Pressure-tuning the conformation of bovine pancreatic trypsin inhibitor studied by Fourier-transform infrared spectroscopy

Correlation between protein conformations and water structure and thermodynamics at high pressure: A molecular dynamics study of the Bovine Pancreatic Trypsin Inhibitor (BPTI) protein

Pressure-induced perturbation of a protein structure leading to its folding-unfolding mechanism is an important yet not fully understood phenomenon. The key point here is the role of water and its coupling with protein conformations as a function of pressure. In the current work, using extensive molecular dynamics simulation at 298 K, we systematically examine the coupling between protein conformations and water structures of pressures of 0.001, 5, 10, 15, 20 kbar, starting from (partially) unfolded structures of the protein Bovine Pancreatic Trypsin Inhibitor (BPTI). We also calculate localized thermodynamics at those pressures as a function of protein-water distance. Our findings show that both protein-specific and generic effects of pressure are operating. In particular, we found that (1) the amount of increase in water density near the protein depends on the protein structural heterogeneity; (2) the intra-protein hydrogen bond decreases with pressure, while the water-water hydrogen bond per water in the first solvation shell (FSS) increases; protein-water hydrogen bonds also found to increase with pressure, (3) with pressure hydrogen bonds of waters in the FSS getting twisted; and (4) water's tetrahedrality in the FSS decreases with pressure, but it is dependent on the local environment. Thermodynamically, at higher pressure, the structural perturbation of BPTI is due to the pressure-volume work, while the entropy decreases with the increase of pressure due to the higher translational and rotational rigidity of waters in the FSS. The local and subtle effects of pressure, found in this work, are likely to be typical of pressure-induced protein structure perturbation.

Exploring the polymorphism, conformational dynamics and function of amyloidogenic peptides and proteins by temperature and pressure modulation

Our understanding of amyloid structures and the mechanisms by which disease-associated peptides and proteins self-assemble into these fibrillar aggregates, has advanced considerably in recent years. It is also established that amyloid fibrils are generally polymorphic. The molecular structures of the aggregation intermediates and the causes of molecular and structural polymorphism are less understood, however. Such information is mandatory to explain the pathological diversity of amyloid diseases. What is also clear is that not only protein mutations, but also the physiological milieu, i.e. pH, cosolutes, crowding and surface interactions, have an impact on fibril formation. In this minireview, we focus on the effect of the less explored physical parameters temperature and pressure on the fibrillization propensity of proteins and how these variables can be used to reveal additional mechanistic information about intermediate states of fibril formation and molecular and structural polymorphism. Generally, amyloids are very stable and can resist harsh environmental conditions, such as extreme pH, high temperature and high pressure, and can hence serve as valuable functional amyloid. As an example, we discuss the effect of temperature and pressure on the catalytic activity of peptide amyloid fibrils that exhibit enzymatic activity.

High hydrostatic pressure induces pro-osteoarthritic changes in cartilage precursor cells: A transcriptome analysis

Due to the high water content of cartilage, hydrostatic pressure is likely one of the main physical stimuli sensed by chondrocytes. Whereas, in the physiological range (0 to around 10 MPa), hydrostatic pressure exerts mostly pro-chondrogenic effects in chondrocyte models, excessive pressures have been reported to induce detrimental effects on cartilage, such as increased apoptosis and inflammation, and decreased cartilage marker expression. Though some genes modulated by high pressure have been identified, the effects of high pressure on the global gene expression pattern have still not been investigated. In this study, using microarray technology and real-time PCR validation, we analyzed the transcriptome of ATDC5 chondrocyte progenitors submitted to a continuous pressure of 25 MPa for up to 24 h. Several hundreds of genes were found to be modulated by pressure, including some not previously known to be mechano-sensitive. High pressure markedly increased the expression of stress-related genes, apoptosis-related genes and decreased that of cartilage matrix genes. Furthermore, a large set of genes involved in the progression of osteoarthritis were also induced by high pressure, suggesting that hydrostatic pressure could partly mimic in vitro some of the genetic alterations occurring in osteoarthritis.

Calculation of the infrared spectra of proteins

The CHARMM22 force field with associated partial charges is used to calculate the infrared spectra of a number of small proteins and some larger biothreat proteins. The calculated high-frequency region, from about 2,500 to 3,500 cm(-1), is dominated by stretching modes of hydrogen bonded to other atoms, and is very similar in all proteins. There is a peak at 3,430 cm(-1) whose intensity is predicted by these calculations to be a direct measure of arginine content. The calculated low-frequency THz region, up to 300 cm(-1), is also very similar in all the proteins and just reflects the vibrational density of states in agreement with experimental results. Calculations show that the intermediate-frequency region between 500 and 1,200 cm(-1) shows the greatest difference between individual proteins and is also the least affected by water absorption. However, to match experimental measurements in the amide region, it was necessary to reduce the hydrogen partial charges.

Understanding the role of hydrogen bonds in water dynamics and protein stability

The mechanisms of cold and pressure denaturation of proteins are a matter of debate, but it is commonly accepted that water plays a fundamental role in the process. It has been proposed that the denaturation process is related to an increase of hydrogen bonds among hydration water molecules. Other theories suggest that the causes of denaturation are the density fluctuations of surface water, or the destabilization of hydrophobic contacts as a consequence of water molecule inclusions inside the protein, especially at high pressures. We review some theories that have been proposed to give insight into this problem, and we describe a coarse-grained model of water that compares well with experiments for proteins' hydration water. We introduce its extension for a homopolymer in contact with the water monolayer and study it by Monte Carlo simulations in an attempt to understand how the interplay of water cooperativity and interfacial hydrogen bonds affects protein stability.

Molecular rearrangement of metal-chelating lipid monolayers upon protein adsorption

The controlled adsorption of proteins to well-defined monolayers is critical to advances in sensor and nanotechnology applications where selective adsorption of targeted species is of interest. In the studies reported here, we developed vibrational spectroscopic methods to gain molecular insight into the effect of single-site versus multiple-site binding of proteins to metal-chelating monolayers at an air-water interface. Analysis of real-time planar array infrared reflection-absorption spectra revealed that a Cu(II)-chelated DSIDA lipid monolayer (Cu(2+)-DSIDA) was readily disrupted by adsorption of myoglobin as demonstrated by a blue shift of 1.7 cm(-1) in the v(as)(CH(2)) stretching mode and a reduced peak intensity over a period of 5 h. However, a Zn(II)-chelated monolayer was not affected by the adsorption of either protein, suggesting that multisite binding of protein on the Cu(2+)-DSIDA results in monolayer disruption. Further studies demonstrated that in film form, adsorption of myoglobin to the Cu(2+)-DSIDA perturbed the secondary structures of myoglobin, especially the alpha-helical, random structure, and extended structures. However, no distinct change was observed during adsorption of lysozyme. These results demonstrate the utility of these methods for monitoring the molecular rearrangement of both metal-charged lipid monolayers and proteins that occur during adsorption of a protein with a strong affinity for the monolayer.

Protein under pressure: Molecular dynamics simulation of the arc repressor

Experimental nuclear magnetic resonance results for the Arc Repressor have shown that this dimeric protein dissociates into a molten globule at high pressure. This structural change is accompanied by a modification of the hydrogen-bonding pattern of the intermolecular beta-sheet: it changes its character from intermolecular to intramolecular with respect to the two monomers. Molecular dynamics simulations of the Arc Repressor, as a monomer and a dimer, at elevated pressure have been performed with the aim to study this hypothesis and to identify the major structural and dynamical changes of the protein under such conditions. The monomer appears less stable than the dimer. However, the complete dissociation has not been seen because of the long timescale needed to observe this phenomenon. In fact, the protein structure altered very little when increasing the pressure. It became slightly compressed and the dynamics of the side-chains and the unfolding process slowed down. Increasing both, temperature and pressure, a tendency of conversion of intermolecular into intramolecular hydrogen bonds in the beta-sheet region has been detected, supporting the mentioned hypothesis. Also, the onset of denaturation of the separated chains was observed.

The in situ observation of the temperature and pressure stability of recombinant Aspergillus aculeatus pectin methylesterase with Fourier transform IR spectroscopy reveals an unusual pressure stability of beta-helices

The stability of recombinant Aspergillus aculeatus PME (pectin methylesterase), an enzyme with high beta-helix content, was studied as a function of pressure and temperature. The conformational stability was monitored using FTIR (Fourier transform IR) spectroscopy whereas the functional enzyme stability was monitored by inactivation studies. Protein unfolding followed by amorphous aggregation, which makes the process irreversible, was observed at temperatures above 50 degrees C. This could be correlated to the irreversible enzyme inactivation observed at that temperature. Hydrostatic pressure greater than 1 GPa was necessary to induce changes in the enzyme's secondary structure. No enzyme inactivation was observed at up to 700 MPa. Pressure increased PME stability towards thermal denaturation. At 200 MPa, temperatures above 60 degrees C were necessary to cause significant PME unfolding and loss of activity. These results may be relevant for an understanding of the extreme stability of amyloid fibrils for which beta-helices have been proposed as a structural element.

Protein stability and dynamics in the pressure–temperature plane

The pressure-temperature stability diagram of proteins and the underlying assumptions of the elliptical shape of the diagram are discussed. Possible extensions, such as aggregation and fibril formation, are considered. An important experimental observation is the extreme pressure stability of the mature fibrils. Molecular origins of the diagram in terms of models of the partial molar volume of a protein focus on cavities and hydration. Changes in thermal expansivity, compressibility and heat capacity in terms of fluctuations of the enthalpy and volume change of the unfolding should also focus on these parameters. It is argued that the study of water-soluble polymers might further our understanding of the stability diagram. Whereas the role of water in protein behaviour is unquestioned, the role of cavities is less clear.

Influence of pressure on structure and dynamics of bovine pancreatic trypsin inhibitor (BPTI): small angle and quasi-elastic neutron scattering studies

We have studied the influence of pressure on structure and dynamics of a small protein belonging to the enzymatic catalysis: the bovine pancreatic trypsin inhibitor (BPTI). Using a copper-beryllium high-pressure cell, we have performed small angle neutron scattering (SANS) experiment on NEAT spectrometer at HMI (Berlin, Germany). In the SANS configuration, the evolution of the radius of gyration and of the shape of the protein under pressures up to 6,000 bar has been studied. When increasing pressure from atmospheric pressure up to 6,000 bar, the pressure effects on the global structure of BPTI result on a reduction of the radius of gyration from 13.4 A down to 12.0 A. Between 5,000 and 6,000 bar, some transition already detected by FTIR [N. Takeda, K. Nakano, M. Kato, Y. Taniguchi, Biospectroscopy, 4, 1998, pp. 209-216] is observed. The pressure effect is not reversible because the initial value of the radius of gyration is not recovered after pressure release. By extending the range of wave-vectors to high q, we have observed a change of the form factor (shape) of the BPTI under pressure. At atmospheric pressure BPTI exhibits an ellipsoidal form factor that is characteristic of the native state. When the pressure is increased from atmospheric pressure up to 6,000 bar, the protein keeps its ellipsoidal shape. The parameters of the ellipsoid vary and the transition detected between 5,000 and 6,000 bar in the form factor of BPTI is in agreement with the FTIR results. After pressure release, the form factor of BPTI is characteristic of an ellipsoid of revolution with a semi-axis a, slightly elongated with respect to that of the native one, indicating that the pressure-induced structural changes on the protein are not reversible. The global motions and the internal dynamics of BPTI protein have been investigated in the same pressure range by quasi-elastic neutron scattering experiments on IN5 time-of-flight spectrometer at ILL (Grenoble, France). The diffusion coefficients D and the internal relaxation times <tau(2)> of BPTI deduced from the analysis of the intermediate scattering functions show a slowing down of protein dynamics when increasing pressure.

Probing the pressure-temperature stability of amyloid fibrils provides new insights into their molecular properties

A number of medical disorders, including Alzheimer's disease and type II diabetes, is characterised by the deposition of amyloid fibrils in tissue. The insolubility and size of the fibrils has largely precluded the determination of their structures at high resolution. Studies probing the stability of amyloid fibrils can reveal which non-covalent interactions are important in the formation and maintenance of the fibril structure. In particular, we review here the use of high hydrostatic pressure and high temperature as perturbation techniques. In general, small aggregates formed early in the assembly process can be dissociated by high pressure, but mature amyloid fibrils are highly pressure stable. This finding suggests that a temporal transition occurs during which side chain packing and hydrogen bond formation are optimised, whereas the hydrophobic effect and electrostatic interactions play a dominant role in the early stages of the aggregation. High temperatures, however, can disrupt most aggregates. Though the observed stability of amyloid fibrils is not unique to these structures, the notion that amyloid fibrils can represent the global minimum in free energy is supported by this type of investigations. Some implications regarding the nature of toxic species, associated with at least many of the amyloid disorders, and recently proposed structural models are discussed.

Insights into the role of hydration in protein structure and stability obtained through hydrostatic pressure studies

A thorough understanding of protein structure and stability requires that we elucidate the molecular basis for the effects of both temperature and pressure on protein conformational transitions. While temperature effects are relatively well understood and the change in heat capacity upon unfolding has been reasonably well parameterized, the state of understanding of pressure effects is much less advanced. Ultimately, a quantitative parameterization of the volume changes (at the basis of pressure effects) accompanying protein conformational transitions will be required. The present report introduces a qualitative hypothesis based on available model compound data for the molecular basis of volume change upon protein unfolding and its dependence on temperature.

Effects of Chaotropic and Kosmotropic Cosolvents on the Pressure-Induced Unfolding and Denaturation of Proteins: An FT-IR Study on Staphylococcal Nuclease†

FT-IR spectroscopy was used to study the effects of various chaotropic and kosmotropic cosolvents (glycerol, sucrose, sorbitol, K(2)SO(4), CaCl(2), and urea) on the secondary structure and thermodynamic properties upon unfolding and denaturation of staphylococcal nuclease (Snase). The data show that the different cosolvents have a profound effect on the denaturation pressure and the Gibbs free energy (DeltaG(o)) and volume (DeltaV(o) change of unfolding. Moreover, by analysis of the amide I' infrared bands, conformational changes of the protein upon unfolding in the different cosolvents have been determined. An increase, a reduction, or an independence of the volume change of unfolding is observed, depending on the type of cosolvent, which can at least in part be attributed to the formation of a different unfolded state structure of the protein. The data are compared with the corresponding thermodynamic values of DeltaV(o) for the temperature-induced unfolding process of Snase as obtained by pressure perturbation calorimetry, and significant differences are observed and discussed.

Characterization of the pressure-induced intermediate and unfolded state of red-shifted green fluorescent protein--a static and kinetic FTIR, UV/VIS and fluorescence spectroscopy study

The green fluorescence proteins (GFP) are widely used as reporters in molecular and cell biology. For their use it in high-pressure microbiology and biotechnology studies, their structural properties, thermodynamic parameters and stability diagrams have to be known. We investigated the pressure stability of the red-shifted green fluorescent protein (rsGFP) using Fourier-transform infrared spectroscopy, fluorescence and UV/Vis spectroscopy. We found that rsGFP does not unfold up to approximately 9kbar at room temperature. Its unique three-dimensional structure is held responsible for the high-pressure stability. At higher temperatures, its secondary structure collapses below 9kbar (e.g. the denaturation pressure at 58 degrees C is 7.8kbar). The analysis of the IR data shows that the pressure-denatured state contains more disordered structures at the expense of a decrease of intramolecular beta-sheets. As indicated by the large volume change of DeltaV degrees (u) approximately -250(+/-50)mlmol(-1) at 58 degrees C, this highly cooperative transition can be interpreted as a collapse of the beta-can structure of rsGFP. For comparison, the temperature-induced unfolding of rsGFP has also been studied. At high temperature (T(m)=78 degrees C), the unfolding resulted in the formation of an aggregated state. Contrary to the pressure-induced unfolding, the temperature-induced unfolding and aggregation of GFP is irreversible. From the FT-IR data, a tentative p,T-stability diagram for the secondary structure collapse of GFP has been obtained. Furthermore, changes in fluorescence and absorptivity were found which are not correlated to the secondary structural changes. The fluorescence and UV/Vis data indicate smaller conformational changes in the chromophore region at much lower pressures ( approximately 4kbar) which are probably accompanied by the penetration of water into the beta-can structure. In order to investigate also the kinetics of this initial step, pressure-jump relaxation experiments were carried out. The partial activation volumes observed indicate that the conformational changes in the chromophore region when passing the transition state are indeed rather small, thus leading to a comparably small volume change of -20 ml mol(-1) only. The use of the chromophore absorption and fluorescence band of rsGFP in using GFP as reporter for gene expression and other microbiological studies under high pressure conditions is thus limited to pressures of about 4kbar, which still exceeds the pressure range relevant for studies in vivo in micro-organisms, including piezophilic bacteria from deep-sea environments.

Quasiequilibrium unfolding thermodynamics of a small protein studied by molecular dynamics simulation with an explicit water model

The 124 independent molecular dynamics simulations are completed with total time of 196.8 ns. The calculated unfolding quasiequilibrium thermodynamics of G-IgG-binding domain B1 (GB1) shows the experimentally observed protein transitions: a coil to disordered globule transition, a disordered globule to molten globule transition, a molten globule to nativelike transition, and a nativelike to solidlike state transition. The first protein unfolding phase diagram has been constructed from molecular dynamics simulations with an explicit water model. The calculated melting temperature of GB1 agrees with early experiment. The results also agree with the recent experiment result in which GB1 has more than one intermediate.

High pressure induces the formation of aggregation-prone states of proteins under reducing conditions

The pressure stability of ribonuclease A and bovine pancreatic trypsin inhibitor has been investigated with Fourier transform infrared spectroscopy in the presence of the disulfide bond reducing agent 2-mercaptoethanol. The secondary structure of the reduced proteins at high pressure (1 GPa) is not significantly different from the pressure-induced conformation of the native form. Upon decompression under reducing conditions, amorphous aggregates are formed. Such aggregates are not formed upon decompression of the native proteins. Our data demonstrate that high pressure populates, and thus allows the potential characterization of highly aggregation-prone conformations. The relevance of these findings with regard to fibril formation is discussed and the possible role of conformational fluctuations of intermediates on the aggregation pathway is emphasized.

Pressure- and temperature-induced unfolding and aggregation of recombinant human interferon-gamma: a Fourier transform infrared spectroscopy study

The effect of hydrostatic pressure on the secondary structure of recombinant human interferon-gamma (rhIFN-gamma) and its biologically inactive truncated form rhIFN-Delta C15 has been studied using Fourier-transform IR (FTIR) spectroscopy. In situ observation of the pressure-induced changes using the diamond anvil cell shows that the alpha-helical structure is mainly transformed into disordered structure at high pressure. Increasing pressure also induces the formation of a gel. Addition of 0.5 M MgCl(2) significantly reduces the pressure stability. Releasing the pressure below 300 MPa results in the formation of intermolecular antiparallel beta-sheets, which is seldom observed. This suggests that the intermolecular beta-sheet of rhIFN-gamma is stabilized by electrostatic interactions that are disrupted at high pressure. For comparison we also studied the effect of temperature. Temperature-induced changes reflect extensive transformation of alpha-helical structure into intermolecular antiparallel beta-sheet, as is usually observed for most proteins.

High-pressure FTIR study of the stability of horseradish peroxidase. Effect of heme substitution, ligand binding, Ca++ removal, and reduction of the disulfide bonds

The pressure stability of horseradish peroxidase isoenzyme C and the identification of possible stabilizing factors are presented. The effect of heme substitution, removal of Ca(2+), binding of a small substrate molecule (benzohydroxamic acid), and reduction of the disulfide bonds on the pressure stability were investigated by FTIR spectroscopy. HRP was found to be extremely stable under high pressure with an unfolding midpoint of 12.0 +/- 0.1 kbar. While substitution of the heme for metal-free mesoporphyrin did not change the unfolding pressure, Ca(2+) removal and substrate binding reduced the midpoint of the unfolding by 2.0 and 1.2 kbar, respectively. The apoprotein showed a transition as high as 10.4 kbar. However, the amount of folded structure present at the atmospheric pressure was considerably lower than that in all the other forms of HRP. Reduction of the disulfide bonds led to the least pressure stable form, with an unfolding midpoint at 9.5 kbar. This, however, is still well above the average pressure stability of proteins. The high-pressure stability and the analysis of the pressure-induced spectral changes indicate that the protein has a rigid core, which is responsible for the high stability, while there are regions with less stability and more conformational mobility.

Insight into the factors influencing the backbone dynamics of three homologous proteins, dendrotoxins I and K, and BPTI: FTIR and time-resolved fluorescence investigations

Attenuated total reflection Fourier transform infrared (ATR-FTIR) spectroscopy, combined with hydrogen/deuterium exchange technique and time-resolved fluorescence spectroscopy, has been used to investigate the changes in structure and dynamics that underlie the thermodynamic stability differences observed for three closely homologous proteins: dendrotoxins I and K, and bovine pancreatic trypsin inhibitor (BPTI). The experiments were performed on proteins under their native state and a modified form, obtained by selective reduction of a disulfide bond at the surface of the molecule, increasing slightly the backbone flexibility without changing the average structure. The data confirmed the high local as well as global rigidity of BPTI. In protein K, the exchange process was slow during the first 2 h of exchange, presumably reflecting a compact three-dimensional conformation, and then increased rapidly, the internal amide protons of the beta-strands exchanging 10-fold faster than in BPTI or protein I. The most probable destabilizing element was identified as Pro32, in the core of the beta-sheet. Protein I was found to present a 10% more expanded volume than protein K or BPTI, and there is a possible correlation between the resulting increased flexibility of the molecule and the lower thermodynamic stability observed for this protein. Interestingly, the interior amide protons of the beta-sheet structure were found to be as protected against exchange in protein I as in BPTI, suggesting that, although globally more flexible than that of Toxin K or BPTI, the structure of Toxin I could be locally quite rigid. The structural factors suspected to be responsible for the differences in internal flexibility of the two toxins could play a significant role in determining their functional properties.

Temperature-pressure stability of green fluorescent protein: a Fourier transform infrared spectroscopy study

Green fluorescent protein (GFP) is widely used as a marker in molecular and cell biology. For its use in high-pressure microbiology experiments, its fluorescence under pressure was recently investigated. Changes in fluorescence with pressure were found. To find out whether these are related to structural changes, we investigated the pressure stability of wild-type GFP (wtGFP) and three of its red shift mutants (AFP, GFP(mut1), and GFP(mut2)) using Fourier transform infrared spectroscopy. For the wt GFP, GFP(mut1), and GFP(mut2) we found that up to 13-14 kbar the secondary structure remains intact, whereas AFP starts unfolding around 10 kbar. The 3-D structure is held responsible for this high-pressure stability. Previously observed changes in fluorescence at low pressure are rationalized in terms of the pressure-induced elastic effect. Above 6 kbar, loss of fluorescence is due to aggregation. Revisiting the temperature stability of GFP, we found that an intermediate state is populated along the unfolding pathway of wtGFP. At higher temperatures, the unfolding resulted in the formation of aggregates of wtGFP and its mutants.

Comparative Fourier transform infrared spectroscopy study of cold-, pressure-, and heat-induced unfolding and aggregation of myoglobin

We studied the cold unfolding of myoglobin with Fourier transform infrared spectroscopy and compared it with pressure and heat unfolding. Because protein aggregation is a phenomenon with medical as well as biotechnological implications, we were interested in both the structural changes as well as the aggregation behavior of the respective unfolded states. The cold- and pressure-induced unfolding both yield a partially unfolded state characterized by a persistent amount of secondary structure, in which a stable core of G and H helices is preserved. In this respect the cold- and pressure-unfolded states show a resemblance with an early folding intermediate of myoglobin. In contrast, the heat unfolding results in the formation of the infrared bands typical of intermolecular antiparallel beta-sheet aggregation. This implies a transformation of alpha-helix into intermolecular beta-sheet. H/2H-exchange data suggest that the helices are first unfolded and then form intermolecular beta-sheets. The pressure and cold unfolded states do not give rise to the intermolecular aggregation bands that are typical for the infrared spectra of many heat-unfolded proteins. This suggests that the pathways of the cold and pressure unfolding are substantially different from that of the heat unfolding. After return to ambient conditions the cold- or pressure-treated proteins adopt a partially refolded conformation. This aggregates at a lower temperature (32 degrees C) than the native state (74 degrees C).

Pressure-temperature phase diagrams of biomolecules

The pressure-temperature phase diagram of various biomolecules is reviewed. Special attention is focused on the elliptic phase diagram of proteins. The phenomenological thermodynamic theory describing this diagram explains the heat, cold and pressure denaturations in a unified picture. The limitations and possible developments of this theory are discussed as well. It is pointed out that a more complex diagram can be obtained when the intermolecular interactions are also taken into account. In this case metastable states appear on the pressure-temperature (p-T) diagram due to intermolecular interactions. Pressure-temperature phase diagrams of other biopolymers are also discussed. While the p-T diagrams of helix-coil transition of nucleic acids and of gel-liquid crystal transition of lipid bilayers are non-elliptical, those of gelatinization of starch and of phase separation of some synthetic polymers show an elliptic profile, similar to that of proteins. Finally, the p-T diagram of bacterial inactivation is shown to be elliptic. From the point of view of basic science, this fact shows that the key factor of inactivation should be the protein type, and from the viewpoint of practical applications, it serves as the theoretical basis of pressure treatment of biosystems.

High pressure simulations of biomolecules

Pressure is a thermodynamic variable which is particularly suitable for exploration of the properties of biological macromolecules. For proteins, in particular, denaturation induced by pressure is different from that induced by temperature or denaturants. The response of proteins to pressure changes can provide information on properties of their native and non-native states. This review focuses on molecular dynamics studies of the effect of pressure on detailed atomic models of proteins. It also reports on other theoretical approaches, such as Monte Carlo simulations, which have been used to study simplified models. Another purpose of this review is to try to point out potential future studies that may be both interesting and feasible, with constantly increasing computing power.

Temperature- and pressure-induced unfolding and refolding of ubiquitin: a static and kinetic Fourier transform infrared spectroscopy study

Temperature- and pressure-induced denaturation of the protein ubiquitin was investigated using FT-IR spectroscopy. On the basis of IR spectral parameters, different states are distinguished and a pressure/temperature-stability diagram of the protein has been determined. The evolution of the secondary structures with temperature illustrates that the band intensities of disordered structures decrease at the expense of the formation of intermolecular beta-sheets at 83 degrees C, pD 7, and ambient pressure, with the population of intramolecular beta-sheets and alpha-helices remaining essentially unchanged. At ambient temperature (T = 21 degrees C) and pD 7, ubiquitin denatures at 5.4 kbar. Contrary to other proteins studied so far, features of secondary structure of ubiquitin remain distinct at high pressure, suggesting that part of this small protein rearranges and does not unfold to disordered structures. The secondary structural changes during compression and decompression are fully reversible, and no aggregation occurs. With corresponding measurements of the pressure-induced denaturation of ubiquitin at different temperatures, a p/T-stability diagram of ubiquitin could be obtained. Furthermore, kinetic FT-IR measurements were carried out using the pressure-jump relaxation technique. The denaturation process is shown to occur on a time scale which is about twice as long as that of the renaturation process, and both processes are much slower than the unfolding-refolding kinetics observed at ambient pressure.

Pressure-induced transformation of alpha-helix to beta-sheet in the secondary structures of amyloid beta (1-40) peptide exacerbated by temperature

The effect of pressure on the conformational structure of amyloid beta (1-40) peptide (A beta(1-40)), exacerbated with or without temperature, was determined by Fourier transform infrared (FT-IR) microspectroscopy. The result indicates the shift of the maximum peak of amide I band of intact solid A beta(1-40) from 1655 cm(-1) (alpha-helix) to 1647-1643 cm(-1) (random coil) with the increase of the mechanical pressure. A new peak at 1634 cm(-1) assigned to beta-antiparallel sheet structure was also evident. Furthermore, the peak at 1540 cm(- 1) also shifted to 1527 (1529) cm(-1) in amide II band. The former was assigned to the combination of alpha-helix and random coil structures, and the latter was due to beta-sheet structure. Changes in the composition of each component in the deconvoluted and curve-fitted amide I band of the compressed A beta(1-40) samples were obtained from 33% to 22% for alpha-helix/random coil structures and from 47% to 57% for beta-sheet structure with the increase of pressure, respectively. This demonstrates that pressure might induce the conformational transition from alpha-helix to random coil and to beta- sheet structure. The structural transformation of the compressed A beta(1-40) samples was synergistically influenced by the combined effects of pressure and temperature. The thermal-induced formation of beta-sheet structure was significantly dependent on the pressures applied. The smaller the pressure applied the faster the beta-sheet structure transformed. The thermal-dependent transition temperatures of solid A beta(1-40) prepared by different pressures were near 55-60 degrees C.

The enzyme horseradish peroxidase is less compressible at higher pressures

Fluorescence line-narrowing (FLN) spectroscopy at 10 K was used to study the effect of high pressure through the prosthetic group in horseradish peroxidase (HRP), which was Mg-mesoporphyrin (MgMP) replacing the heme of the enzyme. The same measurement was performed on MgMP in a solid-state amorphous organic matrix, dimethyl sulfoxide (DMSO). Series of FLN spectra were registered to determine the (0, 0) band shape through the inhomogeneous distribution function (IDF). In the range of 0-2 GPa a red-shift of the IDF was determined, and yielded the isothermal compressibility of MgMP-HRP as 0.066 GPa(-1), which is significantly smaller than that found earlier as 0.106 GPa(-1) by fine-tuning the pressure in the range up to 1.1 MPa. The vibrational frequencies also shifted with pressure increase, as expected. The compressibility in the DMSO matrix was smaller, 0.042 GPa(-1), both when the pressure was applied at room temperature before cooling to 10 K, or at 10 K. At 200 K or above, the bimodal (0, 0) band shape in DMSO showed a population conversion under pressure that was not observed at or below 150 K. A significant atomic rearrangement was estimated from the volume change, 3.3 +/- 0.7 cm(3)/mol upon conversion. The compressibility in proteins and in amorphous solids seems not to significantly depend on the temperature and in the protein it decreases toward higher pressures.

Molecular dynamics simulations of pressure effects on hydrophobic interactions

We report results on the pressure effects on hydrophobic interactions obtained from molecular dynamics simulations of aqueous solutions of methanes in water. A wide range of pressures that is relevant to pressure denaturation of proteins is investigated. The characteristic features of water-mediated interactions between hydrophobic solutes are found to be pressure-dependent. In particular, with increasing pressure we find that (1) the solvent-separated configurations in the solute-solute potential of mean force (PMF) are stabilized with respect to the contact configurations; (2) the desolvation barrier increases monotonically with respect to both contact and solvent-separated configurations; (3) the locations of the minima and the barrier move toward shorter separations; and (4) pressure effects are considerably amplified for larger hydrophobic solutes. Together, these observations lend strong support to the picture of the pressure denaturation process proposed previously by Hummer et al. (Proc. Natl. Acad. Sci. U.S.A. 1998, 95, 1552): with increasing pressure, the transfer of water into protein interior becomes key to the pressure denaturation process, leading to the dissociation of close hydrophobic contacts and subsequent swelling of the hydrophobic protein interior through insertions of water molecules. The pressure dependence of the PMF between larger hydrophobic solutes shows that pressure effects on the interaction between hydrophobic amino acids may be considerably amplified compared to those on the methane-methane PMF.

Horseradish peroxidase monitored by infrared spectroscopy: effect of temperature, substrate and calcium

Horseradish peroxidase was examined as a function of Ca and substrate binding using infrared spectroscopy in the temperature range of 10-300 K. The Ca complex could be identified by the carboxylate stretches. The amide peak positions indicate that the protein remains stable from room temperature to 10 K. Shifts in these peaks are consistent with increased hydrogen bonding as temperature decreases, but the protein conformation is maintained at cryogenic temperatures. The substrate, benzohydroxamic acid, produced no detectable change in the infrared spectrum, consistent with X-ray crystallography results. With removal of Ca, the protein maintained its overall helicity.

Effect of pressure on the tertiary structure and dynamics of folded basic pancreatic trypsin inhibitor

The on-line high-pressure cell NMR technique was used to study pressure-induced changes in the tertiary structure and dynamics of a globular protein, basic pancreatic trypsin inhibitor (BPTI). Practically all the proton signals of BPTI were observed with (1)H two-dimensional NMR spectroscopy at 750 MHz at variable pressure between 1 and 2000 bar. Chemical shifts, nuclear Overhauser effect (NOE), and line shapes were used to analyze conformational and dynamic changes of the protein as functions of pressure. Linear, reversible, but nonuniform pressure-induced chemical shift changes of practically all the C(alpha) protons and side chain protons showed that the entire secondary and tertiary structures are altered by pressure within the folded ensemble of BPTI. The high field shift tendency of most side chain proton signals and the increase in NOE intensities of some specific side chain protons indicated a site-specific compaction of the tertiary structure. Pressure dependence of ring flip rates was deduced from resonance line shapes of the slices of the two-dimensional NMR spectrum for ring proton signals of Tyr-35 and Phe-45. The rates of the flip-flop motions were considerably reduced at high pressure, from which activation volumes were determined to be 85 +/- 20 A(3) (or 51.2 ml/mol) and 46 +/- 9 A(3) (or 27.7 ml/mol) for Tyr-35 and Phe-45, respectively, at 57 degrees C. The present experiments confirm that pressure affects the entire secondary and tertiary structures of a globular protein with specific compaction of a core, leading to quite significant changes in slow internal dynamics of a globular protein.

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.

Pressure effect on the temperature-induced unfolding and tendency to aggregate of myoglobin

This work demonstrates that pressure-induced partially unfolded states play a very important role in the aggregation of proteins. The high-pressure unfolding of horse heart metmyoglobin results in an intermediate form that shows a strong tendency to aggregate after pressure release. These aggregates are similar to those that are usually observed upon temperature denaturation. Infrared spectra in the amide I region indicate the formation of an intermolecular antiparallel beta-sheet stabilized by hydrogen bonding. The formation of the aggregates is temperature-dependent. Below 30 degrees C, no aggregation is taking place as seen from the infrared spectra. At 45 and 60 degrees C, two types of aggregates are formed: one that can be dissociated by moderate pressures and one that is pressure-insensitive. When precompressed at 5 degrees C, temperature-induced aggregation takes place at lower temperature (38 degrees C) than without pressure pretreatment (74 degrees C).

Pressure-denatured state of Escherichia coli ribonuclease HI as monitored by Fourier transform infrared and NMR spectroscopy

Pressure denaturation of Escherichia coli ribonuclease HI (RNase HI) was studied by Fourier transform infrared (FTIR) and two-dimensional NMR spectroscopy at pD* 3.0 and 25 degrees C. A reversible transition in the pressure range of 0.1-1090 MPa was observed with second-derivative FTIR experiments. A cooperative and gradual denaturation, involving both the secondary and tertiary structures, was observed between 240 and 450 MPa. The two peaks at 1629 and 1652 cm(-1), due to beta-strands and alpha-helices, respectively, did not fully disappear after the denaturation, and are different from the spectra of the random coil peptides. The hydrogen-deuterium exchange rates of the individual backbone amide protons were determined by heteronuclear NMR combined with the pressure-jump technique at 500, 650, and 850 MPa. Although most of the amides protected in the native structure are also highly protected in the pressure-denatured state, the rate constants (0.048 +/- 0.007 min(-1)) for the amide protons at 500 MPa are similar regardless of their locations, which is an indication of the EX1 mechanism of hydrogen-deuterium exchange. The pressure-denatured state of RNase HI at 500 MPa represents a novel denatured state, which is different from a typical molten globule state at atmospheric pressure (0.1 MPa), from the viewpoint of the homogeneous rate constants. The observations at 650 MPa are essentially the same as those at 500 MPa. However, at 850 MPa, the amide exchange rates for the highly hydrophobic C-terminal half of alpha-helix I are significantly slower than those for the other part of the protein, which can be interpreted as a hydrophobic collapse centered at the C-terminal half of alpha-helix I.

Protein structure and dynamics at high pressure

The effect of pressure on the structure and dynamics of proteins is discussed in the framework of the pressure-temperature stability phase diagram. The elastic (reversible) properties, thermal expansion, compressibility and heat capacity, are correlated with the entropy, volume, and the coupling between entropy and volume fluctuations respectively. The experimental approaches that can be used to measure these quantities are reviewed. The plastic (conformational) changes reflect the changes in these properties in the cold, pressure and heat denaturation.

Structural characterization of the pressure-denatured state and unfolding/refolding kinetics of staphylococcal nuclease by synchrotron small-angle X-ray scattering and Fourier-transform infrared spectroscopy

The pressure-induced unfolding of wild-type staphylococcal nuclease (Snase WT) was studied using synchrotron X-ray small-angle scattering (SAXS) and Fourier-transform infrared (FT-IR) spectroscopy, which monitor changes in the tertiary and secondary structural properties of the protein upon pressurization. The experimental results reveal that application of high-pressure up to 3 kbar leads to an approximate twofold increase of the radius of gyration Rg of the native protein (Rg approximately 17 A) and a large broadening of the pair-distance-distribution function, indicating a transition from a globular to an ellipsoidal or extended chain structure. Analysis of the FT-IR amide I' spectral components reveals that the pressure-induced denaturation process sets in at 1.5 kbar at 25 degrees C and is accompanied by an increase in disordered and turn structures while the content of beta-sheets and alpha-helices drastically decreases. The pressure-induced denatured state above 3 kbar retains nonetheless some degree of beta-like secondary structure and the molecule cannot be described as a fully extended random coil. Temperature-induced denaturation involves a further unfolding of the protein molecule which is indicated by a larger Rg value and significantly lower fractional intensities of IR-bands associated with secondary-structure elements. In addition, we have carried out pressure-jump kinetics studies of the secondary-structural evolution and the degree of compactness in the folding/unfolding reactions of Snase. The effect of pressure on the kinetics arises from a larger positive activation volume for folding than for unfolding, and leads to a significant slowing down of the folding rate with increasing pressure. Moreover, the system becomes two-state under pressure. These properties make it ideal for probing multiple order parameters in order to compare the kinetics of changes in secondary structure by pressure-jump FT-IR and chain collapse by pressure-jump SAXS. After a pressure jump from 1 bar to 2.4 kbar at 20 degrees C, the radius of gyration increases in a first-order manner from 17 A to 22.4 A over a timescale of approximately 30 minutes. The increase in Rg value is caused by the formation of an extended (ellipsoidal) structure as indicated by the corresponding pair-distance-distribution function. Pressure-jump FT-IR studies reveal that the reversible first order changes in beta-sheet, alpha-helical and random structure occur on the same slow timescale as that observed for the scattering curves and for fluorescence. These studies indicate that the changes in secondary structure and chain compactness in the folding/unfolding reactions of Snase are probably dependent upon the same rate-limiting step as changes in tertiary structure.

Extreme heat- and pressure-resistant 7-kDa protein P2 from the archaeon Sulfolobus solfataricus is dramatically destabilized by a single-point amino acid substitution

This study reports the characterization of the recombinant 7-kDa protein P2 from Sulfolobus solfataricus and the mutants F31A and F31Y with respect to temperature and pressure stability. As observed in the NMR, FTIR, and CD spectra, wild-type protein and mutants showed substantially similar structures under ambient conditions. However, midpoint transition temperatures of the denaturation process were 361, 334, and 347 K for wild type, F31A, and F31Y mutants, respectively: thus, alanine substitution of phenylalanine destabilized the protein by as much as 27 K. Midpoint transition pressures for wild type and F31Y mutant could not be accurately determined because they lay either beyond (wild type) or close to (F31Y) 14 kbar, a pressure at which water undergoes a phase transition. However, a midpoint transition pressure of 4 kbar could be determined for the F31A mutant, implying a shift in transition of at least 10 kbar. The pressure-induced denaturation was fully reversible; in contrast, thermal denaturation of wild type and mutants was only partially reversible. To our knowledge, both the pressure resistance of protein P2 and the dramatic pressure and temperature destabilization of the F31A mutant are unprecedented. These properties may be largely accounted for by the role of an aromatic cluster where Phe31 is found at the core, because interactions among aromatics are believed to be almost pressure insensitive; furthermore, the alanine substitution of phenylalanine should create a cavity with increased compressibility and flexibility, which also involves an impaired pressure and temperature resistance.

A prediction of DPP IV/CD26 domain structure from a physico-chemical investigation of dipeptidyl peptidase IV (CD26) from human seminal plasma

Human DPP IV, isolated from seminal plasma by means of immobilised adenosine deaminase, occurs in different forms which are distinguishable by net charge and native molecular weight. Charge differences arise primarily from different degrees of glycosylation containing various amounts of sialic acid. The majority of DPP IV isolated from total seminal plasma consists of the extracellular part of the protein starting at Gly-31. It is a very stable protein resisting high concentrations of denaturant. Unfolding experiments under reducing conditions are indicative of the existence of at least two domains which function independently. One of these domains is highly stabilised by disulfide bonds. Disruption of the disulfide bonds does not affect the activity, the dimeric state nor the adenosine deaminase binding properties of the protein but renders it more susceptible to proteolysis. The low-angle X-ray scattering spectrum is consistent with a model for a protein containing two subunits, each composed of three domains linked by flexible regions with low average mass. The secondary structure composition, determined by FTIR spectrometry, indicates that 45% of the protein consists of beta-sheets, which is higher than expected from computed secondary structure predictions. Our results provide compelling experimental evidence for the three-domain structure of the extracellular part of DPP IV.

Molecular mechanisms of pressure induced conformational changes in BPTI

We have performed a 800 ps molecular dynamics simulation of bovine pancreatic trypsin inhibitor (BPTI) in water coupled to a pressure bath at 1, 10,000, 15,000, and 20,000 bar. The simulation reproduces quite well the experimental behavior of the protein under high pressure. The protein keeps its globular form, but adopts a different conformation with a very small reduction in volume. Some residues in the hydrophobic core become exposed to water and a large part of the secondary structure of the protein, (60% of the sheet structure and 40% of the helical structure) is denatured between 10 and 15 kbar. This is in good agreement with experimental data (Goossens, K., et al. Eur. J. Biochem, 236:254-262, 1996) that show denaturation of BPTI between 8 and 14 kbar. A further increase of the pressure results in a freezing of the protein as deduced from the large decrease of the mobility of the residues. During the simulation, the normal structure of water changes from an ice Ih-like to an ice VI-like structure, while keeping the liquid state. The driving force of the high pressure induced conformational transition seems be the higher compressibility of the water compared with the protein. This produces a change in the solvent properties and leads to penetration of the solvent into the hydrophobic core.