(A) x poly(U)

The binding parameters (K, omega) and the free energy (DeltaG(0)) of triple helix formation have been estimated for complexes of oligo(U)(n) (n = 5, 7-10) with poly(A) . poly(U) on the basis of hypochromicity measurements. The data were treated according to the formula of McGhee and von Hippel [J. Mol. Biol. 86 (1974) 469] by a computer program ALAU [H. Schütz et al., Stud. Biophys. 104 (1984) 23] which takes absorbancies and total concentrations as input. In 1 mM cacodylate buffer pH 7.0 with 10 mM NaCl and 10 mM MgCl(2) at 5 degrees C the free energy of contiguous binding was found to be a linear function of the oligomer length with a slope of DeltaG(c,U)(0) = -0.72 (+/-0.03) kcal x mol(-1) per nucleotide. The mean cooperativity coefficient (omega) was 24.5 (+/- 5.6), and the corresponding free energy of interaction between the neighbouring oligonucleotides in the third strand was DeltaG(0(omega)) = -1.74 (+/-0.13) kcal x mol(-1).     

Quantitation of metal ion and DNA junction binding to the Holliday junction endonuclease Cce1

Cce1 is a magnesium-dependent Holliday junction endonuclease involved in the resolution of recombining mitochondrial DNA in Saccharomyces cerevisiae. Cce1 binds four-way DNA junctions as a dimer, opening the junction into an extended, 4-fold symmetric structure, and resolves junctions by the introduction of paired nicks in opposing strands at the point of strand exchange. In the present study, we have examined the interactions of wild-type Cce1 with a noncleavable four-way DNA junction and metal ions (Mg(2+) and Mn(2+)) using isothermal titration calorimetry, EPR, and gel electrophoresis techniques. Mg(2+) or Mn(2+) ions bind to Cce1 in the absence of DNA junctions with a stoichiometry of two metal ions per Cce1 monomer. Cce1 binds to four-way junctions with a stoichiometry of two Cce1 dimers per junction molecule in the presence of EDTA, and one dimer of Cce1 per junction in 15 mM magnesium. The presence of 15 mM Mg(2+) dramatically reduces the affinity of Cce1 for four-way DNA junctions, by about 900-fold. This allows an estimation of DeltaG degrees for stacking of four-way DNA junction 7 of -4.1 kcal/mol, consistent with the estimate of -3.3 to -4.5 kcal/mol calculated from branch migration and NMR experiments [Overmars and Altona (1997) J. Mol. Biol. 273, 519-524; Panyutin et al. (1995) EMBO J. 14, 1819-1826]. The striking effect of magnesium ions on the affinity of Cce1 binding to the four-way junction is predicted to be a general one for proteins that unfold the stacked X-structure of the Holliday junction on binding.     

A Cu(I)-sensing ArsR family metal sensor protein with a relaxed metal selectivity profile

ArsR (or ArsR/SmtB) family metalloregulatory homodimeric repressors collectively respond to a wide range of metal ion inducers in regulating homeostasis and resistance of essential and nonessential metal ions in bacteria. BxmR from the cyanobacterium Osciliatoria brevis is the first characterized ArsR protein that senses both Cu (I)/Ag (I) and divalent metals Zn (II)/Cd (II) in cells by regulating the expression of a P-type ATPase efflux pump (Bxa1) and an intracellular metallothionein (BmtA). We show here that both pairs of predicted alpha3N and alpha5 sites bind metal ions, but with distinct physicochemical and functional metal specificities. Inactivation of the thiophilic alpha3N site via mutation (C77S) abolishes regulation by both Cd (II) and Cu (I), while Zn (II) remains a potent allosteric negative effector of operator/promoter binding (Delta G c >or= +3.2 kcal mol (-1)). In contrast, alpha5 site mutant retains regulation by all four metal ions, albeit with a smaller coupling free energy (Delta G c approximately +1.7 (+/-0.1) kcal mol (-1)). Unlike the other metals ions, the BxmR dimer binds 4 mol equiv of Cu (I) to form an alpha3N binuclear Cu (I) 2S 4 cluster by X-ray absorption spectroscopy. BxmR is thus distinguishable from other closely related ArsR family sensors, in having evolved a metalloregulatory alpha3N site that can adopt an expanded range of coordination chemistries while maintaining redundancy in the response to Zn (II). The evolutionary implications of these findings for the ArsR metal sensor family are discussed.     

High pressure NMR reveals a variety of fluctuating conformers in beta-lactoglobulin

High pressure 1H/15N two-dimensional NMR spectroscopy has been used to study conformational fluctuation in bovine beta-lactoglobulin at pH 2.0 and 36 degrees C. Pressure dependencies of 1H and 15N chemical shifts and cross-peak intensities were analyzed at more than 80 independent atom sites between 30 and 2000 bar. Unusually large and non-linear chemical shift pressure dependencies are found for residues centering in the hydrophobic core region, suggesting the existence of low-lying excited native states (N') of the protein. Measurement of 1H/15N cross-peak intensities at individual amide sites as a function of pressure suggests that unfolding events occur independently in two sides of the beta-barrel, i.e. the hydrophobic core side (betaF-H) (producing I2) and the non-core side (betaB-E) (producing I1). At 1 bar the stability is higher for the core region (DeltaG0 = 6.5(+/-2.0) kcal/mol) than for the non-core region (4.6(+/-1.3) kcal/mol), but at high pressure the stability is reversed due to a larger DeltaV value of unfolding for the core region (90.0(+/-35.2) ml/mol) than that for the non-core region (57.4(+/-14.4) ml/mol), possibly due to an uneven distribution of cavities. The DeltaG0 profile along the amino acid sequence obtained from the pressure experiment is found to coincide well with that estimated from hydrogen exchange experiments. Altogether, the high pressure NMR experiment has revealed a variety of fluctuating conformers of beta-lactoglobulin, notably N, N', I1, I2 and the totally unfolded conformer U. Fluctuation of N to I1 and I2 conformers with open barrel structures could be a common design of lipocalin family proteins which bind various hydrophobic compounds in its barrel structure.     

SUPREX (Stability of Unpurified Proteins from Rates of H/D Exchange) analysis of the thermodynamics of synergistic anion binding by ferric-binding protein (FbpA), a bacterial transferrin

SUPREX (stability of unpurified proteins from rates of H/D exchange) is a H/D exchange- and matrix-assisted laser desorption/ionization (MALDI)-based technique for characterizing the equilibrium unfolding/refolding properties of proteins and protein-ligand complexes. Here, we describe the application of SUPREX to the thermodynamic analysis of synergistic anion binding to iron-loaded ferric-binding protein (Fe(3+)FbpA-X, X = synergistic anion). The in vivo function of FbpA is to transport unchelated Fe(3+) across the periplasmic space of certain Gram-negative bacteria, a process that requires simultaneous binding of a synergistic anion. Our results indicate that Fe(3+)FbpA-X is not a so-called "ideal" protein system for SUPREX analyses because it does not exhibit two-state folding properties and it does not exhibit EX2 H/D exchange behavior. However, despite these nonideal properties of the Fe(3+)FbpA-X protein-folding/unfolding reaction, we demonstrate that the SUPREX technique is still amenable to the quantitative thermodynamic analysis of synergistic anion binding to Fe(3+)FbpA. As part of this work, the SUPREX technique was used to evaluate the DeltaDeltaG(f) values of four synergistic anion-containing complexes of Fe(3+)FbpA (i.e., Fe(3+)FbpA-PO(4), Fe(3+)FbpA-citrate, Fe(3+)FbpA-AsO(4), and Fe(3+)FbpA-SO(4)). The DeltaDeltaG(f) value obtained for Fe(3+)FbpA-citrate relative to Fe(3+)FbpA-PO(4) (1.45 +/- 0.44 kcal/mol), is in good agreement with that reported previously (1.98 kcal/mol). The value obtained for Fe(3+)FbpA-AsO(4) (0.58 +/- 0.45 kcal/mol) was also consistent with that reported previously (0.68 kcal/mol), but the measurement error is very close to the magnitude of the value. This work (i) demonstrates the utility of the SUPREX method for studying anion binding by FbpA, (ii) provides the first evaluation of a DeltaDeltaG(f) value for Fe(3+)FbpA-SO(4), -1.43 +/- 0.17 kcal/mol, and (iii) helps substantiate our hypothesis that the synergistic anion plays a role in controlling the lability of iron bound to FbpA in the transport process.     

Kinetic barriers to the folding of horse cytochrome C in the reduced state

To determine the kinetic barrier in the folding of horse cytochrome c, a CO-liganded derivative of cytochrome c, called carbonmonoxycytochrome c, has been prepared by exploiting the thermodynamic reversibility of ferrocytochrome c unfolding induced by guanidinium hydrochloride (GdnHCl), pH 7. The CO binding properties of unfolded ferrocytochrome c, studied by 13C NMR and optical spectroscopy, are remarkably similar to those of native myoglobin and isolated chains of human hemoglobin. Equilibrium unfolding transitions of ferrocytochrome c in the presence and the absence of CO observed by both excitation energy transfer from the lone tryptophan to the ferrous heme and far-UV circular dichroism (CD) indicate no accumulation of structural intermediates to a detectable level. Values of thermodynamic parameters obtained by two-state analysis of fluorescence transitions are DeltaG(H2O) = 11.65(+/-1.13) kcal x mol(-1) and C(m) = 3.9(+/-0.1) M GdnHCl in the presence of CO, and DeltaG(H2O)=19.3(+/-0.5) kcal x mol(-1) and C(m) = 5.1(+/-0.1) M GdnHCl in the absence of CO, indicating destabilization of ferrocytochrome c by approximately 7.65 kcal x mol(-1) due to CO binding. The native states of ferrocytochrome c and carbonmonoxycytochrome c are nearly identical in terms of structure and conformation except for the Fe2+-M80 --> Fe2+-CO replacement. Folding and unfolding kinetics as a function of GdnHCl, studied by stopped-flow fluorescence, are significantly different for the two proteins. Both refold fast, but carbonmonoxycytochrome c refolds 2-fold faster (tau = 1092 micros at 10 degrees C) than ferrocytochrome c. Linear extrapolation of the folding rates to the ordinate of the chevron plot projects this value of tau to 407 micros. The unfolding rate of the former in water, estimated by extrapolation, is faster by more than 10 orders of magnitude. Significant differences are also observed in rate-denaturant gradients in the chevron. Formation and disruption of the Fe2+-M80 coordination contact clearly impose high-energy kinetic barriers to folding and unfolding of ferrocytochrome c. The unfolding barrier due to the Fe2+-M80 bond provides sufficient kinetic stability to the native state of ferrocytochrome c to perform its physiological function as an electron donor.     

Insights into protein-protein binding by binding free energy calculation and free energy decomposition for the Ras-Raf and Ras-RalGDS complexes

Absolute binding free energy calculations and free energy decompositions are presented for the protein-protein complexes H-Ras/C-Raf1 and H-Ras/RalGDS. Ras is a central switch in the regulation of cell proliferation and differentiation. In our study, we investigate the capability of the molecular mechanics (MM)-generalized Born surface area (GBSA) approach to estimate absolute binding free energies for the protein-protein complexes. Averaging gas-phase energies, solvation free energies, and entropic contributions over snapshots extracted from trajectories of the unbound proteins and the complexes, calculated binding free energies (Ras-Raf: -15.0(+/-6.3)kcal mol(-1); Ras-RalGDS: -19.5(+/-5.9)kcal mol(-1)) are in fair agreement with experimentally determined values (-9.6 kcal mol(-1); -8.4 kcal mol(-1)), if appropriate ionic strength is taken into account. Structural determinants of the binding affinity of Ras-Raf and Ras-RalGDS are identified by means of free energy decomposition. For the first time, computationally inexpensive generalized Born (GB) calculations are applied in this context to partition solvation free energies along with gas-phase energies between residues of both binding partners. For selected residues, in addition, entropic contributions are estimated by classical statistical mechanics. Comparison of the decomposition results with experimentally determined binding free energy differences for alanine mutants of interface residues yielded correlations with r(2)=0.55 and 0.46 for Ras-Raf and Ras-RalGDS, respectively. Extension of the decomposition reveals residues as far apart as 25A from the binding epitope that can contribute significantly to binding free energy. These "hotspots" are found to show large atomic fluctuations in the unbound proteins, indicating that they reside in structurally less stable regions. Furthermore, hotspot residues experience a significantly larger-than-average decrease in local fluctuations upon complex formation. Finally, by calculating a pair-wise decomposition of interactions, interaction pathways originating in the binding epitope of Raf are found that protrude through the protein structure towards the loop L1. This explains the finding of a conformational change in this region upon complex formation with Ras, and it may trigger a larger structural change in Raf, which is considered to be necessary for activation of the effector by Ras.     

Spectral, kinetic, and thermodynamic properties of Cu(I) and Cu(II) binding by methanobactin from Methylosinus trichosporium OB3b

To examine the potential role of methanobactin (mb) as the extracellular component of a copper acquisition system in Methylosinus trichosporium OB3b, the metal binding properties of mb were examined. Spectral (UV-visible, fluorescence, and circular dichroism), kinetic, and thermodynamic data suggested copper coordination changes at different Cu(II):mb ratios. Mb appeared to initially bind Cu(II) as a homodimer with a comparatively high copper affinity at Cu(II):mb ratios below 0.2, with a binding constant (K) greater than that of EDTA (log K = 18.8) and an approximate DeltaG degrees of -47 kcal/mol. At Cu(II):mb ratios between 0.2 and 0.45, the K dropped to (2.6 +/- 0.46) x 10(8) with a DeltaG degrees of -11.46 kcal/mol followed by another K of (1.40 +/- 0.21) x 10(6) and a DeltaG degrees of -8.38 kcal/mol at Cu(II):mb ratios of 0.45-0.85. The kinetic and spectral changes also suggested Cu(II) was initially coordinated to the 4-thiocarbonyl-5-hydroxy imidazolate (THI) and possibly Tyr, followed by reduction to Cu(I), and then coordination of Cu(I) to 4-hydroxy-5-thiocarbonyl imidazolate (HTI) resulting in the final coordination of Cu(I) by THI and HTI. The rate constant (k(obsI)) of binding of Cu(II) to THI exceeded that of the stopped flow apparatus that was used, i.e., >640 s(-)(1), whereas the coordination of copper to HTI showed a 6-8 ms lag time followed by a k(obsII) of 121 +/- 9 s(-)(1). Mb also solubilized and bound Cu(I) with a k(obsI) to THI of >640 s(-)(1), but with a slower rate constant to HTI (k(obsII) = 8.27 +/- 0.16 s(-)(1)), and appeared to initially bind Cu(I) as a monomer.     

Triple helix formation by oligopurine-oligopyrimidine DNA fragments. Electrophoretic and thermodynamic behavior

The 26mer oligodeoxynucleotide d(GAAGGAGGAGATTTTTCTCCTCCTTC) adopts in solution a unimolecular hairpin structure (h), with an oligopurine-oligopyrimidine (Pu-Py) stem. When h is mixed with d(CTTCCTCCTCT) (s1) the two strands co-migrate in polyacrylamide gel electrophoresis at pH 5. If s1 is substituted with d(TCTCCTCCTTC) (s2), such behavior is not observed and the two strands migrate separately. This supports the suggestion of the formation of a triple-stranded structure by h and s1 (h:s1) but not by h and s2, and confirms the strand polarity requirement of the third pyrimidine strand, which is necessary for this type of structure. The formation of a triple helix by h:s1 is supported by electrophoretic mobility data (Ferguson plot) and by enzymatic assay with DNase I. Circular dichroism measurements show that, upon triple helix formation, there are two negative ellipticities: a weaker one (delta epsilon = 80 M-1 cm-1) at 242 nm and a stronger one (delta epsilon = 210 M-1 cm-1) at 212 nm. The latter has been observed also in triple-stranded polynucleotides, and can be considered as the trademark for a Py:Pu:Py DNA triplex. Comparison of ultraviolet absorption at 270 nm and temperature measurements shows that the triple-stranded structure melts with a biphasic profile. The lower temperature transition is bimolecular and is attributable to the breakdown of the triplex to give h and s1, while the higher temperature transition is monomolecular and is due to the transition of hairpin to coil structure. The duplex-to-triplex transition is co-operative, fully reversible and with a hyperchromism of about 10%. The analysis of the melting curves, with a three-state model, allows estimation of the thermodynamic parameters of triple helix formation. We found that the duplex-to-triplex transition of h: s1 is accompanied by an average change in enthalpy (less the protonation contribution) of -73(+/- 5) kcal/mol of triplex, which corresponds to -6.6(+/- 0.4) kcal/mol of binding pyrimidine, attributable to stacking and hydrogen bonding interactions.     

The purification and some properties of rusticyanin, a blue copper protein involved in iron(II) oxidation from Thiobacillus ferro-oxidans.

The 'blue' copper-containing protein rusticyanin was purified to homogeneity from cells of the chemolithotrophic bacterium Thiobacillus ferro-oxidans by (NH4)SO4 fractionation and ion-exchange chromatography. The protein, which is stable at low pH, consists of a single polypeptide chain of mol. wt. 16500 and possesses 0.79 (+/- 0.28)g-atom of Cu/mol. The protein, which does not contain arginine residues, has optical absorbance maxima at 287, 450, 597 and 750 nm and is generally similar to azurin. The isolated protein is reduced directly by Fe2+ with a 1:1 stoicheiometry to Cu. On reduction by Fe2+ the absorption peaks at 450, 597 and 750 nm are abolished, with the appearance of a new absorption band at 320 nm. The results obtained are consistent with rusticyanin being the initial acceptor of electrons from Fe2+ during respiratory iron oxidation.