Abstract
In the title compound, C10H16N2 2+·2HSO4 −, the S atoms adopt slightly distorted tetrahedral geometry and the diprotonated piperazine ring adopts a chair conformation. In the crystal, the 1-phenylpiperazine-1,4-diium cations are anchored between chains formed by the sulfate entities via intermolecular bifurcated N—H⋯(O,O) and weak C—H⋯O hydrogen bonds. These hydrogen bonds contribute to the cohesion and stability of the network of the crystal structure.
Related literature
For pharmacological properties of phenylpiperazine, see: Cohen et al. (1982 ▶); Conrado et al. (2008 ▶); Neves et al. (2003 ▶). For related structures, see: Ben Gharbia et al. (2005 ▶). For a discussion on hydrogen bonding, see: Brown (1976 ▶); Blessing (1986 ▶). For structural discussion, see: Arbuckle et al. (2009 ▶). For puckering parameters, see: Cremer & Pople (1975 ▶).
Experimental
Crystal data
C10H16N2 2+·2HSO4 −
M r = 358.38
Monoclinic,
a = 17.535 (6) Å
b = 10.996 (2) Å
c = 7.631 (2) Å
β = 99.86 (2)°
V = 1449.7 (7) Å3
Z = 4
Ag Kα radiation
λ = 0.56083 Å
μ = 0.22 mm−1
T = 293 K
0.5 × 0.4 × 0.1 mm
Data collection
Enraf–Nonius CAD-4 diffractometer
8212 measured reflections
7100 independent reflections
4535 reflections with I > 2σ(I)
R int = 0.022
2 standard reflections every 120 min intensity decay: 1%
Refinement
R[F 2 > 2σ(F 2)] = 0.046
wR(F 2) = 0.127
S = 1.03
7100 reflections
201 parameters
H-atom parameters constrained
Δρmax = 0.43 e Å−3
Δρmin = −0.46 e Å−3
Data collection: CAD-4 EXPRESS (Enraf–Nonius, 1994 ▶); cell refinement: CAD-4 EXPRESS; data reduction: XCAD4 (Harms & Wocadlo, 1995 ▶); program(s) used to solve structure: SHELXS86 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-32 for Windows (Farrugia, 1998 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810037001/pv2328sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810037001/pv2328Isup2.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 |
|---|---|---|---|---|
| O1—H1⋯O3i | 0.82 | 1.80 | 2.6140 (17) | 172 |
| O5—H5⋯O7ii | 0.82 | 1.80 | 2.6066 (18) | 169 |
| N1—H1A⋯O2iii | 0.90 | 2.23 | 2.8636 (19) | 128 |
| N1—H1A⋯O3iv | 0.90 | 2.30 | 3.0279 (19) | 138 |
| N1—H1B⋯O3 | 0.90 | 2.14 | 2.9251 (18) | 145 |
| N1—H1B⋯O2i | 0.90 | 2.35 | 2.9892 (18) | 128 |
| N2—H2⋯O7 | 0.91 | 2.02 | 2.8216 (16) | 146 |
| N2—H2⋯O6ii | 0.91 | 2.32 | 2.9037 (17) | 122 |
Symmetry codes: (i)
; (ii)
; (iii)
; (iv)
.
Acknowledgments
We would like to acknowledge the support provided by the Secretary of State for Scientific Research and Technology of Tunisia.
supplementary crystallographic information
Comment
The phenylpiperazine and its derivatives have been intensively investigated recently owing to their interesting pharmacological, cardiovascular and autonomic properties (Conrado et al., 2008; Cohen et al., 1982; Neves et al., 2003). We report here the preparation and the crystal structure of the title compound, (I).
The asymmetric unit of the title compound (Fig.1) consists of two HSO4- anions and a 1-phenylpiperazine-1,4-diium cation. The interatomic bond lengths and angles of the cation show no significant deviation from those reported in other 1-phenylpiperazinium salts such as [C10H16N2]2ZnCl4 (Ben Gharbia, et al., 2005). In the title compound, the distances S—O are significantly longer than the S═O distances as reported in the hydrogen sulfate ion previously (Arbuckle, et al., 2009). The aromatic ring is essentially planar while the diprotonated piperazine ring adopts a chair conformation, with puckering parameters (Cremer & Pople, 1975): Q = 0.5913 (14) Å, θ = 178.61 (15)° and φ = 76 (5)°.
The atomic arrangement is characterized by infinite chains built by HSO4- anions. The inorganic chains, extending along the c direction, are located around planes perpendicular to the a axis at x = 0 (for HS1O4-) and x = 1/4, x = 3/4 (for HS2O4-). The hydrogen sulfate groups of the same type are interconnected via strong O—H···O hydrogen bonds (Table 1)[d (O···O) < 2.73 Å] (Brown, 1976; Blessing, 1986). Chains formed by HS1O4 are linked by N1 nitrogen atom of the cation to form layers parallel to the bc plane at x = 0. Two chains of different type are bound between them by the cations through their two nitrogen atoms by means of the N—H···O hydrogen bonds (Fig. 2).
The cations are linked onto the anionic chains, by forming H-bonds with the oxygen atoms with N—H···O distances in the range 2.8216 (16)–3.0279 (19) Å and C—H···O distances in the range 2.949 (2)–3.520 (2) Å. It should be noticed that all the amino hydrogen atoms are involved in bifurcated N—H···(O, O) hydrogen bonding. These hydrogen bonds contribute to the cohesion and stability of the network of the studied crystal structure.
Experimental
Single crystals of the title compound were prepared at room temperature from a mixture of an aqueous solution of sulfuric acid (2 mmol), 1-phenylpiperazine (1 mmol), ethanol (10 ml) and water (10 ml). The solution was stirred for 1 h then evaporated slowly at room temperature for several days until the formation of good quality of prismatic single crystals.
Refinement
All H atoms were fixed geometrically and treated as riding with C—H = 0.93 Å (aromatic) or 0.97 Å (methylene), N—H = 0.90 Å or 0.91 Å and O—H = 0.82 Å with Uiso(H) = 1.2Ueq(C or N) or 1.5Ueq(O).
Figures
Fig. 1.
An ORTEP view of (I) with the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level. H atoms are represented as small spheres of arbitrary radii.
Fig. 2.
Projection of (I) along the c axis. H atoms non committed in H-bonds are omitted for clarity.
Crystal data
| C10H16N22+·2HSO4− | F(000) = 752 |
| Mr = 358.38 | Dx = 1.642 Mg m−3 |
| Monoclinic, P21/c | Ag Kα radiation, λ = 0.56083 Å |
| Hall symbol: -P 2ybc | Cell parameters from 25 reflections |
| a = 17.535 (6) Å | θ = 9–11° |
| b = 10.996 (2) Å | µ = 0.22 mm−1 |
| c = 7.631 (2) Å | T = 293 K |
| β = 99.86 (2)° | Prism, colorless |
| V = 1449.7 (7) Å3 | 0.5 × 0.4 × 0.1 mm |
| Z = 4 |
Data collection
| Enraf–Nonius CAD-4 diffractometer | Rint = 0.022 |
| Radiation source: fine-focus sealed tube | θmax = 28.0°, θmin = 2.4° |
| graphite | h = −3→29 |
| non–profiled ω scans | k = −18→0 |
| 8212 measured reflections | l = −12→12 |
| 7100 independent reflections | 2 standard reflections every 120 min |
| 4535 reflections with I > 2σ(I) | intensity decay: 1% |
Refinement
| 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: inferred from neighbouring sites |
| wR(F2) = 0.127 | H-atom parameters constrained |
| S = 1.03 | w = 1/[σ2(Fo2) + (0.0603P)2 + 0.1738P] where P = (Fo2 + 2Fc2)/3 |
| 7100 reflections | (Δ/σ)max = 0.001 |
| 201 parameters | Δρmax = 0.43 e Å−3 |
| 0 restraints | Δρmin = −0.46 e Å−3 |
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 | ||
| S1 | 0.958198 (19) | 0.80824 (3) | 0.59663 (4) | 0.02129 (8) | |
| S2 | 0.68841 (2) | 0.18262 (3) | 0.36929 (5) | 0.02431 (8) | |
| O7 | 0.66990 (8) | 0.31003 (10) | 0.32493 (15) | 0.0332 (2) | |
| O3 | 0.97861 (7) | 0.68051 (10) | 0.64169 (14) | 0.0306 (2) | |
| N2 | 0.73629 (7) | 0.53363 (10) | 0.45259 (15) | 0.0215 (2) | |
| H2 | 0.7163 | 0.4579 | 0.4607 | 0.026* | |
| O2 | 0.97180 (7) | 0.88315 (10) | 0.75428 (14) | 0.0295 (2) | |
| N1 | 0.89625 (7) | 0.46159 (12) | 0.49684 (18) | 0.0273 (2) | |
| H1A | 0.9333 | 0.4041 | 0.5136 | 0.033* | |
| H1B | 0.9194 | 0.5342 | 0.4913 | 0.033* | |
| O1 | 1.01876 (7) | 0.85308 (12) | 0.48419 (14) | 0.0355 (3) | |
| H1 | 1.0036 | 0.8368 | 0.3791 | 0.053* | |
| O4 | 0.88248 (7) | 0.81856 (12) | 0.49109 (16) | 0.0366 (3) | |
| O5 | 0.63020 (7) | 0.13868 (12) | 0.48817 (15) | 0.0356 (3) | |
| H5 | 0.6438 | 0.1639 | 0.5898 | 0.053* | |
| O6 | 0.67139 (8) | 0.10676 (11) | 0.21389 (16) | 0.0371 (3) | |
| C3 | 0.79171 (8) | 0.55729 (14) | 0.62253 (19) | 0.0258 (3) | |
| H3A | 0.7639 | 0.5567 | 0.7220 | 0.031* | |
| H3B | 0.8152 | 0.6368 | 0.6173 | 0.031* | |
| C2 | 0.77975 (9) | 0.53263 (14) | 0.29912 (19) | 0.0266 (3) | |
| H2A | 0.8023 | 0.6122 | 0.2876 | 0.032* | |
| H2B | 0.7442 | 0.5155 | 0.1900 | 0.032* | |
| C5 | 0.67057 (8) | 0.61993 (13) | 0.42348 (19) | 0.0244 (3) | |
| C1 | 0.84293 (8) | 0.43819 (14) | 0.3260 (2) | 0.0284 (3) | |
| H1C | 0.8203 | 0.3578 | 0.3284 | 0.034* | |
| H1D | 0.8716 | 0.4412 | 0.2281 | 0.034* | |
| C4 | 0.85375 (9) | 0.46091 (15) | 0.6493 (2) | 0.0293 (3) | |
| H4A | 0.8895 | 0.4765 | 0.7588 | 0.035* | |
| H4B | 0.8304 | 0.3817 | 0.6588 | 0.035* | |
| O8 | 0.76519 (7) | 0.17042 (14) | 0.47005 (18) | 0.0465 (3) | |
| C10 | 0.68447 (10) | 0.74340 (14) | 0.4204 (3) | 0.0346 (3) | |
| H10 | 0.7348 | 0.7735 | 0.4384 | 0.042* | |
| C6 | 0.59670 (9) | 0.57280 (16) | 0.3966 (2) | 0.0347 (3) | |
| H6 | 0.5887 | 0.4892 | 0.3987 | 0.042* | |
| C9 | 0.62142 (12) | 0.82154 (17) | 0.3896 (3) | 0.0468 (5) | |
| H9 | 0.6293 | 0.9051 | 0.3871 | 0.056* | |
| C8 | 0.54742 (13) | 0.7761 (2) | 0.3629 (3) | 0.0532 (5) | |
| H8 | 0.5055 | 0.8291 | 0.3422 | 0.064* | |
| C7 | 0.53462 (10) | 0.6521 (2) | 0.3664 (3) | 0.0489 (5) | |
| H7 | 0.4843 | 0.6221 | 0.3485 | 0.059* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| S1 | 0.02138 (14) | 0.02425 (15) | 0.01794 (14) | −0.00207 (12) | 0.00249 (10) | −0.00047 (11) |
| S2 | 0.02718 (16) | 0.02462 (15) | 0.02126 (15) | −0.00051 (13) | 0.00451 (12) | 0.00042 (12) |
| O7 | 0.0483 (7) | 0.0228 (5) | 0.0284 (5) | −0.0016 (5) | 0.0067 (5) | −0.0006 (4) |
| O3 | 0.0446 (6) | 0.0249 (5) | 0.0219 (5) | 0.0038 (5) | 0.0047 (4) | 0.0000 (4) |
| N2 | 0.0196 (5) | 0.0189 (5) | 0.0255 (5) | −0.0014 (4) | 0.0029 (4) | 0.0000 (4) |
| O2 | 0.0372 (6) | 0.0288 (5) | 0.0225 (5) | −0.0006 (4) | 0.0055 (4) | −0.0059 (4) |
| N1 | 0.0198 (5) | 0.0266 (6) | 0.0352 (6) | −0.0001 (4) | 0.0037 (5) | 0.0005 (5) |
| O1 | 0.0341 (6) | 0.0512 (7) | 0.0225 (5) | −0.0180 (5) | 0.0087 (4) | −0.0030 (5) |
| O4 | 0.0250 (5) | 0.0474 (7) | 0.0343 (6) | −0.0012 (5) | −0.0036 (4) | 0.0024 (5) |
| O5 | 0.0398 (6) | 0.0412 (7) | 0.0275 (5) | −0.0149 (5) | 0.0103 (5) | −0.0031 (5) |
| O6 | 0.0545 (8) | 0.0298 (5) | 0.0286 (5) | 0.0002 (5) | 0.0116 (5) | −0.0078 (4) |
| C3 | 0.0247 (6) | 0.0278 (6) | 0.0241 (6) | −0.0011 (5) | 0.0015 (5) | −0.0018 (5) |
| C2 | 0.0252 (6) | 0.0316 (7) | 0.0234 (6) | 0.0017 (5) | 0.0052 (5) | 0.0003 (5) |
| C5 | 0.0221 (6) | 0.0232 (6) | 0.0279 (6) | 0.0029 (5) | 0.0040 (5) | 0.0030 (5) |
| C1 | 0.0243 (6) | 0.0297 (7) | 0.0320 (7) | −0.0002 (6) | 0.0068 (5) | −0.0057 (6) |
| C4 | 0.0251 (6) | 0.0347 (8) | 0.0273 (7) | 0.0015 (6) | 0.0019 (5) | 0.0049 (6) |
| O8 | 0.0297 (6) | 0.0652 (9) | 0.0419 (7) | 0.0035 (6) | −0.0015 (5) | 0.0122 (7) |
| C10 | 0.0301 (8) | 0.0244 (7) | 0.0494 (10) | 0.0011 (6) | 0.0071 (7) | 0.0036 (6) |
| C6 | 0.0234 (7) | 0.0330 (8) | 0.0467 (9) | −0.0006 (6) | 0.0029 (6) | 0.0045 (7) |
| C9 | 0.0468 (11) | 0.0280 (8) | 0.0661 (13) | 0.0109 (8) | 0.0110 (10) | 0.0070 (8) |
| C8 | 0.0408 (10) | 0.0490 (11) | 0.0707 (15) | 0.0220 (9) | 0.0123 (10) | 0.0172 (11) |
| C7 | 0.0211 (7) | 0.0548 (12) | 0.0698 (14) | 0.0061 (8) | 0.0050 (8) | 0.0140 (11) |
Geometric parameters (Å, °)
| S1—O4 | 1.4347 (13) | C3—H3B | 0.9700 |
| S1—O2 | 1.4438 (11) | C2—C1 | 1.507 (2) |
| S1—O3 | 1.4754 (11) | C2—H2A | 0.9700 |
| S1—O1 | 1.5553 (12) | C2—H2B | 0.9700 |
| S2—O8 | 1.4378 (14) | C5—C6 | 1.377 (2) |
| S2—O6 | 1.4387 (12) | C5—C10 | 1.380 (2) |
| S2—O7 | 1.4647 (12) | C1—H1C | 0.9700 |
| S2—O5 | 1.5542 (12) | C1—H1D | 0.9700 |
| N2—C5 | 1.4799 (18) | C4—H4A | 0.9700 |
| N2—C2 | 1.5027 (19) | C4—H4B | 0.9700 |
| N2—C3 | 1.5041 (18) | C10—C9 | 1.388 (2) |
| N2—H2 | 0.9100 | C10—H10 | 0.9300 |
| N1—C4 | 1.485 (2) | C6—C7 | 1.383 (2) |
| N1—C1 | 1.491 (2) | C6—H6 | 0.9300 |
| N1—H1A | 0.9000 | C9—C8 | 1.373 (3) |
| N1—H1B | 0.9000 | C9—H9 | 0.9300 |
| O1—H1 | 0.8200 | C8—C7 | 1.383 (3) |
| O5—H5 | 0.8200 | C8—H8 | 0.9300 |
| C3—C4 | 1.507 (2) | C7—H7 | 0.9300 |
| C3—H3A | 0.9700 | ||
| O4—S1—O2 | 115.31 (8) | C1—C2—H2A | 109.4 |
| O4—S1—O3 | 111.75 (7) | N2—C2—H2B | 109.4 |
| O2—S1—O3 | 110.49 (7) | C1—C2—H2B | 109.4 |
| O4—S1—O1 | 108.60 (8) | H2A—C2—H2B | 108.0 |
| O2—S1—O1 | 104.35 (7) | C6—C5—C10 | 122.13 (15) |
| O3—S1—O1 | 105.60 (7) | C6—C5—N2 | 117.99 (13) |
| O8—S2—O6 | 115.46 (9) | C10—C5—N2 | 119.87 (13) |
| O8—S2—O7 | 111.29 (8) | N1—C1—C2 | 109.67 (12) |
| O6—S2—O7 | 110.95 (7) | N1—C1—H1C | 109.7 |
| O8—S2—O5 | 107.90 (8) | C2—C1—H1C | 109.7 |
| O6—S2—O5 | 103.68 (7) | N1—C1—H1D | 109.7 |
| O7—S2—O5 | 106.89 (8) | C2—C1—H1D | 109.7 |
| C5—N2—C2 | 111.93 (11) | H1C—C1—H1D | 108.2 |
| C5—N2—C3 | 112.96 (11) | N1—C4—C3 | 109.71 (12) |
| C2—N2—C3 | 109.52 (11) | N1—C4—H4A | 109.7 |
| C5—N2—H2 | 107.4 | C3—C4—H4A | 109.7 |
| C2—N2—H2 | 107.4 | N1—C4—H4B | 109.7 |
| C3—N2—H2 | 107.4 | C3—C4—H4B | 109.7 |
| C4—N1—C1 | 111.13 (12) | H4A—C4—H4B | 108.2 |
| C4—N1—H1A | 109.4 | C5—C10—C9 | 118.29 (17) |
| C1—N1—H1A | 109.4 | C5—C10—H10 | 120.9 |
| C4—N1—H1B | 109.4 | C9—C10—H10 | 120.9 |
| C1—N1—H1B | 109.4 | C5—C6—C7 | 118.74 (17) |
| H1A—N1—H1B | 108.0 | C5—C6—H6 | 120.6 |
| S1—O1—H1 | 109.5 | C7—C6—H6 | 120.6 |
| S2—O5—H5 | 109.5 | C8—C9—C10 | 120.33 (18) |
| N2—C3—C4 | 109.89 (12) | C8—C9—H9 | 119.8 |
| N2—C3—H3A | 109.7 | C10—C9—H9 | 119.8 |
| C4—C3—H3A | 109.7 | C9—C8—C7 | 120.56 (18) |
| N2—C3—H3B | 109.7 | C9—C8—H8 | 119.7 |
| C4—C3—H3B | 109.7 | C7—C8—H8 | 119.7 |
| H3A—C3—H3B | 108.2 | C8—C7—C6 | 119.95 (18) |
| N2—C2—C1 | 110.98 (12) | C8—C7—H7 | 120.0 |
| N2—C2—H2A | 109.4 | C6—C7—H7 | 120.0 |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| O1—H1···O3i | 0.82 | 1.80 | 2.6140 (17) | 172 |
| O5—H5···O7ii | 0.82 | 1.80 | 2.6066 (18) | 169 |
| N1—H1A···O2iii | 0.90 | 2.23 | 2.8636 (19) | 128 |
| N1—H1A···O3iv | 0.90 | 2.30 | 3.0279 (19) | 138 |
| N1—H1B···O3 | 0.90 | 2.14 | 2.9251 (18) | 145 |
| N1—H1B···O2i | 0.90 | 2.35 | 2.9892 (18) | 128 |
| N2—H2···O7 | 0.91 | 2.02 | 2.8216 (16) | 146 |
| N2—H2···O6ii | 0.91 | 2.32 | 2.9037 (17) | 122 |
| C1—H1C···O8 | 0.97 | 2.59 | 3.500 (2) | 156 |
| C1—H1D···O2i | 0.97 | 2.60 | 3.113 (2) | 114 |
| C3—H3A···O6ii | 0.97 | 2.42 | 2.949 (2) | 114 |
| C3—H3B···O4 | 0.97 | 2.59 | 3.513 (2) | 159 |
| C6—H6···O7 | 0.93 | 2.55 | 3.246 (2) | 132 |
| C10—H10···O4 | 0.93 | 2.60 | 3.520 (2) | 170 |
Symmetry codes: (i) x, −y+3/2, z−1/2; (ii) x, −y+1/2, z+1/2; (iii) −x+2, y−1/2, −z+3/2; (iv) −x+2, −y+1, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: PV2328).
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Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810037001/pv2328sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810037001/pv2328Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


