DNA bending induced during Molecular Dynamics simulations: Basepair Kinks and Hinges
|
|
- Blake Hill
- 5 years ago
- Views:
Transcription
1 DNA bending induced during Molecular Dynamics simulations: Basepair Kinks and Hinges Thursday, October 23, 2008 Theoretical Approaches or the Genome LAPTH-LAMA-LAPP-CNRS-University o Savoie Jeremy Curuksu Computational Biology Lab., Martin Zacharias Jacobs University, Bremen, Germany Annecy-le-Vieux, France
2 TALK OUTLINES INTRODUCTION 1. Developpment: An all-atom DNA Bending Coordinate 2. Application: Molecular Dynamics o DNA kink motis (example o a poly-purine/pyrimidine C/G DNA 15 bp sequence) 3. Further insights rom enhanced sampling techniques CONCLUSION
3 Molecular Dynamics simulation F = m. a V ( q) = M. d q 2 dt 2 q Probability Density at constant N, V and T: Γ : P( Γ) = exp( H ( Γ) / k T Set o particle positions ( q) and momenta ( p) H( q, p) : the Hamiltonian = V( q) + K( p) k B :Boltzmann Constant B ) Time A Molecular Dynamics Trajectory
4 Quasi-ergodicity o MD samples A schematic representation o phase space Order Parameter Y Order Parameter X Region o low energy Region o high energy
5 DNA conormational lexibility δ: C5 C4 C3 O3 γ: O5 C5 C4 C3 β: P O5 C5 C4 α: O3 P O5 C5 ζ: C3 O3 P O5 SHIFT SLIDE TILT ROLL BENDING OF BASEPAIR ε: C4 C3 O3 P RISE TWIST Backbone dihedral angles { Z( Ω) Y ( ρ) X ( )} ( j, k, ) ( j ', k', l') = τ l Helical internal coordinates
6 DNA bend coordinate { A} ( j, k, ) ( j ', k', l') = l (j,k,l ) Harmonic potential U(θ) = k * ( θ - θ re ) 2 triad (j, k, l) Rotation vector Curuksu J., Zakrzewska K., Zacharias M. (2008) Nucleic Acid Research 36(7):
7 Amplitude and Direction o bending Adiabatic Mapping on DNA ds 5 (GCAAAAAACG)3 Energy Minimisation Curuksu J., Zakrzewska K., Zacharias M. (2008) Nucleic Acid Research 36(7):
8 Free Energy (PMF) o DNA bending Umbrella Sampling Molecular Dynamics Protocol DNA bending energy probed by Atomic Force microscopy (Wiggins et al., 2006) w.3 ns w.2 ns bk.1 ns parmbsc0 (Perez et al.,2007) Truncated octahedral box (~7600 water molecules) Neutralising K + counterions PME electrostatics 2 s timestep (SHAKE) NVT (0K 300K) NPT Time rame every 2 ps 31*3ns w trj (0 150 ) using U(θ) = k * ( θ - θ re ) 2 Bending Free Energy (kcal/mol) d(cgcgcgcgcgcgcgc) d(cgcgcaaaaacgcgc) d(catatatatatatatc) d(cgcgcgcgcaaaaac) Bend angle θ (degrees) Curuksu J., Zacharias M., Lavery R., Zakrzewska K., Manuscript in preparation
9 Kinking Occurs during Molecular Dynamics Simulations o Small DNA Minicircles (2006) starting structure kink kink starting structure kink stable conormations Lankas F., Lavery R, Maddocks J.H. (2006) Structure 14:
10 TALK OUTLINES INTRODUCTION 1. Developpment: an all-atom DNA Bending Coordinate 2. Application: Molecular Dynamics o DNA kink motis (example o a poly-purine/pyrimidine C/G DNA 15 bp sequence) 3. Further insights rom enhanced sampling techniques CONCLUSION
11 The poly-purine/pyrimidine C/G DNA sequence (15 bp) Bending Free Energy (kcal/mol) α =6.8 (Linear Sub-Elastic Chain model) rom AFM [ Wiggins et al. (2006) ] E(θ) = 1/2 * k B T* l/ξ * θ 2 based on ξ ~ 144 bp α = 6.9 Bend angle (degrees)
12 The poly-c/g DNA sequence (15 bp) Probability Distribution o basepair bend angles Amber parm-94 orce ield Amber parm-bsc0 orce ield ( roll 2 + tilt 2 ) in degrees ( roll 2 + tilt 2 ) in degrees Legend Row 1: C1G2 C3G4 C5G6 C7G8 C9G10 C11G12 C13G14 Row 2: G2C3 G4C5 G6C7 G8C9 G10C11 G12C13 G14C15
13 The poly-c/g DNA sequence (15 bp, parmbsc0) Basepair Kink (type II) Force Constantes o basepair bend Time Average o local bend and propeller with parmbsc0 ( roll 2 + tilt 2 ) in degrees Junction C7G8 Junction G6C7 K (kcal/mol/degree 2 ) k B T 2 2 σ ( roll + tilt cubic polynomial it 2 ) G6C7 C7G8 Global Bend in degrees Normal probability plots o basepair bend De Santis,2002, thermal stability data Olson,1998, Crystallo. Lankas,2003, MD Robinson,2002, EPR Propeller in degrees base pair at C7 Normalized Sample Junction G6C7 Junction C7G8 Global Bend in degrees Normal Distribution N(0,1)
14 DNA basepair hinge conormations Time Frames / Side View: three DNA kink substates K (kcal/mol/deg 2 ) GCG, type II kink AAC, type II kink CG, middle kink C7G8 A9A10 G6C7 A10C11 C7G8 Bend angle (degrees) Bend angle (degrees) Bend angle (degrees) Curuksu J., Zacharias M., Lavery R., Zakrzewska K., Manuscript in preparation
15 TALK OUTLINES INTRODUCTION 1. Developpment: an all-atom DNA Bending Coordinate 2. Application: Molecular Dynamics o DNA kink motis (example o a poly-purine/pyrimidine C/G DNA 15 bp sequence) 3. Further insights rom enhanced sampling techniques CONCLUSION
16 Molecular Dynamics simulation F = m. a V ( q) = M. d q 2 dt 2 q Probability Density at constant N, V and T: Γ : P( Γ) = exp( H ( Γ) / k T Set o particle positions ( q) and momenta ( p) H( q, p) : the Hamiltonian = V( q) + K( p) k B :Boltzmann Constant B ) Time A Molecular Dynamics Trajectory
17 Replica Exchange simulation??????? Time W ( C) ω( C C ') Detailed = W( C' Balance ac') ) P ( C = W ( C ') ω( C ' C) ) W ( C Replica 1 R2 R3 R4 R5 R6 Replica n
18 The poly-c/g DNA sequence (15 bp, parm94) ds DNA 5 (CGCGCGCGCGCGCGC)3 Replica Exchange Umbrella Sampling (Amber parm94 orce ield) Probability Distribution o base pair bend angles CG junctions original GC junctions 150 Bending Free Energy in kcal.mol -1, parm94 New: WITH REUS 1ns 2ns 1ns 2ns Original: WITHOUT REUS ( roll 2 + tilt 2 ) in degrees Global bend angle in degrees
19 The poly-c/g DNA sequence (15 bp, parmbsc0) ds DNA 5 (CGCGCGCGCGCGCGC)3 Replica Exchange Umbrella Sampling (Amber parmbsc0 orce ield) Probability Distribution o base pair bend angles CG junctions GC junctions 150 (degrees) ( roll 2 + tilt 2 ) at C7G8 bp junction Propeller at C7:G24 Watson-Crick bp 150 ( roll 2 + tilt 2 ) in degrees Time (nanoseconds)
20 Conclusion DNA bending ree energy not quadratic on short length scale [ 5 nm ] Amber parm-94 orce ield: - Type I kink at 5 CG3 requires longitudinal localization o DNA bending energy. (what could be used to code Breakpoints in the Genome) Amber parm-bsc0 orce ield: - No type I kink. - Type II kink at 5 GCG3 and 5 AAC3 ( For Global Bend [ 5 nm ] >> 100 ). - Type II kink is metastable and has reduced basepair bend orce constant. Valid inerence o DNA bend conormers rom MD orce-ield consensus
21 Acknowledgement Martin Zacharias Ragav, Sebastian, Shide and Ranjit Group o Computational Biology Jacobs University (Bremen, Germany) Krystyna Zakrzewska and Richard Lavery Laboratoire de Bioinormatique et RMN structurales Institut de Biologie et Chimie des Protéines (Lyon, France) Computational Laboratories or Analysis, Modelling and Visualization (CLAMV), Jacobs University, Germany. Universite Franco-Allemande (UFA) cotutelle agreement between Universite Paris 7 and Jacobs University. VolkswagenStitung PhD grant. and the Theoretical Approaches or the Genome 2008 organizers.
22
A rigid-base model for DNA structure prediction. O. Gonzalez
A rigid-base model for DNA structure prediction O. Gonzalez Introduction Objective. To develop a model to predict the structure and flexibility of standard, B-form DNA from its sequence. Introduction Objective.
More informationExtended description of the rigid base model (Supplement to Section 2.1: Model)
Supplementary material for cgdna: a software package for the prediction of sequence-dependent coarse-grain free energies of B-form DNA by D. Petkevičiūtė, M. Pasi, O. Gonzalez and J.H. Maddocks S Extended
More informationWhy Proteins Fold? (Parts of this presentation are based on work of Ashok Kolaskar) CS490B: Introduction to Bioinformatics Mar.
Why Proteins Fold? (Parts of this presentation are based on work of Ashok Kolaskar) CS490B: Introduction to Bioinformatics Mar. 25, 2002 Molecular Dynamics: Introduction At physiological conditions, the
More informationExploring the Sequence Dependent Structure and Dynamics of DNA with Molecular Dynamics Simulation
Exploring the Sequence Dependent Structure and Dynamics of DNA with Molecular Dynamics Simulation Sarah Harris School of Physics and Astronomy University of Leeds Introduction Calculations of the charge
More informationSupplementary Figures. Measuring Similarity Between Dynamic Ensembles of Biomolecules
Supplementary Figures Measuring Similarity Between Dynamic Ensembles of Biomolecules Shan Yang, Loïc Salmon 2, and Hashim M. Al-Hashimi 3*. Department of Chemistry, University of Michigan, Ann Arbor, MI,
More informationLimitations of temperature replica exchange (T-REMD) for protein folding simulations
Limitations of temperature replica exchange (T-REMD) for protein folding simulations Jed W. Pitera, William C. Swope IBM Research pitera@us.ibm.com Anomalies in protein folding kinetic thermodynamic 322K
More informationAll-atom Molecular Mechanics. Trent E. Balius AMS 535 / CHE /27/2010
All-atom Molecular Mechanics Trent E. Balius AMS 535 / CHE 535 09/27/2010 Outline Molecular models Molecular mechanics Force Fields Potential energy function functional form parameters and parameterization
More informationThe Molecular Dynamics Method
The Molecular Dynamics Method Thermal motion of a lipid bilayer Water permeation through channels Selective sugar transport Potential Energy (hyper)surface What is Force? Energy U(x) F = d dx U(x) Conformation
More informationNanotube AFM Probe Resolution
Influence of Elastic Deformation on Single-Wall Carbon Nanotube AFM Probe Resolution Ian R. Shapiro, Santiago D. Solares, Maria J. Esplandiu, Lawrence A. Wade, William A. Goddard,* and C. Patrick Collier*
More informationGlass-Transition and Side-Chain Dynamics in Thin Films: Explaining. Dissimilar Free Surface Effects for Polystyrene and Poly(methyl methacrylate)
Supporting Information for Glass-Transition and Side-Chain Dynamics in Thin Films: Explaining Dissimilar Free Surface Effects for Polystyrene and Poly(methyl methacrylate) David D. Hsu, Wenjie Xia, Jake
More informationIntroduction to molecular dynamics
1 Introduction to molecular dynamics Yves Lansac Université François Rabelais, Tours, France Visiting MSE, GIST for the summer Molecular Simulation 2 Molecular simulation is a computational experiment.
More informationA Coarse-Grained Model of DNA with Almost Atomic Resolution
A Coarse-Grained Model of DNA with Almost Atomic Resolution Pablo D. Dans Puiggròs, PhD Joint CRG-BSC-IRB Program on Computational Biology Molecular Modelling & Bioinformatics Group Institute for Research
More informationAtomic-Level Simulations of Seeman DNA Nanostructures: The Paranemic Crossover in Salt Solution
Biophysical Journal Volume 90 March 2006 1463 1479 1463 Atomic-Level Simulations of Seeman DNA Nanostructures: The Paranemic Crossover in Salt Solution Prabal K. Maiti,* y Tod A. Pascal,* Nagarajan Vaidehi,*
More informationElbow Flexibility of the kt38 RNA Kink-Turn Motif Investigated by Free-Energy Molecular Dynamics Simulations
2004 Biophysical Journal Volume 97 October 2009 2004 2013 Elbow Flexibility of the kt38 RNA Kink-Turn Motif Investigated by Free-Energy Molecular Dynamics Simulations Jeremy Curuksu, Jiri Sponer, and Martin
More informationThe Molecular Dynamics Method
H-bond energy (kcal/mol) - 4.0 The Molecular Dynamics Method Fibronectin III_1, a mechanical protein that glues cells together in wound healing and in preventing tumor metastasis 0 ATPase, a molecular
More informationMolecular Mechanics, Dynamics & Docking
Molecular Mechanics, Dynamics & Docking Lawrence Hunter, Ph.D. Director, Computational Bioscience Program University of Colorado School of Medicine Larry.Hunter@uchsc.edu http://compbio.uchsc.edu/hunter
More informationFree energy simulations
Free energy simulations Marcus Elstner and Tomáš Kubař January 14, 2013 Motivation a physical quantity that is of most interest in chemistry? free energies Helmholtz F or Gibbs G holy grail of computational
More informationWritten Test A. [Solve three out of the following five problems.] ψ = B(x + y + 2z)e x 2 +y 2 +z 2
Written Test A Solve three out of the following five problems.] Problem 1. A spinless particle is described by the wave function where B is a constant. ψ = B(x + y + z)e x +y +z 1. Determine the total
More informationA Computational Study of Nucleosomal DNA Flexibility
Biophysical Journal Volume 91 December 2006 4121 4132 4121 A Computational Study of Nucleosomal DNA Flexibility Jory Z. Ruscio* and Alexey Onufriev y *Genetics, Bioinformatics & Computational Biology Program,
More informationEXTENDING THE BOUNDARIES OF STRUCTURAL MODELING EPIGENETIC EFFECTS ON NUCLEOSOME POSITIONING
EXTENDING THE BOUNDARIES OF STRUCTURAL MODELING EPIGENETIC EFFECTS ON NUCLEOSOME POSITIONING Peter Minary Computational Structural Biology Group Stanford University Stanford, CA 94305 ~ 0.3 nm TO MODEL
More informationCoupling the Level-Set Method with Variational Implicit Solvent Modeling of Molecular Solvation
Coupling the Level-Set Method with Variational Implicit Solvent Modeling of Molecular Solvation Bo Li Math Dept & CTBP, UCSD Li-Tien Cheng (Math, UCSD) Zhongming Wang (Math & Biochem, UCSD) Yang Xie (MAE,
More informationA Computational Study of Nucleosomal DNA Flexibility
Biophysical Journal Volume 91 December 26 4121-4132 4121 A Computational Study of Nucleosomal DNA Flexibility Jory Z. Ruscio* and Alexey Onufrievt *Genetics, Bioinformatics & Computational Biology Program,
More informationAtomistic Modeling of Small-Angle Scattering Data Using SASSIE-web
Course Introduction Atomistic Modeling of Small-Angle Scattering Data Using SASSIE-web September 21-23, 2016 Advanced Photon Source Argonne National Laboratory, Argonne, IL ccpsas.org Scatters & Simulators
More information3.320 Lecture 18 (4/12/05)
3.320 Lecture 18 (4/12/05) Monte Carlo Simulation II and free energies Figure by MIT OCW. General Statistical Mechanics References D. Chandler, Introduction to Modern Statistical Mechanics D.A. McQuarrie,
More information5.80 Small-Molecule Spectroscopy and Dynamics
MIT OpenCourseWare http://ocw.mit.edu 5.80 Small-Molecule Spectroscopy and Dynamics Fall 2008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. 5.80 Lecture
More informationEvaluation of Elastic Rod Models with Long Range Interactions for Predicting Nucleosome Stability
Open Access Article The authors, the publisher, and the right holders grant the right to use, reproduce, and disseminate the work in digital form to all users. Journal of Biomolecular Structure & Dynamics,
More informationStatistical thermodynamics for MD and MC simulations
Statistical thermodynamics for MD and MC simulations knowing 2 atoms and wishing to know 10 23 of them Marcus Elstner and Tomáš Kubař 22 June 2016 Introduction Thermodynamic properties of molecular systems
More informationDynamics of Nucleic Acids Analyzed from Base Pair Geometry
Dynamics of Nucleic Acids Analyzed from Base Pair Geometry Dhananjay Bhattacharyya Biophysics Division Saha Institute of Nuclear Physics Kolkata 700064, INDIA dhananjay.bhattacharyya@saha.ac.in Definition
More informationLectures on basic plasma physics: Hamiltonian mechanics of charged particle motion
Lectures on basic plasma physics: Hamiltonian mechanics of charged particle motion Department of applied physics, Aalto University March 8, 2016 Hamiltonian versus Newtonian mechanics Newtonian mechanics:
More informationDNA Polymorphism: A Comparison of Force Fields for Nucleic Acids
Biophysical Journal Volume 84 March 2003 1421 1449 1421 DNA Polymorphism: A Comparison of Force Fields for Nucleic Acids Swarnalatha Y. Reddy,* Fabrice Leclerc,* yz and Martin Karplus* z *Department of
More information2008 Biowerkzeug Ltd.
2008 Biowerkzeug Ltd. 1 Contents Summary...3 1 Simulation...4 1.1 Setup...4 1.2 Output...4 2 Settings...5 3 Analysis...9 3.1 Setup...9 3.2 Input options...9 3.3 Descriptions...10 Please note that we cannot
More informationMethods of Computer Simulation. Molecular Dynamics and Monte Carlo
Molecular Dynamics Time is of the essence in biological processes therefore how do we understand time-dependent processes at the molecular level? How do we do this experimentally? How do we do this computationally?
More informationOrganization of NAMD Tutorial Files
Organization of NAMD Tutorial Files .1.1. RMSD for individual residues Objective: Find the average RMSD over time of each residue in the protein using VMD. Display the protein with the residues colored
More informationMulti-scale Simulations Coupled with Ion Mobility Experiments Reveal the Fate of Nucleic Acids in the Gas Phase
Multi-scale Simulations Coupled with Ion Mobility Experiments Reveal the Fate of Nucleic Acids in the Gas Phase Massimiliano Porrini, Clémence Rabin, Josephine Abi-Ghanem, Frederic Rosu, Leonardo Darré,
More informationSupplementary Information for: The Temperature Dependence of the Helical Twist of DNA
Supplementary Information for: The Temperature Dependence of the Helical Twist of DNA Franziska Kriegel 1, Christian Matek 2, Tomáš Dršata 3, Klara Kulenkampff 1, Sophie Tschirpke 1, Martin Zacharias 4,
More informationPotential Energy (hyper)surface
The Molecular Dynamics Method Thermal motion of a lipid bilayer Water permeation through channels Selective sugar transport Potential Energy (hyper)surface What is Force? Energy U(x) F = " d dx U(x) Conformation
More informationWhy study protein dynamics?
Why study protein dynamics? Protein flexibility is crucial for function. One average structure is not enough. Proteins constantly sample configurational space. Transport - binding and moving molecules
More informationCourse Introduction. SASSIE CCP-SAS Workshop. January 23-25, ISIS Neutron and Muon Source Rutherford Appleton Laboratory UK
Course Introduction SASSIE CCP-SAS Workshop January 23-25, 2017 ISIS Neutron and Muon Source Rutherford Appleton Laboratory UK ccpsas.org Scatters & Simulators Develop a community of users and developers
More informationStructural biomathematics: an overview of molecular simulations and protein structure prediction
: an overview of molecular simulations and protein structure prediction Figure: Parc de Recerca Biomèdica de Barcelona (PRBB). Contents 1 A Glance at Structural Biology 2 3 1 A Glance at Structural Biology
More informationConservation of Linear Momentum : If a force F is acting on particle of mass m, then according to Newton s second law of motion, we have F = dp /dt =
Conservation of Linear Momentum : If a force F is acting on particle of mass m, then according to Newton s second law of motion, we have F = dp /dt = d (mv) /dt where p =mv is linear momentum of particle
More informationONETEP PB/SA: Application to G-Quadruplex DNA Stability. Danny Cole
ONETEP PB/SA: Application to G-Quadruplex DNA Stability Danny Cole Introduction Historical overview of structure and free energy calculation of complex molecules using molecular mechanics and continuum
More informationStructural and mechanistic insight into the substrate. binding from the conformational dynamics in apo. and substrate-bound DapE enzyme
Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 215 Structural and mechanistic insight into the substrate binding from the conformational
More informationWhat is Classical Molecular Dynamics?
What is Classical Molecular Dynamics? Simulation of explicit particles (atoms, ions,... ) Particles interact via relatively simple analytical potential functions Newton s equations of motion are integrated
More informationAdvanced Molecular Dynamics
Advanced Molecular Dynamics Introduction May 2, 2017 Who am I? I am an associate professor at Theoretical Physics Topics I work on: Algorithms for (parallel) molecular simulations including GPU acceleration
More informationNon-bonded interactions
speeding up the number-crunching continued Marcus Elstner and Tomáš Kubař December 3, 2013 why care? number of individual pair-wise interactions bonded interactions proportional to N: O(N) non-bonded interactions
More informationSupplementary Materials for
advances.sciencemag.org/cgi/content/full/4/1/eaau413/dc1 Supplementary Materials for Structure and dynamics conspire in the evolution of affinity between intrinsically disordered proteins Per Jemth*, Elin
More informationForce fields, thermo- and barostats. Berk Hess
Force fields, thermo- and barostats Berk Hess What is a force field? A force field usually consists of three parts: a set of functional forms parameters for the functional forms that, usually, depend on
More information3rd Advanced in silico Drug Design KFC/ADD Molecular mechanics intro Karel Berka, Ph.D. Martin Lepšík, Ph.D. Pavel Polishchuk, Ph.D.
3rd Advanced in silico Drug Design KFC/ADD Molecular mechanics intro Karel Berka, Ph.D. Martin Lepšík, Ph.D. Pavel Polishchuk, Ph.D. Thierry Langer, Ph.D. Jana Vrbková, Ph.D. UP Olomouc, 23.1.-26.1. 2018
More informationGiuseppe Felice Mangiatordi
Charge transport in poly-imidazole membranes: a fresh appraisal of the Grotthuss mechanism Giuseppe Felice Mangiatordi Laboratoire d'electrochimie, Chimie des Interfaces et Modélisation, Chimie ParisTech
More informationExact Theory of Kinkable Elastic Polymers
University of Pennsylvania ScholarlyCommons Department of Physics Papers Department of Physics 2-2005 Exact Theory of Kinkable Elastic Polymers Paul A. Wiggins Rob Phillips Philip C. Nelson University
More informationEnergy Landscapes and Accelerated Molecular- Dynamical Techniques for the Study of Protein Folding
Energy Landscapes and Accelerated Molecular- Dynamical Techniques for the Study of Protein Folding John K. Prentice Boulder, CO BioMed Seminar University of New Mexico Physics and Astronomy Department
More informationIndian Institute of Science, Bangalore, India California Institute of Technology, Pasadena, CA 91125
Date of Submission: Email: maiti@physics.iisc.ernet.in Date of Acceptance: Understanding DNA based Nanostructures Prabal K. Maiti 1+, Tod A.Pascal 2, Nagarajan Vaidehi 2,3, and William A. Goddard III 2,
More informationBioengineering 215. An Introduction to Molecular Dynamics for Biomolecules
Bioengineering 215 An Introduction to Molecular Dynamics for Biomolecules David Parker May 18, 2007 ntroduction A principal tool to study biological molecules is molecular dynamics simulations (MD). MD
More informationReplica exchange methodology. John Karanicolas June 2003
Replica exchange methodology John Karanicolas MMTSB@PSC, June 2003 Outline o Motivation o Theory o Practical considerations o MMTSB Tool Set Why? o Sampling on rugged potential energy surfaces is difficult
More informationVilla et al. (2005) Structural dynamics of the lac repressor-dna complex revealed by a multiscale simulation. PNAS 102:
Villa et al. (2005) Structural dynamics of the lac repressor-dna complex revealed by a multiscale simulation. PNAS 102: 6783-6788. Background: The lac operon is a cluster of genes in the E. coli genome
More informationSolvation and Macromolecular Structure. The structure and dynamics of biological macromolecules are strongly influenced by water:
Overview Solvation and Macromolecular Structure The structure and dynamics of biological macromolecules are strongly influenced by water: Electrostatic effects: charges are screened by water molecules
More informationComputational Studies of the Photoreceptor Rhodopsin. Scott E. Feller Wabash College
Computational Studies of the Photoreceptor Rhodopsin Scott E. Feller Wabash College Rhodopsin Photocycle Dark-adapted Rhodopsin hn Isomerize retinal Photorhodopsin ~200 fs Bathorhodopsin Meta-II ms timescale
More informationMolecular Mechanics. Yohann Moreau. November 26, 2015
Molecular Mechanics Yohann Moreau yohann.moreau@ujf-grenoble.fr November 26, 2015 Yohann Moreau (UJF) Molecular Mechanics, Label RFCT 2015 November 26, 2015 1 / 29 Introduction A so-called Force-Field
More informationNon-bonded interactions
speeding up the number-crunching Marcus Elstner and Tomáš Kubař May 8, 2015 why care? key to understand biomolecular structure and function binding of a ligand efficiency of a reaction color of a chromophore
More informationFree energy calculations and the potential of mean force
Free energy calculations and the potential of mean force IMA Workshop on Classical and Quantum Approaches in Molecular Modeling Mark Tuckerman Dept. of Chemistry and Courant Institute of Mathematical Science
More informationBiophysics Biological soft matter
Biophysics Biological soft matter!"#$%&'(&)%*+,-.& /"#$%("%*+,-.0."122,13$(%4(5+& Biophysics lectures outline Biological soft matter 1. Biopolymers 2. Molecular motors 3. The cytoskeleton Biophysics 1.
More informationSupplementary Information. The Solution Structural Ensembles of RNA Kink-turn Motifs and Their Protein Complexes
Supplementary Information The Solution Structural Ensembles of RNA Kink-turn Motifs and Their Protein Complexes Xuesong Shi, a Lin Huang, b David M. J. Lilley, b Pehr B. Harbury a,c and Daniel Herschlag
More informationAssessing the current state of AMBER force field modifications for DNA.
Assessing the current state of AMBER force field modifications for DNA. Supporting Information. Table S1 Average structural parameters for the DDD system with the ε/ζ OL1 +χ OL4 force field modification.
More informationModeling Biological Systems Opportunities for Computer Scientists
Modeling Biological Systems Opportunities for Computer Scientists Filip Jagodzinski RBO Tutorial Series 25 June 2007 Computer Science Robotics & Biology Laboratory Protein: πρώτα, "prota, of Primary Importance
More informationRetinal Proteins (Rhodopsins) Vision, Bioenergetics, Phototaxis. Bacteriorhodopsin s Photocycle. Bacteriorhodopsin s Photocycle
Molecular chanisms of Photoactivation and Spectral Tuning in Retinal Proteins Emad Tajkhorshid Theoretical and Computational Biophysics Group Beckman Institute University of Illinois at Urbana-Champaign
More informationOverview of sparse system identification
Overview of sparse system identification J.-Ch. Loiseau 1 & Others 2, 3 1 Laboratoire DynFluid, Arts et Métiers ParisTech, France 2 LIMSI, Université d Orsay CNRS, France 3 University of Washington, Seattle,
More informationSupporting Information. The hinge region strengthens the nonspecific interaction. between lac-repressor and DNA: a computer simulation.
Supporting Information The hinge region strengthens the nonspecific interaction between lac-repressor and DNA: a computer simulation study Lili Sun 1, Marcin Tabaka 1, Sen Hou 1, Lin Li 2, Krzysztof Burdzy
More informationInfrared spectra of small biomolecules from first-principle molecular dynamics simulations and effective normal mode analysis
Infrared spectra of small biomolecules from first-principle molecular dynamics simulations and effective normal mode analysis R. Vuilleumier, M.-P. Gaigeot and D. Borgis Département de chimie, Ecole Normale
More informationBiomolecules are dynamic no single structure is a perfect model
Molecular Dynamics Simulations of Biomolecules References: A. R. Leach Molecular Modeling Principles and Applications Prentice Hall, 2001. M. P. Allen and D. J. Tildesley "Computer Simulation of Liquids",
More informationTitle: Robust analysis of synthetic label-free DNA junctions in solution by X-ray scattering and molecular simulation
Supplementary Information Title: Robust analysis of synthetic label-free DNA junctions in solution by X-ray scattering and molecular simulation Kyuhyun Im 1,5, Daun Jeong 2,5, Jaehyun Hur 1, Sung-Jin Kim
More informationHands-on : Model Potential Molecular Dynamics
Hands-on : Model Potential Molecular Dynamics OUTLINE 0. DL_POLY code introduction 0.a Input files 1. THF solvent molecule 1.a Geometry optimization 1.b NVE/NVT dynamics 2. Liquid THF 2.a Equilibration
More informationSupporting Information
Supporting Information ph-responsive self-assembly of polysaccharide through a rugged energy landscape Brian H. Morrow, Gregory F. Payne, and Jana Shen Department of Pharmaceutical Sciences, School of
More informationComputational Studies of Molecular Mechanisms Mediating Protein Adsorption on Material Surfaces
Clemson University TigerPrints All Dissertations Dissertations 8-2016 Computational Studies of Molecular Mechanisms Mediating Protein Adsorption on Material Surfaces Tigran M. Abramyan Clemson University
More informationInvestigation of dsdna Stretching Meso-Mechanics Using LS-DYNA
8 th International LS-DYNA Users Conference Simulation echnology (3) Investigation of dsdna Stretching Meso-Mechanics Using LS-DYNA C. A. Yuan and K. N. Chiang Department of Power Mechanical Engineering,
More information3.052 Nanomechanics of Materials and Biomaterials Thursday 02/08/06 Prof. C. Ortiz, MIT-DMSE I LECTURE 2 : THE FORCE TRANSDUCER
I LECTURE 2 : THE FORCE TRANSDUCER Outline : LAST TIME : WHAT IS NANOMECHANICS... 2 HOW CAN WE MEASURE SUCH TINY FORCES?... 3 EXAMPLE OF A FORCE TRANSDUCER... 4 Microfabricated cantilever beams with nanosized
More informationSequence-dependent persistence lengths of DNA
Sequence-dependent persistence lengths of DNA Jonathan S. Mitchell,, Jaroslaw Glowacki, Alexandre E. Grandchamp, Robert S. Manning, and John H. Maddocks, Ecole Polytechnique Fédérale de Lausanne, Switzerland,
More informationNew Measurements of DNA Twist Elasticity
University of Pennsylvania ScholarlyCommons Department of Physics Papers Department of Physics 5-1998 New Measurements of DNA Twist Elasticity Philip C. Nelson University of Pennsylvania, nelson@physics.upenn.edu
More informationAggregates: solid or liquid?
Aggregates: solid or liquid? François Graner Polarity, Division and Morphogenesis team dir. Yohanns Bellaïche Génétique et Biologie du Développement UMR 3215, CNRS & Institut Curie, Paris, France 2011
More informationDissipative Solitons in Physical Systems
Dissipative Solitons in Physical Systems Talk given by H.-G. Purwins Institute of Applied Physics University of Münster, Germany Chapter 1 Introduction Cosmology and Pattern Formation 1-1 Complex Behaviour
More informationBiomolecular modeling I
2015, December 15 Biomolecular simulation Elementary body atom Each atom x, y, z coordinates A protein is a set of coordinates. (Gromacs, A. P. Heiner) Usually one molecule/complex of interest (e.g. protein,
More informationBchem 675 Lecture 9 Electrostatics-Lecture 2 Debye-Hückel: Continued Counter ion condensation
Bchem 675 Lecture 9 Electrostatics-Lecture 2 Debye-Hückel: Continued Counter ion condensation Ion:ion interactions What is the free energy of ion:ion interactions ΔG i-i? Consider an ion in a solution
More informationDownloaded 07/22/17 to Redistribution subject to SIAM license or copyright; see
MULTISCALE MODEL. SIMUL. Vol. 15, No. 3, pp. 1073 1107 c 2017 SIAM. Published by SIAM under the terms of the Creative Commons 4.0 license ABSOLUTE VERSUS RELATIVE ENTROPY PARAMETER ESTIMATION IN A COARSE-GRAIN
More informationPrinciples and Applications of Molecular Dynamics Simulations with NAMD
Principles and Applications of Molecular Dynamics Simulations with NAMD Nov. 14, 2016 Computational Microscope NCSA supercomputer JC Gumbart Assistant Professor of Physics Georgia Institute of Technology
More informationBiomolecular modeling II
2015, December 16 System boundary and the solvent Biomolecule in solution typical MD simulations molecular system in aqueous solution task make the system as small as possible (reduce cost) straightforward
More informationSupporting Information for: Physics Behind the Water Transport through. Nanoporous Graphene and Boron Nitride
Supporting Information for: Physics Behind the Water Transport through Nanoporous Graphene and Boron Nitride Ludovic Garnier, Anthony Szymczyk, Patrice Malfreyt, and Aziz Ghoufi, Institut de Physique de
More informationMolecular Dynamics Simulations. Dr. Noelia Faginas Lago Dipartimento di Chimica,Biologia e Biotecnologie Università di Perugia
Molecular Dynamics Simulations Dr. Noelia Faginas Lago Dipartimento di Chimica,Biologia e Biotecnologie Università di Perugia 1 An Introduction to Molecular Dynamics Simulations Macroscopic properties
More informationComputational Molecular Modeling
Computational Molecular Modeling Lecture 1: Structure Models, Properties Chandrajit Bajaj Today s Outline Intro to atoms, bonds, structure, biomolecules, Geometry of Proteins, Nucleic Acids, Ribosomes,
More informationThe Molecular Dynamics Simulation Process
The Molecular Dynamics Simulation Process For textbooks see: M.P. Allen and D.J. Tildesley. Computer Simulation of Liquids.Oxford University Press, New York, 1987. D. Frenkel and B. Smit. Understanding
More informationDynamics of fast molecular ions in solids and plasmas
Dynamics of fast molecular ions in solids and plasmas Z.L. Miskovic Department of Applied Mathematics, University of Waterloo, Ontario, Canada & Y.-N. Wang and Y.-H. Song Department of Physics, Dalian
More informationFree energy calculations using molecular dynamics simulations. Anna Johansson
Free energy calculations using molecular dynamics simulations Anna Johansson 2007-03-13 Outline Introduction to concepts Why is free energy important? Calculating free energy using MD Thermodynamical Integration
More informationMolecular dynamics simulations of a single stranded (ss) DNA
Molecular dynamics simulations of a single stranded (ss) DNA Subhasish Chatterjee 1, Bonnie Gersten 1, Siddarth Thakur 2, Alexander Burin 2 1 Department of Chemistry, Queens College and the Graduate Center
More informationZwitterionic i-motif structures are preserved in DNA negatively charged ions. produced by electrospray mass spectrometry
S1 Zwitterionic i-motif structures are preserved in DNA negatively charged ions produced by electrospray mass spectrometry Frederic Rosu 1*, Valérie Gabelica 1, Laure Joly 1, Gilles Grégoire 2, Edwin De
More informationProtein Structure Analysis
BINF 731 Protein Modeling Methods Protein Structure Analysis Iosif Vaisman Ab initio methods: solution of a protein folding problem search in conformational space Energy-based methods: energy minimization
More informationPRACTICAL ASPECTS OF NMR RELAXATION STUDIES OF BIOMOLECULAR DYNAMICS
PRACTICAL ASPECTS OF MR RELAXATIO STUDIES OF BIOMOLECULAR DYAMICS Further reading: Can be downloaded from my web page Korzhnev D.E., Billeter M., Arseniev A.S., and Orekhov V. Y., MR Studies of Brownian
More informationAnalysis of the simulation
Analysis of the simulation Marcus Elstner and Tomáš Kubař January 7, 2014 Thermodynamic properties time averages of thermodynamic quantites correspond to ensemble averages (ergodic theorem) some quantities
More informationThe Dominant Interaction Between Peptide and Urea is Electrostatic in Nature: A Molecular Dynamics Simulation Study
Dror Tobi 1 Ron Elber 1,2 Devarajan Thirumalai 3 1 Department of Biological Chemistry, The Hebrew University, Jerusalem 91904, Israel 2 Department of Computer Science, Cornell University, Ithaca, NY 14853
More informationAnalysis of MD trajectories in GROMACS David van der Spoel
Analysis of MD trajectories in GROMACS David van der Spoel What does MD produce? Energy terms E(t) Coordinates x(t) Velocities v(t) Forces f(t) Managing your files trjcat - merging trajectories concatenating
More informationNon-specific DNA-protein interaction: How proteins can diffuse along DNA
XXIX International Colloquium on Group-Theoretical Methods in Physics, Nankai University, Tianjin, Chine. Non-specific DNA-protein interaction: How proteins can diffuse along DNA Fabien Paillusson, Maria
More informationAb initio molecular dynamics and nuclear quantum effects
Ab initio molecular dynamics and nuclear quantum effects Luca M. Ghiringhelli Fritz Haber Institute Hands on workshop density functional theory and beyond: First principles simulations of molecules and
More informationThermodynamic behaviour of mixtures containing CO 2. A molecular simulation study
Thermodynamic behaviour of mixtures containing. A molecular simulation study V. Lachet, C. Nieto-Draghi, B. Creton (IFPEN) Å. Ervik, G. Skaugen, Ø. Wilhelmsen, M. Hammer (SINTEF) Introduction quality issues
More information