Interaction of HCN with RCHO (R = H, F, Cl,
Br, CH3, NH2) induces twelve stable complexes with
the interaction energy in the range of -5.80 and -
21.07 kJ.mol-1 at the CCSD(T)/aug-ccpVDZ//MP2/aug-cc-pVDZ level. Their stability is
contributed by both Lewis acid-base interaction and
C-H∙∙∙N(O) hydrogen bond. It is remarkable that the
most stable P1-Hb complex of HCHO∙∙∙HCN has
been repoted for the first time. The SAPT analysis
indicates that electrostatic energy overcoming the
induction and dispersion energies plays an important
role in the stabilization of complexes.
The red-shifting hydrogen bonds are observed
in the P1-NH2, P2-NH2, P1-CH3 and P1-Ha
complexes. Remarkably, the red shift of C-H bond is
larger than that of N-H bond in these complexes. On
the contrary, the C-H∙∙∙N(O) blue-shifting hydrogen
bonds are found in the rest of complexes. The C-H
blue shifts in these hydrogen bonds are inversely
proportional to the C-H polarity in the isolated
monomer. NBO analysis is also performed carefully
to clarify the role of changes of σ*(C-H) and σ*(NH) electron density and s-character percentage of C
and N hybrid orbital on type of hydrogen bond in the
complexes examined
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Vietnam Journal of Chemistry, International Edition, 54(4): 448-453, 2016
DOI: 10.15625/0866-7144.2016-00345
448
Interactions of formaldehyde and its substituted derivatives with HCN:
structure, stability and interaction
Nguyen Ngoc Tri, Pham Thi Minh Tam, Nguyen Thi Hong Man, Ho Quoc Dai, Nguyen Phi Hung,
Nguyen Tien Trung
*
Department of Chemistry and Laboratory of Computational Chemistry and Modelling, Quy Nhon University
Received 10 May 2016; Accepted for publication 12 August 2016
Abstract
Twelve stable structures of the interactions of HCN with RCHO (R = H, F, Cl, Br, NH2, CH3) are located on the
potential energy surface at the MP2/aug-cc-pVDZ level. Interaction energies including both ZPE and BSSE corrections
range from -5.80 to -21.07 kJ.mol
-1
. The result of SAPT analysis shows that the electrostatic component has mainly
contributed to the stability of the complexes. It is remarkable that the most stable complex of HCHO∙∙∙HCN is P1-Hb
which has not been reported in the literature. The red-shifting hydrogen bonds of the C-H∙∙∙O and N-H∙∙∙N types are
observed in the P1-Hb, P1-CH3, P1-NH2 and P2-NH2 complexes. On the other hand, the C-H∙∙∙N(O) blue-shifting
hydrogen bonds are observed in the rest of complexes. The contraction of C-H bond and the blue shift of its stretching
vibrational frequency are inversely proportional with its polarity in the isolated monomer.
Keywords. Hydrogen bond, interaction energy, RCHO, HCN, QTAIM, SAPT.
1. INTRODUCTION
The hydrogen bonds of C-H∙∙∙O and C-H∙∙∙N
types play a crucial role in the supramolecular
structures for life, such as DNA, RNA, protein[1]
The investigation into factors affecting the formation
and the origin of hydrogen bonds as well as their
stability in these structures is urgent [2-4]. The HCN
is one of the important model molecules in the
theoretical studies, especially in the complexes of
transitional metals or metal ions [5-8]. As the
previous investigation, the stable complexes of
interaction between HCN and HCHO [8] were
contributed by both C-H∙∙∙O(N) hydrogen bond and
Lewis acid-base interactions. To our best knowledge,
complexes of interactions of HCN with RCHO (R =
F, Cl, Br, CH3, NH2) have not been reported.
Furthermore, this investigation isperformed to
clarify the stable structure, the stability and the role
of Lewis acid-base interactions and C-H∙∙∙O and C-
H∙∙∙N hydrogen bonds in the complex stabilization.
Moreover, in the present study, we use the modern
analysis methods, such as QTAIM, SAPT and NBO,
to thoroughly examine the monomers and their
complexes [9, 10].
2. COMPUTATIONAL METHODS
All the stable structures of monomers and their
complexes are optimized at the MP2/aug-cc-pVDZ
level. Interaction energies are calculated at the
CCSD(T)/aug-cc-pVDZ level with the geometric
structures optimized at the MP2/aug-cc-pVDZ level.
The interaction energy evaluated with only ZPE and
both ZPE and BSEE corrections are symbolized with
∆E and ∆E*, respectively. The topological geometry,
density of electron (ρ(r)), Laplacian of density
((ρ(r))) at the bond critical point (BCP) are
estimated by using AIM2000 program [11]. The
value of the total electron density transfer (EDT), s-
character percentage (%s) and the electron density at
the anti-bonding orbitals are estimated by means of
NBO 5.G program [12]. The energy components
contributing to the stability of the complexes,
namely electrostatic attraction (Eelest), induction
(Eind), dispersion (Edisp), exchange (Eexch) and the
second- and high-order level correlation (δint,r
HF
)
terms are calculated by Psi4 program with SAPT2+
approach [13]. All other calculations are performed
by Gaussian 09 (A.02) package [14].
3. RESULTS AND DISCUSSION
3.1. Geometric structures, interaction energies,
changes of C-H and N-H bond length involved in
hydrogen bond and their stretching vibrational
frequencies
VJC, 54(4) 2016 Nguyen Tien Trung, et al.
449
The interactions between HCN and RCHO (R =
H, F, Cl, Br, CH3, NH2) induce twelve stable
complexes with the Cs symmetry point group
corresponding to two P1 and P2 shapes, presented in
Figure 1. Particularly, P1 shape refers to the
complexes that have >C=O group involving in
interactions, while the P2 shape belongs to only C1-
H2 (or N-H) covalent bond involved in interactions.
Interaction energies (ΔE, ΔE*, kJ.mol-1) at
CCSD(T)/aug-cc-pVDZ//MP2/aug-cc-pVDZ are
given in table 1. The changes of C(N)-H bond length
(Δr, in Å), stretching vibrational frequency (Δν, in
cm
-1
) and its infrared intensity (ΔΙ, in km.mol-1) at
the MP2/aug-cc-pVDZ level, following
complexation, are also given in the table 1.
P1-Ha P1-Hb P1-F P1-Cl
P1-Br P1-NH2 P1-CH3 P2-F
P2-Cl P2-Br P2-CH3 P2-NH2
Figure 1: The optimized geometries of all complexes at the MP2/aug-cc-pVDZ level (distances in Å)
Table 1: Interaction energies and the changes of bond length, stretching vibrational frequency and
infrared intensity of C-H or N-H covalent bonds involved in hydrogen bonds
Shape R ΔE BSSE ΔE* Δr(C-H) Δν(C-H) ΔΙ(C-H)
P1
Ha -14.06 3.35 -10.71
-0.0015 23.00 -45.53
-0.0005(C5-H7) 5.89 2.55
Hb -17.32 4.21 -13.12 0.0073 -107.78 334.46
F -14.16 3.88 -10.28 -0.0002 6.18 -12.28
Cl -14.42 4.18 -10.23 -0.0005 10.06 -14.00
Br -14.88 4.85 -10.03 -0.0005 9.55 -13.55
CH3 -21.28 4.67 -16.61 0.0101 -172.56 564.94
NH2 -25.83 4.76 -21.07 0.0117 -150.99 464.31
P2
F -14.18 3.97 -10.20 -0.0004 15.19 -1.52
Cl -14.68 4.67 -10.01 -0.0014 31.52 16.59
Br -15.57 5.33 -10.24 -0.0013 30.64 28.65
CH3 -9.53 3.73 -5.80
-0.0034 41.88 -22.33
-0.0007(C4-H9(10)) 3.71 -1.04
NH2 -17.58 4.34 -13.24 0.0046 (N4-H9) -36.85 125.40
VJC, 54(4) 2016 Interactions of formaldehyde and its substituted
450
Table 2: Deprotonation energy (DPE) of C-H or N-H bonds involved in hydrogen bond and proton affinity
(PA) at O (N) atoms at the CCSD(T)/aug-cc-pVDZ//MP2/aug-cc-pVDZ level (in kJ.mol
-1
)
Monomer HCHO FCHO ClCHO BrCHO CH3CHO NH2CHO HCN
DPE(C(N)-H) 1681.9 1579.7 1530.4 1497.2 1654.3 1636.7(C); 1533.0(N) 1460.0
PA(O(N)) 709.5 649.0 685.2 694.3 767.7 831.3 704.5(N)
As shown in figure 1, the intermolecular
distances of O3∙∙∙C5, H2(9)∙∙∙N6 and H7∙∙∙O3
contacts are in the range of 2.94-3.07 Å, 2.15-2.73 Å
and 1.98-2.71 Å, respectively. All of them are
smaller than the total of van der Waals radii of two
atoms involved in these interactions (van der Waals
radii of O, H, C, N atoms are in turn 1.52, 1.20, 1.70
and 1.55 Å). These values indicate the presence of
hydrogen bonds and Lewis acid-base interactions
upon complexation, namely H7∙∙∙O3, H2(9)∙∙∙N6 and
O3∙∙∙C5 contacts. It is noticeable that, in the P2-CH3
complex, the hydrogen bonds are formed between
C4-H9(10)∙∙∙N6 contacts in spite of their distance
(ca. 3.08 Å) slightly larger than the sum of van der
Waals radii of H and N atoms. This result should be
assigned to the additional effect of the remaining
interactions in the complex [15].
The interaction energies in the complexes
considered are quite negative, which are in range
from -9.53 to -25.83 with only ZPE correction and
from -5.80 to -21.07 kJ.mol
-1
with both ZPE + BSSE
corrections. In particular, P1-NH2 is the most stable
complex (∆E* = -21.07 kJ.mol-1), while P2-CH3 is
the least complex (∆E* = -5.08 kJ.mol-1). It is
remarkable that the P1-Hb, P1-CH3, P1-NH2 and
P2-NH2 complexes are more stable than the rest of
complexes in spite of only one H∙∙∙O(N) hydrogen
bonding contact in each complex. Generally,
interaction energies of the complexes decrease in the
order of Br ≈ Cl ≈ F ≈ Ha < Hb < CH3 < NH2
derivatives (P1 shape) and CH3 < Cl ≈ F ≈ Br < NH2
derivatives (P2 shape). This trend is due to the
change of DPE values of C-H, N-H bonds and PA at
O and N sites in the isolated monomers that are
involved in the hydrogen bond and Lewis acid-base
interaction (cf. table 2).
The calculated results show that the DPE(C-H)
(in HCN) < DPE(N-H) (in NH2CHO) < DPE(C-H)
(in RCHO). This means that the polarity decreases in
the order of the C-H bond (HCN), to the N-H bond
(NH2CHO) and then to C-H bond (the other
monomers). In addition, the PAs at O site in HCHO,
CH3CHO and NH2CHO are larger than that at N site
in HCN. As a result, the H∙∙∙O intermolecular
interaction is stronger than the H∙∙∙N interaction
upon complexation. The C-H∙∙∙O and N-H∙∙∙N
hydrogen bonds are thus more stable than the C-
H∙∙∙N. Consequently, the P1-Hb, P1-NH2, P1-CH3
and P2-NH2 complexes have the larger stability in
comparision with the remaining complexes. In the
P1-Ha, despite the existence of the C-H∙∙∙O
hydrogen bond, it is less stable than the complexes
mentioned above. It should arise from the steric
effect on interactions formed in complexes. In the
following analyses we consider it more detailed.
Following complexation, the replacement of one
H atom in HCHO by halogen atoms (F, Cl, Br)
causes an increase in strength of hydrogen bond and
a decrease of strength of Lewis acid-base interaction.
Thus, DPE(C-H) decreases in the order: HCHO
> FCHO > ClCHO > BrCHO, and PA(O) decreases
in the order: HCHO > BrCHO > ClCHO > FCHO.
As a consequence, the stability of halogenated
derivatives’ complexes is slightly different and
approximates to the P1-Ha complex. The interaction
energy calculated for P1-Ha complex is in a good
agreement with that in the previous study [8].
Nevertheless, the most stable P1-Hb found in this
present study is more stable than P1-Ha, which has
not been reported in any literature.
In the cyclic and halogenated complexes, a
contraction of C-H bond length compared to that in
the relevant monomer, involved in hydrogen bonds,
ranges from 0.0002 to 0.0034 Å, which is
accompanied by an increase in the strectching
vibrational frequencies and a decrease of the infrared
intensities (see table 1). Our obtained results on
changes of C-H bond length and its stretching
vibrational frequency in HCHO∙∙∙HCN are in a good
agreement with the results reported in ref. [8].
Accordingly, these hydrogen bonds are classified as
blue-shifting hydrogen bonds [2]. The blue shift of
C-H distance is larger in P1-Ha than in P1-X (X = F,
Cl, Br). The C-H blue shift is much larger for P2-
CH3 than for P2-X (X = F, Cl, Br). The magnitude
of C-H blue shift in these complexes is in line with
the trend of polarity of C-H bond in the isolated
monomers. Indeed, as shown in table 2, DPE(C-H)
of CHO group in HCHO and CH3CHO is much
larger than that in XCHO (X = F, Cl, Br). The red-
shifting hydrogen bond is observed in the P1-Hb,
P1-CH3, P1-NH2 and P2-NH2 complexes. It is
remarkable that the C5-H7 red shift in the C5-
H7∙∙∙O3 hydrogen bond is larger than the N4-H5 red
VJC, 54(4) 2016 Nguyen Tien Trung, et al.
451
shift in the N4-H9∙∙∙N6 hydrogen bond, which is due
to both the larger PA at O sites in HCHO, CH3CHO
and NH2CHO, and the larger polarity of C-H bond in
HCN relative to PA at N site in HCN and the
polarity of N4-H9 bond in NH2CHO.
3.2. The AIM-, SAPT- and NBO-analyses
To more understand about the formation,
strength and the nature of interactions in complexes,
we performed the AIM analysis at the same level of
theory, and results are illustrated in figure 2.
P1-Ha P1-Hb P1-F
P1-Cl P1-Br P1-CH3
P1-NH2 P2-F P2-Cl
P2-Br P2-CH3 P2-NH2
Figure 2: The topological geometry of the stable
complexes at the MP2/aug-cc-pVDZ level
The obtained results indicate that there is
existence of BCPs between O3∙∙∙C5 and H∙∙∙O(N)
interactions with their corresponding electron
density and Laplacian in the range of 0.0053-0.0232
au and 0.0161-0.0777 au. All of them fall within the
critical limit for formation of weak interactions [16].
Thus, the O3∙∙∙C5 and H∙∙∙O(N) intermolecular
interactions are Lewis acid-base interactions and
hydrogen bonds, respectively. The electron densities
at the H7∙∙∙O3 and H9∙∙∙N6 BCPs in the noncyclic
complexes by ca. 0.0169-0.0232 au are significantly
larger than those at BCPs of the other hydrogen
bonded contacts and Lewis acid-base interactions in
the rest of complexes (ca. 0.0053-0.0150 au).
Therefore, the intermolecular interactions in the P1-
Hb, P1-CH3, P1-NH2 and P2-NH2 complexes are
more stable than in the remaining complexes.
To gain further insight into the role of
interactions to the complex stability, the energy
components contributing to the stabilization energy
are calculated using SAPT2+ approach at the aug-
cc-pVDZ basis set and tabulated in Table 3. The
SAPT energy (ESAPT) is expressed as the sum of five
terms as given below: ESAPT = Eelest + Eind + Edisp +
Eexch + δEint,r
HF
[9, 10], where Eelest, Eind, Edisp, Eexch
and δint,r
HF
are electrostatic, induction, dispersion,
exchange energy terms and the second- and high-
order level correlation, respectively.
As shown in table 3, the electrostatic attraction
term (Eelest) overcomes the other energy components,
indicating a larger role of this force in stabilizing
complex. In addition, the induction and dispersion
energies also contribute to complexation strength.
The interaction energies of complexes calculated
using SAPT2+ approach (see table 3) are in a good
agreement with the CCSD(T) method (see table 1).
As a result, the P1-Hb, P1-CH3, P1-NH2 and P2-
NH2 complexes are more stable than the remaining
complexes, and P1-Hb is more stable than P1-Ha.
Table 3: The energy components contributing to stability of complexes at
the SAPT2+/aug-cc-pVDZ level (in kJ.mol
-1
)
Shape R Eelest Eind Edisp Eexch δEint,r
HF
ESAPT
P1
Ha -21.71 -8.56 -10.50 26.73 -2.33 -16.36
Hb -27.10 -9.66 -8.07 26.24 -3.51 -22.11
F -18.69 -7.12 -9.08 22.58 -1.71 -14.03
Cl -18.81 -7.83 -10.19 25.20 -2.05 -13.68
Br -18.60 -7.83 -10.40 25.55 -2.15 -13.43
CH3 -32.69 -12.70 -9.74 33.49 -4.73 -26.38
NH2 -39.34 -14.52 -10.53 38.09 -5.59 -31.90
P2
F -18.92 -4.60 -6.04 15.41 -1.58 -15.73
Cl -18.91 -5.06 -6.73 16.53 -1.77 -15.94
Br -20.49 -6.37 -8.51 20.44 -2.17 -17.10
CH3 -9.48 -2.48 -6.31 8.74 -0.49 -10.01
NH2 -26.01 -7.85 -8.39 23.59 -2.47 -21.13
VJC, 54(4) 2016 Interactions of formaldehyde and its substituted
452
NBO analysis is performed for the monomers
and their complexes, and the selected results are
shown in figure 3 and table 4. The existence of
Lewis acid-base interactions and hydrogen bonds as
well as their stability in the complexes might be
further understood by using iso-surface of
complexes (see figure 3). It is clear that there is an
overlap of electron density between monomers
following complexation, implying the presence of
the intermolecular contacts, including the hydrogen
bond and Lewis acid-base interaction in the
complexes.
Furthermore, as shown in table 4, the EDT
values in the halogenated and in P2-CH3, P2-NH2
complexes are negative, and in the rest of complexes
those are positive. This means that for halogenated
and P2-CH3, P2-NH2 complexes, there is a transfer
of electron density from HCN to RCHO, and
inversely the electron density transfer occurs from
RCHO to HCN in the rest of the complexes. A C-H
bond contraction and a blue-shift of its stretching
vibrational frequency in the C-H∙∙∙N(O) hydrogen
bond in P1-F, P2-F, P2-Cl and P2-Br complexes
are determined by an increase of s-character
percentage of C atom overcoming a slight increase
of σ*(C-H) orbital. In P1-Ha, P1-Cl, P1-Br and P2-
CH3 complexes, the blue-shifts depend on both an
increase of s-character percentage of C atom and a
decrease of σ*(C-H) electron density. On the other
hand, an elongation of C-H and N-H bond involved
in hydrogen bond, accompanied by a red-shift of
their stretching vibrational frequencies, in the P1-Hb,
P1-CH3, P1-NH2 and P2-NH2 complexes is due to
an increase of σ*(C-H) and σ*(N-H) electron
density predominating over an increase of s-
character percentage of C and N atoms following
complexation.
P1-Ha P1-Hb P1-F
P1-Cl P1-Br P1-CH3
P1-NH2 P2-F P2-Cl
P2-Br P2-CH3 P2-NH2
Figure 3: The total electronic density for the
complexes at the MP2/aug-cc-pVDZ level
(isovalue = 0.007 au/Å
3
)
Table 4: Selected results of NBO analysis at the MP2/aug-cc-pVDZ level
Shape R EDT (e) Δσ*(C(N)-H) (e) Δs(C/N) (%)
P1
Ha 0.0069
-0.0021 0.61
-0.0002 0.43
Hb 0.0226 0.0165 1.03
F -0.0014 0.0001 0.61
Cl -0.0012 -0.0002 0.68
Br -0.0015 -0.0002 0.75
NH2 0.0282 0.0210 1.37
CH3 0.0273 0.0202 1.18
P2
F -0.0127 0.0018 1.34
Cl -0.0137 0.0006 1.96
Br -0.0141 0.0008 2.23
CH3 -0.0025
-0.0027 0.50
0 0.09
NH2 -0.0143 0.0121 1.78
VJC, 54(4) 2016 Nguyen Tien Trung, et al.
453
4. CONCLUSIONS
Interaction of HCN with RCHO (R = H, F, Cl,
Br, CH3, NH2) induces twelve stable complexes with
the interaction energy in the range of -5.80 and -
21.07 kJ.mol
-1
at the CCSD(T)/aug-cc-
pVDZ//MP2/aug-cc-pVDZ level. Their stability is
contributed by both Lewis acid-base interaction and
C-H∙∙∙N(O) hydrogen bond. It is remarkable that the
most stable P1-Hb complex of HCHO∙∙∙HCN has
been repoted for the first time. The SAPT analysis
indicates that electrostatic energy overcoming the
induction and dispersion energies plays an important
role in the stabilization of complexes.
The red-shifting hydrogen bonds are observed
in the P1-NH2, P2-NH2, P1-CH3 and P1-Ha
complexes. Remarkably, the red shift of C-H bond is
larger than that of N-H bond in these complexes. On
the contrary, the C-H∙∙∙N(O) blue-shifting hydrogen
bonds are found in the rest of complexes. The C-H
blue shifts in these hydrogen bonds are inversely
proportional to the C-H polarity in the isolated
monomer. NBO analysis is also performed carefully
to clarify the role of changes of σ*(C-H) and σ*(N-
H) electron density and s-character percentage of C
and N hybrid orbital on type of hydrogen bond in the
complexes examined.
Acknowledgement. This work is supported by
Vietnam National Foundation for Science and
Technology Development (NAFOSTED) by grant
number 104.06-2014.08.
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Corresponding author: Nguyen Tien Trung
Department of Chemistry and Laboratory of Computational Chemistry
and Modelling, Quy Nhon University
170, An Duong Vuong Street, Quy Nhon City, Binh Dinh Province.
E-mail: nguyentientrung@qnu.edu.vn.
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