Literature DB >> 21583517

Redetermination of 3-(ammonio-meth-yl)pyridinium dichloride.

Wen-Xian Liang1, Gang Wang, Zhi-Rong Qu.   

Abstract

The crystal structure of the title compound, C(6)H(10)N(2) (2+)·2Cl(-), has been reported previously in the non-standard setting P2(1)/a [Genet (1965 ▶). Bull. Soc. Fr. Miner. Crist.88, 463-470], with an R value of 0.16. The current redetermination improves significantly the precision of the geometric parameters. In the crystal packing, cations and anions are linked by inter-molecular N-H⋯Cl and C-H⋯Cl hydrogen bonds into a three-dimensional network.

Entities:  

Year:  2009        PMID: 21583517      PMCID: PMC2977397          DOI: 10.1107/S1600536809025859

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For related structures, see: Genet (1965 ▶); Chtioui & Jouini (2004 ▶); Long et al. (1997 ▶).

Experimental

Crystal data

C6H10N2 2+·2Cl− M = 181.06 Monoclinic, a = 4.5874 (9) Å b = 12.650 (3) Å c = 14.814 (3) Å β = 93.61 (3)° V = 857.9 (3) Å3 Z = 4 Mo Kα radiation μ = 0.69 mm−1 T = 293 K 0.50 × 0.45 × 0.15 mm

Data collection

Rigaku SCXmini diffractometer Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.720, T max = 0.909 8831 measured reflections 1961 independent reflections 1684 reflections with I > 2σ(I) R int = 0.035

Refinement

R[F 2 > 2σ(F 2)] = 0.033 wR(F 2) = 0.076 S = 1.08 1961 reflections 92 parameters H-atom parameters constrained Δρmax = 0.21 e Å−3 Δρmin = −0.19 e Å−3 Data collection: CrystalClear (Rigaku, 2005 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: PRPKAPPA (Ferguson, 1999 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809025859/rz2346sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809025859/rz2346Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C6H10N22+·2ClF(000) = 376
Mr = 181.06Dx = 1.402 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 8048 reflections
a = 4.5874 (9) Åθ = 3.1–27.5°
b = 12.650 (3) ŵ = 0.69 mm1
c = 14.814 (3) ÅT = 293 K
β = 93.61 (3)°Prism, colourless
V = 857.9 (3) Å30.50 × 0.45 × 0.15 mm
Z = 4
Rigaku SCXmini diffractometer1961 independent reflections
Radiation source: fine-focus sealed tube1684 reflections with I > 2σ(I)
graphiteRint = 0.035
Detector resolution: 13.662 pixels mm-1θmax = 27.5°, θmin = 3.2°
CCD_Profile_fitting scansh = −5→5
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005)k = −16→16
Tmin = 0.720, Tmax = 0.909l = −19→19
8831 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.033Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.076H-atom parameters constrained
S = 1.08w = 1/[σ2(Fo2) + (0.0293P)2 + 0.274P] where P = (Fo2 + 2Fc2)/3
1961 reflections(Δ/σ)max = 0.001
92 parametersΔρmax = 0.21 e Å3
0 restraintsΔρmin = −0.19 e Å3
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.
xyzUiso*/Ueq
Cl20.34023 (9)0.98847 (3)0.37672 (3)0.03348 (13)
N10.9075 (3)0.64924 (10)−0.01920 (10)0.0333 (3)
H1A0.78850.60980.01200.050*
H1B0.99050.6091−0.05980.050*
H1C0.80580.7007−0.04740.050*
C61.1364 (4)0.69588 (14)0.04332 (13)0.0365 (4)
H6A1.28880.72530.00840.044*
H6B1.22310.64050.08150.044*
C11.1087 (4)0.88417 (13)0.08977 (12)0.0337 (4)
H11.23490.90000.04490.040*
C50.8274 (4)0.94441 (14)0.20641 (12)0.0370 (4)
H50.76191.00050.24030.044*
C21.0214 (3)0.78119 (13)0.10227 (11)0.0293 (4)
C40.7351 (4)0.84350 (14)0.22213 (12)0.0371 (4)
H40.60600.83040.26680.045*
C30.8357 (4)0.76140 (14)0.17102 (12)0.0349 (4)
H30.77880.69240.18260.042*
Cl10.40819 (11)0.14752 (3)0.10233 (3)0.04427 (15)
N21.0124 (3)0.96146 (11)0.14194 (10)0.0367 (4)
H21.07241.02490.13360.044*
U11U22U33U12U13U23
Cl20.0384 (2)0.0291 (2)0.0340 (2)−0.00167 (16)0.01032 (17)−0.00133 (16)
N10.0389 (8)0.0256 (7)0.0362 (8)0.0047 (6)0.0099 (6)−0.0021 (6)
C60.0310 (9)0.0315 (9)0.0479 (11)0.0040 (7)0.0086 (8)−0.0028 (8)
C10.0347 (9)0.0314 (9)0.0352 (9)0.0001 (7)0.0041 (7)0.0029 (7)
C50.0440 (10)0.0354 (10)0.0311 (9)0.0044 (8)−0.0011 (8)−0.0071 (7)
C20.0260 (8)0.0284 (8)0.0331 (9)0.0020 (6)−0.0008 (7)−0.0010 (7)
C40.0406 (10)0.0407 (10)0.0306 (9)−0.0030 (8)0.0064 (8)−0.0032 (7)
C30.0390 (10)0.0297 (9)0.0363 (10)−0.0038 (7)0.0044 (8)0.0005 (7)
Cl10.0486 (3)0.0305 (2)0.0547 (3)0.00301 (18)0.0108 (2)0.00943 (19)
N20.0462 (9)0.0237 (7)0.0397 (9)−0.0029 (6)−0.0014 (7)0.0013 (6)
N1—C61.478 (2)C1—H10.9300
N1—H1A0.8900C5—N21.334 (2)
N1—H1B0.8900C5—C41.369 (3)
N1—H1C0.8900C5—H50.9300
C6—C21.504 (2)C2—C31.391 (2)
C6—H6A0.9700C4—C31.382 (2)
C6—H6B0.9700C4—H40.9300
C1—N21.338 (2)C3—H30.9300
C1—C21.379 (2)N2—H20.8600
C6—N1—H1A109.5N2—C5—C4119.33 (16)
C6—N1—H1B109.5N2—C5—H5120.3
H1A—N1—H1B109.5C4—C5—H5120.3
C6—N1—H1C109.5C1—C2—C3117.69 (16)
H1A—N1—H1C109.5C1—C2—C6118.97 (16)
H1B—N1—H1C109.5C3—C2—C6123.31 (15)
N1—C6—C2112.88 (13)C5—C4—C3119.34 (17)
N1—C6—H6A109.0C5—C4—H4120.3
C2—C6—H6A109.0C3—C4—H4120.3
N1—C6—H6B109.0C4—C3—C2120.47 (16)
C2—C6—H6B109.0C4—C3—H3119.8
H6A—C6—H6B107.8C2—C3—H3119.8
N2—C1—C2120.23 (16)C5—N2—C1122.89 (15)
N2—C1—H1119.9C5—N2—H2118.6
C2—C1—H1119.9C1—N2—H2118.6
D—H···AD—HH···AD···AD—H···A
N1—H1A···Cl2i0.892.353.1914 (16)157
N1—H1B···Cl2ii0.892.273.1206 (16)159
N1—H1C···Cl1iii0.892.283.1622 (16)170
N2—H2···Cl1iv0.862.253.0520 (16)154
C3—H3···Cl2i0.932.773.606 (2)150
C6—H6A···Cl1v0.972.743.676 (2)163
C6—H6B···Cl2vi0.972.823.700 (2)152
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N1—H1A⋯Cl2i0.892.353.1914 (16)157
N1—H1B⋯Cl2ii0.892.273.1206 (16)159
N1—H1C⋯Cl1iii0.892.283.1622 (16)170
N2—H2⋯Cl1iv0.862.253.0520 (16)154
C3—H3⋯Cl2i0.932.773.606 (2)150
C6—H6A⋯Cl1v0.972.743.676 (2)163
C6—H6B⋯Cl2vi0.972.823.700 (2)152

Symmetry codes: (i) ; (ii) ; (iii) ; (iv) ; (v) ; (vi) .

  2 in total

1.  Crystal Structures and Magnetic Properties of a Novel Layer Perovskite System: (3-Picoliniumylammonium)CuX(4) (X = Cl, Br).

Authors:  Greg S. Long; Mingyi Wei; Roger D. Willett
Journal:  Inorg Chem       Date:  1997-07-02       Impact factor: 5.165

2.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

  2 in total

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