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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Dec 20;65(Pt 1):m111–m112. doi: 10.1107/S1600536808042773

1,3-Bis(thio­phen-2-ylmeth­yl)-3,4,5,6-tetra­hydro­pyrimidinium trichlorido(η6-p-cymene)ruthenate(II)

Hakan Arslan a,b,*, Don VanDerveer c, İsmail Özdemir d, Nevin Gürbüz d, Yetkin Gök d, Bekir Çetinkaya e
PMCID: PMC2968014  PMID: 21581477

Abstract

The asymmetric unit of the title compound, (C14H17N2S2)[Ru(C10H14)Cl3], contains a 1,3-bis­(thio­phen-2-ylmeth­yl)-3,4,5,6-tetra­hydro­pyrimidinium cation and a trichlorido(η6-p-cymene)ruthenate(II) anion. The Ru atom exhibits a distorted octa­hedral coordination with the benzene ring of the p-cymene ligand formally occupying three sites and three chloride atoms occupying the other three sites. The N—C bond lengths of the N—C—N unit of the pyrimidinium cation are shorter than the average single C—N bond length of 1.48 Å, thus showing double-bond character, indicating a partial electron delocalization within the N—C—N fragment. The pyrimidine ring has an envelope conformation. Four inter­molecular C—H⋯Cl hydrogen bonds generate a three-dimensional hydrogen-bonded framework.

Related literature

For the synthesis, see: Yaşar et al. (2008); Özdemir et al. (2005a , 2005b , 2007, 2008). For general background, see: Herrmann et al. (1995); Herrmann (2002); Littke & Fu (2002); Özdemir et al. (2005c ); Arduengo & Krafczyc (1998); Navarro et al. (2006). For related compounds, see: Liu et al. (2004); Therrien et al. (2004); Arslan et al. (2004a ,b , 2005a ,b , 2007a ,b ,c ). For puckering and asymmetry parameters, see: Cremer & Pople (1975); Nardelli (1983). For bond-length data, see: Allen et al. (1987).graphic file with name e-65-0m111-scheme1.jpg

Experimental

Crystal data

  • (C14H17N2S2)[Ru(C10H14)Cl3]

  • M r = 619.05

  • Triclinic, Inline graphic

  • a = 9.989 (2) Å

  • b = 11.404 (2) Å

  • c = 12.922 (3) Å

  • α = 82.10 (3)°

  • β = 67.61 (3)°

  • γ = 72.59 (3)°

  • V = 1298.2 (6) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 1.09 mm−1

  • T = 153 (2) K

  • 0.24 × 0.12 × 0.07 mm

Data collection

  • Rigaku Mercury CCD diffractometer

  • Absorption correction: multi-scan (REQAB; Jacobson, 1998) T min = 0.780, T max = 0.928

  • 9185 measured reflections

  • 4606 independent reflections

  • 4048 reflections with I > 2σ(I)

  • R int = 0.020

Refinement

  • R[F 2 > 2σ(F 2)] = 0.032

  • wR(F 2) = 0.076

  • S = 1.12

  • 4606 reflections

  • 292 parameters

  • H-atom parameters constrained

  • Δρmax = 0.61 e Å−3

  • Δρmin = −0.58 e Å−3

Data collection: CrystalClear (Rigaku/MSC, 2001); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808042773/hg2457sup1.cif

e-65-0m111-sup1.cif (30KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808042773/hg2457Isup2.hkl

e-65-0m111-Isup2.hkl (225.6KB, hkl)

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C1—H1⋯Cl1i 0.96 2.64 3.519 (4) 153
C1—H1⋯Cl2i 0.96 2.82 3.478 (4) 126
C10—H10A⋯Cl3i 0.96 2.75 3.654 (4) 156
C14—H14⋯Cl1ii 0.96 2.63 3.584 (4) 175

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

We thank the Technological and Scientific Research Council of Turkey TÜBİTAK-CNRS [TBAG-U/181 (106 T716)] and İnönü University Research Fund (B.A.P.: 2008-Güdümlü3) for financial support.

supplementary crystallographic information

Comment

N-heterocyclic carbene ligands have emerged as one of the most important classes of compounds used for catalytic reactions such as Suzuki-Miyura, Sonogashira, Stille and Heck reactions (Herrmann et al., 1995; Navarro et al., 2006; Arduengo & Krafczyc, 1998; Herrmann, 2002; Littke & Fu, 2002). Recently, we have focused on the synthesis, characterization and application of palladium, platinum and ruthenium N-heterocyclic carbene complexes as catalysts (Yaşar et al., 2008; Arslan et al., 2007a, 2007b,2007c, 2004a, 2004b, 2005a, 2005b).

To continue our studies on this topic (Özdemir et al. (2005a, 2005b, 2005c, 2007, 2008)), we report herein the X-ray crystal structure of an N-heterocyclic carbene cation (1,3-bis(thiophen-2-ylmethyl)-3,4,5,6-tetrahydropyrimidinium) and trichloro(η6-p-cymene)ruthenat(II) anion compound. The molecular structure of the title compound, (I), is depicted in Fig. 1.

The structure of the title compound consists of [C14H17N2S2]+ cations and [C10H14Cl3Ru]- anions. These groups are connected with four intermolecular C—H···Cl hydrogen bonds, thus forming a three-dimensional hydrogen-bonded network (Fig. 2). The intermolecular contacts are also listed in Table 1.

The thiophene rings are almost planar, while the pyrimidin ring is not planar. The deviations from planarity for the pyrimidin ring are C1 0.111 (4), N1 0.013 (3), C2 0.207 (4), C3 0.328 (4), C4 0.229 (4), and N2 0.010 (3) Å. The puckering parameters (Cremer & Pople, 1975) and the smallest displacement asymmetry parameters (Nardelli, 1983) for the pyrimidin ring are Q = 0.464 (4) Å, Θ = 55.1 (5) ° and φ = 236.6 (5)°, q2 = 0.381 (4) Å, and ΔC2(C1) = 2.8 (4), ΔCs(C1) = 66.6 (3). According to these results, the pyrimidin ring adopts an envelope conformation.

The coordination geometry of ruthenium is pseudooctahedral, with an average Ru—Cl bond distance of 2.427 Å. The ruthenium atom exhibits a distorted octahedral coordination with the benzene ring of the p-cymene ligand formally occupying three sites and three chloride atoms occupying three other sites. The distance between the centroid of the p-cymene ring and ruthenium atom is 1.972 (3) Å, which is longer than reported in other Ruthenium compounds (Liu et al., 2004; Therrien et al., 2004). All the other bond lengths in (I) are in normal ranges (Allen et al., 1987).

Some C—N bond lengths (N1—C1 = 1.313 (4) Å and N2—C1 = 1.312 (4) Å) for the 1,3-bis(thiophen-2-ylmethyl)-3,4,5,6-tetrahydropyrimidinium cation are shorter than the average single C—N bond length of 1.48 Å, thus showing double bond character in these C—N bonds. The other C—N bond lengths (N1—C2 1.468 (4), N1—C10 1.475 (4), N2—C5 1.466 (4) and N2—C4 1.469 (4) Å) are in agreement with the expected 1.48 Å C—N single bond lengths. This information indicates a partial electron delocalization within the N1—C1—N2 fragment.

Experimental

A suspension of 1,3-bis(thiophen-2ylmethyl)-3,4,5,6-tetrahydropyrimidinium chloride (1.1 mmol), Cs2CO3 (1.2 mmol) and [RuCl2(p-cymene)] (0.5 mmol) was heated under reflux in degassed toluene (20 ml) for 7 h. The reaction mixture was then filtered while hot, and the volume was reduced to about 10 ml before addition of n-hexane (15 ml) (Scheme 2). The precipitate formed was crystallized from CH2Cl2/diethylether (5:15 mL) to give complex as red-brown crystals. Yields: 0.232 g; 75%. M.p.: 235–236 oC. 1H NMR (CDCl3) δ: 1.38 (d, 6H, J = 6.9 Hz, CH3(C6H4)CH(CH3)2), 1.86 (quin., 2H, J = 6 Hz, NCH2CH2CH2N), 2.31 (s, 3H,CH3(C6H4)CH(CH3)2), 3.17 (m, 1H, CH3(C6H4)CH(CH3)2), 3.25 (t, 4H, J = 6 Hz, NCH2CH2CH2N), 4.75 (s, 4H, CH2C4H3S), 5.32 and 5.57 (d, 4H, J = 5.8 Hz, CH3(C6H4)CH(CH3)2), 7.05–7.64 (m, 6H, C4H3S), 8.91 (s, 1H, 2-CH). 13C NMR (CDCl3) δ: 19.0 (CH3(C6H4)CH(CH3)2), 19.1 (NCH2CH2CH2N), 22.3 (CH3(C6H4)CH(CH3)2), 30.8 (CH3(C6H4)CH(CH3)2), 42.3 (NCH2CH2CH2N), 54.5 (CH2C4H3S), 79.7, 81.8, 96.4 and 100.8 (CH3(C6H4)CH(CH3)2), 126.7, 127.5, 129.2 and 135.9 (C4H3S), 159.7 (2-CH). Anal. Calc. for C24H31S2N2RuCl3: C, 46.56; H, 5.05; N, 4.53%. Found: C, 47.19; H, 5.15; N, 4.71%.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound, showing the atom-numbering scheme and displacement ellipsoids drawn at the 50% probability level.

Fig. 2.

Fig. 2.

A packing diagram for (I).

Fig. 3.

Fig. 3.

The formetion of the title compound.

Crystal data

(C14H17N2S2)[Ru(C10H14)Cl3] Z = 2
Mr = 619.05 F(000) = 632
Triclinic, P1 Dx = 1.584 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 9.989 (2) Å Cell parameters from 4238 reflections
b = 11.404 (2) Å θ = 2.6–26.4°
c = 12.922 (3) Å µ = 1.09 mm1
α = 82.10 (3)° T = 153 K
β = 67.61 (3)° Rod, red
γ = 72.59 (3)° 0.24 × 0.12 × 0.07 mm
V = 1298.2 (6) Å3

Data collection

Rigaku Mercury CCD diffractometer 4606 independent reflections
Radiation source: Sealed Tube 4048 reflections with I > 2σ(I)
Graphite Monochromator Rint = 0.020
Detector resolution: 14.6306 pixels mm-1 θmax = 25.2°, θmin = 2.6°
ω scans h = −11→11
Absorption correction: multi-scan (REQAB; Jacobson, 1998) k = −13→13
Tmin = 0.780, Tmax = 0.928 l = −12→15
9185 measured reflections

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)] = 0.032 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.076 H-atom parameters constrained
S = 1.12 w = 1/[σ2(Fo2) + (0.0324P)2 + 1.2338P] where P = (Fo2 + 2Fc2)/3
4606 reflections (Δ/σ)max < 0.001
292 parameters Δρmax = 0.61 e Å3
0 restraints Δρmin = −0.58 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
Ru1 0.38371 (3) 0.30813 (2) 0.14309 (2) 0.01843 (9)
Cl1 0.26136 (9) 0.23176 (6) 0.32961 (6) 0.02416 (17)
Cl2 0.52125 (9) 0.38864 (7) 0.22412 (7) 0.02633 (18)
Cl3 0.18305 (9) 0.49582 (7) 0.19463 (7) 0.02786 (18)
C15 0.2964 (4) 0.2481 (3) 0.0344 (3) 0.0228 (7)
C16 0.3788 (4) 0.1460 (3) 0.0795 (3) 0.0235 (7)
H16 0.3314 0.0829 0.1191 0.028*
C17 0.5297 (4) 0.1327 (3) 0.0687 (3) 0.0269 (7)
H17 0.5828 0.0612 0.0998 0.032*
C18 0.6015 (4) 0.2255 (3) 0.0118 (3) 0.0275 (7)
C19 0.5197 (4) 0.3320 (3) −0.0321 (3) 0.0263 (7)
H19 0.5660 0.3965 −0.0692 0.032*
C20 0.3713 (4) 0.3422 (3) −0.0210 (3) 0.0241 (7)
H20 0.3178 0.4142 −0.0514 0.029*
C21 0.1370 (4) 0.2648 (3) 0.0438 (3) 0.0293 (7)
H21 0.0836 0.3498 0.0579 0.035*
C22 0.0538 (4) 0.1876 (4) 0.1380 (3) 0.0413 (9)
H22A 0.0931 0.1026 0.1184 0.062*
H22B −0.0514 0.2140 0.1493 0.062*
H22C 0.0673 0.1975 0.2057 0.062*
C23 0.1396 (5) 0.2341 (5) −0.0692 (3) 0.0540 (12)
H23A 0.2007 0.2774 −0.1284 0.081*
H23B 0.0391 0.2586 −0.0695 0.081*
H23C 0.1808 0.1473 −0.0804 0.081*
C24 0.7590 (4) 0.2154 (4) 0.0009 (3) 0.0415 (9)
H24A 0.7889 0.1509 0.0503 0.062*
H24B 0.7640 0.2918 0.0204 0.062*
H24C 0.8253 0.1969 −0.0749 0.062*
S1 0.88600 (10) 0.14274 (7) 0.52353 (8) 0.0311 (2)
S2 0.82905 (10) 0.82421 (9) 0.36678 (9) 0.0379 (2)
N1 0.7975 (3) 0.4626 (2) 0.4658 (2) 0.0205 (5)
N2 0.6275 (3) 0.6428 (2) 0.4401 (2) 0.0217 (6)
C1 0.7099 (3) 0.5733 (3) 0.4956 (3) 0.0212 (6)
H1 0.7059 0.6053 0.5620 0.025*
C2 0.8165 (4) 0.4094 (3) 0.3623 (3) 0.0306 (8)
H2A 0.7505 0.3575 0.3790 0.037*
H2B 0.9180 0.3600 0.3296 0.037*
C3 0.7812 (4) 0.5106 (3) 0.2804 (3) 0.0287 (7)
H3A 0.7792 0.4758 0.2177 0.034*
H3B 0.8584 0.5531 0.2531 0.034*
C4 0.6305 (4) 0.6005 (3) 0.3367 (3) 0.0259 (7)
H4A 0.6144 0.6696 0.2870 0.031*
H4B 0.5515 0.5614 0.3538 0.031*
C5 0.5506 (4) 0.7712 (3) 0.4710 (3) 0.0251 (7)
H5A 0.5365 0.7804 0.5475 0.030*
H5B 0.4532 0.7926 0.4651 0.030*
C6 0.6390 (4) 0.8577 (3) 0.3967 (3) 0.0236 (7)
C7 0.5853 (4) 0.9710 (3) 0.3540 (3) 0.0299 (7)
H7 0.4822 1.0059 0.3610 0.036*
C8 0.7015 (5) 1.0309 (3) 0.2979 (3) 0.0361 (9)
H8 0.6848 1.1114 0.2634 0.043*
C9 0.8369 (5) 0.9630 (3) 0.2984 (3) 0.0396 (9)
H9 0.9274 0.9892 0.2644 0.048*
C10 0.8822 (4) 0.3889 (3) 0.5353 (3) 0.0223 (6)
H10A 0.8744 0.4396 0.5919 0.027*
H10B 0.9865 0.3610 0.4893 0.027*
C11 0.8250 (3) 0.2799 (2) 0.5904 (3) 0.0202 (6)
C12 0.7240 (4) 0.2726 (3) 0.6959 (3) 0.0283 (7)
H12 0.6772 0.3394 0.7468 0.034*
C13 0.6955 (4) 0.1548 (3) 0.7223 (3) 0.0329 (8)
H13 0.6266 0.1340 0.7929 0.039*
C14 0.7752 (4) 0.0756 (3) 0.6381 (3) 0.0315 (8)
H14 0.7706 −0.0078 0.6417 0.038*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Ru1 0.01972 (14) 0.01801 (13) 0.01928 (14) −0.00846 (9) −0.00606 (11) −0.00118 (9)
Cl1 0.0309 (4) 0.0229 (4) 0.0195 (4) −0.0138 (3) −0.0051 (3) −0.0002 (3)
Cl2 0.0284 (4) 0.0307 (4) 0.0263 (4) −0.0151 (3) −0.0100 (4) −0.0045 (3)
Cl3 0.0270 (4) 0.0215 (4) 0.0339 (4) −0.0038 (3) −0.0104 (4) −0.0048 (3)
C15 0.0270 (17) 0.0242 (15) 0.0205 (16) −0.0072 (13) −0.0104 (14) −0.0056 (13)
C16 0.0302 (18) 0.0184 (14) 0.0228 (16) −0.0097 (12) −0.0065 (14) −0.0052 (12)
C17 0.0283 (18) 0.0237 (15) 0.0237 (17) −0.0007 (13) −0.0061 (15) −0.0085 (13)
C18 0.0225 (17) 0.0365 (18) 0.0220 (17) −0.0069 (14) −0.0030 (14) −0.0128 (14)
C19 0.0278 (18) 0.0365 (17) 0.0169 (16) −0.0164 (14) −0.0036 (14) −0.0040 (14)
C20 0.0305 (18) 0.0237 (15) 0.0200 (16) −0.0098 (13) −0.0097 (14) 0.0009 (13)
C21 0.0239 (18) 0.0356 (18) 0.0310 (19) −0.0116 (14) −0.0091 (15) −0.0032 (15)
C22 0.034 (2) 0.066 (3) 0.032 (2) −0.0290 (19) −0.0075 (18) −0.0043 (19)
C23 0.044 (3) 0.101 (4) 0.035 (2) −0.040 (3) −0.021 (2) 0.008 (2)
C24 0.0243 (19) 0.062 (2) 0.038 (2) −0.0107 (17) −0.0076 (18) −0.0133 (19)
S1 0.0322 (5) 0.0171 (4) 0.0397 (5) −0.0064 (3) −0.0067 (4) −0.0064 (3)
S2 0.0294 (5) 0.0416 (5) 0.0460 (6) −0.0159 (4) −0.0183 (4) 0.0163 (4)
N1 0.0258 (14) 0.0147 (11) 0.0224 (14) −0.0056 (10) −0.0095 (12) −0.0022 (10)
N2 0.0220 (14) 0.0208 (12) 0.0227 (14) −0.0070 (10) −0.0077 (12) 0.0002 (11)
C1 0.0242 (16) 0.0193 (14) 0.0207 (16) −0.0117 (12) −0.0045 (14) 0.0001 (12)
C2 0.039 (2) 0.0231 (16) 0.0313 (19) −0.0050 (14) −0.0151 (17) −0.0069 (14)
C3 0.0338 (19) 0.0314 (17) 0.0236 (17) −0.0093 (14) −0.0113 (16) −0.0051 (14)
C4 0.0288 (18) 0.0279 (16) 0.0261 (17) −0.0112 (13) −0.0128 (15) −0.0004 (14)
C5 0.0206 (16) 0.0211 (15) 0.0306 (18) −0.0015 (12) −0.0091 (15) −0.0007 (13)
C6 0.0245 (17) 0.0241 (15) 0.0235 (17) −0.0059 (13) −0.0106 (14) −0.0007 (13)
C7 0.036 (2) 0.0210 (15) 0.0309 (19) −0.0052 (14) −0.0125 (16) 0.0002 (14)
C8 0.058 (3) 0.0217 (16) 0.031 (2) −0.0154 (16) −0.0158 (19) 0.0032 (14)
C9 0.052 (3) 0.043 (2) 0.033 (2) −0.0312 (19) −0.0139 (19) 0.0075 (17)
C10 0.0242 (17) 0.0186 (14) 0.0259 (17) −0.0070 (12) −0.0108 (14) 0.0012 (12)
C11 0.0201 (16) 0.0152 (13) 0.0263 (17) −0.0044 (11) −0.0097 (14) −0.0005 (12)
C12 0.036 (2) 0.0208 (15) 0.0283 (18) −0.0104 (14) −0.0104 (16) −0.0008 (13)
C13 0.041 (2) 0.0276 (17) 0.0323 (19) −0.0176 (15) −0.0115 (17) 0.0066 (15)
C14 0.0322 (19) 0.0170 (15) 0.050 (2) −0.0090 (13) −0.0184 (18) 0.0012 (15)

Geometric parameters (Å, °)

Ru1—C16 2.144 (3) S2—C9 1.711 (4)
Ru1—C20 2.147 (3) S2—C6 1.717 (3)
Ru1—C19 2.181 (3) N1—C1 1.313 (4)
Ru1—C15 2.181 (3) N1—C2 1.468 (4)
Ru1—C17 2.183 (3) N1—C10 1.475 (4)
Ru1—C18 2.213 (3) N2—C1 1.312 (4)
Ru1—Cl3 2.4185 (13) N2—C5 1.466 (4)
Ru1—Cl1 2.4243 (11) N2—C4 1.469 (4)
Ru1—Cl2 2.4377 (9) C1—H1 0.9600
C15—C16 1.406 (4) C2—C3 1.510 (5)
C15—C20 1.444 (4) C2—H2A 0.9600
C15—C21 1.505 (4) C2—H2B 0.9600
C16—C17 1.423 (5) C3—C4 1.514 (5)
C16—H16 0.9600 C3—H3A 0.9600
C17—C18 1.418 (5) C3—H3B 0.9600
C17—H17 0.9600 C4—H4A 0.9600
C18—C19 1.427 (5) C4—H4B 0.9600
C18—C24 1.496 (5) C5—C6 1.513 (4)
C19—C20 1.404 (5) C5—H5A 0.9600
C19—H19 0.9600 C5—H5B 0.9600
C20—H20 0.9600 C6—C7 1.370 (4)
C21—C22 1.523 (5) C7—C8 1.427 (5)
C21—C23 1.537 (5) C7—H7 0.9600
C21—H21 0.9600 C8—C9 1.345 (6)
C22—H22A 0.9599 C8—H8 0.9600
C22—H22B 0.9599 C9—H9 0.9600
C22—H22C 0.9599 C10—C11 1.500 (4)
C23—H23A 0.9599 C10—H10A 0.9600
C23—H23B 0.9599 C10—H10B 0.9600
C23—H23C 0.9599 C11—C12 1.362 (5)
C24—H24A 0.9599 C12—C13 1.425 (4)
C24—H24B 0.9599 C12—H12 0.9600
C24—H24C 0.9599 C13—C14 1.347 (5)
S1—C14 1.718 (4) C13—H13 0.9600
S1—C11 1.721 (3) C14—H14 0.9600
C16—Ru1—C20 68.78 (12) C21—C22—H22C 109.5
C16—Ru1—C19 81.44 (12) H22A—C22—H22C 109.5
C20—Ru1—C19 37.86 (12) H22B—C22—H22C 109.5
C16—Ru1—C15 37.94 (12) C21—C23—H23A 109.5
C20—Ru1—C15 38.96 (11) C21—C23—H23B 109.5
C19—Ru1—C15 69.75 (12) H23A—C23—H23B 109.5
C16—Ru1—C17 38.37 (12) C21—C23—H23C 109.5
C20—Ru1—C17 81.12 (13) H23A—C23—H23C 109.5
C19—Ru1—C17 68.43 (13) H23B—C23—H23C 109.5
C15—Ru1—C17 69.25 (12) C18—C24—H24A 109.5
C16—Ru1—C18 68.65 (12) C18—C24—H24B 109.5
C20—Ru1—C18 68.32 (13) H24A—C24—H24B 109.5
C19—Ru1—C18 37.89 (13) C18—C24—H24C 109.5
C15—Ru1—C18 81.99 (12) H24A—C24—H24C 109.5
C17—Ru1—C18 37.63 (12) H24B—C24—H24C 109.5
C16—Ru1—Cl3 127.04 (9) C14—S1—C11 92.00 (16)
C20—Ru1—Cl3 86.08 (10) C9—S2—C6 91.74 (18)
C19—Ru1—Cl3 106.63 (10) C1—N1—C2 121.5 (3)
C15—Ru1—Cl3 94.62 (9) C1—N1—C10 120.4 (3)
C17—Ru1—Cl3 163.87 (9) C2—N1—C10 118.1 (2)
C18—Ru1—Cl3 143.21 (10) C1—N2—C5 119.5 (3)
C16—Ru1—Cl1 87.76 (9) C1—N2—C4 120.9 (3)
C20—Ru1—Cl1 142.92 (9) C5—N2—C4 118.8 (3)
C19—Ru1—Cl1 166.75 (9) N2—C1—N1 124.0 (3)
C15—Ru1—Cl1 105.94 (9) N2—C1—H1 118.0
C17—Ru1—Cl1 98.33 (10) N1—C1—H1 118.0
C18—Ru1—Cl1 130.29 (10) N1—C2—C3 110.0 (3)
Cl3—Ru1—Cl1 86.00 (5) N1—C2—H2A 109.7
C16—Ru1—Cl2 143.80 (9) C3—C2—H2A 109.7
C20—Ru1—Cl2 128.81 (8) N1—C2—H2B 109.7
C19—Ru1—Cl2 97.12 (9) C3—C2—H2B 109.7
C15—Ru1—Cl2 166.84 (9) H2A—C2—H2B 108.2
C17—Ru1—Cl2 107.40 (9) C2—C3—C4 110.3 (3)
C18—Ru1—Cl2 88.00 (9) C2—C3—H3A 109.6
Cl3—Ru1—Cl2 88.26 (4) C4—C3—H3A 109.6
Cl1—Ru1—Cl2 87.05 (3) C2—C3—H3B 109.6
C16—C15—C20 116.5 (3) C4—C3—H3B 109.6
C16—C15—C21 123.8 (3) H3A—C3—H3B 108.1
C20—C15—C21 119.6 (3) N2—C4—C3 109.6 (3)
C16—C15—Ru1 69.62 (17) N2—C4—H4A 109.8
C20—C15—Ru1 69.26 (17) C3—C4—H4A 109.8
C21—C15—Ru1 130.4 (2) N2—C4—H4B 109.8
C15—C16—C17 122.4 (3) C3—C4—H4B 109.8
C15—C16—Ru1 72.44 (17) H4A—C4—H4B 108.2
C17—C16—Ru1 72.29 (17) N2—C5—C6 111.7 (3)
C15—C16—H16 118.8 N2—C5—H5A 109.3
C17—C16—H16 118.8 C6—C5—H5A 109.3
Ru1—C16—H16 129.0 N2—C5—H5B 109.3
C18—C17—C16 119.8 (3) C6—C5—H5B 109.3
C18—C17—Ru1 72.33 (18) H5A—C5—H5B 107.9
C16—C17—Ru1 69.34 (17) C7—C6—C5 128.1 (3)
C18—C17—H17 120.1 C7—C6—S2 111.5 (2)
C16—C17—H17 120.1 C5—C6—S2 120.1 (2)
Ru1—C17—H17 130.9 C6—C7—C8 111.7 (3)
C17—C18—C19 119.2 (3) C6—C7—H7 124.1
C17—C18—C24 121.1 (3) C8—C7—H7 124.1
C19—C18—C24 119.7 (3) C9—C8—C7 113.0 (3)
C17—C18—Ru1 70.04 (19) C9—C8—H8 123.5
C19—C18—Ru1 69.82 (18) C7—C8—H8 123.5
C24—C18—Ru1 130.8 (2) C8—C9—S2 112.0 (3)
C20—C19—C18 119.8 (3) C8—C9—H9 124.0
C20—C19—Ru1 69.78 (18) S2—C9—H9 124.0
C18—C19—Ru1 72.29 (19) N1—C10—C11 112.0 (2)
C20—C19—H19 120.1 N1—C10—H10A 109.2
C18—C19—H19 120.1 C11—C10—H10A 109.2
Ru1—C19—H19 130.4 N1—C10—H10B 109.2
C19—C20—C15 122.2 (3) C11—C10—H10B 109.2
C19—C20—Ru1 72.36 (19) H10A—C10—H10B 107.9
C15—C20—Ru1 71.78 (18) C12—C11—C10 126.9 (3)
C19—C20—H20 118.9 C12—C11—S1 111.0 (2)
C15—C20—H20 118.9 C10—C11—S1 122.0 (2)
Ru1—C20—H20 129.6 C11—C12—C13 112.5 (3)
C15—C21—C22 113.6 (3) C11—C12—H12 123.8
C15—C21—C23 108.2 (3) C13—C12—H12 123.8
C22—C21—C23 110.5 (3) C14—C13—C12 113.1 (3)
C15—C21—H21 108.1 C14—C13—H13 123.5
C22—C21—H21 108.1 C12—C13—H13 123.5
C23—C21—H21 108.1 C13—C14—S1 111.4 (2)
C21—C22—H22A 109.5 C13—C14—H14 124.3
C21—C22—H22B 109.5 S1—C14—H14 124.3
H22A—C22—H22B 109.5
C20—Ru1—C15—C16 130.5 (3) Cl3—Ru1—C18—C24 92.4 (4)
C19—Ru1—C15—C16 102.4 (2) Cl1—Ru1—C18—C24 −76.4 (4)
C17—Ru1—C15—C16 28.64 (19) Cl2—Ru1—C18—C24 8.0 (3)
C18—Ru1—C15—C16 65.3 (2) C17—C18—C19—C20 −1.5 (5)
Cl3—Ru1—C15—C16 −151.54 (17) C24—C18—C19—C20 −179.4 (3)
Cl1—Ru1—C15—C16 −64.39 (19) Ru1—C18—C19—C20 −53.1 (3)
Cl2—Ru1—C15—C16 106.2 (4) C17—C18—C19—Ru1 51.5 (3)
C16—Ru1—C15—C20 −130.5 (3) C24—C18—C19—Ru1 −126.3 (3)
C19—Ru1—C15—C20 −28.11 (19) C16—Ru1—C19—C20 66.25 (19)
C17—Ru1—C15—C20 −101.9 (2) C15—Ru1—C19—C20 28.86 (18)
C18—Ru1—C15—C20 −65.2 (2) C17—Ru1—C19—C20 103.8 (2)
Cl3—Ru1—C15—C20 77.93 (18) C18—Ru1—C19—C20 132.3 (3)
Cl1—Ru1—C15—C20 165.08 (16) Cl3—Ru1—C19—C20 −59.96 (18)
Cl2—Ru1—C15—C20 −24.3 (5) Cl1—Ru1—C19—C20 102.0 (4)
C16—Ru1—C15—C21 117.6 (4) Cl2—Ru1—C19—C20 −150.28 (17)
C20—Ru1—C15—C21 −111.8 (4) C16—Ru1—C19—C18 −66.05 (19)
C19—Ru1—C15—C21 −139.9 (3) C20—Ru1—C19—C18 −132.3 (3)
C17—Ru1—C15—C21 146.3 (3) C15—Ru1—C19—C18 −103.44 (19)
C18—Ru1—C15—C21 −177.0 (3) C17—Ru1—C19—C18 −28.52 (18)
Cl3—Ru1—C15—C21 −33.9 (3) Cl3—Ru1—C19—C18 167.74 (15)
Cl1—Ru1—C15—C21 53.3 (3) Cl1—Ru1—C19—C18 −30.3 (5)
Cl2—Ru1—C15—C21 −136.2 (3) Cl2—Ru1—C19—C18 77.42 (17)
C20—C15—C16—C17 −2.0 (4) C18—C19—C20—C15 0.3 (5)
C21—C15—C16—C17 179.7 (3) Ru1—C19—C20—C15 −54.0 (3)
Ru1—C15—C16—C17 −54.6 (3) C18—C19—C20—Ru1 54.3 (3)
C20—C15—C16—Ru1 52.6 (2) C16—C15—C20—C19 1.4 (4)
C21—C15—C16—Ru1 −125.7 (3) C21—C15—C20—C19 179.8 (3)
C20—Ru1—C16—C15 −30.84 (19) Ru1—C15—C20—C19 54.2 (3)
C19—Ru1—C16—C15 −67.9 (2) C16—C15—C20—Ru1 −52.8 (2)
C17—Ru1—C16—C15 −133.8 (3) C21—C15—C20—Ru1 125.6 (3)
C18—Ru1—C16—C15 −105.0 (2) C16—Ru1—C20—C19 −103.8 (2)
Cl3—Ru1—C16—C15 36.5 (2) C15—Ru1—C20—C19 −133.9 (3)
Cl1—Ru1—C16—C15 119.80 (18) C17—Ru1—C20—C19 −66.1 (2)
Cl2—Ru1—C16—C15 −158.27 (15) C18—Ru1—C20—C19 −29.26 (18)
C20—Ru1—C16—C17 102.9 (2) Cl3—Ru1—C20—C19 123.75 (18)
C19—Ru1—C16—C17 65.9 (2) Cl1—Ru1—C20—C19 −158.17 (15)
C15—Ru1—C16—C17 133.8 (3) Cl2—Ru1—C20—C19 39.2 (2)
C18—Ru1—C16—C17 28.82 (19) C16—Ru1—C20—C15 30.09 (18)
Cl3—Ru1—C16—C17 170.29 (15) C19—Ru1—C20—C15 133.9 (3)
Cl1—Ru1—C16—C17 −106.42 (19) C17—Ru1—C20—C15 67.84 (19)
Cl2—Ru1—C16—C17 −24.5 (3) C18—Ru1—C20—C15 104.7 (2)
C15—C16—C17—C18 0.8 (5) Cl3—Ru1—C20—C15 −102.32 (18)
Ru1—C16—C17—C18 −53.8 (3) Cl1—Ru1—C20—C15 −24.2 (3)
C15—C16—C17—Ru1 54.7 (3) Cl2—Ru1—C20—C15 173.08 (14)
C16—Ru1—C17—C18 132.7 (3) C16—C15—C21—C22 19.9 (5)
C20—Ru1—C17—C18 65.8 (2) C20—C15—C21—C22 −158.3 (3)
C19—Ru1—C17—C18 28.70 (19) Ru1—C15—C21—C22 −71.2 (4)
C15—Ru1—C17—C18 104.3 (2) C16—C15—C21—C23 −103.1 (4)
Cl3—Ru1—C17—C18 103.7 (3) C20—C15—C21—C23 78.7 (4)
Cl1—Ru1—C17—C18 −151.71 (18) Ru1—C15—C21—C23 165.7 (3)
Cl2—Ru1—C17—C18 −62.2 (2) C5—N2—C1—N1 −171.2 (3)
C20—Ru1—C17—C16 −66.9 (2) C4—N2—C1—N1 −1.2 (4)
C19—Ru1—C17—C16 −104.0 (2) C2—N1—C1—N2 3.4 (4)
C15—Ru1—C17—C16 −28.34 (18) C10—N1—C1—N2 −177.8 (3)
C18—Ru1—C17—C16 −132.7 (3) C1—N1—C2—C3 23.7 (4)
Cl3—Ru1—C17—C16 −29.0 (4) C10—N1—C2—C3 −155.2 (3)
Cl1—Ru1—C17—C16 75.62 (18) N1—C2—C3—C4 −50.8 (4)
Cl2—Ru1—C17—C16 165.13 (16) C1—N2—C4—C3 −27.5 (4)
C16—C17—C18—C19 1.0 (5) C5—N2—C4—C3 142.6 (3)
Ru1—C17—C18—C19 −51.4 (3) C2—C3—C4—N2 52.6 (3)
C16—C17—C18—C24 178.8 (3) C1—N2—C5—C6 97.4 (3)
Ru1—C17—C18—C24 126.4 (3) C4—N2—C5—C6 −72.8 (3)
C16—C17—C18—Ru1 52.5 (3) N2—C5—C6—C7 140.6 (3)
C16—Ru1—C18—C17 −29.34 (19) N2—C5—C6—S2 −45.6 (4)
C20—Ru1—C18—C17 −104.1 (2) C9—S2—C6—C7 0.7 (3)
C19—Ru1—C18—C17 −133.3 (3) C9—S2—C6—C5 −174.1 (3)
C15—Ru1—C18—C17 −66.2 (2) C5—C6—C7—C8 173.4 (3)
Cl3—Ru1—C18—C17 −153.21 (16) S2—C6—C7—C8 −0.9 (4)
Cl1—Ru1—C18—C17 37.9 (2) C6—C7—C8—C9 0.6 (5)
Cl2—Ru1—C18—C17 122.37 (19) C7—C8—C9—S2 −0.1 (4)
C16—Ru1—C18—C19 104.0 (2) C6—S2—C9—C8 −0.4 (3)
C20—Ru1—C18—C19 29.24 (17) C1—N1—C10—C11 111.5 (3)
C15—Ru1—C18—C19 67.14 (18) C2—N1—C10—C11 −69.6 (4)
C17—Ru1—C18—C19 133.3 (3) N1—C10—C11—C12 −95.8 (4)
Cl3—Ru1—C18—C19 −19.9 (2) N1—C10—C11—S1 85.4 (3)
Cl1—Ru1—C18—C19 171.28 (14) C14—S1—C11—C12 0.0 (3)
Cl2—Ru1—C18—C19 −104.29 (17) C14—S1—C11—C10 179.0 (3)
C16—Ru1—C18—C24 −143.7 (4) C10—C11—C12—C13 −179.3 (3)
C20—Ru1—C18—C24 141.5 (4) S1—C11—C12—C13 −0.3 (4)
C19—Ru1—C18—C24 112.3 (4) C11—C12—C13—C14 0.6 (5)
C15—Ru1—C18—C24 179.4 (4) C12—C13—C14—S1 −0.6 (4)
C17—Ru1—C18—C24 −114.4 (4) C11—S1—C14—C13 0.3 (3)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C1—H1···Cl1i 0.96 2.64 3.519 (4) 153
C1—H1···Cl2i 0.96 2.82 3.478 (4) 126
C10—H10A···Cl3i 0.96 2.75 3.654 (4) 156
C14—H14···Cl1ii 0.96 2.63 3.584 (4) 175

Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x+1, −y, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HG2457).

References

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Associated Data

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

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808042773/hg2457sup1.cif

e-65-0m111-sup1.cif (30KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808042773/hg2457Isup2.hkl

e-65-0m111-Isup2.hkl (225.6KB, hkl)

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


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