Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536804013388/cv6324sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536804013388/cv6324Isup2.hkl |
CCDC reference: 245116
Data collection: KM4B8 (Gałdecki et al., 1997); cell refinement: KM4B8; data reduction: JANA2000 (Petříček & Dusěk, 2000); program(s) used to solve structure: SIR97 (Cascarano et al., 1996); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).
(C4H12N)2[PdCl4] | Dx = 1.479 Mg m−3 |
Mr = 396.49 | Mo Kα radiation, λ = 0.71069 Å |
Tetragonal, P42/mnm | Cell parameters from 46 reflections |
Hall symbol: -P 4n 2n | θ = 10.4–14.0° |
a = 8.8281 (10) Å | µ = 1.62 mm−1 |
c = 11.4206 (10) Å | T = 292 K |
V = 890.07 (16) Å3 | Plate, red |
Z = 2 | 0.61 × 0.41 × 0.12 mm |
F(000) = 400 |
XCalibur (KUMA) diffractometer | 639 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.039 |
Graphite monochromator | θmax = 40.5°, θmin = 2.9° |
ω/2q scans | h = −12→12 |
Absorption correction: gaussian JANA2000 (Petříček, V. & Dušek, M., 2000) | k = −16→16 |
Tmin = 0.553, Tmax = 0.814 | l = 0→15 |
5577 measured reflections | 3 standard reflections every 100 reflections |
962 independent reflections | intensity decay: 4.2% |
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)] = 0.022 | Hydrogen site location: difference Fourier map |
wR(F2) = 0.075 | H-atom parameters constrained |
S = 1.12 | w = 1/[σ2(Fo2) + (0.0375P)2 + 0.0815P] where P = (Fo2 + 2Fc2)/3 |
962 reflections | (Δ/σ)max < 0.001 |
24 parameters | Δρmax = 0.58 e Å−3 |
0 restraints | Δρmin = −0.70 e Å−3 |
9 constraints |
Experimental. The sample was prepared about 10 years ago. IR and Raman spectra were recorded on a FT–IR spectrometer Nicolet Magna 760 equipped with a Nicolet Nexus FT Raman module. The spectra were collected under following conditions: IR spectrum - fluorolube mull, 2 cm${-1}$ resolution, 32 scans, Happ-Genzel apodization; Raman spectrum - polycrystalline sample in glass vial, 2 cm${-1}$ resolution, 512 scans, Happ-Genzel apodization, 260 mW N d:YVO4 laser excitation at 1064 nm. |
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. Extinction parameter if refined converged to 0.0000 (11). |
x | y | z | Uiso*/Ueq | ||
Pd1 | 0.0000 | 0.0000 | 0.5000 | 0.04453 (13) | |
Cl1 | 0.0000 | 0.0000 | 0.70113 (11) | 0.0688 (3) | |
Cl2 | 0.18511 (7) | 0.18511 (7) | 0.5000 | 0.0630 (2) | |
N1 | 0.0000 | 0.5000 | 0.2500 | 0.0505 (6) | |
C1 | 0.1211 (3) | 0.5647 (3) | 0.3257 (2) | 0.0773 (6) | |
H1 | 0.1595 | 0.4873 | 0.3767 | 0.116* | |
H2 | 0.0801 | 0.6460 | 0.3716 | 0.116* | |
H3 | 0.2018 | 0.6025 | 0.2775 | 0.116* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Pd1 | 0.03364 (11) | 0.03364 (11) | 0.0663 (3) | 0.00231 (12) | 0.000 | 0.000 |
Cl1 | 0.0688 (4) | 0.0688 (4) | 0.0688 (6) | −0.0168 (4) | 0.000 | 0.000 |
Cl2 | 0.0514 (3) | 0.0514 (3) | 0.0862 (6) | −0.0134 (4) | 0.000 | 0.000 |
N1 | 0.0438 (8) | 0.0438 (8) | 0.0639 (18) | 0.000 | 0.000 | 0.000 |
C1 | 0.0558 (11) | 0.0837 (15) | 0.0925 (16) | −0.0078 (11) | −0.0123 (11) | −0.0142 (14) |
Pd1—Cl1 | 2.2971 (13) | N1—C1iii | 1.489 (2) |
Pd1—Cl1i | 2.2971 (13) | N1—C1iv | 1.489 (2) |
Pd1—Cl2i | 2.3110 (9) | C1—H1 | 0.9600 |
Pd1—Cl2 | 2.3110 (9) | C1—H2 | 0.9600 |
N1—C1 | 1.489 (2) | C1—H3 | 0.9600 |
N1—C1ii | 1.489 (2) | ||
Cl1—Pd1—Cl1i | 180.0 | C1—N1—C1iv | 109.0 (2) |
Cl1—Pd1—Cl2i | 90.0 | C1ii—N1—C1iv | 109.70 (10) |
Cl1i—Pd1—Cl2i | 90.0 | C1iii—N1—C1iv | 109.70 (10) |
Cl1—Pd1—Cl2 | 90.0 | N1—C1—H1 | 109.5 |
Cl1i—Pd1—Cl2 | 90.0 | N1—C1—H2 | 109.5 |
Cl2i—Pd1—Cl2 | 180.00 (4) | H1—C1—H2 | 109.5 |
C1—N1—C1ii | 109.70 (10) | N1—C1—H3 | 109.5 |
C1—N1—C1iii | 109.70 (10) | H1—C1—H3 | 109.5 |
C1ii—N1—C1iii | 109.0 (2) | H2—C1—H3 | 109.5 |
Symmetry codes: (i) −x, −y, −z+1; (ii) y−1/2, −x+1/2, −z+1/2; (iii) −y+1/2, x+1/2, −z+1/2; (iv) −x, −y+1, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
C1—H1···Cl2 | 0.96 | 3.03 | 3.939 (3) | 160 |
C1—H2···Cl2v | 0.96 | 3.14 | 4.019 (3) | 153 |
C1—H3···Cl1vi | 0.96 | 2.92 | 3.679 (3) | 137 |
Symmetry codes: (v) −x, −y+1, −z+1; (vi) −y+1/2, x+1/2, z−1/2. |