The crystal structure of the title compound, (C
4H
10N)
2[SnCl
6], has been redetermined at 180 K. All atoms were located with higher precision than the previous structure determined at room temperature [Ishida
et al. (2000).
J Mol. Struct.
524, 95–103]. In the crystal, the Sn
IV atom is located on a special position of site symmetry 2/
m and is coordinated by six Cl atoms in a pseudo-octahedral geometry. Of the six Cl atoms, two equivalent axial atoms lie on the mirror plane [Sn—Cl = 2.4281 (6) Å] and the other four equivalent equatorial atoms lie on general positions [Sn—Cl = 2.4285 (4) Å]. The N atom of the pyrrolidinium cation lies on a mirror plane and the other atoms of the cation are disordered over two sites with respect to the mirror plane. Each component of the disordered five-membered rings adopts a twist conformation. The cations and anions are connected
via N—H
Cl hydrogen bonds, forming a tape-like structure propagating along [010].
Supporting information
CCDC reference: 1871008
Key indicators
- Single-crystal X-ray study
- T = 180 K
- Mean (Sn-Cl) = 0.001 Å
- Disorder in main residue
- R factor = 0.024
- wR factor = 0.057
- Data-to-parameter ratio = 19.8
checkCIF/PLATON results
No syntax errors found
Alert level G
PLAT002_ALERT_2_G Number of Distance or Angle Restraints on AtSite 3 Note
PLAT172_ALERT_4_G The CIF-Embedded .res File Contains DFIX Records 2 Report
PLAT232_ALERT_2_G Hirshfeld Test Diff (M-X) Sn1 --Cl1 . 5.3 s.u.
PLAT300_ALERT_4_G Atom Site Occupancy of C1 Constrained at 0.5 Check
PLAT300_ALERT_4_G Atom Site Occupancy of C2 Constrained at 0.5 Check
PLAT300_ALERT_4_G Atom Site Occupancy of C3 Constrained at 0.5 Check
PLAT300_ALERT_4_G Atom Site Occupancy of C4 Constrained at 0.5 Check
PLAT300_ALERT_4_G Atom Site Occupancy of H1NA Constrained at 0.5 Check
PLAT300_ALERT_4_G Atom Site Occupancy of H1A Constrained at 0.5 Check
PLAT300_ALERT_4_G Atom Site Occupancy of H1B Constrained at 0.5 Check
PLAT300_ALERT_4_G Atom Site Occupancy of H1NB Constrained at 0.5 Check
PLAT300_ALERT_4_G Atom Site Occupancy of H2A Constrained at 0.5 Check
PLAT300_ALERT_4_G Atom Site Occupancy of H2B Constrained at 0.5 Check
PLAT300_ALERT_4_G Atom Site Occupancy of H3A Constrained at 0.5 Check
PLAT300_ALERT_4_G Atom Site Occupancy of H3B Constrained at 0.5 Check
PLAT300_ALERT_4_G Atom Site Occupancy of H4A Constrained at 0.5 Check
PLAT300_ALERT_4_G Atom Site Occupancy of H4B Constrained at 0.5 Check
PLAT301_ALERT_3_G Main Residue Disorder ..............(Resd 1 ) 80% Note
PLAT720_ALERT_4_G Number of Unusual/Non-Standard Labels .......... 2 Note
PLAT789_ALERT_4_G Atoms with Negative _atom_site_disorder_group # 14 Check
PLAT811_ALERT_5_G No ADDSYM Analysis: Too Many Excluded Atoms .... ! Info
PLAT860_ALERT_3_G Number of Least-Squares Restraints ............. 2 Note
PLAT910_ALERT_3_G Missing # of FCF Reflection(s) Below Theta(Min). 2 Note
0 ALERT level A = Most likely a serious problem - resolve or explain
0 ALERT level B = A potentially serious problem, consider carefully
0 ALERT level C = Check. Ensure it is not caused by an omission or oversight
23 ALERT level G = General information/check it is not something unexpected
0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data
2 ALERT type 2 Indicator that the structure model may be wrong or deficient
3 ALERT type 3 Indicator that the structure quality may be low
17 ALERT type 4 Improvement, methodology, query or suggestion
1 ALERT type 5 Informative message, check
Data collection: RAPID-AUTO (Rigaku, 2006); cell refinement: RAPID-AUTO (Rigaku, 2006); data reduction: RAPID-AUTO (Rigaku, 2006); program(s) used to solve structure: SHELXT2018/2 (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2018/3 (Sheldrick, 2015b); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012); software used to prepare material for publication: CrystalStructure (Rigaku, 2018) and PLATON (Spek, 2009).
Bis(pyrrolidinium) hexachloridostannate
top
Crystal data top
(C4H10N)2[SnCl6] | F(000) = 468.00 |
Mr = 475.67 | Dx = 1.843 Mg m−3 |
Monoclinic, C2/m | Mo Kα radiation, λ = 0.71075 Å |
a = 16.3784 (11) Å | Cell parameters from 5181 reflections |
b = 7.3134 (3) Å | θ = 3.1–30.0° |
c = 7.1566 (4) Å | µ = 2.41 mm−1 |
β = 91.205 (2)° | T = 180 K |
V = 857.04 (8) Å3 | Platelet, colorless |
Z = 2 | 0.20 × 0.20 × 0.10 mm |
Data collection top
Rigaku R-AXIS RAPIDII diffractometer | 1308 reflections with I > 2σ(I) |
Detector resolution: 10.000 pixels mm-1 | Rint = 0.038 |
ω scans | θmax = 30.0°, θmin = 3.1° |
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | h = −22→22 |
Tmin = 0.579, Tmax = 0.786 | k = −10→9 |
5281 measured reflections | l = −10→10 |
1343 independent reflections | |
Refinement top
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)] = 0.024 | Hydrogen site location: mixed |
wR(F2) = 0.057 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.09 | w = 1/[σ2(Fo2) + (0.035P)2 + 0.3195P] where P = (Fo2 + 2Fc2)/3 |
1343 reflections | (Δ/σ)max = 0.001 |
68 parameters | Δρmax = 0.54 e Å−3 |
2 restraints | Δρmin = −1.10 e Å−3 |
Special details top
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes)
are estimated using the full covariance matrix. The cell esds are taken
into account individually in the estimation of esds in distances, angles
and torsion angles; correlations between esds in cell parameters are only
used when they are defined by crystal symmetry. An approximate (isotropic)
treatment of cell esds is used for estimating esds involving l.s. planes. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | Occ. (<1) |
Sn1 | 0.500000 | 0.500000 | 0.000000 | 0.02448 (8) | |
Cl1 | 0.61941 (4) | 0.500000 | 0.20690 (9) | 0.03911 (14) | |
Cl2 | 0.56208 (3) | 0.26144 (5) | −0.18554 (6) | 0.03335 (10) | |
N1 | 0.61485 (15) | 0.000000 | 0.1846 (3) | 0.0378 (5) | |
H1NA | 0.590 (4) | 0.082 (6) | 0.113 (7) | 0.057* | 0.5 |
H1NB | 0.595 (4) | −0.111 (5) | 0.163 (7) | 0.057* | 0.5 |
C1 | 0.7040 (2) | −0.015 (5) | 0.1454 (6) | 0.054 (3) | 0.5 |
H1A | 0.718653 | −0.141991 | 0.112102 | 0.065* | 0.5 |
H1B | 0.719081 | 0.067232 | 0.041717 | 0.065* | 0.5 |
C2 | 0.7455 (2) | 0.0412 (6) | 0.3229 (7) | 0.0512 (12) | 0.5 |
H2A | 0.750038 | 0.175930 | 0.331790 | 0.061* | 0.5 |
H2B | 0.800714 | −0.013262 | 0.334683 | 0.061* | 0.5 |
C3 | 0.6886 (2) | −0.0348 (6) | 0.4717 (5) | 0.0419 (13) | 0.5 |
H3A | 0.694280 | −0.169065 | 0.484205 | 0.050* | 0.5 |
H3B | 0.699197 | 0.023171 | 0.594843 | 0.050* | 0.5 |
C4 | 0.60557 (18) | 0.017 (3) | 0.3925 (4) | 0.034 (3) | 0.5 |
H4A | 0.562866 | −0.066758 | 0.437619 | 0.041* | 0.5 |
H4B | 0.591198 | 0.143984 | 0.427417 | 0.041* | 0.5 |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Sn1 | 0.02747 (11) | 0.01710 (11) | 0.02918 (12) | 0.000 | 0.00770 (7) | 0.000 |
Cl1 | 0.0362 (3) | 0.0386 (3) | 0.0423 (3) | 0.000 | −0.0047 (2) | 0.000 |
Cl2 | 0.0398 (2) | 0.02416 (18) | 0.0366 (2) | 0.00185 (14) | 0.01405 (15) | −0.00506 (14) |
N1 | 0.0375 (11) | 0.0426 (12) | 0.0334 (10) | 0.000 | 0.0050 (8) | 0.000 |
C1 | 0.0469 (16) | 0.059 (10) | 0.0573 (18) | 0.002 (4) | 0.0289 (14) | −0.009 (6) |
C2 | 0.0279 (14) | 0.047 (3) | 0.079 (3) | −0.0078 (14) | 0.0107 (15) | −0.0076 (19) |
C3 | 0.0323 (14) | 0.044 (4) | 0.0490 (16) | 0.0022 (14) | −0.0033 (12) | 0.0092 (16) |
C4 | 0.0279 (11) | 0.044 (8) | 0.0313 (10) | 0.006 (3) | 0.0072 (8) | 0.004 (2) |
Geometric parameters (Å, º) top
Sn1—Cl1i | 2.4281 (6) | C1—H1A | 0.9900 |
Sn1—Cl1 | 2.4281 (6) | C1—H1B | 0.9900 |
Sn1—Cl2 | 2.4285 (4) | C2—C3 | 1.534 (5) |
Sn1—Cl2i | 2.4285 (4) | C2—H2A | 0.9900 |
Sn1—Cl2ii | 2.4285 (4) | C2—H2B | 0.9900 |
Sn1—Cl2iii | 2.4285 (4) | C3—C4 | 1.512 (8) |
N1—C1 | 1.497 (5) | C3—H3A | 0.9900 |
N1—C4 | 1.504 (4) | C3—H3B | 0.9900 |
N1—H1NA | 0.883 (19) | C4—H4A | 0.9900 |
N1—H1NB | 0.89 (2) | C4—H4B | 0.9900 |
C1—C2 | 1.486 (12) | | |
| | | |
Cl1i—Sn1—Cl1 | 180.0 | N1—C1—H1A | 110.9 |
Cl1i—Sn1—Cl2 | 90.439 (16) | C2—C1—H1B | 110.9 |
Cl1—Sn1—Cl2 | 89.560 (16) | N1—C1—H1B | 110.9 |
Cl1i—Sn1—Cl2i | 89.561 (16) | H1A—C1—H1B | 108.9 |
Cl1—Sn1—Cl2i | 90.440 (16) | C1—C2—C3 | 102.7 (7) |
Cl2—Sn1—Cl2i | 180.000 (18) | C1—C2—H2A | 111.2 |
Cl1i—Sn1—Cl2ii | 89.561 (16) | C3—C2—H2A | 111.2 |
Cl1—Sn1—Cl2ii | 90.440 (16) | C1—C2—H2B | 111.2 |
Cl2—Sn1—Cl2ii | 88.151 (19) | C3—C2—H2B | 111.2 |
Cl2i—Sn1—Cl2ii | 91.849 (19) | H2A—C2—H2B | 109.1 |
Cl1i—Sn1—Cl2iii | 90.439 (16) | C4—C3—C2 | 101.7 (5) |
Cl1—Sn1—Cl2iii | 89.560 (16) | C4—C3—H3A | 111.4 |
Cl2—Sn1—Cl2iii | 91.849 (19) | C2—C3—H3A | 111.4 |
Cl2i—Sn1—Cl2iii | 88.151 (19) | C4—C3—H3B | 111.4 |
Cl2ii—Sn1—Cl2iii | 180.000 (13) | C2—C3—H3B | 111.4 |
C1—N1—C4 | 108.1 (3) | H3A—C3—H3B | 109.3 |
C1—N1—H1NA | 112 (5) | N1—C4—C3 | 104.0 (5) |
C4—N1—H1NA | 118 (4) | N1—C4—H4A | 111.0 |
C1—N1—H1NB | 105 (5) | C3—C4—H4A | 111.0 |
C4—N1—H1NB | 102 (4) | N1—C4—H4B | 111.0 |
H1NA—N1—H1NB | 110 (4) | C3—C4—H4B | 111.0 |
C2—C1—N1 | 104.5 (7) | H4A—C4—H4B | 109.0 |
C2—C1—H1A | 110.9 | | |
| | | |
C4—N1—C1—C2 | −14 (2) | C1—N1—C4—C3 | −13 (2) |
N1—C1—C2—C3 | 36 (2) | C2—C3—C4—N1 | 34.7 (13) |
C1—C2—C3—C4 | −43.9 (15) | | |
Symmetry codes: (i) −x+1, −y+1, −z; (ii) −x+1, y, −z; (iii) x, −y+1, z. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1NA···Cl2 | 0.88 (5) | 2.54 (5) | 3.365 (2) | 156 (5) |
N1—H1NB···Cl2iv | 0.89 (4) | 2.81 (6) | 3.472 (2) | 133 (5) |
N1—H1NB···Cl2v | 0.89 (4) | 2.77 (5) | 3.365 (2) | 126 (4) |
Symmetry codes: (iv) −x+1, −y, −z; (v) x, −y, z. |