supplementary materials


Acta Cryst. (2007). E63, i170    [ doi:10.1107/S1600536807027195 ]

Polymeric KNOF2

T. Liu, Z.-W. Wang, Y.-X. Wang and Z.-P. Xie

Abstract top

The title compound, poly[[mu]-difluoridooxidonitrato-potassium], [KNOF2]n, crystallizes in the orthorhombic system and adopts the ordered KNO3 structure type. A crystallographic mirror plane passes through N, O and K. In the crystal structure, the polymer chains are linked by weak bonds into an infinite three-dimensional framework.

Comment top

Inorganic compounds with various anions attract attention because of the features of their crystal chemistry (Berdonosov et al., 2000; Ruck & Schmidt, 2003; Lipp & Schleid, 2005; Ben Hamida & Wickleder, 2005).The first probable crystallographic path in single crystals of KNO3 was reported by Swaminathan et al. in 1975. In the following years, the compounds KNO3 were synthesized and characterized by Nimmo & Lucas (1976), Soltzberg et al. (1994) and Christensen et al. (1996). We herein report the crystal structure of the title compound, (I).

In the molecule of (I), the bond lengths and angles (Table 1) are within normal ranges. One of F atoms in KNOF2 (Fig. 1) is symmetry related with symmetry code (x, -y + 3/2, z). KNOF2 crystallizes in the orthorhombic system and adopts the ordered KNO3 structure type. The [KNOF2]n structure is a coordination network polymer, in which K+ cations are connected by the anions coordinated through F and O atoms.

Related literature top

For related literature, see: Ben Hamida & Wickleder (2005); Berdonosov et al. (2000); Christensen et al. (1996); Lipp & Schleid (2005); Nimmo & Lucas (1976); Ruck & Schmidt (2003); Soltzberg et al. (1994); Swaminathan & Srinivasan (1975).

Experimental top

Crystals of the title compound were synthesized using solid-state reaction method. KF (58 mg, 1 mmol), NaNO3 (170 mg, 2 mmol), corresponding to a molar ratio of 1:2, were heated in a graphite crucible under a static atmosphere of a (98/2)% mixture of N2/H2 up to 1173 K over the course of 6 h. This temperature was held for 2 h and then decreased to 773 K within 20 h. After cooling to room temperature, the solidified melt was leached with demineralized water. From the remaining residue, colourless plates of KNOF2 could be isolated.

Computing details top

Data collection: APEX2 (Bruker, YEAR?); cell refinement: SAINT (Siemens, 1996); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Siemens, 1996); software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. The molecular structure of the title molecule, with the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level [symmetry code (A): -x + 1, -y + 1, -z + 1; (C): -x + 1, -y + 2, -z + 1; (E): x, -y + 3/2, z; (G): -x + 3/2, -y + 2, z + 1/2].
[Figure 2] Fig. 2. A packing diagram for (I).
poly[µ-difluoridooxidonitrato-potassium] top
Crystal data top
KNOF2F(000) = 208
Mr = 107.11Dx = 2.229 Mg m3
Orthorhombic, PnmaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2nCell parameters from 1198 reflections
a = 6.429 (4) Åθ = 4.4–28.3°
b = 5.417 (3) ŵ = 1.51 mm1
c = 9.164 (5) ÅT = 273 K
V = 319.1 (3) Å3Block, colourless
Z = 40.27 × 0.10 × 0.06 mm
Data collection top
Bruker APEXII area-detector
diffractometer
372 independent reflections
Radiation source: fine-focus sealed tube304 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.018
φ and ω scansθmax = 27.0°, θmin = 3.9°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 78
Tmin = 0.686, Tmax = 0.915k = 66
2043 measured reflectionsl = 1111
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullPrimary atom site location: structure-invariant direct methods
R[F2 > 2σ(F2)] = 0.039Secondary atom site location: difference Fourier map
wR(F2) = 0.163 w = 1/[σ2(Fo2) + (0.128P)2 + 0.1109P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max < 0.001
372 reflectionsΔρmax = 0.37 e Å3
28 parametersΔρmin = 0.55 e Å3
Crystal data top
KNOF2V = 319.1 (3) Å3
Mr = 107.11Z = 4
Orthorhombic, PnmaMo Kα radiation
a = 6.429 (4) ŵ = 1.51 mm1
b = 5.417 (3) ÅT = 273 K
c = 9.164 (5) Å0.27 × 0.10 × 0.06 mm
Data collection top
Bruker APEXII area-detector
diffractometer
372 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
304 reflections with I > 2σ(I)
Tmin = 0.686, Tmax = 0.915Rint = 0.018
2043 measured reflectionsθmax = 27.0°
Refinement top
R[F2 > 2σ(F2)] = 0.039Δρmax = 0.37 e Å3
wR(F2) = 0.163Δρmin = 0.55 e Å3
S = 1.06Absolute structure: ?
372 reflectionsFlack parameter: ?
28 parametersRogers parameter: ?
0 restraints
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
K10.75494 (11)0.75000.58346 (8)0.0285 (5)
O10.4098 (5)0.75000.3901 (3)0.0392 (8)
N10.4145 (5)0.75000.2554 (3)0.0244 (8)
F10.4144 (3)0.9496 (4)0.1866 (2)0.0554 (8)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
K10.0334 (8)0.0254 (8)0.0267 (7)0.0000.0009 (3)0.000
O10.051 (2)0.0380 (19)0.0285 (14)0.0000.0061 (13)0.000
N10.0198 (17)0.0232 (16)0.0303 (16)0.0000.0008 (12)0.000
F10.0757 (17)0.0402 (13)0.0502 (13)0.0044 (10)0.0045 (11)0.0050 (8)
Geometric parameters (Å, º) top
K1—O12.840 (3)K1—N1ii3.272 (2)
O1—N11.235 (4)K1—N1iv3.272 (2)
N1—F11.251 (3)O1—K1iv2.9185 (18)
K1—F1i2.839 (2)O1—K1ii2.9185 (18)
K1—F1ii2.876 (2)N1—F1viii1.251 (3)
K1—F1iii2.889 (2)N1—K1ix3.270 (4)
K1—O1iv2.9185 (18)N1—K1ii3.272 (2)
K1—F1v2.839 (2)N1—K1iv3.272 (2)
K1—F1vi2.876 (2)F1—K1x2.839 (2)
K1—F1vii2.889 (2)F1—K1ii2.876 (2)
K1—O1ii2.9185 (18)F1—K1ix2.889 (2)
K1—N1vii3.270 (4)
F1i—K1—O1142.45 (5)O1—K1—N1ii91.24 (7)
O1—K1—F1ii99.29 (8)F1ii—K1—N1ii22.32 (7)
F1i—K1—F1v69.95 (10)F1vi—K1—N1ii90.68 (8)
F1v—K1—O1142.45 (5)F1iii—K1—N1ii144.56 (7)
F1i—K1—F1ii73.45 (6)F1vii—K1—N1ii101.25 (7)
F1v—K1—F1ii111.33 (6)O1iv—K1—N1ii127.59 (8)
F1i—K1—F1vi111.33 (6)O1ii—K1—N1ii22.07 (8)
F1v—K1—F1vi73.45 (6)N1vii—K1—N1ii122.21 (6)
O1—K1—F1vi99.29 (8)F1i—K1—N1iv124.99 (8)
F1ii—K1—F1vi68.92 (10)F1v—K1—N1iv67.94 (7)
F1i—K1—F1iii103.54 (5)O1—K1—N1iv91.24 (7)
F1v—K1—F1iii78.76 (7)F1ii—K1—N1iv90.68 (8)
O1—K1—F1iii75.08 (8)F1vi—K1—N1iv22.32 (7)
F1ii—K1—F1iii166.82 (9)F1iii—K1—N1iv101.25 (7)
F1vi—K1—F1iii123.38 (4)F1vii—K1—N1iv144.56 (7)
F1i—K1—F1vii78.76 (7)O1iv—K1—N1iv22.07 (8)
F1v—K1—F1vii103.54 (5)O1ii—K1—N1iv127.59 (8)
O1—K1—F1vii75.08 (8)N1vii—K1—N1iv122.21 (6)
F1ii—K1—F1vii123.38 (4)N1ii—K1—N1iv111.77 (10)
F1vi—K1—F1vii166.82 (9)N1—O1—K1127.2 (2)
F1iii—K1—F1vii43.96 (10)N1—O1—K1iv95.27 (9)
F1i—K1—O1iv140.90 (7)K1—O1—K1iv103.40 (6)
F1v—K1—O1iv73.27 (8)N1—O1—K1ii95.27 (9)
O1—K1—O1iv76.60 (6)K1—O1—K1ii103.40 (6)
F1ii—K1—O1iv109.08 (8)K1iv—O1—K1ii136.28 (12)
F1vi—K1—O1iv43.67 (8)O1—N1—F1viii120.23 (17)
F1iii—K1—O1iv81.53 (8)O1—N1—F1120.23 (17)
F1vii—K1—O1iv123.18 (7)F1viii—N1—F1119.5 (3)
F1i—K1—O1ii73.27 (8)O1—N1—K1ix160.3 (2)
F1v—K1—O1ii140.90 (7)F1viii—N1—K1ix61.43 (17)
O1—K1—O1ii76.60 (6)F1—N1—K1ix61.43 (17)
F1ii—K1—O1ii43.67 (8)O1—N1—K1ii62.66 (9)
F1vi—K1—O1ii109.08 (8)F1viii—N1—K1ii160.5 (2)
F1iii—K1—O1ii123.18 (7)F1—N1—K1ii60.79 (13)
F1vii—K1—O1ii81.53 (8)K1ix—N1—K1ii108.92 (7)
O1iv—K1—O1ii136.28 (12)O1—N1—K1iv62.66 (9)
F1i—K1—N1vii94.67 (7)F1viii—N1—K1iv60.79 (13)
F1v—K1—N1vii94.67 (7)F1—N1—K1iv160.5 (2)
O1—K1—N1vii69.66 (9)K1ix—N1—K1iv108.92 (7)
F1ii—K1—N1vii144.52 (5)K1ii—N1—K1iv111.77 (10)
F1vi—K1—N1vii144.52 (5)N1—F1—K1x131.51 (18)
F1iii—K1—N1vii22.36 (5)N1—F1—K1ii96.89 (17)
F1vii—K1—N1vii22.36 (5)K1x—F1—K1ii101.71 (7)
O1iv—K1—N1vii101.11 (6)N1—F1—K1ix96.21 (18)
O1ii—K1—N1vii101.11 (6)K1x—F1—K1ix101.24 (7)
F1i—K1—N1ii67.94 (7)K1ii—F1—K1ix134.83 (8)
F1v—K1—N1ii124.99 (8)
Symmetry codes: (i) x+3/2, y+2, z+1/2; (ii) x+1, y+2, z+1; (iii) x+1/2, y+3/2, z+1/2; (iv) x+1, y+1, z+1; (v) x+3/2, y1/2, z+1/2; (vi) x+1, y1/2, z+1; (vii) x+1/2, y, z+1/2; (viii) x, y+3/2, z; (ix) x1/2, y, z+1/2; (x) x+3/2, y+2, z1/2.
Selected geometric parameters (Å, º) top
K1—O12.840 (3)K1—F1ii2.876 (2)
O1—N11.235 (4)K1—F1iii2.889 (2)
N1—F11.251 (3)K1—O1iv2.9185 (18)
K1—F1i2.839 (2)
F1i—K1—O1142.45 (5)O1—K1—F1ii99.29 (8)
Symmetry codes: (i) x+3/2, y+2, z+1/2; (ii) x+1, y+2, z+1; (iii) x+1/2, y+3/2, z+1/2; (iv) x+1, y+1, z+1.
Acknowledgements top

The authors thank the Youth Programme of Jinggangshan University for financial support of this work.

references
References top

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