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EXPERIMENT 9 預預預預預預預預預預預預預 預預 49812012 預預預 49812051 預預預 49812049 預預預

EXPERIMENT 9

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EXPERIMENT 9. 預測化學反應途徑與反應速率. 化三 49812012 李雨修 49812051 李國禎 49812049 廖偉智. Purpose. Learn the logical of solving Schrödinger equation : Born–Oppenheimer approximation Hartree-Fock method Predict the optimized structure of transition state and calculate the rate constant: - PowerPoint PPT Presentation

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Page 1: EXPERIMENT  9

EXPERIMENT 9預測化學反應途徑與反應速率

化三 49812012 李雨修 49812051 李國禎 49812049 廖偉智

Page 2: EXPERIMENT  9

Purpose• Learn the logical of solving Schrödinger equation :• Born–Oppenheimer approximation• Hartree-Fock method

• Predict the optimized structure of transition state and calculate the rate constant:

• Transition State Theory• Eyring Equation

• Use computer program to investigate some chemical phenomena:• Gaussian 03, Gauss view, ChemDraw

Page 3: EXPERIMENT  9

Schrödinger Equation

Eigenvalue

Eigenfunction

Eigenvector

Page 4: EXPERIMENT  9

The Born-Oppenheimer Approximation• Molecular Hamiltonian (time independent form)

• Electronic Hamiltonian

Kinetic energyof nuclei

Repulsion of nuclei Kinetic energyof electrons

Attractionbetweennuclei andelectrons

Repulsion ofelectrons

Page 5: EXPERIMENT  9

The Born-Oppenheimer Approximation

Nucleus

Electron

too heavy to move

moves aroundvery fast

Nucleus and electron have the same momentum(p=mv). While nucleus is massive(Ma>>Me), relate to electron, it just like nucleus at rest.

Page 6: EXPERIMENT  9

The Born-Oppenheimer Approximation

By the Born-Oppenheimer approximation,

thus, the Schrödinger Equation can be extended as

Assume we had solved the electronic wavefunction:

Nuclei wavefunction and electrons wavefunction are independent from each other.

Page 7: EXPERIMENT  9

The Born-Oppenheimer Approximation

to find out nuclear Hamiltonian, we know

11

Nuclear Hamiltonian

KineticEnergy

PotentialEnergy Surface

Page 8: EXPERIMENT  9

The Born-Oppenheimer Approximation

Page 9: EXPERIMENT  9

The Born-Oppenheimer Approximation• Limitation

The error comes form the following condition :

1.) The movement of nuclei is too violent.

So nuclei can’t be viewed as “stationary”.

2.) 1st exciting electronic energy level is too low.

Any condition of a little change of nuclear coordinate leading severe alternation of electronic wavefunction makes intolerant errors.

Page 10: EXPERIMENT  9

Computational Chemistry• Scheme for solving many-electron system

A molecule

HF

Page 11: EXPERIMENT  9

Computational Chemistry ab initio

Semi-Empirical Molecular Mechanics Density Functional Theory (DFT)

A method simulate molecule behaviors only by some basic physical constants and principles instead of by any simplicity coming from experimental experiences.

Page 12: EXPERIMENT  9

Hartree–fock Method (HF)

electronindices

spin orbitalindices

Page 13: EXPERIMENT  9

Hartree–fock Method (HF)• It contains all possible permutations, all of them are

“indistinguishable” because it’s impossible to distinguish two electron with the difference.

• Interchanging of two rows flips the sign.asymmetry : electron is fermion (Pauli principle)

• If with two identical columns, the determination is always zero.all electrons with different quantum states (Pauli exclusion principle)

Page 14: EXPERIMENT  9

Hartree–fock Method (HF)• Purely many-electron Hamiltonian

• HF Mean-field Hamiltonian

Kinetic energy Electron-electronRepulsion

ColumbicAttraction

Page 15: EXPERIMENT  9

Hartree–fock Method (HF)

(Linear combination of primitive functrion)

Page 16: EXPERIMENT  9

Hartree–fock Method (HF)Split-valence Basis Sets – The Pople Basis Sets • General expression

• Some common types

X – YZ + G*

3-21G 3-21G*3-21+G 3-21+G* 6-21G 6-31G6-31G* 6-31+G*etc.

# basic sets forinert shell orbitals

# basic sets forvalance shell orbitals

with diffuse functions

with polarization functions

John A. Pople (1925-2004)Nobel Prize in Chemistry

(1998)

Gaussian-type

Page 17: EXPERIMENT  9

Hartree–fock Method (HF)Self-consistent Field (SCF)

• Self-consistent Field (SCF)

Directly solve the electronic wavefunction is very difficult because, for one electron, the distribution of other electrons we do not know, but it’s necessary to be known if we want to figure out the electronic wavefunction.

What preferable way is guess an initial condition and then using a mathematical method (i.e. Iterative Method) to approach the exact solution gradually.

Page 18: EXPERIMENT  9

Hartree–fock Method (HF)Self-consistent Field (SCF)

• Solution process

Choose a basic sets

Work many times.

There seems that we almost could find no more lower energy for the system.

Page 19: EXPERIMENT  9

Hartree–fock Method (HF)• Brief conclusions

1.) If the electronic wavefunction can be expressed as a single Slater determinant, we can decompose the many-electron Hamiltonian as the sum of all single-electron Hamiltonian.

i.e. the electron is independent of others, and the correlation and exchanging energy of electrons is neglected.

2.) The electron motion is regarded as on electron under a mean electric field composed by others.

but we do not know any information about the distribution of electrons.

all we can do is guess the value and optimize it.

Page 20: EXPERIMENT  9

Eyring Equation

Henry Eyring (1901-1981)

Page 21: EXPERIMENT  9

Eyring Equation• Transition State Theory

Reaction Coordinate

Page 22: EXPERIMENT  9

Eyring Equation• Derive Eyring eq.

For a reaction

Assume its mechanism: Pre-equilibrium + Transition state

Page 23: EXPERIMENT  9

Eyring Equation

By definition, In gaseous phase, the equilibrium const. for this reaction can be written as:

concentration

Page 24: EXPERIMENT  9

Eyring Equation

Recall, rate const. of the reaction:

Page 25: EXPERIMENT  9

Eyring Equation

Page 26: EXPERIMENT  9

Eyring Equation

Page 27: EXPERIMENT  9

Eyring Equation

Page 28: EXPERIMENT  9

Eyring Equation

Page 29: EXPERIMENT  9

Eyring EquationUntil now, we had deduced:

Recall,

#Eyring eq.

Page 30: EXPERIMENT  9

Procedure

開啟軟體 Gauss View建構 Gaussian03 之imput ↓ 以水分子為例

點選 Element Fragment

分別點選 O 和 H 並在作圖處點擊

點選 modify bond 和 modify angle

Lable 欲調整的原子

選擇 single bond→”OK”

Lable 三個調整其鍵角

點選“ clean” 可調整分子至較佳形狀儲存成 .gjf 檔

Page 31: EXPERIMENT  9

使用軟體 Gaussian03 並開啟GaussView 儲存的 imput 檔更改指令為 HF/6-31G opt freq

開始

計算完成

Page 32: EXPERIMENT  9
Page 33: EXPERIMENT  9

i2 C CH

H

B

H

H

i4

C C

HH

H B

tsi2i4

H i5

C C BHH

H H

tsi4i5

i8

tsi4i8

C C B

H

H H

H

0.0

kcal/mol

Page 34: EXPERIMENT  9

References• Atkins' Physical Chemistry 9/E, Ch24-4• Levine I.N. Quantum Chemistry 4/E, Ch10-Ch13• http://www.iams.sinica.edu.tw/lab/wbtzeng/labtech/

term_calchem.htm, 20120304• http://www.iams.sinica.edu.tw/lab/wbtzeng/labtech/

basis_set.htm, 20120304• http://en.wikipedia.org/wiki/Born

%E2%80%93Oppenheimer_approximation, 20120303• http://www.nobelprize.org/nobel_prizes/chemistry/laureates/

1998/index.html, 20120305• http://www.shodor.org/chemviz/basis/teachers/

background.html, 20120304• http://www.youtube.com/watch?v=EROZXzS51Co, 20120301• http://en.wikipedia.org/wiki/Hartree

%E2%80%93Fock_method, 20120306

Page 35: EXPERIMENT  9

THE ENDThank you for your attention.