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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2014 Jul 5;70(Pt 8):m291–m292. doi: 10.1107/S1600536814015189

Poly[[tri-μ-aqua-do­deca­aqua­tris­(μ3-1-hy­droxy­ethyl­idene-1,1-di­phospho­nato)tricalcium(II)tripalladium(II)] penta­hydrate]

Irina P Kutsenko a,*, Alexandra N Kozachkova a, Natalia V Tsaryk a, Vasily I Pekhnyo a, Julia A Rusanova b
PMCID: PMC4158508  PMID: 25249877

Abstract

The asymmetric unit of the title compound, {[CaPd{CH3OHC(PO3)2}(H2O)5]·5/3H2O}n, consists of one half of the complex [Pd{CH3OHC(PO3)2}]2− anion (point group symmetry m..), one Ca2+ cation [site symmetry (.2.)] that is surrounded by three water mol­ecules (one of which is on the same rotation axis) and by three disordered lattice water mol­ecules. The anions form a trinuclear metallocycle around a crystallographic threefold rotation axis. The cations are related by a twofold rotation axis to form a [Ca2(H2O)10]2+ dimer. The slightly distorted square-planar coordination environment of the PdII atoms in the complex anions is formed by O atoms of the bidentate chelating phospho­nate groups of the 1-hy­droxy­ethyl­idene-1,1-di­phospho­nate ligands. In the crystal, cations are bound to anions through —Ca—O—P—O— bonds, as well as through O—H⋯O hydrogen bonds, resulting in a three-dimensional polymer. The structure is completed by five disordered solvent mol­ecules localized in cavities within the framework.

Keywords: crystal structure

Related literature  

For background to di­phospho­nic acids see: Zhang et al. (2007); Szabo et al. (2002); Matczak-Jon & Videnova-Adrabinska (2005). For background to the anti­tumor activity of palladium(II) complexes, see: Juribašiċ et al. (2011); Curic et al. (1996); Abu-Surrah et al. (2008); Ruiz et al. (2005, 2006); Tušek-Božiċ et al. (2008). For the structures of related complexes, see: Babaryk et al. (2012); Hammerl et al. (2002); Müller (1972). graphic file with name e-70-0m291-scheme1.jpg

Experimental  

Crystal data  

  • [CaPd(C2H4O7P2)(H2O)5]·1.67H2O

  • M r = 468.58

  • Hexagonal, Inline graphic

  • a = 15.9731 (3) Å

  • c = 18.4149 (4) Å

  • V = 4068.91 (14) Å3

  • Z = 12

  • Mo Kα radiation

  • μ = 2.05 mm−1

  • T = 296 K

  • 0.39 × 0.07 × 0.06 mm

Data collection  

  • Bruker APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2009) T min = 0.502, T max = 0.887

  • 37638 measured reflections

  • 1774 independent reflections

  • 1410 reflections with I > 2σ(I)

  • R int = 0.082

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.031

  • wR(F 2) = 0.071

  • S = 1.08

  • 1774 reflections

  • 116 parameters

  • 28 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.56 e Å−3

  • Δρmin = −0.57 e Å−3

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S1600536814015189/br2239sup1.cif

e-70-0m291-sup1.cif (21.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814015189/br2239Isup2.hkl

e-70-0m291-Isup2.hkl (87.6KB, hkl)

CCDC reference: 1010912

Additional supporting information: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O5—H1⋯O1i 0.84 (1) 1.95 (2) 2.756 (3) 160 (4)
O5—H2⋯O5ii 0.79 (2) 2.07 (2) 2.799 (5) 155 (4)
O6—H3⋯O2iii 0.82 (2) 1.87 (2) 2.685 (3) 170 (4)
O7—H4⋯O3i 0.82 (2) 2.07 (2) 2.865 (4) 166 (4)
O4A—H4A⋯O8 0.82 1.99 2.731 (16) 150

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic.

supplementary crystallographic information

S1. Comment

During the last decade, there has been a growing interest in the study of organic diphosphonic acids owing to their potentially very powerful chelating properties used in metal extractions and are tested by the pharmaceutical industry for use as efficient drugs preventing calcification and inhibiting bone resorption (Matczak-Jon & Videnova-Adrabinska, 2005). Diphosphonic acids and their metal complexes are used in the treatment of Pagets disease, osteoporosis and tumoral osteolysis (Szabo et al., 2002). Also in the last years, there has been a surge of interest in palladium complexes as a prospective antitumor preparation (Abu-Surrah et al., 2008, Curic et al., 1996).

The title compound crystallized in centric space group P6/mcc. The square-planar environment of palladium atoms in the complex anion [Pd3{CH3OHC(PO3)2}3]6-is formed by coordination of the oxygen atoms of the chelating phosphonic groups of the ligand. By crystallographic threefold rotation axis it completed to trinuclear species with equilateral triangle geometry (Fig.1). Palladium atoms slightly deviate from the oxygen mean-planes towards the triangle center by 0.12 Å. The range of Pd – O bond distances of 2,006 (2) – 2,010 (2)Å as well cis O–Pd–O angles ranging from 85.78 (9)° to 92.91 (13)° are in a good agreement with literature values (Babaryk et al., 2012 and references therein). CH3 and OH groups of the HEDP are statistically disordered over two positions with equal occupation numbers.

As it shown on Fig. 2, each Ca atom of the complex binuclear cation is surrounded by eight oxygen atoms (six from water molecules, comprising two bridging ones, and two from phosphonic groups of the trinuclear clusters) in the form of a slightly distorted, bi-capped trigonal prism. (Hammerl et al., 2002). The Ca – O bond distances were observed within the range of 2,416 (3) – 2,538 (3)Å. Calcium coordinated by eight water molecules is well known in the literature, and the distances of the bridging and nonbridging oxygen atoms found here agree well with the previously reported values (Müller et al., 1972). Each binuclear cation linked to four trinuclear anions of adjacent layers through -Ca-O-P-O- bonds (Fig. 3) as well thought O-H···O hydrogen bonds. Moreover, each trinuclear anion is linked to six binuclear cations. In the crystal packing cations and anions stacked along the c axis into columns where layer of cations alternates with layer of anions. Resulting layered 3d polymer structure (Fig.4) completed by five disordered solvent water molecules which are located in cavities. The Ca – O and P-O bond distances (2.507 (2)Å and 1.498 (2)Å respectively) as well as D···A distances ranging from 2.756 (3)Å to 2.865 (4)Å are in a good agreement with literature values. Oxygen atom of one of the water solvent molecules O8 is statistically disordered over two positions and linked to cation thought CH3-C-OH···O8 hydrogen bonds with D···A distance about 2.731 (16) Å. Another one water molecule oxygen atom O9 is situated at the origin (0, 0, 0) with 1/12 multiplicity. Remaining 3 oxygen atoms O10 of the water molecules are disordered around 6-fold rotation axis with centre of symmetry over 12 positions with an occupation number of 1/4. Considering this reasonable H-atom positions of the disordered solvent water molecules were not established

S2. Experimental

A solution of AgNO3 (0.3398 g, 2.0 mmol) in H2O (5 ml) was added to a solution of PdCl2 (0.0885 g, 0.5 mmol) in hydrochloric acid (0.1M, 10 ml) and the resulting solution stirred at 276 K for 30 min under protection from light until AgCl was precipitated and filtered off. Hydroxyethylidenediphosphonic acid (0.112 g, 0.5 mmol) and CaCO3 (0.05 g, 0.5 mmol) were added to filtrate. The resulting solution was stirred for 1 h at 276 - 277 K and left staying overnight at room temperature. The solvent was removed from resulting reaction mixture under reduced pressure leaving an yellow solid, which was washed twice with methanol and diethyl ether and dried under vacuum. Yellow rectangular crystals of the title compound suitable for crystallographic study were produced by slow evaporation of a water solution at room temperature.

S3. Refinement

The structure was solved by the direct method. H atoms of methyl groups were placed at calculated positions and treated as riding on the parent atoms, with Uiso(H) = 1.5 Ueq(C). H atoms near of the O4A and O4B atoms, and H atoms of water molecule were located in a difference Fourier map and further refined with SADI instruction to the restraint that they should be equal within about 0.02 Å and Uiso(H) = 1.5Ueq(O). The OH and CH3 groups near C(1) carbon atom are disordered over two position with occupancy factor 0.25 and 0.25 respectively. Oxygen atoms of the water solvent molecules O8, O9, O10 were refined isotropically- O8 is statistically disordered with occupancy 1/2 and it position depends on the disorder of the above mentioned OH group; O9 is situated at the origin (0, 0, 0) with 1/12 multiplicity; three oxygen atoms O10 are disordered around 6-fold rotation axis with centre of symmetry over 12 positions with an occupation number of 1/4. Considering this reasonable H-atom positions of the disordered solvent water molecules were not established.

Figures

Fig. 1.

Fig. 1.

View of the anionic part of [Pd3{O3PC(OH)(CH3)PO3}3]6- unit showing 50% probability displacement ellipsoids for the non-hydrogen atoms.

Fig. 2.

Fig. 2.

View of the cationic part of [(4H2O)O2Ca(2H2O)CaO2(4H2O)]2+ fragments showing 50% probability displacement ellipsoids for the non-hydrogen atoms.

Fig. 3.

Fig. 3.

Linking of cations to anions of adjacent layers in crystal packing.

Fig. 4.

Fig. 4.

Crystal packing of title compound, in a projection along the c axis. Solvate molecules as well as hydrogen bonds are omitted for clarity.

Crystal data

[CaPd(C2H4O7P2)(H2O)5]·1.67H2O F(000) = 2816
Mr = 468.58 Dx = 2.295 Mg m3
Hexagonal, P6/mcc Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 6 2c µ = 2.05 mm1
a = 15.9731 (3) Å T = 296 K
c = 18.4149 (4) Å Rectangular, yellow
V = 4068.91 (14) Å3 0.39 × 0.07 × 0.06 mm
Z = 12

Data collection

Bruker APEXII CCD area-detector diffractometer 1774 independent reflections
Radiation source: fine-focus sealed tube 1410 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.082
phi and ω scans θmax = 28.4°, θmin = 2.6°
Absorption correction: multi-scan (SADABS; Sheldrick, 2009) h = −21→21
Tmin = 0.502, Tmax = 0.887 k = −21→18
37638 measured reflections l = −22→24

Refinement

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)] = 0.031 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.071 H atoms treated by a mixture of independent and constrained refinement
S = 1.08 w = 1/[σ2(Fo2) + (0.0249P)2 + 11.4857P] where P = (Fo2 + 2Fc2)/3
1774 reflections (Δ/σ)max = 0.013
116 parameters Δρmax = 0.56 e Å3
28 restraints Δρmin = −0.57 e Å3

Special details

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq Occ. (<1)
Pd1 0.63688 (3) 0.44960 (3) 0.0000 0.01659 (11)
Ca1 0.37002 (6) 0.37002 (6) 0.2500 0.0182 (2)
P1 0.45030 (6) 0.28992 (6) 0.08236 (4) 0.01779 (18)
O1 0.48149 (18) 0.21370 (18) 0.08028 (12) 0.0246 (5)
O2 0.53726 (17) 0.39316 (17) 0.07897 (12) 0.0223 (5)
O3 0.38931 (18) 0.27739 (18) 0.14777 (12) 0.0218 (5)
O5 0.33373 (19) 0.50409 (19) 0.22123 (13) 0.0243 (5)
H1 0.327 (3) 0.507 (3) 0.1764 (6) 0.037*
H2 0.367 (2) 0.5554 (18) 0.2384 (19) 0.037*
O6 0.5000 0.5000 0.17187 (18) 0.0221 (7)
H3 0.484 (3) 0.526 (3) 0.1407 (15) 0.033*
O7 0.2157 (2) 0.2933 (2) 0.18857 (17) 0.0395 (7)
H4 0.182 (3) 0.318 (3) 0.184 (2) 0.059*
H5 0.238 (3) 0.291 (4) 0.1493 (16) 0.059*
C1 0.3787 (3) 0.2740 (3) 0.0000 0.0224 (10)
O4A 0.2883 (5) 0.1836 (5) 0.0000 0.0311 (19)* 0.50
H4A 0.253 (4) 0.185 (4) −0.031 (6) 0.047* 0.25
C2A 0.3627 (7) 0.3633 (5) 0.0000 0.023 (2)* 0.50
H21 0.3251 0.3600 −0.0416 0.034* 0.25
H22 0.4242 0.4218 −0.0018 0.034* 0.50
H23 0.3291 0.3626 0.0434 0.034* 0.25
C2B 0.3085 (7) 0.1626 (5) 0.0000 0.019 (2)* 0.50
H24 0.2910 0.1403 0.0491 0.029* 0.25
H25 0.3399 0.1310 −0.0219 0.029* 0.25
H26 0.2515 0.1478 −0.0271 0.029* 0.25
O4B 0.3386 (6) 0.3370 (6) 0.0000 0.029* 0.50
H4B 0.298 (7) 0.321 (6) −0.033 (5) 0.029* 0.25
O8 0.1458 (11) 0.1163 (12) −0.1026 (9) 0.169 (6)* 0.50
O9 0.0000 0.0000 0.0000 0.40 (3)*
O10 0.108 (2) 0.079 (3) −0.2084 (13) 0.184 (14)* 0.25

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Pd1 0.01985 (19) 0.0223 (2) 0.00785 (16) 0.01075 (16) 0.000 0.000
Ca1 0.0199 (3) 0.0199 (3) 0.0176 (4) 0.0119 (4) −0.00021 (18) 0.00021 (18)
P1 0.0220 (4) 0.0215 (4) 0.0089 (4) 0.0101 (4) 0.0018 (3) −0.0004 (3)
O1 0.0386 (15) 0.0328 (14) 0.0105 (11) 0.0240 (12) 0.0048 (10) 0.0016 (10)
O2 0.0237 (12) 0.0255 (12) 0.0119 (11) 0.0080 (10) 0.0043 (10) −0.0021 (9)
O3 0.0261 (13) 0.0265 (13) 0.0106 (11) 0.0116 (11) 0.0045 (9) −0.0005 (10)
O5 0.0261 (14) 0.0318 (14) 0.0165 (12) 0.0155 (12) −0.0011 (10) 0.0024 (10)
O6 0.0280 (19) 0.0228 (18) 0.0194 (17) 0.0156 (15) 0.000 0.000
O7 0.0380 (17) 0.0476 (18) 0.0439 (18) 0.0297 (15) −0.0130 (14) −0.0102 (15)
C1 0.021 (2) 0.025 (3) 0.016 (2) 0.007 (2) 0.000 0.000

Geometric parameters (Å, º)

Pd1—O2i 2.006 (2) Ca1—O5iv 2.538 (3)
Pd1—O2 2.006 (2) Ca1—Ca1vi 4.1524 (18)
Pd1—O1ii 2.010 (2) P1—O3 1.498 (2)
Pd1—O1iii 2.010 (2) P1—O1 1.529 (2)
Ca1—O7 2.416 (3) P1—O2 1.537 (2)
Ca1—O7iv 2.416 (3) P1—C1 1.839 (3)
Ca1—O3 2.507 (2) C1—O4B 1.438 (6)
Ca1—O3iv 2.507 (2) C1—O4A 1.444 (6)
Ca1—O6v 2.526 (2) C1—C2B 1.559 (6)
Ca1—O6 2.526 (2) C1—C2A 1.569 (6)
Ca1—O5 2.538 (3) C1—P1i 1.839 (3)
O2i—Pd1—O2 92.91 (13) O6v—Ca1—O5iv 68.18 (6)
O2i—Pd1—O1ii 85.78 (9) O6—Ca1—O5iv 82.30 (7)
O2—Pd1—O1ii 173.09 (10) O5—Ca1—O5iv 144.16 (13)
O2i—Pd1—O1iii 173.09 (10) O7—Ca1—Ca1vi 139.79 (8)
O2—Pd1—O1iii 85.78 (9) O7iv—Ca1—Ca1vi 139.79 (8)
O1ii—Pd1—O1iii 94.70 (14) O3—Ca1—Ca1vi 103.51 (6)
O7—Ca1—O7iv 80.42 (16) O3iv—Ca1—Ca1vi 103.51 (6)
O7—Ca1—O3 75.19 (9) O3—P1—O1 111.26 (14)
O7iv—Ca1—O3 84.19 (10) O3—P1—O2 110.76 (13)
O7—Ca1—O3iv 84.19 (10) O1—P1—O2 111.95 (14)
O7iv—Ca1—O3iv 75.19 (9) O3—P1—C1 109.08 (15)
O3—Ca1—O3iv 152.97 (12) O1—P1—C1 107.27 (16)
O7—Ca1—O6v 153.43 (7) O2—P1—C1 106.30 (16)
O7iv—Ca1—O6v 111.16 (10) P1—O1—Pd1vii 128.04 (14)
O3—Ca1—O6v 128.30 (7) P1—O2—Pd1 126.86 (14)
O3iv—Ca1—O6v 76.37 (7) P1—O3—Ca1 142.04 (15)
O7—Ca1—O6 111.16 (10) Ca1vi—O6—Ca1 110.56 (13)
O7iv—Ca1—O6 153.43 (7) O4B—C1—O4A 97.3 (6)
O3—Ca1—O6 76.37 (7) O4B—C1—C2B 118.7 (6)
O3iv—Ca1—O6 128.30 (7) O4A—C1—C2A 111.9 (6)
O6v—Ca1—O6 69.44 (13) C2B—C1—C2A 133.4 (6)
O7—Ca1—O5 74.02 (9) O4B—C1—P1i 111.5 (2)
O7iv—Ca1—O5 138.18 (9) O4A—C1—P1i 112.3 (2)
O3—Ca1—O5 119.24 (8) C2B—C1—P1i 101.6 (3)
O3iv—Ca1—O5 69.84 (8) C2A—C1—P1i 104.3 (2)
O6v—Ca1—O5 82.30 (7) O4B—C1—P1 111.5 (2)
O6—Ca1—O5 68.18 (6) O4A—C1—P1 112.3 (2)
O7—Ca1—O5iv 138.18 (9) C2B—C1—P1 101.6 (3)
O7iv—Ca1—O5iv 74.02 (9) C2A—C1—P1 104.3 (2)
O3—Ca1—O5iv 69.84 (8) P1i—C1—P1 111.1 (2)
O3iv—Ca1—O5iv 119.24 (8)

Symmetry codes: (i) x, y, −z; (ii) −x+y+1, −x+1, −z; (iii) −x+y+1, −x+1, z; (iv) y, x, −z+1/2; (v) −y+1, −x+1, −z+1/2; (vi) −x+1, −y+1, z; (vii) −y+1, xy, z.

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
O5—H1···O1viii 0.84 (1) 1.95 (2) 2.756 (3) 160 (4)
O5—H2···O5v 0.79 (2) 2.07 (2) 2.799 (5) 155 (4)
O6—H3···O2vi 0.82 (2) 1.87 (2) 2.685 (3) 170 (4)
O7—H4···O3viii 0.82 (2) 2.07 (2) 2.865 (4) 166 (4)
O4A—H4A···O8 0.82 1.99 2.731 (16) 150

Symmetry codes: (v) −y+1, −x+1, −z+1/2; (vi) −x+1, −y+1, z; (viii) xy, x, z.

Footnotes

Supporting information for this paper is available from the IUCr electronic archives (Reference: BR2239).

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S1600536814015189/br2239sup1.cif

e-70-0m291-sup1.cif (21.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814015189/br2239Isup2.hkl

e-70-0m291-Isup2.hkl (87.6KB, hkl)

CCDC reference: 1010912

Additional supporting information: crystallographic information; 3D view; checkCIF report


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