lecture 8. chemical bonding
DESCRIPTION
Separation of variables in the case of atom (Review) An atom has translational and electronic degrees of freedom. To good approximation, degrees of freedom are not coupled. Separation of variables! N N N N + Helec(elec) Eigenvalue (energy) = sum Htrans(rCM) N Enuc,elec Eigenfunction (wave function) = product relec (rCM as origin) N elec(elec) rCM relec (rCM as origin) rCM (~rN)TRANSCRIPT
Lecture 8. Chemical Bonding
Lecture 8. Chemical Bonding.Molecular Orbital Energy Diagram
ofOne-Electron Molecule, H2+ References Engel Ch.12, Ratner &
Schatz, Ch.10, Appendix A.3 Quantum Chemistry, McQuarrie, Ch.9
Molecular Quantum Mechanics, Atkins & Friedman (4th ed. 2005),
Ch.8 Computational Chemistry, Lewars (2003), Ch.4 A Brief Review of
Elementary Quantum Chemistry Separation of variables in the case of
atom (Review)
An atom has translational and electronic degrees of freedom. To
good approximation, degrees of freedom are not coupled. Separation
of variables! N N N N + Helec(elec) Eigenvalue (energy) = sum
Htrans(rCM) N Enuc,elec Eigenfunction (wave function) = product
relec (rCM as origin) N elec(elec) rCM relec (rCM as origin) rCM
(~rN) Previously in Elements of QM (MS5118) (Review)
A molecule has translational, vibrational, rotational (and
electronic) degrees of freedom. To good approximation, degrees of
freedom are not coupled. separation of variables (What about
electronic?) N N N N + Helec(elec)? Eigenvalue (energy)= sum N N N
N +Enuc,elec ? Eigenfunction (wave function) =product N N N N
elec(elec) ? H2+, the simplest (one-electron) molecule
varied varied vibrating varied For molecules, Born-Oppenheimer
approximation (1927)
Simplifies the Schrdinger equation for molecules (allows separation
of variables) Difference in the time scales of nuclear and
electronic motions Nuclei are much heavier (~1800 times) and slower
than electrons. Electrons can be treated as moving in the field of
fixed nuclei. A full Schrdinger equation for a molecule can be
solved in two steps: 1) Motion of electron around the nuclei at
fixed positions 2) Energy curve of the molecule as a function of
nuclei position Allows to focus on the electronic Schrdinger
equation H2+, the simplest (one-electron) molecule
Born-Oppenheimer approximation fixed Constant Constant
Born-Oppenheimer approximation & Potential energy surface
(curve)
E = E(R) A B R Potential energy surface LCAO-MO: Molecular Orbitals
(MO) by
Linear Combination of Atomic Orbitals (LCAO) R ~ ra rb ~ Near the
equilibrium distance, an electron is delocalized over the whole
molecule. (basis functions for) AO AO LCAO (in atomic units)
(homonuclear) MO linear expansion coefficients (in general,
unknowns determined variationally) LCAO-MO approach & Matrix
representation
? ? ? ? LCAO-MO approach & Matrix representation
Hamiltonian matrix element overlap integral where Secular equation,
Eigenvalues & Eigenfunctions
where 22 Secular equation two eigenvalues ? + ? + two eigen-
functions + ? Secular equation, Eigenvalues &
Eigenfunctions
where 22 Secular equation two eigenvalues + ? + two eigen-
functions + ? Secular equation, Eigenvalues &
Eigenfunctions
where 22 Secular equation two eigenvalues + ? + two eigen-
functions + ? Secular equation, Eigenvalues &
Eigenfunctions
where 22 Secular equation two eigenvalues + + two eigen- functions
+ Eigenfunctions, that is, Molecular Orbitals (MO)
Molecular orbitals (MO) of homonuclear diatomic molecules (such as
H2) have g or u symmetry with respect to the inversion operation.
Molecular orbitals & Probability densities Bonding &
Antibonding MOs: Probability density differences
Buildup of electron charge around protons & between protons
Decrease of charge outside of bonding region Decrease of electron
charge around protons & between protons Increase of charge
outside of bonding region 1 c u = ? Overlap integral Hamiltonian
matrix element where
0 |Sab| 1 Hamiltonian matrix element where Energy eigenvalues &
Integrals
two eigenvalues 0 |Sab| 1 Overlap integral We need to evaluate the
overlap integral Sab and the Hamiltonian matrix elements Haa &
Hab between two AOs located at an internuclear distance R.
Born-Oppenheimer approximation fixed Evaluate Haa = Hbb & Hab =
Hba
Coulomb integral in atomic units Exchange or resonance integral in
atomic units Electron energy eigenvalue & Potential energy
curve
Constant E = ?, V = ? Potential energy minimum bound Internuclear
distance R Equilibrium distance, Re MO energy diagram: E(R) as a
function of R
and Hab = Haa and MO energy diagram: E(R) as a function of R
unbound state: antibonding bound state: bonding Molecular energy
diagram for H2+
unbound state: antibonding 1* Haa 1 bound state: bonding