supplementary materials


Acta Cryst. (2009). E65, i42    [ doi:10.1107/S1600536809014652 ]

Lithium diaquanickel(II) catena-borodiphosphate(V) monohydrate

J. Zheng and A. Zhang

Abstract top

The title borophosphate LiNi(H2O)2[BP2O8]·H2O was synthesized under hydrothermal conditions. The crystal structure is isotypic with the Mg analogue and features helical [BP2O8]3- borophosphate ribbons, constructed by BO4 (2 symmetry) and PO4 tetrahedra. The borate groups share all their oxygen apices with adjacent phosphate tetrahedra. The ribbons are connected via Ni2+ cations that are located on twofold rotation axes. The cations have a slightly distorted octahedral oxygen coordination by four O atoms from the anion and by two water molecules. The voids within the helices are occupied by Li+ cations, likewise located on twofold rotation axes, in an irregular environment of five O atoms. The structure is stabilized by O-H...O hydrogen bonds between coordinated or uncoordinated water molecules and O atoms that are part of the helices.

Comment top

With increasing interest in microporous materials, the synthesis of compounds like borophosphates with open framework structures have drawn much attention during the past few years. These compounds show a rich crystal chemistry (Kniep et al., 1998; Ewald et al., 2007).

The crystal structure of LiNi(H2O)2[BP2O8].H2O is isotypic with that of the Mg analogue (Lin et al. 2008) and contains an infinite one-dimensional anionic structure. The condensation of BO4 and PO4 tetrahedra leads to helical ribbons with composition [BP2O8]3- (Fig. 1), whereby each BO4 tetrahedron shares its vertices with four PO4 tetrahedra. Bond lenghts and angles within the anionic structure are consistent with related borophosphates (Boy & Kniep, 2001; Lin et al., 2008).

The free loop of the borophosphate helix is occupied by Li+ cations, which are coordinated by with five O atoms, two from phosphate groups (O2) and three from water molecules (O3), thus completing an helical unit {Li[BP2O8]2-} with a central channel running along the 65 screw axis. The channels are filled up with water of crystallization (O6). The Ni2+ cations, located on a twofold rotation axis, are surrounded in a distorted octahedral coordination by four O atoms from adjacent phosphate groups and two water molecules, leading to the overall formula LiNi(H2O)2[BP2O8].H2O (Fig. 2). The Ni—O distances range from 2.048 (3)–2.130 (3) Å and are in the usual range. The crystal structure is stabilized by O—H···O hydrogen bonds between coordinated or uncoordinated water molecules and O atoms that are part of the helices.

Related literature top

For the isotypic Mg analogue, see: Lin et al. (2008). For other borophosphates, see: Boy & Kniep (2001); Kniep et al. (1998). A review on the structural chemistry of borphosphates is given by Ewald et al. (2007).

Experimental top

Green block-shaped crystals were synthesized hydrothermally from a mixture of Ni(NO3)2, Li2B4O7, water and H3PO4. In a typical synthesis, 0.87 g Ni(NO3)2.6H2O was dissolved in a mixture of 5 mL water, 1.691 g Li2B4O7 and 2 ml H3PO4 (85%wt ) under constant stirring. Finally, the mixture was kept in a 30 ml Teflon-lined steel autoclave at 443 K for 6d. The autoclave was slowly cooled to room temperature.

Refinement top

The highest peak in the difference map is 1.29Å from atom H6, and the minimum peak is 0.48Å from atom P2.

Computing details top

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT (Bruker, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. A part of the structure of LiNi(H2O)2[BP2O8].H2O with displacement ellipsoids drawn at the 50% the probability level. Symmetry codes: (i) 1 - y, 1 - x, 0.16667 - z; (ii) 1 - x, 1 - x + y, 0.33333 - z; (iii) x-y, x, -0.16667 + z; (iv) y, x, 0.66667 - z; (v) y, -x + y, 0.16667 + z; (vi) x, x-y, 0.83333 - z.
[Figure 2] Fig. 2. Polyhedral diagram for LiNi(H2O)2[BP2O8].H2O in projection along [001]. Colour code: purple P, orange B, blue Ni, red OW6 and green Li.
Lithium diaquanickel(II) catena-borodiphosphate(V) monohydrate top
Crystal data top
LiNi(H2O)2[BP2O8]·H2OZ = 6
Mr = 320.44F000 = 960
Hexagonal, P6522Dx = 2.686 Mg m3
Hall symbol: P 65 2 ( 0Mo Kα radiation
λ = 0.71073 Å
a = 9.3359 (3) ÅCell parameters from 1684 reflections
b = 9.3359 (3) Åθ = 2.5–29.5º
c = 15.7497 (11) ŵ = 2.91 mm1
α = 90ºT = 296 K
β = 90ºBlock, green
γ = 120º0.22 × 0.20 × 0.17 mm
V = 1188.82 (10) Å3
Data collection top
Bruker APEXII CCD area-detector
diffractometer
708 independent reflections
Radiation source: fine-focus sealed tube684 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.049
T = 296 Kθmax = 29.5º
φ and ω scansθmin = 2.5º
Absorption correction: multi-scan
(SADABS; Bruker, 2007)
h = 10→11
Tmin = 0.567, Tmax = 0.638k = 8→11
6139 measured reflectionsl = 18→14
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.026  w = 1/[σ2(Fo2) + (0.0284P)2 + 2.1868P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.065(Δ/σ)max = 0.001
S = 1.14Δρmax = 0.68 e Å3
708 reflectionsΔρmin = 0.39 e Å3
75 parametersExtinction correction: none
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack (1983), 235 Friedel pairs
Secondary atom site location: difference Fourier mapFlack parameter: 0.01 (3)
Crystal data top
LiNi(H2O)2[BP2O8]·H2Oγ = 120º
Mr = 320.44V = 1188.82 (10) Å3
Hexagonal, P6522Z = 6
a = 9.3359 (3) ÅMo Kα
b = 9.3359 (3) ŵ = 2.91 mm1
c = 15.7497 (11) ÅT = 296 K
α = 90º0.22 × 0.20 × 0.17 mm
β = 90º
Data collection top
Bruker APEXII CCD area-detector
diffractometer
708 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2007)
684 reflections with I > 2σ(I)
Tmin = 0.567, Tmax = 0.638Rint = 0.049
6139 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.026H-atom parameters constrained
wR(F2) = 0.065Δρmax = 0.68 e Å3
S = 1.14Δρmin = 0.39 e Å3
708 reflectionsAbsolute structure: Flack (1983), 235 Friedel pairs
75 parametersFlack parameter: 0.01 (3)
Special details top

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) top
xyzUiso*/Ueq
Ni10.55533 (4)0.44467 (4)0.08330.0098 (2)
P20.38859 (12)0.21675 (12)0.24795 (7)0.0093 (3)
O50.4156 (3)0.2355 (3)0.34570 (16)0.0108 (6)
O40.2137 (3)0.1899 (4)0.23106 (18)0.0129 (7)
O30.4865 (4)0.1970 (4)0.05090 (19)0.0214 (7)
O20.5200 (4)0.3782 (3)0.21028 (17)0.0142 (7)
O10.3853 (4)0.0644 (4)0.21452 (17)0.0151 (7)
O60.2044 (10)0.1022 (5)0.08330.079 (2)
B0.3037 (8)0.1518 (4)0.41670.0090 (13)
Li0.466 (3)0.2331 (13)0.08330.080 (5)
H3A0.57380.21960.02840.096*
H60.15090.03820.12230.096*
H3B0.44280.15710.09730.096*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ni10.0098 (3)0.0098 (3)0.0100 (3)0.0050 (3)0.0013 (3)0.0013 (3)
P20.0097 (5)0.0097 (5)0.0086 (5)0.0050 (4)0.0015 (4)0.0015 (4)
O50.0095 (14)0.0126 (16)0.0089 (13)0.0044 (12)0.0014 (11)0.0016 (11)
O40.0131 (16)0.0132 (15)0.0157 (16)0.0091 (13)0.0022 (12)0.0030 (12)
O30.0277 (18)0.0162 (18)0.0231 (17)0.0130 (14)0.0121 (14)0.0049 (14)
O20.0143 (16)0.0134 (14)0.0101 (13)0.0032 (13)0.0021 (12)0.0040 (11)
O10.0211 (17)0.0159 (16)0.0147 (14)0.0140 (14)0.0008 (14)0.0017 (12)
O60.083 (6)0.061 (3)0.100 (6)0.042 (3)0.0000.024 (4)
B0.012 (3)0.009 (2)0.007 (3)0.0059 (15)0.0000.001 (2)
Li0.094 (15)0.089 (10)0.058 (10)0.047 (8)0.0000.011 (10)
Geometric parameters (Å, °) top
Ni1—O1i2.048 (3)O4—Bi1.471 (5)
Ni1—O1ii2.048 (3)O3—Li2.164 (4)
Ni1—O2iii2.070 (3)O2—Liiv2.113 (13)
Ni1—O22.070 (3)O1—Ni1v2.048 (3)
Ni1—O32.130 (3)O6—Li2.12 (2)
Ni1—O3iii2.130 (3)B—O5vi1.461 (5)
Ni1—Li3.137 (5)B—O4vii1.471 (5)
Ni1—Liiv3.137 (5)B—O4v1.471 (5)
P2—O11.503 (3)Li—O2iii2.113 (13)
P2—O21.510 (3)Li—O2viii2.113 (13)
P2—O41.546 (3)Li—O3ix2.164 (4)
P2—O51.556 (3)Li—Ni1viii3.137 (5)
O5—B1.461 (5)
O1i—Ni1—O1ii92.58 (18)B—O5—P2131.6 (3)
O1i—Ni1—O2iii88.53 (11)Bi—O4—P2127.8 (3)
O1ii—Ni1—O2iii101.19 (12)Ni1—O3—Li93.87 (18)
O1i—Ni1—O2101.19 (12)P2—O2—Ni1127.36 (17)
O1ii—Ni1—O288.53 (11)P2—O2—Liiv129.2 (4)
O2iii—Ni1—O2166.00 (17)Ni1—O2—Liiv97.1 (2)
O1i—Ni1—O386.52 (13)P2—O1—Ni1v140.72 (18)
O1ii—Ni1—O3177.55 (12)O5vi—B—O5103.4 (4)
O2iii—Ni1—O381.08 (11)O5vi—B—O4vii111.43 (15)
O2—Ni1—O389.40 (11)O5—B—O4vii114.16 (15)
O1i—Ni1—O3iii177.55 (12)O5vi—B—O4v114.16 (15)
O1ii—Ni1—O3iii86.52 (13)O5—B—O4v111.43 (16)
O2iii—Ni1—O3iii89.40 (11)O4vii—B—O4v102.6 (4)
O2—Ni1—O3iii81.08 (11)O2iii—Li—O2viii106.9 (9)
O3—Ni1—O3iii94.47 (19)O2iii—Li—O6126.5 (5)
O1i—Ni1—Li72.0 (4)O2viii—Li—O6126.5 (5)
O1ii—Ni1—Li138.23 (8)O2iii—Li—O379.3 (3)
O2iii—Ni1—Li41.9 (3)O2viii—Li—O395.5 (4)
O2—Ni1—Li131.83 (17)O6—Li—O394.3 (6)
O3—Ni1—Li43.50 (9)O2iii—Li—O3ix95.5 (4)
O3iii—Ni1—Li107.3 (4)O2viii—Li—O3ix79.3 (3)
O1i—Ni1—Liiv138.23 (8)O6—Li—O3ix94.3 (6)
O1ii—Ni1—Liiv72.0 (4)O3—Li—O3ix171.3 (11)
O2iii—Ni1—Liiv131.83 (17)O2iii—Li—Ni140.91 (9)
O2—Ni1—Liiv41.9 (3)O2viii—Li—Ni1118.8 (6)
O3—Ni1—Liiv107.3 (4)O6—Li—Ni1103.3 (4)
O3iii—Ni1—Liiv43.50 (9)O3—Li—Ni142.64 (13)
Li—Ni1—Liiv143.2 (5)O3ix—Li—Ni1134.5 (3)
O1—P2—O2115.38 (17)O2iii—Li—Ni1viii118.8 (6)
O1—P2—O4105.45 (17)O2viii—Li—Ni1viii40.91 (9)
O2—P2—O4111.07 (18)O6—Li—Ni1viii103.3 (4)
O1—P2—O5112.24 (16)O3—Li—Ni1viii134.5 (4)
O2—P2—O5105.75 (16)O3ix—Li—Ni1viii42.64 (13)
O4—P2—O5106.70 (15)Ni1—Li—Ni1viii153.4 (7)
Symmetry codes: (i) xy, x, z−1/6; (ii) −x+1, −x+y+1, −z+1/3; (iii) −y+1, −x+1, −z+1/6; (iv) −x+y+1, −x+1, z+1/3; (v) y, −x+y, z+1/6; (vi) x, xy, −z+5/6; (vii) y, x, −z+2/3; (viii) −y+1, xy, z−1/3; (ix) x, xy, −z−1/6.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O3—H3A···O5viii0.812.012.746 (4)151
O3—H3A···O2viii0.812.603.165 (4)128
O6—H6···O4x0.832.523.331 (4)167
O6—H6···O1x0.832.663.092 (4)114
O3—H3B···O10.832.002.810 (4)167
O3—H3B···O20.832.542.955 (4)112
Symmetry codes: (viii) −y+1, xy, z−1/3; (x) xy, −y, −z.
Table 1
Selected geometric parameters (Å)
top
Ni1—O1i2.048 (3)P2—O51.556 (3)
Ni1—O22.070 (3)O6—Li2.12 (2)
Ni1—O32.130 (3)B—O5ii1.461 (5)
P2—O11.503 (3)B—O4iii1.471 (5)
P2—O21.510 (3)Li—O2iv2.113 (13)
P2—O41.546 (3)Li—O3v2.164 (4)
Symmetry codes: (i) −x+1, −x+y+1, −z+1/3; (ii) x, xy, −z+5/6; (iii) y, x, −z+2/3; (iv) −y+1, xy, z−1/3; (v) x, xy, −z−1/6.
Table 2
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O3—H3A···O5iv0.812.012.746 (4)151
O3—H3A···O2iv0.812.603.165 (4)128
O6—H6···O4vi0.832.523.331 (4)167
O6—H6···O1vi0.832.663.092 (4)114
O3—H3B···O10.832.002.810 (4)167
O3—H3B···O20.832.542.955 (4)112
Symmetry codes: (iv) −y+1, xy, z−1/3; (vi) xy, −y, −z.
Acknowledgements top

This work was supported by the Main Teacher Project of Hena Province (grant No. 649082) and the Foundation of Graduate Produce (reference 2008-M-17).

references
References top

Boy, I. & Kniep, R. J. (2001). Z. Kristallogr. New Cryst. Struct. 216, 9–10.

Bruker (2007). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.

Ewald, B., Huang, Y.-X. & Kniep, R. (2007). Z. Anorg. Allg. Chem. 633, 1517–1540.

Flack, H. D. (1983). Acta Cryst. A39, 876–881.

Kniep, R., Engelhardt, H. & Hauf, C. (1998). Chem. Mater. 10, 2930–2934.

Lin, J.-R., Huang, Y.-X., Wu, Y.-H. & Zhou, Y. (2008). Acta Cryst. E64, i39–i40.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.