Team:UANL Mty-Mexico/Modeling/3Dmodel/structure prediction
From 2012.igem.org
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<p><br><h3>Structure Prediction</h3></p> | <p><br><h3>Structure Prediction</h3></p> | ||
- | <br> | + | <br> |
- | + | <p><b>Theoretical background</b></p> | |
+ | <br> | ||
- | + | <p>Basically, our modelling approach to predict the tertiary structures of the proteins related to our system relies on the Anfinsen's thermodynamic hypothesis; our goal is to obtain models which satisfy the condition of the minimum free-energy states. Although every modelled structure will be validated by means of its energetic state, the sampling in the conformational space will differ according to the type of protein modelled and the type of input information available.</p> | |
- | Basically, our modelling approach to predict the tertiary structures of the proteins related to our system relies on the Anfinsen's thermodynamic hypothesis; our goal is to obtain models which satisfy the condition of the minimum free-energy states. Although every modelled structure will be validated by means of its energetic state, the sampling in the conformational space will differ according to the type of protein modelled and the type of input information available. | + | <br> |
- | Methodology | + | <p><b>Methodology</b></p> |
- | + | <br> | |
- | + | ||
- | + | ||
- | + | ||
- | + | ||
- | + | ||
- | + | <p>Our modelling approach is divided into the two sub-modules which are listed below:</p> | |
- | + | <ul> | |
+ | <li><p>rhMT</p></li> | ||
+ | <li><p>Assemblies</p></li> | ||
+ | <BLOCKQUOTE> | ||
+ | <p>rhMT-L2</p> | ||
+ | <p>OmpA-L2</p> | ||
+ | <p>Mocr-[rhMT]x</p> | ||
+ | </BLOCKQUOTE> | ||
+ | </ul> | ||
+ | <br> | ||
+ | <p>Where rhMT stands for the recombinant human metallothionein, whereas the group “assemblies” includes six fusion proteins: 1.rhMT fused to the E. coli ribosomal protein L2, 2.Outer membrane protein A fused to L2, and 3-6.Mocr tag protein fused to rhMT (subscript “x” refers to the number of copies as integers 1-4). </p> | ||
+ | <br> | ||
+ | |||
+ | <p>We used algorithms of the Rosetta3.4 package (Srivastan et al. 2009) such as AbinitioRelax (<i>ab initio</i> modelling), Comparative modelling, and Clustering application (RMSD calculations and sorting by free-energy). The <i>ab initio</i> approach was used to predict the tertiary structure of rhMT by using a template native structure of an homologous metallothionein (PDB: 4mt2) found by Jpred3 (Cole et al. 2008), in order to obtain an accurate model, we used 3mer and 9mer rotamer library fragments generated by Robetta server. Radius gyration, contact-order and sheet filters as well as secondary structure prediction files were used in order to avoid some noise in a fail-model context. We used default loop and helix reweight factors as well as ab initio cycles. The key flags used in our model with the AbinitioRelax algorithm are showed below.</p> | ||
+ | <br> | ||
+ | |||
+ | <p> | ||
AbinitioRelax.linuxgccrelease \ | AbinitioRelax.linuxgccrelease \ | ||
-database /rosetta_database/ \ | -database /rosetta_database/ \ | ||
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-out:file:silent rhMT_silent.out | -out:file:silent rhMT_silent.out | ||
-nstruct 20000 | -nstruct 20000 | ||
+ | </p> | ||
+ | <br> | ||
+ | |||
+ | <p>rhMT.fas [MKFGSMGKAAAACSCATGGSCTCTGSCKCKECKCNSCKKAAAACCSCCPMSCAKCAQGCVCKGASEKCSCCKKAAAAGS]</p> | ||
+ | <br> | ||
- | |||
+ | <p>Clustering application was used to obtain clusters by calculating RMSD between all the structures and joining them to their corresponding neighbours, the resulting clustered models were sorted by their free-energy in order to obtain the model with the lowest value—which is intended to satisfy the Anfinsen's thermodynamic hypothesis—thus, the most accurate aproximation to the native state (it's sensitivity depends strongly on the size of the explored portion of the conformational space).</p> | ||
+ | <br> | ||
- | + | <p><b>Results</b></p> | |
+ | <br> | ||
- | + | <p>As molecular simulations are time-consuming (computationally), we only have partial results for rhMT <i>ab initio</i> modelling (partial model generated by using 5,000 simulated structures as input for the Cluster application). Unfortunatelly, this model is not accurate enough describe the native structure of rhMT.</p> | |
- | As molecular simulations are time-consuming (computationally), we only have partial results for rhMT ab initio modelling (partial model generated by using | + | <br> |
Revision as of 01:25, 27 September 2012
Structure Prediction
Theoretical background
Basically, our modelling approach to predict the tertiary structures of the proteins related to our system relies on the Anfinsen's thermodynamic hypothesis; our goal is to obtain models which satisfy the condition of the minimum free-energy states. Although every modelled structure will be validated by means of its energetic state, the sampling in the conformational space will differ according to the type of protein modelled and the type of input information available.
Methodology
Our modelling approach is divided into the two sub-modules which are listed below:
rhMT
Assemblies
rhMT-L2
OmpA-L2
Mocr-[rhMT]x
Where rhMT stands for the recombinant human metallothionein, whereas the group “assemblies” includes six fusion proteins: 1.rhMT fused to the E. coli ribosomal protein L2, 2.Outer membrane protein A fused to L2, and 3-6.Mocr tag protein fused to rhMT (subscript “x” refers to the number of copies as integers 1-4).
We used algorithms of the Rosetta3.4 package (Srivastan et al. 2009) such as AbinitioRelax (ab initio modelling), Comparative modelling, and Clustering application (RMSD calculations and sorting by free-energy). The ab initio approach was used to predict the tertiary structure of rhMT by using a template native structure of an homologous metallothionein (PDB: 4mt2) found by Jpred3 (Cole et al. 2008), in order to obtain an accurate model, we used 3mer and 9mer rotamer library fragments generated by Robetta server. Radius gyration, contact-order and sheet filters as well as secondary structure prediction files were used in order to avoid some noise in a fail-model context. We used default loop and helix reweight factors as well as ab initio cycles. The key flags used in our model with the AbinitioRelax algorithm are showed below.
AbinitioRelax.linuxgccrelease \ -database /rosetta_database/ \ -abinitio:relax \ -use_filters true \ -abinitio::increase_cycles 10 \ -abinitio::rg_reweight 0.5 \ -abinitio::rsd_wt_loop 0.5 \ -abinitio::rsd_wt_helix 0.5 \ -relax::fast \ -in:file:fasta rhMT.fas -in:file:frag3 rhMT3_05.200_v1_3 -in:file:frag9 rhMT9_05.200_v1_3 -in:file:native 4mt2.pdb -psipred_ss2 rhMT.psipred_ss2 -out:file:silent rhMT_silent.out -nstruct 20000
rhMT.fas [MKFGSMGKAAAACSCATGGSCTCTGSCKCKECKCNSCKKAAAACCSCCPMSCAKCAQGCVCKGASEKCSCCKKAAAAGS]
Clustering application was used to obtain clusters by calculating RMSD between all the structures and joining them to their corresponding neighbours, the resulting clustered models were sorted by their free-energy in order to obtain the model with the lowest value—which is intended to satisfy the Anfinsen's thermodynamic hypothesis—thus, the most accurate aproximation to the native state (it's sensitivity depends strongly on the size of the explored portion of the conformational space).
Results
As molecular simulations are time-consuming (computationally), we only have partial results for rhMT ab initio modelling (partial model generated by using 5,000 simulated structures as input for the Cluster application). Unfortunatelly, this model is not accurate enough describe the native structure of rhMT.