Alternative prion structural changes revealed by high pressure

At high temperature, recombinant hamster prion protein (SHaPrP(90-231)) undergoes aggregation and changes from a predominantly alpha-helical to beta-sheet conformation. We then applied high pressure (200 MPa) to the beta-sheet-rich conformation. The aggregation was reversed, and the original tertiary and secondary structures were recovered at ambient pressure, after pressure release. The application of a pressure of 200 MPa thus allowed studying the heat-induced equilibrium refolding in the absence of protein aggregation. Prion protein unfolding as a function of high pressure was also investigated. Simple two-state, reversible unfolding transitions were observed, as monitored by spectral changes in the UV and fluorescence of the hydrophobic probe 8-anilino-1-naphthalene sulfonate. However, these heat- and pressure-induced conformers differed in their unfolding free energy. At pressures over 400 MPa, strong thioflavin-T binding was observed, suggesting a further structural change to a metastable oligomeric structure.     

Pressure-Temperature Stability, Ca(2+) Binding, and Pressure-Temperature Phase Diagram of Cod Parvalbumin: Gad m 1

Fish allergy is associated with IgE-mediated hypersensitivity reactions to parvalbumins, which are small calcium-binding muscle proteins and represent the major and sole allergens for 95% of fish-allergic patients. We performed Fourier transform infrared and tryptophan fluorescence spectroscopy to explore the pressure-temperature (p-T) phase diagram of cod parvalbumin (Gad m 1) and to elucidate possible new ways of pressure-temperature inactivation of this food allergen. Besides the secondary structure of the protein, the Ca(2+) binding to aspartic and glutamic acid residues was detected. The phase diagram was found to be quite complex, containing partially unfolded and molten globule states. The Ca(2+) ions were essential for the formation of the native structure. A molten globule conformation appears at 50 °C and atmospheric pressure, which converts into an unordered aggregated state at 75 °C. At >200 MPa, only heat unfolding, but no aggregation, was observed. A pressure of 500 MPa leads to a partially unfolded state at 27 °C. The complete pressure unfolding could only be reached at an elevated temperature (40 °C) and pressure (1.14 GPa). A strong correlation was found between Ca(2+) binding and the protein conformation. The partially unfolded state was reversibly refolded. The completely unfolded molecule, however, from which Ca(2+) was released, could not refold. The heat-unfolded protein was trapped either in the aggregated state or in the molten globule state without aggregation at elevated pressures. The heat-treated and the combined heat- and pressure-treated protein samples were tested with sera of allergic patients, but no change in allergenicity was found.     

High pressure-induced changes of biological membrane. Study on the membrane-bound Na(+)/K(+)-ATPase as a model system.

In order to study the pressure-induced changes of biological membrane, hydrostatic pressures of from 0.1 to 400 MPa were applied to membrane-bound Na(+)/K(+)-ATPase from pig kidney as a model system of protein and lipid membrane. The activity showed at least a three-step change induced by pressures of 0.1-100 MPa, 100-220 MPa, and 220 MPa or higher. At pressures of 100 MPa or lower a decrease in the fluidity of lipid bilayer and a reversible conformational change in transmembrane protein is induced, leading to the functional disorder of membrane-associated ATPase activity. A pressure of 100-220 MPa causes a reversible phase transition in parts of the lipid bilayer from the liquid crystalline to the gel phase and the dissociation of and/or conformational changes in the protein subunits. These changes could cause a separation of the interface between alpha and beta subunits and between protein and the lipid bilayer to create transmembrane tunnels at the interface. Tunnels would be filled with water from the aqueous environment and take up tritiated water. A pressure of 220 MPa or higher irreversibly destroys and fragments the gross membrane structure, due to protein unfolding and interface separation, which is amplified by the increased pressure. These findings provide an explanation for the high pressure-induced membrane-damage to subcellular organelles.     

Pressure-jump-induced kinetics reveals a hydration dependent folding/unfolding mechanism of ribonuclease A

Pressure-jump (p-jump)-induced relaxation kinetics was used to explore the energy landscape of protein folding/unfolding of Y115W, a fluorescent variant of ribonuclease A. Pressure-jumps of 40 MPa amplitude (5 ms dead-time) were conducted both to higher (unfolding) and to lower (folding) pressure, in the range from 100 to 500 MPa, between 30 and 50 degrees C. Significant deviations from the expected symmetrical protein relaxation kinetics were observed. Whereas downward p-jumps resulted always in single exponential kinetics, the kinetics induced by upward p-jumps were biphasic in the low pressure range and monophasic at higher pressures. The relative amplitude of the slow phase decreased as a function of both pressure and temperature. At 50 degrees C, only the fast phase remained. These results can be interpreted within the framework of a two-dimensional energy surface containing a pressure- and temperature-dependent barrier between two unfolded states differing in the isomeric state of the Asn-113-Pro-114 bond. Analysis of the activation volume of the fast kinetic phase revealed a temperature-dependent shift of the unfolding transition state to a larger volume. The observed compensation of this effect by glycerol offers an explanation for its protein stabilizing effect.     

Effects of pressure on the structure of metmyoglobin: molecular dynamics predictions for pressure unfolding through a molten globule intermediate.

We investigated the pathway for pressure unfolding of metmyoglobin using molecular dynamics (MD) for a range of pressures (0.1 MPa to 1.2 GPa) and a temperature of 300 K. We find that the unfolding of metmyoglobin proceeds via a two-step mechanism native --> molten globule intermediate --> unfolded, where the molten globule forms at 700 MPa. The simulation describes qualitatively the experimental behavior of metmyoglobin under pressure. We find that unfolding of the alpha-helices follows the sequence of migrating hydrogen bonds (i,i + 4) --> (i,i + 2).     

High-pressure denaturation of apomyoglobin

The pressure denaturation of wild type and mutant apomyoglobin (apoMb) was investigated using a high-pressure, high-resolution nuclear magnetic resonance and high-pressure fluorescence techniques. Wild type apoMb is resistant to pressures up to 80 MPa, and denatures to a high-pressure intermediate, I(p), between 80 and 200 MPa. A further increase of pressure to 500 MPa results in denaturation of the intermediate. The two tryptophans, both in the A helix, remain sequestered from solvent in the high-pressure intermediate, which retains some native NOESY cross peaks in the AGH core as well as between F33 and F43. High-pressure fluorescence shows that the tryptophans remain inaccessible to solvent in the I(p) state. Thus the high-pressure intermediate has some structural properties in common with the apoMb I(2) acid intermediate. The resistance of the AGH core to pressures up to 200 MPa provides further evidence that the intrinsic stability of these alpha-helices is responsible for their presence in a number of equilibrium intermediates as well as in the earliest kinetic folding intermediate. Mutations in the AGH core designed to disrupt packing by burying a charge or increasing the size of a hydrophobic residue significantly perturbed the unfolding of native apoMb to the high-pressure intermediate. The F123W and S108L mutants both unfolded at lower pressures, while retaining some resistance to pressures below 50 MPa. The charge burial mutants, A130K and S108K, are not stable at very low pressures and both denature to the intermediate by 100 MPa, half of the pressure required for wild type apoMb. Thus a similar intermediate state is created independent of the method of perturbation, and mutations have similar effects on native state destabilization for both methods of denaturation. These data suggest that equilibrium intermediates that can be formed through different means are likely to resemble a kinetic intermediate.     

压强温度耦合作用下小蛋白去折叠过程的分子动力学模拟

在不同温度(280~540K)和压强(1×102~8×105 kPa)的耦合作用下,对GB1(the B1 domain of protein G)进行了56次独立分子动力学模拟,模拟时间达88.8 ns。在此基础上,研究了压强和温度对GB1去折叠过程的耦合效应。结果表明,压强对温度去折叠过程有明显影响,改变了蛋白质二级结构去折叠速度和蛋白质去折叠过程发生事件的先后次序。相同温度下,GB1的α-螺旋和β-折叠的稳定性随压强增大而提高;可及性表面积和其它结构特性参数随压强增大而减小。适度的压强(如2×105 kPa)会抑制温度导致的GB1二级结构去折叠速度,而更大的压强(如8×105 kPa)又加速了GB1的去折叠速度。在模拟的温度范围,当压强为100和2×105 kPa时,GB1疏水核协同暴露于水,而5×105和8×105 kPa时没出现此现象,这与最近的高压变性实验结果一致。     

High-pressure study on bilayer phase behavior of oleoylmyristoyl- and myristoyloleoyl-phosphatidylcholines

We investigated the thermotropic and barotropic bilayer phase behavior of 1-myristoyl-2-oleoyl-sn-glycero-3-phosphocholine (MOPC) and 1-oleoyl-2-myristoyl-sn-glycero-3-phosphocholine (OMPC) by means of the differential scanning calorimetry (DSC) and high-pressure light-transmittance technique. Water could be used as a solvent for measurements at high pressures because of the elevation of the transition temperatures above 0 degrees C by pressurization, whereas aqueous 50 wt.% ethylene glycol solution was used mainly for those at low pressures. Only one phase transition was observed in the DSC thermogram of the MOPC bilayer membrane as an endothermic peak, and also observed at high pressures as an abrupt change of the light-transmittance. The transition was assigned as a main transition between the lamellar gel (L(beta)) and liquid-crystalline (L(alpha)) phases on the basis of the values of enthalpy change (DeltaH) and slope of the transition temperature with respect to pressure (dT/dP). The DSC thermogram of the OMPC bilayer membrane similarly showed a single endothermic peak but two kinds of phase transitions were observed at different temperatures in the light-transmittance profile at high pressures. The extrapolation of the lower-temperature transition in the high-pressure range to an ambient pressure coincided with the transition observed in the DSC thermogram. This transition was identified as a transition between the lamellar crystal (L(c)) and L(alpha) (or L(beta)) phases from the DeltaH and dT/dP values. The higher-temperature transition, appearing only at high pressures, was identified as the L(beta)/L(alpha) transition considering the topological resemblance of its temperature-pressure phase diagram as that of the dioleoylphosphatidylcholine bilayer membrane. The phase diagram of the OMPC bilayer membrane demonstrated that the L(beta) phase cannot exist at pressures below ca. 190 MPa while it can exist stably in a finite temperature range at pressures above the pressure.     

Pressure-exploration of the 33-kDa protein from the spinach photosystem II particle.

The 33-kDa protein isolated from the spinach photosystem II particle is an ideal model to explore high-pressure protein-unfolding. The protein has a very low free energy as previously reported by chemical unfolding studies, suggesting that it must be easy to modulate its unfolding transition by rather mild pressure. Moreover, the protein molecule consists of only one tryptophan residue (Trp241) and eight tyrosine residues, which can be conveniently used to probe the protein conformation and structural changes under pressure using either fluorescence spectroscopy or fourth derivative UV absorbance spectroscopy. The different experimental methods used in the present study indicate that at 20 degrees C and pH 6, the 33-kDa protein shows a reversible two-state unfolding transition from atmospheric pressure to about 180 MPa. This value is much lower than those found for the unfolding of most proteins studied so far. The unfolding transition induces a large red shift of the maximum fluorescence emission of 34 nm (from 316 nm to 350 nm). The change in standard free energy (DeltaGo) and in volume (DeltaV) for the transition at pH 6.0 and 20 degrees C are -14.6 kJ.mol-1 and -120 mL.mol-1, respectively, in which the DeltaGo value is consistent with that obtained by chemical denaturation. We found that pressure-induced protein unfolding is promoted by elevated temperatures, which seem largely attributed to the decrease in the absolute value of DeltaGo (only a minor variation was observed for the DeltaV value). However, the promotion of the unfolding by alkaline pH seems mainly related to the increase in DeltaV without any significant changes in DeltaGo. It was also found that NaCl significantly protects the protein from pressure-induced unfolding. In the presence of 1 M NaCl, the pressure needed to induce the half-unfold of the protein is shifted to a higher value (shift of 75 MPa) in comparison with that observed without NaCl. Interestingly, in the presence of NaCl, the value of DeltaV is significantly reduced whilst that of DeltaGo remains as before. The unfolding-refolding kinetics of the protein has also been studied by pressure-jump, in which it was revealed that both reactions are a two-state transition process with a relatively slow relaxation time of about 102 s.     

Microsecond simulations of the folding/unfolding thermodynamics of the Trp‐cage miniprotein

We study the unbiased folding/unfolding thermodynamics of the Trp‐cage miniprotein using detailed molecular dynamics simulations of an all‐atom model of the protein in explicit solvent using the Amberff99SB force field. Replica‐exchange molecular dynamics simulations are used to sample the protein ensembles over a broad range of temperatures covering the folded and unfolded states at two densities. The obtained ensembles are shown to reach equilibrium in the 1 μs/replica timescale. The total simulation time used in the calculations exceeds 100 μs. Ensemble averages of the fraction folded, pressure, and energy differences between the folded and unfolded states as a function of temperature are used to model the free energy of the folding transition, ΔG(P, T), over the whole region of temperatures and pressures sampled in the simulations. The ΔG(P, T) diagram describes an ellipse over the range of temperatures and pressures sampled, predicting that the system can undergo pressure‐induced unfolding and cold denaturation at low temperatures and high pressures, and unfolding at low pressures and high temperatures. The calculated free energy function exhibits remarkably good agreement with the experimental folding transition temperature (T_f = 321 K), free energy, and specific heat changes. However, changes in enthalpy and entropy are significantly different than the experimental values. We speculate that these differences may be due to the simplicity of the semiempirical force field used in the simulations and that more elaborate force fields may be required to describe appropriately the thermodynamics of proteins. Proteins 2010. © 2010 Wiley‐Liss, Inc.     

Polyhydric alcohol protective effect on Rhizomucor miehei lipase deactivation enhanced by pressure and temperature treatment

The influence of polyhydric alcohols (sorbitol, xylitol, erythritol, glycerol) on the thermal stability of Rhizomucor miehei lipase has been studied at high hydrostatic pressure (up to 500 MPa). In the absence of additives, a protective effect (PE) (the ratio between the residual activities determined at 480 MPa for the enzyme in the presence or absence of polyhydric alcohols) of low-applied pressures (from 50 MPa to 350 MPa) against thermal deactivations (at 50°C and 55°C) has been noticed. In the presence of additives, a strong correlation between PE and the total hydroxyl group concentration has been obtained, for the first time, under treatments of combining denaturing temperatures and high hydrostatic pressures. This relationship does not seem to be dependent on the nature polyhydric alcohols as the same effect could be observed with 1 M sorbitol and 2 M glycerol. This PE, against thermal and high pressure combined lipase deactivation, increases with polyhydric alcohol concentrations, and when temperature increases from 25°C to 55°C.     

Bilayer phase transitions of N-methylated dioleoylphosphatidylethanolamines under high pressure

The bilayer phase transitions of four kinds of unsaturated phospholipids with different-sized polar head groups, dioleoylphosphatidylethanolamine (DOPE), dioleoylphosphatidyl-N-methylethanolamine (DOMePE), dioleoylphosphatidyl-N,N-dimethylethanolamine (DOMe2PE) and dioleoylphosphatidylcholine (DOPC), were observed by means of differential scanning calorimetry (DSC) and high-pressure light-transmittance. DSC thermogram and light-transmittance curve for each phospholipid vesicle solution exhibited only one phase transition under ambient pressure, respectively. The light-transmittance of DOPC solution at pressure higher than 234 MPa abruptly increased stepwise at two temperatures, which corresponds to the appearance of stable subgel and lamellar gel phases under high pressure in addition to the liquid crystal phase. The constructed temperature (T)-pressure (p) phase diagrams were compared among these phospholipids. The phase-transition temperatures of the phospholipids decreased stepwise by N-methylation of the head group. The slops of the T-p phase boundary (dT/dp) of DOPE, DOMePE and DOMe2PE bilayers (0.127-0.145 K MPa-1) were found to be close to that of the transition from the lamellar crystal (or subgel; Lc) phase to the liquid crystal (Lalpha) phase for DOPC bilayer (0.131 K MPa-1). On the other hand, the dT/dp value of the main transition from the lamellar gel (Lbeta) phase to the Lalpha phase for DOPC bilayer (0.233 K MPa-1) was significantly different from that of the Lc/Lalpha transition, hence both curves intersected with each other at 234 MPa. The thermodynamic quantities associated with the phase transition of DOPE, DOMePE and DOMe2PE bilayers had also similar values to those for the Lc/Lalpha transition of DOPC bilayer. Taking into account of the values of transition temperature, dT/dp and thermodynamic quantities compared with the corresponding results of saturated phospholipids, we identified the phase transitions observed in the DOPE, DOMePE and DOMe2PE bilayers as the transition from the Lc phase to the Lalpha phase although they have been regarded as the main transition in the previous studies. The Lbeta phase is probably unstable for DOPE, DOMePE and DOMe2PE bilayers at all pressures, it exists as a metastable phase at pressures below 234 MPa while as a stable phase at pressures above 234 MPa in DOPC bilayer. The difference in phase stability among the phospholipid bilayers is originated from that in hydration structure of the polar head groups.     

Hydrolysis of β-lactoglobulin by thermolysin and pepsin under high hydrostatic pressure

Hydrolysis of β-lactoglobulin with thermolysin and pepsin at pressures ranging between 0.1 and 350 MPa showed a significant increase of cleavage rates. Pressure-induced changes of susceptibility to hydrolysis of β-lactoglobulin proteolytic sites were also observed. The pressure, raised to 200 MPa, accelerates the hydrolysis of β-lactoglobulin by thermolysin and changes obtained peptide profiles. Initially, higher pressure makes the N-terminal, and to a smaller extent, C-terminal peptide fragments of β-lactoglobulin molecule, more susceptible to removal by thermolysin. This indicates combined influence of pressure-induced thermolysin activation and partial unfolding of β-lactoglobulin by compression at neutral pHs. The rates of hydrolysis of β-lactoglobulin by pepsin (negligible at 0.1 MPa) are increased considerably with pressure up to 300 MPa. The Susceptibility of β-lactoglobulin proteolytic sites to peptic cleavage remains constant over all the studied pressure range. The lack of significant qualitative changes in the peptic peptide profiles produced at different pressures and at clearly pressure-dependent rates points to negative reaction volume changes as the major factor in peptic hydrolysis of β-lactoglobulin under high pressure. Thus the β-lactoglobulin molecule resists pressure-induced unfolding in acid pHs and yields to it in neutral pHs. © 1995 John Wiley & Sons, Inc.     

Pressure-jump studies of the folding/unfolding of trp repressor.

The dimeric protein, trp apo-repressor of Escherichia coli has been subjected to high hydrostatic pressure under a variety of conditions, and the effects have been monitored by fluorescence spectroscopic and infra-red absorption techniques. Under conditions of micromolar protein concentration and low, non-denaturing concentrations of guanidinium hydrochloride (GuHCl), tryptophan and 8-anilino-1-naphthalene sulfonate (ANS) fluorescence detected high pressure profiles demonstrate that pressures below 3 kbar result in dissociation of the dimer to a monomeric species that presents no hydrophobic binding sites for ANS. The FTIR-detected high pressure profile obtained under significantly different solution conditions (30 mM trp repressor in absence of denaturant) exhibits a much smaller pressure dependence than the fluorescence detected profiles. The pressure-denatured form obtained under the FTIR conditions retains about 50 % alpha-helical structure. From this we conclude that the secondary structure present in the high pressure state achieved under the conditions of the fluorescence experiments is at least as disrupted as that achieved under FTIR conditions. Fluorescence-detected pressure-jump relaxation studies in the presence of non-denaturing concentrations of GuHCl reveal a positive activation volume for the association/folding reaction and a negative activation volume for dissociation/unfolding reaction, implicating dehydration as the rate-limiting step for association/folding and hydration as the rate-limiting step for unfolding. The GuHCl concentration dependence of the kinetic parameters place the transition state at least half-way along the reaction coordinate between the unfolded and folded states. The temperature dependence of the pressure-jump fluorescence-detected dissociation/unfolding reaction in the presence of non-denaturing GuHCl suggests that the curvature in the temperature dependence of the stability arises from non-Arrhenius behavior of the folding rate constant, consistent with a large decrease in heat capacity upon formation of the transition state from the unfolded state. The decrease in the equilibrium volume change for folding with increasing temperature (due to differences in thermal expansivity of the folded and unfolded states) arises from a decrease in the absolute value for the activation volume for unfolding, thus indicating that the thermal expansivity of the transition state is similar to that of the unfolded state.     

Inactivation of creatine kinase by high pressure may precede dimer dissociation.

The effects of hydrostatic pressure on creatine kinase activity and conformation were investigated using either the high-pressure stopped-flow method in the pressure range 0.1-200 MPa for the activity determination, or the conventional activity measurement and fluorescence spectroscopy up to 650 MPa. The changes in creatine kinase activity and intrinsic fluorescence show a total or partial reversibility after releasing pressure, depending on both the initial value of the high pressure applied and on the presence or absence of guanidine hydrochloride. The study on 8-anilinonaphthalene-1-sulfonate binding to creatine kinase under high pressure indicates that the hydrophobic core of creatine kinase was progressively exposed to the solvent at pressures above 300 MPa. This data shows that creatine kinase is inactivated at low pressure, preceding both the enzyme dissociation and the unfolding of the hydrophobic core occurring at higher pressure. Moreover, in agreement with the recently published structure of the dimer, it can be postulated that the multistate transitions of creatine kinase induced both by pressure and guanidine denaturation are in direct relationship with the existence of hydrogen bonds which maintain the dimeric structure of the enzyme.     

Pressure and denaturants in the unfolding of triosephosphate isomerase: the monomeric intermediates of the enzymes from Saccharomyces cerevisiae and Entamoeba histolytica

Triosephosphate isomerase (TIM) is a dimeric enzyme formed by two identical (beta/alpha)8 barrels. In this work, we compare the unfolding and refolding of the TIMs from Entamoeba histolytica (EhTIM) and baker's yeast (yTIM). A monomeric intermediate was detected in the GdnHCl-induced unfolding of EhTIM. The thermodynamic, spectroscopic, catalytic, and hydrodynamic properties of this intermediate were found to be very similar to those previously described for a monomeric intermediate of yTIM observed in GdnHCl. Monomer unfolding was reversible for both TIMs; however, the dissociation step was reversible in yTIM and irreversible in EhTIM. Monomer unfolding induced by high pressure in the presence of GdnHCl was a reversible process. DeltaGUnf, DeltaVUnf, and P1/2 were obtained for the 0.7-1.2 M GdnHCl range. The linear extrapolation of these thermodynamic parameters to the absence of denaturant showed the same values for both intermediates. The DeltaVUnfH2O values calculated for EhTIM and yTIM monomeric intermediates are the same within experimental error (-57 +/- 10 and -76 +/- 14 mL/mol, respectively). These DeltaVUnf H2O values are smaller than those reported for the unfolding of monomeric proteins of similar size, suggesting that TIM intermediates are only partially hydrated. |DeltaVUnf| increased with denaturant concentration; this behavior is probably related to structural changes in the unfolded state induced by GdnHCl and pressure. From the thermodynamic parameters that were obtained, it is predicted that in the absence of denaturants, pressure would induce monomer unfolding (P1/2 approximately 140 MPa) prior to dimer dissociation (P1/2 approximately 580 MPa). Therefore, dimerization prevents the pressure unfolding of the monomer.     

Effect of Ligands on HP-Induced Unfolding and Oligomerization of β-Lactoglobulin

To probe intermediate states during unfolding and oligomerization of proteins remains a major challenge. High pressure (HP) is a powerful tool for studying these problems, revealing subtle structural changes in proteins not accessible by other means of denaturation. Bovine β-lactoglobulin (BLG), the main whey protein, has a strong propensity to bind various bioactive molecules such as retinol and resveratrol, two ligands with different affinity and binding sites. By combining in situ HP-small-angle neutron scattering (SANS) and HP-ultraviolet/visible absorption spectroscopy, we report the specific effects of these ligands on three-dimensional conformational and local changes in BLG induced by HP. Depending on BLG concentration, two different unfolding mechanisms are observed in situ under pressures up to ∼300 MPa: either a complete protein unfolding, from native dimers to Gaussian chains, or a partial unfolding with oligomerization in tetramers mediated by disulfide bridges. Retinol, which has a high affinity for the BLG hydrophobic cavity, significantly stabilizes BLG both in three-dimensional and local environments by shifting the onset of protein unfolding by ∼100 MPa. Increasing temperature from 30 to 37°C enhances the hydrophobic stabilization effects of retinol. In contrast, resveratrol, which has a low binding affinity for site(s) on the surface of the BLG, does not induce any significant effect on the structural changes of BLG due to pressure. HP treatment back and forth up to ∼300 MPa causes irreversible covalent oligomerization of BLG. Ab initio modeling of SANS shows that the oligomers formed from the BLG-retinol complex are smaller and more elongated compared to BLG without ligand or in the presence of resveratrol. By combining HP-SANS and HP-ultraviolet/visible absorption spectroscopy, our strategy highlights the crucial role of BLG hydrophobic cavity and opens up new possibilities for the structural determination of HP-induced protein folding intermediates and irreversible oligomerization.     

Essential dynamics of the cold denaturation: pressure and temperature effects in yeast frataxin

The cold denaturation of globular proteins is a process that can be caused by increasing pressure or decreasing the temperature. Currently, the action mechanism of this process has not been clearly understood, raising an interesting debate on the matter. We have studied the process of cold denaturation using molecular dynamics simulations of the frataxin system Yfh1, which has a dynamic experimental characterization of unfolding at low and high temperatures. The frataxin model here studied allows a comparative analysis using experimental data. Furthermore, we monitored the cold denaturation process of frataxin and also investigated the effect under the high‐pressure regime. For a better understanding of the dynamics and structural properties of the cold denaturation, we also analyzed the MD trajectories using essentials dynamic. The results indicate that changes in the structure of water by the effect of pressure and low temperatures destabilize the hydrophobic interaction modifying the solvation and the system volume leading to protein denaturation. Proteins 2016; 85:125–136. © 2016 Wiley Periodicals, Inc.     

Temperature and pressure effects on C112S azurin: Volume,expansivity, and flexibility changes

The pressure‐induced unfolding of the mutant C112S azurin from Pseudomonas aeruginosa was monitored both under steady state and dynamic conditions. The unfolding profiles were obtained by recording the spectral shift of the fluorescence emission as well as by phosphorescence intensity measurements. We evaluated the difference in free energy, ΔG, as a function of pressure and temperature. The dependence of ΔG on temperature showed concave profile at all pressures studied. A positive heat capacity change of about 4.3 kJ mol^?1 deg^?1 fitted all the curves. The volume change of the reaction showed a moderate dependence on temperature when compared with other proteins previously studied. The kinetic activation parameters (ΔV*, ΔH*, ΔS*) were obtained from upward and downward pressure‐jump experiments and used to characterize the volumetric and energetic properties of the transition state between native and unfolded protein. Our findings suggest that the folding and unfolding reaction paths passed through different transition states. The change in the phosphorescence lifetime with pressure pointed out that pressure‐induced unfolding occurred within two steps: the first leading to an increased protein flexibility, presumably caused by water penetration into the protein. Major structural changes of the tryptophan environment occurred in a second step at higher pressures. Proteins 2014; 82:1787–1798. © 2014 Wiley Periodicals, Inc.