Entropy and heat capacity of DNA melting from temperature dependence of single molecule stretching

When a single molecule of double-stranded DNA is stretched beyond its B-form contour length, the measured force shows a highly cooperative overstretching transition. We have measured the force at which this transition occurs as a function of temperature. To do this, single molecules of DNA were captured between two polystyrene beads in an optical tweezers apparatus. As the temperature of the solution surrounding a captured molecule was increased from 11 degrees C to 52 degrees C in 500 mM NaCl, the overstretching transition force decreased from 69 pN to 50 pN. This reduction is attributed to a decrease in the stability of the DNA double helix with increasing temperature. These results quantitatively agree with a model that asserts that DNA melting occurs during the overstretching transition. With this model, the data may be analyzed to obtain the change in the melting entropy DeltaS of DNA with temperature. The observed nonlinear temperature dependence of DeltaS is a result of the positive change in heat capacity of DNA upon melting, which we determine from our stretching measurements to be DeltaC(p) = 60 +/- 10 cal/mol K bp, in agreement with calorimetric measurements.     

Triple helix DNA oligomer melting measured by fluorescence polarization anisotropy

A synthetic DNA triple helix sequence was formed by annealing a pyrimidinic 21 mer single strand sequence onto the complementary purinic sequence centred on a 27 mer duplex DNA. Melting of the third strand was monitored by UV spectrophotometry in the temperature range 10-90 degrees C. The T(m) of the triplex, 37 degrees C, was well separated from the onset of duplex melting. When the same triple helix was formed on the duplex bearing one nick in the center of the pyrimidinic sequence the T(m) of the triplex was shifted to approximately 32 degrees C and overlapped the melting of the duplex. We have used fluorescence polarization anisotropy (FPA) measurements of ethidium bromide (EB) intercalated in duplex and triplex samples to determine the hydrodynamic parameters in the temperature range 10-40 degrees C. The fluorescence lifetime of EB in the samples of double and triple stranded DNA is the same (21.3 +/- 0.5 ns) at 20 degrees C, indicating that the geometries of the intercalation sites are similar. The values for the hydration radii of the duplex, normal triplex, and nicked triplex samples were 10.7 +/- 0.2, 12.2 +/- 0.2, and 12.0 +/- 0.2 A. FPA measurements on normal triplex DNA as a function of temperature gave a melting profile very similar to that derived by UV absorption spectroscopy. For the triplex carrying a nick, the melting curve obtained using FPA showed a clear shift compared with that obtained for the normal triplex sample. The torsional rigidity of the triplex forms was found to be higher than that of the duplex form.     

Changes in chromatin structure during the aging of cell cultures as revealed by differential scanning calorimetry

Nuclei from cultured human cells were examined by differential scanning calorimetry. Their melting profiles revealed four structural transitions at 60, 76, 88, and 105 degrees C (transitions I-IV, respectively). In immortalized (i.e., tumor) cell cultures and in normal cell cultures of low passage number, melting profiles were dominated by the 105 degrees C transition (transition IV), but in vitro aging of normal and Werner syndrome cells was associated with a marked decrease in transition IV followed by an increase in transition III at the expense of transition IV. At intermediate times in the aging process, much DNA melted at a temperature range (95-102 degrees C) intermediate between transitions III and IV, and this is consistent with the notion that aging of cell cultures is accompanied by an increase in single-strand character of the DNA. Calorimetric changes were observed in the melting profile of nuclei from UV-irradiated tumor cells that resembled the age-induced intermediate melting of chromatin. It is suggested that aging is accompanied by an increase in single-stranded character of the DNA in chromatin, which lowers its melting temperature, followed by strand breaks in the DNA that destroy its supercoiling potential.     

Salt dependence and thermodynamic interpretation of the thermal denaturation of small DNA restriction fragments.

The influence of cation concentration on the thermal denaturation of DNA restriction fragments from the E. coli lac regulatory region and from pVH51, ranging in size from 43- to 880- bp, is described. Upon increasing the ionic strength, the melting transitions broaden in a cooperative manner at salt concentrations characteristic for the specific fragment. For three fragments studied in detail, the salt concentration dependence at the midpoint varied between 0.03 and 0.19 M Na+. Along with the broadening, the melting transitions become more symmetrical. This result is discussed with respect to the irreversibility of melting transitions at low ionic strength. After a cooperative broadening, the shape of the melting curves remains constant up to salt concentrations of 0.5 M Na+. The dTM/dlog[Na+] values for three fragments fall between 15.7 and 16.7. An easily applicable approximation of the van't Hoff equation is used to evaluate the enthalpies of 13 transitions arising from the denaturation of 43 to 600 bp. The results of this analysis are compared to calculations of the expected enthalpies based on calorimetric measurements. The TMs of most transitions were directly related to the base composition, but several deviations from the predicted behavior were observed. The possible influences of fragment length and sequence on the thermal stability are discussed. The experimental and mathematical procedure to resolve a thermal denaturation transition with a width f 0.17 +/- 0.01 degrees and its distinction from another preceeding transition only approximately 0.15 degrees away in an 880-bp Hae III fragment from pVH51 is described. This transition is about half as wide as the smallest one reported to date.     

Ligase-deficient yeast cells exhibit defective DNA rejoining and enhanced gamma ray sensitivity.

Yeast cells deficient in DNA ligase were also deficient in their capacity to rejoin single-strand scissions in prelabeled nuclear DNA. After high-dose-rate gamma irradiation (10 and 25 krads), cdc9-9 mutant cells failed to rejoin single-strand scissions at the restrictive temperature of 37 degrees C. In contrast, parental (CDC9) cells (incubated with mutant cells both during and after irradiation) exhibited rapid medium-independent DNA rejoining after 10 min of post-irradiation incubation and slower rates of rejoining after longer incubation. Parental cells were also more resistant than mutant cells to killing by gamma irradiation. Approximately 2.5 +/- 0.07 and 5.7 +/- 0.6 single-strand breaks per 10(8) daltons were detected in DNAs from either CDC9 or cdc9-9 cells converted to spheroplasts immediately after 10 and 25 krads of irradiation, respectively. At the permissive temperature of 23 degrees C, the cdc9-9 cells contained 2 to 3 times the number of DNA single-strand breaks as parental cells after 10 min to 4 h of incubation after 10 krads of irradiation, and two- to eightfold more breaks after 10 min to 2.5 h of incubation after 25 krads of irradiation. Rejoining of single-strand scissions was faster in medium. After only 10 min in buffered growth medium and after 10 krads of irradiation, the number of DNA single-strand breaks was reduced to 0.32 +/- 0.3 (at 23 degrees C) or 0.21 +/- 0.05 (at 37 degrees C) per 10(8) daltons in parental cells, but remained at 2.1 +/- 0.06 (at 23 degrees C) or 2.3 +/- 0.07 (at 37 degrees C) per 10(8) daltons in mutant cells. After 10 or 25 krads of irradiation plus 1 h of incubation in medium at 37 degrees C, only DNA from CDC9 cells was rejoined to the size of DNA from unirradiated cells, whereas at 23 degrees C, DNAs in both strains were completely rejoined.     

Conformational stability of the myosin rod

Chymotryptic cleavage patterns of myosin rods from pig stomach, chicken gizzard, and rabbit skeletal muscle indicate that short (approximately 45 nm) heavy meromyosin subfragment 2 (SF2) is a consistent product of all three rods, whereas long (approximately 60 nm) SF2 is derived only from skeletal muscle myosin. Differential scanning calorimetry was used to follow the thermally induced melting transition of the rods and certain of their subfragments. In 0.12 M KCl, sodium phosphate buffer, pH 6.2-7.6, the light meromyosin (LMM) and SF2 domains of each rod had essentially identical conformational stabilities. Temperature midpoints for the melting transitions were 54-56 degrees C for the two smooth muscle myosin rods and 50-53 degrees C for the skeletal muscle myosin rod. In 0.6 M K Cl buffer, melting transitions for the smooth muscle myosin rods were essentially unchanged, but skeletal muscle myosin rods showed multiphase melting, with major transitions at 43 degrees C and 52 degrees C. The first of these was tentatively attributed to LMM, and the second to SF2. In 0.12 M K Cl buffer, the LMM transition was stabilised so that it superimposed on that of SF2. No melting was observed in any of the rods at physiological temperature. These results indicate that, excluding a possible but only narrow hinge region, the entire myosin rod has essentially uniform conformational stability at physiological pH and ionic strength, and thus that the contractile and elastic properties of the cross-bridge exist in the heavy meromyosin subfragment 1 (SF1) domains of the molecule.     

Thermal transitions of myosin and its helical fragments. Regions of structural instability in the myosin molecule.

The structural stabilities of all the familiar proteolytic fragments of myosin have been investigated in melting studies over the pH ranges 5.5-7.0 in 0.5 M KCl. All fragments except subfragment 2 undergo a melting transition manifested by the cooperative uptake of protons in the temperature range 34-47 degrees C, and these fragments experience an increase in transition temperature, Tm as the pH is increased. Subfragment 2 undergoes a melting transition in the 43-55 degrees C range, manifested by the dissociation of protons, and it experiences a decrease in Tm as the pH is increased. These results suggest that pH changes can modulate the relative stabilities of the light meromysin, subfragment-1, and subfragment-2 regions of the myosin molecule.     

Positional independence and additivity of amino acid replacements on helix stability in monomeric peptides

The 17-residue peptide acetylAEAAAKEAAAKEAAAKAamide, described as an autonomous folding unit (Marqusee & Baldwin, 1987), has been used to examine the effect of amino acid replacements on helix stability. Alanine residues(s) at positions 4, 9, and 14 in the peptide sequence were replaced either singly or multiply by either serine or methionine residues with solid-phase peptide synthesis. The thermal dependence of the helix/coil transition of each peptide was observed by far-ultraviolet circular dichroism. Within experimental variation, all three single replacements exhibit a common thermal transition, and all three double replacements exhibit a different common thermal transition. These results suggest that replacement of the central alanine residue in the repeat EAAAK located in the N-terminus, in the middle, or in the C-terminus of the peptide helix has the same effect on helix stability. The melting temperature of each thermal transition was estimated by assuming a linear van't Hoff plot and a change in molar ellipticity of 33,500 deg cm2 dmol-1. Such analysis indicates that each replacement of an alanine residue by a serine residue diminishes the melting temperature by 11 +/- 1 degrees C and that each replacement of an alanine residue by a methionine residue diminishes the melting temperature by 6 +/- 1 degrees C. These results suggest that the effect of these replacements on helix stability is additive.     

Control of local heat gain by vasomotor response of the hand

Finger blood flow (BF) was measured by venous occlusion plethysmography using mercury-in-Silastic strain gauges during immersion of one hand in hot water (raised by steps of 2 degrees C every 10 min from 35 to 43 degrees C), the other being a control (kept immersed in water at 35 degrees C). The measurements were made in three different thermal states on separate days: 1) cool-25 degrees C, 40% rh, esophageal temperature (Tes) = 36.64 +/- 0.10 degrees C; 2) warm-35 degrees C, 40% rh, Tes = 36.71 +/- 0.11 degrees C; and 3) hot-35 degrees C, 80% rh with the legs immersed in water at 42 degrees C, Tes = 37.26 +/- 0.11 degrees C. When water temperature was raised at 42 degrees C, Tes = 37.26 +/- 0.11 When water temperature was raised to 39-41 degrees C in the warm state, finger BF in the hand heated locally (BFw) decreased. When water temperature was raised to 43 degrees C, however, BFw returned to the control value. In the hot state, Tes rose steadily, reaching 37.90 +/- 0.12 degrees C at the end of the 50-min sessions. BF in the control finger also increased gradually during the session. BFw showed a tendency to decrease when water temperature was raised to 39 degrees C, but the change was not greater than that observed in the warm state. In the cool state, no such reduction in BFw was observed when water temperature was raised to 39-41 degrees C. On the contrary, BFw increased at water temperatures of 41-43 degrees C.(ABSTRACT TRUNCATED AT 250 WORDS)     

Thermal stability of PNA/DNA and DNA/DNA duplexes by differential scanning calorimetry

Thermodynamics of the thermal dissociation transitions of 10 bp PNA/DNA duplexes and their corresponding DNA/DNA duplexes in 10 mM sodium phosphate buffer (pH 7.0) were determined from differential scanning calorimetry (DSC) measurements. The PNA/DNA transition temperatures ranged from 329 to 343 K and the calorimetric transition enthalpies ranged from 209 +/- 6 to 283 +/- 37 kJ mol(-1). The corresponding DNA/DNA transition temperatures were 7-20 K lower and the transition enthalpies ranged from 72 +/- 29 to 236 +/- 24 kJ mol(-1). Agreement between the DSC and UV monitored melting (UVM) determined transition enthalpies validated analyzing the UVM transitions in terms of a two-state transition model. The transitions exhibited reversibility and were analyzed in terms of an AB = A + B two-state transition model which yielded van't Hoff enthalpies in agreement with the transition enthalpies. Extrapolation of the transition enthalpies and free energy changes to ambient temperatures yielded more negative values than those determined directly from isothermal titration calorimetry measurements on formation of the duplexes. This discrepancy was attributed to thermodynamic differences in the single-strand structures at ambient and at the transition temperatures, as indicated by UVM measurements on single DNA and PNA strands.     

Relationship of hyperthermia-induced hemolysis of human erythrocytes to the thermal denaturation of membrane proteins

Hemolysis of human erythrocytes as a function of time of exposure to 47.4-54.5 degrees C was measured and correlated to thermal transitions in the membranes of intact erythrocytes as determined by differential scanning calorimetry (DSC). Curves of hemoglobin leakage (a measure of hemolysis) as a function of time have a shoulder region exhibiting no leakage, indicative of the ability to accumulate sublethal damage (i.e., damage not sufficient to cause lysis), followed by a region of leakage approximating pseudo-first-order kinetics. Inverse leakage rates (Do) of 330-21 min were obtained from 47.4-54.5 degrees C, respectively. A relatively high activation energy of 304 +/- 22 kJ/mol was obtained for leakage, eliminating the involvement of metabolic processes but implicating a transition as the rate-limiting step. Membrane protein involvement was suggested by the very low rate (10(-2) of the rate from erythrocytes) and low activation energy (50 +/- 49 kJ/mol) of hemoglobin leakage from liposomes containing no membrane protein. A model was developed that predicts a transition temperature (Tm) for the critical target (rate-limiting step) of 60 degrees C when measured at a scan rate of 1 K/min. DSC scans were obtained from intact erythrocytes and a procedure developed to fit and remove the transition for hemoglobin denaturation which dominated the scan. Three transitions remained (transitions A, B, and C) with Tm values of 50.0, 56.8, and 63.8 degrees C, respectively. These correspond to, but occur at slightly different temperatures than, the A, B, and C transitions of isolated erythrocyte membranes in the same salt solution (Tm = 49.5, 53-58, and 65.5 degrees C, respectively). In addition, the relative enthalpies of the three transitions differ between isolated membranes and erythrocytes, suggestive of membrane alterations occurring during isolation. Thus, all analyses were conducted on DSC scans of intact erythrocytes. The B transition is very broad and probably consists of several transitions. An inflection, which is seen as a distinct peak (transition B3) in fourth-derivative curves, occurs at 60.8 degrees C and correlates well with the predicted Tm of the critical target. Ethanol (2.2%) lowers the Tm of B3 by 4.0-4.5 K, close to the shift of 3.3 K predicted from its effect on hemolysis. Glycerol (10%) has very little effect on both hemolysis and the Tm of B3, but it stabilizes spectrin (delta Tm = 1.5 K) against thermal denaturation.(ABSTRACT TRUNCATED AT 400 WORDS)     

Thermodynamic, thermomechanical, and structural properties of a hydrated asymmetric phosphatidylcholine.

1-Behenyl-2-lauryl-sn-glycero-3-phosphocholine (22/12 PC) belongs to a unique group of phospholipids in which the molecule has one acyl chain almost twice as long as the other. The temperature-composition phase diagram for this lipid in the range of 25-65 degrees C, and 0 to 84.3% (w/w) water has been constructed by using the isoplethal method in the heating direction and x-ray diffraction for phase identification and structure characterization. At water contents between 10.3 and 34% (w/w) and at temperatures below 43 degrees C, a single mixed interdigitated lamellar gel phase (Lm beta, [symbol: see text]) of the type described by Hui et al. (1984. Biochemistry. 23:5570-5577) and McIntosh et al. (1984. Biochemistry. 23:4038-4044) was found. A second phase consisting of bulk aqueous solution coexists with the Lm beta phase at hydration levels above 34% (w/w) water in the temperature range between 25 and 43 degrees C. Above 43 degrees C, a partially interdigitated lamellar liquid crystalline (Lp alpha) phase ([symbol: see text]) is seen in the water concentration range extending from 0 to 84.3% (w/w). The pure Lp alpha phase is found below 43% (w/w) water, while coexistence of the Lp alpha phase and the bulk aqueous solution is observed above this water concentration which marks the hydration boundary. Interestingly, the latter boundary for both Lm beta and Lp alpha phases is nearly vertical in the temperature range studied. Furthermore, the lamellar chain-melting transition temperature appears to be relatively insensitive to hydration in the range 0-85% (w/w) water. We have confirmed the identify of the Lm beta phase by constructing a 5.7-A resolution electron density profile on oriented samples by the swelling method. Temperature-induced chain melting effects an increase in lipid bilayer thickness suggesting that the Lp alpha phase has chains packed in the partially as opposed to the mixed interdigitated configuration. Unlike the symmetric phosphatidylcholines a ripple (P beta') phase was not found as an intermediate between the low and high temperature lamellar phases of 22/12 PC. The specific volume of 22/12 PC is 940 (+/- 1) microliter/g and 946 (+/- 1) microliter/g in the hydrated lamellar gel state at 28 (+/- 2) and 40 (+/- 2) degrees C, respectively, from neutral buoyancy experiments. Based on measurements of the temperature dependence of the various lattice parameters of the different phases encountered in this study the corresponding lattice thermal expansion coefficients have been measured. These are discussed and their dependence on lipid hydration is reported.     

Preliminary dielectric measurement and analysis protocol for determining the melting temperature and binding energy of short sequences of DNA in solution

Measurement of the real dielectric constant of bulk buffer solutions containing short sequences of DNA as a function of temperature through the DNA melting or denaturiztion transition can be used to determine melting temperatures, T(m), and to estimate the binding energy of the complimentary strands. We describe a preliminary dielectric measurement and analysis protocol to determine these parameters and its application to two known short sequences. The relative real dielectric constant for the bulk solutions was determined over the frequency range of 50 Hz-20 kHz and temperature range of <40-65 degrees C. The measurements were performed on dilute solutions and utilized low electric field strengths. Based on fits to the data by modified sigmoid functions, the melting temperatures, width of transition, and binding energy for the two sequences in solution were estimated. It was observed that the order of the transition appeared to be second order. The results were then compared against predictions of a number of models from the literature that provide theoretical estimates for the melting temperatures of known short sequences of DNA.     

The effect of osmotic pressure on the membrane fluidity of Saccharomyces cerevisiae at different physiological temperatures

Membrane fluidity in whole cells of Saccharomyces cerevisiae W303-1A was estimated from fluorescence polarization measurements using the membrane probe, 1,6-diphenyl-1,3,5-hexatriene, over a wide range of temperatures (6-35 degrees C) and at seven levels of osmotic pressure between 1.38 MPa and 133.1 MPa. An increase in phase transition temperatures was observed with increasing osmotic pressure. At 1.38 MPa, a phase transition temperature of 12 +/- 2 degrees C was observed, which increased to 17 +/- 4 degrees C at 43.7 MPa, 21+/- 7 degrees C at 61.8 MPa, and 24 +/- 9 degrees C at an osmotic pressure of 133.1 MPa. From these results we infer that, with increases in osmotic pressure, the change in phospholipid conformation occurs over a larger temperature range. These results allow the representation of membrane fluidity as a function of temperature and osmotic pressure. Osmotic shocks were applied at two levels of osmotic pressure and at nine temperatures, in order to relate membrane conformation to cell viability.     

Elongation of tandem repetitive DNA by the DNA polymerase of the hyperthermophilic archaeon Thermococcus litoralis at a hairpin-coil transitional state: a model of amplification of a primordial simple DNA sequence

DNA is replicated by DNA polymerase semiconservatively in many organisms. Accordingly, the replicated DNA does not become larger than the original DNA (template DNA), implying that replicative synthesis by DNA polymerase alone cannot explain the diversification of primordial simple DNA. We demonstrate that a single-stranded tandem repetitive oligodeoxyribonucleic acid (oligoDNA) composed of a palindromic or quasi-palindromic motif sequence and 25-50% GC content is elongated in vitro to more than 20,000 bases at 70-74 degrees C by the DNA polymerase of the hyperthermophilic archaeon Thermococcus litoralis without a bimolecular primer-template complex. The efficiency of elongation decreased when the palindromic structure of the oligoDNA was destroyed or when the GC content of the oligoDNA was outside the range of 25-50%. The thermal melting transition profile of the oligoDNA, as observed by ultraviolet spectroscopy, exhibited a biphasic curve, reflecting a duplex-hairpin transition at 31-40 degrees C and a hairpin-coil transition at 70-77 degrees C. The optimal reaction temperature for the elongation, for instance, of oligoDNA (AGATATCT)(6) (72 degrees C) was very close to its hairpin-coil transition melting temperature (70.4 degrees C), but was markedly higher than the temperature at which duplex oligoDNA can exist stably (<35.9 degrees C). These results suggest that a hairpin-based "intramolecular primer-template structure" is formed transiently in the oligoDNA, and it is elongated by the DNA polymerase to long DNA through repeated cycles of folding and melting of the hairpin structure. We discuss the implication of this phenomenon, "hairpin elongation", from the standpoint of potential amplification of simple DNA sequences during the evolution of the genome.     

Thermodynamic dependence of DNA/DNA and DNA/RNA hybridization reactions on temperature and ionic strength

The thermodynamics of 5'-ATGCTGATGC-3' binding to its complementary DNA and RNA strands was determined in sodium phosphate buffer under varying conditions of temperature and salt concentration from isothermal titration calorimetry (ITC). The Gibbs free energy change, DeltaG degrees of the DNA hybridization reactions increased by about 6 kJ mol(-1) from 20 degrees C to 37 degrees C and exhibited heat capacity changes of -1.42 +/- 0.09 kJ mol(-1) K(-1) for DNA/DNA and -0.87 +/- 0.05 kJ mol(-1) K(-1) for DNA/RNA. Values of DeltaG degrees decreased non-linearly by 3.5 kJ mol(-1) at 25 degrees C and 6.0 kJ mol(-1) at 37 degrees C with increase in the log of the sodium chloride concentration from 0.10 M to 1.0 M. A near-linear relationship was observed, however, between DeltaG degrees and the activity coefficient of the water component of the salt solutions. The thermodynamic parameters of the hybridization reaction along with the heat capacity changes were combined with thermodynamic contributions from the stacking to unstacking transitions of the single-stranded oligonucleotides from differential scanning calorimetry (DSC) measurements, resulting in good agreement with extrapolation of the free energy changes to 37 degrees C from the melting transition at 56 degrees C.     

Thermodynamic studies of purple membrane

Differential dilatometric and differential scanning calorimetric measurements have been made of purple membrane with an emphasis upon the temperature range 5 degrees C less than T less than 45 degrees C. The coefficient of thermal expansion alpha is about 7 X 10(-4)/Cdeg up to 30 degrees C and decreases at higher temperatures. The specific heat increases rapidly with temperature with absolute values in the range 0.30-0.45 cal/Cdeg per g. A nearly constant alpha juxtaposed with a rapidly increasing specific heat is similar to the properties of lipid bilayers in the gel phase and alkanes in the solid phase. This behavior is explained by the concept of hindered vibrations which would now appear to apply to at least one integral membrane protein. There may also be a small broad transition centered near 20-25 degrees C that would correspond to the melting of less than 25 degrees of freedom per bacteriorhodopsin molecule and associated lipids. Using our measured apparent specific volume the average thickness of purple membrane is calculated to be 43.5 A. The specific volume of interaction of lipids and proteins is estimated, using the amino acid sequence of bacteriorhodopsin and average amino acid volumes from structural studies of other proteins, to be about 11% of the specific volume of the purple membrane lipids or 4% of the volume of the bacteriorhodopsin protein. A positive volume of interaction is consistent with lipid-protein interactions being an important determinant of the thermodynamic properties of purple membrane.     

Temperature transition of human hemoglobin at body temperature: effects of calcium

We studied the effects of calcium ion concentration on the temperature dependence of rheological behavior of human red blood cells (RBCs) and concentrated hemoglobin solutions. Our previous study (G. M. Artmann, C. Kelemen, D. Porst, G. Büldt, and S. Chien, 1998, Biophys. J., 75:3179-3183) showed a critical temperature (Tc) of 36.4 +/- 0.3 degrees C at which the RBCs underwent a transition from non-passage to passage through 1.3 microm micropipettes in response to an aspiration pressure of -2.3 kPa. An increase in intracellular Ca2+ concentration by using the ionophore A23187 reduced the passability of intact RBCs through small micropipettes above T(c); the micropipette diameter needed for >90% passage increased to 1.7 microm. Viscometry of concentrated hemoglobin solutions (45 and 50 g/dl) showed a sudden viscosity transition at 36 +/- 1 degrees C (Tc(eta)) at all calcium concentrations investigated. Below Tc(eta), the viscosity value of the concentrated hemoglobin solution at 1.8 mM Ca(2+) was higher than that at other concentrations (0.2 microM, 9 mM, and 18 mM). Above Tc(eta), the viscosity was almost Ca2+ independent. At 1.8 mM Ca2+ and 36 +/- 1 degrees C, the activation energy calculated from the viscometry data showed a strong dependence on the hemoglobin concentration. We propose that the transition of rheological behavior is attributable to a high-to-low viscosity transition mediated by a partial release of the hemoglobin-bound water.     

Thermal unfolding of myosin rod and light meromyosin: circular dichroism and tryptophan fluorescence studies

Rabbit skeletal myosin rod, which is the coiled-coil alpha-helical portion of myosin, contains two tryptophan residues located in the light meromyosin (LMM) portion whose fluorescence contributes 27% to the fluorescence of the entire myosin molecule. The temperature dependence of several fluorescence parameters (quantum yield, spectral position, polarization) of the rod and its LMM portion was compared to the thermal unfolding of the helix measured with circular dichroism. Rod unfolds with three major helix unfolding transitions: at 43, 47, and 53 degrees C, with the 43 and 53 degrees C transitions mainly located in the LMM region and the 47 degrees C transition mainly located in the subfragment 2 region. The fluorescence study showed that the 43 degrees C transition does not involve the tryptophan-containing region and that the 47 degrees C transition produces an intermediate with different fluorescence properties from both the completely helical and fully unfolded states. That is, although the fluorescence of the 47 degrees C intermediate is markedly quenched, the tryptophyl residues do not become appreciably exposed to solvent until the 53 degrees C transition. It is suggested that although the intermediate that is formed in the 47 degrees C transition contains an extensive region which is devoid of alpha-helix, the unfolded region is not appreciably solvated or flexible. It appears to have the properties of a collapsed nonhelical state rather than a classical random coil.