Tesis doctoral
Departament de Bioquímica i de Biologia Molecular
DEVELOPMENT AND APPLICATION OF COMPUTATIONAL TECHNIQUES TO DRUG DISCOVERY AND STRUCTURE-FUNCTION RELATIONSHIPS
Jose Carlos Gómez Tamayo
Mireia Dunach Masjuan Tutor Gianluigi Caltabiano Arnau Cordomí Montoya Director
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'*3 53 && & * 3 5 53((*" !353&" $+3553*#+3'* +%&3 553*,"23 553 "'+$'/+#"3 53& '035 58<::C9-++"&:C3 ."+"'&5:;5$$"& '* Cluster Number P θ Distance criteria I 191 (24%) 0-45º 0-70º d(R-Sδ) < d(R-Cγ) v d(R-Sδ) < d(R-Cε) II 131 (37%) 45-90º 0-70º d(R-Sδ) < d(R-Cγ) v d(R-Sδ) < d(R-Cε) III 181 (12%) 0-90º 0-90º d(R-Sδ) > d(R-Cγ) ^ d(R-Sδ) > d(R- Cε) IV 204 (28%) 0-90º 70-90º - Table S1. Cluster analysis of Met-Phe interactions in crystal structures. Number (and percentage) of Met-Phe interactions and values of P (angle between the planes defined by Cγ, Sδ and Cε atoms of Met and the aromatic ring of Phe) and θ (angle between the normal vector of the plane defined by the aromatic ring of Phe and the vector connecting the centroid R of the aromatic ring of Phe and Sδ of Met), and distance criteria (R accounts for the centroid of the aromatic ring of Phe, and Sδ, Cγ and Cε represent the atoms of the Met side-chain), in clusters I-IV (see Fig 1). Cluster Number P θ Distance criteria [d(SδA-SδB) < d(SδA-CγΒ) v d(SδA-SδB) < d(SδA-CεΒ )] ^ I 26 (11%) 0-45º 0-60º [d(SδA-SδB) < d(SδB-CγAv d(SδA-SδB) < d(SδB-CεA )] [d(SδA-SδB) < d(SδA-CγΒ) v d(SδA-SδB) < d(SδA-CεΒ )] ^ II 71 (46%) 45º-90º 0-60º [d(SδA-SδB) < d(SδB-CγAv d(SδA-SδB) < d(SδB-CεA )] [d(SδA-SδB) < d(SδA-CγΒ) ^ d(SδA-SδB) < d(SδA-CεΒ )] ^ III 12 (5%) 0-90º 60-90º [d(SδA-SδB) < d(SδB-CγA^ d(SδA-SδB) < d(SδB-CεA )] [d(SδA-SδB) > d(SδA-CγΒ) v d(SδA-SδB) > d(SδA-CεΒ )] ^ IV 43 (15%) 0-90º 60-90º [d(SδA-SδB) < d(SδB-CγAv d(SδA-SδB) < d(SδB-CεA )] [d(SδA-SδB) > d(SδA-CγΒ) ^ d(SδA-SδB) > d(SδA-CεΒ )] ^ V 47 (25%) 0-90º 0-90º [d(SδA-SδB) > d(SδB-CγAv d(SδA-SδB) > d(SδB-CεA )] Table S2. Cluster analysis of Met-Met interactions in crystal structures. Number (and percentage) of Met-Met interactions and values of P (angle between the planes defined by Cγ, Sδ and Cε atoms of Met) and θ (angle between the normal vector of the plane defined by the Cγ, Sδ and Cε atoms of Met and the vector connecting the Sδ atoms of Met), and distance criteria (sub indexes A and B refer to atoms in distinct side-chains) in clusters I-V (see Fig 2). Cluster Number P θ Distance criteria [d(SδA-SδB) < d(SδA-CγΒ) v d(SδA-SδB) < d(SδA-CεΒ )] ^ I 26 (11%) 0-45º 0-60º [d(SδA-SδB) < d(SδB-CγAv d(SδA-SδB) < d(SδB-CεA )] [d(SδA-SδB) < d(SδA-CγΒ) v d(SδA-SδB) < d(SδA-CεΒ )] ^ II 71 (46%) 45º-90º 0-60º [d(SδA-SδB) < d(SδB-CγAv d(SδA-SδB) < d(SδB-CεA )] [d(SδA-SδB) < d(SδA-CγΒ) ^ d(SδA-SδB) < d(SδA-CεΒ )] ^ III 12 (5%) 0-90º 60-90º [d(SδA-SδB) < d(SδB-CγA^ d(SδA-SδB) < d(SδB-CεA )] [d(SδA-SδB) > d(SδA-CγΒ) v d(SδA-SδB) > d(SδA-CεΒ )] ^ IV 43 (15%) 0-90º 60-90º [d(SδA-SδB) < d(SδB-CγAv d(SδA-SδB) < d(SδB-CεA )] [d(SδA-SδB) > d(SδA-CγΒ) ^ d(SδA-SδB) > d(SδA-CεΒ )] ^ V 47 (25%) 0-90º 0-90º [d(SδA-SδB) > d(SδB-CγAv d(SδA-SδB) > d(SδB-CεA )] Table S3. Cluster analysis of Met-Leu interactions in crystal structures. Number (and percentage) of Met-Leu interactions and values of P (angle between the planes defined by the Cγ, Sδ and Cε atoms of Met and the Cδ1, Cγ and Cδ2 atoms of Leu), θ (angle between the normal vector of the plane defined by the Cγ, Sδ and Cε atoms of Met and the vector connecting the Sδ atom of Met and the Cγ atom of Leu) and distance criteria (subindexes A and B refer to atoms in distinct side-chains) in clusters I-V (see Fig 3). Figure S1. Small-molecule models systems mimicking Met-Phe interactions. Geometry optimized, at the ab-initio MP2/6-31+G(d,p) level of theory, of the interactions between benzene (BNZ, mimicking Phe) and dimethyl sulfide (DMS, mimicking Met), dimethyl ether (DME), and propane (PRP, mimicking Leu). Each optimized structure is designated by an arabic number that corresponds to a roman number of the obtained clusters in crystal structures (see Fig 1). The values of d, P, and θ (see Suppl. Table 1 and Fig 1 for definition), and single point energy calculations at the ab-initio CCSD(T)/6-311+G(3df,2p) level of theory (ECCSD) and by molecular mechanics using the AMBER99 forcefield (EAMBER) are shown. Figure S2. Small-molecule models systems mimicking Phe-Phe interactions. Geometry optimized models, at the ab-initio MP2/6-31+G(d,p) level of theory, of benzene-benzene (BNZ, mimicking Phe) interactions in the lowest parallel displaced and T-shaped energy configurations. The values of d (calculated as the distance between the centroid R of the aromatic ring of BNZ), P (calculated as the angle between the planes defined by the aromatic rings of BNZ), and θ (angle between the normal vector of the plane defined by the aromatic ring of Phe and the vector connecting the centroids R of the aromatic rings of BNZ), and single point energy calculations at the ab-initio CCSD(T)/6-311+G(3df,2p) level of theory (ECCSD) and by molecular mechanics using the AMBER99 forcefield (EAMBER). Figure S3. Small-molecule models systems mimicking Met-Met interactions. Geometry optimized models, at the ab-initio MP2/6-31+G(d,p) level of theory, of dimethyl sulfide (DMS, mimicking Met)- DMS and dimethyl ether (DME)-DME interactions. Each energy-minimized structure is designated by an arabic number that corresponds to a roman number of the obtained clusters in crystal structures (see Fig 2). The values of d, P, and θ (see Suppl. Table 2 and Fig 2 for definition), and single point energy calculations at the ab-initio CCSD(T)/6-311+G(3df,2p) level of theory (ECCSD) and by molecular mechanics using the AMBER99 forcefield (EAMBER) are shown. Figure S4. Small-molecule models systems mimicking Met-Leu interactions. Geometry optimized models, at the ab-initio MP2/6-31+G(d,p) level of theory, of dimethyl sulfide (DMS, mimicking Met) and propane (PRP, mimicking Leu) and PRP-PRP interactions. Each optimized structure is designated by an arabic number that corresponds to a roman number of the obtained clusters in crystal structures (see Fig 3). The values of d, P, and θ (see Suppl. Table 3 and Fig 3 for definition), and single point energy calculations at the ab-initio CCSD(T)/6-311+G(3df,2p) level of theory (ECCSD) and by molecular mechanics using the AMBER99 forcefield (EAMBER) are shown. Figure S5. Small-molecule models systems mimicking Cys-Phe, Cys-Met and Cys-Leu interactions. Geometry optimized models, at the ab-initio MP2/6-31+G(d,p) level of theory, of the interactions between methanethiol (MT, mimicking Cys) and benzene (BNZ, mimicking Phe), dimethyl sulfide (DMS, mimicking Met) and propane (PRP, mimicking Leu). 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