organic compounds
4-Acetamidoanilinium nitrate monohydrate
aLaboratoire de Chimie des Matériaux, Faculté des Sciences de Bizerte, 7021 Zarzouna, Tunisia, bDipartimento di Chimica and Centro di Strutturistica Diffrattometrica, University of Ferrara, via L. Borsari 46, I-44121 Ferrara, Italy, and cLaboratoire de Chimie Organometallique de Surface, 43 Bd du 11 Novembre 1918, 69616 Villeurbanne Cedex, France
*Correspondence e-mail: cherif_bennasr@yahoo.fr
In the title hydrated salt, C8H11N2O+·NO3−·H2O, the N—C bond distances [1.349 (2) and 1.413 (2) Å] along with the sum of the angles (359.88°) around the acetamide N atom clearly indicate that the heteroatom has an sp2 character. The ammonium group is involved in a total of three N—H⋯O hydrogen bonds, two of these are with a water molecule, which forms two O—H⋯O hydrogen bonds. All these hydrogen bonds link the ionic units and the water molecule into infinite planar layers parallel to (100). The remaining two N—H⋯O interactions in which the ammoniun group is involved link these layers into an infinite three-dimensional network.
Related literature
For the structural diversity of amine salts, see: Tooke et al. (2004). For related nitrate compounds, see: Dai & Chen (2011); Pourayoubi et al. (2011); Berrah et al. (2011). For hydrogen-bond patterns in related compounds, see: Flores-Alamo et al. (2010). For details of graph-set theory, see: Bernstein et al. (1995).
Experimental
Crystal data
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Data collection
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Refinement
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Data collection: COLLECT (Nonius, 1997); cell DENZO-SMN (Otwinowski & Minor, 1997); data reduction: DENZO-SMN; program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEPIII (Burnett & Johnson, 1996); software used to prepare material for publication: SHELXL97 and WinGX (Farrugia, 1999).
Supporting information
10.1107/S1600536812019393/lr2060sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536812019393/lr2060Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536812019393/lr2060Isup3.cml
Commercial 4-acetamidobenzenamine (3 mmol) was dissolved in water/HNO3 (50:1 v/v) solution. Colorless single crystals of the title compound, suitable for X-ray analysis, were obtained after slowly evaporation of the solvent at room temperature.
All H atoms were located in successive difference Fourier maps and refined riding on its parents atoms with Uiso=1.2 and 1.5Ueq(parent atom).
Data collection: COLLECT (Nonius, 1997); cell
DENZO-SMN (Otwinowski & Minor, 1997); data reduction: DENZO-SMN (Otwinowski & Minor, 1997); program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEPIII (Burnett & Johnson, 1996); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008) and WinGX (Farrugia, 1999).Fig. 1. A view of (I) showing 50% probability displacement ellipsoids. | |
Fig. 2. A view, down the a axis, showing a layer of the structure. The hydrogen bonding transforming the layers in a three-dimenional network has been omitted for clarity. |
C8H11N2O+·NO3−·H2O | F(000) = 488 |
Mr = 231.21 | Dx = 1.413 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 4741 reflections |
a = 4.1059 (1) Å | θ = 3.0–28.0° |
b = 23.1112 (5) Å | µ = 0.12 mm−1 |
c = 11.4702 (3) Å | T = 295 K |
β = 92.942 (1)° | Prismatic, pale yellow |
V = 1087.00 (5) Å3 | 0.41 × 0.32 × 0.25 mm |
Z = 4 |
Nonius KappaCCD diffractometer | 1885 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.022 |
Graphite monochromator | θmax = 28.0°, θmin = 3.7° |
ϕ scans and ω scans | h = −5→5 |
4741 measured reflections | k = −30→27 |
2606 independent reflections | l = −15→15 |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.046 | Hydrogen site location: difference Fourier map |
wR(F2) = 0.142 | All H-atom parameters refined |
S = 1.06 | w = 1/[σ2(Fo2) + (0.0773P)2 + 0.1041P] where P = (Fo2 + 2Fc2)/3 |
2606 reflections | (Δ/σ)max < 0.001 |
197 parameters | Δρmax = 0.24 e Å−3 |
0 restraints | Δρmin = −0.19 e Å−3 |
C8H11N2O+·NO3−·H2O | V = 1087.00 (5) Å3 |
Mr = 231.21 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 4.1059 (1) Å | µ = 0.12 mm−1 |
b = 23.1112 (5) Å | T = 295 K |
c = 11.4702 (3) Å | 0.41 × 0.32 × 0.25 mm |
β = 92.942 (1)° |
Nonius KappaCCD diffractometer | 1885 reflections with I > 2σ(I) |
4741 measured reflections | Rint = 0.022 |
2606 independent reflections |
R[F2 > 2σ(F2)] = 0.046 | 0 restraints |
wR(F2) = 0.142 | All H-atom parameters refined |
S = 1.06 | Δρmax = 0.24 e Å−3 |
2606 reflections | Δρmin = −0.19 e Å−3 |
197 parameters |
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. |
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. |
x | y | z | Uiso*/Ueq | ||
O1 | 0.1624 (3) | 0.11922 (5) | 0.45863 (11) | 0.0662 (4) | |
O2 | 0.6017 (4) | 0.36949 (6) | 0.53827 (14) | 0.0878 (5) | |
O3 | 0.3474 (5) | 0.30471 (6) | 0.63123 (12) | 0.0866 (5) | |
O4 | 0.3293 (4) | 0.30565 (6) | 0.44397 (12) | 0.0766 (4) | |
O1W | 0.2790 (3) | 0.18436 (6) | 0.65055 (11) | 0.0570 (3) | |
N1 | −0.0860 (3) | 0.09798 (5) | 0.28298 (12) | 0.0500 (3) | |
N2 | 0.2062 (4) | −0.13752 (6) | 0.21089 (16) | 0.0543 (4) | |
N3 | 0.4244 (3) | 0.32626 (5) | 0.53870 (12) | 0.0515 (3) | |
C1 | 0.0001 (3) | 0.03922 (6) | 0.27013 (12) | 0.0431 (3) | |
C2 | 0.1814 (4) | 0.00752 (7) | 0.35317 (14) | 0.0515 (4) | |
C3 | 0.2493 (4) | −0.05022 (7) | 0.33325 (15) | 0.0518 (4) | |
C4 | 0.1367 (3) | −0.07607 (6) | 0.23129 (13) | 0.0447 (3) | |
C5 | −0.0431 (4) | −0.04540 (7) | 0.14791 (15) | 0.0524 (4) | |
C6 | −0.1123 (4) | 0.01213 (7) | 0.16734 (14) | 0.0519 (4) | |
C7 | −0.0072 (4) | 0.13406 (6) | 0.37245 (13) | 0.0480 (4) | |
C8 | −0.1396 (5) | 0.19416 (8) | 0.3608 (2) | 0.0621 (5) | |
H1 | 0.259 (4) | 0.0238 (8) | 0.4267 (17) | 0.061 (5)* | |
H2 | 0.369 (5) | −0.0731 (9) | 0.3872 (18) | 0.065 (5)* | |
H3 | −0.205 (5) | 0.1131 (9) | 0.2208 (18) | 0.060 (5)* | |
H4 | 0.374 (5) | −0.1507 (9) | 0.2619 (18) | 0.067 (5)* | |
H5 | 0.243 (6) | −0.1417 (13) | 0.135 (3) | 0.103 (9)* | |
H6 | 0.040 (6) | −0.1603 (12) | 0.239 (2) | 0.095 (8)* | |
H7 | −0.229 (4) | 0.0345 (9) | 0.1086 (19) | 0.065 (5)* | |
H8 | −0.123 (5) | −0.0614 (9) | 0.0796 (18) | 0.064 (5)* | |
H9 | −0.251 (9) | 0.2023 (17) | 0.290 (4) | 0.141 (12)* | |
H10 | 0.017 (8) | 0.2231 (14) | 0.371 (3) | 0.115 (9)* | |
H11 | −0.272 (8) | 0.2008 (15) | 0.415 (3) | 0.124 (11)* | |
H1W | 0.219 (6) | 0.1691 (11) | 0.578 (2) | 0.087 (7)* | |
H2W | 0.288 (6) | 0.2175 (13) | 0.639 (2) | 0.088 (8)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0952 (9) | 0.0479 (7) | 0.0534 (7) | 0.0049 (6) | −0.0168 (6) | −0.0067 (5) |
O2 | 0.1177 (12) | 0.0606 (8) | 0.0825 (10) | −0.0398 (8) | −0.0211 (8) | 0.0080 (7) |
O3 | 0.1328 (13) | 0.0705 (9) | 0.0578 (8) | −0.0060 (8) | 0.0158 (8) | 0.0140 (7) |
O4 | 0.0939 (10) | 0.0746 (9) | 0.0600 (8) | −0.0196 (7) | −0.0086 (7) | −0.0111 (6) |
O1W | 0.0760 (8) | 0.0460 (7) | 0.0485 (7) | −0.0006 (5) | −0.0023 (5) | 0.0004 (5) |
N1 | 0.0605 (7) | 0.0410 (7) | 0.0475 (7) | 0.0017 (5) | −0.0055 (6) | −0.0018 (5) |
N2 | 0.0544 (8) | 0.0424 (7) | 0.0662 (10) | 0.0028 (6) | 0.0025 (7) | −0.0084 (6) |
N3 | 0.0673 (8) | 0.0381 (6) | 0.0479 (7) | −0.0029 (5) | −0.0074 (6) | 0.0047 (5) |
C1 | 0.0473 (7) | 0.0393 (7) | 0.0428 (7) | −0.0037 (5) | 0.0037 (6) | −0.0003 (6) |
C2 | 0.0631 (9) | 0.0466 (8) | 0.0438 (8) | 0.0018 (7) | −0.0059 (7) | −0.0036 (6) |
C3 | 0.0599 (9) | 0.0475 (8) | 0.0472 (8) | 0.0040 (7) | −0.0039 (7) | 0.0018 (7) |
C4 | 0.0451 (7) | 0.0393 (7) | 0.0505 (8) | −0.0025 (5) | 0.0082 (6) | −0.0028 (6) |
C5 | 0.0603 (9) | 0.0493 (8) | 0.0469 (9) | −0.0030 (7) | −0.0046 (7) | −0.0075 (7) |
C6 | 0.0619 (9) | 0.0460 (8) | 0.0467 (8) | 0.0008 (7) | −0.0074 (7) | 0.0005 (7) |
C7 | 0.0531 (8) | 0.0422 (8) | 0.0487 (8) | −0.0052 (6) | 0.0022 (6) | −0.0018 (6) |
C8 | 0.0674 (11) | 0.0448 (9) | 0.0731 (13) | 0.0038 (8) | −0.0067 (10) | −0.0086 (8) |
O1—C7 | 1.2286 (19) | C1—C6 | 1.393 (2) |
O2—N3 | 1.2363 (18) | C2—C3 | 1.385 (2) |
O3—N3 | 1.2284 (19) | C2—H1 | 0.96 (2) |
O4—N3 | 1.2314 (18) | C3—C4 | 1.372 (2) |
O1W—H1W | 0.93 (3) | C3—H2 | 0.93 (2) |
O1W—H2W | 0.78 (3) | C4—C5 | 1.375 (2) |
N1—C7 | 1.349 (2) | C5—C6 | 1.380 (2) |
N1—C1 | 1.4129 (19) | C5—H8 | 0.91 (2) |
N1—H3 | 0.91 (2) | C6—H7 | 0.96 (2) |
N2—C4 | 1.4698 (19) | C7—C8 | 1.495 (2) |
N2—H4 | 0.93 (2) | C8—H9 | 0.93 (4) |
N2—H5 | 0.89 (3) | C8—H10 | 0.93 (3) |
N2—H6 | 0.93 (3) | C8—H11 | 0.86 (4) |
C1—C2 | 1.387 (2) | ||
H1W—O1W—H2W | 103 (2) | C4—C3—H2 | 117.5 (13) |
C7—N1—C1 | 128.48 (14) | C2—C3—H2 | 122.6 (13) |
C7—N1—H3 | 117.0 (12) | C3—C4—C5 | 120.93 (14) |
C1—N1—H3 | 114.4 (12) | C3—C4—N2 | 119.78 (14) |
C4—N2—H4 | 111.1 (13) | C5—C4—N2 | 119.29 (14) |
C4—N2—H5 | 107.7 (19) | C4—C5—C6 | 119.47 (15) |
H4—N2—H5 | 115 (2) | C4—C5—H8 | 123.0 (13) |
C4—N2—H6 | 109.9 (16) | C6—C5—H8 | 117.5 (13) |
H4—N2—H6 | 97.5 (19) | C5—C6—C1 | 120.52 (15) |
H5—N2—H6 | 116 (2) | C5—C6—H7 | 120.4 (12) |
O3—N3—O4 | 121.44 (15) | C1—C6—H7 | 119.0 (12) |
O3—N3—O2 | 120.58 (15) | O1—C7—N1 | 122.92 (14) |
O4—N3—O2 | 117.98 (14) | O1—C7—C8 | 121.34 (15) |
C2—C1—C6 | 119.12 (14) | N1—C7—C8 | 115.75 (15) |
C2—C1—N1 | 124.34 (14) | C7—C8—H9 | 115 (2) |
C6—C1—N1 | 116.53 (13) | C7—C8—H10 | 114.1 (18) |
C3—C2—C1 | 120.07 (15) | H9—C8—H10 | 106 (3) |
C3—C2—H1 | 117.5 (11) | C7—C8—H11 | 110 (2) |
C1—C2—H1 | 122.4 (11) | H9—C8—H11 | 107 (3) |
C4—C3—C2 | 119.89 (15) | H10—C8—H11 | 104 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
O1W—H1W···O1 | 0.93 (3) | 1.79 (3) | 2.689 (2) | 161 (3) |
O1W—H2W···O3 | 0.78 (3) | 2.03 (3) | 2.805 (2) | 172 (3) |
N1—H3···O2i | 0.91 (2) | 2.24 (2) | 3.117 (2) | 161 (2) |
N2—H4···O1Wii | 0.93 (2) | 1.87 (2) | 2.796 (2) | 173 (2) |
N2—H5···O2iii | 0.89 (3) | 2.14 (3) | 3.008 (2) | 165 (3) |
N2—H6···O1Wiv | 0.93 (3) | 1.95 (2) | 2.827 (2) | 156 (2) |
Symmetry codes: (i) x−1, −y+1/2, z−1/2; (ii) −x+1, −y, −z+1; (iii) −x+1, y−1/2, −z+1/2; (iv) −x, −y, −z+1. |
Experimental details
Crystal data | |
Chemical formula | C8H11N2O+·NO3−·H2O |
Mr | 231.21 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 295 |
a, b, c (Å) | 4.1059 (1), 23.1112 (5), 11.4702 (3) |
β (°) | 92.942 (1) |
V (Å3) | 1087.00 (5) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.12 |
Crystal size (mm) | 0.41 × 0.32 × 0.25 |
Data collection | |
Diffractometer | Nonius KappaCCD diffractometer |
Absorption correction | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 4741, 2606, 1885 |
Rint | 0.022 |
(sin θ/λ)max (Å−1) | 0.661 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.046, 0.142, 1.06 |
No. of reflections | 2606 |
No. of parameters | 197 |
H-atom treatment | All H-atom parameters refined |
Δρmax, Δρmin (e Å−3) | 0.24, −0.19 |
Computer programs: COLLECT (Nonius, 1997), DENZO-SMN (Otwinowski & Minor, 1997), SIR97 (Altomare et al., 1999), ORTEPIII (Burnett & Johnson, 1996), SHELXL97 (Sheldrick, 2008) and WinGX (Farrugia, 1999).
D—H···A | D—H | H···A | D···A | D—H···A |
O1W—H1W···O1 | 0.93 (3) | 1.79 (3) | 2.689 (2) | 161 (3) |
O1W—H2W···O3 | 0.78 (3) | 2.03 (3) | 2.805 (2) | 172 (3) |
N1—H3···O2i | 0.91 (2) | 2.24 (2) | 3.117 (2) | 161 (2) |
N2—H4···O1Wii | 0.93 (2) | 1.87 (2) | 2.796 (2) | 173 (2) |
N2—H5···O2iii | 0.89 (3) | 2.14 (3) | 3.008 (2) | 165 (3) |
N2—H6···O1Wiv | 0.93 (3) | 1.95 (2) | 2.827 (2) | 156 (2) |
Symmetry codes: (i) x−1, −y+1/2, z−1/2; (ii) −x+1, −y, −z+1; (iii) −x+1, y−1/2, −z+1/2; (iv) −x, −y, −z+1. |
Acknowledgements
We would like to acknowledge the support provided by the Secretary of State for Scientific Research and Technology of Tunisia.
References
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Salts of amine show interesting structural diversity governed mainly by hydrogen bonds (Tooke et al., 2004), whose crystal pattern seems to be strongly influenced by the nature of the anion (Flores-Alamo et al., 2010). We report here the crystal structure of one such compound, 4-acetamidoanilinium nitrate monohydrate, (I), formed from the reaction of 4-acetamidoaniline and nitric acid. The asymmetric unit of the title salt, shown in Fig. 1, contains one protonated 4-acetamidoanilinium cation, one nitrate anion and one water molecule. The NO3- anion geometry agrees with that observed in similar compounds (Dai & Chen, 2011; Pourayoubi et al., 2011; Berrah et al., 2011). In the organic cation the bond length distance N1—C7 = 1.349 (2) Å and the sum of the angles around N1 atoms = 359.88 ° clearly indicate that the heteroatom N1 has a sp2 character. The N2 nitrogen atom is involved in a positive charge-assisted N—H···O hydrogen bond with a neighboring water molecule (N2···O1w = 2.796 (2) Å). Moreover, the water molecule forms two O—H···O interactions (O1W···O1 = 2.689 (2) Å and O1W···O3 = 2.805 (2) Å) with, respectively, the O1 oxygen atom belonging to the carbonyl group and the O3 atom of the adjacent NO3- anion. The weak hydrogen bond N1—H3···O2 (N1···O2 = 3.117 (2) Å) contributes to the robustness of the crystal architecture but it is not influencing the overall crystal packing pattern (Table 1, Fig. 2). Within the structure, the graph-set motif (Bernstein et al., 1995) R44(22) is formed by two cations and two water molecules, which in turn link cations and anions to form infinite planar layers parallel to (1 0 0) (Fig. 2). These layers are interconnected via further hydrogen bonds to form a three dimensional network.