| Literature DB >> 22581768 |
Pierre Thévenet1, Yimin Shen, Julien Maupetit, Frédéric Guyon, Philippe Derreumaux, Pierre Tufféry.
Abstract
In the context of the renewed interest of peptides as therapeutics, it is important to have an on-line resource for 3D structure prediction of peptides with well-defined structures in aqueous solution. We present an updated version of PEP-FOLD allowing the treatment of both linear and disulphide bonded cyclic peptides with 9-36 amino acids. The server makes possible to define disulphide bonds and any residue-residue proximity under the guidance of the biologists. Using a benchmark of 34 cyclic peptides with one, two and three disulphide bonds, the best PEP-FOLD models deviate by an average RMS of 2.75 Å from the full NMR structures. Using a benchmark of 37 linear peptides, PEP-FOLD locates lowest-energy conformations deviating by 3 Å RMS from the NMR rigid cores. The evolution of PEP-FOLD comes as a new on-line service to supersede the previous server. The server is available at: http://bioserv.rpbs.univ-paris-diderot.fr/PEP-FOLD.Entities:
Mesh:
Substances:
Year: 2012 PMID: 22581768 PMCID: PMC3394260 DOI: 10.1093/nar/gks419
Source DB: PubMed Journal: Nucleic Acids Res ISSN: 0305-1048 Impact factor: 16.971
Figure 1.PEP-FOLD 2012 flowchart.
Results obtained for 13 linear peptides with 25–36 residues
| PDB id | Top | L | RC | sOPEP | best5 | |||
|---|---|---|---|---|---|---|---|---|
| FS-d | RC-d | FS-d | RC-d | Rnk | ||||
| 1by0 | a | 27 | 1:23 | 4.36 | 1.75 | 2.94 | 1.74 | 1 |
| 1yyb | a | 27 | 1:20 | 6.49 | 1.47 | 3.4 | 1.42 | 1 |
| 2kbl | b2 | 29 | 3:4|6:27 | 4.68 | 3.91 | 4.68 | 3.91 | 1 |
| 1fsd | ab2 | 28 | 1:26 | 4.14 | 3.88 | 3.91 | 3.66 | 1 |
| 1psv | ab2 | 28 | 2:25 | 7.19 | 7.44 | 4.61 | 4.6 | 4 |
| 2k76 | ba | 30 | 4:29 | 3.15 | 2.75 | 2.1 | 1.88 | 1 |
| 2gdl | aca | 31 | 8:8|10:11|14:15|21:29 | 7.57 | 4.84 | 6.53 | 4.57 | 3 |
| 2l0g | a2 | 32 | 5:32 | 4.53 | 3.32 | 2.1 | 1.64 | 1 |
| 2bn6 | a2 | 33 | 4:29 | 4.49 | 3.18 | 3.09 | 2.14 | 1 |
| 1e0n | b3 | 35 | 1:25 | 2.16 | 2.16 | 1.68 | 1.68 | 2 |
| 1wr3 | b3 | 36 | 5:15 | 5.72 | 3.74 | 4.26 | 3.5 | 1 |
| 1wr4 | b3 | 36 | 5:34 | 4.68 | 3.26 | 4.68 | 3.26 | 1 |
| 2ki0 | bab | 36 | 5:11|13:36 | 3.56 | 1.99 | 2.66 | 2.43 | 1 |
| Mean | 4.8 | 3.4 | 3.6 | 2.8 | ||||
PDB id, PDB identifier; Top, secondary structure topology (a for helix, b for strand, c for coil); L, peptide length; RC, the definition of the rigid core (PDB positions start at 1); FS-d (RC-d), full structure (rigid core) RMS deviation (Å) for the model of lowest energy (sOPEP) and the best model among the five clusters of lowest energy (best5); Rnk, the rank of the cluster containing the best model.
aThe lowest-energy models for 1e0n, 1psv, 2l0g, 2ki0 and 2gdl are shown on Figure 2.
Figure 2.PEP-FOLD models. The experimental conformation is in green. PEP-FOLD models are in cyan. From left to right, top to bottom: 1e0n (A), 1psv (B), 2l0g (C), 1n0a (D), 2ki0 (E), 1kwd (F) and 2gdl (G) lowest-energy models and 1wm8 (H) best model.
Results obtained for 34 cyclic peptides with disulfide bonds
| pdb Id | L | #SS | RC | sOPEP | best | ||||||
|---|---|---|---|---|---|---|---|---|---|---|---|
| FS-d | RC-d | CG | AA | FS-d | RC-d | CG | AA | ||||
| 1im7 | 21 | 1 | 3:9::15:21 | 3.9 | 3.9 | 100 | 0 | 2.5 | 2.5 | 100 | 1 |
| 1jbl | 16 | 1 | 2:14 | 3.3 | 3.3 | 100 | 1 | 1.8 | 1.8 | 0 | 0 |
| 1n0a | 17 | 1 | 7:15 | 0.7 | 0.7 | 0 | 1 | 0.4 | 0.4 | 0 | 0 |
| 1n0c | 24 | 1 | 2:11::14:24 | 2.3 | 2.3 | 100 | 1 | 0.4 | 0.4 | 0 | 1 |
| 1nim | 24 | 1 | 1:23 | 3.8 | 1.8 | 0 | 0 | 3.4 | 2.8 | 0 | 1 |
| 1gnb | 14 | 2 | 2:9::12:14 | 4.8 | 4.1 | 50 | 1 | 4 | 3.8 | 50 | 0 |
| 1b45 | 13 | 2 | – | 3.6 | 3.3 | 100 | 1 | 2.3 | 2.2 | 0 | 0 |
| 1etl | 22 | 2 | – | 3.1 | 3.1 | 100 | 1 | 1.6 | 1.6 | 0 | 0 |
| 1hje | 19 | 2 | – | 3.6 | 3.6 | 50 | 1 | 2.2 | 2.2 | 50 | 2 |
| 1hp9 | 12 | 2 | 2:11 | 3.5 | 3.5 | 50 | 1 | 2.2 | 2.2 | 50 | 1 |
| 1ien | 13 | 2 | – | 4.8 | 4.8 | 50 | 0 | 2.5 | 2.5 | 0 | 0 |
| 1im1 | 14 | 2 | – | 1.3 | 1.2 | 0 | 1 | 1.2 | 1.2 | 50 | 0 |
| 1kcn | 16 | 2 | – | 5.7 | 5.6 | 100 | 0 | 3.5 | 2.8 | 50 | 1 |
| 1kwd | 30 | 2 | 3:29 | 2.9 | 2.1 | 100 | 2 | 2 | 1.3 | 0 | 1 |
| 1mii | 11 | 2 | – | 1.8 | 1.8 | 50 | 0 | 1.6 | 1.6 | 0 | 0 |
| 1oig | 15 | 2 | 2:7::11:14 | 6.5 | 6.1 | 50 | 1 | 4.8 | 4.7 | 50 | 1 |
| 1r8t | 24 | 2 | 1:22 | 4.5 | 3.4 | 100 | 1 | 2.6 | 2.2 | 50 | 1 |
| 1rpc | 21 | 2 | 3:21 | 6.9 | 6.3 | 50 | 1 | 4.4 | 4 | 0 | 0 |
| 1ter | 21 | 2 | – | 7 | 5.9 | 50 | 1 | 3 | 2.8 | 50 | 0 |
| 1v6r | 26 | 2 | 1:23 | 5.1 | 5.1 | 100 | 2 | 3.9 | 3.9 | 0 | 0 |
| 1wqc | 13 | 2 | 2:13 | 1.7 | 1.3 | 100 | 2 | 1.2 | 1.1 | 100 | 2 |
| 1x7k | 22 | 2 | 1:17 | 4.2 | 2.5 | 0 | 0 | 4.2 | 2.5 | 0 | 0 |
| 1xgb | 16 | 2 | – | 3.5 | 3 | 0 | 0 | 3 | 3 | 50 | 2 |
| 2ajw | 13 | 2 | – | 2.4 | 0.9 | 50 | 2 | 1.3 | 1 | 0 | 0 |
| 2i28 | 28 | 2 | – | 2.1 | 2.1 | 100 | 1 | 1.5 | 1.5 | 0 | 0 |
| 2oq9 | 24 | 2 | 8:24 | 9.2 | 4 | 100 | 1 | 3.5 | 3.3 | 50 | 1 |
| 2efz | 12 | 3 | – | 4.2 | 4.2 | 0 | 1 | 2.1 | 2.1 | 66.7 | 1 |
| 2nx7 | 13 | 3 | 2:13 | 6.9 | 6.9 | 33.3 | 1 | 4.1 | 4 | 33.3 | 1 |
| 1mmc | 10 | 3 | – | 7.1 | 6.1 | 66.7 | 2 | 4.6 | 4.6 | 33.3 | 0 |
| 1orx | 22 | 3 | 1:19 | 4.8 | 4.8 | 33.3 | 1 | 2.9 | 2.7 | 0 | 0 |
| 1sp7 | 28 | 3 | 1:10::12:28 | 4.5 | 4.3 | 66.7 | 2 | 2.6 | 2 | 33.3 | 0 |
| 1v5a | 28 | 3 | – | 5 | 5.1 | 66.7 | 1 | 3.7 | 3.8 | 0 | 0 |
| 1wm8 | 19 | 3 | 6:16 | 7 | 7 | 66.7 | 2 | 3.6 | 3.6 | 66.7 | 2 |
| 2it7 | 28 | 3 | 2:28 | 4 | 4 | 66.7 | 1 | 3.7 | 3.7 | 66.7 | 1 |
| Mean | 4.2 | 3.7 | 61.2 | 2.7 | 2.5 | 29.5 | |||||
PDB id, PDB identifier; L, peptide length; SS, number of disulfide bond; RC, the definition of the rigid core (PDB positions start at 1); FS-d (RC-d), full structure (rigid core) RMS deviation (Å) for the model of lowest energy (sOPEP) and the model of lowest RMSD (best); CG, SS bonds formed in the Coarse Grained representation; AA, SS bonds formed in the final all-atom representation.
aOur criterion for evaluating a disulfide bond formed in the coarse grained structure is that r in equation ( lies within ± 0.7 Å. The discrepancy between the number of disulfide bonds in the atomistic and coarse grained structures comes from the fact that a very stringent condition on the S–S distance must be satisfied (2.0 ± 0.2 Å) in all-atom structures.
bThe lowest-energy models for 1n0a and 1kwd, and the best RMSD model for 1wm8 are shown on Figure 2.