Literature DB >> 21583803

1,4-Diazo-niabicyclo-[2.2.2]octane tetra-chloridozincate monohydrate.

Fangming Wang1.   

Abstract

In the title compound, (C(6)H(14)N(2))[ZnCl(4)]·H(2)O, the crystal packing is governed by an extensive three-dimensional network of N-H⋯Cl, N-H⋯O and O-H⋯Cl hydrogen bonds. The zinc(II) metal centre has a slightly distorted tetra-hedral coordination geometry.

Entities:  

Year:  2009        PMID: 21583803      PMCID: PMC2977617          DOI: 10.1107/S1600536809014822

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


Related literature

For the applications of ferroelectric materials, see: Fu et al. (2007 ▶); Dawber et al. (2005 ▶); Haertling (1999 ▶); Scott (2007 ▶). For the properties and structure of a related diaza­bicyclo­[2.2.2]octane (dabco) salt, see: Szafrański et al. (2002 ▶).

Experimental

Crystal data

(C6H14N2)[ZnCl4]·H2O M = 339.40 Orthorhombic, a = 8.4483 (17) Å b = 11.705 (2) Å c = 12.976 (3) Å V = 1283.2 (5) Å3 Z = 4 Mo Kα radiation μ = 2.72 mm−1 T = 291 K 0.30 × 0.28 × 0.26 mm

Data collection

Rigaku Mercury2 diffractometer Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.462, T max = 0.495 11890 measured reflections 2510 independent reflections 2166 reflections with I > 2σ(I) R int = 0.053

Refinement

R[F 2 > 2σ(F 2)] = 0.046 wR(F 2) = 0.121 S = 1.03 2510 reflections 127 parameters H-atom parameters constrained Δρmax = 0.89 e Å−3 Δρmin = −0.48 e Å−3 Absolute structure: Flack (1983 ▶), 1050 Friedel pairs Flack parameter: 0.07 (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: SHELXTL. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809014822/rz2310sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809014822/rz2310Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
(C6H14N2)[ZnCl4]·H2OF(000) = 688
Mr = 339.40Dx = 1.757 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 11517 reflections
a = 8.4483 (17) Åθ = 3.1–27.5°
b = 11.705 (2) ŵ = 2.72 mm1
c = 12.976 (3) ÅT = 291 K
V = 1283.2 (5) Å3Block, colourless
Z = 40.30 × 0.28 × 0.26 mm
Rigaku Mercury2 diffractometer2510 independent reflections
Radiation source: fine-focus sealed tube2166 reflections with I > 2σ(I)
graphiteRint = 0.053
Detector resolution: 13.6612 pixels mm-1θmax = 26.0°, θmin = 3.1°
ω scansh = −10→10
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005)k = −14→14
Tmin = 0.462, Tmax = 0.495l = −16→16
11890 measured reflections
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.046H-atom parameters constrained
wR(F2) = 0.121w = 1/[σ2(Fo2) + (0.0665P)2 + 1.4482P] where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.001
2510 reflectionsΔρmax = 0.89 e Å3
127 parametersΔρmin = −0.48 e Å3
0 restraintsAbsolute structure: Flack (1983), 1050 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: 0.07 (3)
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
C10.2122 (7)0.3775 (6)0.3733 (5)0.0434 (17)
H1A0.16100.31890.41430.052*
H1B0.23470.44220.41770.052*
C20.3645 (8)0.3316 (7)0.3286 (5)0.0489 (18)
H2A0.36760.24900.33470.059*
H2B0.45470.36320.36500.059*
C30.1700 (9)0.5158 (6)0.2364 (5)0.0415 (16)
H3A0.16550.58090.28260.050*
H3B0.10640.53300.17610.050*
C40.3402 (8)0.4934 (6)0.2046 (6)0.0474 (18)
H4A0.35680.51670.13360.057*
H4B0.41230.53610.24820.057*
C50.0884 (7)0.3177 (5)0.2132 (5)0.0371 (15)
H5A0.00550.33560.16410.045*
H5B0.06020.24770.24870.045*
C60.2468 (8)0.3030 (5)0.1574 (4)0.0405 (14)
H6A0.27450.22270.15360.049*
H6B0.23940.33280.08780.049*
Cl10.20057 (18)−0.18534 (13)1.07634 (13)0.0420 (4)
Cl20.2573 (2)−0.03346 (13)0.81713 (10)0.0444 (4)
Cl30.03672 (18)0.09791 (13)1.03379 (13)0.0371 (4)
Cl40.47943 (19)0.06684 (14)1.03500 (14)0.0414 (4)
N10.1070 (6)0.4132 (4)0.2888 (4)0.0308 (11)
H1C0.01030.43030.31560.037*
N20.3689 (6)0.3664 (5)0.2161 (5)0.0444 (15)
H2C0.46590.34930.18990.053*
O10.6587 (8)0.2561 (5)0.1794 (5)0.086 (2)
H1D0.68490.26590.11670.128*
H1E0.72930.28450.21840.128*
Zn10.24738 (9)−0.01799 (5)0.99321 (4)0.0333 (2)
U11U22U33U12U13U23
C10.043 (4)0.054 (4)0.033 (3)0.007 (3)−0.009 (3)−0.004 (3)
C20.042 (4)0.052 (4)0.052 (4)0.006 (3)−0.020 (3)−0.008 (4)
C30.044 (4)0.031 (3)0.050 (4)0.005 (3)0.005 (3)0.003 (3)
C40.036 (4)0.054 (4)0.053 (4)−0.011 (3)0.012 (3)−0.010 (4)
C50.038 (3)0.037 (4)0.037 (3)−0.003 (3)−0.004 (3)0.003 (3)
C60.034 (3)0.043 (3)0.045 (3)−0.007 (3)−0.007 (3)−0.018 (3)
Cl10.0443 (9)0.0383 (8)0.0435 (8)0.0001 (7)0.0069 (6)0.0048 (7)
Cl20.0477 (9)0.0536 (9)0.0318 (7)−0.0048 (9)0.0041 (8)−0.0058 (6)
Cl30.0322 (8)0.0407 (8)0.0384 (9)0.0023 (6)0.0004 (7)−0.0041 (7)
Cl40.0368 (8)0.0459 (8)0.0414 (9)−0.0079 (7)−0.0055 (7)0.0029 (8)
N10.022 (2)0.042 (3)0.029 (3)0.004 (2)0.0009 (19)−0.002 (2)
N20.022 (3)0.051 (3)0.061 (4)0.003 (2)0.004 (2)−0.018 (3)
O10.067 (4)0.083 (5)0.106 (5)0.004 (4)−0.014 (4)−0.001 (4)
Zn10.0317 (3)0.0375 (3)0.0307 (3)−0.0011 (3)0.0009 (3)0.0002 (3)
C1—N11.472 (7)C5—C61.531 (9)
C1—C21.510 (9)C5—H5A0.9700
C1—H1A0.9700C5—H5B0.9700
C1—H1B0.9700C6—N21.482 (8)
C2—N21.515 (9)C6—H6A0.9700
C2—H2A0.9700C6—H6B0.9700
C2—H2B0.9700Cl1—Zn12.2710 (17)
C3—N11.479 (8)Cl2—Zn12.2936 (15)
C3—C41.519 (9)Cl3—Zn12.2989 (17)
C3—H3A0.9700Cl4—Zn12.2635 (17)
C3—H3B0.9700N1—H1C0.9100
C4—N21.514 (9)N2—H2C0.9100
C4—H4A0.9700O1—H1D0.8499
C4—H4B0.9700O1—H1E0.8500
C5—N11.496 (8)
N1—C1—C2109.2 (5)C6—C5—H5B110.2
N1—C1—H1A109.8H5A—C5—H5B108.5
C2—C1—H1A109.8N2—C6—C5108.0 (5)
N1—C1—H1B109.8N2—C6—H6A110.1
C2—C1—H1B109.8C5—C6—H6A110.1
H1A—C1—H1B108.3N2—C6—H6B110.1
C1—C2—N2107.2 (5)C5—C6—H6B110.1
C1—C2—H2A110.3H6A—C6—H6B108.4
N2—C2—H2A110.3C1—N1—C3110.8 (5)
C1—C2—H2B110.3C1—N1—C5109.9 (5)
N2—C2—H2B110.3C3—N1—C5110.1 (5)
H2A—C2—H2B108.5C1—N1—H1C108.7
N1—C3—C4109.0 (5)C3—N1—H1C108.7
N1—C3—H3A109.9C5—N1—H1C108.7
C4—C3—H3A109.9C6—N2—C4109.2 (5)
N1—C3—H3B109.9C6—N2—C2110.1 (5)
C4—C3—H3B109.9C4—N2—C2110.8 (5)
H3A—C3—H3B108.3C6—N2—H2C108.9
N2—C4—C3107.1 (5)C4—N2—H2C108.9
N2—C4—H4A110.3C2—N2—H2C108.9
C3—C4—H4A110.3H1D—O1—H1E109.5
N2—C4—H4B110.3Cl4—Zn1—Cl1114.55 (7)
C3—C4—H4B110.3Cl4—Zn1—Cl2103.99 (7)
H4A—C4—H4B108.5Cl1—Zn1—Cl2114.29 (6)
N1—C5—C6107.6 (5)Cl4—Zn1—Cl3110.90 (6)
N1—C5—H5A110.2Cl1—Zn1—Cl3105.40 (6)
C6—C5—H5A110.2Cl2—Zn1—Cl3107.63 (7)
N1—C5—H5B110.2
D—H···AD—HH···AD···AD—H···A
N2—H2C···O10.911.962.809 (8)154
N1—H1C···Cl1i0.912.643.338 (5)134
N1—H1C···Cl3i0.912.803.383 (5)123
O1—H1D···Cl3ii0.852.823.410 (7)129
O1—H1E···Cl1iii0.852.753.454 (7)141
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N2—H2C⋯O10.911.962.809 (8)154
N1—H1C⋯Cl1i0.912.643.338 (5)134
N1—H1C⋯Cl3i0.912.803.383 (5)123
O1—H1D⋯Cl3ii0.852.823.410 (7)129
O1—H1E⋯Cl1iii0.852.753.454 (7)141

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

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