Chemistry 4560/5560 Molecular Modeling Fall 2014

Similar documents
MO Calculation for a Diatomic Molecule. /4 0 ) i=1 j>i (1/r ij )

An Introduction to Quantum Chemistry and Potential Energy Surfaces. Benjamin G. Levine

This is a very succinct primer intended as supplementary material for an undergraduate course in physical chemistry.

Introduction to computational chemistry Exercise I: Structure and electronic energy of a small molecule. Vesa Hänninen

AN INTRODUCTION TO QUANTUM CHEMISTRY. Mark S. Gordon Iowa State University

Lec20 Fri 3mar17

Handbook of Computational Quantum Chemistry. DAVID B. COOK The Department of Chemistry, University of Sheffield

Chemistry 334 Part 2: Computational Quantum Chemistry

DFT calculations of NMR indirect spin spin coupling constants

Molecular Simulation I

Electron Correlation

Exercise 1: Structure and dipole moment of a small molecule

Beyond the Hartree-Fock Approximation: Configuration Interaction

Introduction to Computational Quantum Chemistry: Theory

Computational Methods. Chem 561

4 Post-Hartree Fock Methods: MPn and Configuration Interaction

Performance of Hartree-Fock and Correlated Methods

Session 1. Introduction to Computational Chemistry. Computational (chemistry education) and/or (Computational chemistry) education

Handbook of Computational Quantum Chemistry

Quantum Chemical Simulations and Descriptors. Dr. Antonio Chana, Dr. Mosè Casalegno

Density Functional Theory

Advanced Electronic Structure Theory Density functional theory. Dr Fred Manby

Lecture 4: methods and terminology, part II

Computational chemistry with GAMESS: a very brief overview with examples

Electron Correlation - Methods beyond Hartree-Fock

Introduction to Computational Chemistry: Theory

2~:J~ -ryej- r- 2 Jr. A - f3. sr(djk nv~tor rn~ +~ rvjs (::-CJ) ::;-1-.'--~ -. rhd. ('-.Ji.L.~ )- r'-d)c, -r/~ JJr - 2~d ~2-Jr fn'6.

计算物理作业二. Excercise 1: Illustration of the convergence of the dissociation energy for H 2 toward HF limit.

Jack Simons, Henry Eyring Scientist and Professor Chemistry Department University of Utah

Electronic structure calculations: fundamentals George C. Schatz Northwestern University

OVERVIEW OF QUANTUM CHEMISTRY METHODS

Ab initio calculations for potential energy surfaces. D. Talbi GRAAL- Montpellier

Electron Correlation Methods

Introduction to Computational Chemistry

Multi-reference Density Functional Theory. COLUMBUS Workshop Argonne National Laboratory 15 August 2005

The successful wavefunction can be written as a determinant: # 1 (2) # 2 (2) Electrons. This can be generalized to our 2N-electron wavefunction:

CHEM6085: Density Functional Theory Lecture 10

Introduction to Computational Chemistry for Experimental Chemists... (Part 2/2)

QUANTUM CHEMISTRY PROJECT 3: ATOMIC AND MOLECULAR STRUCTURE

This is called a singlet or spin singlet, because the so called multiplicity, or number of possible orientations of the total spin, which is

Computational Chemistry I

G1-3 These methods are based on ab initio molecular orbital calculations. Electron correlation is calculated using MP2 or MP4 and QCI.

Gaussian: Basic Tutorial

Semi-Empirical MO Methods

Lecture 5: More about one- Final words about the Hartree-Fock theory. First step above it by the Møller-Plesset perturbation theory.

NMR and IR spectra & vibrational analysis

Lec20 Wed 1mar17 update 3mar 10am

Vol. 9 COMPUTATIONAL CHEMISTRY 319

LUMO + 1 LUMO. Tómas Arnar Guðmundsson Report 2 Reikniefnafræði G

EXAM INFORMATION. Radial Distribution Function: B is the normalization constant. d dx. p 2 Operator: Heisenberg Uncertainty Principle:

Joint ICTP-IAEA Workshop on Fusion Plasma Modelling using Atomic and Molecular Data January 2012

Introduction to Electronic Structure Theory

Practical Advice for Quantum Chemistry Computations. C. David Sherrill School of Chemistry and Biochemistry Georgia Institute of Technology

Computational Material Science Part II. Ito Chao ( ) Institute of Chemistry Academia Sinica

Coulson's. Valence. ROY McWEENY THIRD EDITION OXFORD UNIVERSITY PRESS

Basic introduction of NWChem software

Quantum Chemical and Dynamical Tools for Solving Photochemical Problems

Electric properties of molecules

Advanced in silico drug design

Jack Simons, Henry Eyring Scientist and Professor Chemistry Department University of Utah

COUPLED-CLUSTER CALCULATIONS OF GROUND AND EXCITED STATES OF NUCLEI

( R)Ψ el ( r;r) = E el ( R)Ψ el ( r;r)

Chemistry 4681 Module: Electronic Structure of Small Molecules Background Handout

Chemistry 433 Computational Chemistry Fall Semester 2002 Dr. Rainer Glaser

Oslo node. Highly accurate calculations benchmarking and extrapolations

Hints on Using the Orca Program

Using Web-Based Computations in Organic Chemistry

Basis Set for Molecular Orbital Theory

Computational Chemistry. An Introduction to Molecular Dynamic Simulations

Additional background material on the Nobel Prize in Chemistry 1998

On the Uniqueness of Molecular Orbitals and limitations of the MO-model.

Hartree, Hartree-Fock and post-hf methods

Jack Smith. Center for Environmental, Geotechnical and Applied Science. Marshall University

The Potential Energy Surface

COPYRIGHTED MATERIAL. Quantum Mechanics for Organic Chemistry &CHAPTER 1

Methods for Treating Electron Correlation CHEM 430

FYS-6306 QUANTUM THEORY OF MOLECULES AND NANOSTRUCTURES

Conformational energy analysis

Exchange Correlation Functional Investigation of RT-TDDFT on a Sodium Chloride. Dimer. Philip Straughn

Walter Kohn was awarded with the Nobel Prize in Chemistry in 1998 for his development of the density functional theory.

Quantum Chemistry Methods

Introduction to DFTB. Marcus Elstner. July 28, 2006

Molecular Modelling for Medicinal Chemistry (F13MMM) Room A36

Transition states and reaction paths

Chemistry 881 Lecture Topics Fall 2001

QUANTUM CHEMISTRY FOR TRANSITION METALS

The Basics of Theoretical and Computational Chemistry

Quantum chemical modelling of molecular properties - parameters of EPR spectra

IFM Chemistry Computational Chemistry 2010, 7.5 hp LAB2. Computer laboratory exercise 1 (LAB2): Quantum chemical calculations

Jack Simons, Henry Eyring Scientist and Professor Chemistry Department University of Utah

ABC of DFT: Hands-on session 1 Introduction into calculations on molecules

Coupled-Cluster Perturbative Triples for Bond Breaking

Fragmentation methods

Simulation Methods II

Chem 4502 Introduction to Quantum Mechanics and Spectroscopy 3 Credits Fall Semester 2014 Laura Gagliardi. Lecture 28, December 08, 2014

Computational Modeling Software and their applications

Advanced Electronic Structure Theory Density functional theory. Dr Fred Manby

Excited States Calculations for Protonated PAHs

AB INITIO METHODS IN COMPUTATIONAL QUANTUM CHEMISTRY

Q-Chem 5: Facilitating Worldwide Scientific Breakthroughs

Transcription:

Final Exam Name:. User s guide: 1. Read questions carefully and make sure you understand them before answering (if not, ask). 2. Answer only the question that is asked, not a different question. 3. Unless directed otherwise (e.g. offered a short answer such as Yes/No) answer in a complete, grammatically meaningful English sentences. 4. Formulate your answers clearly and precisely. 5. Write legibly. Example: Q: What is Huckel theory? A: Huckel theory is an empirical molecular orbital method designed for electronic structure calculations for conjugated hydrocarbons. 1. Potential Energy Surface (PES). a. Potential energy surface (PES) is one of the central concepts in molecular modeling. Define PES: b. Can PES be experimentally measured? (Yes/No) c. What are the so called stationary points on the PES surface? 1

d. Give specific examples of stationary points and briefly explain why they are important: e. For a model molecule (e.g. in Gaussian), conceptually describe how a stationary point on the PES is found: 2

f. Stationary points can be characterized by calculation of vibrational frequencies. For the examples of the stationary points on the PES you gave above, explain how. g. Does it make sense to calculate (harmonic) vibrational frequencies at other than stationary points of the PES? Explain you answer. 3

2. In the following, you will describe in general terms (no specific keywords etc. needed) the sequence of steps and types of calculations that you need to obtain a desired molecular property. For example: Q: NMR chemical shift of molecule X with respect to TMS A: 1. Optimization of X 2. Calculation of NMR shieldings for X 3. Optimization of TMS 4. Calculation of NMR shieldings for TMS 5. Subtraction of TMS shieldings from those of the molecule X yields the desired chemical shifts. For following reaction CH3Cl + OH CH3OH + Cl a. The reaction enthalpy at 450K and 10 atm pressure. 4

b. The equilibrium constant at the same T and p: 5

c. The forward rate of the reaction at the same T and p 6

d. The isotopic effect of deuteration of CH3Cl (i.e. CH3Cl becomes CD3Cl where D stands for deuterium) on the rate of the reaction. Isotopic effects means how the reaction rate changes upon the isotopic substitution. 7

3. When using various computational levels, it is important to pay attention to their availability. This is an excerpt from the Gaussian manual: AVAILABILITY Analytic energies and gradients for CCD and CCSD, numerical gradients for CCSD(T), and numerical frequencies for all methods. The restricted open-shell (RO) method is available for CCSD and CCSD(T) energy calculations. Explain the meaning and practical implications of the availability of a. Analytic gradients: b. Analytic frequencies: 8

c. Numerical gradients: d. Numerical frequencies: 9

5. The Hartree-Fock (HF) theory forms the basis of the entire computational chemistry (as well as computational physics). Yet, as you know, HF theory provides neither correct, nor even very accurate solution to the molecular electronic structure problem (= molecular Schrodinger equation). a. Why, then, is HF theory so important? b. Despite its central importance, however HF level is rarely used in computational chemistry. What is the major drawback of HF that demands use of different (higher-level) methods? 10

c. Even though HF equations significantly simplify the multi-electron problem, they still cannot be solved in the closed form. Rather, they require a procedure known as the Self-Consistent Field (SCF). Describe how this procedure works: 11

d. There are several incarnations of HF methodology in practical use. In particular, we distinguish between the so-called ab initio HF and semi-empirical HF methods. Describe the difference between them. 12

f. Furthermore, HF can be restricted (RHF) or unrestricted (UHF). For what kinds of problems are RHF calculations appropriate, and for what problems UHF ones are used? Explain briefly and illustrate the RHF and UHF electron configuration with a sketch. 13

6. Basis sets a. Molecular orbitals (MO) are generally described as a linear combination of atomic orbitals (MO-LCAO). The AO s are in turn expressed in terms of (atomic) basis functions. The Slater-type orbital (STO) is considered to correct form of the atomic basis function. Why? b. What is the difference, if any, between the Slater-type orbital (STO) and Slater determinant? 14

c. STOs are virtually never used in actual basis sets. What types of functions are used instead and why? d. This is a piece of the Gaussian calculation output: There are 297 symmetry adapted basis functions of A symmetry. Integral buffers will be 131072 words long. Raffenetti 2 integral format. Two-electron integral symmetry is turned on. 297 basis functions, 516 primitive gaussians, 322 cartesian basis functions 86 alpha electrons 86 beta electrons What is the difference between: i) a basis function (297 of them) and a primitive Gaussian (516 of them)? 15

ii) a basis function (297 of them) and a Cartesian basis function (322 of them)? e. Explain what effective core potential (ECP) is and for what types of calculations it is advantageous (or necessary) to use ECPs: 16

7. Post HF methods: configuration interaction (CI), Moller-Plesset perturbation theory (MPn) and coupled cluster (CC) theory. a. What is the objective of the configuration interaction (CI) methods? b. Describe briefly how the CI method works: 17

c. Why is CID (configuration interaction doubles) the lowest possible level of CI? d. Truncated CI (such as CID) is seldom used in practice. What is the main reason? e. On the other hand, coupled clusters (CC) are a very popular and useful (though quite demanding) computational method. How does CC solve the main deficiency of the CI methods? 18

f. Moller-Plesset methods, such as MP2, are also very frequently used in practical calculations. What is the main limitation of MP methods? g. What is meant by non-dynamical electron correlation (as opposed to dynamical electron correlation) and what types of methods are designed to specifically deal with it? 19

8. Density functional theory (DFT). a. Density functional methods account for the vast majority of quantum-chemical calculations done today and over the last two or so decades. Why are DFT methods so popular? b. As you answered above somewhere, HF equations are solved by a SCF procedure. The DFT is formulated in a similar manner the so-called Kohn-Sham (KS) equations. Are the KS equations also solved by the SCF procedure? (Yes/No) c. What is the difference between HF orbitals and Kohn-Sham (KS) orbitals? 20

d. Further contrasting DFT with HF methods (in general, conceptual terms regarding the overall theory, rather than e.g. specific practical results) what are two main disadvantgates of the DFT? e. List five basic classes of DFT functionals: 21

9. Molecular mechanics. a. Molecular mechanics (MM) methods are based on an empirical energy function, called a MM force field (FF). Unlike for quantum calculations, it is necessary to specify not only an atom type (i.e., H, C, etc.) but also how and to what other atoms it is bonded for the MM FF to work. Briefly describe why that is: b. To be useful, a MM FF must be transferable. What is meant by FF transferability and why is it important? 22

c. In general, is it possible to study chemical reactions where covalent bonds are broken and formed by MM? Explain. d. Molecular dynamics (MD) simulations are the most frequently used approach for calculation of equilibrium macroscopic properties of condensed phases, solutions of macromolecules etc. Why is MD simulation, i.e. a run over a period of time necessary for obtaining such properties, rather than e.g. a single calculation? 23

10. Population analyses, implicit solvent, excited states etc. a. Are atomic partial charges uniquely defined? (Yes/No) c. Explain the concept of the reaction field (RF) and how a self-consistent reaction field (SCRF) calculation works: b. The main contributions to the solvation (free) energy are: electrostatics, cavitation and dispersion. Which ones do polarized continuum solvent models (PCM) generally account for and which ones do they neglect? 24

d. Give two main reasons why it is generally incorrect to write an excited state wavefunction as a single (Slater) determinant: e. Why is CIS a method for excited state calculation, while CID for a ground state one? f. Is time-dependent DFT (TD-DFT) used for calculations of any time-dependent properties? Explain. 25