Periodic DFT Calculations—Review of Applications in the Pharmaceutical Sciences
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PDF Hosted at the Radboud Repository of the Radboud University Nijmegen
PDF hosted at the Radboud Repository of the Radboud University Nijmegen The following full text is a publisher's version. For additional information about this publication click this link. http://hdl.handle.net/2066/19078 Please be advised that this information was generated on 2021-09-23 and may be subject to change. Computational Chemistry Metho ds Applications to Racemate Resolution and Radical Cation Chemistry ISBN Computational Chemistry Metho ds Applications to Racemate Resolution and Radical Cation Chemistry een wetenschapp elijkeproeve op het gebied van de Natuurwetenschapp en Wiskunde en Informatica Pro efschrift ter verkrijging van de graad van do ctor aan de KatholiekeUniversiteit Nijmegen volgens b esluit van het College van Decanen in het op enbaar te verdedigen op dinsdag januari des namiddags om uur precies do or Gijsb ert Schaftenaar geb oren op augustus te Harderwijk Promotores Prof dr ir A van der Avoird Prof dr E Vlieg Copromotor Prof dr RJ Meier Leden manuscriptcommissie Prof dr G Vriend Prof dr RA de Gro ot Dr ir PES Wormer The research rep orted in this thesis was nancially supp orted by the Dutch Or ganization for the Advancement of Science NWO and DSM Contents Preface Intro duction Intro duction Chirality Metho ds for obtaining pure enantiomers Racemate Resolution via diastereomeric salt formation Rationalization of diastereomeric salt formation Computational metho ds for mo deling the lattice energy Molecular Mechanics Quantum Chemical -
Dmol Guide to Select a Dmol3 Task 1
DMOL3 GUIDE MATERIALS STUDIO 8.0 Copyright Notice ©2014 Dassault Systèmes. All rights reserved. 3DEXPERIENCE, the Compass icon and the 3DS logo, CATIA, SOLIDWORKS, ENOVIA, DELMIA, SIMULIA, GEOVIA, EXALEAD, 3D VIA, BIOVIA and NETVIBES are commercial trademarks or registered trademarks of Dassault Systèmes or its subsidiaries in the U.S. and/or other countries. All other trademarks are owned by their respective owners. Use of any Dassault Systèmes or its subsidiaries trademarks is subject to their express written approval. Acknowledgments and References To print photographs or files of computational results (figures and/or data) obtained using BIOVIA software, acknowledge the source in an appropriate format. For example: "Computational results obtained using software programs from Dassault Systèmes Biovia Corp.. The ab initio calculations were performed with the DMol3 program, and graphical displays generated with Materials Studio." BIOVIA may grant permission to republish or reprint its copyrighted materials. Requests should be submitted to BIOVIA Support, either through electronic mail to [email protected], or in writing to: BIOVIA Support 5005 Wateridge Vista Drive, San Diego, CA 92121 USA Contents DMol3 1 Setting up a molecular dynamics calculation20 Introduction 1 Choosing an ensemble 21 Further Information 1 Defining the time step 21 Tasks in DMol3 2 Defining the thermostat control 21 Energy 3 Constraints during dynamics 21 Setting up the calculation 3 Setting up a transition state calculation 22 Dynamics 4 Which method to use? -
Density Functional Theory (DFT)
Herramientas mecano-cuánticas basadas en DFT para el estudio de moléculas y materiales en Materials Studio 7.0 Javier Ramos Biophysics of Macromolecular Systems group (BIOPHYM) Departamento de Física Macromolecular Instituto de Estructura de la Materia – CSIC [email protected] Webinar, 26 de Junio 2014 Anteriores webinars Como conseguir los videos y las presentaciones de anteriores webminars: Linkedin: Grupo de Química Computacional http://www.linkedin.com/groups/Química-computacional-7487634 Índice Density Functional Theory (DFT) The Jacob’s ladder DFT modules in Maretials Studio DMOL3, CASTEP and ONETEP XC functionals Basis functions Interfaces in Materials Studio Tasks Properties Example: n-butane conformations Density Functional Theory (DFT) DFT is built around the premise that the energy of an electronic system can be defined in terms of its electron probability density (ρ). (Hohenberg-Kohn Theorem) E 0 [ 0 ] Te [ 0 ] E ne [ 0 ] E ee [ 0 ] (easy) Kinetic Energy for ????? noninteracting (r )v (r ) dr electrons(easy) 1 E[]()()[]1 r r d r d r E e e2 1 2 1 2 X C r12 Classic Term(Coulomb) Non-classic Kohn-Sham orbitals Exchange & By minimizing the total energy functional applying the variational principle it is Correlation possible to get the SCF equations (Kohn-Sham) The Jacob’s Ladder Accurate form of XC potential Meta GGA Empirical (Fitting to Non-Empirical Generalized Gradient Approx. atomic properties) (physics rules) Local Density Approximation DFT modules in Materials Studio DMol3: Combine computational speed with the accuracy of quantum mechanical methods to predict materials properties reliably and quickly CASTEP: CASTEP offers simulation capabilities not found elsewhere, such as accurate prediction of phonon spectra, dielectric constants, and optical properties. -
EPSRC Service Level Agreement with STFC for Computational Science Support
CoSeC Computational Science Centre for Research Communities EPSRC Service Level Agreement with STFC for Computational Science Support FY 2016/17 Report and Update on FY 2017/18 Work Plans This document contains the 2016/17 plans, 2016/17 summary reports, and 2017/18 plans for the programme in support of CCP and HEC communities delivered by STFC and funded by EPSRC through a Service Level Agreement. Notes in blue are in-year updates on progress to the tasks included in the 2016/17 plans. Text highlighted in yellow shows changes to the draft 2017/18 plans that we submitted in January 2017. Contents CCP5 – Computer Simulation of Condensed Phases .......................................................................... 4 CCP5 – 2016 / 17 Plans (1 April 2016 – 31 March 2017) ...................................................... 4 CCP5 – Summary Report (1 April 2016 – 31 March 2017) .................................................... 7 CCP5 –2017 / 18 Plans (1 April 2017 – 31 March 2018) ....................................................... 8 CCP9 – Electronic Structure of Solids .................................................................................................. 9 CCP9 – 2016 / 17 Plans (1 April 2016 – 31 March 2017) ...................................................... 9 CCP9 – Summary Report (1 April 2016 – 31 March 2017) .................................................. 11 CCP9 – 2017 / 18 Plans (1 April 2017 – 31 March 2018) .................................................... 12 CCP-mag – Computational Multiscale -
Prediction of Solubility of Amino Acids Based on Cosmo Calculaition
PREDICTION OF SOLUBILITY OF AMINO ACIDS BASED ON COSMO CALCULAITION by Kaiyu Li A dissertation submitted to Johns Hopkins University in conformity with the requirement for the degree of Master of Science in Engineering Baltimore, Maryland October 2019 Abstract In order to maximize the concentration of amino acids in the culture, we need to obtain solubility of amino acid as a function of concentration of other components in the solution. This function can be obtained by calculating the activity coefficient along with solubility model. The activity coefficient of the amino acid can be calculated by UNIFAC. Due to the wide range of applications of UNIFAC, the prediction of the activity coefficient of amino acids is not very accurate. So we want to fit the parameters specific to amino acids based on the UNIFAC framework and existing solubility data. Due to the lack of solubility of amino acids in the multi-system, some interaction parameters are not available. COSMO is a widely used way to describe pairwise interactions in the solutions in the chemical industry. After suitable assumptions COSMO can calculate the pairwise interactions in the solutions, and largely reduce the complexion of quantum chemical calculation. In this paper, a method combining quantum chemistry and COSMO calculation is designed to accurately predict the solubility of amino acids in multi-component solutions in the ii absence of parameters, as a supplement to experimental data. Primary Reader and Advisor: Marc D. Donohue Secondary Reader: Gregory Aranovich iii Contents -
What's New in Biovia Materials Studio 2020
WHAT’S NEW IN BIOVIA MATERIALS STUDIO 2020 Datasheet BIOVIA Materials Studio 2020 is the latest release of BIOVIA’s predictive science tools for chemistry and materials science research. Materials Studio empowers researchers to understand the relationships between a material’s mo- lecular or crystal structure and its properties in order to make more informed decisions about materials research and development. More often than not materials performance is influenced by phenomena at multiple scales. Scientists using Materials Studio 2020 have an extensive suite of world class solvers and parameter sets operating from atoms to microscale for simulating more materials and more properties than ever before. Furthermore, the predicted properties can now be used in multi-physics modeling and in systems modeling software such as SIMULIA Abaqus and CATIA Dymola to predict macroscopic behaviors. In this way multiscale simulations can be used to solve some of the toughest pro- blems in materials design and product optimization. BETTER MATERIALS - BETTER BATTERIES Safe, fast charging batteries with high energy density and long life are urgently needed for a host of applications - not least for the electrification of all modes of transportation as an alternative to fossil fuel energy sources. Battery design relies on a complex interplay between thermal, mechanical and chemical processes from the smallest scales of the material (electronic structure) through to the geometry of the battery cell and pack design. Improvements to the component materials used in batteries and capacitors are fundamental to providing the advances in performance needed. Materials Studio provides new functionality to enable the simula- tion of key materials parameters for both liquid electrolytes and electrode components. -
Arxiv:1508.02735V1 [Cond-Mat.Mtrl-Sci] 11 Aug 2015
A critical look at methods for calculating charge transfer couplings fast and accurately Pablo Ramos, Marc Mankarious, and Michele Pavanello∗ Department of Chemistry, Rutgers University, Newark, NJ 07102, USA E-mail: [email protected] Abstract We present here a short and subjective review of methods for calculating charge trans- fer couplings. Although we mostly focus on Density Functional Theory, we discuss a small subset of semiempirical methods as well as the adiabatic-to-diabatic transformation methods typically coupled with wavefunction-based electronic structure calculations. In this work, we will present the reader with a critical assessment of the regimes that can be modelled by the various methods – their strengths and weaknesses. In order to give a feeling about the practical aspects of the calculations, we also provide the reader with a practical protocol for running coupling calculations with the recently developed FDE-ET method. arXiv:1508.02735v1 [cond-mat.mtrl-sci] 11 Aug 2015 ∗To whom correspondence should be addressed 1 Contents 1 Introduction 3 2 DFT Based Methods 5 2.1 The Frozen Density Embedding formalism . 5 2.1.1 FDE-ET method . 9 2.1.2 Distance dependence of the electronic coupling . 12 2.1.3 Hole transfer in DNA oligomers . 14 2.2 Constrained Density Functional Theory Applied to Electron Transfer Simulations . 16 2.3 Fragment Orbital DFT . 18 2.3.1 Hole transfer rates on DNA hairpins . 20 2.3.2 The Curious Case of Sulfite Oxidase . 20 2.4 Ultrafast computations of the electronic couplings: The AOM method . 22 2.5 Note on orthogonality . -
Interoperability Between Electronic Structure Codes with the Quippy Toolkit
Interoperability between electronic structure codes with the quippy toolkit James Kermode Department of Physics King’s College London 6 September 2012 Outline Overview of libAtoms and QUIP Scripting interfaces Overview of quippy capabilities Live demo! Summary and Conclusions Outline Overview of libAtoms and QUIP Scripting interfaces Overview of quippy capabilities Live demo! Summary and Conclusions I The QUIP (QUantum mechanics and Interatomic Potentials) package, built on top of libAtoms, implements a wide variety of interatomic potentials and tight binding quantum mechanics, and is also able to call external packages. I Various hybrid combinations are also supported in the style of QM/MM, including ‘Learn on the Fly’ scheme (LOTF).2 3 I quippy is a Python interface to libAtoms and QUIP. The libAtoms, QUIP and quippy packages 1 I The libAtoms package is a software library written in Fortran 95 for the purposes of carrying out molecular dynamics simulations. 1http://www.libatoms.org 2Csányi et al., PRL (2004) 3http://www.jrkermode.co.uk/quippy I Various hybrid combinations are also supported in the style of QM/MM, including ‘Learn on the Fly’ scheme (LOTF).2 3 I quippy is a Python interface to libAtoms and QUIP. The libAtoms, QUIP and quippy packages 1 I The libAtoms package is a software library written in Fortran 95 for the purposes of carrying out molecular dynamics simulations. I The QUIP (QUantum mechanics and Interatomic Potentials) package, built on top of libAtoms, implements a wide variety of interatomic potentials and tight binding quantum mechanics, and is also able to call external packages. 1http://www.libatoms.org 2Csányi et al., PRL (2004) 3http://www.jrkermode.co.uk/quippy 3 I quippy is a Python interface to libAtoms and QUIP. -
Surface Functionalization of H-Terminated Diamond with NH and NH2 on the (1, 0, 0), (1, 1, 0) and (1, 1, 1) Surface Planes Using Density Functional Theory
Uppsala University Bachelor project, 15hp Surface functionalization of H-terminated diamond with NH and NH2 on the (1; 0; 0), (1; 1; 0) and (1; 1; 1) surface planes using Density Functional Theory Sara Kjellberg Supervised by Prof. Karin Larsson October 5, 2017 Abstract The adsorption energy of aminated diamond surfaces on the (1; 1; 1), (1; 1; 0) and (1; 0; 0) diamond surfaces have been calculated with density functional theory (DFT). The resulting values show that bridging is favoured before on-top nitrogen at low coverage for all the low index planes. The trend is even more pronounced as the coverage increases, most likely due to sterical hindrance. As expected, the imidogen (NH) and amidogen (NH2) groups are bonded to the surface planes in the order (1; 0; 0) > (1; 1; 1) > (1; 1; 0) as decrease in energy is the highest on the (1; 0; 0) plane and lowest on the (1 010) plane. The effect of sterical hindrance is largest at the (1; 1; 0) surface while the (1; 0; 0) surface is almost unaffected by neighbouring functional groups. Also, double bonded on-top imidogen (NH) is the least stable group at the (1; 0; 0) surface at low coverage while it is almost as stable as bridging NH when having a full mono-layer. Moreover, on-top imidogen (NH) was highly distorted and forced a change in surface geometry 1 Contents 1 Goal 3 2 Introduction 3 2.1 Background . .3 3 Theory 4 3.1 Surfaces of diamond . .4 3.1.1 General surface theory . -
Trends in Atomistic Simulation Software Usage [1.3]
A LiveCoMS Perpetual Review Trends in atomistic simulation software usage [1.3] Leopold Talirz1,2,3*, Luca M. Ghiringhelli4, Berend Smit1,3 1Laboratory of Molecular Simulation (LSMO), Institut des Sciences et Ingenierie Chimiques, Valais, École Polytechnique Fédérale de Lausanne, CH-1951 Sion, Switzerland; 2Theory and Simulation of Materials (THEOS), Faculté des Sciences et Techniques de l’Ingénieur, École Polytechnique Fédérale de Lausanne, CH-1015 Lausanne, Switzerland; 3National Centre for Computational Design and Discovery of Novel Materials (MARVEL), École Polytechnique Fédérale de Lausanne, CH-1015 Lausanne, Switzerland; 4The NOMAD Laboratory at the Fritz Haber Institute of the Max Planck Society and Humboldt University, Berlin, Germany This LiveCoMS document is Abstract Driven by the unprecedented computational power available to scientific research, the maintained online on GitHub at https: use of computers in solid-state physics, chemistry and materials science has been on a continuous //github.com/ltalirz/ rise. This review focuses on the software used for the simulation of matter at the atomic scale. We livecoms-atomistic-software; provide a comprehensive overview of major codes in the field, and analyze how citations to these to provide feedback, suggestions, or help codes in the academic literature have evolved since 2010. An interactive version of the underlying improve it, please visit the data set is available at https://atomistic.software. GitHub repository and participate via the issue tracker. This version dated August *For correspondence: 30, 2021 [email protected] (LT) 1 Introduction Gaussian [2], were already released in the 1970s, followed Scientists today have unprecedented access to computa- by force-field codes, such as GROMOS [3], and periodic tional power. -
Porting the DFT Code CASTEP to Gpgpus
Porting the DFT code CASTEP to GPGPUs Toni Collis [email protected] EPCC, University of Edinburgh CASTEP and GPGPUs Outline • Why are we interested in CASTEP and Density Functional Theory codes. • Brief introduction to CASTEP underlying computational problems. • The OpenACC implementation http://www.nu-fuse.com CASTEP: a DFT code • CASTEP is a commercial and academic software package • Capable of Density Functional Theory (DFT) and plane wave basis set calculations. • Calculates the structure and motions of materials by the use of electronic structure (atom positions are dictated by their electrons). • Modern CASTEP is a re-write of the original serial code, developed by Universities of York, Durham, St. Andrews, Cambridge and Rutherford Labs http://www.nu-fuse.com CASTEP: a DFT code • DFT/ab initio software packages are one of the largest users of HECToR (UK national supercomputing service, based at University of Edinburgh). • Codes such as CASTEP, VASP and CP2K. All involve solving a Hamiltonian to explain the electronic structure. • DFT codes are becoming more complex and with more functionality. http://www.nu-fuse.com HECToR • UK National HPC Service • Currently 30- cabinet Cray XE6 system – 90,112 cores • Each node has – 2×16-core AMD Opterons (2.3GHz Interlagos) – 32 GB memory • Peak of over 800 TF and 90 TB of memory http://www.nu-fuse.com HECToR usage statistics Phase 3 statistics (Nov 2011 - Apr 2013) Ab initio codes (VASP, CP2K, CASTEP, ONETEP, NWChem, Quantum Espresso, GAMESS-US, SIESTA, GAMESS-UK, MOLPRO) GS2NEMO ChemShell 2%2% SENGA2% 3% UM Others 4% 34% MITgcm 4% CASTEP 4% GROMACS 6% DL_POLY CP2K VASP 5% 8% 19% http://www.nu-fuse.com HECToR usage statistics Phase 3 statistics (Nov 2011 - Apr 2013) 35% of the Chemistry software on HECToR is using DFT methods. -
HPC Issues for DFT Calculations
HPC Issues for DFT Calculations Adrian Jackson EPCC Scientific Simulation • Simulation fast becoming 4 th pillar of science – Observation, Theory, Experimentation, Simulation • Explore universe through simulation rather than experimentation – Test theories – Predict or validate experiments – Simulate “untestable” science • Reproduce “real world” in computers – Generally simplified – Dimensions and timescales restricted – Simulation of scientific problem or environment – Input of real data – Output of simulated data – Parameter space studies – Wide range of approaches http://www.nu-fuse.com Reduce runtime • Serial code optimisations – Reduce runtime through efficiencies – Unlikely to produce required savings • Upgrade hardware – 1965: Moore’s law predicts growth in complexity of processors – Doubling of CPU performance – Performance often improved through on chip parallelism http://www.nu-fuse.com Parallel Background • Why not just make a faster chip? – Theoretical • Physical limitations to size and speed of a single chip • Capacitance increases with complexity • Speed of light, size of atoms, dissipation of heat • The power used by a CPU core is proportional to Clock Frequency x Voltage 2 • Voltage reduction vs Clock speed for power requirements – Voltages become too small for “digital” differences – Practical • Developing new chips is incredibly expensive • Must make maximum use of existing technology http://www.nu-fuse.com Parallel Systems • Different types of parallel systems P M – Shared memory P M P M – Distributed memory P M Interconnect