Thermodynamic characterization of ligand-induced conformational changes in UDP-N-acetylglucosamine enolpyruvyl transferase.

The binding of UDP-N-acetylglucosamine (UDPNAG) to the enzyme UDP-N-acetylglucosamine enolpyruvyl transferase (MurA) was studied in the absence and presence of the antibiotic fosfomycin by isothermal titration calorimetry. Fosfomycin binds covalently to MurA in the presence of UDPNAG and also in its absence as demonstrated by MALDI mass spectrometry. The covalent attachment of fosfomycin affects the thermodynamic parameters of UDPNAG binding significantly: In the absence of fosfomycin the binding of UDPNAG is enthalpically driven (DeltaH = -35.5 kJ mol(-1) at 15 degrees C) and opposed by an unfavorable entropy change (DeltaS = -25 J mol(-1) K(-1)). In the presence of covalently attached fosfomycin the binding of UDPNAG is entropically driven (DeltaS = 187 J mol(-1)K(-1) at 15 degrees C) and associated with unfavorable changes in enthalpy (DeltaH = 28.8 kJ mol(-1)). Heat capacities for UDPNAG binding in the absence or presence of fosfomycin were -1.87 and -2.74 kJ mol(-1) K(-1), respectively, indicating that most ( approximately 70%) of the conformational changes take place upon formation of the UDPNAG-MurA binary complex. The major contribution to the heat capacity of ligand binding is thought to be due to changes in the solvent-accessible surface area. However, associated conformational changes, if any, also contribute to the experimentally measured magnitude of the heat capacity. The changes in solvent-accessible surface area were calculated from available 3D structures, yielding a DeltaC(p) of -1.3 kJ mol(-1) K(-1); i.e., the experimentally determined heat capacity exceeds the calculated one. This implies that other thermodynamic factors exert a large influence on the heat capacity of protein-ligand interactions.

Energetics of coiled coil folding: the nature of the transition states.

Coiled coils are simple models for studying the association of two polypeptide chains to form a folded protein. Previous work has shown that the folding of a coiled coil can be described by a two-state transition between two unfolded monomeric peptide chains and a folded coiled coil dimer. Here we report the thermodynamic activation parameters for the folding and unfolding of two unrelated coiled coils: C62GCN4 and A(2). C62GCN4 corresponds to the 62 C-terminal residues of yeast transcription factor GCN4. The peptide forms a dimeric coiled coil through its 33 C-terminal residues. A(2) is a designed 30-residue dimeric coiled coil whose folding is induced by low pH [Dürr, E., Jelesarov, I., and Bosshard, H. R. (1999) Biochemistry 38, 870-880]. Folding and unfolding were assessed under identical native buffer conditions so that the microscopic reversibility applied and the transition state was the same for folding and unfolding. The time course of folding was followed from the self-quenching of a C-terminal fluorescent label (Texas Red). The overall folding of both peptides is enthalpy-driven and opposed by a loss of entropy. The main energetic changes occur after the system has passed the transition state. In the folding of C62GCN4, only 10-20% of the heat capacity change is attained between the monomeric state and the dimeric transition state. For coiled coil A(2), the fractional heat capacity change preceding the transition state is 30-40%. The results indicate that the activated states of folding of coiled coils are not well structured and differ considerably from the folded coiled coil conformation. These findings are in agreement with a rate-limiting transition state in which the coiled coil helices and the hydrophobic coiled coil interface are poorly developed.

Thermodynamics of trimer-of-hairpins formation by the SIV gp41 envelope protein.

The gp41 envelope protein mediates the entry of primate immunodeficiency viruses into target cells by promoting the fusion of viral and cellular membranes. The structure of the gp41 ectodomain core represents a trimer of identical helical hairpins in which a central trimeric coiled-coil made up of three amino-terminal helices is wrapped in an outer layer of three antiparallel carboxyl-terminal helices. Triggering formation of this fusion-active gp41 conformation appears to cause close membrane apposition and thus overcome the activation energy barrier for lipid bilayer fusion. We present a detailed description of the folding thermodynamics of the simian immunodeficiency virus (SIV) gp41 core by using a recombinant trimeric N34(L6)C28 model. Differential scanning calorimetry and spectroscopic experiments on denaturant-induced and thermal unfolding indicate that the free energy of association of three 68 residue N34(L6)C28 peptides to a trimer-of-hairpins is 76 kJ mol(-1) at pH 7.0 and 25 degrees C in physiological buffer. The associated enthalpy change, Delta H(unf), is 177 kJ mol(-1), while the entropy of unfolding, Delta S(unf), is 0.32 kJ K(-1) mol(-1). The temperature of maximal stability is close to 20 degrees C. The unfolding heat capacity increment is approximately 9 kJ K(-1) mol(-1) (approximately 45 J K(-1) mol residue(-1)), which is lower than expected for unfolding of the trimer to an extended and fully hydrated polypeptide chain. Replacement by isoleucine of the polar residues Thr582 or Thr586 buried in the N-terminal trimeric coiled-coil interface leads to very strong stabilization of the trimer-of-hairpins, 30-35 kJ mol(-1). Single-point mutations in the central coiled-coil thus strongly stabilize the gp41 core structure. These thermodynamic characteristics may be important for the refolding of the gp41 envelope protein into its fusion-active conformation during membrane fusion.

Chorismate synthase from the hyperthermophile Thermotoga maritima combines thermostability and increased rigidity with catalytic and spectral properties similar to mesophilic counterparts.

Chorismate synthase, the last enzyme in the shikimate pathway, catalyzes the transformation of 5-enolpyruvylshikimate 3-phosphate to chorismate, a biochemically unique reaction in that it requires reduced FMN as a cofactor. Here we report on the cloning, expression, and characterization of the protein for the first time from an extremophilic organism Thermotoga maritima which is also one of the oldest and most slowly evolving eubacteria. The protein is monofunctional in that it does not have an intrinsic ability to reduce the FMN cofactor and thereby reflecting the nature of the ancestral enzyme. Circular dichroism studies indicate that the melting temperature of the T. maritima protein is above 92 degrees C compared with 54 degrees C for the homologous Escherichia coli protein while analytical ultracentrifugation showed that both proteins have the same quaternary structure. Interestingly, UV-visible spectral studies revealed that the dissociation constants for both oxidized FMN and 5-enolpyruvylshikimate 3-phosphate decrease 46- and 10-fold, respectively, upon heat treatment of the T. maritima protein. The heat treatment also results in the trapping of the flavin cofactor in an apolar environment, a feature which is enhanced by the presence of the substrate 5-enolpyruvylshikimate 3-phosphate. Nevertheless, stopped-flow spectrophotometric evidence suggests that the mechanism of the T. maritima protein is similar to that of the E. coli protein. In essence, the study shows that T. maritima chorismate synthase exhibits considerably higher rigidity and thermostability while it has conserved features relevant to its catalytic function.

Reversible thermal transition in GrpE, the nucleotide exchange factor of the DnaK heat-shock system.

DnaK, a Hsp70 acting in concert with its co-chaperones DnaJ and GrpE, is essential for Escherichia coli to survive environmental stress, including exposure to elevated temperatures. Here we explored the influence of temperature on the structure of the individual components and the functional properties of the chaperone system. GrpE undergoes extensive but fully reversible conformational changes in the physiologically relevant temperature range (transition midpoint at approximately 48 degrees C), as observed with both circular dichroism measurements and differential scanning calorimetry, whereas no thermal transitions occur in DnaK and DnaJ between 15 degrees C and 48 degrees C. The conformational changes in GrpE appear to be important in controlling the interconversion of T-state DnaK (ATP-liganded, low affinity for polypeptide substrates) and R-state DnaK (ADP-liganded, high affinity for polypeptide substrates). The rate of the T --> R conversion of DnaK due to DnaJ-triggered ATP hydrolysis follows an Arrhenius temperature dependence. In contrast, the rate of the R --> T conversion due to GrpE-catalyzed ADP/ATP exchange increases progressively less with increasing temperature and even decreases at temperatures above approximately 40 degrees C, indicating a temperature-dependent reversible inactivation of GrpE. At heat-shock temperatures, the reversible structural changes of GrpE thus shift DnaK toward its high-affinity R state.

Interhelical ion pairing in coiled coils: solution structure of a heterodimeric leucine zipper and determination of pKa values of Glu side chains.

Residues of opposite charge often populate heptad positions g (heptad i on chain 1) and e' (heptad i + 1 on chain 2) in dimeric coiled coils and may stabilize the dimer by formation of interchain ion pairs. To investigate the contribution to stability of such electrostatic interactions we have designed a disulfide-linked heterodimeric zipper (AB zipper) consisting of the acidic chain Ac-E-VAQLEKE-VAQAEAE-NYQLEQE-VAQLEHE-CG-NH(2) and the basic chain Ac-E-VQALKKR-VQALKAR-NYAAKQK-VQALRHK-CG-NH(2) in which all e and g positions are occupied by either E or K/R to form a maximum of seven interhelical salt bridges. Temperature-induced denaturation experiments monitored by circular dichroism reveal a stable coiled coil conformation below 50 degrees C and in the pH range 1.2-8.0. Stability is highest at pH approximately 4.0 [DeltaG(U) (37 degrees C) = 5.18 +/- 0.51 kcal mol(-)(1)]. The solution structure of the AB zipper at pH 5.65 has been elucidated on the basis of homonuclear (1)H NMR data collected at 800 MHz [heavy atom rmsd's for the ensemble of 50 calculated structures are 0.47 +/- 0.13 A (backbone) and 0.95 +/- 0.16 A (all)]. Both chains of the AB zipper are almost entirely in alpha-helical conformation and form a superhelix with a left-handed twist. Overhauser connectivities reveal close contacts between g position residues (heptad i on chain 1) and residues d/f (heptad i on chain 1), residues a/d (heptad i + 1 on chain 1), and residue a' (heptad i + 1 on chain 2). Residues in position e (heptad i on chain 1) are in contact with residues a/b/d/f (heptad i on chain 1) and residue d' (heptad i on chain 2). These connectivities hint at a relatively defined alignment of the side chains across the helix interface. Partial H-bond formation between the functional groups of residues g and e'(+1) is observed in the calculated structures. NMR pH titration experiments disclose pK(a) values for Glu delta-carboxylate groups: 4.14 +/- 0.02 (E(1)), 4.82 +/- 0.07 (E(6)), 4.52 +/- 0.01 (E(8)), 4.37 +/- 0.03 (E(13)), 4.11 +/- 0.02 (E(15)), 4.41 +/- 0.07 (E(20)), 4.82 +/- 0.03 (E(22)), 4.65 +/- 0.04 (E(27)), 4.63 +/- 0.03 (E(29)), 4.22 +/- 0.02 (E(1)(')). By comparison with pK(a) of Glu in unfolded peptides ( approximately 4. 3 +/- 0.1), our pK(a) data suggest marginal or even unfavorable contribution of charged Glu to the stability of the AB zipper. The electrostatic energy gained from interhelical ion pairs is likely to be surpassed by hydrophobic energy terms upon protonation of Glu, due to increased hydrophobicity of uncharged Glu and, thus, better packing against apolar residues at the chain interface.

Compulsory order of substrate binding to herpes simplex virus type 1 thymidine kinase. A calorimetric study.

Isothermal titration calorimetry has been used to investigate the thermodynamic parameters of the binding of thymidine (dT) and ATP to herpes simplex virus type 1 thymidine kinase (HSV1 TK). Binding follows a sequential pathway in which dT binds first and ATP second. The free enzyme does not bind ATP, whose binding site becomes only accessible in the HSV1 TK.dT complex. At pH 7.5 and 25 degrees C, the binding constants are 1.9 x 10(5) m(-1) for dT and 3.9 x 10(6) m(-1) for ATP binding to the binary HSV1 TK.dT complex. Binding of both substrates is enthalpy-driven and opposed by a large negative entropy change. The heat capacity change (DeltaCp) obtained from DeltaH in the range of 10-25 degrees C is -360 cal K(-1) mol(-1) for dT binding and -140 cal K(-1) mol(-1) for ATP binding. These large DeltaCp values are incompatible with a rigid body binding model in which the dT and ATP binding sites pre-exist in the free enzyme. Values of DeltaCp and TDeltaS strongly indicate large scale conformational adaptation of the active site in sequential substrate binding. The conformational changes seem to be more pronounced in dT binding than in the subsequent ATP binding. Considering the crystal structure of the ternary HSV1 TK.dT.ATP complex, a large movement in the dT binding domain and a smaller but substantial movement in the LID domain are proposed to take place when the enzyme changes from the substrate-free, presumably more open and less ordered conformation to the closed and compact conformation of the ternary enzyme-substrate complex.

Thermodynamic analysis of cavity creating mutations in an engineered leucine zipper and energetics of glycerol-induced coiled coil stabilization.

Protein stability in vitro can be influenced either by introduction of mutations or by changes in the chemical composition of the solvent. Recently, we have characterized the thermodynamic stability and the rate of folding of the engineered dimeric leucine zipper A(2), which has a strengthened hydrophobic core [Dürr, E., Jelesarov, I., and Bosshard, H. R. (1999) Biochemistry 38, 870-880]. Here we report on the energetic consequences of a cavity introduced by Leu/Ala substitution at the tightly packed dimeric interface and how addition of 30% glycerol affects the folding thermodynamics of A(2) and the cavity mutants. Folding could be described by a two-state transition from two unfolded monomers to a coiled coil dimer. Removal of six methylene groups by Leu/Ala substitutions destabilized the dimeric coiled coil by 25 kJ mol(-1) at pH 3.5 and 25 degrees C in aqueous buffer. Destabilization was purely entropic at around room temperature and became increasingly enthalpic at elevated temperatures. Mutations were accompanied by a decrease of the unfolding heat capacity by 0.5 kJ K(-1) mol(-1). Addition of 30% glycerol increased the free energy of folding of A(2) and the cavity mutants by 5-10 kJ mol(-1) and lowered the unfolding heat capacity by 25% for A(2) and by 50% for the Leu/Ala mutants. The origin of the stabilizing effect of glycerol varied with temperature. Stabilization of the parent leucine zipper A(2) was enthalpic with an unfavorable entropic component between 0 and 100 degrees C. In the case of cavity mutants, glycerol induced enthalpic stabilization below 50 degrees C and entropic stabilization above 50 degrees C. The effect of glycerol could not be accounted for solely by the enthalpy and entropy of transfer or protein surface from water to glycerol/water mixture. We propose that in the presence of glycerol the folded coiled coil dimer is better packed and displays less intramolecular fluctuations, leading to enhanced enthalpic interactions and to an increase of the entropy of folding. This work demonstrates that mutational and solvent effects on protein stability can be thermodynamically complex and that it may not be sufficient to only analyze changes of enthalpy and entropy at the unfolding temperature (T(m)) to understand the mechanisms of protein stabilization.

The energetics of HMG box interactions with DNA: thermodynamic description of the target DNA duplexes.

The thermal properties and energetics of formation of 10, 12 and 16 bp DNA duplexes, specifically interacting with the HMG box of Sox-5, have been studied by isothermal titration calorimetry (ITC) and differential scanning calorimetry (DSC). DSC studies show that the partial heat capacity of these short duplexes increases considerably prior to the cooperative process of strand separation. Direct extrapolation of the pre and post-transition heat capacity functions into the cooperative transition zone suggests that unfolding/dissociation of strands results in no apparent heat capacity increment. In contrast, ITC measurements show that the negative enthalpy of complementary strand association increases in magnitude with temperature rise, implying that strand association proceeds with significant decrease of heat capacity. Furthermore, the ITC-measured enthalpy of strand association is significantly smaller in magnitude than the enthalpy of cooperative unfolding measured by DSC. To resolve this paradox, the heat effects upon heating and cooling of the separate DNA strands have been measured by DSC. This showed that cooling of the strands from 100 degrees C to -10 degrees C proceeds with significant heat release associated with the formation of intra and inter-molecular interactions. When the enthalpy of residual structure in the strands and the temperature dependence of the heat capacity of the duplexes and of their unfolded strands have been taken into account, the ITC and DSC results are brought into agreement. The analysis shows that the considerable increase in heat capacity of the duplexes with temperature rise is due to increasing fluctuations of their structure (e.g. end fraying and twisting) and this effect obscures the heat capacity increment resulting from the cooperative separation of strands, which in fact amounts to 200(+/-40) JK(-1) (mol bp)(-1). Using this heat capacity increment, the averaged standard enthalpy, entropy and Gibbs energy of formation of fully folded duplexes from fully unfolded strands have been determined at 25 degrees C as -33(+/-2) kJ (mol bp)(-1), -93(+/-4) J K(-1) (mol bp)(-1) and -5.0(+/-0.5) kJ (mol bp)(-1), respectively.

The energetics of HMG box interactions with DNA: thermodynamics of the DNA binding of the HMG box from mouse sox-5.

The energetics of the Sox-5 HMG box interaction with DNA duplexes, containing the recognition sequence AACAAT, were studied by fluorescence spectroscopy, isothermal titration calorimetry (ITC) and differential scanning calorimetry (DSC). Fluorescence titration showed that the association constant of this HMG box with the duplexes is of the order 4x10(7) M(-1), increasing somewhat with temperature rise, i.e. the Gibbs energy is -40 kJ mol(-1) at 5 degrees C, decreasing to -48 kJ mol(-1) at 32 degrees C. ITC measurements of the enthalpy of association over this temperature range showed an endothermic effect below 17 degrees C and an exothermic effect above, suggesting a heat capacity change on binding of about -4 kJ K(-1) mol(-1), a value twice larger than expected from structural considerations. A straightforward interpretation of ITC data in heat capacity terms assumes, however, that the heat capacities of all participants in the association reaction do not change over the considered temperature range. Our previous studies showed that over the temperature range of the ITC experiments the HMG box of Sox-5 starts to unfold, absorbing heat and the heat capacities of the DNA duplexes also increase significantly. These heat capacity effects differ from that of the DNA/Sox-5 complex. Correcting the ITC measured binding enthalpies for the heat capacity changes of the components and complex yielded the net enthalpies which exhibit a temperature dependence of about -2 kJ K(-1) mol(-1), in good agreement with that predicted on the basis of dehydration of the protein-DNA interface. Using the derived heat capacity change and the enthalpy and Gibbs energy of association measured at 5 degrees C, the net enthalpy and entropy of association of the fully folded HMG box with the target DNA duplexes was determined over a broad temperature range. These functions were compared with those for other known cases of sequence specific DNA/protein association. It appears that the enthalpy and entropy of association of minor groove binding proteins are more positive than for proteins binding in the major groove. The observed thermodynamic characteristics of protein binding to the A+T-rich minor groove of DNA might result from dehydration of both polar and non-polar groups at the interface and release of counterions. The expected entropy of dehydration was calculated and found to be too large to be compensated by the negative entropy of reduction of translational/rotational freedom. This implies that DNA/HMG box association proceeds with significant decrease of conformational entropy, i.e. reduction in conformational mobility.

Isothermal titration calorimetry and differential scanning calorimetry as complementary tools to investigate the energetics of biomolecular recognition.

The principles of isothermal titration calorimetry (ITC) and differential scanning calorimetry (DSC) are reviewed together with the basic thermodynamic formalism on which the two techniques are based. Although ITC is particularly suitable to follow the energetics of an association reaction between biomolecules, the combination of ITC and DSC provides a more comprehensive description of the thermodynamics of an associating system. The reason is that the parameters DeltaG, DeltaH, DeltaS, and DeltaCp obtained from ITC are global properties of the system under study. They may be composed to varying degrees of contributions from the binding reaction proper, from conformational changes of the component molecules during association, and from changes in molecule/solvent interactions and in the state of protonation.

Extremely fast folding of a very stable leucine zipper with a strengthened hydrophobic core and lacking electrostatic interactions between helices.

The dimer interface of a leucine zipper involves hydrophobic as well as electrostatic interactions between the component helices. Here we ask how hydrophobic effects and electrostatic repulsion balance the rate of folding and thermodynamic stability of a designed dimeric leucine zipper formed by the acidic peptide A that contains four repeating sequence units, (abcdefg)4. The aliphatic a and d residues of peptide A were the same as in the GCN4 leucine zipper but the e and g positions were occupied by Glu, which prevented folding above pH 6 because of electrostatic repulsion. Leucine zipper A2 was formed by protonation of the e and g side chains with a sharp transition midpoint at pH 5.2. Folding could be described by a two-state transition from two unfolded random coil monomers to a coiled coil dimer. There was a linear relationship between the logarithm of the rate constants and the number of repulsive charges on the folded leucine zipper dimer. The same linear relationship applied to the free energy of unfolding and the number of repulsive charges at thermodynamic equilibrium. Fully protonated peptide A folded at a near diffusion-limited rate (kon = 3 x 10(8) M-1 s-1), and the free energy of folding was -55 kJ mol-1 at 25 degrees C. The present work shows that protonation of Glu in positions e and g increases both the folding rate and the stability of the leucine zipper in the absence of any interhelical electrostatic interactions. Protonated Glu is proposed to act like a nonpolar residue and to strengthen the hydrophobic core by folding back toward the core residues in the a and d positions. This effect adds more to the free energy of unfolding and to the rate of folding than maximizing the number of salt bridges across the helix interface in an electrostatically stabilized heterodimeric leucine zipper [Wendt, H., Leder, L., Härmä, H., Jelesarov, I., Baici, A., and Bosshard, H. R. (1997) Biochemistry 36, 204-213].

Thermodynamics and kinetics of the reaction of a single-chain antibody fragment (scFv) with the leucine zipper domain of transcription factor GCN4.

Single-chain Fv (scFv) fragments of antibodies have become important analytical and therapeutic tools in biology and medicine. The reaction of scFv fragments has not been well-characterized with respect to the energetics and kinetics of antigen binding. This paper describes the thermodynamic and kinetic behavior of the high-affinity scFv fragment SW1 directed against the dimeric leucine zipper domain of the yeast transcription factor GCN4. The scFv fragment was selected by the phage display technique from the immune repertoire of a mouse that had been immunized with the leucine zipper domain of GCN4. The scFv fragment was produced in high yield in Escherichia coli inclusion bodies and refolded from the denatured state. Differential scanning calorimetry showed that SW1 was stable up to about 50 degreesC, but the subsequent thermal denaturation was irreversible (Tm approximately 68 degreesC). The scFv fragment specifically recognized the dimeric leucine zipper conformation. Two scFv fragments bound to the GCN4 dimer to form the complex (scFv)2-GCN4. Because of its repetitive structure, the rod-shaped GCN4 leucine zipper may present two similar epitopes for the scFv fragment. Surprisingly, the binding reaction was highly cooperative, that is, the species (scFv)2-GCN4 dominated over scFv-GCN4 even in the presence of a large excess of the antigen GCN4. It is speculated that cooperativity resulted from direct interaction between the two GCN4-bound scFv fragments. At 25 degreesC, the average binding enthalpy for a scFv fragment was favorable (-61 kJ mol-1), the entropy change was unfavorable, and the change in heat capacity was -1.27 +/- 0.14 kJ mol-1 K-1. As a result of enthalpy-entropy compensation, the free binding energy was virtually independent of temperature in the physiological temperature range. Antigen binding in solution could be described by a single-exponential reaction with an apparent rate constant of 1 x 10(6) M-1 s-1. Binding followed in a biosensor with the dimeric GCN4 coupled to the surface of the metal oxide sensor chip was 20 times slower.

Salt effects on hydrophobic interaction and charge screening in the folding of a negatively charged peptide to a coiled coil (leucine zipper).

The stability of a coiled coil or leucine zipper is controlled by hydrophobic interactions and electrostatic forces between the constituent helices. We have designed a 30-residue peptide with the repeating seven-residue pattern of a coiled coil, (abcdefg)n, and with Glu in positions e and g of each heptad. The glutamate side chains prevented folding at pH values above 6 because of electrostatic repulsion across the helix dimer interface as well as within the individual helices. Protonation of the carboxylates changed the conformation from a random coil monomer to a coiled coil dimer. Folding at alkaline pH where the peptide had a net charge of -7e was promoted by the addition of salts. The nature of the charge screening cation was less important than that of the anion. The high salt concentrations (>1 M) necessary to induce folding indicated that the salt-induced folding resulted from alterations in the protein-water interaction. Folding was promoted by the kosmotropic anions sulfate and fluoride and to a lesser extent by the weak kosmotrope formate, whereas chloride and the strong chaotrope perchlorate were ineffective. Kosmotropes are excluded from the protein surface, which is preferentially hydrated, and this promotes folding by strengthening hydrophobic interactions at the coiled coil interface. Although charge neutralization also contributed to folding, it was effective only when the screening cation was partnered by a good kosmotropic anion. Folding conformed to a two-state transition from random coil monomer to coiled coil dimer and was enthalpy driven and characterized by a change in the heat capacity of unfolding of 3.9 +/- 1.2 kJ mol-1 K-1. The rate of folding was analyzed by fluorescence stopped-flow measurements. Folding occurred in a biphasic reaction in which the rapid formation of an initial dimer (kf = 2 x 10(7) M-1 s-1) was followed by an equally rapid concentration-independent rearrangement to the folded dimer (k > 100 s-1).

Very rapid, ionic strength-dependent association and folding of a heterodimeric leucine zipper.

Leucine zippers (coiled coils) are dimerization motifs found in several DNA-binding transcription factors. A parallel leucine zipper composed of the acidic chain X1-EYQALEKEVAQLEAENX2-ALEKEVAQLEHEG-amide and the basic chain X1-EYQALKKKVAQLKAKNX2ALKKKVAQLKHKG-amide was designed to study the kinetics of folding of a heterodimeric leucine zipper and to investigate the role of electrostatic attraction between oppositely charged peptide chains to the folding reaction. Each peptide alone did not form a leucine zipper at ionic strength (mu) < 1 M because of electrostatic repulsion between like charges in a homodimer. Therefore, the formation of the heterodimeric leucine zipper could be investigated by simple mixing of acidic and basic chains. To monitor folding, a fluorescent label was located either at the N-terminus (X1 = fluorescein-GGG, X2 = Q) or in the center of the coiled coil (X1 = acetyl, X2 = W). Folding could be described by a simple two-state reaction involving the disordered monomers and the folded heterodimer. The same bimolecular rate constant (k(on)) was observed independent of the location of the fluorescent label, indicating that both fluorescence probes monitored the same reaction. Lowering of the ionic strength increased k(on) from 4 x 10(6) M-1 s-1 (mu = 525 mM) to about 5 x 10(7) M-1 s-1 (mu = 74 mM). When extrapolated to mu = O, k(on) was approximately 10(9) M-1 s-1, which is near the diffusion limit. In contrast, the rate of dissociation depended very weakly on ionic strength; k(off) decreased only by about 2-fold when mu was lowered from 525 to 74 mM. Equilibrium association constants (Ka) of the heterodimeric zippers measured directly and calculated from kinetic constants (Ka = k(on)/k(off) were in good agreement. The observed two-state mechanism, the strong dependence on ionic strength of k(on) but not of k(off), and the nearly diffusion-limited association rate at very low ionic strength point to a folding pathway in which the formation of an electrostatically stabilized dimeric intermediate may be rate-limiting and the subsequent folding to the final dimer is very rapid and follows a "down-hill" free energy landscape. The small increase of k(off) at increasing ionic strength indicates a minor contribution of electrostatics to the stability of the folded leucine zipper.

Coupled folding and site-specific binding of the GCN4-bZIP transcription factor to the AP-1 and ATF/CREB DNA sites studied by microcalorimetry.

The site-specific interaction of the basic leucine zipper protein C62GCN4, which corresponds to the C-terminal sequence 220-281 of the yeast transcription factor GCN4, with the AP-1 and ATF/ CREB DNA recognition sites was analyzed by isothermal titration microcalorimetry. Free C62GCN4 is a dimer composed of a C-terminal leucine zipper and a basic, mainly unstructured DNA binding domain. Upon association with the target DNA, C62GCN4 folds to a fully alpha-helical dimer [Ellenberger et al. (1992) Cell 71, 1223-1237; König and Richmond (1993) J. Mol. Biol. 233, 139-154]. The protein-bound AP-1 site is straight, and the protein-bound ATF/CREB site is bent by 20 degrees toward the leucine zipper domain. The coupling between protein folding and DNA association resulting in two conformationally different complexes with C62GCN4 poses interesting thermodynamic problems. The association was strongly exothermic for both DNA target sites. The free energies of binding were indistinguishable in buffers of low salt concentration, and no change of the protonation state of C62GCN4 and/or the DNA target site occurred on formation of the complexes. Both complexes exhibited large and negative heat capacity changes. The empirical correlation between buried nonpolar and polar surfaces and the reduction in heat capacity concomitant to complexation did hold for the reaction with the AP-1 site at low salt concentration. However, in the case of the ATF/CREB site, the change in heat capacity was larger than could be accounted for by the burial of solvent-accessible surface. Potential sources of the extra decrement in the heat capacity could be restrictions in the vibrational modes of polar groups and of bound water molecules at the protein-DNA interface, thought to result from the bending of the ATF/CREB site. In the presence of high concentrations of glutamate and NaCl, the complex with the ATF/CREB site was significantly weaker than the complex with the AP-1 site.

Thermodynamic characterization of the coupled folding and association of heterodimeric coiled coils (leucine zippers).

Folding thermodynamics of nine heterodimeric, parallel coiled coils were studied by isothermal titration calorimetry (ITC) and thermal unfolding circular dichroism measurements. The heterodimers were composed of an acidic and a basic 30-residue peptide, which when in isolation were monomeric and essentially unstructured. The reaction followed a two-state mechanism indicating that folding and association were coupled. delta Hfold, delta Sfold and delta Cp normalized per mol of residue were of the same magnitude as for monomeric globular proteins, hence the energetics of folding and association of the heterodimeric coiled coils was balanced similarly to the folding of a single polypeptide chain. Cavity creating Leu/Ala substitutions revealed strong and position-dependent energetic coupling between leucine residues in the hydrophobic core of the coiled coil. delta Gunfold (equivalent to -delta Gfold in the two-state reaction) was determined from thermal unfolding. Global stability curves were calculated according to the Gibbs-Helmholtz equation and using the combined free energy data from ITC and thermal unfolding. Maximum stabilities were between 15 and 37 degrees C and cold denaturation could be demonstrated by direct calorimetry. The stability curves were based on free energies of folding measured between 10 and 85 degrees C and under identical solvent conditions. This represents a novel experimental approach which circumvents the use of varying solvent conditions as is typically required to measure protein stability curves. Discrepancies were noticed between van't Hoff enthalpies deduced from thermal unfolding and measured by direct calorimetry. The discrepancies are thought to be due to residual ordered structure in the denatured single chains around room temperature but not near the transition midpoint temperature Tm. This demonstrates that over an extended temperature range the assumption of a common denatured state implicit in the van't Hoff analysis may not always be valid.

Probing the Energetics of Antigen-Antibody Recognition by Titration Microcalorimetry

Our understanding of the energetics that govern antigen-antibody recognition lags behind the increasingly rapid accumulation of structural information on antigen-antibody complexes. Thanks to the development of highly sensitive microcalorimeters, the thermodynamic parameters of antigen-antibody interactions can now be measured with precision and using only nanomole quantities of protein. The method of choice is isothermal titration calorimetry, in which a solution of the antibody (or antigen) is titrated with small aliquots of the antigen (or antibody) and the heat change accompanying the formation of the antigen-antibody complex is measured with a sensitivity as high as 0.1 μcal s-1. The free energy of binding (DeltaG), the binding enthalpy (DeltaH), and the binding entropy (DeltaS) are usually obtained from a single experiment, and no spectroscopic or radioactive label must be introduced into the antigen or antibody. The often large and negative change in heat capacity (DeltaCp) accompanying the formation of an antigen-antibody complex is obtained from DeltaH measured at different temperatures. The basic theory and the principle of the measurements are reviewed and illustrated by examples. The thermodynamic parameters relate to the dynamic physical forces that govern the association of the freely moving antigen and antibody into a well-structured and unique complex. This information complements the static picture of the antigen-antibody complex that results from X-ray diffraction analysis. Attempts to correlate dynamic and static aspects are discussed briefly.

Spectroscopic, calorimetric, and kinetic demonstration of conformational adaptation in peptide-antibody recognition.

Little is known about the extent to which protein flexibility contributes to antigen-antibody recognition and cross-reactivity. Using short coil peptides (leucine zippers) as model antigens, we demonstrate that a monoclonal antibody can force a noncognate peptide into a conformation that is similar to the conformation of the cognate peptide against which the monoclonal antibody is directed. Monoclonal antibodies 29AB and 13AD were raised against the 29-residue peptide LZ (Ac-EYEALEKKLAALEAKLQALEKKLEALEHG-amide) that forms a very stable coiled coil. The two antibodies cross-reacted strongly with the random coil analogue LZ(7P14P) that contains Lys-->Pro and Ala-->Pro substitutions in positions 7 and 14, respectively. The antibody-bound peptide LZ(7P14P) adopted an altered conformation that possibly was coiled coil-like, as shown by CD difference spectroscopy and fluorescence quenching experiments on coumarin-labeled peptides. Isothermal titration calorimetry revealed that the cross-reaction of antibodies 13AD and 29AB with the random coil peptide LZ(7P14P) exhibited a large unfavorable entropy. This, however, was strongly compensated by a more favorable enthalpy, resulting in only a small difference between the association constants for peptide LZ and LZ(7P14P), respectively. To investigate the opposite type of cross-reaction, monoclonal antibody 42PF was raised against the random coil peptide LZ(7P14P). 42PF cross-reacted with coiled coil peptide LZ by forcing it to dissociate into single chains. Enthalpy/entropy compensation again enabled the cross-reaction, which now was entropically favored and enthalpically disfavored. The rate of reaction of antibody 42PF with peptide LZ was controlled by the rate of dissociation of LZ into single chains. This observation, as well as the generally much slower reaction rate with the noncognate peptides, indicated that the cross-reactivity occurred because the antibody selected the conformer of the antigen that binds the strongest, a mechanism we call "induced fit by conformational selection."