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the electrophilicity index have direct link to the process of polarization
and transfer of charge from a substrate and, hence, control the energetic ef-
fect—the protonation energy. Considering all the above-mentioned funda-
mental nature of the physicochemical process of protonation and its prob-
able relationship with the quantum mechanical descriptors, we suggest an
ansatz for the computation of the PA in terms of these theoretical descrip-
tors. The physicochemical process and the energetic effect must entail the
above-stated four parameters. To derive an explicit relation to compute the
PA in terms of the above-stated descriptors, we suggest explicit interrela-
tionships between the protonation energy and the descriptors relying upon
their response toward the protonation.
PA ∞(-I)
(10)
PA ∞ S
(11)
PA ∞ 1 / χ
(12)
PA ∞ 1 / ω
(13)
Combining the above four relations, we obtain
PA=C+C 1 (-I) +C 2 S + C 3 (1/χ)+C 4 (1/ω)
(14)
where PA is the proton affi nity; C, C 1 , C 2 , C 3 , and C 4 are the regression
coeffi cient ; I is ionization energy; S is global softness; χ is the electronega-
tivity; and ω is the global electrophilicity index of the molecule.
In our model, we have invoked multilinear regression (MLR) to evalu-
ate these regression coeffi cient (C, C 1 , C 2 , C 3 , and C 4 ) and then we have
combined these calculated regression coeffi cient (C, C 1 , C 2 , C 3 , and C 4 )
with the aforesaid akin quantum chemical descriptors, the ionization en-
ergy (I), the global softness (S), the electronegativity (χ), and the global
electrophilicity index (ω) according to the Eq. (14) to evaluate the PA of
the individual molecule.
 
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