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The title compound, cis-[C6H5CH2N(CH3)3][Ni(pymt)3], (pymt = pyrimidine-2-thiol­ate, C4H3N2S) consists of discrete cations and anions. The coordination geometry around nickel is highly distorted octahedral due to the presence of three four-membered N,S-chelate rings in a cis configuration. The Ni—S distances are in the range 2.4617 (5)–2.5290 (5) Å and the Ni—N bond distances range from 2.0490 (14) to 2.0689 (14) Å.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536804008128/hb6031sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536804008128/hb6031Isup2.hkl
Contains datablock I

CCDC reference: 239052

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.031
  • wR factor = 0.070
  • Data-to-parameter ratio = 20.4

checkCIF/PLATON results

No syntax errors found



Alert level B PLAT232_ALERT_2_B Hirshfeld Test Diff (M-X) Ni1 - S1 .. 10.24 su
Alert level C PLAT042_ALERT_1_C Calc. and Rep. MoietyFormula Strings Differ .... ? PLAT232_ALERT_2_C Hirshfeld Test Diff (M-X) Ni1 - S2 .. 9.57 su PLAT232_ALERT_2_C Hirshfeld Test Diff (M-X) Ni1 - S3 .. 8.48 su PLAT232_ALERT_2_C Hirshfeld Test Diff (M-X) Ni1 - N5 .. 5.41 su PLAT790_ALERT_4_C Centre of Gravity not Within Unit Cell: Resd. # 2 C10 H16 N
0 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 5 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 4 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 1 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: CrystalClear (Rigaku, 2000); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97; molecular graphics: SHELXL97; software used to prepare material for publication: SHELXL97.

(I) top
Crystal data top
(C10H16N)[Ni(C4H3N2S)3]Z = 2
Mr = 542.38F(000) = 564
Triclinic, P1Dx = 1.467 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 7.5730 (8) ÅCell parameters from 3472 reflections
b = 12.4729 (14) Åθ = 1.5–28.3°
c = 13.5236 (13) ŵ = 1.07 mm1
α = 90.205 (4)°T = 293 K
β = 101.633 (5)°Prism, green
γ = 100.889 (6)°0.20 × 0.20 × 0.20 mm
V = 1227.5 (2) Å3
Data collection top
Mercury CCD
diffractometer
5984 independent reflections
Radiation source: fine-focus sealed tube5426 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.017
ω scansθmax = 28.3°, θmin = 1.5°
Absorption correction: multi-scan
CrystalClear (Rigaku, 2000)
h = 109
Tmin = 0.746, Tmax = 0.807k = 1516
10173 measured reflectionsl = 1718
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.031Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.070H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0287P)2 + 0.6691P]
where P = (Fo2 + 2Fc2)/3
5984 reflections(Δ/σ)max = 0.002
293 parametersΔρmax = 0.66 e Å3
0 restraintsΔρmin = 0.49 e Å3
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
Ni10.55178 (3)0.750189 (16)0.720911 (16)0.01366 (6)
S10.22450 (6)0.66261 (3)0.68577 (3)0.01794 (9)
S20.67683 (6)0.64298 (3)0.86262 (3)0.01655 (9)
S30.55564 (6)0.92518 (3)0.81706 (3)0.02025 (10)
N10.41420 (19)0.79524 (11)0.58400 (10)0.0159 (3)
N20.0934 (2)0.74802 (12)0.50896 (11)0.0220 (3)
N30.65082 (19)0.62154 (11)0.67038 (10)0.0152 (3)
N40.7986 (2)0.49042 (12)0.76515 (11)0.0187 (3)
N50.79084 (19)0.86165 (11)0.72782 (11)0.0163 (3)
N60.8974 (2)1.03614 (13)0.81414 (12)0.0259 (3)*
N70.77060 (19)1.26891 (11)0.99198 (10)0.0159 (3)
C10.2393 (2)0.74043 (13)0.58264 (12)0.0160 (3)
C20.1281 (3)0.81372 (15)0.43428 (14)0.0247 (4)
H2A0.02810.82080.38120.030*
C30.3008 (3)0.87196 (15)0.42979 (14)0.0241 (4)
H3A0.32050.91800.37570.029*
C40.4430 (3)0.85963 (14)0.50811 (13)0.0202 (3)
H4A0.56400.89790.50790.024*
C50.7144 (2)0.57666 (13)0.75904 (12)0.0148 (3)
C60.8196 (2)0.44934 (14)0.67784 (14)0.0209 (4)
H6A0.87820.38820.67990.025*
C70.7612 (2)0.49029 (14)0.58474 (13)0.0206 (4)
H7A0.77880.45930.52400.025*
C80.6758 (2)0.57883 (14)0.58491 (13)0.0184 (3)
H8A0.63390.61000.52260.022*
C90.7679 (2)0.94579 (13)0.78562 (13)0.0173 (3)
C100.9469 (2)0.86963 (15)0.69466 (14)0.0215 (4)
H10A0.96320.81210.65330.026*
C111.0855 (3)0.96107 (17)0.71992 (16)0.0285 (4)
H11A1.19690.96820.69630.034*
C121.0541 (3)1.04107 (16)0.78077 (16)0.0291 (4)
H12A1.14891.10350.80040.035*
C130.7778 (3)1.37935 (15)1.03821 (14)0.0236 (4)
H13A0.90581.41311.06700.035*
H13B0.70671.37171.09170.035*
H13C0.72551.42550.98620.035*
C140.8424 (3)1.19674 (16)1.07283 (14)0.0261 (4)
H14A0.96941.22941.10470.039*
H14B0.83871.12461.04270.039*
H14C0.76591.18911.12380.039*
C150.8899 (2)1.28093 (15)0.91508 (13)0.0207 (4)
H15A1.01501.31700.94720.031*
H15B0.84041.32510.86030.031*
H15C0.89211.20850.88750.031*
C160.5735 (2)1.21341 (14)0.94570 (13)0.0179 (3)
H16A0.57381.13780.92340.021*
H16B0.50001.20880.99890.021*
C170.4798 (2)1.26935 (13)0.85734 (12)0.0159 (3)
C180.3853 (2)1.35207 (14)0.87108 (13)0.0196 (3)
H18A0.38481.37680.93750.023*
C190.2921 (2)1.39864 (15)0.78868 (14)0.0213 (4)
H19A0.22921.45550.79890.026*
C200.2902 (2)1.36252 (15)0.69149 (14)0.0221 (4)
H20A0.22631.39450.63500.027*
C210.3820 (3)1.27934 (15)0.67693 (13)0.0229 (4)
H21A0.38021.25400.61040.027*
C220.4764 (2)1.23317 (14)0.75928 (13)0.0194 (3)
H22A0.53921.17640.74870.023*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ni10.01325 (11)0.01303 (10)0.01471 (11)0.00287 (8)0.00259 (8)0.00043 (7)
S10.0162 (2)0.0180 (2)0.0184 (2)0.00125 (16)0.00240 (16)0.00297 (15)
S20.0174 (2)0.0193 (2)0.01275 (19)0.00365 (16)0.00248 (15)0.00004 (14)
S30.0196 (2)0.0175 (2)0.0254 (2)0.00370 (16)0.00867 (18)0.00287 (16)
N10.0170 (7)0.0146 (7)0.0164 (7)0.0040 (5)0.0032 (5)0.0005 (5)
N20.0203 (8)0.0235 (8)0.0201 (7)0.0051 (6)0.0015 (6)0.0006 (6)
N30.0165 (7)0.0140 (6)0.0147 (7)0.0024 (5)0.0026 (5)0.0014 (5)
N40.0186 (7)0.0168 (7)0.0204 (7)0.0052 (6)0.0018 (6)0.0014 (5)
N50.0150 (7)0.0175 (7)0.0174 (7)0.0053 (6)0.0036 (6)0.0024 (5)
N60.0240 (8)0.0185 (7)0.0299 (8)0.0036 (6)0.0001 (7)0.0005 (6)
N70.0141 (7)0.0187 (7)0.0141 (7)0.0022 (5)0.0017 (5)0.0033 (5)
C10.0178 (8)0.0142 (7)0.0163 (8)0.0047 (6)0.0024 (6)0.0029 (6)
C20.0297 (10)0.0243 (9)0.0177 (9)0.0084 (8)0.0040 (7)0.0002 (7)
C30.0348 (11)0.0212 (9)0.0180 (9)0.0091 (8)0.0057 (8)0.0047 (7)
C40.0252 (9)0.0166 (8)0.0197 (8)0.0046 (7)0.0063 (7)0.0017 (6)
C50.0118 (8)0.0142 (7)0.0166 (8)0.0004 (6)0.0010 (6)0.0006 (6)
C60.0185 (9)0.0162 (8)0.0283 (9)0.0060 (7)0.0032 (7)0.0024 (7)
C70.0218 (9)0.0196 (8)0.0206 (9)0.0030 (7)0.0060 (7)0.0057 (6)
C80.0198 (8)0.0184 (8)0.0154 (8)0.0012 (7)0.0024 (6)0.0002 (6)
C90.0171 (8)0.0158 (8)0.0175 (8)0.0029 (6)0.0006 (6)0.0028 (6)
C100.0164 (8)0.0265 (9)0.0242 (9)0.0090 (7)0.0054 (7)0.0089 (7)
C110.0146 (9)0.0346 (11)0.0371 (11)0.0038 (8)0.0072 (8)0.0153 (9)
C120.0178 (9)0.0256 (10)0.0365 (11)0.0060 (7)0.0021 (8)0.0082 (8)
C130.0218 (9)0.0238 (9)0.0228 (9)0.0026 (7)0.0011 (7)0.0061 (7)
C140.0199 (9)0.0317 (10)0.0244 (9)0.0043 (8)0.0004 (7)0.0132 (8)
C150.0182 (9)0.0260 (9)0.0198 (9)0.0057 (7)0.0074 (7)0.0033 (7)
C160.0147 (8)0.0186 (8)0.0176 (8)0.0009 (6)0.0009 (6)0.0033 (6)
C170.0128 (8)0.0167 (8)0.0156 (8)0.0014 (6)0.0012 (6)0.0019 (6)
C180.0192 (9)0.0235 (9)0.0152 (8)0.0031 (7)0.0028 (7)0.0023 (6)
C190.0194 (9)0.0226 (9)0.0222 (9)0.0068 (7)0.0027 (7)0.0003 (7)
C200.0199 (9)0.0264 (9)0.0188 (8)0.0045 (7)0.0011 (7)0.0044 (7)
C210.0268 (10)0.0274 (9)0.0147 (8)0.0050 (8)0.0048 (7)0.0015 (7)
C220.0188 (8)0.0193 (8)0.0198 (8)0.0041 (7)0.0033 (7)0.0016 (6)
Geometric parameters (Å, º) top
Ni1—N52.0492 (14)C7—C81.381 (2)
Ni1—N32.0635 (14)C7—H7A0.9500
Ni1—N12.0689 (14)C8—H8A0.9500
Ni1—S12.4617 (5)C10—C111.386 (3)
Ni1—S22.4743 (5)C10—H10A0.9500
Ni1—S32.5290 (5)C11—C121.375 (3)
S1—C11.7122 (17)C11—H11A0.9500
S2—C51.7232 (17)C12—H12A0.9500
S3—C91.7179 (17)C13—H13A0.9800
N1—C41.333 (2)C13—H13B0.9800
N1—C11.367 (2)C13—H13C0.9800
N2—C21.339 (2)C14—H14A0.9800
N2—C11.349 (2)C14—H14B0.9800
N3—C81.333 (2)C14—H14C0.9800
N3—C51.363 (2)C15—H15A0.9800
N4—C61.336 (2)C15—H15B0.9800
N4—C51.345 (2)C15—H15C0.9800
N5—C101.333 (2)C16—C171.506 (2)
N5—C91.364 (2)C16—H16A0.9900
N6—C121.343 (3)C16—H16B0.9900
N6—C91.344 (2)C17—C221.393 (2)
N7—C131.498 (2)C17—C181.394 (2)
N7—C151.500 (2)C18—C191.386 (2)
N7—C141.501 (2)C18—H18A0.9500
N7—C161.526 (2)C19—C201.384 (3)
C2—C31.384 (3)C19—H19A0.9500
C2—H2A0.9500C20—C211.387 (3)
C3—C41.382 (3)C20—H20A0.9500
C3—H3A0.9500C21—C221.386 (2)
C4—H4A0.9500C21—H21A0.9500
C6—C71.381 (3)C22—H22A0.9500
C6—H6A0.9500
N5—Ni1—N394.69 (6)N3—C8—C7121.57 (16)
N5—Ni1—N196.66 (6)N3—C8—H8A119.2
N3—Ni1—N199.25 (5)C7—C8—H8A119.2
N5—Ni1—S1162.19 (4)N6—C9—N5123.44 (15)
N3—Ni1—S197.38 (4)N6—C9—S3123.45 (13)
N1—Ni1—S168.52 (4)N5—C9—S3113.10 (12)
N5—Ni1—S295.47 (4)N5—C10—C11120.66 (18)
N3—Ni1—S268.50 (4)N5—C10—H10A119.7
N1—Ni1—S2163.43 (4)C11—C10—H10A119.7
S1—Ni1—S2101.113 (16)C12—C11—C10116.84 (17)
N5—Ni1—S367.63 (4)C12—C11—H11A121.6
N3—Ni1—S3158.31 (4)C10—C11—H11A121.6
N1—Ni1—S395.37 (4)N6—C12—C11123.89 (18)
S1—Ni1—S3102.858 (17)N6—C12—H12A118.1
S2—Ni1—S399.663 (18)C11—C12—H12A118.1
C1—S1—Ni177.83 (6)N7—C13—H13A109.5
C5—S2—Ni177.37 (6)N7—C13—H13B109.5
C9—S3—Ni176.34 (6)H13A—C13—H13B109.5
C4—N1—C1118.37 (15)N7—C13—H13C109.5
C4—N1—Ni1140.66 (13)H13A—C13—H13C109.5
C1—N1—Ni1100.86 (10)H13B—C13—H13C109.5
C2—N2—C1115.99 (16)N7—C14—H14A109.5
C8—N3—C5118.31 (14)N7—C14—H14B109.5
C8—N3—Ni1140.16 (12)H14A—C14—H14B109.5
C5—N3—Ni1101.40 (10)N7—C14—H14C109.5
C6—N4—C5116.22 (15)H14A—C14—H14C109.5
C10—N5—C9119.05 (15)H14B—C14—H14C109.5
C10—N5—Ni1138.16 (13)N7—C15—H15A109.5
C9—N5—Ni1102.77 (10)N7—C15—H15B109.5
C12—N6—C9116.08 (17)H15A—C15—H15B109.5
C13—N7—C15108.94 (13)N7—C15—H15C109.5
C13—N7—C14109.30 (14)H15A—C15—H15C109.5
C15—N7—C14108.97 (13)H15B—C15—H15C109.5
C13—N7—C16111.31 (13)C17—C16—N7115.15 (13)
C15—N7—C16111.59 (13)C17—C16—H16A108.5
C14—N7—C16106.67 (13)N7—C16—H16A108.5
N2—C1—N1123.78 (15)C17—C16—H16B108.5
N2—C1—S1123.47 (13)N7—C16—H16B108.5
N1—C1—S1112.73 (12)H16A—C16—H16B107.5
N2—C2—C3123.91 (17)C22—C17—C18118.77 (15)
N2—C2—H2A118.0C22—C17—C16119.61 (15)
C3—C2—H2A118.0C18—C17—C16121.47 (15)
C4—C3—C2116.53 (16)C19—C18—C17120.60 (16)
C4—C3—H3A121.7C19—C18—H18A119.7
C2—C3—H3A121.7C17—C18—H18A119.7
N1—C4—C3121.41 (17)C20—C19—C18120.20 (17)
N1—C4—H4A119.3C20—C19—H19A119.9
C3—C4—H4A119.3C18—C19—H19A119.9
N4—C5—N3123.68 (15)C19—C20—C21119.68 (17)
N4—C5—S2123.63 (13)C19—C20—H20A120.2
N3—C5—S2112.69 (12)C21—C20—H20A120.2
N4—C6—C7124.00 (16)C22—C21—C20120.18 (16)
N4—C6—H6A118.0C22—C21—H21A119.9
C7—C6—H6A118.0C20—C21—H21A119.9
C6—C7—C8116.22 (16)C21—C22—C17120.54 (16)
C6—C7—H7A121.9C21—C22—H22A119.7
C8—C7—H7A121.9C17—C22—H22A119.7
 

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