Download citation
Download citation
link to html
The title compound, C9H14N3+·Cl, crystallizes at room temperature from chloro­form as a zwitterion. The mol­ecules are linked by N—H...Cl hydrogen bonds into chains. The piperazine ring adopts a chair conformation.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807053470/at2451sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807053470/at2451Isup2.hkl
Contains datablock I

CCDC reference: 672804

Key indicators

  • Single-crystal X-ray study
  • T = 100 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.029
  • wR factor = 0.061
  • Data-to-parameter ratio = 12.2

checkCIF/PLATON results

No syntax errors found



Alert level C ABSTY03_ALERT_1_C The _exptl_absorpt_correction_type has been given as none. However values have been given for Tmin and Tmax. Remove these if an absorption correction has not been applied. From the CIF: _exptl_absorpt_correction_T_min 0.873 From the CIF: _exptl_absorpt_correction_T_max 0.950 PLAT042_ALERT_1_C Calc. and Rep. MoietyFormula Strings Differ .... ? PLAT350_ALERT_3_C Short C-H Bond (0.96A) C6 - H11 ... 0.84 Ang.
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 26.36 From the CIF: _reflns_number_total 1956 Count of symmetry unique reflns 1169 Completeness (_total/calc) 167.32% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 787 Fraction of Friedel pairs measured 0.673 Are heavy atom types Z>Si present yes
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

Piperazine is freely soluble in water and ethylene glycol, but insoluble in diethyl ether. It is a weak base with a pKb of 4.19; the pH of a 10% aqueous solution is 10.8–11.8. A large number of piperazine compounds have anthelmintic action. Piperazines are also used in the manufacture of plastics, resins, pesticides, brake fluid and other industrial materials (The Merck Index, 1989). The structure of (I) is shown in Fig. 1.

The N—C distances in piperazin-4-ium ring are 1.485 (3) and 1.490 (2) Å, while in the pyridine ring the N—C distance are 1.345 (2) Å. Hydrogen bonds of the type N—H···Cl link the molecules into chains, with N···Cl separation of 3.0961 (17) and 3.1020 (17) Å (Fig. 2).

Related literature top

For related literature, see: The Merck Index (1989).

Experimental top

1-(2-Pyridinyl)piperazine (1 mmol) and trimethyltin chloride (1 mmol) were suspended in dry chloroform (150 ml) in a round bottom two necked flask. The mixture was stirred at room temperature. Colourless crystals of the title compound obtained accidently after recrystallization in acetone. (Yield 70%°; m.p. 393 K).

Refinement top

H atoms were included in difference map positions and refined freely, with C—H distances ranging from 0.84 (2) - 1.00 (2) Å and N—H distances of 0.91 (2) and 0.98 (2) Å.

Computing details top

Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2002); data reduction: SAINT (Bruker, 2002); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 2001); software used to prepare material for publication: SHELXTL (Bruker, 2001).

Figures top
[Figure 1] Fig. 1. Structure of (I) with displacement ellipsoids drawn at the 50% probability level.
[Figure 2] Fig. 2. Packing of (I) viewed down a showing the N—H···Cl hydrogen bonding. H atoms not involved in hydrogen bonding have been omitted for clarity.
4-(2-Pyridyl)piperazin-1-ium chloride top
Crystal data top
C9H14ClN3F(000) = 424
Mr = 199.68Dx = 1.364 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 2404 reflections
a = 7.1757 (6) Åθ = 3.0–26.3°
b = 7.2196 (6) ŵ = 0.35 mm1
c = 18.7629 (16) ÅT = 100 K
V = 972.02 (14) Å3Plate, colourless
Z = 40.40 × 0.25 × 0.15 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
1781 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.044
Graphite monochromatorθmax = 26.4°, θmin = 2.2°
ϕ and ω scansh = 88
5613 measured reflectionsk = 98
1956 independent reflectionsl = 2023
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.029Only H-atom coordinates refined
wR(F2) = 0.061 w = 1/[σ2(Fo2) + (0.0272P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.96(Δ/σ)max < 0.001
1956 reflectionsΔρmax = 0.22 e Å3
160 parametersΔρmin = 0.16 e Å3
0 restraintsAbsolute structure: Flack (1983), 787 Freidel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.04 (7)
Crystal data top
C9H14ClN3V = 972.02 (14) Å3
Mr = 199.68Z = 4
Orthorhombic, P212121Mo Kα radiation
a = 7.1757 (6) ŵ = 0.35 mm1
b = 7.2196 (6) ÅT = 100 K
c = 18.7629 (16) Å0.40 × 0.25 × 0.15 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
1781 reflections with I > 2σ(I)
5613 measured reflectionsRint = 0.044
1956 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.029Only H-atom coordinates refined
wR(F2) = 0.061Δρmax = 0.22 e Å3
S = 0.96Δρmin = 0.16 e Å3
1956 reflectionsAbsolute structure: Flack (1983), 787 Freidel pairs
160 parametersAbsolute structure parameter: 0.04 (7)
0 restraints
Special details top

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 F^2^ against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F^2^, conventional R-factors R are based on F, with F set to zero for negative F^2^. The threshold expression of F^2^ > σ(F^2^) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F^2^ 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) top
xyzUiso*/Ueq
Cl10.24771 (7)0.33171 (5)0.23724 (2)0.02020 (12)
N10.3814 (2)0.6758 (2)0.32203 (8)0.0201 (4)
N20.3397 (2)0.90492 (19)0.44477 (7)0.0157 (3)
N30.4096 (2)0.9562 (2)0.56481 (8)0.0194 (3)
C10.4004 (3)0.5979 (3)0.39523 (10)0.0195 (4)
C20.4664 (3)0.7455 (3)0.44616 (10)0.0178 (4)
C30.3159 (3)0.9827 (3)0.37348 (9)0.0186 (4)
C40.2510 (3)0.8355 (3)0.32164 (9)0.0221 (4)
C50.3404 (3)1.0234 (2)0.50341 (9)0.0150 (4)
C60.2672 (3)1.2021 (2)0.49926 (9)0.0174 (4)
C70.2704 (3)1.3113 (2)0.55864 (9)0.0218 (4)
C80.3435 (3)1.2463 (3)0.62216 (10)0.0201 (4)
C90.4074 (3)1.0673 (3)0.62279 (9)0.0202 (4)
H10.494 (3)0.714 (3)0.3056 (9)0.024*
H20.336 (3)0.584 (3)0.2878 (9)0.024*
H30.485 (3)0.500 (3)0.3933 (9)0.024*
H40.274 (3)0.553 (2)0.4082 (8)0.024*
H50.595 (3)0.784 (2)0.4338 (9)0.024*
H60.474 (3)0.697 (2)0.4932 (10)0.024*
H70.219 (3)1.082 (3)0.3732 (9)0.024*
H80.431 (3)1.036 (3)0.3556 (9)0.024*
H90.244 (3)0.885 (2)0.2767 (9)0.024*
H100.129 (3)0.795 (3)0.3334 (9)0.024*
H110.217 (3)1.237 (3)0.4612 (9)0.024*
H120.223 (3)1.440 (2)0.5546 (9)0.024*
H130.350 (3)1.317 (3)0.6642 (9)0.024*
H140.453 (3)1.016 (3)0.6682 (9)0.024*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0216 (2)0.0179 (2)0.0211 (2)0.0011 (2)0.0015 (2)0.00328 (17)
N10.0234 (9)0.0198 (8)0.0171 (8)0.0057 (8)0.0008 (7)0.0045 (7)
N20.0198 (8)0.0144 (7)0.0129 (7)0.0023 (7)0.0015 (6)0.0020 (6)
N30.0203 (8)0.0213 (8)0.0167 (8)0.0004 (7)0.0005 (6)0.0002 (7)
C10.0193 (10)0.0171 (10)0.0222 (10)0.0004 (8)0.0002 (9)0.0002 (8)
C20.0198 (11)0.0171 (9)0.0165 (9)0.0031 (8)0.0025 (8)0.0015 (8)
C30.0229 (10)0.0181 (9)0.0149 (9)0.0010 (8)0.0030 (8)0.0015 (8)
C40.0253 (10)0.0245 (9)0.0164 (8)0.0004 (13)0.0044 (10)0.0020 (8)
C50.0125 (9)0.0167 (9)0.0158 (9)0.0015 (8)0.0024 (7)0.0025 (8)
C60.0179 (10)0.0170 (9)0.0172 (8)0.0007 (9)0.0012 (9)0.0042 (7)
C70.0198 (11)0.0159 (9)0.0297 (10)0.0004 (9)0.0028 (9)0.0016 (8)
C80.0189 (10)0.0222 (10)0.0191 (10)0.0035 (9)0.0039 (8)0.0062 (8)
C90.0185 (10)0.0277 (11)0.0143 (9)0.0012 (8)0.0003 (8)0.0027 (8)
Geometric parameters (Å, º) top
N1—C41.485 (3)C3—C41.514 (2)
N1—C11.490 (2)C3—H70.998 (19)
N1—H10.91 (2)C3—H80.97 (2)
N1—H20.979 (19)C4—H90.918 (17)
N2—C51.394 (2)C4—H100.95 (2)
N2—C31.461 (2)C5—C61.395 (2)
N2—C21.467 (2)C6—C71.365 (2)
N3—C51.345 (2)C6—H110.840 (19)
N3—C91.352 (2)C7—C81.384 (3)
C1—C21.508 (3)C7—H120.991 (19)
C1—H30.93 (2)C8—C91.371 (3)
C1—H41.00 (2)C8—H130.939 (18)
C2—H50.99 (2)C9—H140.985 (17)
C2—H60.951 (18)
C4—N1—C1110.81 (14)N2—C3—H8111.7 (11)
C4—N1—H1108.9 (12)C4—C3—H8108.5 (11)
C1—N1—H1110.2 (11)H7—C3—H8107.6 (15)
C4—N1—H2108.4 (11)N1—C4—C3110.37 (16)
C1—N1—H2112.2 (11)N1—C4—H9110.1 (12)
H1—N1—H2106.2 (15)C3—C4—H9109.3 (11)
C5—N2—C3119.17 (14)N1—C4—H10109.8 (12)
C5—N2—C2117.74 (14)C3—C4—H10110.6 (11)
C3—N2—C2112.98 (14)H9—C4—H10106.5 (17)
C5—N3—C9118.09 (15)N3—C5—N2117.13 (15)
N1—C1—C2110.24 (15)N3—C5—C6121.36 (15)
N1—C1—H3108.1 (11)N2—C5—C6121.48 (15)
C2—C1—H3110.9 (12)C7—C6—C5118.83 (16)
N1—C1—H4105.4 (10)C7—C6—H11121.8 (13)
C2—C1—H4111.3 (9)C5—C6—H11119.2 (13)
H3—C1—H4110.7 (16)C6—C7—C8120.90 (17)
N2—C2—C1110.42 (15)C6—C7—H12118.2 (10)
N2—C2—H5110.6 (11)C8—C7—H12120.9 (10)
C1—C2—H5110.0 (11)C9—C8—C7116.97 (17)
N2—C2—H6110.0 (11)C9—C8—H13119.1 (12)
C1—C2—H6110.3 (10)C7—C8—H13123.9 (12)
H5—C2—H6105.4 (16)N3—C9—C8123.80 (17)
N2—C3—C4110.76 (15)N3—C9—H14118.1 (11)
N2—C3—H7111.3 (10)C8—C9—H14118.1 (11)
C4—C3—H7106.7 (10)
C4—N1—C1—C257.5 (2)C3—N2—C5—N3163.18 (16)
C5—N2—C2—C1158.72 (16)C2—N2—C5—N320.2 (2)
C3—N2—C2—C156.1 (2)C3—N2—C5—C618.7 (3)
N1—C1—C2—N256.1 (2)C2—N2—C5—C6161.74 (17)
C5—N2—C3—C4159.81 (17)N3—C5—C6—C71.5 (3)
C2—N2—C3—C455.5 (2)N2—C5—C6—C7179.50 (18)
C1—N1—C4—C356.9 (2)C5—C6—C7—C80.5 (3)
N2—C3—C4—N155.2 (2)C6—C7—C8—C91.5 (3)
C9—N3—C5—N2178.43 (16)C5—N3—C9—C81.9 (3)
C9—N3—C5—C60.3 (3)C7—C8—C9—N32.8 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H2···Cl10.979 (19)2.15 (2)3.1020 (17)164.3 (15)
N1—H1···Cl1i0.91 (2)2.19 (2)3.0961 (17)174.3 (17)
Symmetry code: (i) x+1, y+1/2, z+1/2.

Experimental details

Crystal data
Chemical formulaC9H14ClN3
Mr199.68
Crystal system, space groupOrthorhombic, P212121
Temperature (K)100
a, b, c (Å)7.1757 (6), 7.2196 (6), 18.7629 (16)
V3)972.02 (14)
Z4
Radiation typeMo Kα
µ (mm1)0.35
Crystal size (mm)0.40 × 0.25 × 0.15
Data collection
DiffractometerBruker SMART CCD area-detector
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
5613, 1956, 1781
Rint0.044
(sin θ/λ)max1)0.625
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.029, 0.061, 0.96
No. of reflections1956
No. of parameters160
H-atom treatmentOnly H-atom coordinates refined
Δρmax, Δρmin (e Å3)0.22, 0.16
Absolute structureFlack (1983), 787 Freidel pairs
Absolute structure parameter0.04 (7)

Computer programs: SMART (Bruker, 2001), SAINT (Bruker, 2002), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 2001).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H2···Cl10.979 (19)2.15 (2)3.1020 (17)164.3 (15)
N1—H1···Cl1i0.91 (2)2.19 (2)3.0961 (17)174.3 (17)
Symmetry code: (i) x+1, y+1/2, z+1/2.
 

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds