Two alternative conformations of S-adenosyl-L-homocysteine bound to Escherichia coli DNA adenine methyltransferase and the implication of conformational changes in regulating the catalytic cycle

The crystal structure of the Escherichia coli DNA adenine methyltransferase (EcoDam) in a binary complex with the cofactor product S-adenosyl-L-homocysteine (AdoHcy) unexpectedly showed the bound AdoHcy in two alternative conformations, extended or folded. The extended conformation represents the catalytically competent conformation, identical to that of EcoDam-DNA-AdoHcy ternary complex. The folded conformation prevents catalysis, because the homocysteine moiety occupies the target Ade binding pocket. The largest difference between the binary and ternary structures is in the conformation of the N-terminal hexapeptide ((9)KWAGGK(14)). Cofactor binding leads to a strong change in the fluorescence of Trp(10), whose indole ring approaches the cofactor by 3.3A(.) Stopped-flow kinetics and AdoMet cross-linking studies indicate that the cofactor prefers binding to the enzyme after preincubation with DNA. In the presence of DNA, AdoMet binding is approximately 2-fold stronger than AdoHcy binding. In the binary complex the side chain of Lys(14) is disordered, whereas Lys(14) stabilizes the active site in the ternary complex. Fluorescence stopped-flow experiments indicate that Lys(14) is important for EcoDam binding of the extrahelical target base into the active site pocket. This suggests that the hexapeptide couples specific DNA binding (Lys(9)), AdoMet binding (Trp(10)), and insertion of the flipped target base into the active site pocket (Lys(14)).     

Molecular mechanics simulation of the interaction of estrogen receptor with estrogen regulatory element.

A model for the interaction of 31 amino acid fragment (protein) from DNA binding domain of human estrogen receptor (hER) with a five base pair DNA sequence 5'GGTCA 3' from estrogen regulatory element (ERE) has been obtained using a step-wise procedure based on structural data on model peptides, DNA binding domain of hER, steric constrains imposed by tetrahedral coordination of the Cys sulphurs with zinc ion and classical secondary structural elements. Structure of the protein as well as its complex with DNA is obtained by energy minimization followed by refinement by molecular mechanics. The complex is stabilized by H-bonds between Lys22, Lys26 and Arg27 with DNA bases G2, T3 and T6. Lys22 also made H-bond with the backbone of G2. The backbone of Cys18 H-bonded with N7 of G1. DNA was in distorted B form and showed evidence of protein-induced conformational changes.     

Minor groove binding of a bis-quaternary ammonium compound: the crystal structure of SN 7167 bound to d(CGCGAATTCGCG)2.

The X-ray crystal structure of the complex between the synthetic antitumour and antiviral DNA binding ligand SN 7167 and the DNA oligonucleotide d(CGCGAATTCGCG)2 has been determined to an R factor of 18.3% at 2.6 A resolution. The ligand is located within the minor groove and covers almost 6 bp with the 1-methylpyridinium ring extending as far as the C9-G16 base pair and the 1-methylquinolinium ring lying between the G4-C21 and A5-T20 base pairs. The ligand interacts only weakly with the DNA, as evidenced by long range contacts and shallow penetration into the groove. This structure is compared with that of the complex between the parent compound SN 6999 and the alkylated DNA sequence d(CGC[e6G]AATTCGCG)2. There are significant differences between the two structures in the extent of DNA bending, ligand conformation and groove binding.     

The structures of RNase A complexed with 3'-CMP and d(CpA): active site conformation and conserved water molecules.

The interactions of RNase A with cytidine 3'-monophosphate (3'-CMP) and deoxycytidyl-3',5'-deoxyadenosine (d(CpA)) were analyzed by X-ray crystallography. The 3'-CMP complex and the native structure were determined from trigonal crystals, and the d(CpA) complex from monoclinic crystals. The differences between the overall structures are concentrated in loop regions and are relatively small. The protein-inhibitor contacts are interpreted in terms of the catalytic mechanism. The general base His 12 interacts with the 2' oxygen, as does the electrostatic catalyst Lys 41. The general acid His 119 has 2 conformations (A and B) in the native structure and is found in, respectively, the A and the B conformation in the d(CpA) and the 3'-CMP complex. From the present structures and from a comparison with RNase T1, we propose that His 119 is active in the A conformation. The structure of the d(CpA) complex permits a detailed analysis of the downstream binding site, which includes His 119 and Asn 71. The comparison of the present RNase A structures with an inhibitor complex of RNase T1 shows that there are important similarities in the active sites of these 2 enzymes, despite the absence of any sequence homology. The water molecules were analyzed in order to identify conserved water sites. Seventeen water sites were found to be conserved in RNase A structures from 5 different space groups. It is proposed that 7 of those water molecules play a role in the binding of the N-terminal helix to the rest of the protein and in the stabilization of the active site.     

"Dilysine trigger" in transferrins probed by mutagenesis of lactoferrin: crystal structures of the R210G,R210E,and R210L mutants of human lactoferrin

The mammalian iron-binding proteins lactoferrin (Lf) and transferrin (Tf) bind iron very tightly, but reversibly. Despite homologous structures and essentially identical iron binding sites, Tf begins to release iron at pH 6.0, whereas Lf retains iron to pH approximately 3.5. This difference in iron retention gives the two proteins different biological roles. Two lysine residues, Lys 206 and Lys 296, which form a hydrogen-bonded dilysine pair in human Tf, have been shown to strongly influence iron release from the N-lobe. The equivalent residues in human Lf are Arg 210 and Lys 301, and we have here mutated Arg 210 in the N-lobe half-molecule of human lactoferrin, Lf(N), to probe its role in iron release. The Lf(N) mutants R210G, R210E, and R210L were expressed, purified, and crystallized, and their crystal structures were determined and refined at resolutions of 1.95 A (R210G), 2.2 A (R210E), and 2.0 A (R210L). The overall structures are very similar to that of wild-type Lf(N), but with small differences in domain orientations. In each of the mutants, however, Lys 301 (equivalent to Lys 296 in Tf) changes its conformation to fill the space occupied by Arg 210 Neta2 in wild-type Lf(N), interacting with the two tyrosine ligands Tyr 92 and Tyr 192. By comparison with other Lf and Tf structures, we conclude that Lys 301 (or Lys 296 in Tf) only occupies this site when residue 210 (206 in Tf) is nonpositive (neutral as in R210G and R210L or negative as in R210E). Thus, Lys 206 in the Tf dilysine pair is identified as having a depressed pK(a). Three specific sites are variably occupied by polar groups in the Lf mutants and other Lf and Tf proteins, and when coupled with iron-release data, these give new insights into the factors that most influence iron retention at low pH.     

Met-Lys-双C肽人胰岛素原基因的构建表达及分离纯化

应用 Ｐ Ｃ Ｒ 定点突变方法构建编码 Ｍ ｅｔ Ｌｙｓ 双 Ｃ 肽人胰岛素原基因,并在大肠杆菌中以包含体方式获得表达 表达产物经还原、重组、 Ｓｅｐｈａｄｅｘ Ｇ ７５ 分离纯化,获得 Ｍ ｅｔ Ｌｙｓ 双 Ｃ 肽人胰岛素原,经胰蛋白酶与羧肽酶 Ｂ的酶解, Ｒｅｓｏｕｒｃｅ Ｔ Ｍ Ｑ 阴离子交换柱层析分离制备得人胰岛素,其放免活性、受体结合活性均与猪胰岛素相同      

Dissection of binding interactions in the complex between the anti-lysozyme antibody HyHEL-63 and its antigen

Alanine-scanning mutagenesis, X-ray crystallography, and double mutant cycles were used to characterize the interface between the anti-hen egg white lysozyme (HEL) antibody HyHEL-63 and HEL. Eleven HEL residues in contact with HyHEL-63 in the crystal structure of the antigen-antibody complex, and 10 HyHEL-63 residues in contact with HEL, were individually truncated to alanine in order to determine their relative contributions to complex stabilization. The residues of HEL (Tyr20, Lys96, and Lys97) most important for binding HyHEL-63 (Delta G(mutant) - Delta G(wild type) > 3.0 kcal/mol) form a contiguous patch at the center of the surface contacted by the antibody. Hot spot residues of the antibody (Delta Delta G > 2.0 kcal/mol) are organized in two clusters that juxtapose hot spot residues of HEL, resulting in energetic complementarity across the interface. All energetically critical residues are centrally located, shielded from solvent by peripheral residues that contribute significantly less to the binding free energy. Although HEL hot spot residues Lys96 and Lys97 make similar interactions with antibody in the HyHEL-63/HEL complex, alanine substitution of Lys96 results in a nearly 100-fold greater reduction in affinity than the corresponding mutation in Lys97. To understand the basis for this marked difference, we determined the crystal structures of the HyHEL-63/HEL Lys96Ala and HyHEL-63/HEL Lys97Ala complexes to 1.80 and 1.85 A resolution, respectively. Whereas conformational changes in the proteins and differences in the solvent networks at the mutation sites appear too small to explain the observed affinity difference, superposition of free HEL in different crystal forms onto bound HEL in the wild type and mutant HyHEL-63/HEL complexes reveals that the side-chain conformation of Lys96 is very similar in the various structures, but that the Lys97 side chain displays considerable flexibility. Accordingly, a greater entropic penalty may be associated with quenching the mobility of the Lys97 than the Lys96 side chain upon complex formation, reducing binding. To further dissect the energetics of specific interactions in the HyHEL-63/HEL interface, double mutant cycles were constructed to measure the coupling of 13 amino acid pairs, 11 of which are in direct contact in the crystal structure. A large coupling energy, 3.0 kcal/mol, was found between HEL residue Lys97 and HyHEL-63 residue V(H)Asp32, which form a buried salt bridge surrounded by polar residues of the antigen. Thus, in contrast to protein folding where buried salt bridges are generally destabilizing, salt bridges in protein-protein interfaces, whose residual composition is more hydrophilic than that of protein interiors, may contribute significantly to complex stabilization.     

Asymmetric assembly of Merkel cell polyomavirus large T-antigen origin binding domains at the viral origin

The double-stranded DNA polyomavirus Merkel cell polyomavirus (MCV) causes Merkel cell carcinoma, an aggressive but rare human skin cancer that most often affects immunosuppressed and elderly persons. As in other polyomaviruses, the large T-antigen of MCV recognizes the viral origin of replication by binding repeating G(A/G)GGC pentamers. The spacing, number, orientation, and necessity of repeats for viral replication differ, however, from other family members such as SV40 and murine polyomavirus. We report here the 2.9 Å crystal structure of the MCV large T-antigen origin binding domain (OBD) in complex with a DNA fragment from the MCV origin of replication. Consistent with replication data showing that three of the G(A/G)GGC-like binding sites near the center of the origin are required for replication, the crystal structure contains three copies of the OBD. This stoichiometry was verified using isothermal titration calorimetry. The affinity for G(A/G)GGC-containing double-stranded DNA was found to be ∼ 740 nM, approximately 8-fold weaker than the equivalent domain in SV40 for the analogous region of the SV40 origin. The difference in affinity is partially attributable to DNA-binding residue Lys331 (Arg154 in SV40). In contrast to SV40, a small protein-protein interface is observed between MCV OBDs when bound to the central region of the origin. This protein-protein interface is reminiscent of that seen in bovine papilloma virus E1 protein. Mutational analysis indicates, however, that this interface contributes little to DNA binding energy.     

Resolution of a disordered region at the entrance of the human sex hormone-binding globulin steroid-binding site

The crystal structure of human sex hormone-binding globulin (SHBG) has revealed how 5alpha-dihydrotestosterone intercalates between the two seven-stranded beta-sheets of its amino-terminal laminin G-like domain. However, a region of disorder (residues 130 to 135 of SHBG) was identified together with a zinc-binding site in immediate proximity to the steroid. It has been important to resolve the structure of this region because previous studies have suggested that these residues may contribute to steroid binding directly. Here, we present the 2.35 A and 1.7 A crystal structures of the amino-terminal LG domain of SHBG obtained from a tetragonal crystal form and by EDTA-soaking of a trigonal crystal form, respectively. In both of these new structures, residues Pro130 to Arg135 are now clearly visible. Substitution of the two residues (Leu131Gly and Lys134Ala) pointing towards the steroid has shown that only Leu131 contributes significantly to steroid binding. Rather than covering the steroid-binding pocket in an extended conformation, a 3(10) helical turn is formed by residues Leu131 to Lys134 in this segment. Unfolding of this secondary structure element can either facilitate the entry of the steroids into the binding site or modulate the important contribution that Leu131 makes to steroid binding. A comparison with previous structures supports the concept that zinc binding re-orients the side-chain of His136, and this residue serves as a lever causing disorder within the loop structure between Pro130 and Arg135.     

Transcription regulation by steroid hormones: a computer simulation study.

Three-dimensional structures of complexes of 66 amino acid-DNA binding domains of human progesterone (hPR), estrogen (hER) and glucocorticoid (hGR) receptors (proteins), with ten base pair DNA duplexes: d(AGGTCATGCT).d(AGCATGACCT) and d(AGAACATGCT).d(AGCATGTTCT) were obtained using computer modeling and molecular mechanics techniques. Cartesian coordinates for the proteins were obtained from: 1) structural data of hER and hGR by NMR spectroscopy; 2) steric constraints imposed by tetrahedral coordination of the zinc ion to Cys residues, and 3) energy minimization in torsional and cartesian space. The proteins were made to interact with DNA (in B-form) in major groove through alpha-helical linker between the two zinc fingers. The geometry of the complexes was obtained by allowing them to slide, glide, penetrate in to and out of the groove, and to rotate about the helical axis. The complexes were energy minimized. Also maximized was the number of H-bonds between proteins and DNA. The complex structures were refined by molecular mechanics using AMBER 3.0. Structural parameters of DNA were analyzed in each complex and compared with those of native DNA optimized separately. The stereochemical differences of the complexes are discussed.     

Substrate-assisted movement of the catalytic Lys 215 during domain closure: site-directed mutagenesis studies of human 3-phosphoglycerate kinase

3-Phosphoglycerate kinase (PGK) is a two-domain hinge-bending enzyme. It is still unclear how the geometry of the active site is formed during domain closure and how the catalytic residues are brought into the optimal position for the reaction. Comparison of the three-dimensional structures in various open and closed conformations suggests a large (10 A) movement of Lys 215 during domain closure. This change would be required for direct participation of this side chain in both the catalyzed phospho transfer and the special anion-caused activation. To test the multiple roles of Lys 215, two mutants (K215A and K215R) were constructed from human PGK and characterized in enzyme kinetic and substrate binding studies. For comparison, mutants (R38A and R38K) of the known essential residue, Arg 38, were also produced. Drastic decreases (1500- and 500-fold, respectively), as in the case of R38A, were observed in the kcat values of mutants K215A and K215R, approving the essential catalytic role of Lys 215. In contrast, the R38K mutation caused an only 1.5-fold decrease in activity. This emphasizes the importance of a very precise positioning of Lys 215 in the active site, in addition to its positive charge. The side chain of Lys 215 is also responsible for the substrate and anion-dependent activation, since these properties are abolished upon mutation. Among the kinetic constants mainly the Km values of MgATP and 1,3-BPG are increased (approximately 20- and approximately 8-fold, respectively) in the case of the neutral K215A mutant, evidence of the interaction of Lys 215 with the transferring phospho group in the functioning complex. Weakening of MgATP binding (a moderate increase in Kd), but not of MgADP binding, upon mutation indicates an initial weak interaction of Lys 215 with the gamma-phosphate already in the nonfunctioning open conformation. Thus, during domain closure, Lys 215 possibly moves together with the transferring phosphate; meanwhile, this group is being positioned properly for catalysis.     

Thermodynamic criterion for the conformation of P1 residues of substrates and of inhibitors in complexes with serine proteinases.

Eglin c, turkey ovomucoid third domain, and bovine pancreatic trypsin inhibitor (Kunitz) are all standard mechanism, canonical protein inhibitors of serine proteinases. Each of the three belongs to a different inhibitor family. Therefore, all three have the same canonical conformation in their combining loops but differ in their scaffoldings. Eglin c (Leu45 at P1) binds to chymotrypsin much better than its Ala45 variant (the difference in standard free energy changes on binding is -5.00 kcal/mol). Similarly, turkey ovomucoid third domain (Leu18 at P1) binds to chymotrypsin much better than its Ala18 variant (the difference in standard free energy changes on binding is -4.70 kcal/mol). As these two differences are within the +/-400 cal/mol bandwidth (expected from the experimental error), one can conclude that the system is additive. On the basis that isoenergetic is isostructural, we expect that within both the P1 Ala pair and the P1 Leu pair, the conformation of the inhibitor's P1 side chain and of the enzyme's specificity pocket will be identical. This is confirmed, within the experimental error, by the available X-ray structures of complexes of bovine chymotrypsin Aalpha with eglin c () and with turkey ovomucoid third domain (). A comparison can also be made between the structures of P1 (Lys+)15 of bovine pancreatic trypsin inhibitor (Kunitz) ( and ) and of the P1 (Lys+)18 variant of turkey ovomucoid third domain (), both interacting with chymotrypsin. In this case, the conformation of the side chains is strikingly different. Bovine pancreatic trypsin inhibitor with (Lys+)15 at P1 binds to chymotrypsin more strongly than its Ala15 variant (the difference in standard free energy changes on binding is -1.90 kcal/mol). In contrast, turkey ovomucoid third domain variant with (Lys+)18 at P1 binds to chymotrypsin less strongly than its Ala18 variant (the difference in standard free energies of association is 0.95 kcal/mol). In this case, P1 Lys+ is neither isostructural nor isoenergetic. Thus, a thermodynamic criterion for whether the conformation of a P1 side chain in the complex matches that of an already determined one is at hand. Such a criterion may be useful in reducing the number of required X-ray crystallographic structure determinations. More importantly, the criterion can be applied to situations where direct determination of the structure is extremely difficult. Here, we apply it to determine the conformation of the Lys+ side chain in the transition state complex of a substrate with chymotrypsin. On the basis of kcat/KM measurements, the difference in free energies of activation for Suc-AAPX-pna when X is Lys+ and X is Ala is 1.29 kcal/mol. This is in good agreement with the corresponding difference for turkey ovomucoid third domain variants but in sharp contrast to the bovine pancreatic trypsin inhibitor (Kunitz) data. Therefore, we expect that in the transition state complex of this substrate with chymotrypsin, the P1 Lys+ side chain is deeply inserted into the enzyme's specificity pocket as it is in the (Lys+)18 turkey ovomucoid third domain complex with chymotrypsin.     

The structural basis of the kinetic mechanism of a gap-filling X-family DNA polymerase that binds Mg(2+)-dNTP before binding to DNA

DNA with single-nucleotide (1-nt) gaps can arise during various DNA processing events. These lesions are repaired by X-family DNA polymerases (PolXs) with high gap-filling activity. Some PolXs can bind productively to dNTPs in the absence of DNA and fill these 1-nt gaps. Although PolXs have a crucial role in efficient gap filling, currently, little is known of the kinetic and structural details of their productive dNTP binding. Here, we show that Thermus thermophilus HB8 PolX (ttPolX) had strong binding affinity for Mg(2+)-dNTPs in the absence of DNA and that it follows a Theorell-Chance (hit-and-run) mechanism with nucleotide binding first. Comparison of the intermediate crystal structures of ttPolX in a binary complex with dGTP and in a ternary complex with 1-nt gapped DNA and Mg(2+)-ddGTP revealed that the conformation of the incoming nucleotide depended on whether or not DNA was present. Furthermore, the Lys263 residue located between two guanosine conformations was essential to the strong binding affinity of the enzyme. The ability to bind to either syn-dNTP or anti-dNTP and the involvement of a Theorell-Chance mechanism are key aspects of the strong nucleotide-binding and efficient gap-filling activities of ttPolX.     

Crystal structures of BnSP-7 and BnSP-6, two Lys49-phospholipases A(2): quaternary structure and inhibition mechanism insights

Phospholipases A(2) are components of Bothrops venoms responsible for disruption of cell membrane integrity via hydrolysis of its phospholipids. A class of PLA(2)-like proteins has been described which despite PLA(2) activity on artificial substrate, due to a D49K mutation, is still highly myonecrotic. This work reports the X-ray structure determination of two Lys49-PLA(2)s from Bothrops neuwiedi pauloensis (BnSP-7 and BnSP-6) and, for the first time, the comparison of eight dimeric Lys49-PLA(2)s. This comparison reveals that there are not just two ("open" and "closed") but at least six different conformations. The binding of fatty acid observed in three recent Lys49-PLA(2) structures seems to be independent of their quaternary conformation. Cys29 polarization by Lys122 is not significant for BnSP-7 and BnSP-6 or other structures not bound by fatty acids. These structures may be in an "active" state when nothing is bound to them and the Lys122/Cys29 interactions are weak or absent.     

Structure of a complex between yeast hexokinase A and glucose: II. Detailed comparisons of conformation and active site configuration with the native hexokinase B monomer and dimer

Detailed comparison of the refined crystal structures of the hexokinase A: glucose complex (HKA · G) and native hexokinase B shows that, in addition to the 12 ° rotation of one lobe of the enzyme relative to the other as described previously (Bennett & Steitz, 1978) there are small systematic differences in the conformation of the polypeptide backbones of the two structures adjacent to the glucose binding site and crystal packing contacts. In the HKA · G complex, the cleft between the two lobes of the hexokinase molecule is narrowed, substantially reducing the accessibility of the active site to solvent. The HKA · G structure suggests specific contacts with a bound glucose molecule that cannot form in the more open native structure. The closed conformation of the HKA · G complex can be formed by either subunit in the heterologous dimer configuration of hexokinase B (Anderson et al. 1974); new or different interactions between subunits, or with ligands bound to the intersubunit ATP site, may be made when the upper subunit of the dimer is in the closed conformation and may contribute to the cooperative interactions observed in the crystalline dimer and in solution.     

Structure of the major single-stranded DNA-binding domain of replication protein A suggests a dynamic mechanism for DNA binding

Although structures of single-stranded (ss)DNA-binding proteins (SSBs) have been reported with and without ssDNA, the mechanism of ssDNA binding in eukarya remains speculative. Here we report a 2.5 Angstroms structure of the ssDNA-binding domain of human replication protein A (RPA) (eukaryotic SSB), for which we previously reported a structure in complex with ssDNA. A comparison of free and bound forms of RPA revealed that ssDNA binding is associated with a major reorientation between, and significant conformational changes within, the structural modules--OB-folds--which comprise the DNA-binding domain. Two OB-folds, whose tandem orientation was stabilized by the presence of DNA, adopted multiple orientations in its absence. Within the OB-folds, extended loops implicated in DNA binding significantly changed conformation in the absence of DNA. Analysis of intermolecular contacts suggested the possibility that other RPA molecules and/or other proteins could compete with DNA for the same binding site. Using this mechanism, protein-protein interactions can regulate, and/or be regulated by DNA binding. Combined with available biochemical data, this structure also suggested a dynamic model for the DNA-binding mechanism.     

Conformational changes within the HLA‐A1:MAGE‐A1 complex induced by binding of a recombinant antibody fragment with TCR‐like specificity

Although there is X‐ray crystallographic evidence that the interaction between major histocompatibility complex (MHC, in humans HLA) class I molecules and T cell receptors (TCR) or killer cell Ig‐like receptors (KIR) may be accompanied by considerable changes in the conformation of selected residues or even entire loops within TCR or KIR, conformational changes between receptor‐bound and ‐unbound MHC class I molecules of comparable magnitude have not been observed so far. We have previously determined the structure of the MHC class I molecule HLA‐A1 bound to a melanoma antigen‐encoding gene (MAGE)‐A1‐derived peptide in complex with a recombinant antibody fragment with TCR‐like specificity, Fab‐Hyb3. Here, we compare the X‐ray structure of HLA‐A1:MAGE‐A1 with that complexed with Fab‐Hyb3 to gain insight into structural changes of the MHC molecule that might be induced by the interaction with the antibody fragment. Apart from the expulsion of several water molecules from the interface, Fab‐Hyb3 binding results in major rearrangements (up to 5.5 Å) of heavy chain residues Arg65, Gln72, Arg145, and Lys146. Residue 65 is frequently and residues 72 and 146 are occasionally involved in TCR binding‐induced conformational changes, as revealed by a comparison with MHC class I structures in TCR‐liganded and ‐unliganded forms. On the other hand, residue 145 is subject to a reorientation following engagement of HLA‐Cw4 and KIR2DL1. Therefore, conformational changes within the HLA‐A1:MAGE‐A1:Fab‐Hyb3 complex include MHC residues that are also involved in reorientations in complexes with natural ligands, pointing to their central importance for the peptide‐dependent recognition of MHC molecules.     

Molecular mechanism underlying inverse agonist of angiotensin II type 1 receptor

To delineate the molecular mechanism underlying the inverse agonist activity of olmesartan, a potent angiotensin II type 1 (AT1) receptor antagonist, we performed binding affinity studies and an inositol phosphate production assay. Binding affinity of olmesartan and its related compounds to wild-type and mutant AT1 receptors demonstrated that interactions between olmesartan and Tyr113, Lys199, His256, and Gln257 in the AT1 receptor were important. The inositol phosphate production assay of olmesartan and related compounds using mutant receptors indicated that the inverse agonist activity required two interactions, that between the hydroxyl group of olmesartan and Tyr113 in the receptor and that between the carboxyl group of olmesartan and Lys199 and His256 in the receptor. Gln257 was found to be important for the interaction with olmesartan but not for the inverse agonist activity. Based on these results, we constructed a model for the interaction between olmesartan and the AT1 receptor. Although the activation of G protein-coupled receptors is initiated by anti-clockwise rotation of transmembrane (TM) III and TM VI followed by changes in the conformation of the receptor, in this model, cooperative interactions between the hydroxyl group and Tyr113 in TM III and between the carboxyl group and His256 in TM VI were essential for the potent inverse agonist activity of olmesartan. We speculate that the specific interaction of olmesartan with these two TMs is essential for stabilizing the AT1 receptor in an inactive conformation. A better understanding of the molecular mechanisms of the inverse agonism could be useful for the development of new G protein-coupled receptor antagonists with inverse agonist activity.