Implementation of Methods to Accurately Predict Transition Pathways and the Underlying Potential Energy Surface of Biomolecular Systems

Total Page:16

File Type:pdf, Size:1020Kb

Implementation of Methods to Accurately Predict Transition Pathways and the Underlying Potential Energy Surface of Biomolecular Systems IMPLEMENTATION OF METHODS TO ACCURATELY PREDICT TRANSITION PATHWAYS AND THE UNDERLYING POTENTIAL ENERGY SURFACE OF BIOMOLECULAR SYSTEMS By DELARAM GHOREISHI A DISSERTATION PRESENTED TO THE GRADUATE SCHOOL OF THE UNIVERSITY OF FLORIDA IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY UNIVERSITY OF FLORIDA 2019 c 2019 Delaram Ghoreishi I dedicate this dissertation to my mother, my brother, and my partner. For their endless love, support, and encouragement. ACKNOWLEDGMENTS I am thankful to my advisor, Adrian Roitberg, for his guidance during my graduate studies. I am grateful for the opportunities he provided me and for allowing me to work independently. I also thank my committee members, Rodney Bartlett, Xiaoguang Zhang, and Alberto Perez, for their valuable inputs. I am grateful to the University of Florida Informatics Institue for providing financial support in 2016, allowing me to take a break from teaching and focus more on research. I like to acknowledge my group members and friends for their moral support and technical assistance. Natali di Russo helped me become familiar with Amber. I thank Pilar Buteler, Sunidhi Lenka, and Vinicius Cruzeiro for daily conversations regarding science and life. Pancham Lal Gupta was my cpptraj encyclopedia. I thank my physicist colleagues, Ankita Sarkar and Dustin Tracy, who went through the intense physics coursework with me during the first year. I thank Farhad Ramezanghorbani, Justin Smith, Kavindri Ranasinghe, and Xiang Gao for helpful discussions regarding ANI and active learning. I also thank David Cerutti from Rutgers University for his help with NEB implementation. I thank Pilar Buteler and Alvaro Gonzalez for the good times we had camping and climbing. Lastly, I express my sincere gratitude to Farhad Ramezanghorbani for always being there for me, for encouraging me, and for his significant scientific inputs. I also thank my mother, Fatemeh Kaheh, and my brother, Ramin Ghoreishi, for their love and encouragement at every step of my life. I am forever grateful to all three of them. 4 TABLE OF CONTENTS page ACKNOWLEDGMENTS...................................4 LIST OF TABLES......................................8 LIST OF FIGURES.....................................9 ABSTRACT......................................... 11 CHAPTER 1 INTRODUCTION................................... 13 1.1 Minimum Energy Path Sampling........................ 13 1.2 Molecular Dynamics with Machine Learned Potentials............. 15 2 THEORY AND METHODS.............................. 17 2.1 Statistical Mechanics............................... 17 2.1.1 Statistical Ensembles........................... 18 2.1.2 Microcanonical Ensembles: Constant N-V-E............... 19 2.1.3 Canonical Ensembles: Constant N-V-T................. 20 2.1.4 Isothermal-Isobaric Ensembles: Constant N-P-T............. 20 2.1.5 Grand Canonical Ensembles: Constant µ-V-T.............. 21 2.2 Nudged Elastic Band............................... 21 2.3 String Method.................................. 25 2.4 Free Energy and Transition Rate Calculations.................. 27 2.5 Computational Methods of Free Energy Calculations.............. 28 2.5.1 Free Energy Perturbation......................... 29 2.5.2 Thermodynamic Integration....................... 31 2.5.3 Bennett Acceptance Ratio........................ 31 2.6 Indirect Approach to Free Energy Calculations................. 33 2.7 Feed-Froward Neural Networks......................... 35 2.8 Active Learning................................. 38 2.9 Transfer Learning................................ 39 2.10 ANI Neural Network Potentials......................... 40 2.10.1 Network Architecture........................... 40 2.10.2 Sampling the Chemical Space...................... 42 2.10.2.1 Normal Mode Sampling.................... 44 2.10.2.2 Molecular Dynamics Sampling................. 44 3 IMPLEMENTATION.................................. 45 3.1 Implementation of Nudged Elastic Band in Amber............... 45 3.2 Implementaion of ANI-Amber Interface..................... 47 3.3 Sample Amber Input Files............................ 50 5 3.3.1 Sample Input File for NEB Simulations................. 50 3.3.2 Sample Input File for ANI Simulations.................. 51 4 NUDGED ELASTIC BAND: VALIDATION AND RESULTS............. 53 4.1 Computational Details.............................. 53 4.1.1 Test Case 1: Conformational Change of Alanine Dipeptide....... 53 4.1.2 Test Case 2: α-helix to β-sheet Transition in Polyalanine........ 54 4.1.3 Test Case 3: Base Eversion Pathway of the OGG1{DNA Complex... 55 4.2 Accuracy Tests.................................. 55 4.2.1 Test Case 1: Conformational Change of Alanine Dipeptide....... 55 4.2.2 Test Case 2: α-helix to β-sheet Transition in Polyalanine........ 57 4.2.3 Test Case 3: Base Eversion Pathway of the OGG1{DNA Complex... 58 4.3 Timing Benchmarks............................... 59 5 FREE ENERGY METHODS WITH MACHINE LEARNING............. 64 5.1 Two Dimensional Energy Surface with ANI-Amber............... 64 5.2 End-State Free Energy Corrections....................... 65 5.2.1 Conformational Free Energy with ANI-Amber.............. 66 5.2.2 Hydration Free Energy with ANI-Amber................. 69 5.2.2.1 Data preparation and network training............ 70 5.2.2.2 Energy prediction results.................... 71 6 CONCLUDING REMARKS AND FUTURE DIRECTIONS.............. 74 6.1 Final Remarks on Nudged Elastic Band..................... 74 6.2 Final Remarks on Free Energy Calculations with ANI-Ambers......... 75 APPENDIX A KABSCH ALGORITHM................................ 77 B PARAMETERIZATION OF A CURVE........................ 79 B.1 Re-parameterization of a Curve......................... 79 B.2 Arclength of a Curve............................... 79 B.3 Arclength Parameterization........................... 80 C DERIVATION OF EQUATION (2-42)........................ 81 D PENALTY METHOD................................. 82 E TWO DIMENSIONAL TEST POTENTIALS..................... 83 E.1 LEPS Potential.................................. 83 E.2 LEPS Harmonic Oscillator Potential....................... 83 F ALANINE DIPEPTIDE CONFORMATIONAL CHANGE............... 85 6 REFERENCES........................................ 86 BIOGRAPHICAL SKETCH................................. 95 7 LIST OF TABLES Table page 5-1 Free energy difference of cis/trans conformational transition............. 69 8 LIST OF FIGURES Figure page 2-1 Mass and spring representation of NEB........................ 22 2-2 Force decoupling representation of NEB........................ 24 2-3 Thermodynamic cycle of indirect approach...................... 34 2-4 Feed-forward neural network.............................. 35 2-5 Active learning work-flow............................... 39 2-6 Transfer learning work-flow.............................. 41 2-7 Radial symmetry functionals.............................. 41 2-8 ANI neural network potential............................. 43 3-1 MPI implementation of NEB in Amber........................ 46 3-2 GPU implementation of NEB in Amber........................ 47 3-3 Amber molecular dynamics.............................. 48 3-4 ANI-Amber molecular dynamics............................ 49 4-1 Alanine dipeptide potential energy surface...................... 56 4-2 Energy of NEB replicas in alanine dipeptide...................... 57 4-3 End to end distance in polyalanine.......................... 58 4-4 Glycosidic angle vs. eversion distance......................... 60 4-5 Performance comparison between sander and pmemd................. 60 4-6 Performance comparison for different nebfreq values................. 62 4-7 Performance dependence on the size of the data transfers.............. 63 5-1 Ethylene glycol..................................... 64 5-2 Two-dimensional energy surface with GAFF..................... 65 5-3 Two-dimensional energy surface with ANI-1x..................... 66 5-4 cis conformer N-methyl acetamide........................... 66 5-5 trans conformer N-methyl acetamide......................... 67 5-6 Umbrella sampling................................... 68 9 5-7 Endpoint correction.................................. 69 5-8 Data preparation.................................... 70 5-9 Energy prediction results................................ 72 5-10 Cumulative number of data-points.......................... 73 F-1 φ dihedral angle change of NEB replicas in alanine dipeptide............. 85 F-2 dihedral angle change of NEB replicas in alanine dipeptide............ 85 10 Abstract of Dissertation Presented to the Graduate School of the University of Florida in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy IMPLEMENTATION OF METHODS TO ACCURATELY PREDICT TRANSITION PATHWAYS AND THE UNDERLYING POTENTIAL ENERGY SURFACE OF BIOMOLECULAR SYSTEMS By Delaram Ghoreishi December 2019 Chair: Adrian Roitberg Major: Physics This thesis focuses on the fast implementation of the nudged elastic band (NEB) method, and the implementation of the interface of a deep neural network potential into the AMBER molecular dynamics package. The details of the implementations and validation results are explored within this document. The reliability of physics-based simulations is restricted by the accuracy of potential energies that regulate the dynamics of a system of particles, as well as the efficiency and the precision of the advanced sampling techniques. Biological systems often experience transitions that completely change their conformations
Recommended publications
  • Multiscale Simulation of Laser Ablation and Processing of Semiconductor Materials
    University of Central Florida STARS Electronic Theses and Dissertations, 2004-2019 2012 Multiscale Simulation Of Laser Ablation And Processing Of Semiconductor Materials Lalit Shokeen University of Central Florida Part of the Materials Science and Engineering Commons Find similar works at: https://stars.library.ucf.edu/etd University of Central Florida Libraries http://library.ucf.edu This Doctoral Dissertation (Open Access) is brought to you for free and open access by STARS. It has been accepted for inclusion in Electronic Theses and Dissertations, 2004-2019 by an authorized administrator of STARS. For more information, please contact [email protected]. STARS Citation Shokeen, Lalit, "Multiscale Simulation Of Laser Ablation And Processing Of Semiconductor Materials" (2012). Electronic Theses and Dissertations, 2004-2019. 2420. https://stars.library.ucf.edu/etd/2420 MULTISCALE SIMULATION OF LASER PROCESSING AND ABLATION OF SEMICONDUCTOR MATERIALS by LALIT SHOKEEN Bachelor of Science (B.Sc. Physics), University of Delhi, India, 2006 Masters of Science (M.Sc. Physics), University of Delhi, India, 2008 Master of Science (M.S. Materials Engg.), University of Central Florida, USA, 2009 A dissertation submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy in the Department of Mechanical, Materials and Aerospace Engineering in the College of Engineering and Computer Science at the University of Central Florida Orlando, Florida, USA Fall Term 2012 Major Professor: Patrick Schelling © 2012 Lalit Shokeen ii ABSTRACT We present a model of laser-solid interactions in silicon based on an empirical potential developed under conditions of strong electronic excitations. The parameters of the interatomic potential depends on the temperature of the electronic subsystem Te, which is directly related to the density of the electron-hole pairs and hence the number of broken bonds.
    [Show full text]
  • UOW High Performance Computing Cluster User's Guide
    UOW High Performance Computing Cluster User’s Guide Information Management & Technology Services University of Wollongong ( Last updated on February 2, 2015) Contents 1. Overview6 1.1. Specification................................6 1.2. Access....................................7 1.3. File System.................................7 2. Quick Start9 2.1. Access the HPC Cluster...........................9 2.1.1. From within the UOW campus...................9 2.1.2. From the outside of UOW campus.................9 2.2. Work at the HPC Cluster.......................... 10 2.2.1. Being familiar with the environment................ 10 2.2.2. Setup the working space...................... 11 2.2.3. Initialize the computational task.................. 11 2.2.4. Submit your job and check the results............... 14 3. Software 17 3.1. Software Installation............................ 17 3.2. Software Environment........................... 17 3.3. Software List................................ 19 4. Queue System 22 4.1. Queue Structure............................... 22 4.1.1. Normal queue............................ 22 4.1.2. Special queues........................... 23 4.1.3. Schedule policy........................... 23 4.2. Job Management.............................. 23 4.2.1. PBS options............................. 23 4.2.2. Submit a batch job......................... 25 4.2.3. Check the job/queue status..................... 27 4.2.4. Submit an interactive job...................... 29 4.2.5. Submit workflow jobs....................... 30 4.2.6. Delete jobs............................. 31 5. Utilization Agreement 32 5.1. Policy.................................... 32 5.2. Acknowledgements............................. 32 5.3. Contact Information............................. 33 Appendices 35 A. Access the HPC cluster from Windows clients 35 A.1. Putty..................................... 35 A.2. Configure ‘Putty’ with UOW proxy.................... 36 A.3. SSH Secure Shell Client.......................... 38 B. Enable Linux GUI applications using Xming 41 B.1.
    [Show full text]
  • Redox Active Iron Nitrosyl Units in Proton Reduction Electrocatalysis
    ARTICLE Received 11 Nov 2013 | Accepted 18 Mar 2014 | Published 2 May 2014 DOI: 10.1038/ncomms4684 Redox active iron nitrosyl units in proton reduction electrocatalysis Chung-Hung Hsieh1, Shengda Ding1,O¨ zlen F. Erdem2, Danielle J. Crouthers1, Tianbiao Liu3, Charles C.L. McCrory4, Wolfgang Lubitz2, Codrina V. Popescu5, Joseph H. Reibenspies1, Michael B. Hall1 & Marcetta Y. Darensbourg1 Base metal, molecular catalysts for the fundamental process of conversion of protons and electrons to dihydrogen, remain a substantial synthetic goal related to a sustainable energy future. Here we report a diiron complex with bridging thiolates in the butterfly shape of the 2Fe2S core of the [FeFe]-hydrogenase active site but with nitrosyl rather than þ carbonyl or cyanide ligands. This binuclear [(NO)Fe(N2S2)Fe(NO)2] complex maintains structural integrity in two redox levels; it consists of a (N2S2)Fe(NO) complex (N2S2 ¼ N,N0-bis(2-mercaptoethyl)-1,4-diazacycloheptane) that serves as redox active metallo- dithiolato bidentate ligand to a redox active dinitrosyl iron unit, Fe(NO)2. Experimental and theoretical methods demonstrate the accommodation of redox levels in both components of the complex, each involving electronically versatile nitrosyl ligands. An interplay of orbital mixing between the Fe(NO) and Fe(NO)2 sites and within the iron nitrosyl bonds in each moiety is revealed, accounting for the interactions that facilitate electron uptake, storage and proton reduction. 1 Department of Chemistry, Texas A&M University, College Station, Texas 77843, USA. 2 Max Planck Institute for Chemical Energy Conversion, Stiftstrasse 34-36, 45470 Muelheim a.d. Ruhr, Germany. 3 Center for Molecular Electrocatalysis, Pacific Northwest National Laboratory, Richland, Washington 99354, USA.
    [Show full text]
  • Computational Chemistry: a Practical Guide for Applying Techniques to Real-World Problems
    Computational Chemistry: A Practical Guide for Applying Techniques to Real-World Problems. David C. Young Copyright ( 2001 John Wiley & Sons, Inc. ISBNs: 0-471-33368-9 (Hardback); 0-471-22065-5 (Electronic) COMPUTATIONAL CHEMISTRY COMPUTATIONAL CHEMISTRY A Practical Guide for Applying Techniques to Real-World Problems David C. Young Cytoclonal Pharmaceutics Inc. A JOHN WILEY & SONS, INC., PUBLICATION New York . Chichester . Weinheim . Brisbane . Singapore . Toronto Designations used by companies to distinguish their products are often claimed as trademarks. In all instances where John Wiley & Sons, Inc., is aware of a claim, the product names appear in initial capital or all capital letters. Readers, however, should contact the appropriate companies for more complete information regarding trademarks and registration. Copyright ( 2001 by John Wiley & Sons, Inc. All rights reserved. No part of this publication may be reproduced, stored in a retrieval system or transmitted in any form or by any means, electronic or mechanical, including uploading, downloading, printing, decompiling, recording or otherwise, except as permitted under Sections 107 or 108 of the 1976 United States Copyright Act, without the prior written permission of the Publisher. Requests to the Publisher for permission should be addressed to the Permissions Department, John Wiley & Sons, Inc., 605 Third Avenue, New York, NY 10158-0012, (212) 850-6011, fax (212) 850-6008, E-Mail: PERMREQ @ WILEY.COM. This publication is designed to provide accurate and authoritative information in regard to the subject matter covered. It is sold with the understanding that the publisher is not engaged in rendering professional services. If professional advice or other expert assistance is required, the services of a competent professional person should be sought.
    [Show full text]
  • Seeding the Multi-Dimensional Nonequilibrium Pulling for Hamiltonian Variation
    Seeding the Multi-dimensional Nonequilibrium Pulling for Hamiltonian Variation: Indirect QM/MM Free Energy Simulations Zhaoxi Sun1* and Qiaole He2 1Beijing National Laboratory for Molecular Sciences, College of Chemistry and Molecular Engineering, Institute of Theoretical and Computational Chemistry, Peking University, Beijing 100871, China 2State Key Laboratory of Bioreactor Engineering, East China University of Science and Technology, 200237 Shanghai, China *To whom correspondence should be addressed: [email protected] Abstract Combination of free energy simulations in the alchemical and configurational spaces provides a feasible route to access the thermodynamic profiles under a computationally demanding target Hamiltonian. Normally, due to the significant differences between the computational cost of ab initio quantum mechanics (QM) calculations and those of semi-empirical quantum mechanics (SQM) and molecular mechanics (MM), this indirect method could be used to obtain the QM thermodynamics by combining the SQM or MM results and the SQM-to-QM or MM-to-QM corrections. In our previous works, a multi-dimensional nonequilibrium pulling framework for Hamiltonian variations has been introduced based on bidirectional pulling and bidirectional reweighting. The method performs nonequilibrium free energy simulations in the configurational space to obtain the thermodynamic profile along the conformational change pathway under a selected computationally efficient Hamiltonian, and uses the nonequilibrium alchemical method to correct or perturb the thermodynamic profile to that under the target Hamiltonian. The BAR-based method is designed to achieve the best generality and transferability and thus leads to modest (~20 folds) speedup. In this work, we explore the possibility of further accelerating the nonequilibrium free energy simulation by employing unidirectional pulling and using the selection criterion to obtain the initial configurations used to initiate nonequilibrium trajectories following the idea of adaptive steered molecular dynamics (ASMD).
    [Show full text]
  • Gaussian 16 Features at a Glance Features Introduced Since Gaussian 09 Rev a Are in Blue
    Gaussian 16 Features at a Glance Features introduced since Gaussian 09 Rev A are in blue. Existing features enhanced in Gaussian 16 are in green. Fundamental Algorithms ◆ empirical dispersion: PFD, GD2, GD3, GD3BJ ◆ Calculation of one- & two-electron integrals over any contracted ◆ functionals including dispersion: APFD, B97D3, B2PLYPD3 gaussian functions ◆ long range-corrected: LC-ωPBE, CAM-B3LYP, ωB97XD and ◆ Conventional, direct, semi-direct and in-core algorithms variations, Hirao’s general LC correction ◆ Linearized computational cost via automated fast multipole ◆ Larger numerical integrations grids methods (FMM) and sparse matrix techniques ◆ Harris initial guess Electron Correlation: ◆ Initial guess generated from fragment guesses or fragment SCF All methods/job types are available for both closed and open shell solutions systems and may use frozen core orbitals; restricted open shell ◆ Density fitting and Coulomb engine for pure DFT calculations, calculations are available for MP2, MP3, MP4 and CCSD/CCSD(T) including automated generation of fitting basis sets energies. ◆ O(N) exact exchange for HF and hybrid DFT ◆ MP2 energies, gradients, and frequencies ◆ 1D, 2D, 3D periodic boundary conditions (PBC) energies & ◆ Double hybrid DFT energies, gradients and frequencies, with gradients (HF & DFT) optional empirical dispersion (see list in “Density Functional ◆ Shared-memory (SMP), cluster/network and GPU-based parallel Theory” above) execution ◆ CASSCF calculations with MP2 correlation for any specified set of states Model Chemistries
    [Show full text]
  • Acronyms Used in Theoretical Chemistry
    Pure & Appl. Chem., Vol. 68, No. 2, pp. 387-456, 1996. Printed in Great Britain. INTERNATIONAL UNION OF PURE AND APPLIED CHEMISTRY PHYSICAL CHEMISTRY DIVISION WORKING PARTY ON THEORETICAL AND COMPUTATIONAL CHEMISTRY ACRONYMS USED IN THEORETICAL CHEMISTRY Prepared for publication by the Working Party consisting of R. D. BROWN* (Australia, Chiman);J. E. BOWS (USA); R. HILDERBRANDT (USA); K. LIM (Australia); I. M. MILLS (UK); E. NIKITIN (Russia); M. H. PALMER (UK). The focal point to which to send comments and suggestions is the coordinator of the project: RONALD D. BROWN Chemistry Department, Monash University, Clayton, Victoria 3 168, Australia. Responses by e-mail would be particularly appreciated, the number being: rdbrown @ vaxc.cc .monash.edu.au another alternative is fax at: +61 3 9905 4597 Acronyms used in theoretical chemistry synogsis An alphabetic list of acronyms used in theoretical chemistry is presented. Some explanatory references have been added to make acronyms better understandable but still more are needed. Critical comments, additional references, etc. are requested. INTRODUC'IION The IUPAC Working Party on Theoretical Chemistry was persuaded, by discussion with colleagues, that the compilation of a list of acronyms used in theoretical chemistry would be a useful contribution. Initial lists of acronyms drawn up by several members of the working party have been augmented by the provision of a substantial list by Chemical Abstract Service (see footnote below). The working party is particularly grateful to CAS for this generous help. It soon became apparent that many of the acron ms needed more than mere spelling out to make them understandable and so we have added expr anatory references to many of them.
    [Show full text]
  • Information to Users
    INFORMATION TO USERS This manuscript has been reproduced from the microfilm master. UMI films the text directly from the original or copy submitted. Thus, some thesis and dissertation copies are in typewriter face, while others may be from any type of computer printer. The quality of this reproduction is dependent upon the quality of the copy submitted. Broken or indistinct print, colored or poor quality illustrations and photographs, print bleedthrough, substandard margins, and improper alignment can adversely affect reproduction. In the unlikely event that the author did not send UMI a complete manuscript and there are missing pages, these will be noted. Also, if unauthorized copyright material had to be removed, a note will indicate the deletion. Oversize materials (e.g., maps, drawings, charts) are reproduced by sectioning the original, beginning at the upper left-hand comer and continuing from left to right in equal sections with small overlaps. Each original is also photographed in one exposure and is included in reduced form at the back of the book. Photographs included in the original manuscript have been reproduced xerographically in this copy. Higher quality 6 " x 9" black and white photographic prints are available for any photographs or illustrations appearing in this copy for an additional charge. Contact UMI directly to order. University Microfilms international A Bell & Howell Information Company 300 North Zeeb Road. Ann Arbor. Ml 48106-1346 USA 313/761-4700 800/521-0600 Order Number 9211140 P a rt 1 . Design, synthesis, and structure-activity studies of molecules with activity at non-NMDA glutamate receptors: Hydroxyphenylalanines, quinoxalinediones and related molecules.
    [Show full text]
  • WHAT INFLUENCE WOULD a CLOUD BASED SEMANTIC LABORATORY NOTEBOOK HAVE on the DIGITISATION and MANAGEMENT of SCIENTIFIC RESEARCH? by Samantha Kanza
    UNIVERSITY OF SOUTHAMPTON Faculty of Physical Sciences and Engineering School of Electronics and Computer Science What Influence would a Cloud Based Semantic Laboratory Notebook have on the Digitisation and Management of Scientific Research? by Samantha Kanza Thesis for the degree of Doctor of Philosophy 25th April 2018 UNIVERSITY OF SOUTHAMPTON ABSTRACT FACULTY OF PHYSICAL SCIENCES AND ENGINEERING SCHOOL OF ELECTRONICS AND COMPUTER SCIENCE Doctor of Philosophy WHAT INFLUENCE WOULD A CLOUD BASED SEMANTIC LABORATORY NOTEBOOK HAVE ON THE DIGITISATION AND MANAGEMENT OF SCIENTIFIC RESEARCH? by Samantha Kanza Electronic laboratory notebooks (ELNs) have been studied by the chemistry research community over the last two decades as a step towards a paper-free laboratory; sim- ilar work has also taken place in other laboratory science domains. However, despite the many available ELN platforms, their uptake in both the academic and commercial worlds remains limited. This thesis describes an investigation into the current ELN landscape, and its relationship with the requirements of laboratory scientists. Market and literature research was conducted around available ELN offerings to characterise their commonly incorporated features. Previous studies of laboratory scientists examined note-taking and record-keeping behaviours in laboratory environments; to complement and extend this, a series of user studies were conducted as part of this thesis, drawing upon the techniques of user-centred design, ethnography, and collaboration with domain experts. These user studies, combined with the characterisation of existing ELN features, in- formed the requirements and design of a proposed ELN environment which aims to bridge the gap between scientists' current practice using paper lab notebooks, and the necessity of publishing their results electronically, at any stage of the experiment life cycle.
    [Show full text]
  • S.A. Raja Pharmacy College Vadakkangulam-627 116
    S.A. RAJA PHARMACY COLLEGE VADAKKANGULAM-627 116 MEDICINAL CHEMISTRY -III VI SEMESTER B. PHARM PRACTICAL MANUAL CONTENT S.No Experiment Name Page No. 1. Synthesis of Sulphanilamide 01 2. Synthesis of 7- Hydroxy -4- methyl coumarin 03 3. Synthesis of Chlorbutanol 05 4. Synthesis of Tolbutamide 07 5. Synthesis of Hexamine 09 6. Assay of Isonicotinic acid hydrazide 11 7. Assay of Metronidazole 13 8. Assay of Dapsone 16 9. Assay of Chlorpheniramine Maleate 18 10. Assay of Benzyl Penicillin 20 11. Synthesis of Phenytoin from Benzil by Microwave 23 Irradiation 12. Synthesis of Aspirin Assisted by Microwave Oven 26 13. Drawing structure and Reaction using Chemsketch 28 MEDICINAL CHEMISTRY- III Experiment No: 01 Synthesis of Sulphanilamide Aim: To synthesis and submit sulphanilamide from p-acetamido benzene sulphanilamide and calculate its percentage yield. Principle: Sulphanilamide can be prepared by the reaction of P-acetamido benzene sulphanilamide with Hydrochloric acid or ammonium carbonate. The acetamido groups are easily undergo acid catalysed hydrolysis reaction to form p-amino benzene sulphonamide. Reaction: O HN H2N HCl O S O O S O NH NH2 2 4 Acetamidobenzene sulphonamide p Amino benzene sulphonamide Chemical Required: Resorcinol - 1.2 g Ethyl acetoacetate - 2.4 ml Conc. Sulphuric acid - 7.5 ml Procedure: 1.5 gm of 4- acetamido benzene sulphonamide is treated with a mixture of 1 ml of conc. Sulphuric acid diluted with 2 ml water. This mixture is gently heated under reflux for 1 hour. Then 3ml of water is added and the solution is boiled again, with the addition of a small quantity of activated charcoal.
    [Show full text]
  • Isurvey - Online Questionnaire Generation from the University of Southampton
    1/17/2018 iSurvey - Online Questionnaire Generation from the University of Southampton Investigating the use of software for Chemists Survey Study Information Study title: Investigating the use of software for Chemists Survey Researcher name: Samantha Kanza Study reference: iSurvey 16857 Ethics reference: Ergo 17642 – Chemistry Tools Survey Participant Information Please read this information carefully before deciding to take part in this research. If you are happy to participate you will be asked to check the consent form box. What is the research about? This research is for my PhD in Computer Science and Chemistry. I am coming to the end of the first year of my PhD and I am looking to investigate the use of chemistry tools to better understand what type of tools chemists actually use. This is a very simple survey that asks what type of chemist you are, and what types of tools you use, and if applicable which specific tools of that type you use. This PhD is part of the Web Science CDT and is funded by EPSRC. Why have I been chosen? You have been chosen because you work in chemistry. What will happen to me if I take part? This is a short survey that is being conducted to get a better idea of the usage of chemistry tools. Are there any benefits in my taking part? This survey will form part of a body of research aimed to improve the understanding of how chemists use technology to assist their work. Are there any risks involved? There are no risks involved. Will my participation be confidential? Your participation will be confidential.
    [Show full text]
  • TDDFT As a Tool in Chemistry II
    TDDFT as a tool in chemistry Summer School on “Time dependent Density-Functional Theory: Prospects and Applications” Benasque, Spain September 2008 Ivano Tavernelli EPFL CH-1015 Lausanne, Switzerland Program (lectures 1 and 2) Definitions (chemistry, photochemistry and photophysics) The Born-Oppenheimer approximation potential energy surfaces (PES) Methods for excited states in quantum chemistry Lecture 1 - HF, TDHF - Configuration interaction, CI - Coupled Cluster, CC - MCSCF TDDFT: Why TDDFT in chemistry and biology? TDDFT: properties and applications in chemistry TDDFT failures Lecture 2 - Accuracy and functionals - charge transfer excitations - topology of the PES Lecture 3: Introduction to Non-adiabatic mixed-quantum classical molecular dynamics Why TDDFT in chemistry? All MR ab-initio methods are still computationally too expensive for large systems (they are limited to few tenths of atoms) and for mixed-quantum classical dynamics. Among the SR (plus perturbation) methods: CIS is practically no longer used in the calculation of excitation energies in molecules. The error in the correlation energy is usually very large and give qualitatively wrong results. STILL good to gain insight on CT state energies! Largely replaced by TDDFT CC2 Is a quite recent development and therefore not widely available Accurate and fast, is the best alternative to TDDFT Good energies also for CT states Among the MR methods, CASSCF is still widely used but is computationally very expensive and the quality of the excited state energies and properties are not necessarily better than the ones obtained from a TDDFT calculation. In addition, all SCF based methods need what is called “chemical intuition” in the construction of the active space.
    [Show full text]