4-(Methyl-sulfon-yl)piperazin-1-ium chloride.

In the title mol-ecular salt, C(5)H(13)N(2)O(2)S(+)·Cl(-), the complete cation is generated by crystallographic mirror symmetry, with both N atoms, the S atom and one C atom lying on the reflecting plane. The chloride ion also lies on the mirror plane. The piperazinium ring adopts a chair conformation and the N-S bond adopts an equatorial orientation. In the crystal structure, the component ions are linked into a three-dimensional framework by inter-molecular N-H⋯Cl and C-H⋯Cl hydrogen bonds.

Related literature

For medicinal background to piperazine derivatives, see: Dinsmore & Beshore (2002 ▶); Berkheij et al. (2005 ▶); Humle & Cherrier (1999 ▶). For related structures, see: Bart et al. (1978 ▶); Girisha et al. (2008 ▶); Homrighausen & Krause Bauer (2002 ▶); Jin et al. (2007 ▶); Kubo et al. (2007 ▶); Parkin et al. (2004 ▶); Shen et al. (2006 ▶), Wang et al. (2006 ▶). For ring conformations, see: Cremer & Pople (1975 ▶). For the stability of the temperature controller used for the data collection, see: Cosier & Glazer (1986 ▶).

Experimental

Crystal data

C5H13N2O2S+·Cl−

M = 200.68

Monoclinic,

a = 6.0231 (1) Å

b = 9.1097 (2) Å

c = 7.9852 (2) Å

β = 100.700 (1)°

V = 430.52 (2) Å3

Z = 2

Mo Kα radiation

μ = 0.64 mm−1

T = 100 K

0.36 × 0.32 × 0.05 mm

Data collection

Bruker APEX Duo CCD diffractometer

Absorption correction: multi-scan (SADABS; Bruker, 2009 ▶) T min = 0.801, T max = 0.968

10626 measured reflections

2790 independent reflections

2419 reflections with I > 2σ(I)

R int = 0.022

Refinement

R[F 2 > 2σ(F 2)] = 0.023

wR(F 2) = 0.072

S = 1.10

2790 reflections

87 parameters

H atoms treated by a mixture of independent and constrained refinement

Δρmax = 0.49 e Å−3

Δρmin = −0.40 e Å−3

Data collection: APEX2 (Bruker, 2009 ▶); cell refinement: SAINT (Bruker, 2009 ▶); data reduction: SAINT 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 and PLATON (Spek, 2009 ▶).

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810001224/hb5306sup1.cif

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810001224/hb5306Isup2.hkl

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

C5H13N2O2S+·Cl−	F(000) = 212
Mr = 200.68	Dx = 1.548 Mg m−3
Monoclinic, P21/m	Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yb	Cell parameters from 4890 reflections
a = 6.0231 (1) Å	θ = 3.4–40.1°
b = 9.1097 (2) Å	µ = 0.64 mm−1
c = 7.9852 (2) Å	T = 100 K
β = 100.700 (1)°	Plate, colourless
V = 430.52 (2) Å3	0.36 × 0.32 × 0.05 mm
Z = 2

Bruker APEX Duo CCD diffractometer	2790 independent reflections
Radiation source: fine-focus sealed tube	2419 reflections with I > 2σ(I)
graphite	Rint = 0.022
φ and ω scans	θmax = 40.1°, θmin = 2.6°
Absorption correction: multi-scan (SADABS; Bruker, 2009)	h = −10→10
Tmin = 0.801, Tmax = 0.968	k = −14→16
10626 measured reflections	l = −14→14

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)] = 0.023	Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.072	H atoms treated by a mixture of independent and constrained refinement
S = 1.10	w = 1/[σ2(Fo2) + (0.0335P)2 + 0.0922P] where P = (Fo2 + 2Fc2)/3
2790 reflections	(Δ/σ)max = 0.001
87 parameters	Δρmax = 0.49 e Å−3
0 restraints	Δρmin = −0.40 e Å−3

Experimental. The crystal was placed in the cold stream of an Oxford Cyrosystems Cobra open-flow nitrogen cryostat (Cosier & Glazer, 1986) operating at 100.0 (1) K.

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
Cl1	0.30674 (3)	0.2500	0.93448 (3)	0.01195 (5)
S1	0.69091 (3)	0.2500	0.56598 (2)	0.00951 (5)
N1	0.82854 (12)	0.2500	0.03611 (9)	0.01007 (11)
N2	0.79320 (12)	0.2500	0.38830 (9)	0.00974 (11)
O1	0.75935 (9)	0.11396 (6)	0.65235 (6)	0.01498 (9)
C1	0.87784 (10)	0.11522 (7)	0.14202 (8)	0.01165 (9)
C2	0.74465 (10)	0.11465 (7)	0.28537 (8)	0.01168 (9)
C3	0.39411 (15)	0.2500	0.50705 (12)	0.01332 (13)
H1A	0.8351 (18)	0.0315 (13)	0.0719 (14)	0.012 (2)*
H1B	1.040 (2)	0.1186 (13)	0.1845 (16)	0.016 (3)*
H2A	0.583 (2)	0.1017 (14)	0.2371 (15)	0.018 (3)*
H2B	0.789 (2)	0.0335 (16)	0.3554 (17)	0.027 (3)*
H3A	0.331 (3)	0.2500	0.606 (2)	0.019 (4)*
H3B	0.350 (2)	0.3381 (15)	0.4460 (16)	0.025 (3)*
H1N1	0.914 (3)	0.2500	−0.048 (2)	0.019 (4)*
H2N1	0.677 (3)	0.2500	−0.017 (2)	0.021 (4)*

	U11	U22	U33	U12	U13	U23
Cl1	0.00886 (7)	0.01261 (8)	0.01485 (9)	0.000	0.00346 (6)	0.000
S1	0.01110 (8)	0.01033 (8)	0.00696 (8)	0.000	0.00128 (6)	0.000
N1	0.0098 (2)	0.0115 (3)	0.0095 (3)	0.000	0.00316 (19)	0.000
N2	0.0126 (2)	0.0084 (2)	0.0087 (2)	0.000	0.0032 (2)	0.000
O1	0.01874 (19)	0.01499 (19)	0.01109 (18)	0.00356 (16)	0.00245 (15)	0.00480 (15)
C1	0.0148 (2)	0.00900 (19)	0.0122 (2)	0.00097 (17)	0.00547 (17)	−0.00041 (17)
C2	0.0162 (2)	0.0083 (2)	0.0117 (2)	−0.00109 (16)	0.00571 (17)	−0.00060 (16)
C3	0.0115 (3)	0.0166 (3)	0.0121 (3)	0.000	0.0027 (2)	0.000

S1—O1i	1.4408 (5)	N2—C2i	1.4806 (7)
S1—O1	1.4408 (5)	C1—C2	1.5148 (8)
S1—N2	1.6484 (7)	C1—H1A	0.953 (11)
S1—C3	1.7621 (9)	C1—H1B	0.976 (12)
N1—C1	1.4892 (7)	C2—H2A	0.983 (13)
N1—C1i	1.4892 (7)	C2—H2B	0.935 (14)
N1—H1N1	0.920 (17)	C3—H3A	0.941 (18)
N1—H2N1	0.933 (19)	C3—H3B	0.951 (14)
N2—C2	1.4806 (7)
O1i—S1—O1	118.67 (4)	N1—C1—C2	110.75 (5)
O1i—S1—N2	107.01 (2)	N1—C1—H1A	108.8 (7)
O1—S1—N2	107.01 (2)	C2—C1—H1A	108.5 (6)
O1i—S1—C3	108.28 (3)	N1—C1—H1B	104.6 (7)
O1—S1—C3	108.29 (3)	C2—C1—H1B	112.1 (7)
N2—S1—C3	107.03 (4)	H1A—C1—H1B	112.0 (9)
C1—N1—C1i	111.07 (7)	N2—C2—C1	109.81 (5)
C1—N1—H1N1	109.7 (5)	N2—C2—H2A	113.4 (7)
C1i—N1—H1N1	109.7 (5)	C1—C2—H2A	109.1 (7)
C1—N1—H2N1	109.5 (5)	N2—C2—H2B	108.7 (8)
C1i—N1—H2N1	109.5 (5)	C1—C2—H2B	108.7 (7)
H1N1—N1—H2N1	107.3 (15)	H2A—C2—H2B	107.1 (10)
C2—N2—C2i	112.77 (7)	S1—C3—H3A	108.9 (11)
C2—N2—S1	114.27 (4)	S1—C3—H3B	108.1 (8)
C2i—N2—S1	114.27 (4)	H3A—C3—H3B	108.3 (9)
O1i—S1—N2—C2	178.10 (5)	C3—S1—N2—C2i	66.00 (5)
O1—S1—N2—C2	49.91 (6)	C1i—N1—C1—C2	56.95 (8)
C3—S1—N2—C2	−65.99 (5)	C2i—N2—C2—C1	56.73 (8)
O1i—S1—N2—C2i	−49.91 (6)	S1—N2—C2—C1	−170.56 (4)
O1—S1—N2—C2i	−178.10 (5)	N1—C1—C2—N2	−55.89 (7)

D—H···A	D—H	H···A	D···A	D—H···A
N1—H1N1···Cl1ii	0.92 (2)	2.40 (2)	3.1341 (8)	137 (1)
N1—H2N1···Cl1iii	0.93 (2)	2.19 (2)	3.0966 (8)	164 (1)
C1—H1A···Cl1iv	0.953 (12)	2.700 (12)	3.5251 (6)	145.2 (9)
C3—H3A···Cl1	0.94 (2)	2.65 (2)	3.5487 (10)	160 (2)

Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A	D—H	H⋯A	D⋯A	D—H⋯A
N1—H1N1⋯Cl1i	0.92 (2)	2.40 (2)	3.1341 (8)	137 (1)
N1—H2N1⋯Cl1ii	0.93 (2)	2.19 (2)	3.0966 (8)	164 (1)
C1—H1A⋯Cl1iii	0.953 (12)	2.700 (12)	3.5251 (6)	145.2 (9)
C3—H3A⋯Cl1	0.94 (2)	2.65 (2)	3.5487 (10)	160 (2)

Symmetry codes: (i) ; (ii) ; (iii) .