Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807030115/rk2020sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807030115/rk2020Isup2.hkl |
CCDC reference: 654812
Key indicators
- Single-crystal X-ray study
- T = 373 K
- Mean (C-C) = 0.002 Å
- R factor = 0.016
- wR factor = 0.033
- Data-to-parameter ratio = 30.6
checkCIF/PLATON results
No syntax errors found
Alert level C PLAT066_ALERT_1_C Predicted and Reported Transmissions Identical . ? PLAT244_ALERT_4_C Low 'Solvent' Ueq as Compared to Neighbors for B1
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 33.17 From the CIF: _reflns_number_total 6509 Count of symmetry unique reflns 3802 Completeness (_total/calc) 171.20% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 2707 Fraction of Friedel pairs measured 0.712 Are heavy atom types Z>Si present yes PLAT794_ALERT_5_G Check Predicted Bond Valency for Pt1 (9) 2.95
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 2 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 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 2 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check
The corresponding complexes with both PtII and PdII have been previously reported as chloride salts (Mason et al., 2006). For related literature, see: Brooks et al. (1989).
The synthesis of (I) was completed through reaction of the previously reported chloride salt with an excess of AgBF4, followed by filtration to remove the solid AgCl (Mason et al., 2006, Brooks et al., 1989). Crystals where grown by slow vapor diffusion of diethylether into a saturated chloroform solution of (I).
All H atoms were placed in calculated positions and constrained to ride on their parent atoms, with C—H distances in the range of 0.93–0.97Å, with Uiso(H) = 1.2 times Ueq(C).
The crystal structure of (I) consists of [Pt(C16H18P2)2]2+ cations and BF4- anions (Fig. 1). The cation shows a distorted square planar geometry around the metal center with two non-coordinating BF4- anions. The P—Pt—P bite angle observed in the structure is 72.908 (13)°. Additionally, the phenyl substituents on the phosphorus atoms are arranged in a parallel fashion, with a distance between the center of the phenyl rings of 3.727 Å and a dihedral angle of 2.15 (4)° between the rings. The parallel arrangement of phenyl rings is not, however, repeated in the unit cell between individual molecules. The parallel arrangement of the phenyl rings within the molecule was also observed in the previously reported analogous PtII an Pd(II) chloride complexes (Mason et al., 2006).
The corresponding complexes with both PtII and PdII have been previously reported as chloride salts (Mason et al., 2006). For related literature, see: Brooks et al. (1989).
Data collection: SMART (Bruker, 2000); cell refinement: SAINT (Bruker, 2000); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 2000); software used to prepare material for publication: SHELXTL.
Fig. 1. The molecular structure of (I), with atom labels and 50% probability displacement ellipsoids. H–atoms are drawn as spheres with arbitrary radius. |
[Pt(C16H18P2)2](BF4)2 | Dx = 1.775 Mg m−3 |
Mr = 913.20 | Melting point: not measured K |
Tetragonal, P41212 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 4abw 2nw | Cell parameters from 8065 reflections |
a = 10.83270 (15) Å | θ = 2.3–33.2° |
c = 29.1244 (6) Å | µ = 4.36 mm−1 |
V = 3417.67 (10) Å3 | T = 373 K |
Z = 4 | Prismatic, colorless |
F(000) = 1792 | 0.47 × 0.25 × 0.10 mm |
Bruker APEXII area-detector diffractometer | 6509 independent reflections |
Radiation source: fine-focus sealed tube | 6151 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.028 |
φ and ω scans | θmax = 33.2°, θmin = 2.0° |
Absorption correction: multi-scan (SADABS; Bruker, 2000) | h = −16→16 |
Tmin = 0.281, Tmax = 0.647 | k = −16→16 |
41078 measured reflections | l = −44→44 |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.016 | H-atom parameters constrained |
wR(F2) = 0.033 | w = 1/[σ2(Fo2) + (0.0084P)2] where P = (Fo2 + 2Fc2)/3 |
S = 0.98 | (Δ/σ)max = 0.003 |
6509 reflections | Δρmax = 0.69 e Å−3 |
213 parameters | Δρmin = −0.87 e Å−3 |
0 restraints | Absolute structure: Flack (1983) |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: 0.007 (3) |
[Pt(C16H18P2)2](BF4)2 | Z = 4 |
Mr = 913.20 | Mo Kα radiation |
Tetragonal, P41212 | µ = 4.36 mm−1 |
a = 10.83270 (15) Å | T = 373 K |
c = 29.1244 (6) Å | 0.47 × 0.25 × 0.10 mm |
V = 3417.67 (10) Å3 |
Bruker APEXII area-detector diffractometer | 6509 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2000) | 6151 reflections with I > 2σ(I) |
Tmin = 0.281, Tmax = 0.647 | Rint = 0.028 |
41078 measured reflections |
R[F2 > 2σ(F2)] = 0.016 | H-atom parameters constrained |
wR(F2) = 0.033 | Δρmax = 0.69 e Å−3 |
S = 0.98 | Δρmin = −0.87 e Å−3 |
6509 reflections | Absolute structure: Flack (1983) |
213 parameters | Absolute structure parameter: 0.007 (3) |
0 restraints |
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 > 2σ(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 | ||
Pt1 | 0.832348 (5) | 0.832348 (5) | 0.0000 | 0.01048 (2) | |
P1 | 0.84079 (4) | 1.00450 (4) | 0.045922 (11) | 0.01195 (6) | |
P2 | 0.84132 (4) | 0.64859 (3) | −0.040032 (12) | 0.01251 (7) | |
C1 | 0.97255 (15) | 1.10328 (14) | 0.05191 (5) | 0.0148 (3) | |
C2 | 0.96273 (16) | 1.23257 (15) | 0.04781 (6) | 0.0184 (3) | |
H2A | 0.8872 | 1.2691 | 0.0411 | 0.022* | |
C3 | 1.06751 (18) | 1.30451 (16) | 0.05401 (6) | 0.0234 (4) | |
H3A | 1.0617 | 1.3900 | 0.0518 | 0.028* | |
C4 | 1.18032 (18) | 1.25058 (17) | 0.06340 (6) | 0.0247 (4) | |
H4A | 1.2497 | 1.2999 | 0.0676 | 0.030* | |
C5 | 1.19046 (15) | 1.12267 (17) | 0.06662 (6) | 0.0221 (3) | |
H5A | 1.2667 | 1.0865 | 0.0725 | 0.026* | |
C6 | 1.08678 (15) | 1.04949 (15) | 0.06097 (5) | 0.0180 (3) | |
H6A | 1.0934 | 0.9641 | 0.0632 | 0.022* | |
C7 | 0.80596 (14) | 0.94231 (14) | 0.10316 (5) | 0.0150 (3) | |
H7A | 0.8759 | 0.8950 | 0.1143 | 0.018* | |
H7B | 0.7912 | 1.0097 | 0.1244 | 0.018* | |
C8 | 0.70129 (14) | 1.09169 (15) | 0.03316 (5) | 0.0163 (3) | |
H8A | 0.6819 | 1.1469 | 0.0584 | 0.020* | |
H8B | 0.7130 | 1.1407 | 0.0056 | 0.020* | |
C9 | 0.85797 (14) | 0.68966 (14) | −0.10070 (5) | 0.0158 (3) | |
H9A | 0.8950 | 0.6219 | −0.1176 | 0.019* | |
H9B | 0.7778 | 0.7074 | −0.1140 | 0.019* | |
C10 | 0.99765 (16) | 0.59454 (13) | −0.02600 (5) | 0.0171 (3) | |
H10A | 1.0004 | 0.5669 | 0.0057 | 0.021* | |
H10B | 1.0192 | 0.5254 | −0.0456 | 0.021* | |
C11 | 0.73590 (14) | 0.52277 (14) | −0.03228 (5) | 0.0152 (3) | |
C12 | 0.70222 (14) | 0.49227 (15) | 0.01255 (5) | 0.0158 (3) | |
H12A | 0.7375 | 0.5341 | 0.0371 | 0.019* | |
C13 | 0.61647 (15) | 0.40002 (15) | 0.02062 (5) | 0.0180 (3) | |
H13A | 0.5941 | 0.3799 | 0.0505 | 0.022* | |
C14 | 0.56379 (15) | 0.33727 (16) | −0.01647 (6) | 0.0192 (3) | |
H14A | 0.5052 | 0.2762 | −0.0112 | 0.023* | |
C15 | 0.59824 (17) | 0.36542 (15) | −0.06104 (6) | 0.0223 (4) | |
H15A | 0.5640 | 0.3220 | −0.0855 | 0.027* | |
C16 | 0.68378 (16) | 0.45819 (14) | −0.06942 (5) | 0.0200 (3) | |
H16A | 0.7064 | 0.4775 | −0.0994 | 0.024* | |
B1 | 1.00964 (16) | 0.65886 (17) | 0.10947 (5) | 0.0167 (3) | |
F1 | 1.01041 (11) | 0.72699 (9) | 0.14989 (4) | 0.0289 (2) | |
F2 | 1.07033 (10) | 0.54795 (10) | 0.11657 (4) | 0.0334 (3) | |
F3 | 0.88695 (10) | 0.63397 (11) | 0.09696 (4) | 0.0319 (3) | |
F4 | 1.06599 (11) | 0.72618 (12) | 0.07492 (4) | 0.0350 (3) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Pt1 | 0.01143 (2) | 0.01143 (2) | 0.00858 (3) | 0.00085 (3) | 0.00064 (2) | −0.00064 (2) |
P1 | 0.01367 (15) | 0.01235 (14) | 0.00981 (13) | 0.00177 (18) | −0.00029 (13) | −0.00078 (13) |
P2 | 0.01565 (16) | 0.01150 (16) | 0.01038 (13) | 0.00070 (17) | 0.00073 (13) | −0.00081 (12) |
C1 | 0.0182 (7) | 0.0147 (7) | 0.0114 (6) | −0.0019 (6) | 0.0002 (5) | −0.0015 (5) |
C2 | 0.0240 (8) | 0.0171 (7) | 0.0143 (7) | 0.0012 (7) | 0.0012 (6) | 0.0002 (6) |
C3 | 0.0348 (9) | 0.0178 (8) | 0.0177 (7) | −0.0063 (8) | 0.0012 (7) | −0.0003 (6) |
C4 | 0.0259 (9) | 0.0275 (8) | 0.0208 (7) | −0.0122 (8) | 0.0007 (7) | −0.0016 (6) |
C5 | 0.0172 (8) | 0.0300 (8) | 0.0190 (7) | −0.0040 (7) | −0.0025 (6) | −0.0013 (6) |
C6 | 0.0197 (7) | 0.0180 (7) | 0.0165 (7) | 0.0010 (7) | −0.0025 (6) | −0.0010 (6) |
C7 | 0.0180 (7) | 0.0175 (7) | 0.0094 (6) | 0.0006 (6) | −0.0012 (5) | −0.0007 (5) |
C8 | 0.0183 (7) | 0.0147 (6) | 0.0158 (7) | 0.0039 (6) | −0.0004 (5) | −0.0013 (5) |
C9 | 0.0192 (7) | 0.0165 (7) | 0.0116 (6) | −0.0016 (6) | −0.0002 (5) | −0.0010 (5) |
C10 | 0.0197 (7) | 0.0142 (6) | 0.0174 (6) | 0.0037 (7) | −0.0004 (6) | 0.0008 (5) |
C11 | 0.0186 (7) | 0.0125 (7) | 0.0145 (6) | 0.0016 (6) | 0.0003 (5) | −0.0006 (5) |
C12 | 0.0210 (7) | 0.0154 (6) | 0.0111 (5) | 0.0010 (7) | −0.0018 (5) | −0.0008 (5) |
C13 | 0.0216 (8) | 0.0157 (7) | 0.0168 (6) | 0.0002 (6) | 0.0004 (6) | 0.0037 (6) |
C14 | 0.0212 (7) | 0.0143 (6) | 0.0222 (7) | −0.0010 (7) | −0.0016 (6) | 0.0014 (6) |
C15 | 0.0280 (8) | 0.0193 (7) | 0.0196 (7) | −0.0043 (7) | −0.0037 (6) | −0.0041 (6) |
C16 | 0.0257 (8) | 0.0188 (7) | 0.0154 (6) | −0.0020 (7) | −0.0001 (6) | −0.0014 (5) |
B1 | 0.0159 (7) | 0.0186 (8) | 0.0157 (6) | −0.0001 (7) | 0.0008 (6) | −0.0001 (6) |
F1 | 0.0368 (6) | 0.0281 (5) | 0.0220 (5) | 0.0017 (6) | 0.0052 (5) | −0.0078 (4) |
F2 | 0.0316 (6) | 0.0203 (5) | 0.0484 (7) | 0.0082 (5) | −0.0111 (5) | −0.0084 (5) |
F3 | 0.0193 (5) | 0.0343 (6) | 0.0422 (7) | −0.0048 (5) | −0.0082 (5) | 0.0085 (5) |
F4 | 0.0357 (6) | 0.0486 (7) | 0.0208 (5) | −0.0118 (6) | 0.0064 (5) | 0.0078 (5) |
Pt1—P1 | 2.2967 (4) | C8—C10i | 1.555 (2) |
Pt1—P1i | 2.2967 (4) | C8—H8A | 0.9700 |
Pt1—P2 | 2.3089 (3) | C8—H8B | 0.9700 |
Pt1—P2i | 2.3089 (3) | C9—C7i | 1.558 (2) |
P1—C1 | 1.7924 (16) | C9—H9A | 0.9700 |
P1—C8 | 1.8204 (16) | C9—H9B | 0.9700 |
P1—C7 | 1.8372 (15) | C10—C8i | 1.555 (2) |
P2—C11 | 1.7924 (16) | C10—H10A | 0.9700 |
P2—C9 | 1.8309 (15) | C10—H10B | 0.9700 |
P2—C10 | 1.8379 (17) | C11—C12 | 1.395 (2) |
C1—C6 | 1.393 (2) | C11—C16 | 1.407 (2) |
C1—C2 | 1.410 (2) | C12—C13 | 1.384 (2) |
C2—C3 | 1.389 (2) | C12—H12A | 0.9300 |
C2—H2A | 0.9300 | C13—C14 | 1.398 (2) |
C3—C4 | 1.382 (3) | C13—H13A | 0.9300 |
C3—H3A | 0.9300 | C14—C15 | 1.384 (2) |
C4—C5 | 1.393 (3) | C14—H14A | 0.9300 |
C4—H4A | 0.9300 | C15—C16 | 1.389 (2) |
C5—C6 | 1.385 (2) | C15—H15A | 0.9300 |
C5—H5A | 0.9300 | C16—H16A | 0.9300 |
C6—H6A | 0.9300 | B1—F4 | 1.3845 (19) |
C7—C9i | 1.558 (2) | B1—F2 | 1.385 (2) |
C7—H7A | 0.9700 | B1—F1 | 1.3894 (18) |
C7—H7B | 0.9700 | B1—F3 | 1.404 (2) |
P1—Pt1—P1i | 105.93 (2) | C10i—C8—P1 | 107.75 (11) |
P1—Pt1—P2 | 172.928 (14) | C10i—C8—H8A | 110.2 |
P1i—Pt1—P2 | 72.908 (13) | P1—C8—H8A | 110.2 |
P1—Pt1—P2i | 72.908 (13) | C10i—C8—H8B | 110.2 |
P1i—Pt1—P2i | 172.928 (13) | P1—C8—H8B | 110.2 |
P2—Pt1—P2i | 109.12 (2) | H8A—C8—H8B | 108.5 |
C1—P1—C8 | 111.79 (7) | C7i—C9—P2 | 107.38 (10) |
C1—P1—C7 | 107.11 (7) | C7i—C9—H9A | 110.2 |
C8—P1—C7 | 101.83 (7) | P2—C9—H9A | 110.2 |
C1—P1—Pt1 | 124.97 (5) | C7i—C9—H9B | 110.2 |
C8—P1—Pt1 | 105.63 (5) | P2—C9—H9B | 110.2 |
C7—P1—Pt1 | 102.85 (5) | H9A—C9—H9B | 108.5 |
C11—P2—C9 | 111.66 (7) | C8i—C10—P2 | 109.69 (10) |
C11—P2—C10 | 108.47 (7) | C8i—C10—H10A | 109.7 |
C9—P2—C10 | 101.61 (7) | P2—C10—H10A | 109.7 |
C11—P2—Pt1 | 124.41 (5) | C8i—C10—H10B | 109.7 |
C9—P2—Pt1 | 106.38 (5) | P2—C10—H10B | 109.7 |
C10—P2—Pt1 | 101.61 (5) | H10A—C10—H10B | 108.2 |
C6—C1—C2 | 119.91 (16) | C12—C11—C16 | 119.80 (14) |
C6—C1—P1 | 118.43 (12) | C12—C11—P2 | 117.68 (12) |
C2—C1—P1 | 121.66 (13) | C16—C11—P2 | 122.48 (12) |
C3—C2—C1 | 119.01 (16) | C13—C12—C11 | 120.34 (14) |
C3—C2—H2A | 120.5 | C13—C12—H12A | 119.8 |
C1—C2—H2A | 120.5 | C11—C12—H12A | 119.8 |
C4—C3—C2 | 120.76 (16) | C12—C13—C14 | 119.59 (14) |
C4—C3—H3A | 119.6 | C12—C13—H13A | 120.2 |
C2—C3—H3A | 119.6 | C14—C13—H13A | 120.2 |
C3—C4—C5 | 120.23 (17) | C15—C14—C13 | 120.48 (15) |
C3—C4—H4A | 119.9 | C15—C14—H14A | 119.8 |
C5—C4—H4A | 119.9 | C13—C14—H14A | 119.8 |
C6—C5—C4 | 119.84 (17) | C14—C15—C16 | 120.28 (15) |
C6—C5—H5A | 120.1 | C14—C15—H15A | 119.9 |
C4—C5—H5A | 120.1 | C16—C15—H15A | 119.9 |
C5—C6—C1 | 120.24 (15) | C15—C16—C11 | 119.50 (15) |
C5—C6—H6A | 119.9 | C15—C16—H16A | 120.2 |
C1—C6—H6A | 119.9 | C11—C16—H16A | 120.2 |
C9i—C7—P1 | 109.84 (10) | F4—B1—F2 | 110.86 (14) |
C9i—C7—H7A | 109.7 | F4—B1—F1 | 109.47 (14) |
P1—C7—H7A | 109.7 | F2—B1—F1 | 109.35 (12) |
C9i—C7—H7B | 109.7 | F4—B1—F3 | 109.26 (13) |
P1—C7—H7B | 109.7 | F2—B1—F3 | 108.75 (14) |
H7A—C7—H7B | 108.2 | F1—B1—F3 | 109.12 (13) |
Symmetry code: (i) y, x, −z. |
Experimental details
Crystal data | |
Chemical formula | [Pt(C16H18P2)2](BF4)2 |
Mr | 913.20 |
Crystal system, space group | Tetragonal, P41212 |
Temperature (K) | 373 |
a, c (Å) | 10.83270 (15), 29.1244 (6) |
V (Å3) | 3417.67 (10) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 4.36 |
Crystal size (mm) | 0.47 × 0.25 × 0.10 |
Data collection | |
Diffractometer | Bruker APEXII area-detector |
Absorption correction | Multi-scan (SADABS; Bruker, 2000) |
Tmin, Tmax | 0.281, 0.647 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 41078, 6509, 6151 |
Rint | 0.028 |
(sin θ/λ)max (Å−1) | 0.770 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.016, 0.033, 0.98 |
No. of reflections | 6509 |
No. of parameters | 213 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.69, −0.87 |
Absolute structure | Flack (1983) |
Absolute structure parameter | 0.007 (3) |
Computer programs: SMART (Bruker, 2000), SAINT (Bruker, 2000), SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 2000), SHELXTL.
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The crystal structure of (I) consists of [Pt(C16H18P2)2]2+ cations and BF4- anions (Fig. 1). The cation shows a distorted square planar geometry around the metal center with two non-coordinating BF4- anions. The P—Pt—P bite angle observed in the structure is 72.908 (13)°. Additionally, the phenyl substituents on the phosphorus atoms are arranged in a parallel fashion, with a distance between the center of the phenyl rings of 3.727 Å and a dihedral angle of 2.15 (4)° between the rings. The parallel arrangement of phenyl rings is not, however, repeated in the unit cell between individual molecules. The parallel arrangement of the phenyl rings within the molecule was also observed in the previously reported analogous PtII an Pd(II) chloride complexes (Mason et al., 2006).