Structure of the PPARalpha and -gamma ligand binding domain in complex with AZ 242; ligand selectivity and agonist activation in the PPAR family.

BACKGROUND: The peroxisome proliferator-activated receptors (PPAR) are ligand-activated transcription factors belonging to the nuclear receptor family. The roles of PPARalpha in fatty acid oxidation and PPARgamma in adipocyte differentiation and lipid storage have been characterized extensively. PPARs are activated by fatty acids and eicosanoids and are also targets for antidyslipidemic drugs, but the molecular interactions governing ligand selectivity for specific subtypes are unclear due to the lack of a PPARalpha ligand binding domain structure. RESULTS: We have solved the crystal structure of the PPARalpha ligand binding domain (LBD) in complex with the combined PPARalpha and -gamma agonist AZ 242, a novel dihydro cinnamate derivative that is structurally different from thiazolidinediones. In addition, we present the crystal structure of the PPARgamma_LBD/AZ 242 complex and provide a rationale for ligand selectivity toward the PPARalpha and -gamma subtypes. Heteronuclear NMR data on PPARalpha in both the apo form and in complex with AZ 242 shows an overall stabilization of the LBD upon agonist binding. A comparison of the novel PPARalpha/AZ 242 complex with the PPARgamma/AZ 242 complex and previously solved PPARgamma structures reveals a conserved hydrogen bonding network between agonists and the AF2 helix. CONCLUSIONS: The complex of PPARalpha and PPARgamma with the dual specificity agonist AZ 242 highlights the conserved interactions required for receptor activation. Together with the NMR data, this suggests a general model for ligand activation in the PPAR family. A comparison of the ligand binding sites reveals a molecular explanation for subtype selectivity and provides a basis for rational drug design.

Towards understanding a molecular switch mechanism: thermodynamic and crystallographic studies of the signal transduction protein CheY.

The signal transduction protein CheY displays an alpha/beta-parallel polypeptide folding, including a highly unstable helix alpha4 and a strongly charged active site. Helix alpha4 has been shown to adopt various positions and conformations in different crystal structures, suggesting that it is a mobile segment. Furthermore, the instability of this helix is believed to have functional significance because it is involved in protein-protein contacts with the transmitter protein kinase CheA, the target protein FliM and the phosphatase CheZ. The active site of CheY comprises a cluster of three aspartic acid residues and a lysine residue, all of which participate in the binding of the Mg(2+) needed for the protein activation. Two steps were followed to study the activation mechanism of CheY upon phosphorylation: first, we independently substituted the three aspartic acid residues in the active site with alanine; second, several mutations were designed in helix alpha 4, both to increase its level of stability and to improve its packing against the protein core. The structural and thermodynamic analysis of these mutant proteins provides further evidence of the connection between the active-site area and helix alpha 4, and helps to understand how small movements at the active site are transmitted and amplified to the protein surface.

Folding kinetics of Che Y mutants with enhanced native alpha-helix propensities.

In this work we study the folding kinetics of Che Y mutants in which the helical propensity of each of its five alpha-helices has been greatly enhanced by local interactions (between residues close in sequence). This constitutes an experimental test on the role of local interactions in protein folding, as well as providing new information on the details of the folding pathway of the protein Che Y. With respect to the first issue, our results show that the enhancement of helical propensities by native-like local interactions in Che Y has the following general effects: (1) the energetics of the whole Che Y folding energy landscape (folded state, intermediate, denatured state and main transition state) are affected by the enhancement of helical propensities, thus, native-like local interactions appear to have a low specificity for the native conformation; (2) our results support the idea, proposed from thermodynamic analysis of the mutants, that the denatured state under native conditions becomes more compact upon enhancement of helical propensities; (3) the rate of folding in aqueous solution decreases in all the mutants, suggesting that the optimization of the folding rate in this protein requires low secondary structure propensities. Regarding the description of the folding pathway of Che Y, we find evidence that the folding transition state of Che Y is constituted by two sub-domains with different degree of helical structure. The first includes helices 1 and 2 which are rather structured, while the second encompasses the last three helices, which are very unstructured. On the other hand, the same analysis for the folding intermediate indicates that all the five alpha-helices are, on average, rather structured. Thus, suggesting that a large structural reorganization of the last three alpha-helices must take place before folding can be completed. This conclusion indicates that the folding intermediate of Che Y is a misfolded species.

The three-dimensional structure of two mutants of the signal transduction protein CheY suggest its molecular activation mechanism.

The three-dimensional crystal structures of the single mutant M17G and the triple mutant F14G-S15G-M17G of the response regulator protein CheY have been determined to 2.3 and 1.9 angstrom, respectively. Both mutants bind the essential Mg2+ cation as determined by the changes in stability, but binding does not cause the intrinsic fluorescence quenching of W58 observed in the wild-type protein. The loop beta4-alpha4 appears to be very flexible in both mutants and helix alpha4, which starts at N94 in the native Mg2+-CheY and at K91 in the native apo-CheY, starts in both mutants at residue K92. The side-chain of K109 appears to be more mobile because of the space freed by the M17G mutation. In the triple mutant the main chain of K109 and adjacent residues (loop beta5-alpha5) is displaced almost by 2 angstrom affecting the main chain at residues T87 to E89 (C terminus of beta4). The triple mutant structure has a Mg2+ bound at the active site, but although the Mg2+ coordination is similar to that of the native Mg2+-CheY, the structural consequences of the metal binding are quite different. It seems that the mutations have disrupted the mechanism of movement transmission observed in the native protein. We suggest that the side-chain of K109, packed between V86, A88 and M17 in the native protein, slides forwards and backwards upon activation and deactivation dragging the main chain at the loop beta5-alpha5 and triggering larger movements at the functional surface of the protein.

Analysis of the effect of local interactions on protein stability.

BACKGROUND: Protein stability appears to be governed by non-covalent interactions. These can be local (between residues close in sequence) or non-local (medium-range and long-range interactions). The specific role of local interactions is controversial. Statistical mechanics arguments point out that local interactions must be weak in stable folded proteins. However, site-directed mutagenesis has revealed that local interactions make a significant contribution to protein stability. Finally, computer simulations suggest that correctly folded proteins require a delicate balance between local and non-local contributions to protein stability. RESULT: To analyze experimentally the effect of local interactions on protein stability, each of the five Che Y alpha-helices was enhanced in its helical propensity. alpha-Helix-promoting mutations have been designed, using a helix/coil transition algorithm tuned for heteropolypeptides, that do not alter the overall hydrophobicity or protein packing. The increase in helical propensity has been evaluated by far-UV CD analysis of the corresponding peptides. Thermodynamic analysis of the five Che Y mutants reveals, in all cases, an increase in half urea ([urea]1/2) and in Tm, and a decrease in the sensitivity to chemical denaturants (m). ANS binding assays indicate that the changes in m are not due to the stabilization of an intermediate, and the kinetic analysis of the mutants shows that their equilibrium unfolding transition can be considered as following a two-state model, while the change in m is found in the refolding reaction (m(k)f). CONCLUSIONS: These results are explained by a variable two-state model in which the changes in half urea and Tm arise from the stabilization of the native state and the decrease in m from the compaction of the denatured state. Therefore, the net change in protein stability in aqueous solution produced by increasing the contribution of native-like local interactions in Che Y is the balance between these two conflicting effects. Our results support the idea that optimization of protein stability and cooperativity involve a specific ratio of local versus non-local interactions.

Determination by NMR spectroscopy of the structure and conformational features of the enterobacterial common antigen isolated from Escherichia coli.

Complete 1H and 13C spectrum of a polysaccharide isolated from Escherichia coli, which is the major component of the enterobacterial common antigen, has been analyzed through two-dimensional nuclear magnetic resonance spectroscopy. In addition, distance constraints from NOESY and ROESY experiments have been combined with molecular dynamic simulations to determine its major conformation in water solution. Data resulting from both free dynamic simulations and restrained dynamic simulations have been compared with experimental data and discussed.

Investigating the structural determinants of the p21-like triphosphate and Mg2+ binding site.

Amongst the superfamily of nucleotide binding proteins, the classical mononucleotide binding fold (CMBF), is the one that has been best characterized structurally. The common denominator of all the members is the triphosphate/Mg2+ binding site, whose signature has been recognized as two structurally conserved stretches of residues: the Kinase 1 and 2 motifs that participate in triphosphate and Mg2+ binding, respectively. The Kinase 1 motif is borne by a loop (the P-loop), whose structure is conserved throughout the whole CMBF family. The low sequence similarity between the different members raises questions about which interactions are responsible for the active structure of the P-loop. What are the minimal requirements for the active structure of the P-loop? Why is the P-loop structure conserved despite the diverse environments in which it is found? To address this question, we have engineered the Kinase 1 and 2 motifs into a protein that has the CMBF and no nucleotide binding activity, the chemotactic protein from Escherichia coli, CheY. The mutant does not exhibit any triphosphate/Mg2+ binding activity. The crystal structure of the mutant reveals that the engineered P-loop is in a different conformation than that found in the CMBF. This demonstrates that the native structure of the P-loop requires external interactions with the rest of the protein. On the basis of an analysis of the conserved tertiary contacts of the P-loop in the mononucleotide binding superfamily, we propose a set of residues that could play an important role in the acquisition of the active structure of the P-loop.

Modeling of transmembrane seven helix bundles.

Transmembrane seven helix bundles form a large family of membrane inserted receptors and are responsible for a wide range of biological functions. Experimental data suggest that their overall structure is similar to bacteriorhodopsin. We describe here a new approach for the modeling of transmembrane seven helix bundles based on statistically derived environmental preference parameters combined with experimentally determined features of the receptors. The method was used to create a model for the human beta 2-adrenoreceptor. This model is physically plausible, is in reasonable agreement with experimental data and may be helpful in planning new receptor engineering experiments.