Chemistry Reference
In-Depth Information
catalysis. Compilations of density functional theory (DFT) applications to catalysis
may be found in the books by van Santen and Neurock [ 40 ] and van Santen
et al. (eds.) [ 41 ].
2 Computational Approaches
Some of the most widely used computational approaches will be briefly described
below, namely some quantum chemical methods, classical simulations by Monte
Carlo and Molecular Dynamics techniques and a few mesoscale methods.
2.1 Quantum Chemistry
In this section a recapitulatory description of the most common ab initio and density
functional approaches will be presented. Ab initio methods calculate the electron
properties of atoms and molecules at the absolute temperature ( T
¼
0). The starting
point is in most cases the non-relativistic Schr
odinger equation
H
c ¼
E
c;
(1)
where H is the Hamiltonian operator which is given by
X
X
X
X
X
X
h 2
2 m e r
h 2
2 m k r
e 2 Z k
r ik þ
e 2
r ij þ
e 2 Z k Z l
r kl
i
k
H
¼
;
(2)
i
k
i
k
i
<
j
k
<
l
where i and j run over electrons, k and l run over nuclei,
h is Planck's constant
divided by 2 p , m e is the mass of the electron, m k is the mass of the nucleus k , r
2 is
the Laplacian operator, e is the charge on the electron, Z is an atomic number and
r ab is the distance between particles (electrons or nuclei) a and b . The wave function
c
is thus a function of 3 n coordinates where n is the total number of particles
(electrons and nuclei).
The Born-Oppenheimer approximation leads to the electronic Schr
odinger
equation
H el c el ¼
E el c el :
(3)
PES can only be computed by employing the Born-Oppenheimer approxima-
tion. The variational principle leads to an upper bound of the electronic energy
Ð c el H
c el d r
Ð c
el d r
E 0 :
(4)
2
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