metal-organic compounds
Bis(N,N-diisopropylbutanaminium) bis[di-μ-chlorido-bis[dichloridocuprate(II)]]
aOrdered Matter Science Research Center, College of Chemistry and Chemical Engineering, Southeast University, Nanjing 210096, People's Republic of China
*Correspondence e-mail: fudavid88@yahoo.com.cn
In the title compound, (C10H24N)2[Cu2Cl6], N,N-diisopropylbutanamine is protonated on the N atom. The CuII atom in the centrosymmetric [Cu2Cl6]2− anion has a distorted tetrahedral geometry. In the crystal, the cations and anions are connected by N—H⋯Cl and C—H⋯Cl hydrogen bonds into layers parallel to (100).
Related literature
For the properties and structures of N,N-diisopropylbutyl-1-amine compounds, see: Fu et al. (2007, 2008, 2009); Fu & Xiong (2008).
Experimental
Crystal data
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Refinement
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Data collection: CrystalClear (Rigaku, 2005); cell 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) and Mercury (Macrae et al., 2006); software used to prepare material for publication: SHELXTL.
Supporting information
10.1107/S1600536810054280/hy2392sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536810054280/hy2392Isup2.hkl
The commercial N,N-diisopropylbutyl-1-amine (10 mmol), HCl (2 ml) and CuCl2 (5 mmol) were dissolved in 10 ml water. The solvent was slowly evaporated in air, affording blue block-shaped crystals of the title compound suitable for X-ray analysis.
The
of the title compound as a function of temperature indicates that the permittivity is basically temperature-independent, suggesting that this compound should not be a real or there may be no distinct occurred within the measured temperature range. Similarly, below the melting point (446–447 K) of the compound, the as a function of temperature also goes smoothly, and there is no dielectric anomaly observed (dielectric constant equaling to 8.9 to 10.6).H atoms were positioned geometrically and treated as riding, with C—H = 0.98 (CH), 0.97 (CH2) and 0.96 (CH3) Å and N—H = 0.91 Å and with Uiso(H) = 1.2(1.5 for methyl)Ueq(C, N).
Data collection: CrystalClear (Rigaku, 2005); cell
CrystalClear (Rigaku, 2005); data reduction: CrystalClear (Rigaku, 2005); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008) and Mercury (Macrae et al., 2006); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).(C10H24N)2[Cu2Cl6] | Z = 1 |
Mr = 656.40 | F(000) = 342 |
Triclinic, P1 | Dx = 1.388 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 8.5697 (17) Å | Cell parameters from 3588 reflections |
b = 10.213 (2) Å | θ = 3.4–27.5° |
c = 10.384 (2) Å | µ = 1.88 mm−1 |
α = 72.43 (3)° | T = 298 K |
β = 68.53 (3)° | Block, blue |
γ = 71.78 (3)° | 0.30 × 0.05 × 0.05 mm |
V = 785.1 (3) Å3 |
Rigaku Mercury2 CCD diffractometer | 3588 independent reflections |
Radiation source: fine-focus sealed tube | 2728 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.044 |
Detector resolution: 13.6612 pixels mm-1 | θmax = 27.5°, θmin = 3.4° |
ω scans | h = −11→11 |
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | k = −13→13 |
Tmin = 0.910, Tmax = 1.000 | l = −13→13 |
8206 measured reflections |
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)] = 0.046 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.107 | H-atom parameters constrained |
S = 1.08 | w = 1/[σ2(Fo2) + (0.0342P)2 + 0.4528P] where P = (Fo2 + 2Fc2)/3 |
3588 reflections | (Δ/σ)max < 0.001 |
141 parameters | Δρmax = 0.45 e Å−3 |
0 restraints | Δρmin = −0.52 e Å−3 |
(C10H24N)2[Cu2Cl6] | γ = 71.78 (3)° |
Mr = 656.40 | V = 785.1 (3) Å3 |
Triclinic, P1 | Z = 1 |
a = 8.5697 (17) Å | Mo Kα radiation |
b = 10.213 (2) Å | µ = 1.88 mm−1 |
c = 10.384 (2) Å | T = 298 K |
α = 72.43 (3)° | 0.30 × 0.05 × 0.05 mm |
β = 68.53 (3)° |
Rigaku Mercury2 CCD diffractometer | 3588 independent reflections |
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | 2728 reflections with I > 2σ(I) |
Tmin = 0.910, Tmax = 1.000 | Rint = 0.044 |
8206 measured reflections |
R[F2 > 2σ(F2)] = 0.046 | 0 restraints |
wR(F2) = 0.107 | H-atom parameters constrained |
S = 1.08 | Δρmax = 0.45 e Å−3 |
3588 reflections | Δρmin = −0.52 e Å−3 |
141 parameters |
x | y | z | Uiso*/Ueq | ||
N1 | 0.7275 (3) | 0.3131 (3) | 0.7043 (3) | 0.0374 (6) | |
H1 | 0.7197 | 0.4066 | 0.6644 | 0.045* | |
C1 | 0.5308 (7) | 0.1423 (5) | 0.8060 (6) | 0.0907 (17) | |
H1A | 0.4248 | 0.1297 | 0.8051 | 0.136* | |
H1B | 0.5300 | 0.1267 | 0.9021 | 0.136* | |
H1C | 0.6256 | 0.0761 | 0.7589 | 0.136* | |
Cu1 | 0.55821 (5) | 0.83754 (4) | 0.59096 (4) | 0.03888 (14) | |
Cl1 | 0.30886 (11) | 1.01180 (9) | 0.60170 (11) | 0.0629 (3) | |
C2 | 0.5495 (4) | 0.2903 (4) | 0.7304 (4) | 0.0510 (9) | |
H2A | 0.5344 | 0.3062 | 0.6374 | 0.061* | |
Cl2 | 0.50922 (16) | 0.75177 (13) | 0.81673 (10) | 0.0778 (4) | |
C3 | 0.4106 (5) | 0.3995 (5) | 0.8062 (5) | 0.0680 (12) | |
H3A | 0.3011 | 0.4003 | 0.8002 | 0.102* | |
H3B | 0.4357 | 0.4909 | 0.7625 | 0.102* | |
H3C | 0.4069 | 0.3766 | 0.9038 | 0.102* | |
Cl3 | 0.70329 (12) | 0.64171 (9) | 0.51116 (9) | 0.0505 (2) | |
C4 | 0.8746 (6) | 0.4013 (5) | 0.8158 (4) | 0.0663 (12) | |
H4A | 0.8994 | 0.3922 | 0.9015 | 0.099* | |
H4B | 0.8065 | 0.4941 | 0.7912 | 0.099* | |
H4C | 0.9805 | 0.3864 | 0.7407 | 0.099* | |
C5 | 0.7756 (4) | 0.2922 (4) | 0.8379 (4) | 0.0449 (8) | |
H5A | 0.6679 | 0.3114 | 0.9140 | 0.054* | |
C6 | 0.8723 (6) | 0.1434 (4) | 0.8862 (4) | 0.0707 (13) | |
H6A | 0.8802 | 0.1331 | 0.9787 | 0.106* | |
H6B | 0.9860 | 0.1261 | 0.8209 | 0.106* | |
H6C | 0.8119 | 0.0771 | 0.8894 | 0.106* | |
C7 | 0.8673 (4) | 0.2391 (4) | 0.5948 (3) | 0.0447 (8) | |
H7A | 0.8709 | 0.1389 | 0.6258 | 0.054* | |
H7B | 0.9768 | 0.2520 | 0.5902 | 0.054* | |
C8 | 0.8484 (5) | 0.2876 (4) | 0.4479 (3) | 0.0452 (8) | |
H8A | 0.8366 | 0.3890 | 0.4183 | 0.054* | |
H8B | 0.7446 | 0.2670 | 0.4494 | 0.054* | |
C9 | 1.0015 (5) | 0.2162 (4) | 0.3426 (4) | 0.0565 (10) | |
H9A | 1.1046 | 0.2375 | 0.3417 | 0.068* | |
H9B | 1.0137 | 0.1149 | 0.3740 | 0.068* | |
C10 | 0.9891 (6) | 0.2596 (5) | 0.1937 (4) | 0.0698 (12) | |
H10A | 1.0904 | 0.2107 | 0.1328 | 0.105* | |
H10B | 0.9796 | 0.3595 | 0.1607 | 0.105* | |
H10C | 0.8893 | 0.2364 | 0.1929 | 0.105* |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1 | 0.0384 (15) | 0.0359 (14) | 0.0347 (15) | −0.0041 (11) | −0.0109 (12) | −0.0078 (12) |
C1 | 0.083 (3) | 0.072 (3) | 0.124 (5) | −0.045 (3) | −0.018 (3) | −0.016 (3) |
Cu1 | 0.0400 (2) | 0.0323 (2) | 0.0370 (2) | −0.00387 (16) | −0.00747 (17) | −0.00665 (17) |
Cl1 | 0.0393 (5) | 0.0424 (5) | 0.0699 (7) | −0.0006 (4) | 0.0065 (4) | 0.0027 (4) |
C2 | 0.043 (2) | 0.066 (2) | 0.047 (2) | −0.0150 (18) | −0.0124 (17) | −0.0148 (19) |
Cl2 | 0.0893 (8) | 0.0808 (8) | 0.0353 (5) | −0.0012 (6) | −0.0073 (5) | −0.0061 (5) |
C3 | 0.040 (2) | 0.084 (3) | 0.070 (3) | −0.007 (2) | −0.009 (2) | −0.019 (2) |
Cl3 | 0.0628 (6) | 0.0332 (4) | 0.0488 (5) | −0.0008 (4) | −0.0151 (4) | −0.0118 (4) |
C4 | 0.073 (3) | 0.083 (3) | 0.058 (3) | −0.023 (2) | −0.031 (2) | −0.017 (2) |
C5 | 0.0412 (19) | 0.053 (2) | 0.0355 (19) | −0.0014 (16) | −0.0136 (15) | −0.0097 (16) |
C6 | 0.084 (3) | 0.065 (3) | 0.054 (3) | 0.011 (2) | −0.039 (2) | −0.005 (2) |
C7 | 0.0429 (19) | 0.0426 (19) | 0.042 (2) | 0.0019 (15) | −0.0118 (16) | −0.0134 (16) |
C8 | 0.051 (2) | 0.0408 (19) | 0.044 (2) | −0.0037 (16) | −0.0172 (17) | −0.0138 (16) |
C9 | 0.057 (2) | 0.062 (2) | 0.046 (2) | −0.0047 (19) | −0.0102 (18) | −0.0212 (19) |
C10 | 0.081 (3) | 0.083 (3) | 0.049 (2) | −0.017 (2) | −0.012 (2) | −0.030 (2) |
N1—C7 | 1.501 (4) | C4—H4B | 0.9600 |
N1—C5 | 1.525 (4) | C4—H4C | 0.9600 |
N1—C2 | 1.528 (4) | C5—C6 | 1.518 (5) |
N1—H1 | 0.9100 | C5—H5A | 0.9800 |
C1—C2 | 1.506 (5) | C6—H6A | 0.9600 |
C1—H1A | 0.9600 | C6—H6B | 0.9600 |
C1—H1B | 0.9600 | C6—H6C | 0.9600 |
C1—H1C | 0.9600 | C7—C8 | 1.508 (4) |
Cu1—Cl2 | 2.1701 (13) | C7—H7A | 0.9700 |
Cu1—Cl3 | 2.2190 (12) | C7—H7B | 0.9700 |
Cu1—Cl1i | 2.2884 (14) | C8—C9 | 1.511 (5) |
Cu1—Cl1 | 2.3051 (13) | C8—H8A | 0.9700 |
Cl1—Cu1i | 2.2884 (14) | C8—H8B | 0.9700 |
C2—C3 | 1.515 (5) | C9—C10 | 1.509 (5) |
C2—H2A | 0.9800 | C9—H9A | 0.9700 |
C3—H3A | 0.9600 | C9—H9B | 0.9700 |
C3—H3B | 0.9600 | C10—H10A | 0.9600 |
C3—H3C | 0.9600 | C10—H10B | 0.9600 |
C4—C5 | 1.519 (5) | C10—H10C | 0.9600 |
C4—H4A | 0.9600 | ||
C7—N1—C5 | 113.3 (2) | C6—C5—C4 | 111.9 (3) |
C7—N1—C2 | 113.5 (3) | C6—C5—N1 | 113.9 (3) |
C5—N1—C2 | 114.8 (3) | C4—C5—N1 | 109.1 (3) |
C7—N1—H1 | 104.6 | C6—C5—H5A | 107.2 |
C5—N1—H1 | 104.6 | C4—C5—H5A | 107.2 |
C2—N1—H1 | 104.6 | N1—C5—H5A | 107.2 |
C2—C1—H1A | 109.5 | C5—C6—H6A | 109.5 |
C2—C1—H1B | 109.5 | C5—C6—H6B | 109.5 |
H1A—C1—H1B | 109.5 | H6A—C6—H6B | 109.5 |
C2—C1—H1C | 109.5 | C5—C6—H6C | 109.5 |
H1A—C1—H1C | 109.5 | H6A—C6—H6C | 109.5 |
H1B—C1—H1C | 109.5 | H6B—C6—H6C | 109.5 |
Cl2—Cu1—Cl3 | 99.48 (5) | N1—C7—C8 | 115.2 (3) |
Cl2—Cu1—Cl1i | 146.21 (6) | N1—C7—H7A | 108.5 |
Cl3—Cu1—Cl1i | 96.22 (5) | C8—C7—H7A | 108.5 |
Cl2—Cu1—Cl1 | 97.69 (6) | N1—C7—H7B | 108.5 |
Cl3—Cu1—Cl1 | 143.17 (5) | C8—C7—H7B | 108.5 |
Cl1i—Cu1—Cl1 | 87.01 (5) | H7A—C7—H7B | 107.5 |
Cu1i—Cl1—Cu1 | 92.99 (5) | C7—C8—C9 | 111.6 (3) |
C1—C2—C3 | 112.0 (4) | C7—C8—H8A | 109.3 |
C1—C2—N1 | 113.3 (3) | C9—C8—H8A | 109.3 |
C3—C2—N1 | 110.3 (3) | C7—C8—H8B | 109.3 |
C1—C2—H2A | 107.0 | C9—C8—H8B | 109.3 |
C3—C2—H2A | 107.0 | H8A—C8—H8B | 108.0 |
N1—C2—H2A | 107.0 | C10—C9—C8 | 114.0 (3) |
C2—C3—H3A | 109.5 | C10—C9—H9A | 108.8 |
C2—C3—H3B | 109.5 | C8—C9—H9A | 108.8 |
H3A—C3—H3B | 109.5 | C10—C9—H9B | 108.8 |
C2—C3—H3C | 109.5 | C8—C9—H9B | 108.8 |
H3A—C3—H3C | 109.5 | H9A—C9—H9B | 107.6 |
H3B—C3—H3C | 109.5 | C9—C10—H10A | 109.5 |
C5—C4—H4A | 109.5 | C9—C10—H10B | 109.5 |
C5—C4—H4B | 109.5 | H10A—C10—H10B | 109.5 |
H4A—C4—H4B | 109.5 | C9—C10—H10C | 109.5 |
C5—C4—H4C | 109.5 | H10A—C10—H10C | 109.5 |
H4A—C4—H4C | 109.5 | H10B—C10—H10C | 109.5 |
H4B—C4—H4C | 109.5 | ||
Cl2—Cu1—Cl1—Cu1i | 146.38 (6) | C2—N1—C5—C6 | 92.1 (4) |
Cl3—Cu1—Cl1—Cu1i | −96.39 (7) | C7—N1—C5—C4 | 85.3 (4) |
Cl1i—Cu1—Cl1—Cu1i | 0.0 | C2—N1—C5—C4 | −142.1 (3) |
C7—N1—C2—C1 | 70.5 (4) | C5—N1—C7—C8 | −163.7 (3) |
C5—N1—C2—C1 | −62.1 (4) | C2—N1—C7—C8 | 63.0 (4) |
C7—N1—C2—C3 | −163.1 (3) | N1—C7—C8—C9 | 175.3 (3) |
C5—N1—C2—C3 | 64.3 (4) | C7—C8—C9—C10 | 179.4 (3) |
C7—N1—C5—C6 | −40.5 (4) |
Symmetry code: (i) −x+1, −y+2, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···Cl3 | 0.91 | 2.44 | 3.336 (3) | 168 |
C2—H2A···Cl3ii | 0.98 | 2.82 | 3.668 (5) | 146 |
C5—H5A···Cl2iii | 0.98 | 2.64 | 3.511 (4) | 149 |
C8—H8A···Cl3 | 0.97 | 2.78 | 3.617 (4) | 144 |
Symmetry codes: (ii) −x+1, −y+1, −z+1; (iii) −x+1, −y+1, −z+2. |
Experimental details
Crystal data | |
Chemical formula | (C10H24N)2[Cu2Cl6] |
Mr | 656.40 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 298 |
a, b, c (Å) | 8.5697 (17), 10.213 (2), 10.384 (2) |
α, β, γ (°) | 72.43 (3), 68.53 (3), 71.78 (3) |
V (Å3) | 785.1 (3) |
Z | 1 |
Radiation type | Mo Kα |
µ (mm−1) | 1.88 |
Crystal size (mm) | 0.30 × 0.05 × 0.05 |
Data collection | |
Diffractometer | Rigaku Mercury2 CCD diffractometer |
Absorption correction | Multi-scan (CrystalClear; Rigaku, 2005) |
Tmin, Tmax | 0.910, 1.000 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 8206, 3588, 2728 |
Rint | 0.044 |
(sin θ/λ)max (Å−1) | 0.649 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.046, 0.107, 1.08 |
No. of reflections | 3588 |
No. of parameters | 141 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.45, −0.52 |
Computer programs: CrystalClear (Rigaku, 2005), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008) and Mercury (Macrae et al., 2006), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···Cl3 | 0.91 | 2.44 | 3.336 (3) | 168 |
C2—H2A···Cl3i | 0.98 | 2.82 | 3.668 (5) | 146 |
C5—H5A···Cl2ii | 0.98 | 2.64 | 3.511 (4) | 149 |
C8—H8A···Cl3 | 0.97 | 2.78 | 3.617 (4) | 144 |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x+1, −y+1, −z+2. |
Acknowledgements
This work was supported by a start-up grant from Southeast University, China.
References
Fu, D.-W., Ge, J.-Z., Dai, J., Ye, H.-Y. & Qu, Z.-R. (2009). Inorg. Chem. Commun. 12, 994–997. Web of Science CSD CrossRef CAS Google Scholar
Fu, D.-W., Song, Y.-M., Wang, G.-X., Ye, Q., Xiong, R.-G., Akutagawa, T., Nakamura, T., Chan, P. W. H. & Huang, S. D. (2007). J. Am. Chem. Soc. 129, 5346–5347. Web of Science CSD CrossRef PubMed CAS Google Scholar
Fu, D.-W. & Xiong, R.-G. (2008). Dalton Trans. pp. 3946–3948. Web of Science CSD CrossRef Google Scholar
Fu, D.-W., Zhang, W. & Xiong, R.-G. (2008). Cryst. Growth Des. 8, 3461–3464. Web of Science CSD CrossRef CAS Google Scholar
Macrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst. 39, 453–457. Web of Science CrossRef CAS IUCr Journals Google Scholar
Rigaku (2005). CrystalClear. Rigaku Corporation, Tokyo, Japan. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
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Salts of amide have attracted more attention as phase transition dielectric materials for its applications in memory storage (Fu et al., 2007, 2008, 2009; Fu & Xiong, 2008). With the purpose of obtaining phase transition crystals of N,N-diisopropylbutyl-1-amine salts, its interactions with various metal ions have been studied and we have elaborated a series of new materials with this organic molecule. In this paper, we describe the crystal structure of the title compound,
The asymmetric unit is composed of half [Cu2Cl6]2- anion and one [C10H24N]+ cation (Fig. 1). The N atom of N,N-diisopropylbutyl-1-amine is protonated, thus indicating one positive charge in the amide N atom. The half [Cu2Cl6]2- anion showing one negative charge makes charge balance. The geometric parameters of the title compound are in a normal range. In the crystal structure, the cations and anions are involved in N—H···Cl and C—H···Cl hydrogen bonds (Table 1), which link the cations and anions into a two-dimensional network (Fig. 2).