Abstract
In the title compound, C11H17ClNO+·Cl−, the side chain of the ethylamine group is orientated approximately perpendicular to the benzene ring, the dihedral angle between the C/C/N plane of the ethylamine group and the benzene plane being 83.5 (3)°. In the crystal structure, intermolecular O—H⋯Cl and N—H⋯Cl hydrogen bonds are observed. The crystal studied was an inversion twin with a 0.51 (10):0.49 (10) domain ratio.
Related literature
For a related structure, see: Tang et al. (2009 ▶).
Experimental
Crystal data
C11H17ClNO+·Cl−
M r = 250.16
Orthorhombic,
a = 7.3460 (3) Å
b = 11.7721 (5) Å
c = 15.2377 (8) Å
V = 1317.72 (10) Å3
Z = 4
Mo Kα radiation
μ = 0.47 mm−1
T = 296 K
0.40 × 0.36 × 0.32 mm
Data collection
Rigaku R-AXIS RAPID diffractometer
Absorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T min = 0.835, T max = 0.864
12577 measured reflections
2977 independent reflections
1874 reflections with I > 2σ(I)
R int = 0.031
Refinement
R[F 2 > 2σ(F 2)] = 0.032
wR(F 2) = 0.107
S = 1.00
2977 reflections
140 parameters
H-atom parameters constrained
Δρmax = 0.29 e Å−3
Δρmin = −0.29 e Å−3
Absolute structure: Flack (1983 ▶), 1243 Friedel pairs
Flack parameter: 0.51 (10)
Data collection: PROCESS-AUTO (Rigaku, 2006 ▶); cell refinement: PROCESS-AUTO; data reduction: CrystalStructure (Rigaku/MSC, 2007 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶).
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809031146/is2447sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809031146/is2447Isup2.hkl
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 |
|---|---|---|---|---|
| N1—H112⋯Cl2 | 0.90 | 2.36 | 3.199 (2) | 156 |
| O1—H1⋯Cl2i | 0.82 | 2.33 | 3.143 (2) | 169 |
| N1—H111⋯Cl2ii | 0.90 | 2.28 | 3.138 (2) | 160 |
Symmetry codes: (i)
; (ii)
.
supplementary crystallographic information
Comment
The title compound (clorprenaline hydrochloride) is one of a series of structurally related β-adrenoceptorblocking drugs.
In the molecular structure (Fig. 1), there are no unusual bond distances or angles. The Cl atom and the phenyl plane is almost planar with the deviation of 0.0037 Å. The dihedral angle between the plane formed by C7/C8/N1 and the phenyl plane is 83.5 (3)°, which shows that the two planes are almost perpendicular. The C9—N1 distance of 1.506 Å is longer than the value of the similar bond distance of 1.474 Å (Tang et al., 2009).
O—H···Cl and N—H···Cl hydrogen bonds are found in the crystal structure and are essential forces in crystal formation. The hydroxyl hydrogen at O1 acts as a donor to Cl2. The ethylamine hydrogens at N1 also act as donors to Cl2.
Experimental
Racemic Clorprenaline hydrochloride was purchased from ShangHai Shengxin Medicine & Chemical Co., Ltd. ShangHai, China. Racemic Clorprenaline hydrochloride (5 g) was dissolved in ethanol (75 ml) and then hydrochloric acid was added to give pH of about 4. Colorless crystal of (I) separated from the solution in about 80% yield after one day.
Refinement
All of the H atoms were placed in calculated positions and allowed to ride on their parent atoms, with C—H = 0.93 (aromatic), 0.98 (methine), 0.97 (methylene), 0.96 Å (methyl), O—H = 0.82 Å and N—H = 0.90 Å, and with Uiso(H) = 1.2–1.5 times Ueq of the parent atoms.
Figures
Fig. 1.
The molecular structure of (I) with atom labels, showing 40% probability displacement ellipsoids.
Crystal data
| C11H17ClNO+·Cl− | F(000) = 528 |
| Mr = 250.16 | Dx = 1.261 Mg m−3 |
| Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P 2ac 2ab | Cell parameters from 8627 reflections |
| a = 7.3460 (3) Å | θ = 3.1–27.4° |
| b = 11.7721 (5) Å | µ = 0.47 mm−1 |
| c = 15.2377 (8) Å | T = 296 K |
| V = 1317.72 (10) Å3 | Chunk, colorless |
| Z = 4 | 0.40 × 0.36 × 0.32 mm |
Data collection
| Rigaku R-AXIS RAPID diffractometer | 2977 independent reflections |
| Radiation source: rotating anode | 1874 reflections with I > 2σ(I) |
| graphite | Rint = 0.031 |
| Detector resolution: 10.00 pixels mm-1 | θmax = 27.4°, θmin = 3.1° |
| ω scans | h = −9→9 |
| Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | k = −15→14 |
| Tmin = 0.835, Tmax = 0.864 | l = −19→19 |
| 12577 measured reflections |
Refinement
| Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
| Least-squares matrix: full | H-atom parameters constrained |
| R[F2 > 2σ(F2)] = 0.032 | w = 1/[σ2(Fo2) + (0.0431P)2 + 0.5P] where P = (Fo2 + 2Fc2)/3 |
| wR(F2) = 0.107 | (Δ/σ)max < 0.001 |
| S = 1.00 | Δρmax = 0.29 e Å−3 |
| 2977 reflections | Δρmin = −0.29 e Å−3 |
| 140 parameters | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| 0 restraints | Extinction coefficient: 0.0054 (12) |
| Primary atom site location: structure-invariant direct methods | Absolute structure: Flack (1983), 1243 Friedel pairs |
| Secondary atom site location: difference Fourier map | Flack parameter: 0.51 (10) |
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 | ||
| Cl2 | 0.51205 (10) | 0.14865 (6) | 0.44638 (6) | 0.0648 (2) | |
| Cl1 | 0.44580 (11) | 0.75320 (8) | 0.58138 (6) | 0.0779 (3) | |
| O1 | 0.3177 (3) | 0.44304 (18) | 0.42787 (16) | 0.0698 (6) | |
| H1 | 0.2294 | 0.4174 | 0.4542 | 0.105* | |
| N1 | 0.5869 (3) | 0.37691 (19) | 0.55437 (15) | 0.0522 (6) | |
| H111 | 0.7029 | 0.3550 | 0.5628 | 0.063* | |
| H112 | 0.5341 | 0.3244 | 0.5198 | 0.063* | |
| C7 | 0.4020 (4) | 0.5277 (2) | 0.4795 (2) | 0.0489 (7) | |
| H7 | 0.3296 | 0.5422 | 0.5323 | 0.059* | |
| C6 | 0.4249 (3) | 0.6368 (2) | 0.42750 (19) | 0.0488 (6) | |
| C1 | 0.4496 (3) | 0.7418 (2) | 0.4678 (2) | 0.0546 (7) | |
| C8 | 0.5901 (4) | 0.4868 (2) | 0.5047 (2) | 0.0537 (7) | |
| H8A | 0.6623 | 0.4771 | 0.4519 | 0.064* | |
| H8B | 0.6487 | 0.5443 | 0.5405 | 0.064* | |
| C9 | 0.4922 (4) | 0.3739 (2) | 0.64202 (18) | 0.0579 (7) | |
| H9 | 0.3639 | 0.3936 | 0.6332 | 0.069* | |
| C5 | 0.4305 (4) | 0.6352 (3) | 0.3365 (2) | 0.0680 (9) | |
| H5 | 0.4144 | 0.5669 | 0.3069 | 0.082* | |
| C11 | 0.5028 (6) | 0.2537 (3) | 0.6769 (2) | 0.0777 (9) | |
| H11A | 0.6279 | 0.2330 | 0.6854 | 0.093* | |
| H11B | 0.4477 | 0.2027 | 0.6355 | 0.093* | |
| H11C | 0.4393 | 0.2492 | 0.7319 | 0.093* | |
| C2 | 0.4764 (4) | 0.8401 (3) | 0.4204 (3) | 0.0729 (10) | |
| H2 | 0.4904 | 0.9091 | 0.4494 | 0.088* | |
| C3 | 0.4824 (5) | 0.8360 (4) | 0.3318 (3) | 0.0920 (13) | |
| H3 | 0.5018 | 0.9022 | 0.2998 | 0.110* | |
| C4 | 0.4597 (5) | 0.7344 (5) | 0.2889 (3) | 0.0897 (12) | |
| H4 | 0.4639 | 0.7319 | 0.2279 | 0.108* | |
| C10 | 0.5746 (6) | 0.4584 (3) | 0.7044 (2) | 0.0928 (13) | |
| H10A | 0.5099 | 0.4564 | 0.7591 | 0.111* | |
| H10B | 0.5665 | 0.5332 | 0.6797 | 0.111* | |
| H10C | 0.7001 | 0.4396 | 0.7144 | 0.111* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cl2 | 0.0489 (4) | 0.0509 (3) | 0.0944 (6) | 0.0007 (3) | 0.0009 (4) | −0.0054 (4) |
| Cl1 | 0.0692 (5) | 0.0819 (6) | 0.0825 (6) | −0.0038 (5) | −0.0021 (4) | −0.0313 (5) |
| O1 | 0.0628 (13) | 0.0559 (12) | 0.0909 (18) | −0.0136 (10) | −0.0123 (12) | −0.0113 (12) |
| N1 | 0.0435 (11) | 0.0498 (13) | 0.0633 (15) | −0.0017 (10) | −0.0009 (11) | 0.0057 (11) |
| C7 | 0.0399 (13) | 0.0455 (14) | 0.0613 (17) | −0.0049 (12) | −0.0016 (12) | −0.0044 (13) |
| C6 | 0.0393 (12) | 0.0465 (14) | 0.0606 (18) | 0.0017 (12) | −0.0015 (12) | 0.0003 (13) |
| C1 | 0.0364 (13) | 0.0510 (15) | 0.0765 (19) | 0.0010 (13) | 0.0021 (13) | −0.0009 (15) |
| C8 | 0.0438 (14) | 0.0483 (15) | 0.069 (2) | −0.0023 (13) | 0.0006 (13) | 0.0073 (13) |
| C9 | 0.0513 (15) | 0.0647 (18) | 0.0577 (17) | −0.0011 (16) | 0.0030 (15) | 0.0076 (13) |
| C5 | 0.0671 (19) | 0.080 (2) | 0.057 (2) | 0.0136 (19) | 0.0015 (15) | 0.0010 (17) |
| C11 | 0.087 (2) | 0.074 (2) | 0.071 (2) | −0.006 (3) | 0.003 (2) | 0.0193 (17) |
| C2 | 0.0455 (15) | 0.0489 (16) | 0.124 (3) | −0.0015 (15) | 0.007 (2) | 0.0108 (18) |
| C3 | 0.059 (2) | 0.082 (3) | 0.135 (4) | 0.012 (2) | 0.010 (2) | 0.050 (3) |
| C4 | 0.076 (3) | 0.125 (3) | 0.068 (2) | 0.020 (3) | 0.0058 (19) | 0.039 (2) |
| C10 | 0.123 (3) | 0.086 (3) | 0.069 (2) | −0.011 (3) | −0.002 (2) | −0.012 (2) |
Geometric parameters (Å, °)
| Cl1—C1 | 1.736 (3) | C9—C11 | 1.514 (4) |
| O1—C7 | 1.413 (3) | C9—H9 | 0.9800 |
| O1—H1 | 0.8200 | C5—C4 | 1.391 (5) |
| N1—C8 | 1.499 (3) | C5—H5 | 0.9300 |
| N1—C9 | 1.506 (3) | C11—H11A | 0.9600 |
| N1—H111 | 0.9000 | C11—H11B | 0.9600 |
| N1—H112 | 0.9000 | C11—H11C | 0.9600 |
| C7—C8 | 1.513 (4) | C2—C3 | 1.352 (6) |
| C7—C6 | 1.518 (4) | C2—H2 | 0.9300 |
| C7—H7 | 0.9800 | C3—C4 | 1.373 (7) |
| C6—C5 | 1.387 (4) | C3—H3 | 0.9300 |
| C6—C1 | 1.393 (4) | C4—H4 | 0.9300 |
| C1—C2 | 1.378 (5) | C10—H10A | 0.9600 |
| C8—H8A | 0.9700 | C10—H10B | 0.9600 |
| C8—H8B | 0.9700 | C10—H10C | 0.9600 |
| C9—C10 | 1.503 (5) | ||
| C7—O1—H1 | 109.5 | C10—C9—H9 | 108.5 |
| C8—N1—C9 | 118.4 (2) | N1—C9—H9 | 108.5 |
| C8—N1—H111 | 107.7 | C11—C9—H9 | 108.5 |
| C9—N1—H111 | 107.7 | C6—C5—C4 | 121.0 (4) |
| C8—N1—H112 | 107.7 | C6—C5—H5 | 119.5 |
| C9—N1—H112 | 107.7 | C4—C5—H5 | 119.5 |
| H111—N1—H112 | 107.1 | C9—C11—H11A | 109.5 |
| O1—C7—C8 | 108.5 (2) | C9—C11—H11B | 109.5 |
| O1—C7—C6 | 110.8 (2) | H11A—C11—H11B | 109.5 |
| C8—C7—C6 | 107.5 (2) | C9—C11—H11C | 109.5 |
| O1—C7—H7 | 110.0 | H11A—C11—H11C | 109.5 |
| C8—C7—H7 | 110.0 | H11B—C11—H11C | 109.5 |
| C6—C7—H7 | 110.0 | C3—C2—C1 | 119.9 (3) |
| C5—C6—C1 | 116.7 (3) | C3—C2—H2 | 120.1 |
| C5—C6—C7 | 120.9 (3) | C1—C2—H2 | 120.1 |
| C1—C6—C7 | 122.4 (2) | C2—C3—C4 | 120.2 (3) |
| C2—C1—C6 | 122.2 (3) | C2—C3—H3 | 119.9 |
| C2—C1—Cl1 | 117.4 (3) | C4—C3—H3 | 119.9 |
| C6—C1—Cl1 | 120.4 (2) | C3—C4—C5 | 120.1 (4) |
| N1—C8—C7 | 112.9 (2) | C3—C4—H4 | 120.0 |
| N1—C8—H8A | 109.0 | C5—C4—H4 | 120.0 |
| C7—C8—H8A | 109.0 | C9—C10—H10A | 109.5 |
| N1—C8—H8B | 109.0 | C9—C10—H10B | 109.5 |
| C7—C8—H8B | 109.0 | H10A—C10—H10B | 109.5 |
| H8A—C8—H8B | 107.8 | C9—C10—H10C | 109.5 |
| C10—C9—N1 | 111.1 (3) | H10A—C10—H10C | 109.5 |
| C10—C9—C11 | 112.1 (3) | H10B—C10—H10C | 109.5 |
| N1—C9—C11 | 108.0 (2) | ||
| O1—C7—C6—C5 | −23.6 (4) | C6—C7—C8—N1 | −178.2 (2) |
| C8—C7—C6—C5 | 94.8 (3) | C8—N1—C9—C10 | −58.5 (3) |
| O1—C7—C6—C1 | 159.4 (2) | C8—N1—C9—C11 | 178.2 (3) |
| C8—C7—C6—C1 | −82.2 (3) | C1—C6—C5—C4 | 0.1 (4) |
| C5—C6—C1—C2 | 0.6 (4) | C7—C6—C5—C4 | −177.1 (3) |
| C7—C6—C1—C2 | 177.8 (2) | C6—C1—C2—C3 | −1.1 (4) |
| C5—C6—C1—Cl1 | −179.8 (2) | Cl1—C1—C2—C3 | 179.4 (3) |
| C7—C6—C1—Cl1 | −2.7 (3) | C1—C2—C3—C4 | 0.7 (5) |
| C9—N1—C8—C7 | −62.6 (3) | C2—C3—C4—C5 | 0.0 (6) |
| O1—C7—C8—N1 | −58.4 (3) | C6—C5—C4—C3 | −0.5 (5) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H112···Cl2 | 0.90 | 2.36 | 3.199 (2) | 156 |
| O1—H1···Cl2i | 0.82 | 2.33 | 3.143 (2) | 169 |
| N1—H111···Cl2ii | 0.90 | 2.28 | 3.138 (2) | 160 |
Symmetry codes: (i) x−1/2, −y+1/2, −z+1; (ii) x+1/2, −y+1/2, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: IS2447).
References
- Farrugia, L. J. (1997). J. Appl. Cryst.30, 565.
- Farrugia, L. J. (1999). J. Appl. Cryst.32, 837–838.
- Flack, H. D. (1983). Acta Cryst. A39, 876–881.
- Higashi, T. (1995). ABSCOR Rigaku Corporation, Tokyo, Japan.
- Rigaku (2006). PROCESS-AUTO Rigaku Corporation, Tokyo, Japan.
- Rigaku/MSC (2007). CrystalStructure Rigaku/MSC. The Woodlands, Texas, USA.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Tang, Z., Xu, M., Zheng, G.-R. & Feng, H. (2009). Acta Cryst. E65, o1501. [DOI] [PMC free article] [PubMed]
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809031146/is2447sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809031146/is2447Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

