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Original article
10 (
2_suppl
); S1847-S1854
doi:
10.1016/j.arabjc.2013.07.011

Synthesis, characterization and density functional theory investigations of the N,N-diacylaniline derivatives

Department of Chemistry, Faculty of Science, King Khalid University, P.O. Box 9004, Abha 61413, Saudi Arabia
Unit of Science and Technology, Faculty of Science, King Khalid University, P.O. Box 9004, Abha 61413, Saudi Arabia

⁎Corresponding authors. Tel.: +966 72418632; fax: +966 72418426. agmasq@gmail.com (Abdullah G. Al-Sehemi), irfaahmad@gmail.com (Ahmad Irfan)

Disclaimer:
This article was originally published by Elsevier and was migrated to Scientific Scholar after the change of Publisher.

Peer review under responsibility of King Saud University.

Abstract

Different N,N-diacylaniline derivatives such as N-acetyl-N-(2-methoxyphenyl)acetamide, N-acetyl-N-(2-Methoxy-phenyl)-4-nitrobenzamide, N-(4-nitrobenzamide)-N-(2-Methoxy-phenyl)-4-bromobenzamide, N-Acetyl-4-nitro-N-o-tolyl-benzamide, N-Acetyl-N-o-tolyl-acetamide, and 2-Chloro-N-(2-chloro-acetyl)-N-o-tolyl-acetamide have been synthesized and characterized by FTIR and NMR techniques. The ground state geometries have been optimized by using density functional theory (DFT) at B3LYP/6–31G∗ level. The frequencies have been computed at the same level of theory. To shed light on the rotational barrier, the electron correlation has been taken into account. The steric effect of o-substituents twists the aromatic ring out of planarity with the imide moieties, creating an axis of chirality. The introduction of different substituents on the benzene ring causes some changes in the ring C–C bond distances. The observed vibrational assignments and analysis of DAA (2f) have been discussed in terms of fundamental bands.

Keywords

N,N-Diacylaniline derivatives
Density functional theory
Geometric parameters
FTIR
1

1 Introduction

The 4(3H)-Quinazolinones and their derivatives (Panicker et al., 2009; El-Hiti, 1999) are found in a number of biologically active compounds. They are used in medicine because of their wide spectrum of biological activities such as antitumor, antibacterial and antifungal, antimicrobial activities (Pendergast et al., 1993). Several quinazoline derivatives have been reported for their antibacterial, antifungal, anti-Human Immunodeficiency Virus (HIV) (Alagarsamy et al., 2006), anti-inflammatory (Alagarsamy et al., 2006), anticonvulsant (Gupta et al., 1988), antidepressant (Jatav et al., 2008), hypolipidemic (Joshi and Chaurasia, 1987), antiulcer (Prouse, 1993), analgesic (Bhandari et al., 2008) or immunotropic activities (Azza et al., 2004). Some of the aminoquinazoline derivatives were found to be inhibitors of the tyrosine kinase (Fry et al., 1994) or dihydrofolate reductase enzymes (Traxler et al., 1996) and so they work as potent anticancer agents. Yamada reported that twisted amide groups e.g., ones in which >NC(=O) and NC = O planes are not coincident, are more reactive to nucleophiles than planar ones (Yamada, 1995, 1992a,b; Yamada and Ohe, 1996; Yamada et al., 1996).

Kondo and co-workers reported the synthesis of N-aryl imides (Kondo et al., 1999) which possess axial chirality, in enantiopure form. The planes containing the imide groups and the phenyl ring of diacylanilines (DAA) in their most stable conformations are twisted to relieve unfavorable steric interaction between the ortho-substituent on the phenyl ring and the imide. Both the torsion angle between their planes and the barrier to rotation around the N-Ar bond are increased by an increase in the size of the ortho-substituent on the phenyl ring. A number of groups have attempted to predict barriers to rotation by computational methods. The Charlton’s group at the University of Manitoba used semi empirical (AM1) methods to calculate the expected barriers to rotation in arylnaphalene lignans (Charlton et al., 1996). The absolute values of the calculated barriers were off by more than (5 kcal/mol−1) in some cases. Pregosin’s group attempted to use molecular mechanic (MM+) calculations to predict the rotational barriers of biaryl phosphine ligands with slightly less reliable relative prediction (Trabesinger et al., 1997). They also found that the absolute values of the calculated barriers were far removed from the experimentally determined values. Ab initio calculations of the rotational barrier of 2,2′-bipyridine were carried out by Sean Howard at the University of Wales (Howard, 1996). Even at the ab initio level, the absolute value of the barrier to rotation of 2,2′-bipyridine was underestimated by 20–30%. Density functional theory (DFT) calculations of the rotational barrier of 3-(o-aryl)-5-methyl-rhodanines were carried out by (Aydeniz et al., 2004). They found good agreement with the available experimental result.

In the present study, we have synthesized new derivatives of DAA then characterized by advanced techniques like FTIR spectrometry and NMR. With the aim to shed light on the geometrical parameters, we have optimized the ground state geometries by using DFT which has been proved to be an efficient and reliable approach (Irfan et al., 2008, 2009, 2010, 2011, 2012, 2013; Irfan and Al-Sehemi, 2011, 2012). The effect of different substituents has been investigated on the rotation barriers. The 2a2f have been synthesized by substituting methyl and methoxy at position R; methyl, p-nitrobenzene, p-bromobenzene, and methyl chloride at R1 and R2, see Fig. 1 and Scheme 1. The FTIR spectra computed at the DFT level has been compared with experimental one for 2f. By using advanced computational means we have shed light on the geometrical parameters and the vibrational modes of C–H Vibrations, C = O Vibrations, C–C Vibrations, and N–C Vibrations.

Optimized geometries of the studied diacylaniline DAA (2a–2f) for the most stable conformers at the B3LYP/6–31G∗ level of theory.
Figure 1 Optimized geometries of the studied diacylaniline DAA (2a–2f) for the most stable conformers at the B3LYP/6–31G∗ level of theory.
Schematic diagram of the investigated DAA in the present study.
Scheme 1 Schematic diagram of the investigated DAA in the present study.

2

2 Experimental details

2.1

2.1 General procedure for di-acylation of aniline derivatives (DAA)

To a solution of the monoacyl aniline derivative (details can be found in Supporting Information) (1) (1 mol. eq.), in dry dichloromethane (2 cm3/g) containing dry pyridine (1.5 mol. eq.), was added acid chloride (2–3 mol. eq.) dropwise over 10 min. and the mixture was stirred and heated under reflux for 2–4 days, monitoring the disappearance of the starting N-acylanthranilate by TLC. After cooling, additional dichloromethane was added, the solution washed with aqueous sodium hydrogen carbonate, then water, dried and the solvent removed under reduced pressure to give the di acyl aniline DAA (2). General synthetic procedure for such kind of materials can be found in references (Al-Sehemi et al., 2013).

2.2

2.2 N-acetyl-N-(2-methoxyphenyl)acetamide (2a)

The general procedure for the N-acylation of amines was followed using 2-methoxy phenyl acetamide (1a) (2 g, 16.2 mmol), pyridine (3.86 g, 48.8 mmol) and acetyl chloride (3.83 g, 48.8 mmol). After work-up, N-acetyl-N-(2-methoxyphenyl) acetamide (2a) was obtained as a light brown oil (2.8 g, 83%). b.p 185 - 199 ° C , δ 1H NMR (CDCl3) 2.06 (6H, s, 2 × CH3CO), 3.59 (3H, s, CH3O), 6.85, 6.94 and 7.20 [4H, m, 4 × CH (ph)]; δ C (CDCl3, 125 MHz) 26.27 and 26.39 (2 × CH3CO), 55.55 (OCH3), 112.3, 120.9, 128.1 and 129.6 [4 × CH (Ar) ], 121.3 (C = CN), 154.75 (OCH3) and 172.67 and 172.99 (2 × CO).

2.3

2.3 N-acetyl-N-(2-Methoxy-phenyl)-4-nitro-benzamide (2b)

The general procedure for the N-acylation of amines was followed using N-(2-Methoxy-phenyl)-4-nitro-benzamide (1b) (1 g, 3.7 mmol), pyridine (0.72 g, 9.2 mmol) and acetyl chloride (0.73 g, 9.2 mmol). After work-up, N-acetyl-N-(2-Methoxy-phenyl)-4-nitro-benzamide (2b) was obtained as a light brown powder (0.8 g, 69%). m. p 132 ° C , δ 1H NMR (DMSO) 2.48–2.5 (3H, overlap with DMSO signal, s, CH3CO), 3.84 (3H, s, OCH3), 6.99 [1H, ddd, J 8.6, 7.6 and 1.1, CH (Ar) ], 7.12 [1H, dd, J 8.6 and 1.1, CH (Ar)], 7.23 [1H, ddd, J 8.6, 7.6 and 1.1, CH (Ar)], 7.72 [1H, ddd, J 8.6, 7.6 and 1.1, CH (Ar)], 8.19 and 8.36 [4H, m, CH (Ar)]; δ C (DMSOd, 125 MHz) 39.2 (CH3CO), 55.7 (OCH3), 111.5, 123.6, 124.9, 125.0, 126.1, 126.2, 126.4 and 129.1 [8 × CH (Ar) ], 140 (C-CO), 149.1 (C-NO2) and 151.8 and 151.9 (2 × CO).

2.4

2.4 N-(4-nitrobenzamide)-N-(2-Methoxy-phenyl)-4-bromo-benzamide (2c)

The general procedure for the N-acylation of amines was followed using N-(2-Methoxy-phenyl)-4-bromo-benzamide (1c) (1 g, 3,3 mmol), pyridine (0.65 g, 8.2 mmol) and 4-nitrobenzoyl chloride (1.52 g, 8.2 mmol). After work-up, N-(4-nitrobenzamide)-N-(2-Methoxy-phenyl)-4-bromo-benzamide (2c) was obtained as a yellowish white powder (1 g, 67%). m. p 139 - 142 ° C , δ 1H NMR (CDCl3) 3.86 (3H, s, OCH3), 6.85 [1H, dd, J 8.1 and 1.3, CH (Ar)], 6.95 [1H, ddd, J 9.1, 7.8 and 1.4, CH (Ar)], 7.03 [1H, ddd, J 9.1, 7.8 and 1.4, CH (Ar)], 7.56 [3H, m, CH (Ar)], 7.68–7.7 [3H, m, CH (Ar)], and 8.40–8.45 [2H, m, CH (Ar)]; δ C (DMSOd, 125 MHz) 55.9 (OCH3), 109.9, 119.9, 121.3, 124.1, 126.4, 127.5, 128.7, 132.0 and 134.2 [CH (Ar)], 148.3 [C = C–NO2] and 164.3 (CO); FTIR ν/cm−1:3409 (N–C = O), 1717(C = O),1667(C = O), 1490(N–O), 1480(N = O), 1341(C–O–C).

2.5

2.5 N-Acetyl-4-nitro-N-o-tolyl-benzamide (2d)

The general procedure for the N-acylation of amines was followed using 4-Nitro-N-o-tolyl-benzamide (1d) (1 g, 3.9 mmol), pyridine (0.77 g, 9.8 mmol) and acetyl chloride (0.77 g, 9.8 mmol). After work-up, N-Acetyl-4-nitro-N-o-tolyl-benzamide (2d) was obtained as a yellowish brown powder (0.8 g, 69%). m. p 120 - 123 ° C, δ 1H NMR (CDCl3) 2.20 (3H, s, CH3), 2.21 (3H, s, CH3CO), 7.0–7.3 [4H, m, CH (Ar)], 7.62 [2H, m, CH (Ar)] and 8.13 [2H, m, CH (Ar)]; δC (DMSOd, 125 MHz) 17.9 (CH3), 25.5 (CH3CO), 123.5, 127.6, 128.8, 129.1, 129.6, 131.7, 135.9 and 137.3 [8 × CH (Ar)], 134.5 (C = C–CH3), 138.2 (C = C–N), 141.5 (C = C–CO), 149.0 (C = C–NO2) and 170.6 and (CO).

2.6

2.6 N-Acetyl-N-o-tolyl-acetamide (2e)

The general procedure for the N-acylation of amines was followed using 2-methyl aniline (2 g, 18.7 mmol), pyridine (4.43 g, 56 mmol) and acetyl chloride (4.4 g, 56 mmol). After work-up, N-Acetyl-N-o-tolyl-acetamide (2e) was obtained as a clear pale yellow liquid (3.1 g, 87%). b. p 139 - 142 ° C, δ 1H NMR (CDCl3) 1.96 (3H, br s, CH3), 2.03 (6H, br s, CH3CO), 6.8–7.13 [4H, br m, CH (Ar)]; δ C (DMSOd, 125 MHz) 17.6 (CH3), 26.3 (2 × CH3CO), 126.9, 127.2, 127.4 and 131.1 [4 × CH(Ar)], 135.9 (C = C–CH3), 138.5(C = C–N) and 127.2 (C = O).

2.7

2.7 2-Chloro-N-(2-chloro-acetyl)-N-o-tolyl-acetamide (2f)

The general procedure for the N-acylation of amines was followed using 2-methyl aniline (2 g, 18.7 mmol), pyridine (4.43 g, 56 mmol) and chloro acetyl chloride (6.32 g, 56 mmol). After work-up, 2-Chloro-N-(2-chloro-acetyl)-N-o-tolyl-acetamide (2f) was obtained as a beige powder (3.9 g, 80%). m. p 103 - 108 ° C , δ 1H NMR (CDCl3) 2.10 (3H, s, CH3), 4.23 and 4.36 (4H, br m, CH2) and 7.0–7.4 [4H, br m, CH (Ar)]; δ C (DMSOd, 125 MHz) 17.5 (CH3), 45.3 (2 × CH2), 127.9, 128.7, 130.5 and 131.9 [4 × CH(Ar)], 135.1 (C = C–CH3), 136.3 (C = C–N) and 168.5 (CO).

2.8

2.8 Synthesis of 2-Substituted N,N-Diacylanilines

Ortho-(or 2-) Substituted anilines (1) undergo N-N-diacetylation more easily than ortho-unsubstituted ones (Scheme 1). On the basis of our investigations on the N,N-diacetylation of ortho-substituted anilines (1), we planned to explore the potential applications of the ortho-substituted N,N-diacetylanilines in acetylation reaction. The imide character of the N,N-diacetylanilines (2), which was easily prepared from the corresponding ortho-substituted anilines (1). It is expecting that it would serve as a good acetylating reagent to nucleophiles. Acetylation of amines is one of the most fundamental transformations in organic chemistry and selective acetylation of the less hindered amino group in polyamines is often required. In this work a simple but powerful reagent for selective acetylation in a series of structurally diverse diamines is described. The general route for the synthesis of N-N-diacetylation aniline derivative is shown in Scheme 1. In general diacylation of the aniline with acid chloride and pyridine proceeded in high yields and in most of the products diacylanline was crystalline with short reaction times and absence of excess acid chloride.

3

3 Computational Study

All the calculations have been performed by using Gaussian09 package (Frisch et al., 2009). The ground state geometries have been optimized using DFT. Becke’s three parameter gradient-corrected exchange potential and the Lee–Yang–Parr gradient-corrected correlation potential (B3LYP) (Becke, 1993; Miehlich et al., 1989; Lee et al., 1988; Al-Sehemi et al., 2012, 2013; Al-Sehemi and Irfan, 2017) and 6–31G∗ basis set (Sun et al., 2007) have been used for all the calculations. The frequencies have been computed at the same level of theory and no imaginary frequency has been observed. ChemCraft (Rofouei et al., 2010) graphical interface was used to assign the calculated harmonic wave numbers using scaled displacement vectors to identify the motion of modes.

4

4 Results and discussions

4.1

4.1 Molecular geometries

The optimized structures of the DAA (2a2f) for the most stable conformers and atomic numbering are presented in Fig. 1. The optimized geometric parameters (bond lengths, bond angles and dihedral angles) calculated by DFT/B3LYP with 6–31G∗ basis set are listed in Tables S1–S3.

Since it is known that the electron correlation should be taken into account when dealing with rotational barriers in imide in order to keep the computational effort within reasonable limits we choose the DFT approach as a theoretical method. It is known that this method may achieve a greater accuracy than the Hartree–Fock (HF) theory. Recently we showed that DFT is good to reproduce the experimental data (Al-Sehemi et al., 2012, 2013; Al-Sehemi and Irfan, 2017; Irfan et al., 2008, 2009, 2010, 2011, 2012, 2013; Irfan and Al-Sehemi et al., 2011, 2012). The DFT approach overcomes the major limitation of the HF theory, i.e., the negligence of electron correlation, by including some of the electron correlation effects. Also it has been shown that DFT calculations provide the torsional barriers in good accord with the experimental values.

The amide functional group contains planar, sp2-hybridized nitrogen resulting from the conjugation of the nitrogen lone pair with the adjacent carbonyl functionality granting the carbonyl-nitrogen bond a partial double bond character. Unsymmetrical N,N-disubstituted imides have two possible ground states that interconvert by a single rotation of the N-carbonyl bond. We expect the barrier to rotation around N-CO bond to be too high, due to the both steric and electronic effects of substituents. The steric effect of o-substituents (such as OMe and Me in the present case) twists the aromatic ring out of planarity with the imide moieties, creating an axis of chirality. The DFT calculations showed that the amide and aryl planes were roughly perpendicular to one another with torsion angles of 94°, 112°, 51°, 100°, 83° and 72° for the C1–C6–N1–C8 and 90°, 87°, 107°, 93°, 96° and 101° for torsion angle C1–C6–N1–C15.

The optimized structures have been compared with some available previous studies having similar parent compounds. The introduction of different substituent groups on the benzene ring causes some changes in the ring C–C bond distances. Changing the position of the substituents in the benzene ring also affects the C–C bond distances. The electron donor/acceptor capabilities play a very important role in shaping the structural and electronic properties of the molecules. The optimized bond lengths of C-C in the phenyl ring fall in the range from 1.388 to 1.418 Å at B3LYP/6–311G∗ level of theory while 1.375 to 1.407 Å at HF/6–311 + G∗∗ level of theory, which are in good agreement with experimental evidences 1.378–1.407 Å (Rofouei et al., 2010). The optimized C6–N2 bond length is in range 1.438–1.454 Å at B3LYP/6–31G∗ level of theory. The experimental C6-N2 bond length is reported as 1.413 Å (Rofouei et al., 2010).

4.2

4.2 Experimental and Calculated FTIR Assignments

The 2f molecule consists of 27 atoms, so it has 75 normal vibrational modes. The observed vibrational assignments and analysis of 2f are discussed in terms of fundamental bands. The FTIR spectrum of 2f has been illustrated in Fig. 2. Table 1 summarizes the experimental and calculated vibrational frequencies. According to the theoretical calculations, the 2f has C1 point group symmetry. The comparison of the frequencies calculated by DFT with the experimental values reveals good agreement with calculated vibrational modes due to the inclusion of electron correlation for this method. It should be noted that calculations were made for a free molecule in vacuum, while experiments were performed for solid sample. In this study, we have used the scaling factor of 0.9585.

Experimental and calculated FTIR spectra of the DAA (2f) at B3LYP/6–31G∗ level of theory.
Figure 2 Experimental and calculated FTIR spectra of the DAA (2f) at B3LYP/6–31G∗ level of theory.
Table 1 Comparison of the calculated and experimental FTIR vibrational spectrum of DAA (2f).
Mode nos. b3lyp/6–31G(d,p) Experimental Vibrational Assignments
1 3085 υas. C–H (CH2Cl)
2 3083 υsy. C–H (Ph–ring)
3 3070 υas. C–H(Ph–ring)
4 3060 υas. C–H (CH2Cl)
5 3059 υas. C–H(Ph–ring)
6 3054 υas. C–H(Ph–ring)
7 3017 υsy. C–H (CH2Cl)
8 3010 υas. C–H (CH3)
9 3008 υsy. C–H (CH2Cl)
10 2991 υas. C–H (CH3)
11 2932 υsy. C–H (CH3)
12 1745 1734 υ C = O
13 1709 1715 υ C = O
14 1593 1583 υas. C–C (Ph–ring)
15 1568 1490 υas. C–C (Ph–ring)
16 1477 υas. C–C (Ph–ring)
17 1464 υas. C–C (Ph–ring)
18 1453 sciss C–H (CH3)
19 1433 ρ C–H(Ph–ring) + sciss C–H (CH2Cl)
20 1427 ρ C–H(Ph–ring) + sciss C–H (CH2Cl)
21 1392 1387 υas. C–N
22 1382 1317 υsy. C–N
23 1293 1317 β C–H (Ph–ring) + C–H (CH2Cl)
24 1287 β C–H (Ph–ring) + C–H (CH2Cl)
25 1281 υsy .C–N + ω C–H (CH2Cl)
26 1265 1259 ρ C–H(Ph–ring)
27 1258 1232 ρ C–H(Ph–ring)
28 1216 ρ C–H(Ph–ring)
29 1173 ρ C–H(Ph–ring)
30 1161 τ C–H (CH2Cl)
31 1146 sciss C–H(Ph–ring)
32 1130 ρ C–H(Ph–ring)
33 1110
34 1072
35 1035 1042 γ C–H(Ph–ring) + τ C–H (CH3)
36 1033 γ C–H(Ph–ring) + ω C–H (CH3)
37 979 990 γ C–H(Ph–ring) + ω C–H (CH3)
38 972 944 γ C–H(Ph–ring)
39 949 932 γ C–H(Ph–ring)
40 921 τ C–H (CH2Cl) + υ C–N
41 908 γ C–H(Ph–ring)
42 903 862 γ C–H(Ph–ring)
43 867 γ C–H(Ph–ring)
44 845 790 γ C–H(Ph–ring)
45 776 γ C–H(Ph–ring)
46 763 υsy C–C(Ph–ring) + ω C–H (CH2Cl)
47 757 ρ C–H(Ph–ring) + τ C–H (CH3)
48 744 ρ C–H(Ph–ring) + τ C–H (CH3)
49 709
50 694
51 648 sciss C–H (CH2Cl)
52 613
53 582 ω C–H (CH3)
54 550
55 530
56 510 τ C–H(Ph–ring)
57 456 τ C–H(Ph–ring)
58 444
59 401 τ C–H(Ph–ring)
60 380
61 319
62 307
63 255
64 238
65 192
66 180
67 153
68 134 ω C–H (CH3)
69 127 ρ C–H (CH3)
70 106 τ C–H (CH3)
71 77
72 73
73 47
74 25 ω C–Cl
75 15

υ:stretching; υsy. Symmetric stretching; υas: asymmetric stretching; β: in-plane bending; γ: out of plane bending; ρ: rocking; ω: wagging and τ: twisting.

4.2.1

4.2.1 C–H Vibrations

The hetero-aromatic structure shows the presence of C–H stretching vibration in the region 3100–3000 cm−1, which is the characteristic region for the identification of C–H stretching vibration (Rastogi et al., 2002). In this region, the bands are not affected appreciably by the nature of the substituents. The 2f molecule consists of four adjacent C–H benzene ring systems, CH3 and CH2. The FTIR bands observed at 3062, 3019 and 2967 cm−1 are assigned to C–H stretching vibration. The scaled vibration (mode numbers, 1–11) that has been predicted at 3085–2932 cm−1 shows very good agreement with the recorded spectral data. The in-plane aromatic C–H bending vibration occurs in the region 1300–1000 cm−1, the bands are sharp but have weak-to-medium intensity. The C–H in-plane bending vibration computed at 1293, 1287, 1281, 1265, 1258, 1216, 1173, 1161, 1146 and 1130 cm−1 shows excellent agreement with FTIR bands at 1317, 1259 and 1232 cm−1. The bands observed at 1042, 990, 944, 932, 862 and 790 cm−1 are assigned to C–H out-of-plane bending vibration for 2f. This also shows good agreement with theoretically scaled harmonic wave number values at 1035, 1033, 979, 972, 949, 921, 908,903, 867, 845, 776 and 763 cm−1.

4.2.2

4.2.2 C=O Vibrations

The strong absorption band due to the C = O stretching vibration has been observed in the region 1850–1550 cm−1 (Engasser and Horvath, 1975). If a carbonyl group is part of a conjugated system, then the wave number of the carbonyl stretching vibration decreases, the reason being that the double bond character of the C = O group is less due to the p-electron conjugation being localized. The νC = O mode has been seen as a strong band at 1734 and 1715 cm−1 in the FTIR spectrum. The same mode has been observed at 1745 and 1709 cm−1 by DFT calculations which are also in good agreement with the experimental data.

4.2.3

4.2.3 C–C Vibrations

The ring C–C stretching vibrations occur in the region 1625–1430 cm−1. In general, the bands are of variable intensity and were observed at 1625–1590, 1590–1575, 1540–1470, 1465–1430 and 1380–1280 cm−1 from the wave number ranges for the five bands in the region (Engasser and Horvath, 1975). In the present work, the wave numbers observed in the FTIR spectrum at 1583 and 1490 cm−1 have been assigned to C–C stretching vibrations. The computed values at 1593, 1568, 1477 and 1464 cm−1 showed an excellent agreement with experimental data (Mode nos.14–17).

4.2.4

4.2.4 N–C vibrations

Strong bands can be observed at 1387 and 1317 cm−1 of the studied compound, in the FTIR spectrum. Taking into account the vibrational properties reported previously (Srinivasan et al., 2010), it is expected that the C–N stretching modes, which are usually coupled in symmetric and antisymmetric motions, appear in this region (Kolodziejski et al., 1993). The computed value at the B3LYP/6–31G∗ level of theory has been observed at 1392 and 1382 cm−1 and corresponds to the most intense absorption which is in good agreement with the experimental evidence.

5

5 Conclusions

N-acetyl-N-(2-methoxyphenyl)acetamide, N-acetyl-N-(2-Methoxy-phenyl)-4-nitro-benzamide, N-(4-nitrobenzamide)-N-(2-Methoxy-phenyl)-4-bromo-benzamide, N-Acetyl-4-nitro-N-o-tolyl-benzamide, N-Acetyl-N-o-tolyl-acetamide, and 2-Chloro-N-(2-chloro-acetyl)-N-o-tolyl-acetamide have been synthesized and characterized. The DFT calculations showed that the amide and aryl planes were roughly perpendicular to one another. The FTIR bands observed at 3062, 3019 and 2967 cm−1 were assigned to C-H stretching vibration. The scaled vibration at B3LYP/6–31G∗ level of theory has been predicted at 3085–2932 cm−1 which is in very good agreement with the recorded spectral data. The νC = O mode has been seen as a strong band at 1734 and 1715 cm−1 in the FTIR spectrum. The DFT calculations give this mode at 1745 and 1709 cm−1. The wave numbers observed in the FTIR spectrum at 1583 and 1490 cm−1 have been assigned to C–C stretching vibrations. The computed values at 1593, 1568, 1477 and 1464 cm−1 showed an excellent agreement with experimental data. Strong bands can be observed at 1387 and 1317 cm−1 for N–C vibrations of the studied compound in the FTIR spectrum. The computed value has been observed at 1392 and 1382 cm−1 and corresponds to the most intense absorption.

Acknowledgement

We thank King Abdul Aziz city of Science and technology (KACST) for their financial support to Reem Saied Abdulaziz Muhammad Al-Yabess Al-Amri by the grant No. GSP-18-138.

References

  1. , , , , , , . Indian J. Pharm. Sci.. 2006;68:532.
  2. Al-Sehemi, A.G., Irfan, A., 2017. Arabian J. Chem. 10, S1703–S1710.
  3. , , , . Theor. Chem. Acc.. 2012;131:1199.
  4. , , , , . J. Mol. Struc.. 2012;1019:130.
  5. , , , , . Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy. 2012;91:239.
  6. , , , . Acta Phys. Chim. Sin.. 2013;29:55.
  7. Al-Sehemi, A.G., Al-Amri, R.S.A., Irfan, A., 2013. J. Chem. Soc. Pak. (in press).
  8. , , , . Struc. Chem.. 2013;24:499.
  9. , , , . J. Mol. Struc.. 2013;1018:171.
  10. , , , . Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy. 2013;111:223.
  11. , , , , , , , . Org. Biomol. Chem.. 2004;2:2426.
    [Google Scholar]
  12. , , , . Arch. Pharm.. 2004;337:527.
  13. , . J. Chem. Phys.. 1993;98:5648.
  14. , , , , , , , . Pharmacologyonline. 2008;2:604.
  15. , , , . J. Org. Chem.. 1996;61:3452.
  16. , . Spectro. lett.. 1999;32:671.
  17. , , . Biochem. J.. 1975;45:43158.
  18. , . Gaussian 09 Revision A.1. Wallingford, CT.: Gaussian, Inc.; .
  19. , , , , , , , , . Science. 1994;265:1093.
  20. , , , , . Indian J. Chem.. 1988;27:1060.
  21. , . J. Am. Chem. Soc.. 1996;118:10269.
  22. Irfan, A., Al-Sehemi, A.G. 2011. J. Saudi Chem. Soc. <http://dx.doi.org/10.1016/j.jscs.2011.11.006>.
  23. Irfan, A., Al-Sehemi, A.G. 2011. J. Saudi Chem. Soc. <http://dx.doi.org/10.1016/j.jscs.2012.03.005>.
  24. , , . J. Mol. Model.. 2012;18:4893.
  25. , , , . J. Mol. Struc. (TheoChem). 2008;850:79.
  26. , , , . Chem. Phys.. 2009;358:25.
  27. , , , . Chem. Phys. Lett.. 2009;483:143.
  28. , , , . J. Mol. Struc. (TheoChem). 2010;956:61.
  29. , , , , . Australian J. Chem.. 2010;63:1283.
  30. , , , . Theor. Chem. Acc.. 2010;127:587.
  31. Irfan, A., Aftab, H., Al-Sehemi, A.G. J. Saudi Chem. Soc. 2011, <http://dx.doi.org/10.1016/j.jscs.2011.11.013>.
  32. , , , , , . Comput. Theor. Chem.. 2011;977:9.
    [Google Scholar]
  33. , , , , . Australian J. Chem.. 2011;64:1587.
  34. , , , . Theor. Comp. Chem.. 2012;11:631.
  35. , , , . J. Mol. Model.. 2012;18:3609.
  36. , , , , . J. Mol. Model.. 2012;18:4199.
  37. , , , , . Comput. Electron.. 2012;11:374.
  38. Irfan, A., Al-Sehemi, A.G., Al-Assiri, M.S. 2013. J. Mol. Graphics and Model. <http://dx.doi.org/10.1016/j.jmgm.2013.06.003>.
  39. Irfan, A., Al-Sehemi, A.G., Kalam, A. 2013. J. Mol. Struc. <http://dx.doi.org/10.1016/j.molstruc.2013.06.023>.
  40. , , , . Asiri. Spectrochimica Acta Part A: Mol. Biomol. Spect.. 2013;110:60.
    [Google Scholar]
  41. , , , , . Eur. J. Med. Chem.. 2008;43:135.
  42. , , . Indian J. Chem.. 1987;26:602.
  43. , , , , . J. Phys. Chem. A. 1993;97:12147.
  44. , , , , . Tetrahedron Lett.. 1999;40:5577.
  45. , , , . Phys. Rev. B. 1988;37:785.
  46. , , , , . Chem. Phys. Lett.. 1989;157:200.
  47. , , , , , , , . J. Raman Spect.. 2009;40:1262.
  48. , , , , , , , , , , . J. Med. Chem.. 1993;36:2279.
  49. , . Drugs Future. 1993;18:475.
  50. , , , , . Spectrochim Acta, A. 2002;58:1989.
  51. , , , , , , . Spectrochimica, Acta Part A. 2010;76:182.
  52. , , , . Spectrochim. Acta A. 2010;75:1171.
  53. , , , , . J. Chem. Phys.. 2007;127:234107.
  54. , , , , , . J. Am. Chem. Soc.. 1997;119:6315.
  55. , , , , , , . J. Med. Chem.. 1996;39:2285.
  56. , . Tetrahedron Lett.. 1992;33:2171.
  57. , . J. Org. Chem.. 1992;57:1591.
  58. , . Angew Chem. Int. Ed.. 1995;34:1113.
  59. , , . Tetrahedron Lett.. 1996;37:6777.
  60. , , , . J. Org. Chem.. 1996;61:5996.

Appendix A

Supplementary data

Supplementary data associated with this article can be found, in the online version, at http://dx.doi.org/10.1016/j.arabjc.2013.07.011.

Appendix A

Supplementary data

Supplementary data 1

Supplementary data 1 Supplementary material.

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