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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jun 11;67(Pt 7):i40. doi: 10.1107/S1600536811021167

Disilver(I) trinickel(II) hydrogenphos­phate bis­(phosphate), Ag2Ni3(HPO4)(PO4)2

Abderrazzak Assani a,*, Lahcen El Ammari a, Mohammed Zriouil a, Mohamed Saadi a
PMCID: PMC3151764  PMID: 21836825

Abstract

The title compound, Ag2Ni3(HPO4)(PO4)2, has been synthesized by the hydro­thermal method. Its structure is formed by two types of chains running along the b axis. The first chain results from a linear and continuous succession of NiO6 octa­hedra linked to PO4 tetra­hedra by a common vertex. The second chain is built up from two adjacent edge-sharing octa­hedra (dimers) whose ends are linked to two PO4 tetra­hedra by a common edge. Those two types of chains are linked together by the phosphate groups to form polyhedral sheets parallel to the (001) plane. The three-dimensional framework delimits two types of hexa­gonal tunnels parallel to the a-axis direction, at (x, 1/2, 0) and (x, 0, 1/2), where the Ag atoms are located. Each silver cation is surrounded by eight O atoms. The same Ag+ coordination is found in other phosphates with the alluaudite structure, for example, AgMn3(PO4)(HPO4)2. Moreover, O—H⋯O hydrogen bonds link three PO4 tetra­hedra so as to build a three-dimensional network.

Related literature

For related applications, see: Viter & Nagornyi (2009); Gao & Gao (2005); Clearfield (1988); Trad et al. (2010). For compounds with the same structure, see: Assani et al. (2010, 2011); Leroux et al. (1995); Ben Smail & Jouini (2002).

Experimental

Crystal data

  • Ag2Ni3(HPO4)(PO4)2

  • M r = 677.79

  • Orthorhombic, Inline graphic

  • a = 12.9233 (3) Å

  • b = 6.5678 (2) Å

  • c = 10.6629 (3) Å

  • V = 905.04 (4) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 10.98 mm−1

  • T = 296 K

  • 0.25 × 0.13 × 0.08 mm

Data collection

  • Bruker X8 APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (MULABS; Blessing, 1995) T min = 0.382, T max = 0.471

  • 3762 measured reflections

  • 1125 independent reflections

  • 1103 reflections with I > 2σ(I)

  • R int = 0.017

Refinement

  • R[F 2 > 2σ(F 2)] = 0.024

  • wR(F 2) = 0.060

  • S = 1.06

  • 1125 reflections

  • 99 parameters

  • 1 restraint

  • H-atom parameters constrained

  • Δρmax = 1.81 e Å−3

  • Δρmin = −1.12 e Å−3

  • Absolute structure: Flack (1983), 467 Friedel pairs

  • Flack parameter: 0.55 (3)

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT; data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997) and DIAMOND (Brandenburg, 2006); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811021167/ru2005sup1.cif

e-67-00i40-sup1.cif (21.5KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811021167/ru2005Isup2.hkl

e-67-00i40-Isup2.hkl (55.8KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

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

D—H⋯A D—H H⋯A DA D—H⋯A
O7—H7⋯O6i 0.86 2.06 2.847 (6) 151

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors thank the Unit of Support for Technical and Scientific Research (UATRS, CNRST) for the X-ray measurements.

supplementary crystallographic information

Comment

As the improvement has arisen in the synthesis of a variety of interesting porous materials and open-framework structures, extensive studies are devoted to the metal phosphates which exhibit a rich structural diversity and have been widely studied as catalysts (Viter & Nagornyi, 2009; Gao & Gao, 2005), ion-exchangers (Clearfield, 1988) and as positive electrode in the lithium and sodium batteries (Trad et al. (2010)).

Within this family of compounds, the resulting anionic frameworks, generally constructed from the alternation of PO4 tetrahedra connected to metal cations in different coordinate geometry MOn (with n=4, 5 and 6), generate pores and channels offering suitable environment to accommodate different other cations. In our search for new phosphates with microporous framework, our most attention has been paid to the hydrothermal investigation of the A2O—MO—P2O5 systems, with A = monovalent cations and M = divalent cations. Accordingly, we have succeed, for instance, to isolate new form of silver zinc phosphate (γ-AgZnPO4) related to the ABW zeolite structure (Assani et al. 2010) while the silver magnesium phosphate, namely AgMg3(PO4)(HPO4)2, represent a new member of the well known alluaudite-like structure family (Assani et al. 2011). The present paper aims to develop the hydrothermal synthesis and the structural characterization of a new silver nickel phosphate, namely, Ag2Ni3(HPO4)(PO4)2.

The structure of this compound is formed by two types of chains running along the b axis. The first chain (Ni2P2HO9)∞ is built up from Ni2 and P2 atoms in special Wyckoff position 4 b (m) of the space group Ima2. This chain results from linear and continuous succession of octahedron (Ni2O6) and P2O3OH tetrahedron which share a vertex. The second chain (Ni2P2O14)n is built up from two adjacent edge sharing octahedra ((Ni1)2O10 dimmers) whose ends are linked to two P1O4 tetrahedra by a common edge (Fig.1). Those chains are linked together by the phosphate groups to form polyhedral sheets parallel to the (0 0 1) plane as shown in Fig.2.

The three dimensional framework delimits two types of hexagonal tunnels running along the a direction, at x 1/2 0 and x 0 1/2 (Fig.3). The Ag2 atom is located at centre of tunnels, this explains the high value of its anisotropic displacement U11, whereas Ag1 is slightly shifted from this center (Wyckoff positions: Ag2 at 2a: 0, 0, z and Ag1 at 2 b: 1/4, y, z). However, each Ag+ ion is surrounded by 8 O atoms with different Ag–O distances. Indeed, the first coordination environment of Ag2+ is almost square planar with four short Ag2—O distances between 2.373 (4) and 2.421 (4) Å and the other four larger distances are in the range of 2.869 (4) to 3.133 (4) Å. A similar coordination surrounding Ag1+ is observed with Ag1—O bond lengths in the range of 2.537 (4)–2.616 (4) Å and the longest bonds are situated between 2.661 (4) and 2.963 (4) Å. The same coordination for this cation is found in other phosphate with alluaudite structure like AgMn3(PO4)(HPO4)2 (Leroux et al. (1995)) and AgNi3(PO4)(HPO4)2 (Ben Smail & Jouini (2002)).

Moreover, O—H···O hydrogen bondings link two adjacent P2O4 tetrahedra via a strong hydrogen bond O7–H7···O6 to two P1O4 tetrahedra through weak bonds O7–H7···O4 in the way to build an infinite three-dimensional network as shown in Table 1.

Experimental

By means of hydrothermal synthesis, we have isolate a new silver nickel phosphate from the reaction mixture of silver nitrate (AgNO3; 0.1699 g), metallic nickel (Ni; 0.0881 g), 85%wt phosphoric acid (H3PO4; 0,10 ml) and water (12 ml). The hydrothermal treatment was conducted in a 23 ml Teflon-lined autoclave under autogeneous pressure at 468 K for two days. After being filtered off, washed with deionized water and air dried, the reaction product consists of a monophasic green powder and some green parallelepipedic crystals corresponding to the title compound.

Refinement

The structure is solved by direct method technique and refined by full-matrix least-squares using SHELXS97 and SHELXL97 program packages. The structure refinement in the centrosymmetric space group was unsuccessful. Infact the crystal is a racemic twinned with a refined ratio of 0.479 (26), which explains the ambiguity in the Flack parameter. The space group is not centro symmetric and the polar axis restraint is generated automatically by SHELXL program. Friedel opposites reflections are not merged. The O-bound H atom is initially located unambiguously in a difference map and refined with O—H distance restraints of 0.86 (1). In a the last cycle ther is refined in the riding model approximation with Uiso(H) set to 1.2Ueq(O). The highest and deepest hole residual peak in the final difference Fourier map are located at 0.72 Å and 0.62 Å, from Ag1.

Figures

Fig. 1.

Fig. 1.

Partial plot of Ag2Ni3(HPO4)(PO4)2 crystal structure. Displacement ellipsoids are drawn at the 50% probability level. Symmetry codes: (i) -x, -y + 1, z; (ii) x + 1/2, -y + 1, z; (iii) x, -y + 3/2, z - 1/2; (iv) -x + 1/2, -y + 3/2, z - 1/2; (v) -x + 1/2, -y + 1/2, z - 1/2; (vi) -x, y + 1/2, z - 1/2; (vii) x + 1/2, y + 1/2, z - 1/2; (viii) x, -y + 1/2, z - 1/2; (ix) -x, -y, z; (x) -x, y + 1/2, z + 1/2; (xi) x, -y + 1/2, z + 1/2; (xii) -x + 1/2, y, z.

Fig. 2.

Fig. 2.

View along the b axis of polyhedral sheets parallel to the (0 0 1) plane.

Fig. 3.

Fig. 3.

A three-dimensional polyhedral view of the crystal structure of the Ag2Ni3(HPO4)(PO4)2, showing tunnels running along the a direction, at x, 1/2, 0 and x, 0, 1/2.

Crystal data

Ag2Ni3(HPO4)(PO4)2 F(000) = 1280
Mr = 677.79 Dx = 4.974 Mg m3
Orthorhombic, Ima2 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: I 2 -2a Cell parameters from 1125 reflections
a = 12.9233 (3) Å θ = 3.2–29.0°
b = 6.5678 (2) Å µ = 10.98 mm1
c = 10.6629 (3) Å T = 296 K
V = 905.04 (4) Å3 Prism, green
Z = 4 0.25 × 0.13 × 0.08 mm

Data collection

Bruker X8 APEXII CCD area-detector diffractometer 1125 independent reflections
Radiation source: fine-focus sealed tube 1103 reflections with I > 2σ(I)
graphite Rint = 0.017
φ and ω scans θmax = 29.0°, θmin = 3.2°
Absorption correction: multi-scan (MULABS; Blessing, 1995) h = −13→14
Tmin = 0.382, Tmax = 0.471 k = −16→17
3762 measured reflections l = −8→8

Refinement

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)] = 0.024 H-atom parameters constrained
wR(F2) = 0.060 w = 1/[σ2(Fo2) + (0.0356P)2 + 1.7344P] where P = (Fo2 + 2Fc2)/3
S = 1.06 (Δ/σ)max < 0.001
1125 reflections Δρmax = 1.81 e Å3
99 parameters Δρmin = −1.12 e Å3
1 restraint Absolute structure: Flack (1983), 467 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.55 (3)

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
Ag1 0.2500 0.60793 (8) −0.01513 (7) 0.02914 (18)
Ag2 0.0000 0.5000 −0.03769 (5) 0.0443 (2)
Ni1 0.13623 (4) 0.24801 (10) 0.20871 (7) 0.00699 (13)
Ni2 0.0000 0.5000 0.45735 (7) 0.00462 (15)
P1 −0.07279 (7) 0.25722 (19) 0.20677 (13) 0.00587 (19)
P2 0.2500 0.4102 (2) 0.45653 (15) 0.0042 (3)
O1 −0.1343 (3) 0.4456 (5) 0.1739 (3) 0.0091 (7)
O2 0.0044 (3) 0.2070 (6) 0.1000 (3) 0.0056 (6)
O3 0.0036 (3) 0.2785 (5) 0.3204 (3) 0.0072 (8)
O4 −0.1494 (3) 0.0786 (5) 0.2360 (3) 0.0096 (9)
O5 0.1543 (2) 0.5443 (4) 0.4552 (3) 0.0085 (5)
O6 0.2500 0.2617 (8) 0.3420 (5) 0.0090 (12)
O7 0.2500 0.2692 (7) 0.5756 (5) 0.0064 (12)
H7 0.2500 0.3065 0.6529 0.008*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Ag1 0.0491 (4) 0.0158 (3) 0.0225 (3) 0.000 0.000 0.0048 (3)
Ag2 0.1145 (7) 0.0083 (2) 0.0101 (3) −0.0020 (3) 0.000 0.000
Ni1 0.0058 (2) 0.0092 (3) 0.0060 (3) 0.0005 (2) 0.0005 (3) −0.00135 (19)
Ni2 0.0052 (3) 0.0049 (3) 0.0037 (3) 0.0006 (2) 0.000 0.000
P1 0.0064 (4) 0.0064 (5) 0.0047 (4) −0.0001 (5) 0.0008 (6) 0.0004 (4)
P2 0.0043 (6) 0.0054 (6) 0.0030 (7) 0.000 0.000 −0.0012 (6)
O1 0.0086 (16) 0.0100 (18) 0.0088 (15) 0.0003 (14) −0.0017 (10) −0.0010 (12)
O2 0.0044 (18) 0.0088 (15) 0.0035 (15) −0.0002 (15) −0.0010 (12) −0.0029 (13)
O3 0.012 (2) 0.0044 (17) 0.0049 (15) 0.0009 (15) −0.0005 (12) −0.0010 (12)
O4 0.010 (2) 0.0023 (18) 0.016 (2) −0.0011 (13) 0.0015 (11) 0.0017 (11)
O5 0.0077 (12) 0.0082 (12) 0.0096 (15) 0.0014 (10) −0.0008 (13) −0.0003 (12)
O6 0.005 (3) 0.013 (3) 0.009 (2) 0.000 0.000 −0.0007 (16)
O7 0.007 (3) 0.007 (3) 0.005 (2) 0.000 0.000 0.0023 (16)

Geometric parameters (Å, °)

Ag1—O1i 2.534 (3) Ni2—O2xi 2.041 (3)
Ag1—O1ii 2.535 (3) Ni2—O3i 2.062 (4)
Ag1—O5iii 2.617 (3) Ni2—O3 2.062 (4)
Ag1—O5iv 2.617 (3) P1—O1 1.511 (4)
Ag1—O7v 2.659 (5) P1—O2 1.549 (4)
Ag1—O6v 2.866 (5) P1—O4 1.566 (4)
Ag1—O4vi 2.962 (3) P1—O3 1.569 (4)
Ag1—O4vii 2.962 (3) P2—O5 1.518 (3)
Ag1—Ag2 3.31641 (16) P2—O5xii 1.518 (3)
Ag2—O3vi 2.375 (4) P2—O6 1.563 (6)
Ag2—O3viii 2.375 (4) P2—O7 1.572 (5)
Ag2—O2 2.421 (4) O1—Ni1i 2.046 (4)
Ag2—O2i 2.421 (4) O1—O4 2.507 (5)
Ag2—O1 2.869 (4) O1—Ag1i 2.534 (3)
Ag2—O1i 2.869 (4) O2—Ni2xiii 2.041 (3)
Ag2—O4viii 3.133 (4) O3—Ag2xiv 2.375 (4)
Ag2—O4vi 3.133 (4) O4—Ni1ix 2.172 (4)
Ni1—O1i 2.046 (4) O4—Ag1xv 2.962 (3)
Ni1—O7v 2.047 (3) O4—Ag2xiv 3.133 (4)
Ni1—O6 2.047 (4) O5—Ag1xvi 2.617 (3)
Ni1—O2 2.079 (4) O6—Ni1xii 2.047 (4)
Ni1—O3 2.097 (4) O6—Ag1xvii 2.866 (5)
Ni1—O4ix 2.172 (4) O7—Ni1xi 2.047 (3)
Ni2—O5i 2.015 (3) O7—Ni1xvii 2.047 (3)
Ni2—O5 2.015 (3) O7—Ag1xvii 2.659 (5)
Ni2—O2x 2.041 (3) O7—H7 0.8600
O1i—Ag1—O1ii 72.33 (16) O3viii—Ag2—O4vi 67.92 (11)
O1i—Ag1—O5iii 86.46 (10) O2—Ag2—O4vi 125.71 (11)
O1ii—Ag1—O5iii 119.74 (11) O2i—Ag2—O4vi 110.51 (11)
O1i—Ag1—O5iv 119.74 (11) O1—Ag2—O4vi 177.43 (10)
O1ii—Ag1—O5iv 86.46 (10) O1i—Ag2—O4vi 102.27 (8)
O5iii—Ag1—O5iv 56.41 (12) O4viii—Ag2—O4vi 79.25 (12)
O1i—Ag1—O7v 65.26 (11) Ag1i—Ag2—Ag1 171.68 (3)
O1ii—Ag1—O7v 65.26 (11) O1i—Ni1—O7v 86.42 (17)
O5iii—Ag1—O7v 148.99 (7) O1i—Ni1—O6 95.26 (18)
O5iv—Ag1—O7v 148.99 (7) O7v—Ni1—O6 88.15 (12)
O1i—Ag1—O6v 107.78 (12) O1i—Ni1—O2 90.92 (15)
O1ii—Ag1—O6v 107.78 (12) O7v—Ni1—O2 101.25 (13)
O5iii—Ag1—O6v 132.46 (11) O6—Ni1—O2 169.08 (15)
O5iv—Ag1—O6v 132.46 (11) O1i—Ni1—O3 89.93 (14)
O7v—Ag1—O6v 53.46 (12) O7v—Ni1—O3 170.53 (14)
O1i—Ag1—O4vi 116.39 (11) O6—Ni1—O3 100.89 (14)
O1ii—Ag1—O4vi 164.32 (10) O2—Ni1—O3 70.05 (11)
O5iii—Ag1—O4vi 74.98 (10) O1i—Ni1—O4ix 175.34 (13)
O5iv—Ag1—O4vi 98.97 (10) O7v—Ni1—O4ix 88.97 (17)
O7v—Ag1—O4vi 105.40 (12) O6—Ni1—O4ix 83.92 (17)
O6v—Ag1—O4vi 57.90 (11) O2—Ni1—O4ix 90.62 (14)
O1i—Ag1—O4vii 164.32 (10) O3—Ni1—O4ix 94.73 (14)
O1ii—Ag1—O4vii 116.39 (11) O5i—Ni2—O5 178.70 (19)
O5iii—Ag1—O4vii 98.97 (10) O5i—Ni2—O2x 94.43 (14)
O5iv—Ag1—O4vii 74.98 (10) O5—Ni2—O2x 86.54 (14)
O7v—Ag1—O4vii 105.40 (12) O5i—Ni2—O2xi 86.55 (14)
O6v—Ag1—O4vii 57.90 (11) O5—Ni2—O2xi 94.42 (14)
O4vi—Ag1—O4vii 52.10 (14) O2x—Ni2—O2xi 83.6 (2)
O3vi—Ag2—O3viii 100.81 (18) O5i—Ni2—O3i 94.10 (14)
O3vi—Ag2—O2 177.72 (14) O5—Ni2—O3i 84.97 (15)
O3viii—Ag2—O2 76.92 (10) O2x—Ni2—O3i 93.29 (11)
O3vi—Ag2—O2i 76.92 (10) O2xi—Ni2—O3i 176.91 (18)
O3viii—Ag2—O2i 177.72 (14) O5i—Ni2—O3 84.97 (15)
O2—Ag2—O2i 105.35 (15) O5—Ni2—O3 94.10 (14)
O3vi—Ag2—O1 125.84 (12) O2x—Ni2—O3 176.91 (18)
O3viii—Ag2—O1 114.65 (11) O2xi—Ni2—O3 93.29 (11)
O2—Ag2—O1 55.82 (11) O3i—Ni2—O3 89.8 (2)
O2i—Ag2—O1 66.92 (11) O1—P1—O2 110.0 (2)
O3vi—Ag2—O1i 114.65 (11) O1—P1—O4 109.1 (2)
O3viii—Ag2—O1i 125.84 (12) O2—P1—O4 113.2 (2)
O2—Ag2—O1i 66.92 (11) O1—P1—O3 115.89 (19)
O2i—Ag2—O1i 55.82 (11) O2—P1—O3 100.46 (15)
O1—Ag2—O1i 76.28 (13) O4—P1—O3 108.1 (2)
O3vi—Ag2—O4viii 67.92 (11) O5—P2—O5xii 109.1 (2)
O3viii—Ag2—O4viii 52.70 (12) O5—P2—O6 110.77 (16)
O2—Ag2—O4viii 110.51 (11) O5xii—P2—O6 110.77 (16)
O2i—Ag2—O4viii 125.71 (11) O5—P2—O7 110.44 (16)
O1—Ag2—O4viii 102.27 (8) O5xii—P2—O7 110.44 (16)
O1i—Ag2—O4viii 177.43 (10) O6—P2—O7 105.3 (2)
O3vi—Ag2—O4vi 52.70 (12) P2—O7—H7 127.4

Symmetry codes: (i) −x, −y+1, z; (ii) x+1/2, −y+1, z; (iii) x, −y+3/2, z−1/2; (iv) −x+1/2, −y+3/2, z−1/2; (v) −x+1/2, −y+1/2, z−1/2; (vi) −x, y+1/2, z−1/2; (vii) x+1/2, y+1/2, z−1/2; (viii) x, −y+1/2, z−1/2; (ix) −x, −y, z; (x) −x, y+1/2, z+1/2; (xi) x, −y+1/2, z+1/2; (xii) −x+1/2, y, z; (xiii) −x, y−1/2, z−1/2; (xiv) −x, y−1/2, z+1/2; (xv) x−1/2, y−1/2, z+1/2; (xvi) −x+1/2, −y+3/2, z+1/2; (xvii) −x+1/2, −y+1/2, z+1/2.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O7—H7···O6xvii 0.86 2.06 2.847 (6) 151.

Symmetry codes: (xvii) −x+1/2, −y+1/2, z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RU2005).

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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, global. DOI: 10.1107/S1600536811021167/ru2005sup1.cif

e-67-00i40-sup1.cif (21.5KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811021167/ru2005Isup2.hkl

e-67-00i40-Isup2.hkl (55.8KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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