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Published byMae Anthony Modified over 9 years ago
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Computing Missing Loops in Automatically Resolved X-Ray Structures Itay Lotan Henry van den Bedem (SSRL)
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Bioinformatics core UCSD, SDSC Crystallomics core TSRI, GNF Structure Determination Core SSRL Crystal screening / X-ray data collection Structure determination Structure refinement Funding from NIH Protein Structure Initiative 10 centers Funding for five years from July 2000 Ongoing projects at SDC: Beam line automation: Sample mounting robotics, automated diffraction quality assessment Automated structure determination: Structure Solution Pipeline Joint Center for Structural Genomics : Create new technologies to drive high throughput structure determination
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From Model Building to Refinement Structure Solution Pipeline Initial Model(s) Diffraction Images Final Model Mostly Automated Manual Finalizing model: Labor intensive, time consuming. Existing tools to assist in model building unsatisfactory: 1.Produce incorrect configurations 2.Lack meaningful scoring algorithm to rank configurations 3.Remain highly interactive – difficult to integrate in Structure Solution Pipeline Initial models (RESOLVE, ARP/WARP): Several chains and gaps
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The Problem We are given: –A density map –A solved structure with a gap (5 – 15 res.) Goal: –Automatically compute backbone conformation for the gap region
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Gaps The structure is solved automatically Gaps appear in areas of “poor” density –Signal is indistinguishable from noise –Disconnected iso-surfaces –Automatic solver bails out
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Things we can use The loop-closure constraint What density there is The solved structure The sequence is known (C β atoms) Preferred backbone angles (Ramchandran plots)
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Loop Closure: CCD algorithm Robot Inverse Kinematics ( Wang & Chen ’91 ) Protein loops ( Canutescu & Dunbrack ’03 ) Algorithm: 1.Fix loop at one end 2.Repeat until closure For each DOF of loop Minimize closure score for DOF
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CCD for Proteins Closure score: Sum of squared distances of N, C α and C atoms of final residue from their target positions
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Our Approach 1. Generate closed loops using density, Ramachandran plot bias and solved structure 2. Optimize highest scoring loops using density and solved structure
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Stage 1: Generate Closed Loops Perform one big CCD run For residue i : –Compute closure moves of ( φ,ψ ) angles –Compute max density of residue i+1 –Combine and bias toward peaks in Ramachandran plot Weight of closure move is increased gradually
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Stage 2: Loop Optimization Choose residue i and φ or ψ DOF at random –Apply random change –Use DOFs of residues [ i-1, i+2 ] to close loop using CCD –Compute new score Accept change using Metropolis-like criterion Slowly decrease temperature and reduce StDev of random changes
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Score Density: Weighted sum of density at atom centers and points away from center along coordinate axes. Collision: Penalize overlap of loop atoms with solved structure atoms as function penetration depth. Self Collision: Penalize overlap of atoms in loop
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Local Loop Changes My CCD method: –Choose DOF at random (from ALL DOFs) with biases –Compute Direction of change –Move only a little –Allowed change in N-Cα and Cα-C bond lengths, N-Cα-C angle and Ω angle decreases with distance from optimal value Repeat until closed or maximum iterations
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3.7Å 0.35Å 8 Residue Loop: Example 1
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8 Residue Loop: Example 2 0.3Å 2.79Å
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12 Residue Loop: 1.29Å0.28Å
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9 Residue Loop: 3Å0.32Å
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Open Issues Many parameters that are determined arbitrarily –Annealing regimen –Weight of collision penalty –Acceptance criterion Have one set of parameters that works for all loops lengths and density qualities
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