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Leavitt S, Freire E. Direct measurement of protein binding energetics by isothermal titration calorimetry. Curr Opin Struct Biol 2001; 11:560-6. [PMID: 11785756 DOI: 10.1016/s0959-440x(00)00248-7] [Citation(s) in RCA: 483] [Impact Index Per Article: 20.1] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 10/18/2022]
Abstract
Of all the techniques that are currently available to measure binding, isothermal titration calorimetry is the only one capable of measuring not only the magnitude of the binding affinity but also the magnitude of the two thermodynamic terms that define the binding affinity: the enthalpy (AH) and entropy (AS) changes. Recent advances in instrumentation have facilitated the development of experimental designs that permit the direct measurement of arbitrarily high binding affinities, the coupling of binding to protonation/deprotonation processes and the analysis of binding thermodynamics in terms of structural parameters. Because isothermal titration calorimetry has the capability to measure different energetic contributions to the binding affinity, it provides a unique bridge between computational and experimental analysis. As such, it is increasingly becoming an essential tool in molecular design.
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Review |
24 |
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Murphy KP, Freire E. Thermodynamics of structural stability and cooperative folding behavior in proteins. ADVANCES IN PROTEIN CHEMISTRY 1992; 43:313-61. [PMID: 1442323 DOI: 10.1016/s0065-3233(08)60556-2] [Citation(s) in RCA: 439] [Impact Index Per Article: 13.3] [Reference Citation Analysis] [MESH Headings] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 12/27/2022]
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Review |
33 |
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Abstract
The heat capacity plays a major role in the determination of the energetics of protein folding and molecular recognition. As such, a better understanding of this thermodynamic parameter and its structural origin will provide new insights for the development of better molecular design strategies. In this paper we have analyzed the absolute heat capacity of proteins in different conformations. The results of these studies indicate that three major terms account for the absolute heat capacity of a protein: (1) one term that depends only on the primary or covalent structure of a protein and contains contributions from vibrational frequencies arising from the stretching and bending modes of each valence bond and internal rotations; (2) a term that contains the contributions of noncovalent interactions arising from secondary and tertiary structure; and (3) a term that contains the contributions of hydration. For a typical globular protein in solution the bulk of the heat capacity at 25 degrees C is given by the covalent structure term (close to 85% of the total). The hydration term contributes about 15 and 40% to the total heat capacity of the native and unfolded states, respectively. The contribution of non-covalent structure to the total heat capacity of the native state is positive but very small and does not amount to more than 3% at 25 degrees C. The change in heat capacity upon unfolding is primarily given by the increase in the hydration term (about 95%) and to a much lesser extent by the loss of noncovalent interactions (up to approximately 5%).(ABSTRACT TRUNCATED AT 250 WORDS)
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Comparative Study |
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Hilser VJ, Freire E. Structure-based calculation of the equilibrium folding pathway of proteins. Correlation with hydrogen exchange protection factors. J Mol Biol 1996; 262:756-72. [PMID: 8876652 DOI: 10.1006/jmbi.1996.0550] [Citation(s) in RCA: 197] [Impact Index Per Article: 6.8] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 02/02/2023]
Abstract
A new statistical thermodynamic formalism has been developed in order to describe the equilibrium folding pathway of proteins. The resulting formalism allows calculation of the probabilities that individual amino acid residues will be in a native or native-like conformation for any given degree of folding of the protein molecule. The residue probabilities are defined by the probability distribution of conformational states and can be used to calculate experimental quantities like native-state, hydrogen exchange protection factors. A combinatorial algorithm aimed at generating a large ensemble of conformational states (10(4) to 10(6)) using the native structure as a template has been developed. The Gibbs energy and corresponding probability of each conformational state is estimated by using a previously developed structural parametrization of the energetics. The approach has been applied to five different proteins: hen egg-white lysozyme, equine lysozyme, bovine pancreatic trypsin inhibitor, staphylococcal nuclease and turkey ovomucoid third domain. The validity of the approach has been tested by comparing predicted and experimental hydrogen exchange protection factors. It is shown that for the above proteins 76%, 73%, 74%, 78% and 81% of all observed protection factors are predicted correctly. Furthermore, on average, the magnitude of the predicted protection factors, expressed as apparent free energies per residue deviate less than 1 kcal/mol from those obtained experimentally. These results represent the first attempt at predicting both the location and magnitude of hydrogen exchange protection factors from the high-resolution structure of a protein. The good agreement between experimental and predicted values has permitted a close examination of the nature of the equilibrium folding intermediates existing under conditions of maximal stability of the native state.
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Gómez J, Freire E. Thermodynamic mapping of the inhibitor site of the aspartic protease endothiapepsin. J Mol Biol 1995; 252:337-50. [PMID: 7563055 DOI: 10.1006/jmbi.1995.0501] [Citation(s) in RCA: 193] [Impact Index Per Article: 6.4] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/26/2023]
Abstract
The discovery that the protease from the human immunodeficiency virus (HIV) belongs to the aspartic protease family has generated renewed interest in this class of proteins. In this paper, the interactions of endothiapepsin, an aspartic proteinase from the fungus Endothia parasitica, with the inhibitor pepstatin A have been studied by high-sensitivity calorimetric techniques. These experiments have permitted a complete characterization of the temperature and pH-dependence of the binding energetics. The binding reaction is characterized by negative intrinsic binding enthalpy and negative heat capacity changes. The association constant is maximal at low pH (2 x 10(9) M-1 at pH 3) but decreases upon increasing pH (8.1 x 10(6) M-1 at pH 7). The binding of the inhibitor is coupled to the protonation of one of the aspartic moieties in the Asp dyad of the catalytic site of the protein. This phenomenon is responsible for the decrease in the apparent affinity of the inhibitor for the enzyme upon increasing pH. The experimental results presented here indicate that the binding of the inhibitor is favored both enthalpically and entropically. While the favorable enthalpic contribution is intuitively expected, the favorable entropic contribution is due to the large gain in solvent-related entropy associated with the burial of a large hydrophobic surface, that overcompensates the loss in conformational and translational/rotational degrees of freedom upon complex formation. The characteristics of the molecular recognition process have been evaluated by means of structure-based thermodynamic analysis. Three regions in the protein contribute significantly to the free energy of binding: the residues surrounding the Asp dyad (Asp32 in the N-terminal lobe and Asp215 in the C-terminal domain) and the flap region (Ile73 to Asp77). In addition, the rearrangement of residues that are not in immediate contact with the inhibitor provides close to 40% of the protease contribution to the binding free energy. On the other hand, the two statine residues provide more than half of the inhibitor contributions to the total free energy of binding. It is demonstrated that a previously developed empirical structural parametrization of the thermodynamic parameters that define the Gibbs energy, accurately accounts for the binding energetics and its temperature and pH-dependence.
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Comparative Study |
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Freire E, van Osdol WW, Mayorga OL, Sanchez-Ruiz JM. Calorimetrically determined dynamics of complex unfolding transitions in proteins. ANNUAL REVIEW OF BIOPHYSICS AND BIOPHYSICAL CHEMISTRY 1990; 19:159-88. [PMID: 2194474 DOI: 10.1146/annurev.bb.19.060190.001111] [Citation(s) in RCA: 183] [Impact Index Per Article: 5.2] [Reference Citation Analysis] [MESH Headings] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 12/30/2022]
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Review |
35 |
183 |
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Lee KH, Xie D, Freire E, Amzel LM. Estimation of changes in side chain configurational entropy in binding and folding: general methods and application to helix formation. Proteins 1994; 20:68-84. [PMID: 7824524 DOI: 10.1002/prot.340200108] [Citation(s) in RCA: 180] [Impact Index Per Article: 5.8] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/27/2023]
Abstract
Theoretical estimations of changes in side chain configurational entropy are essential for understanding the different contributions to the overall thermodynamic behavior of important biological processes like folding and binding. The configurational entropy of any given side chain in any particular protein can be evaluated from the complete energy profile of the side chain. Calculations of the energy profiles can be performed using the side chain single bond dihedrals as the only independent variables as long as the structures at each value of the dihedrals are allowed to relax through small changes in the valence bond angles. The probabilities of different side chain conformers obtained from these energy profiles are very similar to the conformer populations obtained by analysis of side chain preferences in the proteins of the Protein Data Bank. Also, side chain conformational entropies obtained from the energy profiles agree extremely well with those obtained from the Protein Data Bank conformer populations. Changes in side chain configurational entropy in binding and folding can be computed as differences in conformational entropy because, in most cases, the frequency of the rotational oscillation around the energy minimum of any given conformer does not appear to change significantly in the reactions. Changes of side chain conformational entropy calculated in this way were compared with experimental values. The only available experimental data--the effect of side chain substitution on the stability of alpha-helices--were used for this comparison. The experimental values were corrected to subtract the solvent contributions. This comparison yields an excellent agreement between calculated and experimental values, validating not only the theoretical estimates but also the separability of the entropic contributions into configurational terms and solvation related terms.
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Hilser VJ, Dowdy D, Oas TG, Freire E. The structural distribution of cooperative interactions in proteins: analysis of the native state ensemble. Proc Natl Acad Sci U S A 1998; 95:9903-8. [PMID: 9707573 PMCID: PMC21434 DOI: 10.1073/pnas.95.17.9903] [Citation(s) in RCA: 172] [Impact Index Per Article: 6.4] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/18/2022] Open
Abstract
Cooperative interactions link the behavior of different amino acid residues within a protein molecule. As a result, the effects of chemical or physical perturbations to any given residue are propagated to other residues by an intricate network of interactions. Very often, amino acids "sense" the effects of perturbations occurring at very distant locations in the protein molecule. In these studies, we have investigated by computer simulation the structural distribution of those interactions. We show here that cooperative interactions are not intrinsically bi-directional and that different residues play different roles within the intricate network of interactions existing in a protein. The effect of a perturbation to residue j on residue k is not necessarily equal to the effect of the same perturbation to residue k on residue j. In this paper, we introduce a computer algorithm aimed at mapping the network of cooperative interactions within a protein. This algorithm exhaustively performs single site thermodynamic mutations to each residue in the protein and examines the effects of those mutations on the distribution of conformational states. The algorithm has been applied to three different proteins (lambda repressor fragment 6-85, chymotrypsin inhibitor 2, and barnase). This algorithm accounts well for the observed behavior of these proteins.
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27 |
172 |
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Lichtenberg D, Freire E, Schmidt CF, Barenholz Y, Felgner PL, Thompson TE. Effect of surface curvature on stability, thermodynamic behavior, and osmotic activity of dipalmitoylphosphatidylcholine single lamellar vesicles. Biochemistry 1981; 20:3462-7. [PMID: 6894860 DOI: 10.1021/bi00515a024] [Citation(s) in RCA: 164] [Impact Index Per Article: 3.7] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/22/2023]
Abstract
The size and surface curvature dependence of the properties and stability of single lamellar vesicles have been investigated by using a variety of physicochemical techniques. Dipalmitoylphosphatidylcholine single lamellar vesicles of sizes ranging between 200 and 900 A in diameter have been prepared by the French press method and characterized with respect to their size distribution, stability, and thermotropic behavior by negative stain electron microscopy, molecular sieve chromatography, nuclear magnetic resonance spectroscopy, and differential scanning calorimetry. Vesicles with a diameter smaller than 400 A are unstable below their transition temperature and fuse spontaneously to form larger single lamellar vesicles. Correlation analysis of experimentally obtained size distributions and calorimetric phase transitions profiles allowed estimation of the size dependence of the transition temperature. The phase transition temperature depends on the vesicle size in a sigmoidal fashion. Throughout the entire 200-700 A diamter range, the phase transition parameters are sensitive to size; however, the size dependence is especially pronounced around 400 A in diameter. The anomalous size dependence of the transition temperature for vesicles smaller than 400 A in diameter has been attributed to a decrease in the effective bilayer curvature due to packing rearrangements of the lipid molecules. Changes in the fractional degree of self-quenching of trapped 6-carboxyfluorescein induced by osmotic stress indicate that large single lamellar vesicles are not spherical under isoosmotic conditions. These vesicles are relatively flexible and can sustain almost a 2-fold increase in their internal aqueous volume without any leakage of the internal content.
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44 |
164 |
10
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Privalov G, Kavina V, Freire E, Privalov PL. Precise scanning calorimeter for studying thermal properties of biological macromolecules in dilute solution. Anal Biochem 1995; 232:79-85. [PMID: 8600837 DOI: 10.1006/abio.1995.9957] [Citation(s) in RCA: 159] [Impact Index Per Article: 5.3] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/31/2023]
Abstract
A precise scanning calorimeter for studying the heat capacity of liquids in a broad temperature range has been developed. By its design and capabilities this calorimeter is the first of a new generation for this type of instrument. This new scanning calorimeter operates differentially, is equipped with a pair of gold capillary cells and semiconductor sensors, and is able to scan up and down in temperature at user-selected rates. This instrument is completely operated by an integrated computer which also provides a full thermodynamic analysis of the results. Its construction does not involve the use of organic compounds, thus eliminating a source of baseline noise that has affected previous calorimeters. The operational temperature range of the instrument can be varied between 0 and 120 degrees C. The gold capillary cells (operational volume 0.8 ml) minimize temperature gradients in the heated/cooled liquid sample and permit easy washing and reloading without air bubbles. These features are crucial for the accuracy of difference heat capacity measurements and determination of the absolute value of the partial heat capacity of solute molecules. The measurements can be performed under an excess constant pressure (up to 3 atm) to prevent formation of gas bubbles and boiling of aqueous solutions above 100 degrees C. The noise level of the recorded heating/cooling power difference is below 50 x 10(-9) W (i.e., below 10 ncal/s) with a response half-time of 5 s. The reproducibility of the baseline without refilling the capillary cells is on the order of 0.5 x 10(-6) W. Reproducibility of the baseline upon refilling the cell is of the same order of magnitude. This provides an accuracy in difference heat capacity determination on the order of 10 mu cal/degrees Kml at a heating rate of 1 degree K/min.
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159 |
11
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Murphy KP, Xie D, Thompson KS, Amzel LM, Freire E. Entropy in biological binding processes: estimation of translational entropy loss. Proteins 1994; 18:63-7. [PMID: 8146122 DOI: 10.1002/prot.340180108] [Citation(s) in RCA: 153] [Impact Index Per Article: 4.9] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/29/2023]
Abstract
The loss of translational degrees of freedom makes an important, unfavorable contribution to the free energy of binding. Examination of experimental values suggest that calculation of this entropy using the Sackur-Tetrode equation produces largely overestimated values. Better agreement is obtained using the cratic entropy. Theoretical considerations suggest that the volumes available for the movement of a ligand in solution and in a complex are rather similar, suggesting also that the cratic entropy provides the best estimate of the loss of translational entropy.
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31 |
153 |
12
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Freire E. The propagation of binding interactions to remote sites in proteins: analysis of the binding of the monoclonal antibody D1.3 to lysozyme. Proc Natl Acad Sci U S A 1999; 96:10118-22. [PMID: 10468572 PMCID: PMC17852 DOI: 10.1073/pnas.96.18.10118] [Citation(s) in RCA: 149] [Impact Index Per Article: 5.7] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/18/2022] Open
Abstract
The interaction of a ligand with a protein occurs at a local site (the binding site) and involves only a few residues; however, the effects of that interaction are often propagated to remote locations. The chain of events initiated by binding provides the basis for fundamental biological phenomena such as allosterism, signal transduction, and structural-stability modification. In this paper, a structure-based statistical thermodynamic approach is presented and used to predict the propagation of the stabilization effects triggered by the binding of the monoclonal antibody D1.3 to hen egg white lysozyme. Previously, Williams et al. [Williams, D. C., Benjamin, D. C., Poljak, R. J. & Rule, G. S. (1996) J. Mol. Biol. 257, 866-876] showed that the binding of this antibody affects the stability of hen egg white lysozyme and that the binding effects propagate to a selected number of residues at remote locations from the binding epitope. In this paper, we show that this phenomenon can be predicted from structure. The formalism presented here permits the identification of the structural path followed by cooperative interactions that originate at the binding site. It is shown that an important condition for the propagation of binding effects to distal regions is the presence of a significant fraction of residues with low structural stability in the uncomplexed binding site. A survey of protein structures indicates that many binding sites have a dual character and are defined by regions of high and low structural stabilities. The low-stability regions might be involved in the transmission of binding information to other regions in the protein.
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26 |
149 |
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Schön A, Freire E. Thermodynamics of intersubunit interactions in cholera toxin upon binding to the oligosaccharide portion of its cell surface receptor, ganglioside GM1. Biochemistry 1989; 28:5019-24. [PMID: 2765522 DOI: 10.1021/bi00438a017] [Citation(s) in RCA: 141] [Impact Index Per Article: 3.9] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/02/2023]
Abstract
The binding and the energetics of the interaction of cholera toxin with the oligosaccharide portion of ganglioside GM1 (oligo-GM1), the toxin cell surface receptor, have been studied by high-sensitivity isothermal titration calorimetry and differential scanning calorimetry. Previously, we have shown that the association of cholera toxin to ganglioside GM1 enhances the cooperative interactions between subunits in the B-subunit pentamer [Goins, B., & Freire, E. (1988) Biochemistry 27, 2046-2052]. New experiments presented in this paper reveal that the oligosaccharide portion of the receptor is by itself able to enhance the intersubunit cooperative interactions within the B pentamer. This effect is seen in the protein unfolding transition as a shift from independent unfolding of the B promoters toward a cooperative unfolding. To identify the origin of this effect, the binding of cholera toxin to oligo-GM1 has been measured calorimetrically under isothermal conditions. The binding curve at 37 degrees C is sigmoidal, indicating cooperative binding. The binding data can be described in terms of a nearest-neighbor cooperative interaction binding model. In terms of this model, the association of a oligo-GM1 molecule to a B protomer affects the association to adjacent B promoters within the pentameric ring. The measured intrinsic binding enthalpy per protomer is -22 kcal/mol and the cooperative interaction enthalpy -11 kcal/mol. The intrinsic binding constant determined calorimetrically is 1.05 x 10(6) M-1 at 37 degrees C and the cooperative Gibbs free energy equal to -850 cal/mol.(ABSTRACT TRUNCATED AT 250 WORDS)
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141 |
14
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Thompson KS, Vinson CR, Freire E. Thermodynamic characterization of the structural stability of the coiled-coil region of the bZIP transcription factor GCN4. Biochemistry 1993; 32:5491-6. [PMID: 8504069 DOI: 10.1021/bi00072a001] [Citation(s) in RCA: 140] [Impact Index Per Article: 4.4] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/31/2023]
Abstract
The thermal stability of a 56 amino acid fragment of GCN4 has been studied by high-sensitivity differential scanning calorimetry and circular dichroism spectroscopy. This fragment contains the leucine zipper and part of the basic region. The thermal unfolding of GCN4-56 is a reversible process and can be well represented by a reaction of the form N2<-->2U, indicating that the unfolding of the leucine zipper is a two-state process in which the helices are only stable when they are in the coiled-coil conformation. As expected, the transition temperature is concentration dependent. At pH 7.06 and a protein concentration of 5 x 10(-4) M the transition temperature is close to 70 degrees C while at 5 x 10(-6) M it is close to 50 degrees C. The enthalpy change for unfolding is 31.5 kcal mol-1 at 70 degrees C. Since the isolated helices are unstable, interactions at the interface between the two helices play a key role in the stabilization of the native dimer. These interactions primarily involve the burial of apolar surface from the solvent (hydrophobic effect) and electrostatic interactions. Structural thermodynamic calculations have permitted a dissection of the magnitude of the various contributions to the total Gibbs free energy of stabilization.
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Abstract
The most common strategy in the development of HIV-1 protease inhibitors has been the design of high affinity transition state analogs that effectively compete with natural substrates for the active site. A second approach has been the development of compounds that inactivate the protease by destabilizing its quaternary or tertiary structure. A successful optimization of these strategies requires an accurate knowledge of the energetics of structural stabilization and binding, and the identification of those regions in the protease molecule that are critical to stability and function. Here the energetics of stabilization of the HIV-1 protease has been measured for the first time by high sensitivity differential scanning calorimetry. These studies have permitted the evaluation of the different components of the Gibbs energy of stabilization (the enthalpy, entropy and heat capacity changes). The stability of the protease is pH-dependent and due to its dimeric nature is also concentration-dependent. At pH 3.4 the Gibbs energy of stabilization is close to 10 kcal/mol at 25 degreesC, consistent with a dissociation constant of 5x10(-8) M. The stability of the protease increases at higher pH values. At pH 5, the Gibbs energy of stabilization is 14.5 kcal/mol at 25 degreesC, consistent with a dissociation constant of 2.3x10(-11) M. The pH dependence of the Gibbs energy of stabilization indicates that between pH 3.4 and pH 5 an average of 3-4 ionizable groups per dimer become protonated upon unfolding. A structure-based thermodynamic analysis of the protease molecule indicates that most of the Gibbs energy of stabilization is provided by the dimerization interface and that the isolated subunits are intrinsically unstable. The Gibbs energy, however, is not uniformly distributed along the dimerization interface. The dimer interface is characterized by the presence of clusters of residues (hot spots) that contribute significantly and other regions that contribute very little to subunit association. At the dimerization interface, residues located at the carboxy and amino termini contribute close to 75% of the total Gibbs energy (Cys95, Thr96, Leu97, Asn98 and Phe99 and Pro1, Ile3, Leu5). Residues Thr26, Gly27 and Asp29 located at the base of the active site are also important, and to a lesser extent Gly49, Ile50, Gly51 located at the tip of the flap region. The structure-based thermodynamic analysis also predicts the existence of regions of the protease with only marginal stability and a high propensity to undergo independent local unfolding. In particular, the flap region occupies a very shallow energy minimum and its conformation can easily be affected by relatively small perturbations. This property of the protease can be related to the ability of some mutations to elicit resistance towards certain inhibitors.
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Murphy KP, Xie D, Garcia KC, Amzel LM, Freire E. Structural energetics of peptide recognition: angiotensin II/antibody binding. Proteins 1993; 15:113-20. [PMID: 8441749 DOI: 10.1002/prot.340150203] [Citation(s) in RCA: 138] [Impact Index Per Article: 4.3] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/30/2023]
Abstract
The ability to predict the strength of the association of peptide hormones or other ligands with their protein receptors is of fundamental importance in the fields of protein engineering and rational drug design. To form a tight complex between a flexible peptide hormone and its receptor, the largeloss of configurational entropy must be overcome. Recently, the crystallographic structure of the complex between angiotensin II and the Fab fragment of a high affinity monoclonal antibody has been determined (Garcia, K.C., Ronco, P.M., Verroust, P.J., Brünger, A.T., Amzel, L.M. Three-dimensional structure of an angiotensin II-Fab complex at 3 A: Hormone recognition by an anti-idiotypic antibody. Science 257:502-507, 1992). In this paper we present a study of the thermodynamics of the association by high sensitivity isothermal titration calorimetry. The results of the experiments indicate that at 30 degrees C the binding is characterized by (1) a delta H of -8.9 +/- 0.7 kcal mol-1, (2) a delta Cp of -240 +/- 20 cal K-1 mol-1, and (3) the release of 1.1 +/- 0.1 protons per binding site in the pH range 6.0-7.3. Using these values and the previously determined binding constant in phosphate buffer, delta G at 30 degrees C is estimated as -11 kcal mol-1 and delta S as 6.9 cal K-1 mol-1. The calorimetric data indicate that binding is favored both enthalpically and entropically. These results have been complemented by structural thermodynamic calculations. The calculated and experimentally determined thermodynamic quantities are in good agreement.(ABSTRACT TRUNCATED AT 250 WORDS)
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Murphy KP, Bhakuni V, Xie D, Freire E. Molecular basis of co-operativity in protein folding. III. Structural identification of cooperative folding units and folding intermediates. J Mol Biol 1992; 227:293-306. [PMID: 1522594 DOI: 10.1016/0022-2836(92)90699-k] [Citation(s) in RCA: 135] [Impact Index Per Article: 4.1] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 12/27/2022]
Abstract
The hierarchical partition function formalism for protein folding developed earlier has been extended through the use of three-dimensional polar and apolar contact plots. For each amino acid residue in the protein, these plots indicate the apolar and polar surfaces that are buried from the solvent, the identity of all amino acid residues that contribute to this shielding, and the magnitude of their contributions. These contact plots are then used to examine the distribution of the free energy of stabilization throughout the protein molecule. Analysis of these data allows identification of co-operative folding units and their hierarchical levels, and the identification of partially folded intermediates with a significant probability of being populated. The overall folding/unfolding thermodynamics of 12 globular proteins, for which crystallographic and experimental thermodynamics are available, is predicted within error. An energetic classification of partially folded intermediates is presented and the results compared to those cases for which structural and thermodynamic experimental information is available. Four different types of partially folded states and their structural energies are considered. (1) Local intermediates, in which only a local region of the protein loses secondary and tertiary interactions, while the rest of the protein remains intact. (2) Global intermediates, corresponding to the standard molten globule definition, in which significant secondary structure is maintained but native-like tertiary structure contacts are disrupted. (3) Extended intermediates characterized by the existence of secondary structure elements (e.g. alpha-helices) exposed to solvent. (4) Folding intermediates in proteins with two structural domains. The structure and energetics of folding intermediates of apo-myoglobin, alpha-lactalbumin, phosphoglycerate kinase and arabinose-binding protein are considered in detail.
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Griko YV, Freire E, Privalov PL. Energetics of the alpha-lactalbumin states: a calorimetric and statistical thermodynamic study. Biochemistry 1994; 33:1889-99. [PMID: 8110793 DOI: 10.1021/bi00173a036] [Citation(s) in RCA: 132] [Impact Index Per Article: 4.3] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/28/2023]
Abstract
The temperature dependence of the heat capacity function of holo and apo alpha-lactalbumin has been studied by high sensitivity differential scanning microcalorimetry. The heat capacities of the holo and apo forms in the native state were found to be close to, but somewhat higher than, that of lysozyme, which has a similar structure. At pH values higher than 5, the heat-denatured state and the unfolded state are indistinguishable. At lower pH values, the heat capacity of the state obtained by heat or acid denaturation is lower than what is expected for the completely unfolded polypeptide chain, but it approaches that value at higher temperatures. The heat capacity increment of the denatured state correlates well with the amount of residual structure measured by ellipticity (i.e., the lower the residual structure, the higher the heat capacity). The extent of residual structure in the denatured state, which is exceptionally high in alpha-lactalbumin, decreases upon increasing temperature and at approximately 110 degrees C becomes close to that observed in 6 M GdmCl. Above 110 degrees C, the denatured state of alpha-lactalbumin is practically indistinguishable in heat capacity and ellipticity from the fully unfolded state. The calorimetric data have been analyzed quantitatively using a statistically thermodynamic formalism. This analysis indicates that the long-range or global cooperativity of the protein is lost after heat denaturation of the native state, causing the remaining elements of residual structure to behave in a more or less independent fashion. At pH values close to neutral, heat denaturation occurs at high temperature and yields a totally unfolded polypeptide with no measurable population of partly folded intermediates. At lower pH values, denaturation occurs at lower temperatures and a progressively higher population of intermediates is observed. At pH 4.2, about 50% of the molecules is in compact intermediate states immediately after heat denaturation; however, at pH 3.5, this percentage is close to 80% and at pH 3.0 it reaches about 100% of the protein molecules. Upon heating, the unfolded state progressively becomes the predominant species. The analysis of the heat capacity data for alpha-lactalbumin indicates that the best model to account for the observed behavior is one in which the denatured state is represented as a distribution of substates with varying degrees of residual structure. At low temperatures, the distribution is centered around rather compact substates with significant residual structure. At higher temperatures, the distribution shifts toward states with less residual structure and eventually to the completely unfolded state.
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Comparative Study |
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Lentz BR, Freire E, Biltonen RL. Fluorescence and calorimetric studies of phase transitions in phosphatidylcholine multilayers: kinetics of the pretransition. Biochemistry 1978; 17:4475-80. [PMID: 581473 DOI: 10.1021/bi00614a018] [Citation(s) in RCA: 131] [Impact Index Per Article: 2.8] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 12/23/2022]
Abstract
Discrepancies between calorimetric and fluorescence depolarization monitoring of the pretransition in multilamellar vesicles of synthetic phosphatidylcholines are shown to result primarily from the slow rate of this transition. The depolarization of fluorescence of the membrane-associated dye 1,6-diphenyl-1,3,5-hexatriene was used to determine the temperature of the pretransition for a series of heating and cooling scan rates. These temperatures, when plotted vs. scan rate, extrapolated linearly to the transition temperature at zero-scan rate, Tm = 29.8 +/- 0.8 degrees C. The slopes obtained from these plots yielded characteristic times for the transition of 8 to 30 min. In addition, analysis of temperature-jump experiments, assuming first-order kinetics, gave characteristic times in the range 4--8 min. The data are taken to suggest a most likely value for the pretransition characteristic time of 5 +/- 2 min, with larger values possibly explainable by supercooling effects. Slight differences between the calorimetrically and fluorimetrically determined main transition temperatures appear to result from perturbation of the phosphatidylcholine bilayer by the fluorescent probe.
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Abstract
Certain partly ordered protein conformations, commonly called "molten globule states," are widely believed to represent protein folding intermediates. Recent structural studies of molten globule states of different proteins have revealed features which appear to be general in scope. The emerging consensus is that these partly ordered forms exhibit a high content of secondary structure, considerable compactness, nonspecific tertiary structure, and significant structural flexibility. These characteristics may be used to define a general state of protein folding called "the molten globule state," which is structurally and thermodynamically distinct from both the native state and the denatured state. Despite extensive knowledge of structural features of a few molten globule states, a cogent thermodynamic argument for their stability has not yet been advanced. The prevailing opinion of the last decade was that there is little or no enthalpy difference or heat capacity difference between the molten globule state and the unfolded state. This view, however, appears to be at variance with the existing database of protein structural energetics and with recent estimates of the energetics of denaturation of alpha-lactalbumin, cytochrome c, apomyoglobin, and T4 lysozyme. We discuss these four proteins at length. The results of structural studies, together with the existing thermodynamic values for fundamental interactions in proteins, provide the foundation for a structural thermodynamic framework which can account for the observed behavior of molten globule states. Within this framework, we analyze the physical basis for both the high stability of several molten globule states and the low probability of other potential folding intermediates. Additionally, we consider, in terms of reduced enthalpy changes and disrupted cooperative interactions, the thermodynamic basis for the apparent absence of a thermally induced, cooperative unfolding transition for some molten globule states.
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Biltonen RL, Freire E. Thermodynamic characterization of conformational states of biological macromolecules using differential scanning calorimetry. CRC CRITICAL REVIEWS IN BIOCHEMISTRY 1978; 5:85-124. [PMID: 363351 DOI: 10.3109/10409237809177141] [Citation(s) in RCA: 122] [Impact Index Per Article: 2.6] [Reference Citation Analysis] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 12/14/2022]
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Haltia T, Freire E. Forces and factors that contribute to the structural stability of membrane proteins. BIOCHIMICA ET BIOPHYSICA ACTA 1995; 1228:1-27. [PMID: 7857960 DOI: 10.1016/0005-2728(94)00161-w] [Citation(s) in RCA: 120] [Impact Index Per Article: 4.0] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 01/27/2023]
Abstract
While a considerable amount of literature deals with the structural energetics of water-soluble proteins, relatively little is known about the forces that determine the stability of membrane proteins. Similarly, only a few membrane protein structures are known at atomic resolution, although new structures have recently been described. In this article, we review the current knowledge about the structural features of membrane proteins. We then proceed to summarize the existing literature regarding the thermal stability of bacteriorhodopsin, cytochrome-c oxidase, the band 3 protein, Photosystem II and porins. We conclude that a fundamental difference between soluble and membrane proteins is the high thermal stability of intrabilayer secondary structure elements in membrane proteins. This property manifests itself as incomplete unfolding, and is reflected in the observed low enthalpies of denaturation of most membrane proteins. By contrast, the extramembranous parts of membrane proteins may behave much like soluble proteins. A brief general account of thermodynamics factors that contribute to the stability of water soluble and membrane proteins is presented.
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Shortle D, Meeker AK, Freire E. Stability mutants of staphylococcal nuclease: large compensating enthalpy-entropy changes for the reversible denaturation reaction. Biochemistry 1988; 27:4761-8. [PMID: 3167015 DOI: 10.1021/bi00413a027] [Citation(s) in RCA: 117] [Impact Index Per Article: 3.2] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/04/2023]
Abstract
By use of intrinsic fluorescence to determine the apparent equilibrium constant Kapp as a function of temperature, the midpoint temperature Tm and apparent enthalpy change delta Happ on reversible thermal denaturation have been determined over a range of pH values for wild-type staphylococcal nuclease and six mutant forms. For wild-type nuclease at pH 7.0, a Tm of 53.3 +/- 0.2 degrees C and a delta Happ of 86.8 +/- 1.4 kcal/mol were obtained, in reasonable agreement with values determined calorimetrically, 52.8 degrees C and 96 +/- 2 kcal/mol. The heat capacity change on denaturation delta Cp was estimated at 1.8 kcal/(mol K) versus the calorimetric value of 2.2 kcal/(mol K). When values of delta Happ and delta Sapp for a series of mutant nucleases that exhibit markedly altered denaturation behavior with guanidine hydrochloride and urea were compared at the same temperature, compensating changes in enthalpy and entropy were observed that greatly reduce the overall effect of the mutations on the free energy of denaturation. In addition, a correlation was found between the estimated delta Cp for the mutant proteins and the d(delta Gapp)/dC for guanidine hydrochloride denaturation. It is proposed that both the enthalpy/entropy compensation and this correlation between two seemingly unrelated denaturation parameters are consequences of large changes in the solvation of the denatured state that result from the mutant amino acid substitutions.
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Velazquez-Campoy A, Todd MJ, Vega S, Freire E. Catalytic efficiency and vitality of HIV-1 proteases from African viral subtypes. Proc Natl Acad Sci U S A 2001; 98:6062-7. [PMID: 11353856 PMCID: PMC33422 DOI: 10.1073/pnas.111152698] [Citation(s) in RCA: 112] [Impact Index Per Article: 4.7] [Reference Citation Analysis] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/18/2000] [Accepted: 03/28/2001] [Indexed: 11/18/2022] Open
Abstract
The vast majority of HIV-1 infections in Africa are caused by the A and C viral subtypes rather than the B subtype prevalent in the United States and Western Europe. Genomic differences between subtypes give rise to sequence variations in the encoded proteins, including the HIV-1 protease. Because some amino acid polymorphisms occur at sites that have been associated with drug resistance in the B subtype, it is important to assess the effectiveness of protease inhibitors that have been developed against different subtypes. Here we report the enzymatic characterization of HIV-1 proteases with sequences found in drug-naive Ugandan adults. The A protease used in these studies differs in seven positions (I13V/E35D/M36I/R41K/R57K/H69K/L89M) in relation to the consensus B subtype protease. Another protease containing a subset of these amino acid polymorphisms (M36I/R41K/H69K/L89M), which are found in subtype C and other HIV subtypes, also was studied. Both proteases were found to have similar catalytic constants, k(cat), as the B subtype. The C subtype protease displayed lower K(m) values against two different substrates resulting in a higher (2.4-fold) catalytic efficiency than the B subtype protease. Indinavir, ritonavir, saquinavir, and nelfinavir inhibit the A and C subtype proteases with 2.5-7-fold and 2-4.5-fold weaker K(i)s than the B subtype. When all factors are taken into consideration it is found that the C subtype protease has the highest vitality (4-11 higher than the B subtype) whereas the A subtype protease exhibits values ranging between 1.5 and 5. These results point to a higher biochemical fitness of the A and C proteases in the presence of existing inhibitors.
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Abstract
Two effects are mainly responsible for the observed enthalpy change in protein unfolding: the disruption of internal interactions within the protein molecule (van der Waals, hydrogen bonds, etc.) and the hydration of the groups that are buried in the native state and become exposed to the solvent on unfolding. In the traditional thermodynamic analysis, the effects of hydration have usually been evaluated using the thermodynamic data for the transfer of small model compounds from the gas phase to water. The contribution of internal interactions, on the other hand, are usually estimated by subtracting the hydration effects from the experimental enthalpy of unfolding. The main drawback of this approach is that the enthalpic contributions of hydration, and those due to the disruption of internal interactions, are more than one order of magnitude larger than the experimental enthalpy value. The enthalpy contributions of hydration and disruption of internal interactions have opposite signs and cancel each other almost completely resulting in a final value that is over 10 times smaller than the individual terms. For this reason, the classical approach cannot be used to accurately predict unfolding enthalpies from structure: any error in the estimation of the hydration enthalpy will be amplified by a factor of 10 or more in the estimation of the unfolding enthalpy. Recently, it has been shown that simple parametric equations that relate the enthalpy change with certain structural parameters, especially changes in solvent accessible surface areas have considerable predictive power. In this paper, we provide a physical foundation to that parametrization and in the process we present a system of equations that explicitly includes the enthalpic effects of the packing density between the different atoms within the protein molecule. Using this approach, the error in the prediction of folding/unfolding enthalpies at 60 degrees C, the median temperature for thermal unfolding, is better than +/- 3% (standard deviation = 4 kcal/mol).
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