Practicalities on using MD

Slides:



Advertisements
Similar presentations
Precalculus 2 Section 10.6 Parametric Equations
Advertisements

Statistical mechanics
Introducing the coordinates in Z-matrix form Objectives study how to introduce the coordinates of a molecule in Z-matrix form.
Where and When?! Ch. 3 Section 2. Coordinate Systems Tells you where the zero point of the variable is located and the direction in which the values measured.
What is shape function ? shape function is a function that will give the displacements inside an element if its displacement at all the node locations.
Specifying Molecular Electronic and Geometrical Structures.
(4C) N1 O2 O3 O4 O5 O6 H14 H13 H7 H8 H9 H10 H11 H12 (4F) N1 O2 O3 O4 O5 O6 H13 H14 H7 H8 H9 H10 H11 H12 Supplementary Figure1. Calculated structures of.
Analyzing MD Results. Extracting system properties from the data written to the mdout files MD information is written in the form: NSTEP = 100 TIME(PS)
CSCE 641: Forward kinematics and inverse kinematics Jinxiang Chai.
Molecular dynamics and applications to amyloidogenic sequences Nurit Haspel, David Zanuy, Ruth Nussinov (in cooperation with Ehud Gazit’s group)
Geometry Optimization Pertemuan VI. Geometry Optimization Backgrounds Real molecules vibrate thermally about their equilibrium structures. Finding minimum.
Arborless Bender Analytical Model. Arborless Bender Geometry Diagram - top viewCorresponding geometry.
Levels of protein structure organization
Computer Animations of Molecular Vibration Michael McGuan and Robert M. Hanson Summer Research 2004 Department of Chemistry St. Olaf College Northfield,
Vector Operation and Force Analysis
Introduction to run Siesta
Springs And pendula, and energy. Harmonic Motion Pendula and springs are examples of things that go through simple harmonic motion. Simple harmonic motion.
 From TI-83 Plus Graphing Calculator For Dummies by C. C. EdwardsTI-83 Plus Graphing Calculator For Dummies  The TI-83 Plus graphing calculator is designed.
Inverse Kinematics for Molecular World Sadia Malik April 18, 2002 CS 395T U.T. Austin.
Valence bond theory Electrons are not simply dots And bonds are not sticks.
Javier Junquera Molecular dynamics in the microcanonical (NVE) ensemble: the Verlet algorithm.
PRESENTATION Presentation of Coordinate system. APPLICATION OF COORDINATE SYSTEM Modeling small molecules building 3D- structures of small molecules of.
Basic Computations with 3D Structures
1 CE 530 Molecular Simulation Lecture 17 Beyond Atoms: Simulating Molecules David A. Kofke Department of Chemical Engineering SUNY Buffalo
Kinematics Velocity and Acceleration. Motion Change in position of object in relation to things that are considered stationary Usually earth is considered.
E-science grid facility for Europe and Latin America E2GRIS1 André A. S. T. Ribeiro – UFRJ (Brazil) Itacuruça (Brazil), 2-15 November 2008.
Molecular Specification Anan Wu Typical Gaussian Input Molecular specification This input section mainly specifies the nuclear positions.
Molecular simulation methods Ab-initio methods (Few approximations but slow) DFT CPMD Electron and nuclei treated explicitly. Classical atomistic methods.
Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Covalent Bonding: Hybrid Atomic Orbitals.
Specifying Molecular Electronic and Geometrical Structures
Warm-Up What is the scale factor (or similarity ratio) of the following two triangles?
How to generate a mixed pseudopotential Objectives Generate a mixed pseudopotential to be used in the Virtual Crystal Approximation or in simulations at.
Motion IPC NOTES. MOTION & POSITION motion – a change in an object’s position relative to a reference point.
Section 3: Molecular Geometry.  Multiple Bonds – occur in covalent compounds when atoms share more than one pair of electrons  Double Bond – atoms share.
WS3-1 ADM740, Workshop 3, June 2007 Copyright  2007 MSC.Software Corporation WORKSHOP 3 CREATING AND ADJUSTING SUSPENSIONS.
Use Similar Right Triangles
Geometry Section 6.6 Use Proportionality Theorems.
TODAY IN GEOMETRY…  Learning Target: 6.6 You will calculate missing sides of triangles using proportionality with parallel lines  Independent Practice.
Graphing Motion Physics 11. Some humour to start…..
Orbital Hybridisation & VSEPR Learning Goals Students will be able to predict the hybridization in a variety of compounds using Lewis Structures & energy.
1.What kind of energy do these apples have, KE, PE, or both? 2.Is there any other type of energy the apples could have? Bellringer.
Geometry Optimizations Lecture CompChem 2 Chemistry 347 Hope College.
Parallel Molecular Dynamics A case study : Programming for performance Laxmikant Kale
Bell Ringer Solve even #’s Pg. 34.
CSCE 441: Computer Graphics Forward/Inverse kinematics
Springs And pendula, and energy.
Make sure your worksheet from Friday is complete and turn it in
Kinematics in Two Dimensions
Motion with Constant Acceleration
Lecture #2 (ref Ch 2) Vector Operation and Force Analysis 1 R. Michael PE 8/14/2012.
DL_POLY Miguel A. Gonzalez Institut Laue-Langevin
Chemical Bonding: Valence Bond Theory “in a nutshell” Chapter 10 Section 4 through 6 of Jespersen 6th Ed) Dr. C. Yau Spring
Section 3.2 – The Dot Product
CSCE 441: Computer Graphics Forward/Inverse kinematics
Graphing Motion Walk Around
1. Pure Protein (0.3 mL, mM; ~ 10 mg)
Exploring Four Empires of Mesopotamia
Section 1 Displacement and Velocity
Velocity Pages.
Section 1: Measuring Motion
Shape of the Molecule Use VSEPR Theory
Ch. 11: Motion 11.1: Distance and Displacement
LMC Little Man Computer What do you know about LMC?
Section 9.4 – Solving Differential Equations Symbolically
Section 1: Measuring Motion
More to Learn Viewing file details
Section 1: Measuring Motion
Vector Equations Trig 6.12 Obj: Find the vector equation parallel to a given vector and through a given point.
In what follows we present some QCT movies
Kinematics in Two Dimensions
Presentation transcript:

Practicalities on using MD Geometry constraints: Z-matrix Equilibration of MD Restart of phonon calculations

Z-Matrix coordinate format Internal coordinates: Molecules represented by : Bond lengths i Bending angles i Dihedral angles i  

Z-Matrix Allows for mixing of generalised and Cartesian coordinates: Useful for constraint relaxations Explore the PES by using A relevant coordinate: Useful for estimating barriers

Z-matrix Symbol Section ------- Variables zm1 2.55000000000000 Constants cc 1.41700000000000 ccc 120.000000000000 ch 1.11200000000000 cch 120.000000000000 ------------ End of Z-matrix Information

Equilibration of MD

Moving -windows Divide the trajectories in overlapping windows of 7.5 ps length and 2 ps interval Moving -windows

Output files SystemLabel.XV Stores coordinates and Velocities, necessary for restarts (keep always a backup copy!!) SystemLabel.MDE SystemLabel.MD : Saves positions and Velocities for each time frame, formatted.

Phonon Calculations Easy to parallelize: Each displacement is independent of others. We can parallelize by atoms. Care is needed when reassembling the .FC files. If calculation crashes we can restart it without loosing information, but doing it with care.