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f
(
r
) = [δμ/δv(
r
)]
N
(16)
Assuming that the total energy
E
as a function of
N
and functional of
v
(
r
)
is an exact differential, the Maxwell relations between derivatives may
be applied to write the Fukui function or the frontier function as
f
(
r
) =
[∂ρ(
r
)]/∂
N
]
v
.
A very important condition can be found for the Fukui function is that
it must be normalized to 1.
∫
f
(
r
)d
r
= 1
(17)
Owing to the discontinuity of the chemical potential at integer
N
, the de-
rivative of μ= (d
E
/d
N
) will be different if taken from the right or the left-
hand side. One has μ
when the derivative is taken from above (
N
+ δ,
δ→0), μ
when the derivative is taken from below (
N
− δ, δ→0), and for the
cases where is not a net charge exchange a good approximation is to use
the average μ
= ½(μ + μ). Therefore, one has three different functions
f
(
r
)
= [∂ρ(
r
)/∂
N
], where the subscript α
= ± indicate whether the derivative is
evaluated at (
N
±
δ, δ→0), and
f
(
r
), which is the average of the other two.
Now, to answer the question “If a reagent (
R
) approaches to substrate (
S
),
what direction will be preferred?” one can assume that in the usual cases
the preferred direction is the one for which the initial dμ for the species
S
is
a maximum. The first term from the RHS of the Eq. (17) involved only the
global quantity and at the large distant is ordinary less direction sensitive
than second. Parr et al. [26, 28], therefore, opinioned that “
the preferred
direction is the one with largest f(r) at the direction side
” and gave us the
firm prediction -
Governing electrophilic attack
f
−
(
r
) = [∂
ρ
(
r
)/∂
N
]
−
v
(18)
Governing nucleophilic attack
f
+
(
r
) = [∂
ρ
(
r
)/∂
N
]
+
v
(19)
Governing neutral attack
f
0
(
r
) = [∂
ρ
(
r
)/∂
N
]
0
v
(20)
These three cases have μ
s
>μ
r
, μ
s
<μ
r
and μ
s
~μ
r
.
Computation of the local reactivity indices like the Fukui function in
the real molecular space is a very demanding task but diffi cult to evaluate
without further approximation. A “frozen core” approximation now gives
d
ρ
= d
ρ
value
in each case and therefore governs electrophilic attack,
f
−
(
r
) ≈ ρ
(HOMO)
(
r
)
(21)
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