metal-organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

Journal logoIUCrDATA
ISSN: 2414-3146

4,4′-Bi­pyridine-1,1′-diium tetra­chloridodi­fluorido­stannate(IV) monohydrate

crossmark logo

aEcole Nationale Superieure de Biotechnologie de Constantine, Algeria, bLaboratoire de Technologie des Materiaux Avances, Ecole Nationale Polytechnique de Constantine, Algeria, and cUnite De Recherche Chimie De L'Environnement Et Moleculaire Structurale, URCHEMS, University of Constantine 1-Mentouri Brothers, Algeria
*Correspondence e-mail: [email protected]

Edited by W. T. A. Harrison, University of Aberdeen, United Kingdom (Received 5 June 2025; accepted 1 July 2025; online 11 July 2025)

In the title hydrated salt, (C10H10N2)[SnF2Cl4]·H2O, the dihedral angle between the pyridinium rings in the cation is 40.5 (4)° and the F atoms in the octa­hedral complex anion have a cis disposition [F—Sn—F = 85.32 (17)°]. In the extended structure, alternating cationic and anionic layers occur, linked by extensive hydrogen bonding, with water mol­ecules inserted between the layers.

3D view (loading...)
[Scheme 3D1]
Chemical scheme
[Scheme 1]

Structure description

The title compound, (C10H10N22+)[SnF2Cl4]2–·H2O, crystallizes in the non-centrosymmetric ortho­rhom­bic space group Pna21 with one cation, one anion and one water mol­ecule in the asymmetric unit (Fig. 1[link]). The bipyridinium cation exhibits structural parameters indicative of protonation: the inter-ring C—C bond length is 1.476 (7) Å, while the average intra-ring C—C bond length is 1.384 (3) Å, reflecting aromatic conjugation. The C—N bonds measure 1.341 (9) Å or less, which are shorter than those in neutral bi­pyridine, due to the cationic charge. Angular distortions are observed with C—C—C angles in the range 117.9 (5)°–121.0 (6)° and C—N—C angles of 122.4 (5) and 123.0 (6)°, in agreement with literature data (e.g., Horiacha et al., 2022[Horiacha, M., Nychyporuk, G., Pöttgen, R., Kaczorowski, D. & Zaremba, V. (2022). Z. Krist. 237, 281-286.]). The dihedral angle between the C1–C5/N1 and C6–C10/N2 pyridinium rings is 40.5 (4)°, which can be attributed to intra­molecular (steric) inter­actions (Gheribi et al., 2022[Gheribi, R., Hadji, D., Ghallab, R., Medjani, M., Benslimane, M., Trifa, C., Dénès, G. & Merazig, H. (2022). J. Mol. Struct. 1248, 131392.]). The [SnF2Cl4]2– anion adopts a distorted octa­hedral coordination sphere around the SnIV atom, with Sn—Cl bond lengths ranging from 2.383 (2) to 2.418 (2) Å and Sn—F bonds of 2.030 (4) and 2.096 (4) Å. The bond angles deviate somewhat from ideal octa­hedral values, with notable examples being 87.98 (13)° for F1—Sn1—F2 and 93.84 (8)° for Cl2—Sn1—Cl4, consistent with previous reports (Bruhn & Preetz, 1996[Bruhn, C. & Preetz, W. (1996). Acta Cryst. C52, 321-325.]).

[Figure 1]
Figure 1
The mol­ecular structure of the title compound with displacement ellipsoids drawn at the 50% probability level.

The extended structure reveals alternating layers of cations and anions separated by inter­stitial water mol­ecules (Fig. 2[link]). Eight hydrogen bonds consolidate the tri-periodic network (Table 1[link]), including one strong (N1—H1⋯F2), two moderate (N2—H2⋯O1W and O1W—H1WA⋯Cl1), and five weak inter­actions (O1W—H1WB⋯Cl4, O1W—H1WB⋯F2, N2—H2⋯F1, C1—H1A⋯Cl3 and C9—H9⋯F1). Water mol­ecules mediate cyclic motifs in the bc plane via O1W—H⋯Cl/F inter­actions, generating a supra­molecular R44(12) graph-set motif (Fig. 3[link]). Intra­layer cohesion is ensured by weak ππ stacking inter­actions with centroid–centroid distances of 3.950 (4) Å, while inter­layer bridging is provided by a Sn—Cl4⋯Cg(2 − x, 1 − y, −Mathematical equation + z) halogen⋯π contact [Cl⋯π = 3.472 (4) Å, Sn—Cl⋯π = 110.42 (9)°] linking the [SnF2Cl4]2– anion to the N2 ring of the bipyridinium cation. The crystal packing is thus supported by directional hydrogen bonds, face-to-face π-stacking within cationic layers, and anion–cation halogen⋯π contacts.

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1⋯F2i 0.86 1.79 2.629 (6) 163
N2—H2⋯F1 0.86 2.32 2.989 (6) 134
N2—H2⋯O1Wii 0.86 2.11 2.819 (10) 140
O1W—H1WA⋯Cl1iii 0.85 2.51 3.324 (8) 159
O1W—H1WB⋯Cl4ii 0.85 2.72 3.366 (8) 134
O1W—H1WB⋯F2iv 0.85 2.32 2.906 (9) 126
C1—H1A⋯Cl3iv 0.93 2.82 3.473 (6) 128
C9—H9⋯F1ii 0.93 2.44 3.109 (9) 129
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation; (iv) Mathematical equation.
[Figure 2]
Figure 2
Projection of the crystal packing on (a) the ab plane and (b) the bc plane.
[Figure 3]
Figure 3
Sequence of R44(12) loops in the structure.

Synthesis and crystallization

Tin(II) fluoride (1.56 mmol) was combined with 4,4′-bi­pyridine (1.56 mmol) in a 1:1 molar ratio. A few drops of hydro­chloric acid were added to the mixture in a minimal volume of distilled water to facilitate dissolution. After thorough stirring, the solution was transferred into a Biotage microwave vial (2–5 ml) and heated in an oven at 393 K for three days. Upon gradual cooling to room temperature, prismatic crystals of the title compound formed and were isolated under an optical microscope for further analysis.

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link]. The crystal studied was refined as a two-component inversion twin.

Table 2
Experimental details

Crystal data
Chemical formula (C10H10N2)[SnCl4F2]·H2O
Mr 474.71
Crystal system, space group Orthorhombic, Pna21
Temperature (K) 293
a, b, c (Å) 7.5641 (2), 26.5989 (5), 7.9422 (2)
V3) 1597.94 (7)
Z 4
Radiation type Mo Kα
μ (mm−1) 2.28
Crystal size (mm) 0.08 × 0.08 × 0.07
 
Data collection
Diffractometer Bruker SMART APEXII area detector
Absorption correction Multi-scan (SADABS; Krause et al., 2015[Krause, L., Herbst-Irmer, R., Sheldrick, G. M. & Stalke, D. (2015). J. Appl. Cryst. 48, 3-10.])
Tmin, Tmax 0.852, 0.852
No. of measured, independent and observed [I > 2σ(I)] reflections 16855, 7535, 6299
Rint 0.030
(sin θ/λ)max−1) 0.837
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.047, 0.107, 1.04
No. of reflections 7535
No. of parameters 182
No. of restraints 1
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 1.11, −2.00
Absolute structure Ad
Absolute structure parameter 0.06 (4)
Computer programs: APEX2 and SAINT (Bruker, 2014[Bruker (2014). APEX2 and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.]), OLEX2.solve (Bourhis et al., 2015[Bourhis, L. J., Dolomanov, O. V., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2015). Acta Cryst. A71, 59-75.]), SHELXL2019/3 (Sheldrick, 2015[Sheldrick, G. M. (2015). Acta Cryst. C71, 3-8.]) and OLEX2 (Dolomanov et al., 2009[Dolomanov, O. V., Bourhis, L. J., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2009). J. Appl. Cryst. 42, 339-341.]).

Structural data


Computing details top

4,4'-Bipyridine-1,1'-diium tetrachloridodifluoridostannate(IV) monohydrate top
Crystal data top
(C10H10N2)[SnCl4F2]·H2ODx = 1.973 Mg m3
Mr = 474.71Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, Pna21Cell parameters from 6299 reflections
a = 7.5641 (2) Åθ = 1.5–36.5°
b = 26.5989 (5) ŵ = 2.28 mm1
c = 7.9422 (2) ÅT = 293 K
V = 1597.94 (7) Å3Prism, colourless
Z = 40.08 × 0.08 × 0.07 mm
F(000) = 920
Data collection top
Bruker SMART APEXII area detector
diffractometer
6299 reflections with I > 2σ(I)
ω and φ scansRint = 0.030
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
θmax = 36.5°, θmin = 1.5°
Tmin = 0.852, Tmax = 0.852h = 1112
16855 measured reflectionsk = 4420
7535 independent reflectionsl = 1313
Refinement top
Refinement on F2Hydrogen site location: mixed
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.047 w = 1/[σ2(Fo2) + (0.0043P)2 + 2.4611P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.107(Δ/σ)max = 0.003
S = 1.04Δρmax = 1.11 e Å3
7535 reflectionsΔρmin = 2.00 e Å3
182 parametersAbsolute structure: ad
1 restraintAbsolute structure parameter: 0.06 (4)
Primary atom site location: dual
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.

Refinement. Refined as a 2-component inversion twin. Hydrogen atoms on the aromatic rings were geometrically positioned and refined as riding atoms with Uiso(H) = 1.2Ueq(C).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
N10.5711 (7)0.22347 (18)0.5432 (7)0.0394 (10)
H10.5673630.1927340.5101670.047*
N20.6786 (8)0.4709 (2)0.7922 (10)0.0567 (16)
H20.6975430.5015020.8228410.068*
C10.5305 (8)0.2597 (2)0.4340 (8)0.0389 (11)
H1A0.4954690.2515270.3251480.047*
C20.5406 (8)0.3090 (2)0.4830 (7)0.0355 (10)
H2A0.5119690.3344010.4072060.043*
C30.5935 (6)0.32135 (16)0.6459 (10)0.0321 (10)
C40.6285 (8)0.2819 (2)0.7580 (8)0.0383 (11)
H40.6594050.2887400.8689820.046*
C50.6171 (9)0.2333 (2)0.7030 (8)0.0437 (13)
H50.6411720.2069370.7766000.052*
C60.6192 (7)0.37422 (19)0.6967 (7)0.0337 (11)
C70.6957 (9)0.4080 (2)0.5833 (9)0.0449 (13)
H70.7246990.3981890.4743670.054*
C80.7270 (10)0.4569 (2)0.6390 (15)0.061 (2)
H80.7823810.4798120.5680100.073*
C90.6021 (9)0.4396 (3)0.9022 (11)0.0561 (19)
H90.5695900.4510081.0085520.067*
C100.5717 (9)0.3902 (2)0.8562 (10)0.0440 (13)
H100.5199590.3678920.9317870.053*
Sn10.90313 (4)0.61887 (2)0.66064 (6)0.03161 (8)
Cl11.0622 (3)0.54461 (7)0.7330 (3)0.0588 (5)
Cl21.16953 (18)0.66810 (5)0.6621 (3)0.0487 (3)
Cl30.7297 (2)0.69369 (5)0.6093 (2)0.0436 (3)
Cl40.9182 (3)0.60193 (8)0.3643 (2)0.0545 (4)
F10.6661 (6)0.57916 (12)0.6921 (6)0.0594 (12)
F20.8830 (6)0.63386 (14)0.9106 (5)0.0449 (8)
O1W0.2936 (11)0.4547 (3)0.5435 (9)0.081 (2)
H1WA0.2597040.4783050.6083290.122*
H1WB0.2509340.4269750.5774990.122*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.045 (3)0.028 (2)0.045 (3)0.0004 (17)0.001 (2)0.0094 (18)
N20.052 (3)0.037 (3)0.081 (5)0.008 (2)0.002 (3)0.024 (3)
C10.044 (3)0.037 (3)0.036 (3)0.001 (2)0.002 (2)0.009 (2)
C20.040 (2)0.034 (2)0.032 (2)0.001 (2)0.005 (2)0.0021 (19)
C30.0323 (17)0.0280 (16)0.036 (3)0.0013 (14)0.005 (2)0.005 (2)
C40.046 (3)0.035 (2)0.034 (3)0.001 (2)0.005 (2)0.001 (2)
C50.055 (3)0.033 (2)0.043 (4)0.001 (2)0.001 (2)0.003 (2)
C60.033 (2)0.031 (2)0.037 (3)0.0004 (15)0.0019 (17)0.0056 (17)
C70.050 (3)0.033 (2)0.052 (4)0.006 (2)0.003 (3)0.005 (2)
C80.059 (4)0.039 (3)0.085 (7)0.018 (3)0.011 (4)0.003 (4)
C90.052 (4)0.049 (4)0.068 (5)0.001 (3)0.009 (3)0.028 (3)
C100.047 (3)0.037 (3)0.049 (3)0.004 (2)0.001 (3)0.013 (2)
Sn10.03949 (14)0.02310 (11)0.03226 (13)0.00219 (10)0.00508 (19)0.00433 (15)
Cl10.0618 (10)0.0384 (7)0.0760 (12)0.0042 (7)0.0140 (8)0.0060 (7)
Cl20.0445 (6)0.0452 (6)0.0565 (8)0.0130 (5)0.0003 (10)0.0090 (10)
Cl30.0535 (8)0.0351 (6)0.0422 (7)0.0112 (5)0.0033 (6)0.0005 (5)
Cl40.0669 (10)0.0578 (9)0.0387 (8)0.0074 (8)0.0084 (7)0.0199 (7)
F10.095 (3)0.0278 (13)0.055 (3)0.0150 (16)0.033 (2)0.0077 (15)
F20.071 (2)0.0327 (15)0.0306 (16)0.0019 (16)0.0021 (16)0.0019 (13)
O1W0.102 (5)0.074 (4)0.067 (4)0.022 (4)0.009 (4)0.025 (3)
Geometric parameters (Å, º) top
N1—H10.8593C6—C101.384 (9)
N1—C11.332 (8)C7—H70.9300
N1—C51.341 (9)C7—C81.394 (9)
N2—H20.8611C8—H80.9300
N2—C81.325 (13)C9—H90.9300
N2—C91.338 (12)C9—C101.385 (9)
C1—H1A0.9300C10—H100.9300
C1—C21.372 (8)Sn1—Cl12.3831 (18)
C2—H2A0.9300Sn1—Cl22.4032 (12)
C2—C31.393 (9)Sn1—Cl32.4183 (14)
C3—C41.401 (8)Sn1—Cl42.3994 (17)
C3—C61.476 (7)Sn1—F12.096 (4)
C4—H40.9300Sn1—F22.030 (4)
C4—C51.368 (9)O1W—H1WA0.8512
C5—H50.9300O1W—H1WB0.8498
C6—C71.397 (9)
C1—N1—H1118.8C8—C7—H7121.1
C1—N1—C5122.4 (5)N2—C8—C7120.5 (7)
C5—N1—H1118.8N2—C8—H8119.8
C8—N2—H2118.7C7—C8—H8119.8
C8—N2—C9123.0 (6)N2—C9—H9120.3
C9—N2—H2118.3N2—C9—C10119.3 (7)
N1—C1—H1A120.2C10—C9—H9120.3
N1—C1—C2119.6 (5)C6—C10—C9119.3 (7)
C2—C1—H1A120.2C6—C10—H10120.3
C1—C2—H2A119.8C9—C10—H10120.3
C1—C2—C3120.3 (5)Cl1—Sn1—Cl291.56 (6)
C3—C2—H2A119.8Cl1—Sn1—Cl3175.29 (7)
C2—C3—C4117.9 (5)Cl1—Sn1—Cl493.27 (7)
C2—C3—C6121.0 (5)Cl2—Sn1—Cl390.42 (5)
C4—C3—C6121.0 (6)Cl4—Sn1—Cl293.84 (8)
C3—C4—H4120.2Cl4—Sn1—Cl390.87 (6)
C5—C4—C3119.6 (6)F1—Sn1—Cl189.16 (12)
C5—C4—H4120.2F1—Sn1—Cl2172.46 (14)
N1—C5—C4120.1 (6)F1—Sn1—Cl388.32 (12)
N1—C5—H5119.9F1—Sn1—Cl493.60 (14)
C4—C5—H5119.9F2—Sn1—Cl187.98 (13)
C7—C6—C3119.4 (5)F2—Sn1—Cl287.21 (13)
C10—C6—C3120.5 (6)F2—Sn1—Cl387.85 (12)
C10—C6—C7120.0 (5)F2—Sn1—Cl4178.34 (13)
C6—C7—H7121.1F2—Sn1—F185.32 (17)
C8—C7—C6117.8 (7)H1WA—O1W—H1WB109.4
N1—C1—C2—C30.2 (9)C3—C6—C10—C9178.1 (6)
N2—C9—C10—C60.8 (11)C4—C3—C6—C7138.5 (6)
C1—N1—C5—C41.9 (10)C4—C3—C6—C1040.1 (8)
C1—C2—C3—C42.5 (8)C5—N1—C1—C22.1 (9)
C1—C2—C3—C6174.9 (5)C6—C3—C4—C5174.8 (5)
C2—C3—C4—C52.7 (8)C6—C7—C8—N22.7 (11)
C2—C3—C6—C738.8 (7)C7—C6—C10—C90.5 (10)
C2—C3—C6—C10142.5 (6)C8—N2—C9—C100.2 (12)
C3—C4—C5—N10.6 (9)C9—N2—C8—C71.6 (13)
C3—C6—C7—C8176.4 (6)C10—C6—C7—C82.2 (9)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···F2i0.861.792.629 (6)163
N2—H2···F10.862.322.989 (6)134
N2—H2···O1Wii0.862.112.819 (10)140
O1W—H1WA···Cl1iii0.852.513.324 (8)159
O1W—H1WB···Cl4ii0.852.723.366 (8)134
O1W—H1WB···F2iv0.852.322.906 (9)126
C1—H1A···Cl3iv0.932.823.473 (6)128
C9—H9···F1ii0.932.443.109 (9)129
Symmetry codes: (i) x+3/2, y1/2, z1/2; (ii) x+1, y+1, z+1/2; (iii) x1, y, z; (iv) x+1, y+1, z1/2.
 

Acknowledgements

Thanks are due to DRSDT-Algeria.

References

First citationBourhis, L. J., Dolomanov, O. V., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2015). Acta Cryst. A71, 59–75.  Web of Science CrossRef IUCr Journals Google Scholar
First citationBruhn, C. & Preetz, W. (1996). Acta Cryst. C52, 321–325.  CSD CrossRef CAS Web of Science IUCr Journals Google Scholar
First citationBruker (2014). APEX2 and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationDolomanov, O. V., Bourhis, L. J., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2009). J. Appl. Cryst. 42, 339–341.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationGheribi, R., Hadji, D., Ghallab, R., Medjani, M., Benslimane, M., Trifa, C., Dénès, G. & Merazig, H. (2022). J. Mol. Struct. 1248, 131392.  Web of Science CrossRef Google Scholar
First citationHoriacha, M., Nychyporuk, G., Pöttgen, R., Kaczorowski, D. & Zaremba, V. (2022). Z. Krist. 237, 281–286.  CAS Google Scholar
First citationKrause, L., Herbst-Irmer, R., Sheldrick, G. M. & Stalke, D. (2015). J. Appl. Cryst. 48, 3–10.  Web of Science CSD CrossRef ICSD CAS IUCr Journals Google Scholar
First citationSheldrick, G. M. (2015). Acta Cryst. C71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar

This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.

Journal logoIUCrDATA
ISSN: 2414-3146