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computer modeling in molecular biology.pdf

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7 Major Histocompatibility Complex Class I Prote<strong>in</strong>-Peptide Interactions 1937.6 Modell<strong>in</strong>g and Simulationof an Influenza Virus Peptide with theHuman MHC Class I Molecule HLA-Aw68The human class I allele HLA-Aw68 provides a good basis for <strong>molecular</strong> simulations.It presents a wide variety of peptides of differ<strong>in</strong>g lengths, and there are X-raycrystallographic structures for the molecule both with a collection of endogenouspeptides, at 2.6 A and 1.9 A resolution and with a s<strong>in</strong>gle peptide derived from the<strong>in</strong>fluenza virus nucleoprote<strong>in</strong> peptide (Np91-99) at 2.8 A resolution. The high resolutionstructure for HLA-Aw68 with different length multiple endogenous peptidesclearly demonstrates that the term<strong>in</strong>i of the peptide are <strong>in</strong> highly similar positionsregardless of the length of the central bulge. This allows for the construction of aseries of models which have the different length peptides bound to the HLA-Aw68molecule. In addition we have constructed a model of HLA-Aw68 complexed withthe flu peptide which may be used for model validation purposes by comparison tothe recently determ<strong>in</strong>ed crystallographic structure.The major epitope derived from the <strong>in</strong>fluenza virus to elicit a response from CTLwhen presented by HLA-Aw68 is a nonamer fragment (KTGGPIYKR) derived fromthe <strong>in</strong>fluenza virus nucleoprote<strong>in</strong> compris<strong>in</strong>g of residues 91-99 [42] (Np91-99). Thispeptide has recently been studied bound <strong>in</strong> the groove of HLA-Aw68 by the groupof Don Wiley us<strong>in</strong>g X-ray cryo-crystallography. The result<strong>in</strong>g peptide structure hasbeen compared to that of the model nonamer peptide built <strong>in</strong>to the observed density<strong>in</strong> HLA-B27 at 2.1 A resolution, and the deviations between the two peptide modelsappear to be limited to small sequence dependant changes <strong>in</strong> the backbones of thepeptides.The peptide model and the 15 solvent molecules <strong>in</strong> the cleft of HLA-B27 weremoved <strong>in</strong>to the start<strong>in</strong>g structure and mutated to the sequence of the <strong>in</strong>fluenza viruspeptide. The waters were redef<strong>in</strong>ed as TIP3P waters and the assembly of MHCmolecule peptide and waters was geometry optimised. The SYBYL 5.5 implementationof the Kollman united atom force field was used with polar atoms def<strong>in</strong>ed astheir Kollman all atom counterparts. Charges were taken from the <strong>in</strong>ternal dictionaryand the 1-4 scal<strong>in</strong>g term was def<strong>in</strong>ed to give a direct parity between the energiesgenerated by SYBYL and by Amber. Once the convergence criteria of an RMS deviationof 0.05 <strong>in</strong> the total energy term had been achieved the molecule was soaked <strong>in</strong>a bath of random water molecules compris<strong>in</strong>g 2304 solvent molecules <strong>in</strong> a box whose<strong>in</strong>itial periodic boundary size was 49.29 x 55.50 x 34.44 A (xyz). This assembly wasenergy m<strong>in</strong>imised to convergence with periodic boundary conditions <strong>in</strong>voked andHLA-Aw68 held rigid. This geometry optimisation step was used to remove holesand van der Waals (VDW) clashes with<strong>in</strong> the random solvent field. A sphere of <strong>in</strong>-

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