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Assessment of stability differences in the protein G B1 and B2 domains from hydrogen-deuterium exchange: comparison with calorimetric data.

Hydrogen-deuterium (H-D) exchange experiments have been used to measure exchange rates for almost all of the main-chain amide protons (NHs) in the B1 and B2 IgG-binding domains of protein G. For H-bonded NHs, exchange rates were also measured as a function of temperature from 25 to 65 degrees C for B1 and from 25 to 60 degrees C for B2. A number of NHs exchange by a mechanism consistent with global unfolding. For these residues, the free energy required for transient opening of a H-bonded NH (delta Gop) from H-D exchange approximates the extrapolated free energy of thermal unfolding (delta Gu) from calorimetry in B1 and B2. The difference in exchange rates between B1 and B2 for these residues reflects the 1 kcal mol-1 difference in stability from calorimetry. The more stable B1 domain appears to have a slightly larger core of residues which exchange by global unfolding than B2. The delta Gop values for slow exchange H-bonded NHs and calorimetric delta Gu provide highly complementary information on the delta G versus temperature stability profiles of B1 and B2. Furthermore, NH exchange rates provide a very sensitive measure of local stability differences between B1 and B2. In both domains, the beta 2-strand is the least stable of the beta-sheet although it is more stable in B1 than B2. The largest local stability differences occur at residues Y3 and T18 which exchange 40-fold and 100-fold slower in B1, respectively. These residues form a H-bond donor-acceptor pair at one end of the beta 1-beta 2 region. Local stability differences are also evident near the beta 1-beta 2 turn. These stability differences are, at least in part, due to subtle differences in hydrophobic packing effects. They are not obvious from inspection of the B1 and B2 structures but are manifested as readily measurable changes in NH exchange rates for individual residues. Knowledge of these local stability differences in the beta 1-beta 2 region provides potential approaches for designing new stability mutants in protein G. Most non-H-bonded NHs have exchange rates that are < 15 times slower than their intrinsic rates. In marked contrast, the NHs of K10, T11, and L12 in the beta 1-beta 2 turn and V21 have exchange rates which are five to > or = 24 times faster than their intrinsic rates, probably due to local electrostatic effects.(ABSTRACT TRUNCATED AT 400 WORDS)

Bacterial Proteins↗

Thermotropic phase behavior of mixtures of long chain fatty acid species of cerebroside sulfate with different fatty acid chain length species of phospholipid.

The thermotropic phase behavior of asymmetric, long fatty acid chain species of cerebroside sulfate, C24-CBS and C26-CBS, with symmetric species of phosphatidylcholine (PC) containing fatty acid chains of 14-18 carbons in length (diC14-PC, diC16-PC, diC18-PC) and dimyristoylphosphatidylethanolamine (diC14-PE) in 0.1 M KCl was studied by differential scanning calorimetry. Novel cerebroside sulfate (CBS) spin labels containing long chain C24 and C26 fatty acid spin labels with the nitroxide group on the twenty-second carbon were used to study the lipid organization of the gel phases of these mixtures. The phase diagrams of all the mixtures indicated the presence of two immiscible gel phases at low CBS concentrations. All except the C26-CBS/diC14-PC mixture had eutectic phase behavior at low CBS concentrations suggesting that the long fatty acid chain of the CBS species had a destabilizing effect on the gel phase of most of the phospholipids. The C26-CBS/diC14-PC mixture had peritectic phase behavior at low CBS concentrations indicating a stabilizing effect of the CBS C26 acyl chain on diC14-PC. These results are consistent with the relative compatibility of the CBS acyl chain length with the bilayer thickness of the PC; only in the case of the C26-CBS/diC14-PC mixture is the acyl chain of CBS long enough to span the PC bilayer. At intermediate to high CBS concentrations, the CBS and phospholipid (PL) were miscible with the exception of the C24-CBS/diC18-PC combination, which had eutectic phase behavior over a wide concentration range. Thus when the PL acyl chain length was similar to the sphingosine chain length of CBS, CBS bilayers could accommodate symmetric phospholipid molecules better than phospholipid bilayers could accommodate asymmetric molecules of CBS. Use of the spin labels indicated that, at low temperatures and at intermediate to high CBS concentrations, all of the mixtures were in a triple chain mixed interdigitated gel phase which immobilized the spin label. This gel phase slowly transformed over a wide temperature range to a double chain partially interdigitated gel phase in which the spin labels had much more motion. This transformation could be detected as a broad low enthalpy transition by differential scanning calorimetry. In all cases the presence of phospholipid destabilized the mixed interdigitated phase. Stabilization of the partially interdigitated bilayer by intermolecular hydrogen bonding interactions must outweigh the destabilizing forces caused by disruptions in packing and van der Waals interactions between CBS molecules resulting from insertion of molecules of phospholipid into this type of bilayer.(ABSTRACT TRUNCATED AT 400 WORDS)

Calorimetry, Differential Scanning↗

Thermodynamics of ligand-induced assembly of tubulin.

The equilibrium assembly of purified GDP-tubulin into microtubules induced by taxol and Taxotere has been studied as a function of solution variables, ligand, and nucleotide, in 10 mM sodium phosphate buffers. Assembly is coupled to the binding of one taxoid molecule per tubulin heterodimer, while binding to the unassembled protein is not detected within ligand solubility limits. Linked functions analysis has indicated that two Mg2+ and no more H+ ions are bound per tubulin-taxoid polymerized, and the heat capacity change is negligible within experimental error (determined by van't Hoff analysis and by differential scanning calorimetry), in contrast with drug-free control microtubule assembly and with the abnormal polymerization of the tubulin-colchicine complex. The apparent enthalpy change is ca. 240 kJ mol-1 (calorimetry), and the process is entropy driven. The apparent standard free energy change of taxoid-induced elongation at 2 mM free Mg2+, pH 6.1-6.7, and 37 degrees C is -29.5 +/- 0.4 (taxol) or -31.5 +/- 0.4 kJ mol-1 (Taxotere). This is independent of taxoid excess, which has indicated that the process measured corresponds to the elongation equilibrium of the fully liganded protein. Comparison to elongation in the absence of drug suggests an apparent linkage free energy change of binding and polymerization of -11.3 +/- 1.2 kJ mol-1. The taxoid-induced elongation of GTP-tubulin proceeds with an increment of apparent free energy change of -2.5 +/- 0.4 kJ mol-1 over GDP-tubulin. It is proposed that the taxoid binding changes the conformation of GDP-tubulin from inactive to active, allowing productive binding and elongation at the microtubule end. Among several possible model mechanisms discussed, it is particularly attractive to think of taxoids as double-sided ligands, which bind to tubulin at the microtubule end and participate in a lateral contact interface with the newly added tubulin molecule. In the kinetic pathway of assembly, these ligands should bind first to inactive Mg(2+)-induced linear GDP-tubulin oligomers and transform them into active bidimensional polymerization nuclei.

Antineoplastic Agents, Phytogenic↗

Thermodynamics of ribonuclease T1 denaturation.

Differential scanning calorimetry has been used to investigate the thermodynamics of denaturation of ribonuclease T1 as a function of pH over the pH range 2-10, and as a function of NaCl and MgCl2 concentration. At pH 7 in 30 mM PIPES buffer, the thermodynamic parameters are as follows: melting temperature, T1/2 = 48.9 +/- 0.1 degrees C; enthalpy change, delta H = 95.5 +/- 0.9 kcal mol-1; heat capacity change, delta Cp = 1.59 kcal mol-1 K-1; free energy change at 25 degrees C, delta G degrees (25 degrees C) = 5.6 kcal mol-1. Both T1/2 = 56.5 degrees C and delta H = 106.1 kcal mol-1 are maximal near pH 5. The conformational stability of ribonuclease T1 is increased by 3.0 kcal/mol in the presence of 0.6 M NaCl or 0.3 M MgCl2. This stabilization results mainly from the preferential binding of cations to the folded conformation of the protein. The estimates of the conformational stability of ribonuclease T1 from differential scanning calorimetry are shown to be in remarkably good agreement with estimates derived from an analysis of urea denaturation curves.

Calorimetry, Differential Scanning↗

Antigen binding thermodynamics and antiproliferative effects of chimeric and humanized anti-p185HER2 antibody Fab fragments.

The murine monoclonal antibody 4D5 (anti-p185HER2) inhibits the proliferation of human tumor cells overexpressing p185HER2 in vitro and has been "humanized" [Carter, P., Presta, L., Gorman, C. M., Ridgway, J. B. B., Henner, D., Wong, W.-L. T., Rowland, A. M., Kotts, C., Carver, M. E., & Shepard, H. M. (1992) Proc. Natl. Acad. Sci. U.S.A. (in press)] for use in human cancer therapy. We have determined the antigen binding thermodynamics and the antiproliferative activities of chimeric 4D5 Fab (ch4D5 Fab) fragment and a series of eight humanized Fab (hu4D5 Fab) fragments differing by amino acid substitutions in the framework regions of the variable domains. Fab fragments were expressed by secretion from Escherichia coli and purified from fermentation supernatants by using affinity chromatography on immobilized streptococcal protein G or staphylococcal protein A for ch4D5 and hu4D5, respectively. Circular dichroism spectroscopy indicates correct folding of the E. coli produced Fab, and scanning calorimetry shows a greater stability for hu4D5 (Tm = 82 degrees C) as compared with ch4D5 Fab (Tm = 72 degrees C). KD values for binding to the extracellular domain (ECD) of p185HER2 were determined by using a radioimmunoassay; the delta H and delta Cp for binding were determined by using isothermal titration calorimetry. ch4D5 Fab and one of the humanized variants (hu4D5-8 Fab) bind p185HER2-ECD with comparable affinity (delta G degrees = -13.6 kcal mol-1).(ABSTRACT TRUNCATED AT 250 WORDS)

Amino Acid Sequence↗

Peptide binding to lipid bilayers. Nonclassical hydrophobic effect and membrane-induced pK shifts.

The binding of the cyclic peptide (+)-D-Phe1-Cys2-Phe3-D-Trp4-(+)-Lys5-Thr6- Cys7-Thr(ol)8, a somatostatin analogue (SMS 201-995), and the potential-sensitive dye 2-(p-toluidinyl)naphthalene-6-sulfonate (TNS) to lipid membranes was investigated with high-sensitivity titration calorimetry. The binding enthalpy of the peptide was found to vary dramatically with the vesicle size. For highly curved vesicles with a diameter of d congruent to 30 nm, the binding reaction was enthalpy-driven with delta H congruent to -7.0 +/- 0.3 kcal/mol; for large vesicles with more tightly packed lipids, the binding reaction became endothermic with delta H congruent to +1.0 +/- 0.3 kcal/mol and was entropy-driven. In contrast, the free energy of binding was almost independent of the vesicle size. The thermodynamic analysis suggests that the observed enthalpy-entropy compensation of about 8 kcal/mol can be related to a change in the internal tension of the bilayer and is brought about by an entropy increase of the lipid matrix. The "entropy potential" of the membrane may have its molecular origin in the excitation of the hydrocarbon chains to a more disordered configuration and may play a more important role in membrane partition equilibria than the classical hydrophobic effect. The binding of the peptide to the membrane surface induced a pK shift of the peptide terminal amino group. Neutral membranes were found to destabilize the NH3+ group, leading to a decrease in pK; negatively charged membranes, generated an apparent increase in pK due to the increase in proton concentration near the membrane surface. No pK shifts were seen for TNS. Titration calorimetry combined with the Gouy-Chapman theory can be used to determine both the reaction enthalpy and the binding constant of the membrane-binding equilibrium.

Amino Acid Sequence↗

Energetic characterization of the basic fibroblast growth factor-heparin interaction: identification of the heparin binding domain.

Fibroblast growth factors (FGF's) interact on cell surfaces with "low-affinity" heparan sulfate proteoglycans (HSPG) and "high-affinity" FGF receptors (FGFR) to initiate cell proliferation. Previous reports have implicated the binding of heparin, or heparan sulfate, to FGF as essential for FGF-mediated signal transduction and mitogenicity. However, the molecular recognition events which dictate the specificity of this interaction have remained elusive. Amino acid residues on the surface of basic FGF (bFGF) were targeted as potential heparin contacts on the basis of the position of sulfate anions in the X-ray crystal structure of bFGF and of a modeled pentasaccharide heparin-bFGF complex. Each identified amino acid was replaced individually with alanine by site-directed mutagenesis, and the resulting mutant proteins were characterized for differences in binding to a low molecular weight heparin (approximately 3000) by isothermal titrating calorimetry and also for differences in [NaCl] elution from a heparin-Sepharose affinity resin. The combination of site-directed mutagenesis and titrating calorimetry permitted an analysis of the energetic contributions of individual bFGF residues in the binding of heparin to bFGF. The key amino acids which comprise the heparin binding domain on bFGF constitute a discontinuous binding epitope and include K26, N27, R81, K119, R120, T121, Q123, K125, K129, Q134, and K135. Addition of the observed delta delta G degrees of binding for each single site mutant accounts for 8.56 kcal/mol (> 95%) of the free energy of binding. The delta delta G degrees values for N27A, R120A, K125A, and Q134A are all greater than 1 kcal/mol each, and these four amino acids together contribute 4.8 kcal/mol (56%) to the total binding free energy. Amino acid residues K119 through K135 reside in the C-terminal domain of bFGF and collectively contribute 6.6 kcal/mol (76%) of the binding free energy. Although 7 out of the 11 identified amino acids in the heparin binding domain are positively charged, a 7-fold increase in [NaCl] decreases the affinity of wild-type bFGF binding to heparin only 37-fold (Kd at 0.1 M NaCl = 470 nM vs Kd at 0.7 M NaCl = 17.2 microM). This indicates that pure electrostatic interactions contribute only 30% of the binding free energy as analyzed by polyelectrolyte theory and that more specific nonionic interactions, such as hydrogen bonding and van der Waals packing, contribute the majority of the free energy for this binding reaction.

Binding Sites↗

Alzheimer beta-amyloid peptide 25-35: electrostatic interactions with phospholipid membranes.

The role of lipids in the aggregation of three Alzheimer model peptides was investigated with circular dichroism spectroscopy and high-sensitivity titration calorimetry under conditions of low ionic strength. In solution, the peptides beta AP(25-35)OH and beta AP(25-35Nle)NH2 exhibit a reversible random-coil<-->beta-sheet (or beta-structured aggregate) transition. Addition of lipid vesicles containing negatively charged lipids shifts the random-coil<-->beta-sheet equilibrium almost completely toward beta-sheet structure, which can be explained by the specific conditions created at the membrane surface: the cationic peptides are attracted to the negatively charged membrane, and the increase in peptide concentration together with the partial alignment of the peptide molecules then facilitates beta-sheet formation. The third peptide, beta AP-(25-35)NH2, also binds to the lipid membrane but was found to adopt an essentially random-coil structure, both with and without lipids. A quantitative characterization of the binding equilibrium was possible with high-sensitivity titration calorimetry. All three peptides exhibited exothermic binding enthalpies which varied between delta H approximately -2 kcal/mol for beta AP(25-35)OH and -8 kcal/mol for beta AP(25-35)NH2. The apparent binding constants, calculated with bulk concentrations, were large and varied between 500 and 5 x 10(4) M-1, depending on the experimental conditions. However, after correction for electrostatic charge effects using the Gouy-Chapman theory, the intrinsic binding constants were found to be constant and much smaller with K approximately 2-10 M-1.(ABSTRACT TRUNCATED AT 250 WORDS)

Alzheimer Disease↗

Kinetic study on the irreversible thermal denaturation of yeast phosphoglycerate kinase.

Differential scanning calorimetry transitions for the irreversible thermal denaturation of yeast phosphoglycerate kinase at pH 7.0 are strongly scanning-rate dependent, suggesting that the denaturation is, at least in part, under kinetic control. To test this possibility, we have carried out a kinetic study on the thermal inactivation of the enzyme. The inactivation kinetics are comparatively fast within the temperature range of the calorimetric transitions and can be described phenomenologically by the equation dC/dt = -alpha C2/(beta + C), where C is the concentration of active enzyme at a given time, t, and alpha and beta are rate coefficients that depend on temperature. This equation, together with the values of alpha and beta (within the temperature range 50-59 degrees C) have allowed us to calculate the fraction of irreversibly denatured protein versus temperature profiles corresponding to the calorimetric experiments. We have found that (a) irreversible denaturation takes place during the time the protein spends in the transition region and (b) there is an excellent correlation between the temperatures of the maximum of the calorimetric transitions (Tm) and the temperatures (Th) at which half of the protein is irreversibly denatured. These results show that the differential scanning calorimetry transitions for the denaturation of phosphoglycerate kinase are highly distorted by the rate-limited irreversible process. Finally, some comments are made as to the use of equilibrium thermodynamics in the analysis of irreversible protein denaturation.

Calorimetry, Differential Scanning↗

Diacetylenic lipid microstructures: structural characterization by X-ray diffraction and comparison with the saturated phosphatidylcholine analogue.

Thermotropic and lyotropic mesomorphism in the polymerizable lecithin 1,2-ditricosa-10,12-diynoyl-sn-glycero-3-phosphocholine and its saturated analogue, 1,2-ditricosanoyl-sn-glycero-3-phosphocholine, has been investigated by wide- and low-angle X-ray diffraction of both powder and oriented samples and by differential scanning calorimetry. Previous studies have shown that the hydrated diacetylenic lipid forms novel microstructures (tubules and stacked bilayer sheets) in its low-temperature phase. The diffraction results indicate that at low temperatures fully hydrated tubules and sheets have an identical lamellar repeat size (d001 = 66.4 A) and crystalline-like packing of the acyl chains. Chain packing in the lamellar crystalline phase is hydration independent. A model for the polymerizable lecithin with (1) fully extended all-trans methylene segments, (2) a long-axis tilt of 32 degrees, and (3) minimal chain interdigitation seems most reasonable on energetic grounds, is consistent with the diffraction data (to 3.93-A resolution), and is likely to support facile polymerization. Above the chain "melting" transition the lamellar repeat of the polymerizable lipid increases to 74 A. The conformational similarity between tubules, sheets, and the dry powder is corroborated by calorimetry, which reveals a cooling exotherm at the same temperature where tubules form upon cooling hydrated sheets. The data suggest that although a high degree of conformational order is a pertinent feature of tubules, this character alone is not sufficient to account for tubule formation. The conformation of the corresponding saturated phosphatidylcholine appears to be similar to that of other saturated phosphatidylcholines in the lamellar gel phase. Furthermore, above the main transition temperature, the dry, saturated lipid shows evidence of a P delta phase (112 degrees C), whereas the diacetylenic lipid appears to exhibit a centered rectangular phase, R alpha (55 degrees C).

1,2-Dipalmitoylphosphatidylcholine↗

The vnd/NK-2 homeodomain: thermodynamics of reversible unfolding and DNA binding for wild-type and with residue replacements H52R and H52R/T56W in helix III.

The conformational stabilities of the vnd (ventral nervous system defective)/NK-2 homeodomain [HD(wt); residues 1-80 that encompass the 60-residue homeodomain] and those harboring mutations in helix III of the DNA recognition site [HD(H52R) and HD(H52R/T56W)] have been investigated by differential scanning calorimetry (DSC) and ellipticity changes at 222 nm. Thermal unfolding reactions at pH 7.4 are reversible and repeatable in the presence of 50-500 mM NaCl with DeltaC(p) = 0.52 +/- 0.04 kcal K(-1) mol(-1). A substantial stabilization of HD(wt) is produced by 50 mM phosphate or by the addition of 100-500 mM NaCl to 50 mM Hepes, pH 7.4, buffer (from T(m) = 35.5 degrees C to T(m) 43-51 degrees C; DeltaH(vH) congruent with 47 +/- 5 kcal mol(-1)). The order of stability is HD(H52R/T56W) > HD(H52R) > HD(wt), irrespective of the anions present. Progress curves for ellipticity changes at 222 nm as a function of increasing temperature are fitted well by a two-state unfolding model, and the cooperativity of secondary structure changes is greater for mutant homeodomains than for HD(wt) and also is increased by adding 100 mM NaCl to Hepes buffer. A 33% quench of the intrinsic tryptophanyl residue fluorescence of HD(wt) by phosphate binding (K(D)' = 2.6 +/- 0.3 mM phosphate) is reversed approximately 60% by DNA binding. Thermodynamic parameters for vnd/NK-2 homeodomain proteins binding sequence-specific 18 bp DNA have been determined by isothermal titration calorimetry (10-30 degrees C). Values of DeltaC(p) are +0.25, -0.17, and -0.10 +/- 0.04 kcal K(-1) mol(-1) for HD(wt), HD(H52R), and HD(H52R/T56W) binding duplex DNA, respectively. Interactions of homeodomains with DNA are enthalpically controlled at 298 K and pH 7.4 with corresponding DeltaH values of -6.6 +/- 0.5, -10.8 +/- 0.1, and -9.0 +/- 0.6 kcal mol(-1) and DeltaG' values of -11.0 +/- 0.1, -11.0 +/- 0.1, and -11.3 +/- 0.3 kcal mol(-1) with a binding stoichiometry of 1.0 +/- 0.1. Thermodynamic parameters for DNA binding are not predicted from homeodomain structural changes that occur upon complexing to DNA and must reflect also solvent and possibly DNA rearrangements.

Amino Acid Substitution↗

Thermodynamic identification of stable folding intermediates in the B-subunit of cholera toxin.

The structural stability and domain structure of the pentameric B-subunit of cholera toxin have been measured as a function of different perturbants in order to assess the magnitude of the interactions within the B-subunits. For these studies, temperature, guanidine hydrochloride (GuHCl), and pH were used as perturbants, and the effects were measured by high-sensitivity differential scanning calorimetry, isothermal reaction calorimetry, fluorescence spectroscopy, and partial protease digestion. At pH 7.5 and in the absence of any additional perturbants, the thermal unfolding of the B-subunit pentamer is characterized by a single peak in the heat capacity function centered at 77 degrees C and characterized by a delta Hcal of 328 kcal/mol of B-subunit pentamer and delta Hvh/delta Hcal of 0.3. Lowering the pH down to 4 or adding GuHCl up to 2 M results in a decrease of the calorimetric enthalpy with no significant effect on the van't Hoff enthalpy. The transition enthalpy decreases in a sigmoidal fashion with pH, with an inflection point centered at pH 5.3. Isothermal titration calorimetric studies as a function of pH also report a transition centered at pH 5.3 and characterized by an enthalpy change of 27 kcal/mol of B-subunit pentamer at 27 degrees C. Below this pH, the enthalpy change for the unfolding transition is reduced to approximately 100 kcal/mol of B-subunit pentamer. Similar behavior is obtained with GuHCl. In this case, a first transition is observed at 0.5 M GuHCl and a second one at 3 M GuHCl.(ABSTRACT TRUNCATED AT 250 WORDS)

Calorimetry, Differential Scanning↗

Equilibrium analysis of ethidium binding to DNA containing base mismatches and branches.

In the processes of DNA replication, recombination, and repair, duplex DNA can transiently form branched structures, such as Holliday junctions, as well as base pair mismatches and bulges. These stages have altered ligand and protein binding properties from normal double helical DNA. A variety of ligands have been reported to interact more tightly at branches and bulges than to normal duplex sites. The stoichiometry, structural basis, and thermodynamics of this effect have not been determined. We have investigated the binding of the intercalator, ethidium bromide, to several DNA constructs including base mismatches, bulges, and three- and four-arm branched structures, using chemical footprinting, titration calorimetry, and fluorescence lifetime measurements. Two classes of binding sites are detected in three- and four-arm junctions in our high ionic strength conditions: one class is characterized by a small number of ligands (2-4 per DNA), with high binding affinity (K > 10(5)), and the second by a larger number of sites (10-12 per DNA) with lower affinity (K approximately 10(4)). By use of appropriate control experiments, the former appear to be associated with sites at or near the branch point or mismatch, while the latter are consistent with binding to the normal duplex DNA region(s) of the molecule. Titration calorimetry indicates an enthalpy of -10 to -13 kcal/mol for binding of ethidium to a mismatch or three- and four-arm branch point. The tight binding class is associated with a fluorescence lifetime of 12-16 ns, distinct from that of free ethidium (ca. 2 ns) and the longer lifetime observed for ethidium intercalated in duplex DNA (22-26 ns).

Base Composition↗

Order-disorder phase transition and lipid dynamics in rabbit small intestinal brush border membranes. Effect of proteins.

The total lipids extracted from brush border membranes form smectic lamellar phases when dispersed in water. 31P broad-band nuclear magnetic resonance (NMR) shows that between body temperature (37 degrees C) and freezing of the solvent, the extracted lipids form bilayers with the lipid molecules undergoing fast anisotropic motion. This is also true for the lipids present in the brush border membrane. The electron spin resonance (ESR) results obtained with various hydrophobic spin probes incorporated in either brush border vesicle membranes or their extracted lipids are consistent with this interpretation. By use of a variety of chemically different spin-labels, the temperature dependence of brush border membranes and their extracted lipids was probed. The temperature dependence of various ESR spectral parameters shows discontinuities that, by comparison with differential scanning calorimetry, are assigned to a lipid thermotropic phase transition. Differential scanning calorimetry shows that the lipid in brush border membranes undergoes a broad, reversible phase transition of low enthalpy between 10 and 30 degrees C, with a peak temperature of about 25 degrees C. Hence, the brush border membrane of rabbit small intestine functions in the liquid-crystalline state, well above the peak temperature and also above the upper limit of the lipid phase transition. Therefore, in itself, the thermotropic lipid phase transition is unlikely to play a physiological role. The low enthalpy of the lipid phase transition, indicative of a lack of cooperativity, is primarily attributed to the relatively high cholesterol content and to heterogeneity in the lipid composition of this membrane [Hauser, H., Howell, K., Dawson, R. M. C., & Bowyer, D. E. (1980) Biochim. Biophys. Acta 602, 567-577].(ABSTRACT TRUNCATED AT 250 WORDS)

Animals↗

X-ray diffraction study of the polymorphism of hydrated diacyl- and dialkylphosphatidylethanolamines.

The structure and polymorphism of a homologous series of diacyl- and of dialkylphosphatidylethanolamines have been investigated by X-ray diffraction, calorimetry, and density measurement. The compositional dependence of the repeat spacings of the gel (L beta or L beta'), fluid bilayer (L alpha), and inverted hexagonal (HII) phases has been determined both for the short chain length (di-C12) dialkyl didodecylphosphatidylethanolamine (DDPE) and for the long chain length (di-C20) diacyl diarachinoylphosphatidylethanolamine (DAPE). These data, in conjunction with the measured phase transition temperatures obtained both by X-ray diffraction and by differential scanning calorimetry, have been used to construct phase diagrams for the two lipids. DDPE exhibits metastable behavior in the L beta and L alpha phases below 44 degrees C at all water contents and forms cubic and other nonlamellar phases between the L alpha and HII phases. At low water contents, crystalline and fluid phases coexist at temperatures up to 83 degrees C. For DAPE, the behavior is simpler. In the gel phase, the hydrocarbon chains are tilted at 29 degrees to the bilayer normal, and metastability is only observed at water contents below 3 wt %. The L alpha phase is adopted within a narrow temperature range and then transforms directly to the HII phase. The structural parameters of the L beta (L beta'), L alpha, and HII phases of DDPE and DAPE have been calculated from the X-ray data, in conjunction with the measured values of lipid partial specific volume. In addition, the chain-length dependence of the repeat spacings of the phases has been measured for the homologous series of diacyl and dialkyl lipids. Taken together, the results allow a detailed description of the effects of temperature, hydration, and chain length on the polymorphism of the saturated phosphatidylethanolamines.

Calorimetry↗

Protein and lipid structural transitions in cytochrome c oxidase-dimyristoylphosphatidylcholine reconstitutions.

The thermotropic behavior of the mitochondrial enzyme cytochrome c oxidase (EC 1.9.3.1) reconstituted in dimyristoylphosphatidylcholine (DMPC) vesicles has been studied by using high-sensitivity differential scanning calorimetry and fluorescence spectroscopy. The incorporation of cytochrome c oxidase into the phospholipid bilayer perturbs the thermodynamic parameters associated with the lipid phase transition in a manner analogous to other integral membrane proteins: it reduces the enthalpy change, lowers the transition temperature, and reduces the cooperative behavior of the phospholipid molecules. Analysis of the dependence of the enthalpy change on the protein:lipid molar ratio indicates that cytochrome c oxidase prevents 99 +/- 5 lipid molecules from participating in the main gel-liquid-crystalline transition. These phospholipid molecules presumably remain in the same physical state below and above the transition temperature of the bulk lipid, thus providing a more or less constant microenvironment to the protein molecule. The effect of the phospholipid bilayer matrix on the thermodynamic stability of the cytochrome c oxidase complex was examined by high-sensitivity differential scanning calorimetry. Detergent (Tween 80)-solubilized cytochrome c oxidase undergoes a complex, irreversible thermal denaturation process centered at 56 degrees C and characterized by an enthalpy change of 550 +/- 50 kcal/mol of enzyme complex. Reconstitution of the cytochrome c oxidase complex into DMPC vesicles shifts the transition temperature upward to 63 degrees C, indicating that the phospholipid bilayer moiety stabilizes the native conformation of the enzyme. The lipid bilayer environment contributes approximately 10 kcal/mol to the free energy of stabilization of the enzyme complex. The thermal unfolding of cytochrome c oxidase is not a two-state process.(ABSTRACT TRUNCATED AT 250 WORDS)

Animals↗

Direct measurement of the energetics of association between myelin basic protein and phosphatidylserine vesicles.

A newly designed high-sensitivity isothermal reaction calorimetry system has been used to investigate the thermodynamics of the association between myelin basic protein and phosphatidylserine vesicles. This instrument has allowed us to measure directly the energetics of the protein-lipid interaction under various conditions. Above the phospholipid phase transition temperature the enthalpy of association is highly exothermic amounting to -160 kcal/mol of protein. Below the phospholipid phase transition temperature the enthalpy of association is exothermic at protein/lipid ratios smaller than 1/50 and endothermic at higher protein/lipid ratios. These studies indicate that the association of myelin basic protein to phosphatidylserine vesicles consists of at least two stages involving different types of binding. The first stage, at low protein/lipid ratios, involves a strong exothermic association of the protein to the membrane and the second, at high protein/lipid ratios, a weaker association probably involving attachment of the protein to the membrane surface only. In the gel phase the second binding stage is endothermic and appears to be correlated with the formation of large vesicle aggregates. This vesicle aggregation is a reversible process dependent upon the physical state of the membrane. The isothermal titration studies have been complemented with high-sensitivity differential scanning calorimetry experiments. It is shown that the dependence of the phospholipid transition enthalpy on the protein/lipid molar ratio can be expressed in terms of the different protein-membrane association enthalpies in the gel and fluid phases of the membrane.

Animals↗

Thermodynamic study of yeast phosphoglycerate kinase.

Enthalpies of binding of MgADP, MgATP, and 3-phosphoglycerate to yeast phosphoglycerate kinase have been determined by flow calorimetry at 9.95-32.00 degrees C. Combination of these data with published dissociation constants [Scopes, R.K. (1978) Eur. J. Biochem. 91, 119-129] yielded the following thermodynamic parameters for the binding of 3-phosphoglycerate at 25 degrees C: delta Go = -6.76 +/- 0.11 kcal mol-1, delta H = 3.74 +/- 0.08 kcal mol-1, delta So = 35.2 +/- 0.6 cal K-1 mol-1, and delta Cp = 0.12 +/- 0.32 kcal K-1 mol-1. The thermal unfolding of phosphoglycerate kinase in the absence and presence of the ligands listed above was studied by differential scanning calorimetry. The temperature of half-completion, t 1/2, of the denaturation and the denaturational enthalpy are increased by the binding of the ligands, the increase in t 1/2 being a manifestation of Le Chatelier's principle and that in enthalpy reflecting the enthalpy of dissociation of the ligand. Only one denaturational peak was observed under all conditions, and in contrast with the case of yeast hexokinase [Takahashi, K., Casey, J.L., & Sturtevant, J.M. (1981) Biochemistry 20, 4693-4697], no definitive evidence for the unfolding of more than one domain was obtained.

Calorimetry, Differential Scanning↗