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Zn(dabcoH)Cl3 (dabco is 1,4-bi­cyclo­[2.2.2]­octane), [ZnCl3(C6H13N2)], crystallizes as a neutral monomeric species with approximate C3 symmetry. The tetrahedrally coordinated ZnII ion has Zn-Cl distances ranging from 2.239 (2) to 2.250 (2) Å and a Zn-N distance of 2.094 (4) Å. The Cl-Zn-Cl angles are slightly larger than tetrahedral [112.44 (6)-114.38 (6)°]. The protonated aza group forms a weak interaction with a Cl atom of an adjacent mol­ecule.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536801004822/wn6008sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536801004822/wn6008Isup2.hkl
Contains datablock I

CCDC reference: 162805

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.009 Å
  • R factor = 0.031
  • wR factor = 0.077
  • Data-to-parameter ratio = 9.4

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
ABSTM_02 Alert C The ratio of Tmax/Tmin expected RT(exp) is > 1.10 Absorption corrections should be applied. Tmin and Tmax expected: 0.417 0.469 RT(exp) = 1.125 General Notes
REFLT_03 From the CIF: _diffrn_reflns_theta_max 25.00 From the CIF: _reflns_number_total 1038 Count of symmetry unique reflns 972 Completeness (_total/calc) 106.79% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 66 Fraction of Friedel pairs measured 0.068 Are heavy atom types Z>Si present yes WARNING: Large fraction of Friedel related reflns may be needed to determine absolute structure
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
1 Alert Level C = Please check

Comment top

The title compound, (I), was prepared in an attempt to make non-Jahn–Teller analogs to (dabcoH2)2Cl3[CuCl3(H2O)2]·H2O (Wei & Willett, 1996) and to (dabcoH2)CuCl4 and (dabco2)CuCl4·H2O (Wei & Willett, 2001).

Experimental top

A procedure similar to that employed in the synthesis of (dabcoH2)2Cl3[CuCl3(H2O)2]·H2O (Wei & Willett, 1996) was followed. Equimolar mixtures of the dabco ligand and ZnCl2 were dissolved in a dilute HCl solution. Colorless crystals separated out of the solution after several days of slow evaporation at room temperature. These were filtered off and air-dried.

Computing details top

Data collection: XSCANS (Siemens, 1992); cell refinement: XSCANS; data reduction: XSCANS; program(s) used to solve structure: SHELXS90 (Sheldrick, 1990); program(s) used to refine structure: SHELXL92 (Sheldrick, 1992); molecular graphics: SHELXL97 (Sheldrick, 1997); software used to prepare material for publication: SHELXL97.

Zn(1-aza-4-azinium-bicyclo[2.2.2]octane)trichloride top
Crystal data top
[ZnCl3(C6H13N2)]F(000) = 288
Mr = 284.94Dx = 1.789 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
a = 6.7475 (10) ÅCell parameters from 25 reflections
b = 12.5446 (16) Åθ = 13.5–14°
c = 6.9788 (17) ŵ = 3.03 mm1
β = 116.430 (14)°T = 293 K
V = 528.98 (17) Å3Rhomboids, colorless
Z = 20.3 × 0.3 × 0.25 mm
Data collection top
Bruker P4
diffractometer
Rint = 0.030
Radiation source: fine-focus sealed tubeθmax = 25.0°, θmin = 3.3°
Graphite monochromatorh = 17
ω scansk = 114
1317 measured reflectionsl = 87
1038 independent reflections3 standard reflections every 97 reflections
1005 reflections with I > 2σ(I) intensity decay: <1%
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)] = 0.031H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.077 w = 1/[σ2(Fo2) + (0.0523P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max < 0.001
1038 reflectionsΔρmax = 0.80 e Å3
110 parametersΔρmin = 0.56 e Å3
1 restraintAbsolute structure: Flack (1983)
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.00 (2)
Crystal data top
[ZnCl3(C6H13N2)]V = 528.98 (17) Å3
Mr = 284.94Z = 2
Monoclinic, P21Mo Kα radiation
a = 6.7475 (10) ŵ = 3.03 mm1
b = 12.5446 (16) ÅT = 293 K
c = 6.9788 (17) Å0.3 × 0.3 × 0.25 mm
β = 116.430 (14)°
Data collection top
Bruker P4
diffractometer
Rint = 0.030
1317 measured reflections3 standard reflections every 97 reflections
1038 independent reflections intensity decay: <1%
1005 reflections with I > 2σ(I)
Refinement top
R[F2 > 2σ(F2)] = 0.031H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.077Δρmax = 0.80 e Å3
S = 1.08Δρmin = 0.56 e Å3
1038 reflectionsAbsolute structure: Flack (1983)
110 parametersAbsolute structure parameter: 0.00 (2)
1 restraint
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 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) top
xyzUiso*/Ueq
Zn0.43560 (8)0.88492 (5)0.29074 (8)0.0255 (2)
Cl10.7743 (2)0.83248 (13)0.5277 (2)0.0355 (3)
Cl20.2905 (2)1.01529 (12)0.4079 (2)0.0353 (3)
Cl30.4150 (3)0.92037 (13)0.0336 (2)0.0430 (4)
C80.1499 (9)0.5639 (5)0.1314 (10)0.0340 (13)
H8A0.24590.50720.21780.041*
H8B0.07400.53960.01560.041*
C70.2853 (10)0.6642 (5)0.1460 (9)0.0303 (12)
H7A0.25910.68550.00310.036*
H7B0.44150.64790.22640.036*
C20.0077 (8)0.7823 (5)0.1193 (8)0.0309 (12)
H2A0.04960.83760.19140.037*
H2B0.02780.81010.01790.037*
C50.2563 (9)0.7170 (5)0.4636 (8)0.0295 (12)
H5A0.40880.69550.54920.035*
H5B0.22490.77560.53640.035*
C60.1057 (10)0.6247 (5)0.4461 (10)0.0382 (14)
H6A0.00070.64530.49930.046*
H6B0.19170.56490.53040.046*
N10.2286 (7)0.7538 (4)0.2503 (6)0.0227 (9)
C30.1564 (10)0.6847 (5)0.0838 (12)0.0458 (17)
H3A0.22770.66600.06680.055*
H3B0.27040.70040.12840.055*
N40.0151 (8)0.5936 (4)0.2132 (9)0.0399 (12)
H4A0.10320.53650.20000.048*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Zn0.0272 (3)0.0177 (3)0.0334 (3)0.0013 (3)0.0152 (2)0.0005 (3)
Cl10.0289 (6)0.0310 (7)0.0419 (6)0.0043 (6)0.0115 (5)0.0035 (6)
Cl20.0381 (7)0.0252 (7)0.0433 (7)0.0040 (6)0.0186 (6)0.0059 (6)
Cl30.0510 (8)0.0456 (9)0.0426 (6)0.0143 (7)0.0301 (6)0.0166 (6)
C80.033 (3)0.020 (3)0.052 (3)0.001 (2)0.022 (2)0.006 (3)
C70.037 (3)0.023 (3)0.040 (3)0.000 (3)0.026 (2)0.006 (2)
C20.023 (2)0.027 (3)0.035 (3)0.000 (2)0.005 (2)0.003 (2)
C50.033 (3)0.031 (3)0.024 (2)0.000 (3)0.012 (2)0.004 (2)
C60.052 (4)0.025 (3)0.052 (3)0.007 (3)0.037 (3)0.000 (3)
N10.024 (2)0.018 (2)0.028 (2)0.0003 (19)0.0136 (16)0.0012 (18)
C30.023 (3)0.033 (4)0.072 (4)0.003 (3)0.013 (3)0.016 (3)
N40.033 (3)0.020 (2)0.072 (4)0.008 (2)0.027 (2)0.007 (2)
Geometric parameters (Å, º) top
Zn—N12.094 (4)C2—N11.486 (6)
Zn—Cl22.2394 (15)C2—C31.532 (9)
Zn—Cl12.2418 (14)C5—N11.489 (6)
Zn—Cl32.2495 (15)C5—C61.509 (8)
C8—N41.506 (7)C6—N41.510 (8)
C8—C71.531 (8)C3—N41.505 (9)
C7—N11.479 (7)
N1—Zn—Cl2104.43 (12)C7—N1—C2108.8 (4)
N1—Zn—Cl1105.59 (13)C7—N1—C5108.1 (4)
Cl2—Zn—Cl1114.38 (6)C2—N1—C5108.2 (4)
N1—Zn—Cl3106.31 (12)C7—N1—Zn111.1 (3)
Cl2—Zn—Cl3112.44 (6)C2—N1—Zn111.2 (3)
Cl1—Zn—Cl3112.73 (6)C5—N1—Zn109.2 (3)
N4—C8—C7106.9 (5)N4—C3—C2108.4 (5)
N1—C7—C8112.3 (4)C3—N4—C8109.8 (5)
N1—C2—C3110.7 (5)C3—N4—C6110.2 (5)
N1—C5—C6112.1 (4)C8—N4—C6109.6 (5)
N4—C6—C5107.8 (5)
N4—C8—C7—N15.0 (7)Cl2—Zn—N1—C251.2 (3)
N1—C5—C6—N44.2 (6)Cl1—Zn—N1—C2172.2 (3)
C8—C7—N1—C262.1 (6)Cl3—Zn—N1—C267.9 (3)
C8—C7—N1—C555.3 (6)Cl2—Zn—N1—C568.2 (3)
C8—C7—N1—Zn175.1 (4)Cl1—Zn—N1—C552.8 (3)
C3—C2—N1—C755.1 (6)Cl3—Zn—N1—C5172.7 (3)
C3—C2—N1—C562.2 (6)N1—C2—C3—N45.7 (7)
C3—C2—N1—Zn177.8 (4)C2—C3—N4—C864.2 (6)
C6—C5—N1—C760.9 (5)C2—C3—N4—C656.6 (7)
C6—C5—N1—C256.8 (6)C7—C8—N4—C357.6 (6)
C6—C5—N1—Zn178.0 (4)C7—C8—N4—C663.5 (6)
Cl2—Zn—N1—C7172.6 (3)C5—C6—N4—C362.3 (6)
Cl1—Zn—N1—C766.5 (3)C5—C6—N4—C858.6 (6)
Cl3—Zn—N1—C753.5 (3)

Experimental details

Crystal data
Chemical formula[ZnCl3(C6H13N2)]
Mr284.94
Crystal system, space groupMonoclinic, P21
Temperature (K)293
a, b, c (Å)6.7475 (10), 12.5446 (16), 6.9788 (17)
β (°) 116.430 (14)
V3)528.98 (17)
Z2
Radiation typeMo Kα
µ (mm1)3.03
Crystal size (mm)0.3 × 0.3 × 0.25
Data collection
DiffractometerBruker P4
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
1317, 1038, 1005
Rint0.030
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.031, 0.077, 1.08
No. of reflections1038
No. of parameters110
No. of restraints1
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.80, 0.56
Absolute structureFlack (1983)
Absolute structure parameter0.00 (2)

Computer programs: XSCANS (Siemens, 1992), XSCANS, SHELXS90 (Sheldrick, 1990), SHELXL92 (Sheldrick, 1992), SHELXL97 (Sheldrick, 1997), SHELXL97.

 

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