Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805027674/ng6186sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536805027674/ng6186Isup2.hkl |
CCDC reference: 287666
Key indicators
- Single-crystal X-ray study
- T = 193 K
- Mean (N-C) = 0.003 Å
- R factor = 0.023
- wR factor = 0.062
- Data-to-parameter ratio = 11.8
checkCIF/PLATON results
No syntax errors found
Alert level C PLAT062_ALERT_4_C Rescale T(min) & T(max) by ..................... 0.99 PLAT164_ALERT_4_C Nr. of Refined C-H H-Atoms in Heavy-At Struct... 5 PLAT220_ALERT_2_C Large Non-Solvent C Ueq(max)/Ueq(min) ... 2.98 Ratio PLAT380_ALERT_4_C Check Incorrectly? Oriented X(sp2)-Methyl Moiety C3 PLAT380_ALERT_4_C Check Incorrectly? Oriented X(sp2)-Methyl Moiety C4 PLAT731_ALERT_1_C Bond Calc 0.94(2), Rep 0.938(9) ...... 2.22 su-Rat C4 -H4B 1.555 1.555
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 6 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 4 ALERT type 4 Improvement, methodology, query or suggestion
An aqueous solution (10 ml) of Ni(NO3)2·6H2O (0.146 g, 0.5 mmol) was added to a DMF solution (10 ml) of Na[N(CN)2] (0.090 g, 1.0 mmol). Slow evaporation of the resulting mixture led to green crystals suitable for X-ray diffraction analysis. Analysis found: C 35.53, H 4.12, N 33.31%; calculated for C10H14N8NiO2: C 35.64, H 4.19, N 33.26%.
H atoms were found in a difference Fourier map and refined with bond-length restraints of C—H = 0.95 (1) Å for the methyl groups and the H···H distance restrained to 1.50 (1) Å. One of two independent H atoms lies on the mirror plane.
Dicyanamide (dca), [N(CN)2]-, complexes have been studied extensively recently because of their fascinating topologies and interesting magnetic properties (Batten et al., 1998; Miller & Manson 2001; Jensen et al., 2000; Riggio et al., 2001). A number of nickel(II)–dca complexes have been reported (Sun, et al., 2000; Wang et al., 2004; Konor et al., 2005). Our research interest is construction of novel topologies of cyano complexes and studying the magnetic properties (Shen et al., 2004, 2003). In the present work, we report the crystal structure of a one-dimensional chain polymer, viz. [Ni(dca)2(DMF)2]n, (I).
Fig. 1 shows the local coordination about the nickel(II) center in (I). The structure of (I) is isostructural with [Co(dca)2(DMF)2]n (Tong et al., 2003) and not isostructural with [Mn(dca)2(DMF)2]n (Batten et al., 1999). The space group of [Co(dca)2(DMF)2]n reported by Dong et al. (2003) has been described incorrectly in C2; it should be C2/m, as reported by Tong et al. (2003). The structure of (I) consists of uniform neutral chains where neighboring nikel(II) atoms are connected through two asymmetric end-to-end dca bridges. The coordination geometry of the nickel(II) atom is distorted octahedral, being coordinated by four N atoms of four symmetry-related dca ligands in the equatorial plane and two O atoms of two symmetry-related DMF ligands at the axial positions. The N—Ni—N bond angles are in the range 87.84 (6) to 92.16 (6)°, close to 90°. The four Ni—N(dca) bond lengths in (I) are all 2.0733 (11) Å, corresponding to the values reported in the dca-bridged nickel(II) complexes [Ni(apo)(dca)2] [2.043 (4)–2.096 (4) Å; apo = 2-aminopyridine N-oxide; Sun et al., 2000] and [Ni(tn)2(dca)](ClO4) [2.095 (4) and 2.116 (4) Å; tn = trimethylenediamine; Li et al., 2002], and shorter than the Mn—N bond lengths [2.218 (2) and 2.203 (2) Å] in [Mn(dca)2(DMF)2]n (Batten et al., 1999) and the Co—N bond lengths [2.123 (2) Å] in [Co(dca)2(DMF)2]n (Tong et al., 2003); this is what one would expect from the ionic radii (Ni2+ < Co2+ < Mn2+). The two Ni—O (DMF) bond lengths are both 2.0670 (13) Å, corresponding to the values [2.0776 (19) Å] in [Ni(pmbp)2(DMF)2] [Hpmbp = 1-phenyl-3-methyl-4-benzoyl-1H-pyrazol-5(4H)-one; Shen & Yuan 2004] and shorter than the M—O bond lengths in [Mn(dca)2(DMF)2]n [Mn—O = 2.199 (2) Å] and in [Co(dca)2(DMF)2]n [Co—O = 2.096 (2) Å].
The dicyanamide (dca) ligand adopts an end-to-end coordination mode. Two dca ions link two nickel(II) atoms to form a 12-membered Ni(dca)2Ni ring and the neighboring rings share the nickel(II) atoms to form a chain of [Ni(dca)2]n. The chains are linear, the Ni(dca)2Ni rings being in a slight chair conformation.
Free dicyanamide (dca) ligand possesses C2v symmetry. The dca ligand in (I) also adopts C2v symmetry with a nitrile C≡ N bond length of 1.1545 (18) Å for N1≡C1, showing the triple-bond character. The bond angle related to the amide N atom, C1—N2—C1(x, 1 - y, z), is 118.61 (16)°, corresponding to an amide N atom with an sp2 hybrid orbital; tha related to the nitrile group, N1≡ C1—N2, is 174.95 (13)°, corresponding to N1 and C1 with an sp hybrid orbital.
The chains propagate parallel to the crystallographic b axis, the Ni···Ni distance along the chain being equal to the b cell length 7.3166 (7) Å. The chains interdigate such that each DMF ligand lies between two DMF ligands of an adjacent chain, with a shortest Ni···Ni interchain distance of 7.628 (2) Å (Fig. 3). Adjacent chains are held together by a weak C—H···N hydrogen bond, forming layers parallel to the ab plane (Fig. 2 and Table 2).
Data collection: CrystalClear (Rigaku, 2000); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: the coordinates of the Co structure of Tong et al. (2003) were used; program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1998); software used to prepare material for publication: SHELXTL.
[Ni(C2N3)2(C3H7NO)2] | F(000) = 348 |
Mr = 336.98 | Dx = 1.535 Mg m−3 |
Monoclinic, C2/m | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -C 2y | Cell parameters from 1804 reflections |
a = 13.3866 (17) Å | θ = 3.2–27.5° |
b = 7.3166 (7) Å | µ = 1.35 mm−1 |
c = 8.0595 (10) Å | T = 193 K |
β = 112.503 (3)° | Block, blue |
V = 729.28 (15) Å3 | 0.40 × 0.21 × 0.20 mm |
Z = 2 |
Rigaku Mercury CCD diffractometer | 900 independent reflections |
Radiation source: fine-focus sealed tube | 887 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.018 |
ω scans | θmax = 27.5°, θmin = 3.2° |
Absorption correction: multi-scan (Jacobson, 1998) | h = −17→15 |
Tmin = 0.646, Tmax = 0.774 | k = −8→9 |
4029 measured reflections | l = −10→10 |
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)] = 0.023 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.062 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.03 | w = 1/[σ2(Fo2) + (0.0436P)2 + 0.3824P] where P = (Fo2 + 2Fc2)/3 |
900 reflections | (Δ/σ)max < 0.001 |
76 parameters | Δρmax = 0.15 e Å−3 |
9 restraints | Δρmin = −0.47 e Å−3 |
[Ni(C2N3)2(C3H7NO)2] | V = 729.28 (15) Å3 |
Mr = 336.98 | Z = 2 |
Monoclinic, C2/m | Mo Kα radiation |
a = 13.3866 (17) Å | µ = 1.35 mm−1 |
b = 7.3166 (7) Å | T = 193 K |
c = 8.0595 (10) Å | 0.40 × 0.21 × 0.20 mm |
β = 112.503 (3)° |
Rigaku Mercury CCD diffractometer | 900 independent reflections |
Absorption correction: multi-scan (Jacobson, 1998) | 887 reflections with I > 2σ(I) |
Tmin = 0.646, Tmax = 0.774 | Rint = 0.018 |
4029 measured reflections |
R[F2 > 2σ(F2)] = 0.023 | 9 restraints |
wR(F2) = 0.062 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.03 | Δρmax = 0.15 e Å−3 |
900 reflections | Δρmin = −0.47 e Å−3 |
76 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Ni1 | 0.5000 | 0.5000 | 0.5000 | 0.01621 (13) | |
O1 | 0.58082 (11) | 0.5000 | 0.77586 (18) | 0.0230 (3) | |
N1 | 0.59942 (9) | 0.70410 (15) | 0.47063 (15) | 0.0231 (3) | |
N2 | 0.63339 (15) | 1.0000 | 0.3571 (2) | 0.0255 (4) | |
N3 | 0.73719 (13) | 0.5000 | 1.0204 (2) | 0.0256 (4) | |
C1 | 0.61394 (9) | 0.84635 (18) | 0.42201 (16) | 0.0181 (3) | |
C2 | 0.68128 (15) | 0.5000 | 0.8455 (2) | 0.0210 (4) | |
H2 | 0.7242 (17) | 0.5000 | 0.774 (3) | 0.026 (6)* | |
C3 | 0.6836 (2) | 0.5000 | 1.1460 (3) | 0.0541 (8) | |
H3A | 0.7060 (14) | 0.6031 (7) | 1.217 (2) | 0.075 (8)* | |
H3B | 0.6084 (9) | 0.5000 | 1.089 (4) | 0.073 (11)* | |
C4 | 0.85511 (17) | 0.5000 | 1.0956 (3) | 0.0320 (5) | |
H4A | 0.8843 (13) | 0.6028 (7) | 1.1684 (16) | 0.044 (6)* | |
H4B | 0.882 (2) | 0.5000 | 1.004 (2) | 0.042 (8)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Ni1 | 0.01952 (19) | 0.01301 (18) | 0.01555 (18) | 0.000 | 0.00610 (13) | 0.000 |
O1 | 0.0218 (6) | 0.0294 (7) | 0.0161 (6) | 0.000 | 0.0052 (5) | 0.000 |
N1 | 0.0268 (6) | 0.0182 (5) | 0.0264 (6) | −0.0022 (4) | 0.0127 (5) | −0.0017 (4) |
N2 | 0.0383 (9) | 0.0164 (7) | 0.0318 (9) | 0.000 | 0.0245 (8) | 0.000 |
N3 | 0.0235 (8) | 0.0343 (9) | 0.0171 (7) | 0.000 | 0.0057 (6) | 0.000 |
C1 | 0.0173 (6) | 0.0192 (6) | 0.0190 (6) | 0.0000 (5) | 0.0084 (5) | −0.0038 (5) |
C2 | 0.0242 (9) | 0.0206 (8) | 0.0182 (8) | 0.000 | 0.0082 (7) | 0.000 |
C3 | 0.0369 (13) | 0.108 (3) | 0.0189 (10) | 0.000 | 0.0127 (9) | 0.000 |
C4 | 0.0234 (10) | 0.0381 (12) | 0.0272 (10) | 0.000 | 0.0017 (8) | 0.000 |
Ni1—O1 | 2.0670 (13) | N2—C1 | 1.3074 (15) |
Ni1—O1i | 2.0670 (13) | N3—C2 | 1.319 (2) |
Ni1—N1 | 2.0733 (11) | N3—C3 | 1.448 (3) |
Ni1—N1i | 2.0733 (11) | N3—C4 | 1.458 (3) |
Ni1—N1ii | 2.0733 (11) | C2—H2 | 0.954 (10) |
Ni1—N1iii | 2.0733 (11) | C3—H3A | 0.923 (8) |
O1—C2 | 1.243 (2) | C3—H3B | 0.933 (10) |
N1—C1 | 1.1545 (18) | C4—H4A | 0.942 (8) |
N2—C1iv | 1.3074 (15) | C4—H4B | 0.938 (9) |
O1—Ni1—O1i | 180.0 | C1—N1—Ni1 | 152.49 (11) |
O1—Ni1—N1 | 91.61 (4) | C1iv—N2—C1 | 118.61 (16) |
O1i—Ni1—N1 | 88.39 (4) | C2—N3—C3 | 121.12 (18) |
O1—Ni1—N1i | 88.39 (4) | C2—N3—C4 | 121.70 (17) |
O1i—Ni1—N1i | 91.61 (4) | C3—N3—C4 | 117.18 (18) |
N1—Ni1—N1i | 180.0 | N1—C1—N2 | 174.95 (13) |
O1—Ni1—N1ii | 91.61 (4) | O1—C2—N3 | 123.76 (17) |
O1i—Ni1—N1ii | 88.39 (4) | O1—C2—H2 | 121.7 (15) |
N1—Ni1—N1ii | 92.16 (6) | N3—C2—H2 | 114.6 (15) |
N1i—Ni1—N1ii | 87.84 (6) | N3—C3—H3A | 107.4 (14) |
O1—Ni1—N1iii | 88.39 (4) | N3—C3—H3B | 113 (2) |
O1i—Ni1—N1iii | 91.61 (4) | H3A—C3—H3B | 109.9 (11) |
N1—Ni1—N1iii | 87.84 (6) | N3—C4—H4A | 112.6 (10) |
N1i—Ni1—N1iii | 92.16 (6) | N3—C4—H4B | 110.5 (16) |
N1ii—Ni1—N1iii | 180.00 (6) | H4A—C4—H4B | 107.4 (10) |
C2—O1—Ni1 | 121.06 (12) | ||
N1—Ni1—O1—C2 | −46.10 (3) | N1ii—Ni1—N1—C1 | 145.1 (2) |
N1i—Ni1—O1—C2 | 133.90 (3) | N1iii—Ni1—N1—C1 | −34.9 (2) |
N1ii—Ni1—O1—C2 | 46.10 (3) | Ni1—O1—C2—N3 | 180.0 |
N1iii—Ni1—O1—C2 | −133.90 (3) | C3—N3—C2—O1 | 0.0 |
O1—Ni1—N1—C1 | −123.3 (2) | C4—N3—C2—O1 | 180.0 |
O1i—Ni1—N1—C1 | 56.7 (2) |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) x, −y+1, z; (iii) −x+1, y, −z+1; (iv) x, −y+2, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
C2—H2···N2v | 0.95 (1) | 2.51 (1) | 3.453 (2) | 169 (2) |
Symmetry code: (v) −x+3/2, −y+3/2, −z+1. |
Experimental details
Crystal data | |
Chemical formula | [Ni(C2N3)2(C3H7NO)2] |
Mr | 336.98 |
Crystal system, space group | Monoclinic, C2/m |
Temperature (K) | 193 |
a, b, c (Å) | 13.3866 (17), 7.3166 (7), 8.0595 (10) |
β (°) | 112.503 (3) |
V (Å3) | 729.28 (15) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 1.35 |
Crystal size (mm) | 0.40 × 0.21 × 0.20 |
Data collection | |
Diffractometer | Rigaku Mercury CCD |
Absorption correction | Multi-scan (Jacobson, 1998) |
Tmin, Tmax | 0.646, 0.774 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 4029, 900, 887 |
Rint | 0.018 |
(sin θ/λ)max (Å−1) | 0.649 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.023, 0.062, 1.03 |
No. of reflections | 900 |
No. of parameters | 76 |
No. of restraints | 9 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.15, −0.47 |
Computer programs: CrystalClear (Rigaku, 2000), CrystalClear, the coordinates of the Co structure of Tong et al. (2003) were used, SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 1998), SHELXTL.
Ni1—O1 | 2.0670 (13) | N2—C1 | 1.3074 (15) |
Ni1—N1 | 2.0733 (11) | N3—C2 | 1.319 (2) |
O1—C2 | 1.243 (2) | N3—C3 | 1.448 (3) |
N1—C1 | 1.1545 (18) | N3—C4 | 1.458 (3) |
O1—Ni1—N1 | 91.61 (4) | N1—Ni1—N1iii | 87.84 (6) |
O1i—Ni1—N1 | 88.39 (4) | C1iv—N2—C1 | 118.61 (16) |
N1—Ni1—N1ii | 92.16 (6) | N1—C1—N2 | 174.95 (13) |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) x, −y+1, z; (iii) −x+1, y, −z+1; (iv) x, −y+2, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
C2—H2···N2v | 0.954 (10) | 2.511 (11) | 3.453 (2) | 169 (2) |
Symmetry code: (v) −x+3/2, −y+3/2, −z+1. |
Dicyanamide (dca), [N(CN)2]-, complexes have been studied extensively recently because of their fascinating topologies and interesting magnetic properties (Batten et al., 1998; Miller & Manson 2001; Jensen et al., 2000; Riggio et al., 2001). A number of nickel(II)–dca complexes have been reported (Sun, et al., 2000; Wang et al., 2004; Konor et al., 2005). Our research interest is construction of novel topologies of cyano complexes and studying the magnetic properties (Shen et al., 2004, 2003). In the present work, we report the crystal structure of a one-dimensional chain polymer, viz. [Ni(dca)2(DMF)2]n, (I).
Fig. 1 shows the local coordination about the nickel(II) center in (I). The structure of (I) is isostructural with [Co(dca)2(DMF)2]n (Tong et al., 2003) and not isostructural with [Mn(dca)2(DMF)2]n (Batten et al., 1999). The space group of [Co(dca)2(DMF)2]n reported by Dong et al. (2003) has been described incorrectly in C2; it should be C2/m, as reported by Tong et al. (2003). The structure of (I) consists of uniform neutral chains where neighboring nikel(II) atoms are connected through two asymmetric end-to-end dca bridges. The coordination geometry of the nickel(II) atom is distorted octahedral, being coordinated by four N atoms of four symmetry-related dca ligands in the equatorial plane and two O atoms of two symmetry-related DMF ligands at the axial positions. The N—Ni—N bond angles are in the range 87.84 (6) to 92.16 (6)°, close to 90°. The four Ni—N(dca) bond lengths in (I) are all 2.0733 (11) Å, corresponding to the values reported in the dca-bridged nickel(II) complexes [Ni(apo)(dca)2] [2.043 (4)–2.096 (4) Å; apo = 2-aminopyridine N-oxide; Sun et al., 2000] and [Ni(tn)2(dca)](ClO4) [2.095 (4) and 2.116 (4) Å; tn = trimethylenediamine; Li et al., 2002], and shorter than the Mn—N bond lengths [2.218 (2) and 2.203 (2) Å] in [Mn(dca)2(DMF)2]n (Batten et al., 1999) and the Co—N bond lengths [2.123 (2) Å] in [Co(dca)2(DMF)2]n (Tong et al., 2003); this is what one would expect from the ionic radii (Ni2+ < Co2+ < Mn2+). The two Ni—O (DMF) bond lengths are both 2.0670 (13) Å, corresponding to the values [2.0776 (19) Å] in [Ni(pmbp)2(DMF)2] [Hpmbp = 1-phenyl-3-methyl-4-benzoyl-1H-pyrazol-5(4H)-one; Shen & Yuan 2004] and shorter than the M—O bond lengths in [Mn(dca)2(DMF)2]n [Mn—O = 2.199 (2) Å] and in [Co(dca)2(DMF)2]n [Co—O = 2.096 (2) Å].
The dicyanamide (dca) ligand adopts an end-to-end coordination mode. Two dca ions link two nickel(II) atoms to form a 12-membered Ni(dca)2Ni ring and the neighboring rings share the nickel(II) atoms to form a chain of [Ni(dca)2]n. The chains are linear, the Ni(dca)2Ni rings being in a slight chair conformation.
Free dicyanamide (dca) ligand possesses C2v symmetry. The dca ligand in (I) also adopts C2v symmetry with a nitrile C≡ N bond length of 1.1545 (18) Å for N1≡C1, showing the triple-bond character. The bond angle related to the amide N atom, C1—N2—C1(x, 1 - y, z), is 118.61 (16)°, corresponding to an amide N atom with an sp2 hybrid orbital; tha related to the nitrile group, N1≡ C1—N2, is 174.95 (13)°, corresponding to N1 and C1 with an sp hybrid orbital.
The chains propagate parallel to the crystallographic b axis, the Ni···Ni distance along the chain being equal to the b cell length 7.3166 (7) Å. The chains interdigate such that each DMF ligand lies between two DMF ligands of an adjacent chain, with a shortest Ni···Ni interchain distance of 7.628 (2) Å (Fig. 3). Adjacent chains are held together by a weak C—H···N hydrogen bond, forming layers parallel to the ab plane (Fig. 2 and Table 2).