Interactions of formaldehyde and its substituted derivatives with HCN: structure, stability and interaction - Nguyen Ngoc Tri

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. REFERENCES 1. Grabowski S. J. Hydrogen bond - New Insight, Springer, Dordrecht, The Netherlands (2006). 2. Hobza P. and Havlas Z. Blue-shifting hydrogen bonds, Chem. Rev., 100, 4253-4264 (2000). 3. Domagala M. and Grabowski S. J. C-H∙∙∙N and C- H∙∙∙S hydrogen bonds – influence of hybridization on their strength, J. Phys. Chem. A, 109, 5683-5688 (2005). 4. Huang C. Y., Li Y. and Wang Ch. Sh. Rapid and accurate evaluation of the binding energies and the individual N-H∙∙∙O=C, N-H∙∙∙N, C-H∙∙∙O=C, and C- H∙∙∙N interaction energies of hydrogen-bonded peptide-base complexes, Sci. China Chem., 56, 238- 248 (2013). 5. Adrian-Scotto M. and Vasilescu D. Density functional theory study of (HCN)n clusters up to n = 10, J. Mol. Struc., 803, 45-60 (2007). 6. Rivelino R. and Canuto S. 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GenNBO 5.G, Theoretical Chemistry Institute, University of Wisconsin: Madison, WI (2001). 13. Crawford T.D. et al. WIREs Comput. Mol. Sci., 2, 556-565 (2012). 14. Frisch M. J. et al. Gaussian 09 (Revision A.02), Gaussian, Inc.: Wallingford, CT (2009). 15. Ho Quoc Dai, Nguyen Ngoc Tri, Nguyen Thi Thu Trang and Nguyen Tien Trung. Remarkable effects of substitution on stability of complexes and origin of the C-H∙∙∙O(N) hydrogen bonds formed between acetone’s derivative and CO2, XCN (X = F, Cl, Br), RSC. Adv., 4, 13901-13908 (2014). 16. Popelier P. L. A. atoms in molecules, Pearson Education Ltd.: Essex, UK (2000). 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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