Entropy-driven binding of picomolar transition state analogue inhibitors to human 5'-methylthioadenosine phosphorylase

Human 5'-methylthioadenosine phosphorylase (MTAP) links the polyamine biosynthetic and S-adenosyl-l-methionine salvage pathways and is a target for anticancer drugs. p-Cl-PhT-DADMe-ImmA is a 10 pM, slow-onset tight-binding transition state analogue inhibitor of the enzyme. Titration of homotrimeric MTAP with this inhibitor established equivalent binding and independent catalytic function of the three catalytic sites. Thermodynamic analysis of MTAP with tight-binding inhibitors revealed entropic-driven interactions with small enthalpic penalties. A large negative heat capacity change of -600 cal/(mol K) upon inhibitor binding to MTAP is consistent with altered hydrophobic interactions and release of water. Crystal structures of apo MTAP and MTAP in complex with p-Cl-PhT-DADMe-ImmA were determined at 1.9 and 2.0 ? resolution, respectively. Inhibitor binding caused condensation of the enzyme active site, reorganization at the trimer interfaces, the release of water from the active sites and subunit interfaces, and compaction of the trimeric structure. These structural changes cause the entropy-favored binding of transition state analogues. Homotrimeric human MTAP is contrasted to the structurally related homotrimeric human purine nucleoside phosphorylase. p-Cl-PhT-DADMe-ImmA binding to MTAP involves a favorable entropy term of -17.6 kcal/mol with unfavorable enthalpy of 2.6 kcal/mol. In contrast, binding of an 8.5 pM transition state analogue to human PNP has been shown to exhibit the opposite behavior, with an unfavorable entropy term of 3.5 kcal/mol and a favorable enthalpy of -18.6 kcal/mol. Transition state analogue interactions reflect protein architecture near the transition state, and the profound thermodynamic differences for MTAP and PNP suggest dramatic differences in contributions to catalysis from protein architecture.     

HIV-1 protease inhibitors: enthalpic versus entropic optimization of the binding affinity

Existing experimental as well as computational screening methods select potential ligands or drug candidates on the basis of binding affinity. Since the binding affinity is a function of the enthalpy (DeltaH) and entropy (DeltaS) changes, it is apparent that improved binding can be achieved in different ways: by optimizing DeltaH, DeltaS, or a combination of both. However, the behavior of enthalpically or entropically optimized inhibitors is fundamentally different, including their response to mutations that may elicit drug resistance. In the design of HIV-1 protease inhibitors, high binding affinity has usually been achieved by preshaping lead compounds to the geometry of the binding site and by incorporating a high degree of hydrophobicity. The thermodynamic consequence of that approach is that the binding affinity of the resulting inhibitors becomes entropically favorable but enthalpically unfavorable. Specifically, the resulting high binding affinity is due to an increased solvation entropy (hydrophobic effect) combined with a reduced loss of conformational entropy of the inhibitor upon binding (structural rigidity). Here we report that tripeptide inhibitors derived from the transframe region of Gag-Pol (Glu-Asp-Leu and Glu-Asp-Phe) bind to the HIV-1 protease with a favorable enthalpy change. This behavior is qualitatively different from that of known inhibitors and points to new strategies for inhibitor design. Since the binding affinities of enthalpically favorable and enthalpically unfavorable inhibitors have opposite temperature dependence, it is possible to design fast screening protocols that simultaneously select inhibitors on the basis of affinity and enthalpy.     

Factorising ligand affinity: a combined thermodynamic and crystallographic study of trypsin and thrombin inhibition.

The binding of a series of low molecular weight ligands towards trypsin and thrombin has been studied by isothermal titration calorimetry and protein crystallography. In a series of congeneric ligands, surprising changes of protonation states occur and are overlaid on the binding process. They result from induced pK(a) shifts depending on the local environment experienced by the ligand and protein functional groups in the complex (induced dielectric fit). They involve additional heat effects that must be corrected before any conclusion on the binding enthalpy (DeltaH) and entropy (DeltaS) can be drawn. After correction, trends in both contributions can be interpreted in structural terms with respect to the hydrogen bond inventory or residual ligand motions. For all inhibitors studied, a strong negative heat capacity change (DeltaC(p)) is detected, thus binding becomes more exothermic and entropically less favourable with increasing temperature. Due to a mutual compensation, Gibbs free energy remains virtually unchanged. The strong negative DeltaC(p) value cannot solely be explained by the removal of hydrophobic surface portions of the protein or ligand from water exposure. Additional contributions must be considered, presumably arising from modulations of the local water structure, changes in vibrational modes or other ordering parameters. For thrombin, smaller negative DeltaC(p) values are observed for ligand binding in the presence of sodium ions compared to the other alkali ions, probably due to stabilising effects on the protein or changes in the bound water structure.     

Comparisons of pressure and temperature activation parameters for amide hydrogen exchange in T4 lysozyme

Activation enthalpies and entropies are reported for proton-deuteron exchange at 42 amide sites in T4 lysozyme and compared with activation volumes for the same residues obtained earlier [Hitchens, T. K., and Bryant, R. G. (1998) Biochemistry 37, 5878-5887]. There is no correlation found between activation volume and activation entropy or activation enthalpy. The activation enthalpy is linearly related to the activation entropy in part as a consequence of a relatively narrow sampling window for the rate constants that corresponds to a narrow range of activation free energy. A consequence of the entropy-enthalpy compensation is preservation of rank order of proton exchange. Variations in DeltaH, DeltaS, and DeltaV for residues that are structurally close together in the folded protein suggest that there may be a variety of energetically distinct pathways for the access of solvent to these structurally related exchange sites.     

Structural parameterization of the binding enthalpy of small ligands

A major goal in ligand and drug design is the optimization of the binding affinity of selected lead molecules. However, the binding affinity is defined by the free energy of binding, which, in turn, is determined by the enthalpy and entropy changes. Because the binding enthalpy is the term that predominantly reflects the strength of the interactions of the ligand with its target relative to those with the solvent, it is desirable to develop ways of predicting enthalpy changes from structural considerations. The application of structure/enthalpy correlations derived from protein stability data has yielded inconsistent results when applied to small ligands of pharmaceutical interest (MW < 800). Here we present a first attempt at an empirical parameterization of the binding enthalpy for small ligands in terms of structural information. We find that at least three terms need to be considered: (1) the intrinsic enthalpy change that reflects the nature of the interactions between ligand, target, and solvent; (2) the enthalpy associated with any possible conformational change in the protein or ligand upon binding; and, (3) the enthalpy associated with protonation/deprotonation events, if present. As in the case of protein stability, the intrinsic binding enthalpy scales with changes in solvent accessible surface areas. However, an accurate estimation of the intrinsic binding enthalpy requires explicit consideration of long-lived water molecules at the binding interface. The best statistical structure/enthalpy correlation is obtained when buried water molecules within 5-7 A of the ligand are included in the calculations. For all seven protein systems considered (HIV-1 protease, dihydrodipicolinate reductase, Rnase T1, streptavidin, pp60c-Src SH2 domain, Hsp90 molecular chaperone, and bovine beta-trypsin) the binding enthalpy of 25 small molecular weight peptide and nonpeptide ligands can be accounted for with a standard error of +/-0.3 kcal x mol(-1).     

The thermodynamics of protein-ligand interaction and solvation: insights for ligand design

Isothermal titration calorimetry is able to provide accurate information on the thermodynamic contributions of enthalpy and entropy changes to free energies of binding. The Structure/Calorimetry of Reported Protein Interactions Online database of published isothermal titration calorimetry studies and structural information on the interactions between proteins and small-molecule ligands is used here to reveal general thermodynamic properties of protein-ligand interactions and to investigate correlations with changes in solvation. The overwhelming majority of interactions are found to be enthalpically favoured. Synthetic inhibitors and biological ligands form two distinct subpopulations in the data, with the former having greater average affinity due to more favourable entropy changes on binding. The greatest correlation is found between the binding free energy and apolar surface burial upon complex formation. However, the free-energy contribution per unit area buried is only 30-50% of that expected from earlier studies of transfer free energies of small molecules. A simple probability-based estimator for the maximal affinity of a binding site in terms of its apolar surface area is proposed. Polar surface area burial also contributes substantially to affinity but is difficult to express in terms of unit area due to the small variation in the amount of polar surface buried and a tendency for cancellation of its enthalpic and entropic contributions. Conventionally, the contribution of apolar desolvation to affinity is attributed to gain of entropy due to solvent release. Although data presented here are supportive of this notion, because the correlation of entropy change with apolar surface burial is relatively weak, it cannot, on present evidence, be confidently considered to be correct. Further, thermodynamic changes arising from small differences between ligands binding to individual proteins are relatively large and, in general, uncorrelated with changes in solvation, suggesting that trends identified across widely differing proteins are of limited use in explaining or predicting the effects of ligand modifications.     

What drives proteins into the major or minor grooves of DNA?

The energetic profiles of a significant number of protein-DNA systems at 20 °C reveal that, despite comparable Gibbs free energies, association with the major groove is primarily an enthalpy-driven process, whereas binding to the minor groove is characterized by an unfavorable enthalpy that is compensated by favorable entropic contributions. These distinct energetic signatures for major versus minor groove binding are irrespective of the magnitude of DNA bending and/or the extent of binding-induced protein refolding. The primary determinants of their different energetic profiles appear to be the distinct hydration properties of the major and minor grooves; namely, that the water in the A+T-rich minor groove is in a highly ordered state and its removal results in a substantial positive contribution to the binding entropy. Since the entropic forces driving protein binding into the minor groove are a consequence of displacing water ordered by the regular arrangement of polar contacts, they cannot be regarded as hydrophobic.     

Conformational Changes and Ligand Recognition of Escherichia colid-Xylose Binding Protein Revealed

ATP binding cassette transport systems account for most import of necessary nutrients in bacteria. The periplasmic binding component (or an equivalent membrane-anchored protein) is critical to recognizing cognate ligand and directing it to the appropriate membrane permease. Here we report the X-ray structures of d-xylose binding protein from Escherichia coli in ligand-free open form, ligand-bound open form, and ligand-bound closed form at 2.15 Å, 2.2 Å, and 2.2 Å resolutions, respectively. The ligand-bound open form is the first such structure to be reported at high resolution; the combination of the three different forms from the same protein furthermore gives unprecedented details concerning the conformational changes involved in binding protein function. As is typical of the structural family, the protein has two similar globular domains, which are connected by a three-stranded hinge region. The open liganded structure shows that xylose binds first to the C-terminal domain, with only very small conformational changes resulting. After a 34° closing motion, additional interactions are formed with the N-terminal domain; changes in this domain are larger and serve to make the structure more ordered near the ligand. An analysis of the interactions suggests why xylose is the preferred ligand. Furthermore, a comparison with the most closely related proteins in the structural family shows that the conformational changes are distinct in each type of binding protein, which may have implications for how the individual proteins act in concert with their respective membrane permeases.     

Enthalpy–entropy compensation phenomena in water solutions of proteins and small molecules: A ubiquitous properly of water

This article presents evidence for the existence of a specific linear relationship between the entropy change and the enthalpy change in a variety of processes of small solutes in water solution. The processes include solvation of ions and nonelectrolytes, hydrolysis, oxidation–reduction, ionization of weak electrolytes, and quenching of indole fluorescence among others. The values of the proportionality constant, called the compensation temperature, lie in a relatively narrow range, from about 250 to 315 °K, for all these processes. Such behavior can be a consequence of experimental errors but for a number of the processes the precision of the data is sufficient to show that the enthalpy–entropy compensation pattern is real. It is tentatively concluded that the pattern is real, very common and a consequence of the properties of liquid water as a solvent regardless of the solutes and the solute processes studied. As such the phenomenon requires that theoretical treatments of solute processes in water be expanded by inclusion of a specific treatment of the characteristic of water responsible for compensation behavior. The possible bases of the effect are proposed to be temperature-independent heat-capacity changes and/or shifts in concentrations of the two phenomenologically significant species of water. The relationship of these alternatives to the two-state process of water suggested by spectroscopic and relaxation studies is examined. The existence of a similar and probably identical relationship between enthalpy and entropy change in a variety of protein reactions suggests that liquid water plays a direct role in many protein processes and may be a common participant in the physiological function of proteins. It is proposed that the linear enthalpy–entropy relationship be used as a diagnostic test for the participation of water in protein processes. On this basis the catalytic processes of chymotrypsin and acetylcholinesterase are dominated by the properties of bulk water. The binding of oxygen by hemoglobin may fall in the same category. Similarities and differences in the behavior of small-solute and protein processes are examined to show how they may be related. No positive conclusions are established, but it is possible that protein processes are coupled to water via expansions and contractions of the protein and that in general the special pattern of enthalpy–entropy compensation is a consequent of the properties of water which require that expansions and contractions of solutes effect changes in the free volume of the nearby liquid water. It is shown that proteins can be expected to respond to changes in nearby water and interfacial free energy by expansions and contractions. Such responses may explain a variety of currently unexplained characteristics of protein solutions. More generally, the enthalpy–entropy compensation pattern appears to be the thermodynamic manifestation of “structure making” and “structure breaking,” operationally defined terms much used in discussions of water solutions. If so, the compensation pattern is ubiquitous and requires re-examination of a large body of molecular interpretations derived from quantitative studies of processes in water. Theories of processes in water may have to be expanded to accommodate this aspect of water behavior.     

Thermodynamic basis of resistance to HIV-1 protease inhibition: calorimetric analysis of the V82F/I84V active site resistant mutant

One of the most serious side effects associated with the therapy of HIV-1 infection is the appearance of viral strains that exhibit resistance to protease inhibitors. The active site mutant V82F/I84V has been shown to lower the binding affinity of protease inhibitors in clinical use. To identify the origin of this effect, we have investigated the binding thermodynamics of the protease inhibitors indinavir, ritonavir, saquinavir, and nelfinavir to the wild-type HIV-1 protease and to the V82F/I84V resistant mutant. The main driving force for the binding of all four inhibitors is a large positive entropy change originating from the burial of a significant hydrophobic surface upon binding. At 25 degrees C, the binding enthalpy is unfavorable for all inhibitors except ritonavir, for which it is slightly favorable (-2.3 kcal/mol). Since the inhibitors are preshaped to the geometry of the binding site, their conformational entropy loss upon binding is small, a property that contributes to their high binding affinity. The V82F/I84V active site mutation lowers the affinity of the inhibitors by making the binding enthalpy more positive and making the entropy change slightly less favorable. The effect on the enthalpy change is, however, the major one. The predominantly enthalpic effect of the V82F/I84V mutation is consistent with the idea that the introduction of the bulkier Phe side chain at position 82 and the Val side chain at position 84 distort the binding site and weaken van der Waals and other favorable interactions with inhibitors preshaped to the wild-type binding site. Another contribution of the V82F/I84V to binding affinity originates from an increase in the energy penalty associated with the conformational change of the protease upon binding. The V82F/I84V mutant is structurally more stable than the wild-type protease by about 1.4 kcal/mol. This effect, however, affects equally the binding affinity of substrate and inhibitors.     

Energetics of peptide recognition by the second PDZ domain of human protein tyrosine phosphatase 1E

Formation of protein-protein assemblies is essential in maintaining cell structure and function. Conservation of structural motifs and binding sites is the result of evolutionary pressure for solutions compatible with both molecular economy and regulation. PDZ domains are a typical example: A conserved fold governs specificity toward recognition of C-terminal protein sequences by small sequential and/or structural deviations within a canonical binding mode. The energetic principles underlying the strength and specificity of PDZ-protein interactions are practically unknown. We use the second PDZ domain (PDZ2) of the human protein tyrosine phosphatase (hPTP1E) as a model to study the energetics of peptide binding to a class I PDZ domain. Calorimetric experiments reveal the enthalpy, entropy, and heat capacity changes accompanying PDZ2 binding to the C-terminal pentadecapeptide derived from the guanine nucleotide exchange factor RA-GEF2. Association is driven by favorable enthalpy and entropy changes below 18 degrees C. Above that temperature the entropy change opposes complex formation. Structure-based predictions poorly reproduce the observed thermodynamic profile of the PDZ-peptide complex. On the basis of MD simulations and experimental findings by others we suggest that changes in the dynamics of the PDZ domain upon peptide binding make a large contribution to the observed thermodynamic parameters. Possible impacts of subtle, ligand-induced structural "stiffening" of PDZ domains are discussed. In our hands, the C-terminal segment of the tumor suppressor APC binds much less tightly to PDZ2 than what has been proposed earlier from surface plasmon resonance experiments.     

Further studies on the temperature dependence of the binding of testosterone to human pregnancy plasma proteins

The binding of testosterone by pregnancy plasma proteins has been studied by a new equilibrium dialysis system. The temperature dependence on the association constant has been investigated and the enthalpy change ΔH and entropy change ΔS have been calculated.By a computer optimization program, the binding constant of the high affinity testosterone binding protein has been estimated from Scatchard plots. The binding reactions were carried out at 5°, 25° and 37° C. The corresponding values were 3.1.10 1.2.10⁹ and 7.2.10⁸ liter/mole. The resulting enthalpy and entropy changes were ?2.0 kcal/mole and 35.0 cal/(mole.degree) respectively.It can be concluded that the binding of testosterone to the specific binding protein is an exothermic reaction and is stabilized by hydrophobic binding forces.     

Thermodynamic analysis of an entropically driven,high-affinity nanobody-HIV p24 interaction

Protein-protein interactions are fundamental to life processes. Complementary computational, structural, and biophysical studies of these interactions enable the forces behind their specificity and strength to be understood. Antibody fragments such as single-chain antibodies have the specificity and affinity of full antibodies but a fraction of their size, expediting whole molecule studies and distal effects without exceeding the computational capacity of modeling systems. We previously reported the crystal structure of a high-affinity nanobody 59H10 bound to HIV-1 capsid protein p24 and deduced key interactions using all-atom molecular dynamics simulations. We studied the properties of closely related medium (37E7) and low (48G11) affinity nanobodies, to understand how changes of three (37E7) or one (48G11) amino acids impacted these interactions; however, the contributions of enthalpy and entropy were not quantified. Here, we report the use of qualitative and quantitative experimental and in silico approaches to separate the contributions of enthalpy and entropy. We used complementary circular dichroism spectroscopy and molecular dynamics simulations to qualitatively delineate changes between nanobodies in isolation and complexed with p24. Using quantitative techniques such as isothermal titration calorimetry alongside WaterMap and Free Energy Perturbation protocols, we found the difference between high (59H10) and medium (37E7) affinity nanobodies on binding to HIV-1 p24 is entropically driven, accounted for by the release of unstable waters from the hydrophobic surface of 59H10. Our results provide an exemplar of the utility of parallel in vitro and in silico studies and highlight that differences in entropic interactions between amino acids and water molecules are sufficient to drive orders of magnitude differences in affinity.     

Calculation of Proteins’ Total Side-Chain Torsional Entropy and Its Influence on Protein-Ligand Interactions

Despite the high density within a typical protein fold, the ensemble of sterically permissible side-chain repackings is vast. Here, we examine the extent of this variability that survives energetic biases due to van der Waals interactions, hydrogen bonding, salt bridges, and solvation. Monte Carlo simulations of an atomistic model exhibit thermal fluctuations among a diverse set of side-chain arrangements, even with the peptide backbone fixed in its crystallographic conformation. We have quantified the torsional entropy of this native-state ensemble, relative to that of a noninteracting reference system, for 12 small proteins. The reduction in entropy per rotatable bond due to each kind of interaction is remarkably consistent across this set of molecules. To assess the biophysical importance of these fluctuations, we have estimated side-chain entropy contributions to the binding affinity of several peptide ligands with calmodulin. Calculations for our fixed-backbone model correlate very well with experimentally determined binding entropies over a range spanning more than 80 kJ/(mol·308 K).     

Alternate Binding Modes for a Ubiquitin-SH3 Domain Interaction Studied by NMR Spectroscopy

Surfaces of many binding domains are plastic, enabling them to interact with multiple targets. An understanding of how they bind and recognize their partners is therefore predicated on characterizing such dynamic interfaces. Yet, these interfaces are difficult to study by standard biophysical techniques that often ‘freeze’ out conformations or that produce data averaged over an ensemble of conformers. In this study, we used NMR spectroscopy to study the interaction between the C-terminal SH3 domain of CIN85 and ubiquitin that involves the ‘classical’ binding sites of these proteins. Notably, chemical shift titration data of one target with another and relaxation dispersion data that report on millisecond time scale exchange processes are both well fit to a simple binding model in which free protein is in equilibrium with a single bound conformation. However, dissociation constants and chemical shift differences between free and bound states measured from both classes of experiment are in disagreement. It is shown that the data can be reconciled by considering three-state binding models involving two distinct bound conformations. By combining titration and dispersion data, kinetic and thermodynamic parameters of the three-state binding reaction are obtained along with chemical shifts for each state. A picture emerges in which one bound conformer has increased entropy and enthalpy relative to the second and chemical shifts similar to that of the free state, suggesting a less packed interface. This study provides an example of the interplay between entropy and enthalpy to fine-tune molecular interactions involving the same binding surfaces.     

Peptide selectivity between the PDZ domains of human pregnancy‐related serine proteases (HtrA1, HtrA2, HtrA3, and HtrA4) can be reshaped by different halogen probes

The human HtrA family of serine proteases (HtrA1, HtrA2, HtrA3, and HtrA4) are the key enzymes associated with pregnancy and closely related to the development and progression of many pathological events. Previously, it was found that halogen substitution at the indole moiety of peptide Trp‐1 residue can form a geometrically satisfactory halogen bond with the Drosophila discs large, zona occludens‐1 (PDZ) domain of HtrA proteases. Here, we attempt to systematically investigate the effect of substitution with 4 halogen types and 2 indole positions on the binding affinity and specificity of peptide ligands to the 4 HtrA PDZ domains. The complex structures, interaction energies, halogen‐bonding strength, and binding affinity of domain‐peptide systems were modeled, analyzed, and measured via computational modeling and fluorescence‐based assay. It is revealed that there is a compromise between the local rearrangement of halogen bond involving different halogen atoms and the global optimization of domain‐peptide interaction; the substitution position is fundamentally important for peptide‐binding affinity, while the halogen type can effectively shift peptide selectivity between the 4 domains. The HtrA1‐PDZ and HtrA4‐PDZ as well as HtrA2‐PDZ and HtrA3‐PDZ respond similarly to different halogen substitutions of peptide; –Br substitution at R2‐position and –I substitution at R4‐position are most effective in improving peptide selectivity for HtrA1‐PDZ/HtrA4‐PDZ and HtrA2‐PDZ/HtrA3‐PDZ, respectively; –F substitution would not address substantial effect on peptide selectivity for all the 4 domains. Consequently, the binding affinities of a native peptide ligand DSRIWWV^–COOH as well as its 4 R2‐halogenated counterparts were determined as 1.9, 1.4, 0.5, 0.27, and 0.92 μM, which are basically consistent with computational analysis. This study would help to rationally design selective peptide inhibitors of HtrA family members by using different halogen substitutions.     

Identification of Clausine E as an inhibitor of fat mass and obesity‐associated protein (FTO) demethylase activity

The alkaloids containing a carbazole nucleus are an established class of natural products with wide range of biological activities. A combination of thermodynamic and enzymatic activity studies provides an insight into the recognition of Clausine E by the fat mass and obesity‐associated protein (FTO). The binding of Clausine E to FTO was driven by positive entropy and negative enthalpy changes. Results also indicated that the hydroxyl group was crucial for the binding of small molecules with FTO. The structural and thermodynamic information provides the basis for the design of more effective inhibitors for FTO demethylase activity.     

Congeneric but still distinct: how closely related trypsin ligands exhibit different thermodynamic and structural properties

A congeneric series of benzamidine-type ligands with a central proline moiety and a terminal cycloalkyl group—linked by a secondary amine, ether, or methylene bridge—was synthesized as trypsin inhibitors. This series of inhibitors was investigated by isothermal titration calorimetry, crystal structure analysis in two crystal forms, and molecular dynamics simulations. Even though all of these congeneric ligands exhibited essentially the same affinity for trypsin, their binding profiles at the structural, dynamic, and thermodynamic levels are very distinct. The ligands display a pronounced enthalpy/entropy compensation that results in a nearly unchanged free energy of binding, even though individual enthalpy and entropy terms change significantly across the series. Crystal structures revealed that the secondary amine-linked analogs scatter over two distinct conformational families of binding modes that occupy either the inside or of the outside the protein's S3/S4 specificity pocket. In contrast, the ether-linked and methylene-linked ligands preferentially occupy the hydrophobic specificity pocket. This also explains why the latter ligands could only be crystallized in the conformationally restricting closed crystal form whereas the derivative with the highest residual mobility in the series escaped our attempts to crystallize it in the closed form; instead, a well-resolved structure could only be achieved in the open form with the ligand in disordered orientation. These distinct binding modes are supported by molecular dynamics simulations and correlate with the shifting enthalpic/entropic signatures of ligand binding. The examples demonstrate that, at the molecular level, binding modes and thermodynamic binding signatures can be very different even for closely related ligands. However, deviating binding profiles provide the opportunity to optimally address a given target.     

Thermodynamics of Ras/effector and Cdc42/effector interactions probed by isothermal titration calorimetry

Proliferation, differentiation, and morphology of eucaryotic cells is regulated by a large network of signaling molecules. Among the major players are members of the Ras and Rho/Rac subfamilies of small GTPases that bind to different sets of effector proteins. Recognition of multiple effectors is important for communicating signals into different pathways, leading to the question of how an individual GTPase achieves tight binding to diverse targets. To understand the observed specificity, detailed information about binding energetics is expected to complement the information gained from the three-dimensional structures of GTPase/effector protein complexes. Here, the thermodynamics of the interaction of four closely related members of the Ras subfamily with four different effectors and, additionally, the more distantly related Cdc42/WASP couple were quantified by means of isothermal titration calorimetry. The heat capacity changes upon complex formation were rationalized in light of the GTPase/effector complex structures. Changes in enthalpy, entropy, and heat capacity of association with various Ras proteins are similar for the same effector. In contrast, although the structures of the Ras-binding domains are similar, the thermodynamics of the Ras/Raf and Ras/Ral guanine nucleotide dissociation stimulator interactions are quite different. The energy profile of the Cdc42/WASP interaction is similar to Ras/Ral guanine nucleotide dissociation stimulator, despite largely different structures and interface areas of the complexes. Water molecules in the interface cannot fully account for the observed discrepancy but may explain the large range of Ras/effector binding specificity. The differences in the thermodynamic parameters, particularly the entropy changes, could help in the design of effector-specific inhibitors that selectively block a single pathway.     

Binding of nonphysiological protein and peptide substrates to proteases: differences between urokinase-type plasminogen activator and trypsin and contributions to the evolution of regulated proteolysis

Understanding the regulation of physiological processes requires detailed knowledge of the recognition of substrates by enzymes. One of the most productive model systems for the study of enzyme-substrate interactions is the serine protease family; however, most studies of protease action have used small substrates that contain an activated, non-natural scissile bond. Because few kinetic or structural studies have used protein substrates, the physiologically relevant target of most proteases, it seems likely that important mechanisms of substrate recognition and processing by proteases have not yet been fully elucidated. Consistent with this hypothesis, we have observed that K(m) values for protein substrates are reduced as much as 200-15000-fold relative to those of analogous peptide substrates. Here we examine the thermodynamic consequences of interactions between proteases and their substrates using staphylococcal nuclease (SNase) and SNase variants as model protein substrates. We have obtained values for enthalpy, entropy, and K(d) for binding of proteins and peptides by the nonspecific protease trypsin and the highly specific protease urokinase-type plasminogen activator (u-PA). To avoid cleavage of substrates during these measurements, we used inactive variants of trypsin and u-PA whose catalytic serine S195 had been replaced by alanine. Differences in the K(d) values for binding of protein and peptide substrates closely approximate the large differences observed in the corresponding K(m) values. Improved binding of protein substrates is due to decreased enthalpy, and this effect is pronounced for the selective protease u-PA. Fundamental differences in recognition of analogous protein and peptide substrates may have influenced the evolution of protease specificity.