Download citation
Download citation
link to html
The title synthesized hypophosphite has the formula V(H2PO2)3. Its structure is based on VO6 octa­hedra and (H2PO2)- pseudo-tetra­hedra. The asymmetric unit contains two crystallographically distinct V atoms and six independent (H2PO2)- groups. The connection of the polyhedra generates [VPO6H2]6- chains extended along a, b and c, leading to the first three-dimensional network of an anhydrous transition metal hypophosphite.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270109021325/fn3018sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270109021325/fn3018Isup2.hkl
Contains datablock I

Comment top

During the past few decades, several metal hypophosphite compounds have been reported in the literature, incorporating alkali, alkaline earth (Galigné & Dumas, 1973; Kuratieva et al., 2005), transition (Marcos et al., 1993, 1994; Kuratieva et al., 2002), lanthanide and group 14 metals. Several line of interest have led us to investigate this class of compounds. Among them are (i) the study of low-dimensional structures suitable for catalytic or ion-exchange properties supported by the low degree of connectivity of the oxoanion H2PO2- ; (ii) the characterization of lanthanide ions involving the use of the (H2PO2)- ligand (Seddon et al., 1999; Tanner et al., 1999, 2000); and (iii) the application of anhydrous metal hypophosphites as mild reducing agents, reagents in catalytic syntheses of organophosphorous compounds and antioxidants (Naumova et al., 2004a,b ?????). Another interest was the magnetic properties of some hypophosphite complexes of transtion metals (Marcos et al., 1992; Yoshida et al., 2009).

Although a number of crystal structures of hypophosphites are known, there is a lack of structural data for anhydrous transition metal hypophosphites. In fact, only two such compounds have been characterized by X-ray diffraction, namely Fe(H2PO2)3 (Kuratieva & Naumov, 2006), exhibiting a layered structure built up from iron hypophosphite chains, and Zn(H2PO2)2 (Tanner et al., 1997), comprising a two-dimensional structure.

At the same time and to the best of our knowledge, only one vanadium hypophosphite has been isolated. It is hydrated and exhibits a one-dimensional structure (Le Bail et al., 1994) where the metallic cation is involved in an oxovanadium group. The aim of our study is to enlarge the hypophosphite family compounds, especially for metals like vanadium, which adopts different coordination geometries.

Our study reports the first anhydrous vanadium phosphinate. The asymmetric unit (Fig. 1) contains two independent V atoms and six phosphinate ions, all situated on general positions. Atoms V1 and V2 both exhibit a slightly distorted octahedral geometry, where the mean values of the V—O bonds are 1.998 (3) Å and 1.997 (3) Å, respectively. The hypophosphite groups have pseudotetrahedral geometry. The bond distances and angles (Table 1) in the H2PO2- pseudotetrahedra are similar to those observed in other hypophosphite compounds. The VIIIO6 octahedra share all their vertices with six distinct pseudotetrahedra, and each H2PO2- anion has both of its O atoms linked to two adjacent metallic centers, acting as a bidentate bridging ligand. This type of connection involves the formation of V—O—P—O—V chains through the three directions of the space, leading therefore to a three-dimensional network. The junction of the V1, V2, O and P atoms along the a axis describes helicoidal chains, while along the c-axis direction it forms a sawtooth curve (Figs. 3a and 3b). Along the b axis, the V2—O—P—O—V2 chains follow a helicoidal pattern with an elliptical cross section and the V1—O—P—O—V1 chains might be assimilated to a sinusoid (Fig. 3c). While in the oxovanadium(IV) hypophosphite (Le Bail et al., 1994) the one-dimensional aspect of the structure is related to the anisotropic environment of the vanadium, in the title compound the three-dimensionality is favoured by the isotropic bonding scheme of the cation owing to its +3 oxidation state.

Related literature top

For related literature, see: Galigné & Dumas (1973); Kuratieva, Naumova & Naumov (2005); Kuratieva et al. (2005); Marcos et al. (1992, 1993); Seddon et al. (1999); Tanner et al. (1997, 1999); Yoshida et al. (2009).

Experimental top

Vanadium(III) hypophosphite was synthesized by a hydrothermal method. A mixture of deionzed water, vanadium(V) oxide, 50% hypophosphoric acid and lithium carbonate in a molar ratio of 10.437:0.1:2:0.428 was placed in a Teflon acid digestion bomb (23 ml, Parr Instruments), heated at 423 K for 48 h and cooled to room temperature over a period of 24 h. The green product was filtered off, washed with deionized water and dried at room temperature in a desiccator.

The comparison of the X-ray powder diffraction pattern of the synthesized product with the simulated one from this structure revealed that the title compound is present as a minor phase. The major phase remains unknown.

While lithium ions are not present in this structure, the presence of lithium carbonate seems to be necessary to obtain the title compound, as synthesis attempts performed without the lithium source were unsuccessful.

We assume that the hypophosphoric acid is responsible of the reduction of the vanadium ions observed during the synthesis (V5+ to V3+), as no other reducing agent is present.

Refinement top

The H atoms were located in a Fourier difference map and their positional parameters were refined freely, while their Uiso(H) values were fixed at 0.049 Å2. The refinement of the structure was carried out on a twinned crystal. The transformation matrix used is (001, 010, 100). The refined volume fractions are 94.7 and 5.3%. [Please check modifications to text, inline with data in CIF.]

Computing details top

Data collection: COLLECT (Nonius, 1998); cell refinement: DIRAX/LSQ (Duisenberg, 1992); data reduction: EVALCCD (Duisenberg, 1998); program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2005); software used to prepare material for publication: WinGX (Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. : The asymmetric unit of [V2P6O12H12]12-; displacement ellipsoids of the independent atoms are plotted at the 50% probability level and H atoms are drawn as small spheres of arbitrary radii. [Symmetry codes: (i) x, y, z - 1; (ii) -x + 1/2, y + 1/2, -z + 1/2; (iii) -x + 1/2, y - 1/2, -z + 3/2; (iv) x + 1/2, -y + 1/2, z + 1/2; (v) x - 1/2, -y + 1/2, z + 1/2.]
[Figure 2] Fig. 2. : A perspective view of V(H2PO2)3 along the [001] direction.
[Figure 3] Fig. 3. : A representation of the V—O—P—O—V chains along (a) the [100] direction, (b) the [001] direction and (c) the [010] direction.
vanadium hypophosphite top
Crystal data top
V(H2PO2)3F(000) = 976
Mr = 491.8Dx = 2.11 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 9018 reflections
a = 11.4985 (3) Åθ = 2.9–27.5°
b = 11.7771 (5) ŵ = 1.88 mm1
c = 11.5999 (4) ÅT = 293 K
β = 99.807 (2)°Prism, green
V = 1547.89 (9) Å30.15 × 0.05 × 0.04 mm
Z = 4
Data collection top
Nonius KappaCCD
diffractometer
Rint = 0.117
CCD rotation images, thick slices scansθmax = 27.5°, θmin = 3.6°
20258 measured reflectionsh = 1414
3550 independent reflectionsk = 1513
2426 reflections with I > 2σ(I)l = 1515
Refinement top
Refinement on F2Only H-atom coordinates refined
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0199P)2 + 4.0183P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.053(Δ/σ)max = 0.006
wR(F2) = 0.091Δρmax = 0.50 e Å3
S = 1.04Δρmin = 0.54 e Å3
3550 reflectionsExtinction correction: (SHELXL97; Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
219 parametersExtinction coefficient: 0.0013 (3)
0 restraints
Crystal data top
V(H2PO2)3V = 1547.89 (9) Å3
Mr = 491.8Z = 4
Monoclinic, P21/nMo Kα radiation
a = 11.4985 (3) ŵ = 1.88 mm1
b = 11.7771 (5) ÅT = 293 K
c = 11.5999 (4) Å0.15 × 0.05 × 0.04 mm
β = 99.807 (2)°
Data collection top
Nonius KappaCCD
diffractometer
2426 reflections with I > 2σ(I)
20258 measured reflectionsRint = 0.117
3550 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0530 restraints
wR(F2) = 0.091Only H-atom coordinates refined
S = 1.04Δρmax = 0.50 e Å3
3550 reflectionsΔρmin = 0.54 e Å3
219 parameters
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
V10.24603 (7)0.18513 (6)0.69692 (7)0.01900 (19)
V20.22812 (6)0.20319 (7)0.18963 (7)0.0203 (2)
P10.35198 (11)0.02754 (11)0.30844 (13)0.0302 (3)
P20.04238 (10)0.22262 (11)0.06807 (11)0.0245 (3)
P30.47390 (11)0.34106 (12)0.23653 (12)0.0281 (3)
P40.30125 (14)0.08384 (12)0.95864 (12)0.0357 (4)
P50.23503 (15)0.41320 (12)0.84204 (14)0.0399 (4)
P60.11404 (12)0.20824 (14)0.42549 (12)0.0334 (3)
O10.2886 (3)0.5289 (3)0.8650 (3)0.0331 (8)
O20.3095 (3)0.1342 (3)0.3592 (3)0.0320 (8)
O30.1071 (3)0.3117 (3)0.1251 (3)0.0303 (8)
O40.2596 (3)0.1751 (3)1.0298 (3)0.0377 (9)
O50.3366 (3)0.1189 (3)0.8447 (3)0.0302 (8)
O60.6033 (3)0.3188 (3)0.2748 (3)0.0300 (8)
O70.2806 (3)0.3429 (3)0.7523 (3)0.0342 (9)
O80.2606 (3)0.0390 (3)0.2302 (4)0.0415 (10)
O90.1450 (3)0.2435 (3)0.5517 (3)0.0301 (8)
O100.0580 (3)0.1621 (3)0.1444 (3)0.0332 (9)
O110.2025 (3)0.2393 (4)0.3511 (3)0.0473 (11)
O120.3974 (3)0.2392 (3)0.2420 (3)0.0409 (10)
H1A0.401 (5)0.035 (5)0.403 (5)0.049*
H1B0.448 (5)0.043 (5)0.247 (5)0.049*
H2A0.118 (5)0.142 (5)0.003 (5)0.049*
H2B0.001 (5)0.278 (5)0.027 (5)0.049*
H3A0.451 (4)0.423 (5)0.311 (5)0.049*
H3B0.462 (5)0.387 (5)0.127 (5)0.049*
H4A0.205 (5)0.013 (5)0.935 (5)0.049*
H4B0.387 (4)0.013 (5)1.006 (5)0.049*
H5A0.224 (5)0.365 (5)0.936 (5)0.049*
H5B0.116 (5)0.411 (5)0.829 (5)0.049*
H6A0.091 (5)0.095 (5)0.421 (5)0.049*
H6B0.007 (5)0.249 (5)0.386 (5)0.049*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
V10.0206 (4)0.0182 (4)0.0190 (4)0.0005 (3)0.0058 (3)0.0008 (3)
V20.0204 (4)0.0220 (4)0.0187 (4)0.0005 (3)0.0033 (3)0.0005 (4)
P10.0271 (7)0.0223 (7)0.0383 (8)0.0031 (6)0.0028 (6)0.0086 (6)
P20.0207 (6)0.0283 (7)0.0242 (7)0.0002 (5)0.0027 (5)0.0041 (6)
P30.0204 (6)0.0313 (7)0.0329 (8)0.0017 (6)0.0050 (5)0.0047 (6)
P40.0600 (10)0.0244 (7)0.0273 (8)0.0120 (7)0.0201 (7)0.0067 (6)
P50.0637 (10)0.0181 (7)0.0469 (10)0.0038 (7)0.0351 (8)0.0032 (7)
P60.0290 (7)0.0503 (9)0.0208 (7)0.0022 (7)0.0035 (5)0.0003 (7)
O10.046 (2)0.0171 (17)0.034 (2)0.0030 (16)0.0025 (17)0.0014 (16)
O20.045 (2)0.0203 (18)0.031 (2)0.0015 (16)0.0077 (16)0.0057 (15)
O30.0289 (17)0.0278 (19)0.038 (2)0.0020 (16)0.0153 (15)0.0021 (16)
O40.061 (2)0.032 (2)0.023 (2)0.0132 (19)0.0158 (18)0.0015 (16)
O50.0291 (18)0.043 (2)0.0199 (18)0.0078 (16)0.0071 (15)0.0030 (16)
O60.0160 (15)0.049 (2)0.0257 (18)0.0016 (16)0.0048 (13)0.0000 (17)
O70.043 (2)0.027 (2)0.036 (2)0.0029 (17)0.0155 (17)0.0055 (16)
O80.0305 (19)0.029 (2)0.059 (3)0.0004 (17)0.0079 (18)0.0171 (19)
O90.0386 (19)0.0309 (19)0.0213 (18)0.0118 (16)0.0067 (15)0.0007 (15)
O100.0246 (17)0.0252 (19)0.047 (2)0.0027 (15)0.0034 (16)0.0076 (17)
O110.051 (2)0.068 (3)0.026 (2)0.016 (2)0.0163 (18)0.007 (2)
O120.0247 (18)0.044 (2)0.050 (2)0.0100 (17)0.0043 (17)0.0121 (19)
Geometric parameters (Å, º) top
V1—O71.984 (3)P3—O61.502 (3)
V1—O1i1.991 (3)P3—H3A1.35 (6)
V1—O91.998 (3)P3—H3B1.37 (6)
V1—O6ii2.004 (3)P4—O41.484 (4)
V1—O3iii2.006 (3)P4—O51.505 (4)
V1—O52.007 (3)P4—H4A1.38 (6)
V2—O4iv1.976 (3)P4—H4B1.34 (5)
V2—O121.984 (3)P5—O71.493 (4)
V2—O111.990 (4)P5—O11.500 (4)
V2—O101.996 (3)P5—H5A1.25 (6)
V2—O82.010 (4)P5—H5B1.36 (5)
V2—O2v2.023 (3)P6—O111.488 (4)
P1—O81.488 (4)P6—O91.505 (3)
P1—O21.504 (3)P6—H6A1.36 (6)
P1—H1A1.36 (6)P6—H6B1.32 (5)
P1—H1B1.43 (5)O1—V1vi1.991 (3)
P2—O31.504 (3)O2—V2vii2.023 (3)
P2—O101.508 (3)O3—V1viii2.006 (3)
P2—H2A1.42 (5)O4—V2ix1.976 (3)
P2—H2B1.43 (5)O6—V1x2.004 (3)
P3—O121.495 (4)
O7—V1—O1i177.79 (15)O3—P2—H2B106 (2)
O7—V1—O990.39 (15)O10—P2—H2B110 (2)
O1i—V1—O987.82 (14)H2A—P2—H2B99 (3)
O7—V1—O6ii90.56 (15)O12—P3—O6114.1 (2)
O1i—V1—O6ii90.71 (15)O12—P3—H3A112 (2)
O9—V1—O6ii89.14 (14)O6—P3—H3A103 (2)
O7—V1—O3iii88.90 (14)O12—P3—H3B113 (2)
O1i—V1—O3iii89.90 (14)O6—P3—H3B106 (2)
O9—V1—O3iii93.05 (14)H3A—P3—H3B108 (3)
O6ii—V1—O3iii177.75 (15)O4—P4—O5116.8 (2)
O7—V1—O592.36 (15)O4—P4—H4A103 (2)
O1i—V1—O589.51 (15)O5—P4—H4A109 (2)
O9—V1—O5175.46 (15)O4—P4—H4B121 (2)
O6ii—V1—O587.22 (13)O5—P4—H4B104 (2)
O3iii—V1—O590.62 (14)H4A—P4—H4B102 (3)
O4iv—V2—O1289.79 (17)O7—P5—O1116.4 (2)
O4iv—V2—O11176.70 (17)O7—P5—H5A117 (3)
O12—V2—O1187.77 (16)O1—P5—H5A111 (3)
O4iv—V2—O1092.31 (16)O7—P5—H5B113 (2)
O12—V2—O10177.05 (15)O1—P5—H5B114 (2)
O11—V2—O1090.21 (16)H5A—P5—H5B81 (3)
O4iv—V2—O890.13 (16)O11—P6—O9115.2 (2)
O12—V2—O890.02 (15)O11—P6—H6A112 (2)
O11—V2—O892.08 (18)O9—P6—H6A108 (2)
O10—V2—O887.90 (14)O11—P6—H6B113 (2)
O4iv—V2—O2v87.75 (14)O9—P6—H6B107 (2)
O12—V2—O2v92.00 (15)H6A—P6—H6B100 (3)
O11—V2—O2v90.13 (17)P5—O1—V1vi136.4 (2)
O10—V2—O2v90.16 (14)P1—O2—V2vii138.6 (2)
O8—V2—O2v177.06 (15)P2—O3—V1viii135.3 (2)
O8—P1—O2115.8 (2)P4—O4—V2ix140.5 (2)
O8—P1—H1A111 (2)P4—O5—V1132.7 (2)
O2—P1—H1A105 (2)P3—O6—V1x135.8 (2)
O8—P1—H1B107 (2)P5—O7—V1132.1 (2)
O2—P1—H1B115 (2)P1—O8—V2137.1 (2)
H1A—P1—H1B103 (3)P6—O9—V1137.1 (2)
O3—P2—O10117.3 (2)P2—O10—V2131.1 (2)
O3—P2—H2A113 (2)P6—O11—V2136.0 (3)
O10—P2—H2A110 (2)P3—O12—V2135.4 (2)
Symmetry codes: (i) x+1/2, y1/2, z+3/2; (ii) x1/2, y+1/2, z+1/2; (iii) x+1/2, y+1/2, z+1/2; (iv) x, y, z1; (v) x+1/2, y+1/2, z+1/2; (vi) x+1/2, y+1/2, z+3/2; (vii) x+1/2, y1/2, z+1/2; (viii) x1/2, y+1/2, z1/2; (ix) x, y, z+1; (x) x+1/2, y+1/2, z1/2.

Experimental details

Crystal data
Chemical formulaV(H2PO2)3
Mr491.8
Crystal system, space groupMonoclinic, P21/n
Temperature (K)293
a, b, c (Å)11.4985 (3), 11.7771 (5), 11.5999 (4)
β (°) 99.807 (2)
V3)1547.89 (9)
Z4
Radiation typeMo Kα
µ (mm1)1.88
Crystal size (mm)0.15 × 0.05 × 0.04
Data collection
DiffractometerNonius KappaCCD
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
20258, 3550, 2426
Rint0.117
(sin θ/λ)max1)0.650
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.053, 0.091, 1.04
No. of reflections3550
No. of parameters219
H-atom treatmentOnly H-atom coordinates refined
Δρmax, Δρmin (e Å3)0.50, 0.54

Computer programs: COLLECT (Nonius, 1998), DIRAX/LSQ (Duisenberg, 1992), EVALCCD (Duisenberg, 1998), SIR97 (Altomare et al., 1999), SHELXL97 (Sheldrick, 2008), DIAMOND (Brandenburg, 2005), WinGX (Farrugia, 1999).

Selected geometric parameters (Å, º) top
V1—O71.984 (3)P1—H1B1.43 (5)
V1—O52.007 (3)P2—O101.508 (3)
V2—O4i1.976 (3)P4—O41.484 (4)
V2—O2ii2.023 (3)P5—H5A1.25 (6)
O7—V1—O1iii177.79 (15)O12—P3—O6114.1 (2)
O9—V1—O3iv93.05 (14)H3A—P3—H3B108 (3)
O9—V1—O5175.46 (15)O4—P4—H4A103 (2)
O6v—V1—O587.22 (13)O4—P4—H4B121 (2)
O3—P2—O10117.3 (2)H5A—P5—H5B81 (3)
Symmetry codes: (i) x, y, z1; (ii) x+1/2, y+1/2, z+1/2; (iii) x+1/2, y1/2, z+3/2; (iv) x+1/2, y+1/2, z+1/2; (v) x1/2, y+1/2, z+1/2.
 

Follow Acta Cryst. C
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds