Conformational stability of ribonuclease T1. I. Thermal denaturation and effects of salts.

The thermal transition of RNase T1 was studied by two different methods; tryptophan residue fluorescence and circular dichroism. The fluorescence measurements provide information about the environment of the indole group and CD measurements on the gross conformation of the polypeptide chain. Both measurements at pH 5 gave the same transition temperature of 56 degrees C and the same thermodynamic quantities, delta Htr (= 120 kcal/mol) and delta Str (= 360 eu/mol), for the transition from the native state to the thermally denatured state, indicating simultaneous melting of the whole molecule including the hydrophobic region where the tryptophan residue is buried. Stabilization by salts was observed in the pH range from 2 to 10, since the presence of 0.5 m NaCL caused an increase of about 5 degrees C to 10 degrees C in the transition temperature, depending on the pH. The fluorescence measurements on the RNase T1 complexed with 2'-GMP showed a transition with delta Htr =167 kcal/mol and delta Str =497 eu/mol at a transition temperature about 6 degrees C higher than that for the free enzyme. The large value of delta Htr for RNase T1 indicates the highly cooperative nature of the thermal transition; this value is much higher than those of other globular proteins. Analysis of the CD spectrum of thermally denatured RNase T1 suggests that the denatured state is not completely random but retains some ordered structures.     

Temperature dependence of enthalpy changes for ethidium and propidium binding to DNA: effect of alkylamine chains

Calorimetric titrations have been performed on the binding of ethidium and propidium to calf thymus DNA at temperatures in the 15-60 degrees C range. Enthalpy changes (delta HB) derived from these experiments performed with the new Omega reaction calorimeter have a precision of +/- 0.10 kcal/mol or less at all temperatures. For ethidium (a monocation), delta HB varies little with temperature, and the heat capacity change (delta CP) for the binding reaction derived from these parameters is 10 cal/deg/mol. In contrast, delta HB changes from -6.5 to -8.1 kcal/mol for DNA binding of propidium (a dication due to a charged amine group at the end of an alkyl chain attached to the phenanthridine ring nitrogen), and delta CP is -57 cal/deg/mol. At 21 degrees C a plot of delta HB vs mole ratio is curved downward for propidium in the 0.08-0.25 range, whereas the same plot at 45 degrees C is a straight line from 0.05 to 0.15 and sharply downward thereafter. Similar plots for ethidium follow the latter pattern between 25 and 50 degrees C. These observations and our analyses of delta HB and delta SB are consistent with the hypothesis that the location in the DNA complex and the rotational motion of the alkylamine chain change substantially over the temperature range in this study. Only near 50 degrees C is delta HB equal for the binding of these two cations to DNA, and caution must be used in analyses of enthalpic effects when the temperature dependence for delta HB is not available.     

Tris buffer causes acyl chain interdigitation in phosphatidylglycerol

The structure of the gel phase and the properties of the acyl chain disordering transition of dipalmitoyl phosphatidylglycerol (DPPG) have been studied using differential scanning calorimetry, differential scanning dilatometry, and X-ray diffraction. In the presence of small, monovalent cations, DPPG at 22 degrees C exists in a lamellar phase in which the hydrocarbon chains are tilted from the perpendicular to the bilayer surface. Around 34 degrees C, there is a small pretransition (delta H less than 1 kcal/mol) followed by the main transition at 40.4 degrees C (delta H = 8.3 kcal/mol; delta V = 0.0381 ml/g). If DPPG is suspended in Tris-HCl buffer in the absence of other monovalent cations, X-ray diffraction data show that at 22 degrees C, the gel phase consists of interdigitated acyl chains perpendicular to the plane of the bilayer. No pretransition is observed and the main transition occurs at 41.3 degrees C with delta H = 9.1 kcal/mol and delta V = 0.0514 ml/g. If sufficient Na+ or K+ ions are added to the Tris-buffered DPPG, the phase behavior reverts to what is observed in the absence of Tris. Analysis of the energetics of the main transition shows that the increase in van der Waals interaction energy resulting from the larger delta V in Tris can be compensated by the favorable energetics of removing terminal methyl groups from the bilayer surface. The amount of disordering, i.e. formation of gauche rotamers, is likely to be the same in Tris as it is in buffers without amphiphilic cations.     

Lack of communication between LC2 light chain and the SH1 region of myosin S-1 studied by 19F-NMR

Myosin subfragment-1 (S-1) which contains the LC2 light chain has been labelled with fluorine to allow an 19F-NMR study of the coupling and energetics of structural changes in the myosin head. Two fluorine-containing reagents, N-4-(trifluoromethyl)phenyl iodoacetamide and N-3,5-di(trifluoromethyl)phenyl iodoacetamide, have been used to label the myosin heavy chain at the unusually reactive sulfhydryl-1 (SH1) position. The chemical shift of both reagents on S-1 is sensitive to a structural transition in the region of SH1 which occurs upon increasing the temperature from 0 degrees C to 35 degrees C. The midpoint of the transition in both papain and chymotryptic S-1 is at approximately 11 degrees C at pH 7 (0.1 M CKl). The temperature dependence of the chemical shift may be fit assuming a two-state equilibrium where delta G degree' (T) = 101-110T +0.386 T2 (where T is the temperature in Kelvin). Both delta H degree' (T) and delta S degree' (T) have a small temperature dependence from 0 to 35 degrees C: at 20 degrees C, delta H degree' (T) = -33 kcal/mol. delta S degree' (T) = -116 e.u. and delta Cp = -226 cal/mol per deg (pH 7.0, 0.1 M KCl). The NMR data indicate that the presence of the LC2 light chain in papain S-1 does not modify the structure of S-1 in the vicinity of SH1, nor does it modify the energetics of the structural transition from that seen in its absence with chymotryptic S-1. The presence of calcium which is bound by the LC2 of papain S-1 also does not alter the energetics of the transition. Thus it would appear that the LC2 light chain (on myosin S-1) does not participate in the two-state transition, nor does it interact strongly with regions of the heavy chain which participate in the transition.     

Thermodynamics of phospholipid bilayer assembly

Thermodynamic properties of bilayer assembly have been obtained from measurements of the solubility of the sodium salt of dimyristoylphosphatidylglycerol (DMPG) in water. The standard free energy of bilayer assembly delta G degree a is shown to be RT 1n Xs + zF psi 0 where Xs is the mole fraction of dissolved lipid, F is the Faraday constant, z is the valence of the counterion (Na+), and psi 0 is the electrical double-layer potential of the ionized bilayer. The function d 1n Xs/dT was found to be discontinuous at 24 degrees C, the gel-liquid-crystal transition temperature (Tm) for DMPG. This function was unaffected when solubilities were measured in 0.001 M NaCl solutions; thus, psi 0 is constant in the experimental temperature interval (4-40 degrees C). Using a value of psi 0 = -180 mV [Eisenberg et al. (1979) Biochemistry 18, 5213-5223], and the temperature dependence of delta G degrees a, values for delta H degrees a and delta S degree a at 24 degrees C were calculated for the gel and liquid-crystal states of DMPG. For the gel, delta H degrees a and T delta S a are -26.2 and 12.7 kcal/mol, respectively; for the liquid-crystal, delta H degrees a and T delta S degrees a are -19.2 and -5.7 kcal/mol, respectively. The calculated value for the latent heat of the gel-liquid-crystal transition is 7 kcal/mol, in agreement with calorimetric measurements.     

Titration of the phase transition of phosphatidylserine bilayer membranes. Effects of pH, surface electrostatics, ion binding, and head-group hydration

The dependence of the gel-to-fluid phase transition temperature of dimyristoyl- and dipalmitoylphosphatidylserine bilayers on pH, NaCl concentration, and degree of hydration has been studied with differential scanning calorimetry and with spin-labels. On protonation of the carboxyl group (pK2app = 5.5), the transition temperature increases from 36 to 44 degrees C in the fully hydrated state of dimyristoylphosphatidylserine (from 54 to 62 degrees C for dipalmitoylphosphatidylserine), at ionic strength J = 0.1. In addition, at least two less hydrated states, differing progressively by 1 H2O/PS, are observed at low pH with transition temperatures of 48 and 52 degrees C for dimyristoyl- and 65 and 68.5 degrees C for dipalmitoylphosphatidylserine. On deprotonation of the amino group (pK3app = 11.55) the transition temperature decreases to approximately 15 degrees C for dimyristoyl- and 32 degrees C for dipalmitoylphosphatidylserine, and a pretransition is observed at approximately 6 degrees C (dimyristoylphosphatidylserine) and 21.5 degrees C (dipalmitoylphosphatidylserine), at J = 0.1. No titration of the transition is observed for the fully hydrated phosphate group down to pH less than or equal to 0.5, but it affinity for water binding decreases steeply at pH greater than or equal to 2.6. Increasing the NaCl concentration from 0.1 to 2.0 M increases the transition temperature of dimyristoyphosphatidylserine by approximately 8 degrees C at pH 7, by approximately 5 degrees at pH 13, and by approximately 0 degrees C at pH 1. These increases are attributed to the screening of the electrostatic titration-induced shifts in transition temperature. On a further increase of the NaCl concentration to 5.5 M, the transition temperature increases by an additional 9 degree C at pH 7, 13 degree C at pH 13, approximately 7 degree C in the fully hydrated state at pH 1, and approximately 4 and approximately 0 degree C in the two less hydrated states. These shifts are attributed to displacement of water of hydration by ion binding. From the salt dependence it is deduced that the transition temperature shift at the carboxyl titration can be accounted for completely by the surface charge and change in hydration of approximately 1 H2O/lipid, whereas that of the amino group titration arises mostly from other sources, probably hydrogen bonding. The shifts in pK (delta pK2 = 2.85, delta pK3 = 1.56) are consistent with a reduced polarity in the head-group region, corresponding to an effective dielectric constant epsilon approximately or equal to 30, together with surface potentials of psi congruent to -100 and -150 mV at the carboxyl and amino group pKs, respectively. The transition temperature of dimyristoylphosphatidylserine-water mixtures decreases by approximately 4 degree C each water/lipid molecule added, reaching a limiting value at a water content of approximately 9-10 H2O/lipid molecule.     

Thermodynamics of ion binding to phosphatidic acid bilayers. Titration calorimetry of the heat of dissociation of DMPA.

The heat of dissociation of the second proton of 1,2-dimyristoylphosphatidic acid (DMPA) was studied as a function of temperature using titration calorimetry. The dissociation of the second proton of DMPA was induced by addition of NaOH. From the calorimetric titration experiment, the intrinsic pK0 for the dissociation reaction could be determined by applying the Gouy-Chapman theory. pK0 decreases with temperature from ca. 6.2 at 11 degrees C to 5.4 at 54 degrees C. From the total heat of reaction, the dissociation enthalpy, delta Hdiss, was determined by subtracting the heat of neutralization of water and the heat of dilution of NaOH. In the temperature range between 2 and 23 degrees C, delta Hdiss is endothermic with an average value of ca. 2.5 kcal.mol-1 and shows no clear-cut temperature dependence. In the temperature range between 23 and 52 degrees C, delta Hdiss calculated after subtraction of the heat of neutralization and dilution is not the true dissociation enthalpy but includes contributions from the phase transition enthalpy, delta Htrans, as the pH jump induces a transition from the gel to the liquid-crystalline phase. The delta Cp for the reaction enthalpy observed in this temperature range is positive. Above 53 degrees C, the pH jump induces again only the dissociation of the second proton, and the bilayers stay in the liquid-crystalline phase. In this temperature range, delta Hdiss seems to decrease with temperature. The thermodynamic data from titration calorimetry and differential scanning calorimetry as a function of pH can be combined to construct a complete enthalpy-temperature diagram of DMPA in its two ionization states.     

Effect of basic oligopeptides on the B-Z transition of poly(dG-dC). poly(dG-dC) in water-methanol solutions

The effect of basic oligopeptides (Lys-Ala-Ala)n (n = 1-5, 10) and (Lys-Leu-Ala)n (n = 1-4) on the B-Z transition of poly(dG-dC).poly(dG-dC) in water-methanol solutions was investigated using CD and uv spectroscopy. In the absence of peptides, the concentration of methanol at the midpoint of the B-Z transition is 64% at 25 degrees C. The transition is temperature dependent and the B conformation is preferred at higher temperatures. All peptides tested shift the midpoint of the B-Z transition to lower concentrations of methanol. For shorter peptides this effect increases with an increasing number of monomeric units, showing the importance of the number of positive charges in the peptide molecule. Al conditions of low methanol content, the trimer and tetramer of the (Lys-Leu-Ala)n series have a greater effect on the B-Z transition than the corresponding oligomers of the (Lys-Ala-Ala)n series. This indicates an important influence of the presence of hydrophobic groups in the peptide side chains on the binding. In the presence of peptides, the B-Z transition is also temperature dependent and the B conformation is preferred at higher temperatures. The addition of peptides results in an increase of the transition midpoint and of the transition width. These parameters were used for the calculation of the transition enthalpy delta HB-Z in 65% methanol, which is -1.15 +/- 0.25 kcal/base pair. Since the van't Hoff enthalpy delta HVH calculated from the temperature dependence of the B-Z transition in the absence of peptides is -130 kcal/mol, the length of the cooperative unit is about 110 base pairs. The results suggest that the mechanism of Z-DNA induction is similar but not identical with that involved in the action of metal cations in aqueous solution.     

Thermodynamic parameters associated with the binding of adrenalin and norephedrine to heparin

Pulse radiolysis has been used to determine the thermodynamic parameters (delta G', delta H' and delta S') governing the binding of adrenalin and norephedrine to heparin. These complexes were completely dissociated by increasing concentrations of inorganic salts. Lower concentrations of divalent cations (e.g. Ca2+) than of monovalent cations (e.g. Na+) were necessary to effect dissociation of the complex. For each interaction an increase in drug binding occurred as the temperature was increased from ambient. However, a transition temperature was observed (48 degrees C) above which the drug was progressively released as the temperature was increased. These observations are discussed in terms of conformational changes induced in the polymer below and above its melting temperature.     

Temperature dependence of mammalian muscle contractions and ATPase activities

Isolated rat and mouse extensor digitorum longus (EDL) and soleus muscles were studied under isometric and isotonic conditions at temperatures from approximately 8 degrees -38 degrees C. The rate constant for the exponential rise of tension during an isometric tetanus had a Q10 of approximately 2.5 for all muscles (corresponding to an enthalpy of activation, delta H = 66 kJ/mol, if the rate was determined by a single chemical reaction). The half-contraction time, contraction time, and maximum rate of rise for tension in an isometric twitch and the maximum shortening velocity in an isotonic contraction all had a similar temperature dependence (i.e., delta H approximately 66 kJ/mol). The Mg++ ATPase rates of myofibrils prepared from rat EDL and soleus muscles had a steeper temperature dependence (delta H = 130 kJ/mol), but absolute rates at 20 degrees C were lower than the rate of rise of tension. This suggests that the Mg++ ATPase cycle rate is not limiting for force generation. A substantial fraction of cross-bridges may exist in a resting state that converts to the force-producing state at a rate faster than required to complete the cycle and repopulate the resting state. The temperature dependence for the rate constant of the exponential decay of tension during an isometric twitch or short tetanus (and the half-fall time of a twitch) had a break point at approximately 20 degrees C, with apparent enthalpy values of delta H = 117 kJ/mol below 20 degrees C and delta H = 70 kJ/mol above 20 degrees C. The break point and the values of delta H at high and low temperatures agree closely with published values for the delta H of the sarcoplasmic reticulum (SR) Ca++ ATPase. Thus, the temperature dependence for the relaxation rate of a twitch or a short tetanus is consistent with that for the reabsorption rate of Ca++ into the SR.     

A differential scanning calorimetric study of the conformational transitions of schizophyllan in mixtures of water and dimethylsulfoxide

The thermal conformational transitions of two sonicated samples of schizophyllan were studied in water-dimethylsulfoxide (DMSO) mixtures by high-sensitivity differential scanning calorimetry (DSC). Two transitions were observed over most of the range of solvent compositions. These were assigned to an internal change of the triple helix [T. Itou et al. (1986) Macromolecules 19, 1234-1240] and a triple-helix-single-coil transition [T. Sato et al. (1981) Carbohydr. Res. 95, 195-204], respectively. In water, the former transition observed at lower temperature for a low molecular weight sample, U-1, is centered at 3 degrees C and characterized by the specific enthalpy, delta hcal = 3.29 J g-1. A higher molecular weight sample, M-2, showed this transition at 7 degrees C with delta hcal = 4.39 J g-1. The transition temperature for both samples increased with increasing DMSO concentration up to about 50 degrees C at 70 weight % DMSO, and then rapidly decreased with increasing DMSO concentration, with about 3 degrees C higher for M-2 than for U-1 over the DMSO concentration. The transition was not observed when the concentration of DMSO exceeded 87%. It was found that delta hcal for both samples was a linear function of t 1/2, the temperature of half-completion in degrees C, delta hcal = 0.177t + 2.96. The triple helix-coil transition was observed at around 127 degrees C for U-1 and above 130 degrees C for M-2 in the range of DMSO composition below about 70%. The transition temperature decreased with increasing DMSO concentration at above 70%, and the transition finally disappeared when the DMSO concentration exceeded 90%. The plot of delta hcal vs. t 1/2 for the transition of both samples gave a linear relation, delta hcal = 0.253t - 10.58. The reversibility of the transition at lower temperature was demonstrated by the reversibility of the curves when the first heating was stopped before the second transition. Once the heating was performed over the second transition, the reheating DSC curves showed several endothermic peaks, indicating the irreversibility of the transition and heterogeneity in the conformation of the heated schizophyllan.     

Differences in thermal stability between reduced and oxidized cytochrome b562 from Escherichia coli

The thermal stabilities of ferri- and ferrocytochrome b562 were examined. Thermally induced spectral changes, monitored by absorption and second-derivative spectroscopies, followed the dissociation of the heme moiety and the increased solvation of tyrosine residue(s) located in close proximity to the heme binding site. All observed thermal transitions were independent of the rate of temperature increase (0.5-2 degrees C/min), and the denatured protein exhibited partial to near-complete reversibility upon return to ambient temperature. The extent of renaturation of cytochrome b562 is dependent on the amount of time the unfolded conformer is exposed to temperatures above the transition temperature, Tm. All thermally induced spectra changes fit a simple two-state model, and the thermal transition was assumed to be reversible. The thermal transition for ferrocytochrome b562 yielded Tm and van't Hoff enthalpy (delta HvH) values of 81.0 degrees C and 137 kcal/mol, respectively. In contrast, Tm and delta HvH values obtained for the ferricytochrome were 66.7 degrees C and 110 kcal/mol, respectively. The estimated increase in the stabilization free energy at the Tm of ferricytochrome b562 following the one-electron reduction to the ferrous form, where delta delta G = delta Tm delta Sm [delta Sm = 324 cal/(K.mol), delta Tm = 14.3 degrees C] [Becktel, W. J., & Schellman, J. A. (1987) Biopolymers 26, 1859-1877], is 4.6 kcal/mol.     

Anomalous change in the specific conductivity in lipoproteins at around physiologic temperatures

Studying the temperature dependence of conductivity sigma of rat and human lipoproteins and apoprotein A-I fractions revealed an anomalous region in the range of temperatures (35-38) +/- 0.5 degree C. The activation energy delta H and temperature coefficient sigma (delta sigma/delta T) on both sides of Tc and the heat of transition (delta H of transition) were calculated. In high-density human lipoproteins and apoA-I, the delta H value was found to be very low. Some mechanisms of interaction of hydrocortizone with high-density lipoproteins and apoA-I were studied by using IR-spectroscopy and conductometry were studied. It was found that the hormone considerably increases the portion of alpha-helices and beta-structures in these proteins (coil<-->alpha-helix and coil<-->beta-structure transitions). In this case, delta H value of the transition increases 13-fold; in addition, the abnormal region in apoA-I shifts 1-2 degrees C downwards. The anomalous changes in conductivity in the range of physiological temperatures in all lipoprotein fractions including apoA-I are probably related to structural phase transitions both in proteins and in phospholipids. Since the delta H value of the transition in human high-density lipoproteins is small, it is assumed that, in phospholipids of these particles, an orientation transition of the A<-->C smectic type takes place, which is assigned to the second-order phase transition. The structural transition in apoA-I can probably also be assigned to the second-order phase transition since the enthalpia of the transition is very small; presumably, this transition is related to changes in symmetry due to changes in the secondary structure (coil<-->beta-tructure transition).     

The cholesterol-side-chain-cleaving cytochrome P450 spin-state equilibrium. 1. Thermodynamic analysis.

We have investigated the spin-state equilibrium of adrenal mitochondrial P450scc (cholesterol-side-chain-cleaving, CYP11A1) by absorption spectroscopy in the Soret band as a function of pH and temperature. The van't Hoff plot of the high-spin/low-spin equilibrium is not linear and is shifted towards high spin by lowering the pH. This non-linearity resolves clearly into two phases when the temperature range is extended from 37 degrees C to -20 degrees C using ethylene glycol as anti-freeze cosolvent. This enabled us to measure the enthalpy and entropy changes which are delta HA = 0.7 kJ.mol-1 and delta SA = 5J.K-1.mol-1 at low temperatures and delta HB = -42 kJ.mol-1 and delta SB = -152 J.K-1.mol-1 at high temperatures. The transition temperature, Tbreak, between both phases decreases as a function of pH. The experimental data can be fitted by a minimal reactional model comprising a temperature dependent conformational transition and two ionisation steps (one for each conformation), the pK of which is 1.5 +/- 0.5 higher in the low-temperature conformation. The deduced conformational equilibrium is affected by physiological effectors: Tbreak depends on the nature of the substrate intermediate and on the presence of the physiological electron donor, adrenodoxin.     

Interactions of divalent cations with phosphatidylserine bilayer membranes

The interaction of divalent cations with a homologous series of diacylphosphatidylserines (diacyl-PS) has been studied by differential scanning calorimetry and X-ray diffraction. Hydrated di-C14-PS (DMPS) exhibits a gel leads to liquid-crystal bilayer transition at 39 degrees C (delta H = 7.2 kcal/mol of DMPS). With increasing MgCl2 concentration, progressive conversion to a phase exhibiting a high melting (98 degrees C), high enthalpy (delta H congruent to 11.0 kcal/mol of DMPS) transition is observed. Similar behavior is observed for DMPS with increasing CaCl2 concentration. In this case, the high-temperature transition of the Ca2+-DMPS complex occurs at approximately 155 degrees C and is immediately followed by an exothermic transition probably associated with PS decomposition. For di-C12-, di-C14-, di-C16- (DPPS), and di-C18-PS, the transition temperatures of the Ca2+-PS complexes are in the range 151-155 degrees C; only di-C10-PS exhibits a significantly lower value, 142 degrees C. A different pattern of behavior is exhibited by DPPS in the presence of Sr2+ or Ba2+, with transitions in the range 70-80 degrees C being observed. X-ray diffraction of the Ca2+-PS complexes at 20 degrees C provides evidence of structural homology. All Ca2+-PS complexes exhibit bilayer structures, the bilayer periodicity increasing linearly from 35.0 A for di-C10-PS to 52.5 A for di-C18-PS. Wide-angle X-ray diffraction data indicate that hydrocarbon chain "crystallization" occurs on Ca2+-PS complex formation.(ABSTRACT TRUNCATED AT 250 WORDS)     

Calorimetric and spectroscopic investigation of the unfolding of human apolipoprotein B

The unfolding of human apolipoprotein B-100 in its native lipid environment, low density lipoprotein (LDL), and in a soluble, lipid-free complex with sodium deoxycholate (NaDC) has been examined using differential scanning calorimetry (DSC) and near UV circular dichroic (CD) spectroscopy. High resolution DSC shows that LDL undergoes three thermal transitions. The first is reversible and corresponds to the order-disorder transition of the core-located cholesteryl esters (CE) (Tm = 31.1 degrees C, delta H = 0.75 cal/g CE). The second, previously unreported, is reversible with heating up to 65 degrees C (Tm = 57.1 degrees C, delta H = 0.20 cal/g apoB) and coincides with a reversible change in the tertiary structure of apoB as shown by near UV-CD. No alteration in the secondary structure of apoB is observed over this temperature range. The third transition is irreversible (Tm = 73.5 degrees C, delta H = 0.99 cal/g apoB) and coincides with disruption of the LDL particle and denaturation of apoB. The ratio of delta H/delta HvH for the reversible protein-related transition suggests that this is a two-state event that correlates with a change in the overall tertiary structure of the entire apoB molecule. The second protein-related transition is complex and coincides with irreversible denaturation. ApoB solubilized in NaDC undergoes three thermal transitions. The first two are reversible (Tm = 49.7 degrees C, delta H = 1.13 cal/g apoB; Tm = 56.4 degrees C, delta H = 2.55 cal/g apoB, respectively) and coincide with alterations in both secondary and tertiary structure of apoB. The changes in secondary structure reflect an increase in random coil conformation with a concomitant decrease in beta-structure, while the change in tertiary structure suggests that the conformation of the disulfide bonds is altered. The third transition is irreversible (Tm = 66.6 degrees C, delta H = 0.54 cal/g apoB) and coincides with complete denaturation of apoB and disruption of the NaDC micelle. The ratio of delta H/delta HvH for the two reversible transitions indicates that each of these transitions is complex which may suggest that several regions or domains of apoB are involved in each thermal event.     

Calorimetric studies of the effects of cholesterol on the phase transition of C(18):C(10) phosphatidylcholine.

Differential scanning calorimetry (DSC) has been employed to study the effects of cholesterol on the phase transition of C(18):C(10) phosphatidylcholine (C(18):C(10)PC). C(18):C(10)PC is an asymmetric mixed-chain phosphatidylcholine known to form mixed-interdigitated structures below the transition temperature and form partially interdigitated lipid bilayers above the transition. Three types of samples were used. The treated sample is the lipid dispersion that had undergone three freeze-thaw cycles and stored at 4 degrees C for more than 48 h. The untreated sample was made by vortexing the dry lipid in 50 mM KCl, without the above-mentioned pretreatment. The cold-treated sample was prepared by incubating the treated sample at -20 degrees C for 15 d. There is no apparent difference in the DSC curves between the treated and cold-treated samples. The data derived from the treated samples seem to be more reproducible. The DSC curves between the cholesterol/C(18):C(10)PC and cholesterol/symmetric diacylphosphatidylcholine mixtures are different in three aspects: overall appearance, the cholesterol dependence of delta H, and the effect of cholesterol on the maximal transition temperature Tm, the onset temperature To, and the completion temperature Tc. for both the treated and untreated samples, the total enthalpy change delta H of the phase transition of C(18):C(10)PC decreases with increasing cholesterol content, approaching zero at approximately 25 mol%. This level is lower than the total enthalpy changes reported previously for the cholesterol/symmetric diacylphosphatidylcholine mixtures. Both the heating and cooling thermograms show that Tm, To, and Tc decrease with increasing cholesterol content. The decreasing rates of these temperatures with cholesterol are in the neighborhood of -0.24 degree per mol% of cholesterol.(ABSTRACT TRUNCATED AT 250 WORDS)     

A jump in an Arrhenius plot can be the consequence of a phase transition. The binding of ATP to myosin subfragment 1

The temperature dependence of the kinetics of the binding of ATP to myosin subfragment-1 was studied by an ATP chase technique in a rapid-flow-quench apparatus: (formula; see text) A temperature range of 30 degrees C to -15 degrees C was obtained with ethylene glycol as antifreeze. The Arrhenius plot of k2 is discontinuous with a jump at 12 degrees C. Above the jump delta H+ = 9.5 kcal/mol, below delta H+ = 28.5 kcal/mol. Few such Arrhenius plots are recorded in the literature but they are predicted from theory. Thus, we explain our results as a phase change of the subfragment 1-ATP system at 12 degrees C. This is in agreement with certain structural studies.     

Static response in body temperature regulation of the euthermic warm-acclimated golden hamster (Mesocricetus auratus)

A characteristic feature of the body temperature regulation of euthermic golden hamsters is a great individual variability of body temperature in the thermoneutral zone. Resting values of the total metabolic rate (M) at ambient temperature 30-34 degrees C vary from 5.3 to 8.8 W.kg-1 between individuals, body temperature reaching 33.5-37.7 degrees C (subcutaneous temperature, Ts) and 35.4-39.0 degrees C (hypothalamic temperature, Th). The dependence of metabolic heat production on steady deviations of peripheral and central body temperature from the resting values in nonlinear in general, but the unknown functional relationship delta M = f (delta Th, delta Ts) can be replaced by a single linear regression function of Ts by neglecting the change of central body temperature: delta M = 2.14-2.00. delta Ts. Total body thermosensitivity of the golden hamster determined from steady changes of rectal temperature and metabolic rate after external cooling is -6.8 +/- 1.3 W.kg-1. degrees C-1.     

Alpha-DNA VIII: thermodynamic parameters of complexes formed between the oligo-alpha-deoxynucleotides: alpha-d(GGAAGG) and alpha-d(CCTTCC) and their complementary oligo-beta-deoxynucleotides: beta-d(CCTTCC) and beta-d(GGAAGG) are different.

The temperature dependence of the formation of a complex between an alpha-d(CCTTCC) hexanucleotide and its complementary beta-d(GGAAGG) sequence was studied and compared to the formation of the beta-d(CCTTCC):beta-d(GGAAGG) complex. Such alpha-beta complex is more stable than the regular beta:beta complex. The Tm value for the alpha:beta complex is 28 degrees C (delta G degrees = -7.3 kcal/mole) while Tm = 20, 1 degree C (delta G degrees = -6.3 kcal/mole) for the beta:beta complex. The stoechiometry of the alpha:beta complex corresponds to the formation of a 1:1 duplex. However, when the alpha- strand is made of alpha-purines: alpha-d(GGAAGG), the stability of the alpha:beta complex, alpha-d(GGAAGG):beta-d(CCTTCC) is found to be lower (Tm = 13.8 degrees C) than the stability of the regular beta-beta complex, leading to the conclusion that the nature of the alpha-sequence is important in terms of stability when considering the synthesis of such a sequence for using it as antisense oligonucleotide.