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A Winter Short Course on Statistical Mechanics for Molecular Simulations Lecture 5: Free Energy Calculations Yuan-Chung Cheng yuanchung@ntu.edu.tw 2/9/2015 Enhanced Sampling Methods n Biasing potential methods Umbrella sampling


  1. A Winter Short Course on Statistical Mechanics for Molecular Simulations Lecture 5: Free Energy Calculations Yuan-Chung Cheng yuanchung@ntu.edu.tw 2/9/2015

  2. Enhanced Sampling Methods n Biasing potential methods ¨ Umbrella sampling ¨ Metadynamics ¨ Steered MD/Local elevation/Conformational flooding/adaptive force bias … n Multicanonical methods ¨ Parallel Tempering (Replica exchange) ¨ Integrate-over-temperature (Yi Qin Gao) n Transition path methods …

  3. Umbrella Sampling n Sample with umbrella potential U'(x) n Compute biased probability P'(x) n Estimate unbiased free energy A(x) = − k B T ln P’(x) − U’(x)+F n F is undetermined n Multiple biasing potentials can be used (multiple windows) Steven O. Nielsen's slides (http://www.utdallas.edu/~son051000/comp/FreeE.pdf)

  4. Weighted Histogram Analysis Method n Potentials can be combined using WHAM ( Kumar, et al. J Comput Chem, 13, 1011,1992 ) Steven O. Nielsen's slides (http://www.utdallas.edu/~son051000/comp/FreeE.pdf)

  5. Steven O. Nielsen's slides (http://www.utdallas.edu/~son051000/comp/FreeE.pdf)

  6. Steven O. Nielsen's slides (http://www.utdallas.edu/~son051000/comp/FreeE.pdf)

  7. Steven O. Nielsen's slides (http://www.utdallas.edu/~son051000/comp/FreeE.pdf)

  8. Potential of mean force from constrained MD simulations Steven O. Nielsen's slides (http://www.utdallas.edu/~son051000/comp/FreeE.pdf)

  9. Umbrella sampling Steven O. Nielsen's slides (http://www.utdallas.edu/~son051000/comp/FreeE.pdf)

  10. Steven O. Nielsen's slides (http://www.utdallas.edu/~son051000/comp/FreeE.pdf)

  11. Steven O. Nielsen's slides (http://www.utdallas.edu/~son051000/comp/FreeE.pdf)

  12. Replica Exchange - Overcoming Free Energy Barrier n Non-directed method (no reaction coordinate) n How to sample unfavorable states? n At high T, barriers are easier to overcome. n Heat and cool the system to push it over barriers to sample new configurations Steven O. Nielsen's slides (http://www.utdallas.edu/~son051000/comp/FreeE.pdf)

  13. Replica Exchange - Overcoming Free Energy Barrier Monte Carlo step: exchanged n Launch simulations at different temperatures n Swap configurations based on the metropolis criterion: Monte Carlo step: exchange rejected n The lowest temperature overlap is important for “trajectory” samples from the efficiency of sampling Boltzmann distribution. n Swapping configurations effectively improves sampling Steven O. Nielsen's slides (http://www.utdallas.edu/~son051000/comp/FreeE.pdf)

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