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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