Ionic volumes in solution

The volumetric properties of electrolytes in solutions indicate the interactions of the constituent ions with their environment: the solvent and other ions. The interactions with the solvent alone are manifested at infinite dilution by the standard partial molar volume, V(infinity)(salt), obtained from density measurements. To study the interactions, it is necessary to split V(infinity)(salt) into the additive ionic contributions, V(infinity)(ion), using an extra-thermodynamic assumption. Values of V(infinity)(ion) for small ions depend cardinally on the electrostriction of the solvent that can be obtained from an iterative shell-by-shell calculation from a continuum model of the solvent. The solvent shrinkage per mol of ions is DeltaV(el)(ion)<0. Also, the molar electrostriction of the solvent S, DeltaV(el)(S)<0, is calculable. The ratio DeltaV(el)(ion)/DeltaV(el)(S)=n(infinity) is the solvation number of the ion in S at infinite dilution. The calculated V(infinity)(ion)(calc) are compared with the experimental values, showing good agreement for many univalent ions in both single solvents and in some binary solvent mixtures, where no appreciable preferential solvation takes place. Ion pairing sets in under certain circumstances of ionic charge and solvent permittivity. The difference DeltaV(ip)=V(ip)(infinity)-[V(infinity)(+)+V(infinity)(-)]>0 is obtained experimentally from the pressure derivative of the association constant. The ratio Deltan(ip)=DeltaV(ip)/DeltaV(el)(S) represents the number of solvent molecules released to the bulk on ion pairing by the diminution of the electrostriction.     

Oxidation-state-dependent protein docking between cytochrome c and cytochrome b(5): high-pressure laser flash photolysis study

To characterize the protein-protein interaction during electron transfer, we used Zn-substituted cytochrome c (ZnCytc) as a model of ferrous Cytc and determined the volume change, DeltaV(d)(Zn), for the dissociation of its complex with ferric cytochrome b(5) (Cytb(5)) by the pressure dependence of its photoinduced electron-transfer kinetics. Under ambient pressure, the dissociation constant, K(d)(Zn), of the ZnCytc/Cytb(5) complex was dependent on the buffer concentration, 1.5 and 12 microM in 2 and 10 mM Tris-HCl, pH 7.4, respectively, which was consistent with formation of salt bridges in its complexation. The dissociation of one salt bridge is usually associated with large volume changes of -10 to -30 cm(3) mol(-1), while pressure dependence of K(d)(Zn) resulted in smaller value of DeltaV(d)(Zn), -8.5 cm(3) mol(-1). Therefore, the interaction between ZnCytc and Cytb(5) cannot be explained only by salt bridge interaction, and the partial cancellation by the positive volume change due to the additional hydrophobic interaction is a plausible explanation for the observed DeltaV(d)(Zn). In addition, DeltaV(d)(Zn) of -8.5 cm(3) mol(-1) was considerably smaller than the previously reported volume change, DeltaV(d)(Fe), of -122 cm(3) mol(-1) in the ferric Cytc/Cytb(5) complex dissociation [Rodgers and Sligar (1991) J. Mol. Biol. 221, 1453-1460]. ZnCytc used here has been assumed to be a reliable model of ferrous Cytc, and thus the discrepancy between our present DeltaV(d)(Zn) and the previous DeltaV(d)(Fe) is discussed on the basis of the protein docking dependent on the oxidation states of heme iron in Cytc.     

Hindlimb unweighting affects rat vascular capacitance function

Microgravity is associated with an impaired stroke volume and, therefore, cardiac output response to orthostatic stress. We hypothesized that a decreased venous filling pressure due to increased venous compliance may be an important contributing factor in this response. We used a constant flow, constant right atrial pressure cardiopulmonary bypass procedure to measure total systemic vascular compliance (C(T)), arterial compliance (C(A)), and venous compliance (C(V)) in seven control and seven 21-day hindlimb unweighted (HLU) rats. These compliance values were calculated under baseline conditions and during an infusion of 0.2 microg*kg(-1)*min(-1) norepinephrine (NE). The change in reservoir volume, which reflects changes in unstressed vascular volume (DeltaV(0)) that occurred upon infusion of NE, was also measured. C(T) and C(V) were larger in HLU rats both at baseline and during the NE infusion (P < 0.05). Infusion of NE decreased C(T) and C(V) by ~20% in both HLU and control rats (P < 0.01). C(A) was also significantly decreased in both groups of rats by NE (P < 0.01), but values of C(A) were similar between HLU and control rats both at baseline and during the NE infusion. Additionally, the NE-induced DeltaV(0) was attenuated by 53% in HLU rats compared with control rats (P < 0.05). The larger C(V) and attenuated DeltaV(0) in HLU rats could contribute to a decreased filling pressure during orthostasis and thus may partially underlie the mechanism leading to the exaggerated fall in stroke volume and cardiac output seen in astronauts during an orthostatic stress after exposure to microgravity.     

Application of pressure perturbation calorimetry to lipid bilayers

Pressure perturbation calorimetry (PPC) is a new method that measures the heat consumed or released by a sample after a sudden pressure jump. The heat change can be used to derive the thermal volume expansion coefficient, alpha(V), as a function of temperature and, in the case of phase transitions, the volume change, DeltaV, occurring at the phase transition. Here we present the first report on the application of PPC to determine these quantities for lipid bilayers. We measure the volume changes of the pretransition and main transition of 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC), and the thermal expansivity of the fluid phase of DMPC and of two unsaturated lipids, 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine and 1,2-dioleoyl-sn-glycero-3-phosphocholine. The high sensitivity of PPC instrumentation gives accurate data for alpha(V) and DeltaV even upon the application of relatively low pressures of approximately 5 bar.     

Nonlinear changes of transmembrane potential caused by defibrillation shocks in strands of cultured myocytes

Organization of cardiac tissue into cell strands and layers has been implicated in changes of transmembrane potential (DeltaV(m)) during defibrillation. To determine the shock-induced DeltaV(m) in such structures, cell strands of variable width [strand width (SW) = 0.15-2 mm] were grown in culture. Uniform-field shocks with variable strength [shock strength (SS) = 2-50 V/cm] were applied across strands during the action potential (AP) plateau, and DeltaV(m) were measured optically. Three different types of DeltaV(m) were observed. Small DeltaV(m) [<40%AP amplitude (APA)] were linearly dependent on SS and SW and were symmetrically distributed about a strand centerline with maximal positive and negative DeltaV(m) on opposite strand sides being equal. Intermediate DeltaV(m) (<200%APA) were strongly asymmetric with negative DeltaV(m) > positive DeltaV(m) because of a negative time-dependent shift of V(m) at the depolarized side of the strands. For large DeltaV(m) (>200%APA), a second time-dependent shift of V(m) to more positive levels was observed in the hyperpolarized portions of strands, causing reduction of the DeltaV(m) asymmetry. We conclude that during application of shocks to cell strands during the AP plateau, passive changes of V(m) were followed by two voltage- and time-dependent shifts of V(m), possibly reflecting changes of ionic currents or membrane electroporation.     

Partial phase diagram of aqueous bovine carbonic anhydrase: analyses of the pressure-dependent temperatures of the low- to physiological-temperature nondenaturational conformational change and of unfolding to the molten globule state

At 1.0 atm pressure and in 150 mM sodium phosphate (pH = 7.0), bovine carbonic anhydrase undergoes a nondenaturational conformational change at 30.3 degrees C and an unfolding transition from the physiological conformer to the molten globule state at 67.4 degrees C. The pressure dependences of the temperatures of these transitions have been studied under reversible conditions for the purpose of understanding DeltaH degrees , DeltaS degrees , and DeltaV for each conformational change. Temperatures for the low-temperature to physiological-temperature conformational change T(L-->P) are obtained from physiologically relevant conditions using slow-scan-rate differential scanning calorimetry. Temperatures for the physiological-temperature conformation to molten globule state conversion T(P-->MG) are obtained from differential scanning calorimetry measurements of the apparent transition temperature in the presence of guanidine hydrochloride extrapolated to zero molar denaturant. The use of slow-scan-rate differential scanning calorimetry permits the calculation of the activation volume for the conversion of the low-temperature conformer to the physiological-temperature conformer DeltaV(double dagger)(L-->P). At 1.0 atm pressure, the transition from the low-temperature conformer to the physiological-temperature conformer involves a volume change DeltaV(L-->P) = 15 +/- 2 L/mole, which contrasts with the partial unfolding of the physiological-temperature conformer to the molten globule state (DeltaV(P-->MG) = 26 +/- 9 L/mole). The activation volume for this process DeltaV(double dagger)(L-->P) = 51 +/- 9 L/mole and is consistent with a prior thermodynamic analysis that suggests the conformational transition from the low-temperature conformation to the physiological-temperature conformation possesses a substantial unfolding quality. These results provide further evidence the structure of the enzyme obtained from crystals grown below 30 degrees C should not be regarded as the physiological structure (the normal bovine body temperature is 38.3 degrees C). These results should therefore have implications in any area that seeks to correlate the crystal structure of bovine carbonic anhydrase to physiological function.     

The thermodynamic analysis of protein stabilization by sucrose and glycerol against pressure-induced unfolding.

We have studied the reaction native left arrow over right arrow denatured for the 33-kDa protein isolated from photosystem II. Sucrose and glycerol have profound effects on pressure-induced unfolding. The additives shift the equilibrium to the left; they also cause a significant decrease in the standard volume change (DeltaV). The change in DeltaV was related to the sucrose and glycerol concentrations. The decrease in DeltaV varied with the additive: sucrose caused the largest effect, glycerol the smallest. The theoretical shift of the half-unfolding pressure (P1/2) calculated from the net increase in free energy by addition of sucrose and glycerol was lower than that obtained from experimental mea- surements. This indicates that the free energy change caused by preferential hydration of the protein is not the unique factor involved in the protein stabilization. The reduction in DeltaV showed a large contribution to the theoretical P1/2 shift, suggesting that the DeltaV change, caused by the sucrose or glycerol was associated with the protein stabilization. The origin of the DeltaV change is discussed. The rate of pressure-induced unfolding in the presence of sucrose or glycerol was slower than the refolding rate although both were significantly slower than that observed without any stabilizers.     

Effects of pressure on the kinetics of capture by yeast alcohol dehydrogenase.

High pressure causes biphasic effects on the oxidation of benzyl alcohol by yeast alcohol dehydrogenase as expressed in the kinetic parameter V/K which measures substrate capture. Moderate pressure increases the rate of capture of benzyl alcohol by activating the hydride transfer step. This means that the transition state for hydride transfer has a smaller volume than the free alcohol plus the capturing form of enzyme, with a DeltaV of -39 +/- 1 mL/mol, a value that is relatively large. This is the first physical property of an enzymatic transition state thus characterized, and it offers new possibilities for structure-activity analyses. Pressures of >1.5 kbar decrease the rate of capture of benzyl alcohol by favoring a conformation of the enzyme which binds nicotinamide adenine dinucleotide (NAD+) less tightly. This means that the ground state for tight binding, E-NAD+, has a larger volume than the collision complex, E-NAD+, with a DeltaV of 73 +/- 2 mL/mol. The equilibrium constant of the conformational change Keq is 75 +/- 13 at 1 atm. The effects of pressure on the capture of NAD+ have no activation phase because the conformational change is now being expressed kinetically instead of thermodynamically, together with but in opposition to hydride transfer, causing the effects to cancel. For yeast alcohol dehydrogenase, this conformational change had not been detected previously, but similar conformational changes have been found by spectroscopic means in other dehydrogenases, and some of them are also sensitive to pressure. The opposite signs for the volume change of tighter binding and hydride transfer run contrary to Pauling's hypothesis that substrates are bound more tightly in the transition state than in the Michaelian reactant state.     

Packing properties of 1-alkanols and alkanes in a phospholipid membrane

We have used vibrating tube densitometry to investigate the packing properties of four alkanes and a homologous series of ten alcohols in fluid-phase membranes of dimyristoyl phosphatidylcholine (DMPC). It was found that the volume change of transferring these compounds from their pure states into the membrane, DeltaV(m)(pure-->mem), was positive for small (C4-C6) 1-alkanols while it was negative for larger alcohols and all alkanes. The magnitude of DeltaV(m)(pure-->mem) ranged from about +4 cm3/mol for alcohols with an alkyl chain about half the length of the fatty acids of DMPC, to -10 to -15 cm3/mol for the alkanes and long chain alcohols. On the basis of these observations, previously published information on the structure of the membrane-solute complexes and the free volume properties of (pure) phospholipid membranes, we suggest that two effects dominate the packing properties of hydrophobic solutes in DMPC. First, perturbation of the tightly packed interfacial zone around the ester bonds and first few methylene groups of DMPC brings about a positive contribution to DeltaV(m)(pure-->mem). This effect dominates the volume behavior for alcohols like 1-butanol, 1-pentanol and 1-hexanol. More hydrophobic solutes penetrate into the membrane core, which is loosely packed. In this region, they partially occupy interstitial (or free-) volume, which bring about a denser molecular packing and generate a negative contribution to DeltaV(m)(pure-->mem).     

High-pressure refolding of bikunin: efficacy and thermodynamics

Bikunin is a glycosylated protein that aggregates extensively during mammalian cell culture, resulting in loss of activity, loss of native secondary structure, and the formation of nonnative disulfide bonds. We investigated the use of high hydrostatic pressure (1000-3000 bar) for the refolding of bikunin aggregates. The refolding yield obtained with pressure-modulated refolding at 2000 bar was 70 (+/-5%) by reverse-phase chromatography (RP-HPLC), significantly higher than the value of 55 (+/-6%) (RP-HPLC) obtained with traditional guanidine HCl "dilution-refolding." In addition, we determined the thermodynamics of pressure-modulated refolding. The change in volume for the transition of aggregate to monomer DeltaV(refolding) was calculated to be -28 (+/-5) mL/mole. Refolding was accompanied by a loss of hydrophobic exposure, resulting in a positive contribution to the DeltaV(refolding). These findings suggest that the disruption of electro-static interactions or the differences in size of solvent-free cavities between the aggregate and the monomer are the prevailing contributions to the negative DeltaV(refolding).     

Recording of blue light-induced energy and volume changes within the wild-type and mutated phot-LOV1 domain from Chlamydomonas reinhardtii

The time-resolved thermodynamics of the flavin mononucleotide (FMN)-binding LOV1 domain of Chlamydomonas reinhardtii phot (phototropin homolog) was studied by means of laser-induced optoacoustic spectroscopy. In the wild-type protein the early red-shifted intermediate LOV(715) exhibits a small volume contraction, DeltaV(715) = -1.50 ml/mol, with respect to the parent state. LOV(715) decays within few micro s into the covalent FMN-Cys-57 adduct LOV(390), that shows a larger contraction, DeltaV(390) = -8.8 ml/mol, suggesting a loss of entropy and conformational flexibility. The high energy content of LOV(390), E(390) = 180 kJ/mol, ensures the driving force for the completion of the photocycle and points to a strained photoreceptor conformation. In the LOV-C57S mutated protein the photoadduct is not formed and DeltaV(390) is undetected. Large effects on the measured DeltaVs are observed in the photochemically competent R58K and R58K/D31Q mutated proteins, with DeltaV(390) = -2.0 and -1.9 ml/mol, respectively, and DeltaV(715) approximately 0. The D31Q and D31N substitutions exhibit smaller but well-detectable effects. These results show that the photo-induced volume changes involve the protein region comprising Arg-58, which tightly interacts with the FMN phosphate group.     

Cardiovascular and renal characteristics, and responses to acute volume expansion of a rat model of diabetic pregnancy

The objective of this study was to characterize the cardiovascular and renal alterations that occur during diabetic pregnancy, and to evaluate the effect of insulin treatment in 12-14 days pregnant diabetic rats. Four groups of female Sprague Dawley rats were studied: virgin control group (NP), pregnant control group (CP), diabetic pregnant group (DP), and diabetic pregnant group with insulin treatment (DPI). Systolic arterial pressure (SAP) was increased on day 12, whereas heart rate (HR) decreased starting with day 3 in DP group of rats. DP rats exhibited marked renal hypertrophy with greater kidney weight (wt) and kidney wt/body wt ratio. Insulin treatment normalized blood glucose (BG) concentration, SAP and HR, and prevented the increase in kidney wt/body wt ratio in DPI rats. At the time of the terminal acute experiment, acute saline volume expansion (VE, 5% body wt/30 min) significantly increased renal interstitial hydrostatic pressure (RIHP), urinary sodium excretion (U(Na)V) and urine flow rate (V) in all groups, but the increases (Delta) were significantly attenuated in both CP (1.7 +/- 0.2mmHg, 12.0 +/- 1.5 microEq.min(-1).g kidney wt(-1) and 76.2 +/- 10.9 microl.min(-1).g kidney wt(-1) for DeltaRIHP, DeltaU(Na)V and DeltaV respectively) and DP (1.3 +/- 0.1 mmHg, 6.8 +/- 1.8 microEq.min(-1).g kidney wt(-1) and 32.3 +/- 9.3 microl.min(-1).g kidney wt(-1) for DeltaRIHP, DeltaU(Na)V and DeltaV respectively) group of rats as compared to NP (4.0 +/- 0.6 mmHg, 21.6 +/- 1.4 microEq.min(-1).g kidney wt(-1)and 136.8 +/- 10.5 microl.min(-1).g kidney wt(-1) for DeltaRIHP, DeltaU(Na)V and DeltaV respectively) group of rats. Although RIHP response to VE was similar in DP and CP group of rats, the natriuretic and diuretic responses to VE were significantly lower in DP as compared to CP group of rats. Insulin treatment had no effect on RIHP response (DeltaRIHP = 1.5 +/- 0.3 mmHg), but restored most of the natriuretic (DeltaU(Na)V = 15.7 +/- 2.9 microEq.min(-1).g kidney wt(-1)) and diuretic (DeltaV = 100.2 +/- 19.3 microl.min(-1).g kidney wt(-1)) responses to VE in DPI as compared with CP group of rats. These data suggest that with VE, the restoration of the increase in U(Na)V and V with insulin treatment in diabetic pregnant rats is not mediated by changes in RIHP.     

Effect of pressure on deuterium isotope effects of formate dehydrogenase

High pressure causes biphasic effects on the oxidation of formate by yeast formate dehydrogenase as expressed on the kinetic parameter V/K, which measures substrate capture. Moderate pressure increases capture by accelerating hydride transfer. The transition state for hydride transfer has a smaller volume than the free formate plus the capturing form of enzyme, with DeltaV(double dagger) = -9.7 +/- 1.0 mL/mol. Pressures above 1.5 kbar decrease capture, reminiscent of effects on the conformational change associated with the binding of nicotinamide adenine dinucleotide (NAD(+)) to yeast alcohol dehydrogenase [Northrop, D. B., and Y. K. Cho (2000) Biochemistry 39, 2406-2412]. The collision complex, E-NAD(+), has a smaller volume than the more tightly bound reactant-state complex, E-NAD(+), with DeltaV = +83.4 +/- 5.2 mL/mol. A comparison of the effects of pressure on the oxidation of normal and deuteroformate shows that the entire isotope effect on hydride transfer, 2.73 +/- 0.20, arises solely from transition-state phenomena, as was also observed previously with yeast alcohol dehydrogense. In contrast, normal primary isotope effects arise solely from different zero-point energies in reactant states, and those that express hydrogen tunneling arise from a mixture of both reactant-state and transition-state phenomena. Moreover, pressure increases the primary intrinsic deuterium isotope effect, the opposite of what was observed with yeast alcohol dehydrogense. The lack of a decrease in the isotope effect is also contrary to empirical precedents from chemical reactions suspected of tunneling and to theoretical constructs of vibrationally enhanced tunneling in enzymatic reactions. Hence, this new experimental design penetrates transition states of enzymatic catalysis as never before, reveals the presence of phenomena foreign to chemical kinetics, and calls for explanations of how enzymes work beyond the tenants of physical organic chemistry.     

Effect of hydrostatic pressure on conformational changes of canine milk lysozyme between the native, molten globule, and unfolded states

The effect of pressure on the unfolding of the native (N) and molten globule (MG) state of canine milk lysozyme (CML) was examined using ultraviolet (UV) spectroscopy at pH 4.5 and 2.0, respectively. It appeared that the thermally induced unfolding was promoted by the increase of pressure from atmospheric to 100 MPa, which indicates that both the N and MG states of CML unfolded with the decrease of the partial molar volume change (DeltaV). The volume changes needed for unfolding were estimated from the free energy change vs. pressure plots, and these volume changes became less negative from 20 to 60 degrees C. The DeltaV values at 25 degrees C were obtained for the N-MG (-46 cm3/mol) and MG-unfolded-state (U) transition (-40 cm3/mol). With regards to the MG-U transition, this value is contrastive to that of bovine alpha-lactalbumin (BLA) (0.9 cm3/mol), which is homologous to CML. Previous studies revealed that the MG state of CML was significantly more stable, and closer to the N state in structure, than that of BLA. In contrast to the swollen hydrophobic core of the MG state of BLA, our results suggest that the MG state of CML possesses a tightly packed hydrophobic core into which water molecules cannot penetrate.     

Antibody responses elicited in macaques immunized with human immunodeficiency virus type 1 (HIV-1) SF162-derived gp140 envelope immunogens: comparison with those elicited during homologous simian/human immunodeficiency virus SHIVSF162P4 and heterologous HIV-1 infection

The antibody responses elicited in rhesus macaques immunized with soluble human immunodeficiency virus (HIV) Env gp140 proteins derived from the R5-tropic HIV-1 SF162 virus were analyzed and compared to the broadly reactive neutralizing antibody responses elicited during chronic infection of a macaque with a simian/human immunodeficiency virus (SHIV) expressing the HIV-1 SF162 Env, SHIV(SF162P4), and humans infected with heterologous HIV-1 isolates. Four gp140 immunogens were evaluated: SF162gp140, DeltaV2gp140 (lacking the crown of the V2 loop), DeltaV3gp140 (lacking the crown of the V3 loop), and DeltaV2DeltaV3gp140 (lacking both the V2 and V3 loop crowns). SF162gp140 and DeltaV2gp140 have been previously evaluated by our group in a pilot study, but here, a more comprehensive analysis of their immunogenic properties was performed. All four gp140 immunogens elicited stronger anti-gp120 than anti-gp41 antibodies and potent homologous neutralizing antibodies (NAbs) that primarily targeted the first hypervariable region (V1 loop) of gp120, although SF162gp140 also elicited anti-V3 NAbs. Heterologous NAbs were elicited by SF162gp140 and DeltaV2gp140 but were weak in potency and narrow in specificity. No heterologous NAbs were elicited by DeltaV3gp140 or DeltaV2DeltaV3gp140. In contrast, the SHIV(SF162P4)-infected macaque and HIV-infected humans generated similar titers of anti-gp120 and anti-gp41 antibodies and NAbs of significant breadth against primary HIV-1 isolates, which did not target the V1 loop. The difference in V1 loop immunogenicity between soluble gp140 and virion-associated gp160 Env proteins derived from SF162 may be the basis for the observed difference in the breadth of neutralization in sera from the immunized and infected animals studied here.     

Pressure perturbation and differential scanning calorimetric studies of bipolar tetraether liposomes derived from the thermoacidophilic archaeon Sulfolobus acidocaldarius

Differential scanning calorimetry (DSC) and pressure perturbation calorimetry (PPC) were used to characterize thermal phase transitions, membrane packing, and volumetric properties in multilamellar vesicles (MLVs) composed of the polar lipid fraction E (PLFE) isolated from the thermoacidophilic archaeon Sulfolobus acidocaldarius grown at different temperatures. For PLFE MLVs derived from cells grown at 78 degrees C, the first DSC heating scan exhibits an endothermic transition at 46.7 degrees C, a small hump near 60 degrees C, and a broad exothermic transition at 78.5 degrees C, whereas the PPC scan reveals two transitions at approximately 45 degrees C and 60 degrees C. The endothermic peak at 46.7 degrees C is attributed to a lamellar-to-lamellar phase transition and has an unusually low DeltaH (3.5 kJ/mol) and DeltaV/V (0.1%) value, as compared to those for the main phase transitions of saturated diacyl monopolar diester lipids. This result may arise from the restricted trans-gauche conformational changes in the dibiphytanyl chain due to the presence of cyclopentane rings and branched methyl groups and due to the spanning of the lipid molecules over the whole membrane. The exothermic peak at 78.5 degrees C probably corresponds to a lamellar-to-cubic phase transition and exhibits a large and negative DeltaH value (-23.2 kJ/mol), which is uncommon for normal lamellar-to-cubic phospholipid phase transformations. This exothermic transition disappears in the subsequent heating scans and thus may involve a metastable phase, which is irreversible at the scan rate used. Further, there is no distinct peak in the plot of the thermal expansion coefficient alpha versus temperature near 78.5 degrees C, indicating that this lamellar-to-cubic phase transition is not accompanied by any significant volume change. For PLFE MLVs derived from cells grown at 65 degrees C, similar DSC and PPC profiles and thermal history responses were obtained. However, the lower growth temperature yields a higher DeltaV/V ( approximately 0.25%) and DeltaH (14 kJ/mol) value for the lamellar-to-lamellar phase transition measured at the same pH (2.1). A lower growth temperature also generates a less negative temperature dependence of alpha. The changes in DeltaV/V, DeltaH, and the temperature dependence of alpha can be attributed to the decrease in the number of cyclopentane rings in PLFE at the lower growth temperature. The relatively low DeltaV/V and small DeltaH involved in the phase transitions help to explain why PLFE liposomes are remarkably thermally stable and also echo the proposal that PLFE liposomes are generally rigid and tightly packed. These results help us to understand why, despite the occurrence of thermal-induced phase transitions, PLFE liposomes exhibit a remarkably low temperature sensitivity of proton permeation and dye leakage.     

Pressure equilibrium and jump study on unfolding of 23-kDa protein from spinach photosystem II

Pressure-induced unfolding of 23-kDa protein from spinach photosystem II has been systematically investigated at various experimental conditions. Thermodynamic equilibrium studies indicate that the protein is very sensitive to pressure. At 20 degrees C and pH 5.5, 23-kDa protein shows a reversible two-state unfolding transition under pressure with a midpoint near 160 MPa, which is much lower than most natural proteins studied to date. The free energy (DeltaG(u)) and volume change (DeltaV(u)) for the unfolding are 5.9 kcal/mol and -160 ml/mol, respectively. It was found that NaCl and sucrose significantly stabilize the protein from unfolding and the stabilization is associated not only with an increase in DeltaG(u) but also with a decrease in DeltaV(u). The pressure-jump studies of 23-kDa protein reveal a negative activation volume for unfolding (-66.2 ml/mol) and a positive activation volume for refolding (84.1 ml/mol), indicating that, in terms of system volume, the protein transition state lies between the folded and unfolded states. Examination of the temperature effect on the unfolding kinetics indicates that the thermal expansibility of the transition state and the unfolded state of 23-kDa protein are closer to each other and they are larger than that of the native state. The diverse pressure-refolding pathways of 23-kDa protein in some conditions were revealed in pressure-jump kinetics.     

Thermodynamics of electron transfer in oxygenic photosynthetic reaction centers: volume change, enthalpy, and entropy of electron-transfer reactions in manganese-depleted photosystem II core complexes

We have previously reported the thermodynamic data of electron transfer in photosystem I using pulsed time-resolved photoacoustics [Hou et al. (2001) Biochemistry 40, 7109-7116]. In the present work, using preparations of purified manganese-depleted photosystem II (PS II) core complexes from Synechocystis sp. PCC 6803, we have measured the DeltaV, DeltaH, and estimated TDeltaS of electron transfer on the time scale of 1 micros. At pH 6.0, the volume contraction of PS II was determined to be -9 +/- 1 A3. The thermal efficiency was found to be 52 +/- 5%, which corresponds to an enthalpy change of -0.9 +/- 0.1 eV for the formation of the state P680+Q(A-) from P680*. An unexpected volume expansion on pulse saturation of PS II was observed, which is reversible in the dark. At pH 9.0, the volume contraction, the thermal efficiency, and the enthalpy change were -3.4 +/- 0.5 A3, 37 +/- 7%, and -1.15 +/- 0.13 eV, respectively. The DeltaV of PS II, smaller than that of PS I and bacterial centers, is assigned to electrostriction and analyzed using the Drude-Nernst equation. To explain the small DeltaV for the formation of P680+Q(A-) or Y(Z*)Q(A-), we propose that fast proton transfer into a polar region is involved in this reaction. Taking the free energy of charge separation of PS II as the difference between the energy of the excited-state P680* and the difference in the redox potentials of the donor and acceptor, the apparent entropy change (TDeltaS) for charge separation of PS II is calculated to be negative, -0.1 +/- 0.1 eV at pH 6.0 (P680+Q(A-)) and -0.2 +/- 0.15 eV at pH 9.0 (Y(Z*)Q(A-)). The thermodynamic properties of electron transfer in PS II core reaction centers thus differ considerably from those of bacterial and PS I reaction centers, which have DeltaV of approximately -27 A3, DeltaH of approximately -0.4 eV, and TDeltaS of approximately +0.4 eV.     

Effects of inspiratory flow on diaphragmatic motor output in normal subjects.

Increasing inspiratory flow (V) has been shown to shorten neural inspiratory time (TI(n)) in normal subjects breathing on a mechanical ventilator, but the effect of V on respiratory motor output before inspiratory termination has not previously been studied in humans. While breathing spontaneously on a mechanical ventilator, eight normal subjects were intermittently exposed to 200-ms-duration positive pressure pulses of different amplitudes at the onset of inspiration. Based on the increase in V above control breaths (DeltaV), trials were grouped into small, medium, and large groups (mean DeltaV: 0.51, 1.11, and 1.65 l/s, respectively). We measured TI(n), transdiaphragmatic pressure (Pdi), and electrical activity (electromyogram) of the diaphragm (EMGdi). Transient increases in V caused shortening of TI(n) from 1.34 to 1.10 (not significant), 1.55 to 1.11 (P < 0.005), and 1.58 to 1.17 s (P < 0. 005) in the small, medium, and large DeltaV groups, respectively. EMGdi measured at end TI(n) of the pulse breaths was 131 (P < 0.05), 142, and 155% (P < 0.05) of the EMGdi of the control breaths at an identical time point in the small, medium, and large trials, respectively. The latency of the excitation was 126 +/- 42 (SD) ms, consistent with a reflex effect. Increasing V had two countervailing effects on Pdi: 1) a depressant mechanical effect due primarily to the force-length (11.2 cmH(2)O/l) relation of the diaphragm, and 2) an increase in diaphragm activation. For the eight subjects, mean peak Pdi did not change significantly, but there was significant intersubject variability, reflecting variability in the strength of the excitation reflex. We conclude that increasing inspiratory V causes a graded facilitation of EMGdi, which serves to counteract the negative effect of the force-length relation on Pdi.     

High-pressure studies of aggregation of recombinant human interleukin-1 receptor antagonist: thermodynamics, kinetics, and application to accelerated formulation studies

Recombinant human interleukin-1 receptor antagonist (IL-1ra) in aqueous solutions unfolds and aggregates when subjected to hydrostatic pressures greater than about 180 MPa. This study examined the mechanism and thermodynamics of pressure-induced unfolding and aggregation of IL-1ra. The activation free energy for growth of aggregates (DeltaG-/+(aggregation)) was found to be 37 +/- 3 kJ/mol, whereas the activation volume (DeltaV-/+(aggregation)) was -120 +/- 20 mL/mol. These values compare closely with equilibrium values for denaturation: The free energy for denaturation, DeltaG(denaturation), was 20 +/- 5 kJ/mol, whereas the partial specific volume change for denaturation, DeltaV(denaturation), was -110 +/- 30 mL/mol. When IL-1ra begins to denature at pressures near 140 MPa, cysteines that are normally buried in the native state become exposed. Under oxidizing conditions, this results in the formation of covalently cross-linked aggregates containing nonnative, intermolecular disulfide bonds. The apparent activation free energy for nucleation of aggregates, DeltaG-/+(nuc), was 42 +/- 4 kJ/mol, and the activation volume for nucleation, DeltaV-/+(nuc),was -175 +/- 37 mL/mol, suggesting that a highly solvent-exposed conformation is needed for nucleation. We hypothesize that the large specific volume of IL-1ra, 0.752 +/- 0.004 mL/g, coupled with its relatively low conformational stability, leads to its susceptibility to denaturation at relatively low pressures. The positive partial specific adiabatic compressibility of IL-1ra, 4.5 +/- 0.7 +/- 10(-12) cm2/dyn, suggests that a significant component of the DeltaV(denaturation) is attributable to the elimination of solvent-free cavities. Lastly, we propose that hydrostatic pressure is a useful variable to conduct accelerated formulation studies of therapeutic proteins.