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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jun 18;67(Pt 7):m943. doi: 10.1107/S1600536811022550

Bis[1-(4-cyano­benz­yl)pyrazinium] bis­(1,2-dicyano­ethene-1,2-dithiol­ato)nickelate(II)

Hui Zhang a, Wen-Bo Pei a, Shan-Shan Yu b, Xiao-Ming Ren a,*
PMCID: PMC3152075  PMID: 21836926

Abstract

The asymmetric unit of the title complex, (C12H10N3)2[Ni(C4N2S2)2], consists of one 1-(4-cyano­benz­yl)pyrazinium cation and one half of an [Ni(mnt)2]2− dianion (mnt2− is 1,2-dicyano­ethene-1,2-dithiol­ate). The Ni2+ ion is located on an inversion center and is coordinated by four S atoms from two mnt2− ligands, exhibiting a square-planar coordination geometry. The cation adopts a conformation where both the pyrazine ring and the benzene ring are twisted with respect to the C—C—N reference plane by 16.5 (2) and 69.8 (1)°, respectively.

Related literature

For general background to square-planar bis-1,2-dithiol­ato complexes of transition metals showing potential application as magnetic or conducting materials and other properties, see: Bigoli et al. (2002); Duan et al. (2010); Pei et al. (2011). For the synthesis, see: Davison & Holm (1967).graphic file with name e-67-0m943-scheme1.jpg

Experimental

Crystal data

  • (C12H10N3)2[Ni(C4N2S2)2]

  • M r = 731.53

  • Monoclinic, Inline graphic

  • a = 7.115 (3) Å

  • b = 13.623 (6) Å

  • c = 17.186 (8) Å

  • β = 101.671 (5)°

  • V = 1631.4 (13) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.89 mm−1

  • T = 298 K

  • 0.30 × 0.20 × 0.15 mm

Data collection

  • Bruker SMART APEX CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2002) T min = 0.807, T max = 0.875

  • 8060 measured reflections

  • 2871 independent reflections

  • 2586 reflections with I > 2σ(I)

  • R int = 0.020

Refinement

  • R[F 2 > 2σ(F 2)] = 0.026

  • wR(F 2) = 0.074

  • S = 1.06

  • 2871 reflections

  • 214 parameters

  • H-atom parameters constrained

  • Δρmax = 0.21 e Å−3

  • Δρmin = −0.26 e Å−3

Data collection: SMART (Siemens, 1996); cell refinement: SAINT (Siemens, 1996); data reduction: SAINT; 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.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811022550/im2295sup1.cif

e-67-0m943-sup1.cif (16.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811022550/im2295Isup2.hkl

e-67-0m943-Isup2.hkl (141KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Acknowledgments

The authors thank the Science and Technology Department of Jiangsu Province, China (grant No. BK2007184).

supplementary crystallographic information

Comment

Bis-1,2-dithiolene complexes of transition metals have been widely studied because of their novel properties and applications in the areas of conducting and magnetic materials, dyes, nonlinear optics, catalysis and others. These applications arise due to a combination of functional properties, specific geometries and intermolecular interactions. (Bigoli et al., 2002; Duan et al., 2010; Pei et al., 2011). Herein we report the crystal structure of the title compound (Fig. 1).

An asymmetric unit consists of one half [Ni(mnt)2]2- dianion and one 1-N-(4'-cyano-benzyl)-pyrazinium cation. In the [Ni(mnt)2]2- moiety, the Ni atom is situated at a inversion center and is coordinated by four S atoms from two mnt2- ligands, forming a square-planar coordination geometry. The cation adopts a conformation where the bond lengths and bond angles were normal, and both the pyrazine ring and the phenyl ring are twisted with respect to the C8—C12—N4 reference plane with the corresponding dihedral angles of 16.5 (2)° and 69.8 (1)°.

Experimental

Disodium maleonitriledithiolate (456 mg, 2.5 mmol) and nickel chloride hexahydrate (297 mg, 1.25 mmol) were mixed under stirring in water (20 ml) and heated to boiling for about 20 min. After the red solution was filtered an aqueous solution of 1-N-(4'-cyano-benzyl)-pyrazinium chloride (579 mg, 2.5 mmol) was added dropwise to the filtrate. The immediately formed dark red precipitate was filtered off, washed with water and dried in vacuum (yield: 722 mg, 79%). Block shaped single crystals suitable for X-ray analysis were obtained via recrystallization of the corresponding complex in acetone.

Refinement

All non-hydrogen atoms were refined anisotropically, whereas the H atoms were calculated and placed to the bonded parent atoms in geometrically idealized positions (C—H = 0.93 or 0.97 Å) and refined as riding atoms, with Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

Molecular structure of (I). Displacement ellipsoids are drawn at the 30% probability level (i = -x, -y, -z).

Fig. 2.

Fig. 2.

Packing diagram for (I) viewed along a axis.

Crystal data

(C12H10N3)2[Ni(C4N2S2)2] F(000) = 748
Mr = 731.53 Dx = 1.489 Mg m3
Monoclinic, P21/n Melting point: 456 K
Hall symbol: -P 2yn Mo Kα radiation, λ = 0.71073 Å
a = 7.115 (3) Å Cell parameters from 8060 reflections
b = 13.623 (6) Å θ = 2.4–25.0°
c = 17.186 (8) Å µ = 0.89 mm1
β = 101.671 (5)° T = 298 K
V = 1631.4 (13) Å3 Block, red
Z = 2 0.30 × 0.20 × 0.15 mm

Data collection

Bruker SMART APEX CCD diffractometer 2871 independent reflections
Radiation source: fine-focus sealed tube 2586 reflections with I > 2σ(I)
graphite Rint = 0.020
φ and ω scans θmax = 25.0°, θmin = 2.4°
Absorption correction: multi-scan (SADABS; Sheldrick, 2002) h = −8→4
Tmin = 0.807, Tmax = 0.875 k = −16→15
8060 measured reflections l = −20→20

Refinement

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)] = 0.026 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.074 H-atom parameters constrained
S = 1.06 w = 1/[σ2(Fo2) + (0.0431P)2 + 0.3009P] where P = (Fo2 + 2Fc2)/3
2871 reflections (Δ/σ)max < 0.001
214 parameters Δρmax = 0.21 e Å3
0 restraints Δρmin = −0.26 e Å3

Special details

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)

x y z Uiso*/Ueq
Ni1 0.0000 0.0000 0.0000 0.04070 (11)
C1 0.0668 (2) 0.13286 (12) 0.14603 (9) 0.0452 (4)
C2 0.2425 (2) 0.09233 (12) 0.14864 (10) 0.0464 (4)
C3 0.4020 (3) 0.11475 (13) 0.21086 (11) 0.0566 (4)
C4 0.0334 (2) 0.19910 (13) 0.20637 (10) 0.0508 (4)
C5 0.3059 (2) 0.61780 (13) −0.03334 (11) 0.0515 (4)
C6 0.4014 (3) 0.67295 (15) −0.08013 (11) 0.0608 (5)
H6A 0.3440 0.6865 −0.1326 0.073*
C7 0.5826 (3) 0.70790 (15) −0.04870 (11) 0.0594 (5)
H7A 0.6473 0.7448 −0.0805 0.071*
C8 0.6697 (2) 0.68900 (12) 0.02927 (10) 0.0473 (4)
C9 0.5730 (2) 0.63300 (13) 0.07578 (10) 0.0513 (4)
H9A 0.6311 0.6190 0.1281 0.062*
C10 0.3910 (3) 0.59771 (13) 0.04520 (11) 0.0550 (4)
H10A 0.3260 0.5608 0.0769 0.066*
C11 0.1164 (3) 0.58128 (16) −0.06742 (13) 0.0670 (5)
C12 0.8708 (2) 0.72452 (14) 0.06029 (11) 0.0541 (4)
H12A 0.9486 0.6693 0.0833 0.065*
H12B 0.9232 0.7484 0.0159 0.065*
C13 0.7384 (3) 0.85735 (13) 0.13272 (12) 0.0558 (4)
H13A 0.6171 0.8476 0.1014 0.067*
C14 0.7677 (3) 0.92685 (15) 0.19170 (13) 0.0672 (5)
H14A 0.6632 0.9643 0.1989 0.081*
C15 1.0821 (3) 0.89226 (14) 0.22341 (12) 0.0658 (5)
H15A 1.2038 0.9037 0.2539 0.079*
C16 1.0618 (3) 0.82300 (14) 0.16465 (11) 0.0573 (5)
H16A 1.1684 0.7893 0.1549 0.069*
N1 0.0083 (2) 0.25233 (14) 0.25432 (10) 0.0707 (5)
N2 0.5329 (3) 0.13221 (16) 0.25944 (11) 0.0842 (6)
N3 −0.0327 (3) 0.55373 (19) −0.09570 (13) 0.0963 (7)
N4 0.88726 (18) 0.80422 (10) 0.12132 (8) 0.0455 (3)
N5 0.9357 (3) 0.94368 (12) 0.23882 (10) 0.0677 (4)
S1 −0.12375 (6) 0.10653 (3) 0.06901 (3) 0.05089 (13)
S2 0.28315 (7) 0.01308 (3) 0.07488 (3) 0.05495 (14)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Ni1 0.04532 (18) 0.03877 (17) 0.03648 (17) −0.00199 (11) 0.00463 (12) −0.00037 (10)
C1 0.0529 (9) 0.0417 (8) 0.0406 (8) −0.0064 (7) 0.0085 (7) −0.0019 (7)
C2 0.0511 (9) 0.0440 (8) 0.0423 (8) −0.0041 (7) 0.0051 (7) −0.0038 (7)
C3 0.0564 (11) 0.0559 (10) 0.0541 (10) 0.0060 (8) 0.0036 (9) −0.0140 (8)
C4 0.0470 (9) 0.0544 (10) 0.0508 (9) −0.0046 (7) 0.0094 (8) −0.0047 (8)
C5 0.0449 (9) 0.0502 (9) 0.0585 (10) 0.0017 (7) 0.0079 (8) −0.0081 (8)
C6 0.0608 (11) 0.0711 (12) 0.0473 (10) 0.0045 (9) 0.0033 (8) 0.0033 (9)
C7 0.0599 (11) 0.0661 (11) 0.0531 (10) −0.0045 (9) 0.0135 (8) 0.0121 (9)
C8 0.0461 (9) 0.0454 (9) 0.0512 (9) −0.0015 (7) 0.0118 (7) 0.0002 (7)
C9 0.0520 (10) 0.0547 (10) 0.0463 (9) −0.0037 (8) 0.0074 (7) 0.0036 (7)
C10 0.0533 (10) 0.0555 (10) 0.0577 (10) −0.0076 (8) 0.0147 (8) 0.0039 (8)
C11 0.0542 (12) 0.0750 (13) 0.0690 (13) −0.0025 (10) 0.0059 (10) −0.0086 (10)
C12 0.0479 (9) 0.0575 (10) 0.0587 (10) −0.0046 (8) 0.0153 (8) −0.0027 (8)
C13 0.0464 (9) 0.0524 (10) 0.0664 (11) −0.0008 (8) 0.0066 (8) 0.0011 (8)
C14 0.0634 (12) 0.0577 (11) 0.0791 (14) 0.0017 (9) 0.0111 (10) −0.0062 (10)
C15 0.0651 (12) 0.0559 (11) 0.0669 (12) −0.0098 (9) −0.0091 (10) 0.0106 (9)
C16 0.0455 (9) 0.0546 (10) 0.0673 (11) −0.0028 (8) 0.0006 (8) 0.0099 (9)
N1 0.0665 (11) 0.0800 (12) 0.0676 (11) 0.0002 (9) 0.0182 (8) −0.0250 (9)
N2 0.0671 (11) 0.0967 (14) 0.0773 (12) 0.0143 (10) −0.0129 (10) −0.0363 (11)
N3 0.0612 (12) 0.1261 (19) 0.0940 (15) −0.0216 (12) −0.0021 (11) −0.0063 (14)
N4 0.0427 (7) 0.0434 (7) 0.0499 (8) −0.0049 (6) 0.0080 (6) 0.0103 (6)
N5 0.0823 (12) 0.0551 (9) 0.0618 (10) −0.0071 (9) 0.0051 (9) 0.0015 (8)
S1 0.0477 (2) 0.0538 (3) 0.0488 (2) 0.00206 (18) 0.00416 (18) −0.00887 (18)
S2 0.0479 (3) 0.0615 (3) 0.0517 (3) 0.00499 (19) 0.0009 (2) −0.01617 (19)

Geometric parameters (Å, °)

Ni1—S2 2.1674 (9) C8—C12 1.502 (2)
Ni1—S2i 2.1674 (9) C9—C10 1.382 (2)
Ni1—S1 2.1704 (7) C9—H9A 0.9300
Ni1—S1i 2.1704 (7) C10—H10A 0.9300
C1—C2 1.359 (2) C11—N3 1.138 (3)
C1—C4 1.430 (2) C12—N4 1.498 (2)
C1—S1 1.7302 (17) C12—H12A 0.9700
C2—C3 1.426 (2) C12—H12B 0.9700
C2—S2 1.7334 (18) C13—N4 1.330 (2)
C3—N2 1.143 (2) C13—C14 1.372 (3)
C4—N1 1.139 (2) C13—H13A 0.9300
C5—C6 1.376 (3) C14—N5 1.322 (3)
C5—C10 1.390 (3) C14—H14A 0.9300
C5—C11 1.445 (3) C15—N5 1.325 (3)
C6—C7 1.378 (3) C15—C16 1.368 (3)
C6—H6A 0.9300 C15—H15A 0.9300
C7—C8 1.382 (2) C16—N4 1.337 (2)
C7—H7A 0.9300 C16—H16A 0.9300
C8—C9 1.384 (2)
S2—Ni1—S2i 180.00 (2) C9—C10—C5 119.44 (17)
S2—Ni1—S1 92.96 (3) C9—C10—H10A 120.3
S2i—Ni1—S1 87.04 (3) C5—C10—H10A 120.3
S2—Ni1—S1i 87.04 (3) N3—C11—C5 178.5 (3)
S2i—Ni1—S1i 92.96 (3) N4—C12—C8 114.59 (14)
S1—Ni1—S1i 180.00 (2) N4—C12—H12A 108.6
C2—C1—C4 121.29 (15) C8—C12—H12A 108.6
C2—C1—S1 120.95 (13) N4—C12—H12B 108.6
C4—C1—S1 117.76 (13) C8—C12—H12B 108.6
C1—C2—C3 121.67 (15) H12A—C12—H12B 107.6
C1—C2—S2 121.17 (12) N4—C13—C14 118.57 (17)
C3—C2—S2 117.14 (13) N4—C13—H13A 120.7
N2—C3—C2 178.3 (2) C14—C13—H13A 120.7
N1—C4—C1 179.3 (2) N5—C14—C13 123.76 (19)
C6—C5—C10 120.33 (16) N5—C14—H14A 118.1
C6—C5—C11 118.78 (17) C13—C14—H14A 118.1
C10—C5—C11 120.88 (17) N5—C15—C16 122.83 (19)
C5—C6—C7 119.54 (17) N5—C15—H15A 118.6
C5—C6—H6A 120.2 C16—C15—H15A 118.6
C7—C6—H6A 120.2 N4—C16—C15 119.37 (18)
C6—C7—C8 121.07 (17) N4—C16—H16A 120.3
C6—C7—H7A 119.5 C15—C16—H16A 120.3
C8—C7—H7A 119.5 C13—N4—C16 119.44 (16)
C7—C8—C9 119.00 (16) C13—N4—C12 123.08 (14)
C7—C8—C12 119.48 (16) C16—N4—C12 117.47 (15)
C9—C8—C12 121.42 (16) C14—N5—C15 115.85 (18)
C10—C9—C8 120.61 (16) C1—S1—Ni1 102.41 (7)
C10—C9—H9A 119.7 C2—S2—Ni1 102.28 (6)
C8—C9—H9A 119.7

Symmetry codes: (i) −x, −y, −z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: IM2295).

References

  1. Bigoli, F., Deplano, P., Mercuri, M. L., Pellinghelli, M. A., Pilia, L., Pintus, G., Serpe, A. & Trogu, E. F. (2002). Inorg. Chem. 41, 5241–5248. [DOI] [PubMed]
  2. Davison, A. & Holm, H. R. (1967). Inorg. Synth. 10, 8–26.
  3. Duan, H.-B., Ren, X.-M. & Meng, Q.-J. (2010). Coord. Chem. Rev. 254, 1509–1522.
  4. Pei, W.-B., Wu, J.-S., Tian, Z.-F., Ren, X.-M. & Song, Y. (2011). Inorg. Chem. 50, 3970–3980. [DOI] [PubMed]
  5. Sheldrick, G. M. (2002). SADABS University of Göttingen, Germany.
  6. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  7. Siemens (1996). SMART and SAINT Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811022550/im2295sup1.cif

e-67-0m943-sup1.cif (16.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811022550/im2295Isup2.hkl

e-67-0m943-Isup2.hkl (141KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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