Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807008483/dn2131sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807008483/dn2131Isup2.hkl |
CCDC reference: 640319
Data collection: SMART (Bruker, 2006); cell refinement: SMART; data reduction: SAINT (Bruker, 2006); program(s) used to solve structure: SHELXTL (Sheldrick, 2000); program(s) used to refine structure: SHELXTL; molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: publCIF Westrip, 2007) and enCIFer (Allen et al., 2004).
(C10H10N2)[PdCl4] | F(000) = 396 |
Mr = 406.40 | Dx = 2.133 Mg m−3 |
Monoclinic, I2/m | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -I 2y | Cell parameters from 2186 reflections |
a = 6.718 (1) Å | θ = 3.1–25.4° |
b = 11.754 (2) Å | µ = 2.29 mm−1 |
c = 8.015 (2) Å | T = 298 K |
β = 90.649 (3)° | Prism, yellow |
V = 632.9 (2) Å3 | 0.19 × 0.08 × 0.07 mm |
Z = 2 |
Bruker SMART APEX CCD diffractometer | 613 independent reflections |
Radiation source: fine-focus sealed tube | 591 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.037 |
Detector resolution: 0.661 pixels mm-1 | θmax = 25.4°, θmin = 3.1° |
ω scans | h = −8→8 |
Absorption correction: analytical (Sheldrick, 2000) | k = −14→14 |
Tmin = 0.670, Tmax = 0.855 | l = −9→9 |
2552 measured reflections |
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) = 0.058 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.10 | w = 1/[σ2(Fo2) + (0.0295P)2 + 0.5871P] where P = (Fo2 + 2Fc2)/3 |
613 reflections | (Δ/σ)max < 0.001 |
46 parameters | Δρmax = 0.58 e Å−3 |
1 restraint | Δρmin = −0.29 e Å−3 |
Experimental. The non-standard setting I2/m for the space group C2/m was selected following the suggestions of Alan D. Mighell (Mighell, 2002) for monoclinic conventional cells |
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 | ||
Pd1 | 1.0000 | 0.0000 | 0.0000 | 0.03097 (18) | |
Cl1 | 0.79728 (13) | 0.13796 (7) | 0.10751 (11) | 0.0519 (3) | |
N1 | 0.4434 (6) | 0.0000 | 0.2829 (5) | 0.0489 (10) | |
H1 | 0.558 (4) | 0.0000 | 0.234 (6) | 0.059* | |
C2 | 0.3630 (5) | 0.0972 (3) | 0.3246 (5) | 0.0560 (9) | |
H2 | 0.4243 | 0.1651 | 0.2950 | 0.067* | |
C3 | 0.1888 (5) | 0.0993 (3) | 0.4116 (5) | 0.0502 (8) | |
H3 | 0.1330 | 0.1686 | 0.4417 | 0.060* | |
C4 | 0.0965 (6) | 0.0000 | 0.4544 (5) | 0.0333 (9) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Pd1 | 0.0321 (3) | 0.0306 (3) | 0.0304 (3) | 0.000 | 0.00733 (17) | 0.000 |
Cl1 | 0.0506 (6) | 0.0374 (5) | 0.0684 (6) | 0.0049 (3) | 0.0275 (4) | −0.0009 (4) |
N1 | 0.035 (2) | 0.074 (3) | 0.038 (2) | 0.000 | 0.0092 (16) | 0.000 |
C2 | 0.048 (2) | 0.056 (2) | 0.065 (2) | −0.0062 (18) | 0.0137 (17) | 0.0120 (18) |
C3 | 0.0444 (19) | 0.0395 (19) | 0.067 (2) | −0.0008 (14) | 0.0182 (16) | 0.0016 (16) |
C4 | 0.034 (2) | 0.036 (2) | 0.0301 (19) | 0.000 | 0.0019 (16) | 0.000 |
Pd1—Cl1 | 2.2920 (8) | C2—H2 | 0.9300 |
N1—C2i | 1.309 (4) | C3—C4 | 1.367 (4) |
N1—C2 | 1.309 (4) | C3—H3 | 0.9300 |
N1—H1 | 0.87 (3) | C4—C3i | 1.367 (4) |
C2—C3 | 1.369 (5) | C4—C4ii | 1.496 (8) |
Cl1iii—Pd1—Cl1 | 89.94 (4) | C3—C2—H2 | 119.9 |
Cl1i—Pd1—Cl1 | 90.06 (4) | C4—C3—C2 | 120.3 (3) |
Cl1iv—Pd1—Cl1 | 180.00 (5) | C4—C3—H3 | 119.8 |
C2i—N1—C2 | 121.6 (4) | C2—C3—H3 | 119.8 |
C2i—N1—H1 | 119.1 (3) | C3i—C4—C3 | 117.2 (4) |
C2—N1—H1 | 119.1 (3) | C3i—C4—C4ii | 121.4 (2) |
N1—C2—C3 | 120.2 (4) | C3—C4—C4ii | 121.4 (2) |
N1—C2—H2 | 119.9 |
Symmetry codes: (i) x, −y, z; (ii) −x, −y, −z+1; (iii) −x+2, y, −z; (iv) −x+2, −y, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···Cl1 | 0.87 (3) | 2.51 (3) | 3.214 (3) | 139 (1) |