Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806004971/ng2003sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536806004971/ng2003Isup2.hkl |
CCDC reference: 601220
Key indicators
- Single-crystal X-ray study
- T = 291 K
- Mean (C-C) = 0.004 Å
- R factor = 0.040
- wR factor = 0.153
- Data-to-parameter ratio = 21.5
checkCIF/PLATON results
No syntax errors found
Alert level B PLAT232_ALERT_2_B Hirshfeld Test Diff (M-X) Ni - N2 .. 11.13 su
Alert level C PLAT152_ALERT_1_C Supplied and Calc Volume s.u. Inconsistent ..... ? PLAT232_ALERT_2_C Hirshfeld Test Diff (M-X) Ni - N1 .. 6.98 su PLAT232_ALERT_2_C Hirshfeld Test Diff (M-X) Ni - N3 .. 9.42 su PLAT420_ALERT_2_C D-H Without Acceptor N1 - H1D ... ? PLAT420_ALERT_2_C D-H Without Acceptor N2 - H2D ... ? PLAT480_ALERT_4_C Long H...A H-Bond Reported H2D .. O1 .. 2.64 Ang. PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 5 N1 -NI -N1 -C1 -28.01 0.18 4.555 1.555 1.555 1.555 PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 7 N3 -NI -N2 -C2 -25.60 0.60 4.555 1.555 1.555 1.555 PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 12 N2 -NI -N3 -C3 -36.30 0.60 4.555 1.555 1.555 1.555
Alert level G REFLT03_ALERT_1_G ALERT: Expected hkl max differ from CIF values From the CIF: _diffrn_reflns_theta_max 27.99 From the CIF: _reflns_number_total 1785 From the CIF: _diffrn_reflns_limit_ max hkl 18. 21. 13. From the CIF: _diffrn_reflns_limit_ min hkl -18. -21. -13. TEST1: Expected hkl limits for theta max Calculated maximum hkl 21. 21. 13. Calculated minimum hkl -21. -21. -13.
0 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 9 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 5 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
Data collection: MSC/AFC Diffractometer Control Software (Molecular Structure Corporation, 1987); cell refinement: TEXSAN (Molecular Structure Corporation, 1987); data reduction: TEXSAN; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL/PC (Sheldrick, 1990); software used to prepare material for publication: SHELXL97.
[Ni(C2H8N2)3][MoO4] | Dx = 1.799 Mg m−3 |
Mr = 398.96 | Mo Kα radiation, λ = 0.71073 Å |
Trigonal, P3c1 | Cell parameters from 200 reflections |
Hall symbol: -P 3 2"c | θ = 10–20° |
a = 16.0024 (16) Å | µ = 2.15 mm−1 |
c = 9.9608 (19) Å | T = 291 K |
V = 2209.0 (5) Å3 | Block, violet |
Z = 6 | 0.20 × 0.12 × 0.08 mm |
F(000) = 1224 |
Rigaku AFC-5R diffractometer | 1538 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.037 |
Graphite monochromator | θmax = 28.0°, θmin = 2.6° |
ω–2θ scans | h = −18→18 |
Absorption correction: ψ scan (North et al., 1968) | k = −21→21 |
Tmin = 0.674, Tmax = 0.847 | l = −13→13 |
5355 measured reflections | 3 standard reflections every 150 reflections |
1785 independent reflections | intensity decay: 0.2% |
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)] = 0.040 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.153 | H-atom parameters constrained |
S = 1.02 | w = 1/[σ2(Fo2) + (0.0867P)2 + 1.4958P] where P = (Fo2 + 2Fc2)/3 |
1785 reflections | (Δ/σ)max = 0.001 |
83 parameters | Δρmax = 0.94 e Å−3 |
0 restraints | Δρmin = −0.53 e Å−3 |
Experimental. crystal coated in epoxy glue |
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 | ||
Ni | 0.33135 (2) | 0.33135 (2) | 0.2500 | 0.0317 (2) | |
Mo | 0.0000 | 0.334817 (15) | 0.2500 | 0.0356 (2) | |
O1 | 0.07418 (13) | 0.43261 (13) | 0.15839 (17) | 0.0483 (5) | |
O2 | 0.06951 (12) | 0.31208 (13) | 0.36123 (16) | 0.0431 (4) | |
N1 | 0.40297 (17) | 0.27074 (17) | 0.3637 (3) | 0.0428 (5) | |
H1C | 0.3957 | 0.2761 | 0.4524 | 0.051* | |
H1D | 0.3782 | 0.2079 | 0.3436 | 0.051* | |
N2 | 0.4603 (2) | 0.38995 (19) | 0.1322 (3) | 0.0493 (6) | |
H2C | 0.4458 | 0.3813 | 0.0442 | 0.059* | |
H2D | 0.4977 | 0.4536 | 0.1481 | 0.059* | |
N3 | 0.25274 (18) | 0.20474 (19) | 0.1309 (3) | 0.0475 (6) | |
H3C | 0.2574 | 0.2206 | 0.0434 | 0.057* | |
H3D | 0.2768 | 0.1650 | 0.1422 | 0.057* | |
C1 | 0.5037 (2) | 0.3249 (3) | 0.3269 (3) | 0.0513 (7) | |
H1A | 0.5372 | 0.2890 | 0.3553 | 0.062* | |
H1B | 0.5369 | 0.3868 | 0.3691 | 0.062* | |
C2 | 0.5113 (2) | 0.3377 (2) | 0.1724 (3) | 0.0460 (6) | |
H2A | 0.5785 | 0.3742 | 0.1456 | 0.055* | |
H2B | 0.4820 | 0.2751 | 0.1288 | 0.055* | |
C3 | 0.1560 (2) | 0.1590 (2) | 0.1721 (3) | 0.0436 (6) | |
H3A | 0.1204 | 0.0942 | 0.1356 | 0.052* | |
H3B | 0.1255 | 0.1952 | 0.1427 | 0.052* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Ni | 0.0324 (3) | 0.0324 (3) | 0.0306 (4) | 0.01642 (19) | 0.00001 (6) | −0.00001 (6) |
Mo | 0.0365 (2) | 0.0363 (2) | 0.0340 (3) | 0.01827 (12) | −0.00001 (9) | 0.00000 (4) |
O1 | 0.0501 (10) | 0.0460 (10) | 0.0460 (9) | 0.0219 (8) | −0.0011 (8) | 0.0002 (7) |
O2 | 0.0445 (9) | 0.0446 (9) | 0.0416 (8) | 0.0233 (8) | −0.0011 (7) | −0.0006 (7) |
N1 | 0.0439 (12) | 0.0447 (11) | 0.0417 (12) | 0.0235 (10) | −0.0011 (9) | 0.0007 (9) |
N2 | 0.0506 (14) | 0.0502 (13) | 0.0481 (14) | 0.0259 (11) | 0.0026 (10) | 0.0013 (10) |
N3 | 0.0464 (12) | 0.0460 (13) | 0.0476 (13) | 0.0213 (10) | −0.0018 (10) | −0.0021 (10) |
C1 | 0.0492 (15) | 0.0560 (17) | 0.0506 (16) | 0.0277 (13) | −0.0011 (12) | −0.0010 (13) |
C2 | 0.0437 (14) | 0.0510 (15) | 0.0450 (15) | 0.0249 (12) | 0.0024 (11) | 0.0003 (12) |
C3 | 0.0413 (13) | 0.0421 (13) | 0.0443 (14) | 0.0185 (11) | −0.0019 (11) | −0.0021 (10) |
Ni—N1i | 2.156 (2) | N2—H2C | 0.9000 |
Ni—N2i | 2.140 (3) | N2—H2D | 0.9000 |
Ni—N3 | 2.132 (3) | N3—C3 | 1.403 (4) |
Ni—N3i | 2.132 (3) | N3—H3C | 0.9000 |
Ni—N2 | 2.140 (3) | N3—H3D | 0.9000 |
Ni—N1 | 2.156 (2) | C1—C2 | 1.550 (5) |
Mo—O1ii | 1.6832 (18) | C1—H1A | 1.0022 |
Mo—O1 | 1.6832 (18) | C1—H1B | 0.9560 |
Mo—O2ii | 1.7326 (17) | C2—H2A | 0.9700 |
Mo—O2 | 1.7326 (17) | C2—H2B | 0.9700 |
N1—C1 | 1.445 (4) | C3—C3i | 1.553 (5) |
N1—H1C | 0.9000 | C3—H3A | 0.9700 |
N1—H1D | 0.9000 | C3—H3B | 0.9700 |
N2—C2 | 1.485 (4) | ||
N3—Ni—N3i | 79.28 (14) | Ni—N2—H2C | 110.4 |
N3—Ni—N2i | 170.85 (11) | C2—N2—H2D | 110.4 |
N3i—Ni—N2i | 95.32 (11) | Ni—N2—H2D | 110.4 |
N3—Ni—N2 | 95.32 (11) | H2C—N2—H2D | 108.6 |
N3i—Ni—N2 | 170.85 (11) | C3—N3—Ni | 107.80 (19) |
N2i—Ni—N2 | 90.95 (15) | C3—N3—H3C | 110.1 |
N3—Ni—N1i | 90.24 (10) | Ni—N3—H3C | 110.1 |
N3i—Ni—N1i | 93.36 (11) | C3—N3—H3D | 110.1 |
N2i—Ni—N1i | 82.65 (12) | Ni—N3—H3D | 110.1 |
N2—Ni—N1i | 94.05 (10) | H3C—N3—H3D | 108.5 |
N3—Ni—N1 | 93.36 (11) | N1—C1—C2 | 108.7 (2) |
N3i—Ni—N1 | 90.24 (10) | N1—C1—H1A | 109.9 |
N2i—Ni—N1 | 94.05 (10) | C2—C1—H1A | 109.1 |
N2—Ni—N1 | 82.65 (12) | N1—C1—H1B | 112.6 |
N1i—Ni—N1 | 175.32 (13) | C2—C1—H1B | 109.5 |
O1ii—Mo—O1 | 109.50 (13) | H1A—C1—H1B | 107.0 |
O1ii—Mo—O2ii | 108.27 (9) | N2—C2—C1 | 108.3 (2) |
O1—Mo—O2ii | 107.42 (8) | N2—C2—H2A | 110.0 |
O1ii—Mo—O2 | 107.42 (8) | C1—C2—H2A | 110.0 |
O1—Mo—O2 | 108.27 (9) | N2—C2—H2B | 110.0 |
O2ii—Mo—O2 | 115.85 (11) | C1—C2—H2B | 110.0 |
C1—N1—Ni | 106.35 (19) | H2A—C2—H2B | 108.4 |
C1—N1—H1C | 110.5 | N3—C3—C3i | 105.4 (2) |
Ni—N1—H1C | 110.5 | N3—C3—H3A | 110.7 |
C1—N1—H1D | 110.5 | C3i—C3—H3A | 110.7 |
Ni—N1—H1D | 110.5 | N3—C3—H3B | 110.7 |
H1C—N1—H1D | 108.7 | C3i—C3—H3B | 110.7 |
C2—N2—Ni | 106.63 (18) | H3A—C3—H3B | 108.8 |
C2—N2—H2C | 110.4 | ||
N3—Ni—N1—C1 | 112.3 (2) | N3i—Ni—N3—C3 | 18.12 (14) |
N3i—Ni—N1—C1 | −168.41 (18) | N2i—Ni—N3—C3 | −36.3 (6) |
N2i—Ni—N1—C1 | −73.1 (2) | N2—Ni—N3—C3 | −169.35 (19) |
N2—Ni—N1—C1 | 17.38 (17) | N1i—Ni—N3—C3 | −75.3 (2) |
N1i—Ni—N1—C1 | −28.01 (18) | N1—Ni—N3—C3 | 107.7 (2) |
N3—Ni—N2—C2 | −79.0 (2) | Ni—N1—C1—C2 | −44.5 (3) |
N3i—Ni—N2—C2 | −25.6 (6) | Ni—N2—C2—C1 | −41.0 (3) |
N2i—Ni—N2—C2 | 107.7 (2) | N1—C1—C2—N2 | 59.5 (4) |
N1i—Ni—N2—C2 | −169.60 (18) | Ni—N3—C3—C3i | −47.5 (3) |
N1—Ni—N2—C2 | 13.74 (17) |
Symmetry codes: (i) y, x, −z+1/2; (ii) −x, −x+y, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1C···O2iii | 0.90 | 2.19 | 3.028 (3) | 154 |
N2—H2C···O1iv | 0.90 | 2.04 | 2.934 (3) | 170 |
N2—H2D···O1v | 0.90 | 2.64 | 3.510 (3) | 164 |
N3—H3C···O2vi | 0.90 | 2.42 | 3.236 (3) | 152 |
N3—H3D···O2i | 0.90 | 1.88 | 2.765 (3) | 169 |
Symmetry codes: (i) y, x, −z+1/2; (iii) y, −x+y, −z+1; (iv) y, −x+y, −z; (v) −y+1, x−y+1, z; (vi) −x+y, y, z−1/2. |
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