Abstract
The asymmetric unit of the title salt, C7H9N2O2 +·Cl−, contains two independent cations and anions. In the crystal, each N-methyl-4-nitroanilinium cation is linked to two Cl− anions via N—H⋯Cl hydrogen bonds. π–π stacking is observed between the benzene rings of adjacent cations [centroid-to-centroid distances = 3.7684 (14) and 3.7917 (7) Å].
Related literature
For applications of N-methyl-4-nitrobenzenamine, see: Bellamy & Sammour (1993 ▶); Sammour (1994 ▶); Williams & Friedlander (2000 ▶); Davies & Provatas (2006 ▶).
Experimental
Crystal data
C7H9N2O2 +·Cl−
M r = 188.61
Monoclinic,
a = 7.0509 (14) Å
b = 19.120 (4) Å
c = 13.443 (3) Å
β = 95.20 (3)°
V = 1804.8 (6) Å3
Z = 8
Mo Kα radiation
μ = 0.39 mm−1
T = 293 K
0.20 × 0.20 × 0.12 mm
Data collection
Rigaku Saturn diffractometer
Absorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T min = 0.927, T max = 0.955
17869 measured reflections
4282 independent reflections
3022 reflections with I > 2σ(I)
R int = 0.051
Refinement
R[F 2 > 2σ(F 2)] = 0.046
wR(F 2) = 0.124
S = 1.03
4282 reflections
236 parameters
4 restraints
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.24 e Å−3
Δρmin = −0.27 e Å−3
Data collection: RAPID-AUTO (Rigaku, 2000 ▶); cell refinement: RAPID-AUTO; data reduction: CrystalStructure (Rigaku/MSC, 2000 ▶); program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812024117/xu5532sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812024117/xu5532Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812024117/xu5532Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N2—H2A⋯Cl2i | 0.90 (1) | 2.18 (1) | 3.0702 (17) | 170 (2) |
| N2—H2B⋯Cl1i | 0.89 (1) | 2.16 (1) | 3.0482 (19) | 173 (2) |
| N4—H4A⋯Cl2ii | 0.90 (1) | 2.15 (1) | 3.0361 (18) | 168 (2) |
| N4—H4B⋯Cl1 | 0.89 (1) | 2.26 (1) | 3.1157 (18) | 163 (2) |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
The authors thank China North Industries Group Corporation for financial support.
supplementary crystallographic information
Comment
As a stablizer, N-methyl-4-nitrobenzenamine is used in order to lengthen the useful service life of double-base and minimum smoke propellants (Bellamy & Sammour, 1993; Sammour, 1994; Williams & Friedlander, 2000). As a important ingredient, N-methyl-4-nitrobenzenamine can improve melt-cast explosive systems mechanical properties (Davies & Provatas, 2006). In order to research reaction properties, here we report the synthesis and the crystal structure of the title compound (Fig. 1).
The title compound consists of a N-(4-nitrophenyl)-methylammonium cation and a chloride anion. The hydrochloric acid deprotonated and the N-methyl-4-nitrobenzenamine accepts the proton to produce the protonated organic cation, namely N-(4-nitrophenyl)-methylammonium chloride. In the crystal structure, contains two cations and two anions. They are linked by N—H···Cl hydrogen bonds to form a three-dimensional complex network.
Experimental
The title compound was synthesized by N-methyl-4-nitrobenzenamine and concentrated hydrochloric acid in acetone at room temperature. Single crystals suitable for X-ray diffraction were obtained by evaporation of a solution of the title compound in acetone at room temperature.
Refinement
H atoms bonded to N atoms were located in a difference Fourier map and refined isotropically with bond restraint of N—H = 0.89 (2) Å. Other H atoms were positioned geometrically and treated as riding with C—H = 0.93–0.96 Å, and refined as riding with Uiso(H) = 1.2–1.5Ueq(C).
Figures
Fig. 1.
The molecular structure of the title compound.
Fig. 2.
The packing of the title compound.
Crystal data
| C7H9N2O2+·Cl− | F(000) = 784 |
| Mr = 188.61 | Dx = 1.388 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 4042 reflections |
| a = 7.0509 (14) Å | θ = 2.6–27.9° |
| b = 19.120 (4) Å | µ = 0.39 mm−1 |
| c = 13.443 (3) Å | T = 293 K |
| β = 95.20 (3)° | Block, yellow |
| V = 1804.8 (6) Å3 | 0.20 × 0.20 × 0.12 mm |
| Z = 8 |
Data collection
| Rigaku Saturn diffractometer | 4282 independent reflections |
| Radiation source: rotating anode | 3022 reflections with I > 2σ(I) |
| Multilayer monochromator | Rint = 0.051 |
| Detector resolution: 7.31 pixels mm-1 | θmax = 27.9°, θmin = 2.6° |
| ω scans | h = −9→9 |
| Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | k = −25→25 |
| Tmin = 0.927, Tmax = 0.955 | l = −17→12 |
| 17869 measured reflections |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.046 | H atoms treated by a mixture of independent and constrained refinement |
| wR(F2) = 0.124 | w = 1/[σ2(Fo2) + (0.0651P)2] where P = (Fo2 + 2Fc2)/3 |
| S = 1.03 | (Δ/σ)max = 0.001 |
| 4282 reflections | Δρmax = 0.24 e Å−3 |
| 236 parameters | Δρmin = −0.27 e Å−3 |
| 4 restraints | Extinction correction: SHELXTL (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.073 (4) |
Special details
| 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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | ||
| O1 | 0.5920 (3) | 0.47358 (8) | 0.82213 (13) | 0.0978 (7) | |
| O2 | 0.6814 (3) | 0.46456 (9) | 0.97433 (15) | 0.1113 (9) | |
| O3 | 0.2318 (3) | 0.28345 (10) | 1.09445 (12) | 0.0814 (6) | |
| O4 | 0.1062 (3) | 0.20296 (9) | 0.99778 (13) | 0.0869 (6) | |
| N1 | 0.6303 (3) | 0.43952 (9) | 0.89526 (14) | 0.0532 (5) | |
| N2 | 0.5910 (2) | 0.14490 (8) | 0.86838 (12) | 0.0408 (4) | |
| N3 | 0.1557 (2) | 0.26321 (10) | 1.01448 (14) | 0.0542 (5) | |
| N4 | 0.0461 (2) | 0.45901 (8) | 0.70054 (11) | 0.0400 (4) | |
| C1 | 0.5619 (3) | 0.26091 (10) | 0.79113 (13) | 0.0405 (4) | |
| H1 | 0.5343 | 0.2393 | 0.7295 | 0.049* | |
| C2 | 0.5707 (3) | 0.33269 (10) | 0.79740 (13) | 0.0414 (4) | |
| H2 | 0.5485 | 0.3603 | 0.7406 | 0.050* | |
| C3 | 0.6131 (2) | 0.36260 (9) | 0.88971 (14) | 0.0394 (4) | |
| C4 | 0.6468 (3) | 0.32360 (10) | 0.97592 (14) | 0.0442 (5) | |
| H4 | 0.6757 | 0.3453 | 1.0374 | 0.053* | |
| C5 | 0.6365 (3) | 0.25178 (10) | 0.96866 (13) | 0.0416 (4) | |
| H5 | 0.6580 | 0.2242 | 1.0256 | 0.050* | |
| C6 | 0.5942 (2) | 0.22099 (9) | 0.87655 (12) | 0.0351 (4) | |
| C7 | 0.4023 (3) | 0.11454 (11) | 0.83074 (18) | 0.0602 (6) | |
| H7A | 0.3053 | 0.1324 | 0.8696 | 0.090* | |
| H7B | 0.4074 | 0.0645 | 0.8365 | 0.090* | |
| H7C | 0.3732 | 0.1272 | 0.7620 | 0.090* | |
| C8 | 0.0468 (3) | 0.33800 (9) | 0.76075 (13) | 0.0388 (4) | |
| H8 | 0.0125 | 0.3233 | 0.6956 | 0.047* | |
| C9 | 0.0732 (3) | 0.28977 (9) | 0.83732 (14) | 0.0411 (4) | |
| H9 | 0.0568 | 0.2422 | 0.8251 | 0.049* | |
| C10 | 0.1243 (3) | 0.31429 (10) | 0.93243 (13) | 0.0402 (4) | |
| C11 | 0.1482 (3) | 0.38398 (10) | 0.95434 (14) | 0.0474 (5) | |
| H11 | 0.1817 | 0.3987 | 1.0195 | 0.057* | |
| C12 | 0.1211 (3) | 0.43201 (10) | 0.87722 (13) | 0.0423 (4) | |
| H12 | 0.1360 | 0.4796 | 0.8898 | 0.051* | |
| C13 | 0.0720 (2) | 0.40829 (9) | 0.78202 (12) | 0.0347 (4) | |
| C14 | 0.1958 (3) | 0.45515 (11) | 0.62862 (15) | 0.0557 (6) | |
| H14A | 0.3184 | 0.4640 | 0.6634 | 0.084* | |
| H14B | 0.1701 | 0.4896 | 0.5772 | 0.084* | |
| H14C | 0.1948 | 0.4094 | 0.5991 | 0.084* | |
| Cl1 | 0.10531 (8) | 0.61298 (3) | 0.77271 (4) | 0.05256 (19) | |
| Cl2 | 0.31979 (7) | 0.57619 (3) | 0.42629 (3) | 0.04808 (18) | |
| H2A | 0.632 (3) | 0.1249 (11) | 0.9271 (10) | 0.062 (7)* | |
| H2B | 0.684 (2) | 0.1328 (12) | 0.8311 (15) | 0.075 (8)* | |
| H4A | −0.0708 (18) | 0.4519 (12) | 0.6697 (15) | 0.068 (7)* | |
| H4B | 0.041 (3) | 0.5011 (7) | 0.7277 (15) | 0.064 (7)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.187 (2) | 0.0365 (10) | 0.0681 (12) | −0.0036 (11) | 0.0040 (12) | 0.0119 (8) |
| O2 | 0.181 (2) | 0.0497 (11) | 0.0926 (13) | −0.0070 (12) | −0.0467 (15) | −0.0217 (10) |
| O3 | 0.1046 (14) | 0.0890 (14) | 0.0489 (10) | 0.0101 (11) | −0.0028 (9) | 0.0215 (9) |
| O4 | 0.1261 (17) | 0.0515 (11) | 0.0827 (12) | 0.0016 (10) | 0.0070 (11) | 0.0284 (9) |
| N1 | 0.0590 (11) | 0.0368 (10) | 0.0633 (12) | −0.0019 (8) | 0.0029 (9) | −0.0075 (9) |
| N2 | 0.0475 (10) | 0.0353 (9) | 0.0395 (9) | 0.0044 (7) | 0.0038 (7) | 0.0004 (7) |
| N3 | 0.0558 (11) | 0.0538 (12) | 0.0544 (11) | 0.0097 (9) | 0.0121 (9) | 0.0178 (9) |
| N4 | 0.0442 (9) | 0.0350 (9) | 0.0396 (9) | −0.0033 (7) | −0.0021 (7) | 0.0040 (7) |
| C1 | 0.0491 (11) | 0.0400 (11) | 0.0317 (9) | −0.0016 (8) | 0.0002 (8) | −0.0022 (7) |
| C2 | 0.0455 (11) | 0.0402 (11) | 0.0380 (10) | 0.0005 (8) | 0.0019 (8) | 0.0049 (8) |
| C3 | 0.0381 (10) | 0.0339 (10) | 0.0463 (11) | −0.0009 (7) | 0.0047 (8) | −0.0031 (8) |
| C4 | 0.0525 (12) | 0.0453 (11) | 0.0341 (10) | −0.0021 (9) | −0.0003 (8) | −0.0069 (8) |
| C5 | 0.0477 (11) | 0.0428 (11) | 0.0337 (9) | 0.0026 (8) | 0.0001 (8) | 0.0035 (8) |
| C6 | 0.0331 (9) | 0.0339 (9) | 0.0381 (10) | 0.0019 (7) | 0.0026 (7) | −0.0008 (7) |
| C7 | 0.0611 (14) | 0.0381 (12) | 0.0789 (16) | −0.0080 (10) | −0.0066 (12) | −0.0052 (10) |
| C8 | 0.0414 (10) | 0.0345 (10) | 0.0400 (10) | −0.0010 (8) | 0.0009 (8) | −0.0033 (8) |
| C9 | 0.0399 (10) | 0.0312 (10) | 0.0526 (12) | 0.0011 (7) | 0.0065 (8) | 0.0024 (8) |
| C10 | 0.0398 (10) | 0.0397 (11) | 0.0416 (10) | 0.0034 (8) | 0.0067 (8) | 0.0108 (8) |
| C11 | 0.0588 (13) | 0.0462 (12) | 0.0364 (10) | 0.0007 (9) | −0.0010 (9) | 0.0004 (8) |
| C12 | 0.0534 (12) | 0.0314 (10) | 0.0408 (10) | −0.0031 (8) | −0.0028 (8) | −0.0024 (8) |
| C13 | 0.0332 (9) | 0.0340 (9) | 0.0366 (9) | −0.0004 (7) | 0.0015 (7) | 0.0048 (7) |
| C14 | 0.0711 (15) | 0.0500 (13) | 0.0483 (12) | −0.0070 (10) | 0.0177 (10) | 0.0066 (10) |
| Cl1 | 0.0642 (4) | 0.0381 (3) | 0.0568 (3) | −0.0017 (2) | 0.0129 (2) | 0.0025 (2) |
| Cl2 | 0.0535 (3) | 0.0514 (3) | 0.0381 (3) | −0.0033 (2) | −0.0030 (2) | −0.0018 (2) |
Geometric parameters (Å, º)
| O1—N1 | 1.190 (2) | C4—C5 | 1.378 (3) |
| O2—N1 | 1.191 (2) | C4—H4 | 0.9300 |
| O3—N3 | 1.220 (2) | C5—C6 | 1.379 (2) |
| O4—N3 | 1.218 (2) | C5—H5 | 0.9300 |
| N1—C3 | 1.477 (2) | C7—H7A | 0.9600 |
| N2—C6 | 1.459 (2) | C7—H7B | 0.9600 |
| N2—C7 | 1.497 (3) | C7—H7C | 0.9600 |
| N2—H2A | 0.901 (9) | C8—C9 | 1.382 (2) |
| N2—H2B | 0.891 (10) | C8—C13 | 1.382 (2) |
| N3—C10 | 1.475 (2) | C8—H8 | 0.9300 |
| N4—C13 | 1.462 (2) | C9—C10 | 1.379 (3) |
| N4—C14 | 1.496 (3) | C9—H9 | 0.9300 |
| N4—H4A | 0.898 (10) | C10—C11 | 1.372 (3) |
| N4—H4B | 0.885 (10) | C11—C12 | 1.385 (3) |
| C1—C2 | 1.376 (3) | C11—H11 | 0.9300 |
| C1—C6 | 1.380 (2) | C12—C13 | 1.372 (2) |
| C1—H1 | 0.9300 | C12—H12 | 0.9300 |
| C2—C3 | 1.374 (2) | C14—H14A | 0.9600 |
| C2—H2 | 0.9300 | C14—H14B | 0.9600 |
| C3—C4 | 1.380 (3) | C14—H14C | 0.9600 |
| O1—N1—O2 | 123.02 (19) | C5—C6—C1 | 121.13 (16) |
| O1—N1—C3 | 119.47 (17) | C5—C6—N2 | 119.60 (15) |
| O2—N1—C3 | 117.52 (18) | C1—C6—N2 | 119.23 (15) |
| C6—N2—C7 | 114.80 (14) | N2—C7—H7A | 109.5 |
| C6—N2—H2A | 110.9 (14) | N2—C7—H7B | 109.5 |
| C7—N2—H2A | 109.6 (14) | H7A—C7—H7B | 109.5 |
| C6—N2—H2B | 107.1 (16) | N2—C7—H7C | 109.5 |
| C7—N2—H2B | 112.7 (16) | H7A—C7—H7C | 109.5 |
| H2A—N2—H2B | 101 (2) | H7B—C7—H7C | 109.5 |
| O4—N3—O3 | 123.90 (19) | C9—C8—C13 | 119.26 (16) |
| O4—N3—C10 | 117.86 (18) | C9—C8—H8 | 120.4 |
| O3—N3—C10 | 118.23 (19) | C13—C8—H8 | 120.4 |
| C13—N4—C14 | 113.82 (15) | C10—C9—C8 | 118.03 (17) |
| C13—N4—H4A | 107.0 (14) | C10—C9—H9 | 121.0 |
| C14—N4—H4A | 111.5 (14) | C8—C9—H9 | 121.0 |
| C13—N4—H4B | 107.5 (14) | C11—C10—C9 | 123.10 (17) |
| C14—N4—H4B | 111.6 (15) | C11—C10—N3 | 118.39 (17) |
| H4A—N4—H4B | 104.9 (19) | C9—C10—N3 | 118.50 (17) |
| C2—C1—C6 | 119.82 (16) | C10—C11—C12 | 118.52 (17) |
| C2—C1—H1 | 120.1 | C10—C11—H11 | 120.7 |
| C6—C1—H1 | 120.1 | C12—C11—H11 | 120.7 |
| C3—C2—C1 | 118.37 (16) | C13—C12—C11 | 119.01 (17) |
| C3—C2—H2 | 120.8 | C13—C12—H12 | 120.5 |
| C1—C2—H2 | 120.8 | C11—C12—H12 | 120.5 |
| C2—C3—C4 | 122.68 (17) | C12—C13—C8 | 122.08 (16) |
| C2—C3—N1 | 118.04 (16) | C12—C13—N4 | 118.90 (16) |
| C4—C3—N1 | 119.23 (16) | C8—C13—N4 | 119.02 (15) |
| C5—C4—C3 | 118.36 (16) | N4—C14—H14A | 109.5 |
| C5—C4—H4 | 120.8 | N4—C14—H14B | 109.5 |
| C3—C4—H4 | 120.8 | H14A—C14—H14B | 109.5 |
| C4—C5—C6 | 119.64 (16) | N4—C14—H14C | 109.5 |
| C4—C5—H5 | 120.2 | H14A—C14—H14C | 109.5 |
| C6—C5—H5 | 120.2 | H14B—C14—H14C | 109.5 |
| C6—C1—C2—C3 | 0.4 (3) | C13—C8—C9—C10 | −0.1 (3) |
| C1—C2—C3—C4 | −0.1 (3) | C8—C9—C10—C11 | 0.7 (3) |
| C1—C2—C3—N1 | 177.47 (17) | C8—C9—C10—N3 | −179.08 (16) |
| O1—N1—C3—C2 | 6.2 (3) | O4—N3—C10—C11 | 168.9 (2) |
| O2—N1—C3—C2 | −174.3 (2) | O3—N3—C10—C11 | −12.1 (3) |
| O1—N1—C3—C4 | −176.2 (2) | O4—N3—C10—C9 | −11.3 (3) |
| O2—N1—C3—C4 | 3.3 (3) | O3—N3—C10—C9 | 167.65 (18) |
| C2—C3—C4—C5 | −0.3 (3) | C9—C10—C11—C12 | −0.5 (3) |
| N1—C3—C4—C5 | −177.77 (17) | N3—C10—C11—C12 | 179.22 (17) |
| C3—C4—C5—C6 | 0.3 (3) | C10—C11—C12—C13 | −0.1 (3) |
| C4—C5—C6—C1 | 0.0 (3) | C11—C12—C13—C8 | 0.6 (3) |
| C4—C5—C6—N2 | 177.53 (17) | C11—C12—C13—N4 | −179.17 (17) |
| C2—C1—C6—C5 | −0.4 (3) | C9—C8—C13—C12 | −0.5 (3) |
| C2—C1—C6—N2 | −177.88 (17) | C9—C8—C13—N4 | 179.30 (16) |
| C7—N2—C6—C5 | 118.4 (2) | C14—N4—C13—C12 | 111.3 (2) |
| C7—N2—C6—C1 | −64.1 (2) | C14—N4—C13—C8 | −68.5 (2) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N2—H2A···Cl2i | 0.90 (1) | 2.18 (1) | 3.0702 (17) | 170 (2) |
| N2—H2B···Cl1i | 0.89 (1) | 2.16 (1) | 3.0482 (19) | 173 (2) |
| N4—H4A···Cl2ii | 0.90 (1) | 2.15 (1) | 3.0361 (18) | 168 (2) |
| N4—H4B···Cl1 | 0.89 (1) | 2.26 (1) | 3.1157 (18) | 163 (2) |
Symmetry codes: (i) −x+1, y−1/2, −z+3/2; (ii) −x, −y+1, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU5532).
References
- Bellamy, A. J. & Sammour, M. H. (1993). Propell. Explos. Pyrot. 18, 46–50.
- Davies, P. J. & Provatas, A. (2006). DSTO Publications Online, DSTO-TR-1904, http://hdl.handle.net/1947/4431.
- Higashi, T. (1995). ABSCOR Rigaku Corporation, Tokyo, Japan.
- Rigaku (2000). RAPID-AUTO Rigaku Corporation, Tokyo, Japan.
- Rigaku/MSC (2000). CrystalClear Rigaku Corporation, Tokyo, Japan.
- Sammour, M. H. (1994). Propell. Explos. Pyrot. 19, 82–86.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Williams, E. M. & Friedlander, C. (2000). US Patent No. 6126763.
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812024117/xu5532sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812024117/xu5532Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812024117/xu5532Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


