The contribution of residue ion pairs to the helical stability of a model peptide.

Comparative CD measurements were made on the model helical peptides acetylYEAAAKEAXAKEAAAKAamide and acetylYEAAAEKAXAKEAAAKAamide in which X represents a nonaromatic nonionic residue. The former peptide contains three potential i, i + 4 complementary ion pairs at neutral pH, while the latter peptide contains one potential complementary and two potential antagonistic i, i + 4 ion pairs. The effect of pH and ionic strength on the mean residue ellipticity of these peptides was measured at 222 nm and 0 degrees C. These measurements were analyzed assuming a common two-state helix/coil transition and only i, i, + 4 ion-pair interactions. The analyses suggest that the central ion pairs do modulate helical content while the peripheral ion pairs do not, presumably due to the location of the peripheral ion pairs in the frayed ends of the helix. The complementary central ion pair stabilizes the helix by about 0.4 kcal/mole and the antagonistic central ion pair destabilizes the helix by about 0.2 kcal/mole.     

Binding of antibacterial magainin peptides to electrically neutral membranes: thermodynamics and structure.

Magainins are positively charged amphiphatic peptides which permeabilize cell membranes and display antimicrobial activity. They are usually thought to bind specifically to anionic lipids, and binding studies have been performed almost exclusively with negatively charged membranes. Here we demonstrate that binding of magainins to neutral membranes, a reaction which is difficult to assess with spectroscopic means, can be followed with high accuracy using isothermal titration calorimetry. The binding mechanism can be described by a surface partition equilibrium after correcting for electrostatic repulsion by means of the Gouy-Chapman theory. Unusual thermodynamic parameters are observed for the binding process. (i) The three magainin analogues that were investigated bind to neutral membranes with large exothermic reaction enthalpies DeltaH of -15 to -18 kcal/mol (at 30 degrees C). (ii) The reaction enthalpies increase with increasing temperature, leading to a large positive heat capacity DeltaC(p) of approximately 130 cal mol(-)(1) K(-)(1) (at 25 degrees C). (iii) The Gibbs free energies of binding DeltaG are between -6.4 and -8.6 kcal/mol, resulting in a large negative binding entropy DeltaS. The binding of magainin to small unilamellar vesicles is hence an enthalpy-driven reaction. The negative DeltaH and DeltaS and the large positive DeltaC(p) contradict the conventional understanding of the hydrophobic effect. CD experiments reveal that the membrane-bound fraction of magainin is approximately 80% helical at 8 degrees C, decreasing to approximately 60% at 45 degrees C. Since the random coil --> alpha-helix transition in aqueous solution is known to be an exothermic process, the same process occurring at the membrane surface is shown to account for up to 65% of the measured reaction enthalpy. In addition to membrane-facilitated helix formation, the second main driving force for membrane binding is the insertion of the nonpolar amino acid side chains into the lipid bilayer. It also contributes a negative DeltaH and follows the pattern for the nonclassical hydrophobic effect. Addition of cholesterol drastically reduces the extent of peptide binding and reveals an enthalpy-entropy compensation mechanism. Membrane permeability was measured with a dye assay and correlated with the extent of peptide binding. The level of dye efflux is linearly related to the amount of surface-bound peptide and can be traced back to a membrane perturbation effect.     

Spectroscopic analysis of DNA base-pair opening by Escherichia coli RNA polymerase. Temperature and ionic strength effects

The interaction of Escherichia coli RNA polymerase with poly[d(A-T)] and poly[d-(I-C)] was studied by difference absorption spectroscopy at temperatures, from 5 to 45 degrees C in the absence and presence of Mg2+. The effect of KCl concentration, at a fixed temperature, was studied from 12.5 to 400 mM. Difference absorption experiments permitted calculation of the extent of DNA opening induced by RNA polymerase and estimation of the equilibrium constant associated with the isomerization from a closed to an open RNA polymerase-DNA complex. delta H0 and delta S0 for the closed-to-open transition with poly[d(A-T)] or poly[d(I-C)] complexed with RNA polymerase are significantly lower than the values associated with the helix-to-coil transition for the free polynucleotides. For the RNA polymerase complexes with poly[d(A-T)] and poly[d(I-C)] in 50 mM KCl, delta H0 approximately 15-16 kcal/mol (63-67 kJ/mol) and delta S0 approximately 50-57 cal/K per mol (209-239 J/K per mol). The presence of Mg2+ does not change these parameters appreciably for the RNA polymerase-poly[d(A-T)] complex, but for the RNA polymerase-poly[d(I-C)] complex in the presence of Mg2+, the delta H0 and delta S0 values are larger and temperature-dependent, with delta H0 approximately 22 kcal/mol (92 kJ/mol) and delta S0 approximately 72 cal/K per mol (approx. 300 J/K per mol) at 25 degrees C, and delta Cp0 approximately 2 kcal/K per mol (approx. 8.3 kJ/K per mol). The circular dichroism (CD) changes observed for helix opening induced by RNA polymerase are qualitatively consistent with the thermally induced changes observed for the free polynucleotides, supporting the difference absorption method. The salt-dependent studies indicate that two monovalent cations are released upon helix opening. For poly[d(A-T)], the temperature-dependence of enzyme activity correlates well with the helix opening, implying this step to be the rate-determining step. In the case of poly[d(I-C)], the same is not true, and so the rate-determining step must be a process subsequent to helix opening.     

Enthalpic and entropic contributions to actin stability: calorimetry, circular dichroism, and fluorescence study and effects of calcium

The delta H associated with the thermal unfolding of G-actin has been determined by differential scanning calorimetry (DSC) to be 142 +/- 5 kcal/mol, with the Tm (melting temperature) at 57.2 +/- 0.5 degrees C, at pH 8.0 (heating rate 0.5 K/min). The transition is broad and cannot be treated as a single transition that mimics a two-state process, suggesting the existence of domains. Deconvolution is done to fit it into two quasi-independent two-state transitions. For F-actin, the transition is more cooperative, with a cooperative ratio (the ratio of van't Hoff enthalpy and calorimetric enthalpy) of 1.4, indicating intermonomer interaction. The delta H of the thermal unfolding of F-actin is 162 +/- 10 kcal/mol with a Tm at 67.0 +/- 0.5 degrees C. A state of G-actin similar to that of the heat-denatured form, designated D-actin, is obtained by removing tightly bound Ca2+ with EGTA. The DSC-detectable cooperative transition is completely lost when the free calcium concentration of the medium is 1 x 10(-11) M or lower, using a Ca2+/EGTA buffer system. However, circular dichroism (CD) shows that the helix content of actin, 32% in the G-form, is only partially reduced to 19% in this apo form. The CD spectrum and the helix content of the calcium-depleted actin are almost identical with those of the heat-denatured D form. This loss of 40% of the native helical content is irreversible in both cases. The remaining 60% of the native helical content cannot be further eliminated by heating to 95 degrees C.(ABSTRACT TRUNCATED AT 250 WORDS)     

Proline affects oligomerization of a coiled coil by inducing a kink in a long helix

The structural effect of a proline in a helix in trifluoroethanol (TFE)/water medium was examined on a 29-mer peptide and its proline analog derived from the leucine zipper (LZ)-like motif of gp41 (the transmembrane glycoprotein of HIV-1) by NMR and circular dichroism (CD) spectroscopies. Lower helical content was found for the proline mutant from the CD study. NMR data show that distortion of the helix by proline is local and occurs mainly on the N-terminal side of the substitution site. Molecular dynamics computation exhibits a bending of the helical axis of 30 degrees +/- 10 degrees, in agreement with X-ray diffraction results. Light-scattering experiments indicated that the average aggregation number of the proline-substituted mutant is substantially lower than that of the wild-type peptide. From the ratio of dissociation constants of the wild-type and the proline mutant peptides, the difference in free energy of trimeric formation is calculated to be 2.1 kcal/mol. Thermal stability, helicity, and the average aggregation number for the helix oligomers were found to be correlated. The structural alteration and the reduced coiled coil stability may account for the deficiency in the biological functions of the proline mutants of gp41 and in the inhibitory action of proline-substituted peptides. These effects may also be important in unraveling the roles played by proline in transmembrane proteins.     

Conformational intermediates in the folding of a coiled-coil model peptide of the N-terminus of tropomyosin and alpha alpha-tropomyosin.

Circular dichroism was used to study the folding of alpha alpha-tropomyosin and AcTM43, a 43-residue peptide designed to serve as a model for the N-terminal domain of tropomyosin. The sequence of the peptide is AcMDAIKKKMQMLKLDVENLLDRLEQLEADLKALEDRYKQLEGGC. The peptide appeared to form a coiled coil at low temperatures (< 25 degrees C) in buffers with physiological ionic strength and pH. The folding and unfolding of the peptide, however, were noncooperative. When CD spectra were examined as a function of temperature, the apparent degree of folding differed when the ellipticity was followed at 222, 208, and 280 nm. Deconvolution of the spectra suggested that at least three component curves contributed to the CD in the far UV. One component curve was similar to the CD spectrum of the coiled-coil alpha-helix of native alpha alpha-tropomyosin. The second curve resembled the spectrum of single-stranded short alpha-helical segments found in globular proteins. The third was similar to that of polypeptides in the random coil conformation. These results suggested that as the peptide folded, the alpha-helical content increased before most of the coiled coil was formed. When the CD spectrum of striated muscle alpha alpha-tropomyosin was examined as a function of temperature, the unfolding was also not totally cooperative. As the temperature was raised from 0 to 25 degrees C, there was a decrease in the coiled coil and an increase in the conventional alpha-helix type spectrum without formation of random coil. The major transition, occurring at 40 degrees C, was a cooperative transition characterized by the loss of all of the remaining coiled coil and a concomitant increase in random coil.     

1H NMR and circular dichroism studies of the B and Z conformations of the self-complementary deoxyhexanucleotide d(m5C-G-C-G-m5-C-G): mechanism of the Z-B-coil transitions

The double-helical conformations of d(m5-C-G-C-G-m5-C-G) in aqueous solution were studied by circular dichroism and 1H NMR spectroscopy. In 0.1 M NaCl, only the B form is detected whereas the Z form is strongly predominant in 3 M NaCl. In the presence of 2 M NaCl, two resonance signals corresponding to the B and Z duplexes were observed for each proton below 50 degrees C, indicating a slow exchange between B and Z. However, the B-Z exchange becomes intermediate or fast in the 55-80 degrees C temperature interval. By contrast the exchange between B helix and single-stranded (or coil) forms is much faster for the same temperature conditions. The Z form is only detectable when the coil form is practically absent. With decreasing temperature the B form decreases in favor of the Z form. From proton line-width measurements under various experimental conditions, it was also shown that Z exchanges only with B, while the latter also exchanges with the single-stranded form (S): Z in equilibrium B in equilibrium S. The enthalpy value is about 8 +/- 1 kcal/mol for the B-Z transition and about 40 +/- 2 kcal/mol for the B-S dissociation (2 M NaCl solution). The activation energy is about 47 +/- 2 kcal/mol for the Z----B and 39 +/- 2 kcal/mol for the B----Z reaction. Very good agreement between the experimental results and computed data (based on the above kinetic reaction model) was found for the B, Z, and coil proportions. The B-Z transition of methylated d(C-G)n oligomers is only possible when the Watson-Crick hydrogen bonds between the CG base pairs are firmly maintained; otherwise, the transformation from B to Z would not occur, and B-S dissociation would take place instead.     

Identification of a major heparin-binding site in kallistatin

Kallistatin is a heparin-binding serine proteinase inhibitor (serpin), which specifically inhibits human tissue kallikrein by forming a covalent complex. The inhibitory activity of kallistatin is blocked upon its binding to heparin. In this study we attempted to locate the heparin-binding site of kallistatin using synthetic peptides derived from its surface regions and by site-directed mutagenesis of basic residues in these surface regions. Two synthetic peptides, containing clusters of positive-charged residues, one derived from the F helix and the other from the region encompassing the H helix and C2 sheet of kallistatin, were used to assess their heparin binding activity. Competition assay analysis showed that the peptide derived from the H helix and C2 sheet displayed higher and specific heparin binding activity. The basic residues in both regions were substituted to generate three kallistatin double mutants K187A/K188A (mutations in the F helix) and K307A/R308A and K312A/K313A (mutations in the region between the H helix and C2 sheet), using a kallistatin P1Arg variant as a scaffold. Analysis of these mutants by heparin-affinity chromatography showed that the heparin binding capacity of the variant K187A/K188A was not altered, whereas the binding capacity of K307A/R308A and K312A/K313A mutants was markedly reduced. Titration analysis with heparin showed that the K312A/K313A mutant has the highest dissociation constant. Like kallistatin, the binding activity of K187A/K188A to tissue kallikrein was blocked by heparin, whereas K307A/R308A and K312A/K313A retained significant binding and inhibitory activities in the presence of heparin. These results indicate that the basic residues, particularly Lys(312)-Lys(313), in the region between the H helix and C2 sheet of kallistatin, comprise a major heparin-binding site responsible for its heparin-suppressed tissue kallikrein binding.     

Interaction of a mitochondrial presequence with lipid membranes: role of helix formation for membrane binding and perturbation

The binding of a peptide to a biological membrane is often accompanied by a transition from a random coil structure to an amphipathic alpha-helix. Recently, we have presented a new approach which allows the determination of the thermodynamic parameters of membrane-induced helix formation [Wieprecht et al. (1999) J. Mol Biol. 294, 785]. It involves a systematic variation of the helix content of a given peptide by double D-substitution and a correlation of the binding parameters with the helicity. Here we have used this method to study membrane-induced helix formation for the presequence of rat mitochondrial rhodanese (RHD). The thermodynamic parameters of binding of the peptide RHD and of four of its double D-isomers were determined for 30 nm (SUVs) and 100 nm (LUVs) unilamellar vesicles composed of phosphatidylcholine/phosphatidylglycerol (3:1) using circular dichroism spectroscopy, fluorescence spectroscopy, and isothermal titration calorimetry. The incremental changes of the thermodynamic parameters of helix formation were found to be very similar for SUVs and LUVs. Membrane-induced helix formation of RHD entailed a negative enthalpy of Delta H(helix) = -0.5 to -0.6 kcal/mol/residue and was opposed by an entropy of about Delta S(helix) = -1 to -1.4 cal/mol K/residue. The free energy of helix formation, Delta G(helix), was about -0.2 kcal/mol, and helix formation accounted for 50-60% of the total free energy of membrane binding. Dye-release experiments were used to assess the role of helix formation for the membrane perturbation potential of the peptides. While helix formation plays a major role for membrane binding, it appears to have little importance for inducing membrane leakiness.     

Thermal and structural behavior of natural cerebroside 3-sulfate in bilayer membranes

Differential scanning calorimetry (DSC), polarizing microscopy and X-ray diffraction studies have been performed on dry and hydrated natural bovine brain sulfatides. Dry sulfatide fractions exhibit a high temperature transition (delta H = 6.6 kcal/mol sulfatide) at 87.3 degrees C. X-ray diffraction shows this transition to be associated with a hydrocarbon chain order-disorder transformation between two lamellar phases. Hydrated sulfatide dispersions undergo a complex chain order-disorder transition (delta H = 7.5 kcal/mol sulfatide) at 32 degrees C with two peak temperatures at 35 degrees C and 47 degrees C. Structural studies performed on hydrated liquid-crystal sulfatide dispersions at 75 degrees C verify the existence of a bilayer structure over the 16 wt.% to 50 wt.% phosphate buffer (pH = 7.4) range. The interbilayer separation between galactosyl-3-sulfate groups averages 48 A as the multilamellar bilayers swell with the addition of phosphate buffer. The formation of micellar phases is not observed at high water contents. The comparison of the structural characteristics of dry and hydrated sulfatides with structural data for dry and hydrated bovine brain non-sulfated glycolipid (cerebroside) is discussed in molecular terms.     

MEARA sequence repeat of human CstF-64 polyadenylation factor is helical in solution. A spectroscopic and calorimetric study.

The primary structure of the human CstF-64 polyadenylation factor contains 12 nearly identical repeats of a consensus motif of five amino acid residues with the sequence MEAR(A/G). No known function has yet been ascribed to this motif; however, according to secondary structure prediction algorithms, it should form a helical structure in solution. To validate this theoretical prediction, we synthesized a 31 amino acid residue peptide (MEARA(6)) containing six repeats of the MEARA sequence and characterized its structure and stability by circular dichroism (CD) spectroscopy and differential scanning calorimetry (DSC). No effects of concentration on the CD or DSC properties of MEARA(6) were observed, indicating that the peptide is monomeric in solution at concentrations up to 2 mM. The far UV-CD spectra of MEARA(6) indicates that at a low temperature (1 degrees C) the MEARA(6) peptide has a relatively high helical content (76% at pH 2.0 and 65% at pH 7.0). The effects of pH and ionic strength on the CD spectrum of MEARA(6) suggest that a number of electrostatic interactions (e.g., i, i + 3 Arg/Glu ion pair, charge-dipole interactions) contribute to the stability of the helical structure in this peptide. DSC profiles show that the melting of MEARA(6) helix is accompanied by positive change in the enthalpy. To determine thermodynamic parameters of helix-coil transition from DSC profiles for this peptide, we developed a new, semiempirical procedure based on the calculated function for the heat capacity of the coiled state for a broad temperature range. The application of this approach to the partial molar heat capacity function for MEARA(6) provides the enthalpy change for helix formation calculated per amino acid residue as 3.5 kJ/mol.     

Electrostatic interactions in a peptide--RNA complex

Parallel experimental measurements and theoretical calculations have been used to investigate the energetics of electrostatic interactions in the complex formed between a 22 residue, alpha-helical peptide from the N protein of phage lambda and its cognate 19 nucleotide box B RNA hairpin. Salt-dependent free energies were measured for both peptide folding from coil to helix and peptide binding to RNA, and from these the salt-dependence of binding pre-folded, helical peptide to RNA was determined ( partial differential (DeltaG degrees (dock))/ partial differential log[KCl]=5.98(+/-0.21)kcal/mol). (A folding transition taking place in the RNA hairpin loop was shown to have a negligible dependence on salt concentration.) The non-linear Poisson-Boltzmann equation was used to calculate the same salt dependence of the binding free energy as 5.87(+/-0.22)kcal/mol, in excellent agreement with the measured value. Close agreement between experimental measurements and calculations was also obtained for two variant peptides in which either a basic or acidic residue was replaced with an uncharged residue, and for an RNA variant with a deletion of a single loop nucleotide. The calculations suggest that the strength of electrostatic interactions between a peptide residue and RNA varies considerably with environment, but that all 12 positive and negative N peptide charges contribute significantly to the electrostatic free energy of RNA binding, even at distances up to 11A from backbone phosphate groups. Calculations also show that the net release of ions that accompanies complex formation originates from rearrangements of both peptide and RNA ion atmospheres, and includes accumulation of ions in some regions of the complex as well as displacement of cations and anions from the ion atmospheres of the RNA and peptide, respectively.     

Structure and metastability of N-lignocerylgalactosylsphingosine (cerebroside) bilayers

Differential scanning calorimetry (DSC) and X-ray diffraction have been used to study hydrated N-lignocerylgalactosylsphingosine (NLGS) bilayers. DSC of fully hydrated NLGS shows an endothermic transition at 69-70 degrees C, immediately followed by an exothermic transition at 72-73 degrees C; further heating shows a high-temperature (Tc = 82 degrees C), high-enthalpy (delta H = 15.3 kcal/mol NLGS) transition. Heating to 75 degrees C, cooling to 20 degrees C and subsequent reheating shows no transitions at 69-73 degrees C; only the high-temperature (82 degrees C), high-enthalpy (15.3 kcal/mol) transition. Two exothermic transitions are observed on cooling; for the upper transition its temperature (about 65 degrees C) and enthalpy (about 6 kcal/mol NLGS) are essentially independent of cooling rate, whereas the lower transition exhibits marked changes in both temperature (30----60 degrees C) and enthalpy (2.2----9.5 kcal/mol NLGS) as the cooling rate decreases from 40 to 0.625 Cdeg/min. On reheating, the enthalpy of the 69-70 degrees C transition is dependent on the previous cooling rate. The DSC data provide clear evidence of conversions between metastable and stable forms. X-ray diffraction data recorded at 26, 75 and 93 degrees C show clearly that NLGS bilayer phases are present at all temperatures. The X-ray diffraction pattern at 75 degrees C shows a bilayer periodicity d = 65.4 A, and a number of sharp reflections in the wide-angle region indicative of a crystalline chain packing mode. This stable bilayer form converts to a liquid-crystal bilayer phase; at 93 degrees C, the bilayer periodicity d = 59.1 A, and a diffuse reflection at 1/4.6 A-1 is observed. The diffraction pattern at 22 degrees C represents a combination of the stable and metastable low-temperature bilayer forms. NLGS exhibits a complex pattern of thermotropic changes related to conversions between metastable (gel), stable (crystalline) and liquid-crystalline bilayer phases. The structure and thermotropic properties of NLGS are compared with those of hydrated N-palmitoylgalactosylsphingosine reported previously (Ruocco, M.J., Atkinson, D., Small, D.M., Skarjune, R.P., Oldfield, E. and Shipley, G.G. (1981) Biochemistry 20, 5957-5966).     

High-resolution differential scanning calorimetric study of myosin, functional domains, and supramolecular structures

High-resolution differential scanning calorimetry (DSC) has been employed to study the thermal stability of myosin, its major constitutive fragments (S-1, light chains, and rod), and also reconstituted thick filaments. The thermal denaturation of soluble myosin was complex and was characterized by a multistep endothermic process for the temperature range from 41 to 60 degrees C. The shape of the endotherm was highly dependent on the pH and the ionic strength of the solution, although the delta Hcal (calorimetric enthalpy) of denaturation (1715 +/- 75 kcal/mol) was insensitive to these changes for the solvent conditions used in this study. This value also agrees, within experimental error, with the sum of the denaturation enthalpies obtained for isolated fragments (1724 +/- 79 kcal/mol). In identical conditions of ionic strength, pH, and heating rate, the computer-calculated differential endotherms of domains belonging to S-1 and light chains were superimposable with those of the isolated fragments. Their responses to changes in the solvent condition were also similar. We suggest that the observed functional independence of the major domains in myosin reflects also the independence of their structural stability. The thermal unfolding of the isolated rod was multiphasic and readily reversible (95%). It occurred between 41 and 60 degrees C, with an delta Hcal of 1058 +/- 59 kcal/mol. The melting of S-1 showed a single peak at 46.3 +/- 0.1 degrees C with an delta Hcal of 255 +/- 12 kcal/mol. Light chains melted at 51.0 +/- 0.2 degrees C with an delta Hcal of 85 +/- 15 kcal/mol.(ABSTRACT TRUNCATED AT 250 WORDS)     

Importance of tryptophan 49 of antithrombin in heparin binding and conformational activation

Tryptophan 49 of antithrombin, the primary inhibitor of blood clotting proteinases, has previously been implicated in binding the allosteric activator, heparin, by chemical modification and mutagenesis studies. However, the X-ray cocrystal structure of the antithrombin-pentasaccharide complex shows that Trp49 does not contact the bound saccharide. Here, we provide a detailed thermodynamic and kinetic characterization of heparin binding to a Trp49 to Lys variant of antithrombin and suggest a model for how Trp49 participates in heparin binding and activation. Mutation of Trp49 to Lys resulted in substantial losses of 16-24% in heparin-binding energy at pH 7.4, I 0.15, and 25 degrees C. These losses were due to both the loss of one ionic interaction ( approximately 30%) and the loss of nonionic interactions ( approximately 70%). Rapid kinetics analyses showed that the mutation minimally affected the initial weak binding of heparin to antithrombin or the rate constant for the subsequent conformational activation of the serpin. Rather, the principal effect of the mutation was to increase the rate constant for reversal of the conformational activation step by 70-100-fold, thereby destabilizing the activated conformation. This destabilization could be accounted for by the disruption of a network of interactions involving Trp49, Glu50, and Lys53 of helix A and Ser112 of helix P, which stabilizes the activated conformation.     

Unusual enthalpy changes which accompany the titration of dimyristoylphosphatidylcholine vesicles with Triton X-100

The enthalpy changes which accompany the titration of 0.1% and 0.25% small unilamellar and multiameller vesicle samples of dimyristoylphosphatidylcholine with 2% Triton X-100 in 0.067 M phosphate buffer (pH 7.4) containing 0.15 M NaCl have been determined by titration calorimetry at 21 degrees C and 28 degrees C, the enthalpy change for both type of vesicles was zero within the limits of experimental error. At 21 degrees C, the multilamellar vesicle samples exhibited an enthalpy change of 1.35 +/- 0.48 and 2.47 +/- 0.98 kcal/mol dimyristoylphosphatidylcholine which was complete at a molar ratio of dimyristoylphosphatidylcholine to Triton of 3.21 +/- 0.84 and 5.77 +/- 1.05 for 0.1% and 0.25% dimyristoylphosphatidylcholine solutions, respectively. An exothermic transition of -2.39 +/- 0.30 and -2.05 +/- 0.69 kcal/mol phospholipid followed by an endothermic transition of 1.37 +/- 0.12 and 1.94 +/- 0.20 kcal/mol dimyristoylphosphatidylcholine was observed at 21 degrees C for 0.1% and 0.25% small unilamellar vesicle samples, respectively. In addition the nearly athermal association of the small unilemellar vesicle samples at 21 degrees C was observed, which may be an appropriate model for biological membrane fusion.     

The Alzheimer beta-peptide shows temperature-dependent transitions between left-handed 3-helix, beta-strand and random coil secondary structures

The temperature-induced structural transitions of the full length Alzheimer amyloid beta-peptide [A(beta)(1-40) peptide] and fragments of it were studied using CD and 1H NMR spectroscopy. The full length peptide undergoes an overall transition from a state with a prominent population of left-handed 3(1) (polyproline II; PII)-helix at 0 degrees C to a random coil state at 60 degrees C, with an average DeltaH of 6.8 +/- 1.4 kJ.mol(-1) per residue, obtained by fitting a Zimm-Bragg model to the CD data. The transition is noncooperative for the shortest N-terminal fragment A(beta)(1-9) and weakly cooperative for A(beta)(1-40) and the longer fragments. By analysing the temperature-dependent 3J(HNH(alpha)) couplings and hydrodynamic radii obtained by NMR for A(beta)(1-9) and A(beta)(12-28), we found that the structure transition includes more than two states. The N-terminal hydrophilic A(beta)(1-9) populates PII-like conformations at 0 degrees C, then when the temperature increases, conformations with dihedral angles moving towards beta-strand at 20 degrees C, and approaches random coil at 60 degrees C. The residues in the central hydrophobic (18-28) segment show varying behaviour, but there is a significant contribution of beta-strand-like conformations at all temperatures below 20 degrees C. The C-terminal (29-40) segment was not studied by NMR, but from CD difference spectra we concluded that it is mainly in a random coil conformation at all studied temperatures. These results on structural preferences and transitions of the segments in the monomeric form of A(beta) may be related to the processes leading to the aggregation and formation of fibrils in the Alzheimer plaques.     

Position dependence of amino acid intrinsic helical propensities II: non-charged polar residues: Ser, Thr, Asn, and Gln.

The assumption that the intrinsic alpha-helical propensities of the amino acids are position independent was critical in several helix/coil transition theories. In the first paper of these series, we reported that this is not the case for Gly and nonpolar aliphatic amino acids (Val, Leu, Met, and Ile). Here we have analyzed the helical intrinsic propensities of noncharged polar residues (Ser, Thr, Asn, and Gln) at different positions of a model polyalanine-based peptide. We found that Thr is more favorable (by approximately 0.3 kcal/mol) at positions N1 and N2 than in the helix center, although for Ser, Asn, and Gln the differences are smaller (+/-0.2 kcal/mol), and in many cases within the experimental error. There is a reasonable agreement (+/-0.2 kcal/mol) between the calculated free energies, using the ECEPP/2 force field equipped with a hydration potential, and the experimental data, except at position N1.     

Thermal unfolding of helices of a C-peptide analogue of ribonuclease A in sodium dodecyl sulfate solution

The conformation of a 13-residue C-peptide analogue of ribonuclease A, suc-AET-AAAKFLRAHA-CONH2, in NaDodSO4 solutions with respect to temperature was studied with CD. The equilibrium constant of unfolding yielded a straight line in a van't Hoff plot. In 10 mM NaDodSO4, delta G mu = 120 cal/mol, delta H mu = 700 cal/mol, and delta S mu = 2.0 entropy units all on per helical residue. These values compared fairly well with the thermodynamic parameters of the uncharged helix-coil transition of (Glu)n in 0.1 M NaCl based on the theories of Zimm and Bragg and Zimm and Rice. The peptide was not unfolded at 75 degrees C completely. Even in water without surfactant it was not a "random coil."     

Reversible helix/coil transitions of left-handed Z-DNA structures. Comparison of the thermodynamic properties of poly(dG).poly(dC), poly[d(G-C)].poly[d(G-C)], and poly(dG-m5dC).poly(dG-m5dC)

In contrast to poly(dG).poly(dC), which remains in the B-DNA conformation under all experimental conditions the polynucleotides with the strictly alternating guanine/cytosine or guanine/5'-methylcytosine sequences can change from the classical right-handed B-DNA structure to the left-handed Z-DNA structure when certain experimental conditions such as ionic strength or solvent composition are fulfilled. Up to now the investigation of the helix/coil transition of left-handed DNA structures was not possible because the transition temperature exceeds 98 degrees C. By applying moderate external pressure to the surface of the aqueous polymer solution in the sample cell the boiling point of the solvent water is shifted up the temperature scale without shifting the transition temperature, so that we can measure the helix/coil transition of the polynucleotides at all experimental conditions applied. It can thus be shown that the Z-DNA/coil transition is cooperative and reversible. The Tm is 125 degrees C for poly(dG-m5dC).poly(dG-m5dC) in 2mM Mg2+, 50mM Na+, pH 7.2 and 115 degrees c for poly[d(G-C)].poly[d(G-C)] in 3.04M Na+. The transition enthalpy per base pair was determined by the help of an adiabatic scanning microcalorimeter.